Kvant
Kvant 1971, No. 3

Kvant 1971, No. 3 · Pages

Sheet 1

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Popular science physics and mathematics
quantum
3
1971
magazine
Academy
Sciences of the USSR
And
Academy of Pedagogical
Sciences of the USSR

Sheet 2

unnumberedTranscribed from the scan · Rough draft translation, low quality

In the room:

Economics and linear inequalities 1
A. B. Skating rink

Converting electrical circuits 10
A. R. Zilberman

Do you like messing around with goal numbers! 15
M. I. Batsimakov

Amazing skating rinks 21
B. Yu. Kodan

Math club
Semiregular polygons 25
L. M. Lopovok

Problem «Kvant»
Problems 30

Solutions to problems M26—M28; F35—F40 32
N. B. Vasiliev,
A. N. Vilenkin,
I. Sh. Slobodetsky

Applicant’s workshop
Exponential Equations 40
V. V. Goldberd

Written exam in mathematics at mexmate Moscow State University in 1970 45
N. N. Kolesnikov

Written exam in physics at the Moscow Automobile and Road Institute 51
A. N. Ageev,
Yu. G. Rudoy

Physics News 57

Reviews, bibliography
If you need to calculate something…
57
R. S. Guter

The Sorcerer from Plutalova Street 58
G. I. Mishchevich

Answers, directions, solutions 62

Collector’s Corner
Stamps dedicated to N. E. Zhukovsky 64
A. V. Altykis

«Kvant» for younger students
3rd cover page
Crossword
4th cover page

Sheet 4

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2

that together with two road bicycles the plant can produce one racing bicycle, and the racing bicycle brings 1.5 times more profit. The factory can produce 700 road bikes per day, but the warehouse can only accept 500 bikes per day. How many racing bikes and how many road bikes do you need to produce per day in order for the plant to get the maximum approximation?

  1. Problem about quarries. At points A and B there are brick factories, and at points C and D there are quarries that supply them with sand. The need of factories for sand is no more than the productivity of quarries. It is known how much sand each plant needs and how much is added to each quarry. In addition, it is known how much it costs to transport a ton of sand from each quarry to the factories. It is necessary to organize the supply of sand to factories so that costs are minimal. (Such tasks are called transortins.)

  2. Problem about chicken feed. The poultry farmer is engaged in open-casting of chickens. Let us assume for simplicity that two products can serve as food - wheat and peas. In order for a chicken to grow normally, its daily diet must contain at least a certain amount of calories, as well as proteins, fats and carbohydrates. These quantities are established by esophageal specialists, and we should consider them as given. Let it be known how much fat, proteins, fats and carbohydrates are contained in one gram of wheat and one gram of peas, and the price of each type of food is also known. How to create the cheapest but most complete diet?

In each of the above, it is necessary to make the optimal choice, although in each problem it is understood differently.

In order to see what mathematical questions arose when solving such problems, let us analyze in detail the problem of chicken feed.

To analyze this problem, you will receive all the information that is included in the school course, and all calculations can be easily checked using pencil and paper.

Let one gram of wheat contain a1a_1 calories, one gram of peas contain b1b_1 calories, and the minimum required number of calories in the daily diet is c1c_1. We will depict menus containing xx grams of wheat and yy grams of peas by point (x,y)(x, y) on the plane. Let’s try to highlight those points on the plane that correspond to diets containing at least c1c_1 calories. Since a menu consisting of xx grams of wheat and yy grams of peas contains a1x+b1ya_1x+b_1y calories, the inequality a1x+b1y≥c1a_1x+b_1y \geq c_1 holds for such points.

From your school algebra course you know that the points for which a1x+b1y=c1a_1x+b_1y=c_1 lie on the line l1l_1 passing through the points (0,c1b1)(0, \frac{c_1}{b_1}) and (c1a1,0)(\frac{c_1}{a_1}, 0). This straight line divides the plane into two parts. For the point (x,y)(x, y), lying on one side of the line l1l_1, the inequality a1x+b1y>c1a_1x+b_1y > c_1 is satisfied, and for the point lying on the other side, the inequality a1x+b1y<c1a_1x+b_1y < c_1 is satisfied. Each of these parts, together with the straight line l1l_1, is called a half-plane. Thus, one half-plane consists of all points (x,y)(x, y) for which a1x+b1y≥c1a_1x+b_1y \geq c_1,

and the other from the point for which a1x+b1y≤c1a_1x+b_1y \leq c_1.

Since in our case a1a_1 and b1b_1 are positive numbers, then the first half-plane is the half-plane L1L_1,

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Which is highlighted at figure 1. In addition, from the conditions of our problem it is clear that xx and yy are non-negative numbers (you MUST NOT give the chicken a negative amount of food). The condition x≥0x \geq 0 is satisfied by the points of the right half-plane (limited by the ordinat axis), the condition y≥0y \geq 0 is satisfied by the points of the upper half-plane (limited by the abscissa axis), and the portions containing at least c1c_1 calories are satisfied by the points (x,y)(x, y), for which three inequalities are simultaneously satisfied:

{x≥0,y≥0,a1x+b1y≥c1,\begin{cases} x \geq 0, y \geq 0, \\ a_1 x + b_1 y \geq c_1, \end{cases}

that is, points lying in the intersection of the right half-plane, the upper half-plane L1L_1. On figure 2 a set of points corresponding to the solution of the system of inequalities (1) is highlighted. Let’s move on to other limited ones. If one gram of solutions contains a2a_2 grams of protein, one gram of peas contains b2b_2 grams of protein, and the daily diet of a chicken should contain at least c2c_2 grams of protein, then, obviously, those diets containing xx grams of solutions and yy grams of peas contain sufficient protein for which

a2x+b2y≥c2.a_2 x + b_2 y \geq c_2.

Corresponding to these ratios, the points lie in the half-plane L2L_2, bounded by the straight line l2l_2, which is given by the equation a2x+b2y=c2a_2 x + b_2 y = c_2. Similarly, the diet must satisfy the inequalities

{a3x+b3y≥c3,a4x+b4y≥c4,\begin{cases} a_3 x + b_3 y \geq c_3, \\ a_4 x + b_4 y \geq c_4, \end{cases}

where a3a_3 and a4a_4 are the amount of fats and carbohydrates in one gram of wheat, b3b_3 and b4b_4 are the amount of fats and carbohydrates in one gram of peas, c3c_3 and c4c_4 are the minimum amount of fats and carbohydrates in the daily diet of a chicken. (All quantities are measured in grams.) Points (x,y)(x, y) that satisfy the first of these two inequalities lie in the half-plane L3L_3, and points satisfying the second inequality lie in the half-plane L4L_4. We will call a diet containing a sufficient amount of all components (calories, proteins, fats and carbohydrates) acceptable. Thus, acceptable diets consisting of xx grams of wheat and yy grams of peas will be those that satisfy the system of six linear inequalities

{x≥0,y≥0,a1x+b1y≥c1,a2x+b2y≥c2,a3x+b3y≥c3,a4x+b4y≥c4.\begin{cases} x \geq 0, y \geq 0, \\ a_1 x + b_1 y \geq c_1, \\ a_2 x + b_2 y \geq c_2, \\ a_3 x + b_3 y \geq c_3, \\ a_4 x + b_4 y \geq c_4. \end{cases}

Correspondence to the admissible ration of the half-plane points lies at the intersection of the right half-plane, the upper half-plane L1L_1, L2L_2, L3L_3, L4L_4, that is, inside or on the boundary of the figure (infinite set-

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4

Fig. 3.

sovereign) AA, allocated to figure 3.

This figure depicts the case when each inequality in system (2) exists, that is, for each of the six inequalities there is a solution to the system of the remaining five inequalities that does not satisfy this inequality. Another possible case is depicted at figure 4.

Geometrically, this means that one of the lines (on Fig. 4 is the line l4l_4) lies outside the set AA, and algebraically, that system (2) is equivalent to a system from which one of the inequalities is excluded (in our case, the last inequality). Throughout what follows, in order not to make special reservations, we will assume that the case depicted in figure 3 occurs.

A set of points on a plane is called convex if, together with any two properties of points, it entirely contains a segment connecting these points. On figure 5, aa the selected non-convex sets are convex, and on figure 5, bb the selected non-convex sets.

A half-plane is a convex set, and since the intersection of any number of a convex set is also a convex set, then the set AA is convex.

Fig. 4.

Now we will try to choose the cheapest one from all acceptable razions. Let 1 gram of wheat cost pp kopecks, and 1 gram of peas cost qq kopecks. then a diet of xx grams of wheat and yy grams of peas costs px+qypx+qy kopecks. Thus, the price is a linear function of xx and yy, and the task of finding the cheapest ratio is to find among all pairs of numbers (x,y)(x, y) that satisfy the system of inequalities (2), such pairs for which the value of this linear function reaches a minimum. In other words, you need to find those from the point of the set AA at which the function px+qypx+qy reaches the smallest value of all the values ​​​​accepted by this function at the points of the set AA.

The set of points (x,y)(x, y) of the plane for which the expression px+qypx+qy is equal to some number kk is a pr-

Fig. 5, aa.

Fig. 5, bb.

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My. For different kk such lines are parallel. For negative and sufficiently small positive values ​​of kk this line does not intersect the set AA and, therefore, there is no admissible ration worth kk kopecks. If we increase the values ​​of kk, starting, for example, with k=0k=0, then the straight line given by the equation

px+qy=k,px + qy = k,

will blend to the right (see Fig. 6). Finally, for some value of k=k0k=k_0 the line px+qy=k0px + qy=k_0 will intersect the set AA for the first time, “stumbling upon” one of its vertices (point MM on Fig. 6) or immediately on the whole side (this can happen if the lines px+qy=kpx + qy=k are parallel to one of the lines l1,l2,l3,l4l_1, l_2, l_3, l_4 or, which is the same, if the relation pq\frac{p}{q} is equal to one of the ratios

a1b1,a2b2,a3b3,a4b4;\frac{a_1}{b_1}, \frac{a_2}{b_2}, \frac{a_3}{b_3}, \frac{a_4}{b_4};

see further, Fig. 8).

A prinya is called an operon to a convex set on a plane if this set lies entirely in one of the half-planes into which this line divides the plane, and at the same time at least one point of the set lies on the line. Thus, the equation px+qy=k0px + qy=k_0 defines the operatic line to the set AA.

Let us now examine separately the two cases mentioned above. Suppose first that the relation pq\frac{p}{q} is not equal to any of the relations

a1b1,a2b2,a3b3,a4b4.\frac{a_1}{b_1}, \frac{a_2}{b_2}, \frac{a_3}{b_3}, \frac{a_4}{b_4}.

Then point M=(x0,y0)M=(x_0, y_0) is the only solution to the problem of the cheapest admissible ration. Indeed, any other point of the set AA lies in the half-plane KK given by the inequality px+qy≥k0px + qy \geq k_0, and therefore corresponds to a more expensive diet. The lines of the infinite polygon AA are the rays of the coordinate axes and the line segments l1,l2,l3,l4l_1, l_2, l_3, l_4. Therefore, on each of these sides, one of the six inequalities of system (2) turns into equality, and at each vertex of the polygon AA two inequalities of system (2) turn into equalities. In the case chosen at figure 6, the point MM lies at the intersection of the lines l1l_1 and l3l_3 (see Fig. 3); hence,

{a1x0+b1y0=c1,a3x0+b3y0=c3,\begin{cases} a_1x_0 + b_1y_0 = c_1, \\ a_3x_0 + b_3y_0 = c_3, \end{cases}

where

x0=b1c3−b3c1a3b1−a1b3;y0=c1a3−a1c3a3b1−a1b3.x_0 = \frac{b_1c_3 - b_3c_1}{a_3b_1 - a_1b_3}; \quad y_0 = \frac{c_1a_3 - a_1c_3}{a_3b_1 - a_1b_3}.

But the remaining four inequalities at this point are satisfied in the strict sense, that is, with the sign “greater than” and not “equal”. This means that a diet consisting of x0x_0 grams of solutions and y0y_0 grams of peas contains the minimum required amount of protein and fat, but an excessive amount of protein and carbohydrates (if point MM lay at the intersection of other lines, then the conclusion would change accordingly).

If food scientists had decided that chickens needed a little more than c2c_2 grams of protein or a little more than c4c_4 grams of carbohydrates per day, then the cheapest diet we found would meet this new requirement (indeed, this means that the straight l2l_2 or l4l_4 would shift slightly to the right, but if such a shift is small enough, then the point MM still remains the vertex of the reduced polygon AA). However, if you need to give the chickens a little more than c3c_3

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6

Fig. 7.

grams of fat per day, then the problem of the cheapest diet must be solved anew, since the diet corresponding to point MM will cease to be acceptable, and the cheapest diet becomes expensive (see Figure 7, where, with the conditional requirement a3x+b3y≥c3+δa_3x+b_3y \geq c_3+\delta, the cheapest diet corresponds to point M′M', lying inside the half-plane KK).

Let us now consider the case where the ratio pq\frac{p}{q} is equal to one of the four ratios, for example a1b1\frac{a_1}{b_1} (see Fig. 8).

In this case, line px+qy=k0px+qy=k_0 coincides with line l1l_1. All points of the set AA, with the exception of the point of the segment M1M2M_1M_2, lie inside the half-plane KK, and therefore the ration corresponding to any point of the segment M1M2M_1M_2 is the cheapest admissible ration. Thus, among the points corresponding to the solution to the problem of the cheapest ration, there are always the vertices of the polygon AA.

A little theory

To find a solution, it is enough to compare the values ​​of the function px+qypx+qy at all vertices. If there is one of these values ​​that is smaller than all the others, then the corresponding vertex is the only solution to the problem; if the values ​​at two vertices are equal and less than the values ​​at the other vertices, then these vertices are necessarily adjacent, and all points on the side connecting these vertices serve as solutions to the problem.

For brevity we will call

Fig. 8.

an acute angle formed by a straight line with the abscissa axis, the angle of inclination of the straight line. If dwir lies along the boundary of a set of permissible points, starting from the abscissa ray towards the ray of the ordinat axis, then each subsequent side lies on a straight line with a greater angle of inclination than the previous one. The tangents of these angles will also increase. The tangent of the angle of inclination α\alpha of the straight line ax+by=cax+by=c (a>0,b>0a>0, b>0) is ab\frac{a}{b}. (If b=0b=0, α=π2\alpha=\frac{\pi}{2} and it is generally accepted that tgα\tg\alpha is equal to infinity.)

Let the reference line pass through the vertex MM of the set of admissible points and the inclination angle of this line is equal to β\beta, and the inclination angles of the straight lines on which the sides adjacent to the vertex MM lie are equal to α1\alpha_1 and α2\alpha_2. Then the angle β\beta is greater than one of these angles and less than the other (see Fig. 9).

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7

Thus, in order to find the vertex through which a reference line of a given direction passes, you need to compare the slope angle of the lines in a given direction with the slope angles of the lines on which the sides of the set of admissible points lie, and select two adjacent sides between whose slope angles the angle β lies. The intersection point of these sides will be the desired vertex. If the angle β coincides with the angle of inclination of one of the sides, then the desired reference line coincides with the line on which this side lies. Instead of comparing slope angles, you can compare their tangents, which is much more convenient, since the tangent of the slope angle is simply expressed through the coefficients of the equation of the straight line.

Numerical examples

  1. Among the solutions to the system of linear inequalities 2x+y≥102x+y \geq 10, x≥0,y≥0x \geq 0, y \geq 0, x+y≥8x+y \geq 8, 3x+7y≥423x+7y \geq 42, x+5y≥20x+5y \geq 20, find those for which the linear function 4x+3y4x+3y reaches a minimum*).

Table 1

| Equation of a line | A point on the coordinate axis through which a straight line passes | Tangent of the angle of inclination of a straight line |
| :— | :— | :— |
| y=0y=0 | (0,4),(20,0)(0,4), (20,0) | 15\frac{1}{5} |
| x+5y=20x+5y=20 | (0,6),(14,0)(0,6), (14,0) | 37\frac{3}{7} |
| 3x+7y=423x+7y=42 | (0,8),(8,0)(0,8), (8,0) | 12\frac{1}{2} |
| x+y=8x+y=8 | (0,10),(5,0)(0,10), (5,0) | ∞\infty |
| 2x+y=102x+y=10 | (0,3c),(c4,0)(0, \frac{3}{c}), (\frac{c}{4}, 0) | 43\frac{4}{3} |

The set of feasible points is depicted on figure 10, from which

*) The numerical data of this example are in no way related to the values ​​​​that are given in the problem of chicken feed.

Fig. 10.

it is clear that the sides of this set are the rays of the coordinate axes and the segments of all four straight lines: x+5y=20x+5y=20, 3x+7y=423x+7y=42, x+y=8x+y=8, 2x+y=102x+y=10.

A supporting straight line with a slope angle 43\frac{4}{3} must pass through a vertex lying at the intersection of a pair of neighboring sides, one of which has a slope angle less than 43\frac{4}{3}, and the other greater than 43\frac{4}{3}. Such a pair is formed by sides lying on straight lines

x+y=8x+y=8 and 2x+y=102x+y=10,

with slope angles of 1 and 2, respectively. Thus, the coordinates of the desired vertex are determined from the system

{x+y=8,2x+y=10,\begin{cases} x+y=8, \\ 2x+y=10, \end{cases}

whence x=2x=2, y=6y=6. The value of the function 4x+3y4x+3y at this point is 4⋅2+3⋅6=264 \cdot 2 + 3 \cdot 6 = 26, and the reference line is determined by the equation 4x+3y=264x+3y=26.

For comparison, let’s calculate the values ​​of the function 4x+3y4x+3y at all other vertices of the set of admissible points (see Table 2 on page 8).

  1. Among the solutions to the system of linear inequalities x≥0,y≥0,3x+y≥15,3x+4y≥36,x+2y≥12,2x+8y≥32x \geq 0, y \geq 0, 3x+y \geq 15, 3x+4y \geq 36, x+2y \geq 12, 2x+8y \geq 32, find those for which the function 3x+12y3x+12y reaches a minimum.

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Table 2

Equation of lines, the vertex lies at the intersection of coordinates
| vertex coordinates | |
| :— | :— |
| xx | yy |
| x=0,2x+y=10x = 0, 2x + y = 10 | 0,100, 10 |
| 2x+y=10,x+y=82x + y = 10, x + y = 8 | 2,62, 6 |
| x+y=8,3x+7y=42x + y = 8, 3x + 7y = 42 | 3,5,4,53, 5, 4, 5 |
| 3x+7y=42,x+5y=203x + 7y = 42, x + 5y = 20 | 8,75,2,258, 75, 2, 25 |
| x+5y=20,y=0x + 5y = 20, y = 0 | 20,020, 0 |

Function values ​​4x+3y4x + 3y at vertex
| xx | yy |
| :— | :— |
| 00 | 1010 |
| 22 | 66 |
| 3,53,5 | 4,54,5 |
| 8,758,75 | 2,252,25 |
| 2020 | 00 |

Table 3

Equation of a line
y=0y = 0
2x+8y=322x + 8y = 32
x+2y=12x + 2y = 12
3x+4y=363x + 4y = 36
3x+y=153x + y = 15
x=0x = 0
3x+12y=c3x + 12y = c

Points on the coordinate axes through which a straight line passes
(0,4),(16,0)(0, 4), (16, 0)
(0,6),(12,0)(0, 6), (12, 0)
(0,9),(12,0)(0, 9), (12, 0)
(0,15),(5,0)(0, 15), (5, 0)
(0,c12),(c3,0)(0, \frac{c}{12}), (\frac{c}{3}, 0)

Tangent of the angle of inclination of a straight line
0140 \frac{1}{4}
12\frac{1}{2}
34\frac{3}{4}
3∞1/43 \frac{\infty}{1/4}

The set of admissible points is depicted in figure 11, from which it is clear that the straight line x+2y=12x + 2y = 12 lies entirely outside this set. Thus, the sides of this set are the rays of the coordinate axes and the segments.

The solutions to the problem are all points on the side lying on this line. The ends of this side are the vertices lying at the points of intersection of the line 2x+8y=322x + 8y = 32 with the neighboring lines y=0y = 0 and 3x+4y=363x + 4y = 36 (recall that we excluded the line x+2y=12x + 2y = 12 from consideration).

So, the coordinates (x1,y1)(x_1, y_1) of the first vertex M1M_1 are determined from the system of equations
{2x1+8y1=32,y1=0,\begin{cases} 2x_1 + 8y_1 = 32, \\ y_1 = 0, \end{cases}

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Fig. 12.

whence x1=16,y1=0x_1=16, y_1=0, and the coordinates (x2,y2)(x_2, y_2) of the second vertex M2M_2 are determined from the system of equations

{2x2+8y2=32,3x2+4y2=36,\begin{cases} 2x_2 + 8y_2 = 32, \\ 3x_2 + 4y_2 = 36, \end{cases}

whence x2=10,y2=1,5x_2=10, y_2=1,5.

The solutions to the problem are all points of the segment M1M2M_1M_2, in other words, points of the form (16λ+10(1−λ),1,5⋅(1−λ))=(10+6λ,1,5−1,5λ)(16\lambda + 10(1-\lambda), 1,5\cdot(1-\lambda)) = (10+6\lambda, 1,5-1,5\lambda), where λ\lambda is any number between 0 and 1. The value of the function 3x+12y3x+12y at all points of the segment M1M2M_1M_2 is 48.

Exercises *)

  1. Solve the bicycle problem.
  2. Solve the “carber problem” with the data given in figure 12.
  3. How will the set of admissible points in the problem of the cheapest ration change if we additionally require that all rationals do not exceed s gram? Could such a limitation influence the decision?
  4. Prove that any convex polygon on a plane can be represented as a polygon of a system of linear inequalities.
  5. Let pq=a1b1\frac{p}{q} = \frac{a_1}{b_1} (see Fig. 3 and 8). How does the solution to the problem of the cheapest diet change in this situation if we replace in system (2)

{a)c1наc1+δ,b)cnнаcn+δ;\begin{cases} a) c_1 на c_1 + \delta, \\ b) c_n на c_n + \delta; \end{cases}

Is δ a positive but very small number?

*) Answers to these exercises will be published in the next issue.

2, Quantum No. 3

QUARTZ HAIRY

There is a stone known in nature that is called “hairy quartz” in Russia. This is a rich quartz crystal produced with shiny gold threads (see figure on the cover).

Pliny called the threads “Hairs of Venus”, and in the east they are called “Hairs of Mohammed” and the stone was considered a binding. Currently, these “Hairs”, or whiskers as they are now called, are grown in laboratory conditions. Studies using an electron microscope showed that the “Hair of Venus” is nothing more than very thin and long crystals of titanium oxide (TiO2−рубин)(\text{TiO}_2 - \text{рубин}), which are tubes of rectangular cross-section with a wall thickness of 1–2 µm (see photograph).

Whiskers have a number of very interesting properties, one of which—high strength—makes it possible to create new, so-called composite materials based on them.

M. A. Golosova

Sheet 12

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This article describes a method that allows you to simplify complex problems in calculating electrical circuits.

What do we mean by “chain conversion”? Let’s assume that we have a complex circuit of resistances that has many pins and connections to sources. Let’s replace this circuit with another one, with the same number of terminals, and so that the resistance between any two terminals of the new circuit is the same as that of the old one. It is clear that the sources “will not know anything” about this replacement, and the points consumed by the circuit will remain the same. But finding these points may be easier.

Therefore, if we want to count currents in a complex circuit, it can be replaced by a simpler equivalent circuit. In this case, the currents inside the replaced part change. Therefore, we can do this only with that part of the scheme that does not directly interest us.

You have already encountered similar substitutions.

Let, for example, in the circuit two resistances r1r_1 and r2r_2 are connected in series, we can replace them with one, equal in value to the sum r1+r2r_1 + r_2. If two resistances are connected in parallel, then they can also be replaced with one, the value of which is R=r1r2r1+r2R = \frac{r_1 r_2}{r_1 + r_2}

These are the simplest examples of circuit conversion. We will focus on more complex schemes.

Let’s see how circuits that have three terminals each are converted into each other - “star” (Fig. 1, a) and “triangle” (Fig. 1, b).

The slightly unusual designations (Fig. 1, b) are very convenient, the index showed between which points the resistance is connected. For example, resistance R13R_{13} is connected between points 1 and 3, etc.

If we want to replace one of these circuits with another, we need to obtain such correspondences between rr and RR that the resistances between any points are the same for both circuits.

In the “star” circuit (Fig. 1, a) the resistor

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Fig. 4.

“triangle” ACD “star” as shown in Fig. 4.

Now it is clear that the resistance between points A and B will be equal to
13+2833=1311 ома.\frac{1}{3} + \frac{28}{33} = \frac{13}{11} \text{ ома}.

We replaced the “triangle” ACD with a “star”, but it was possible to solve the problem differently - replacing the “star” ADB with a “triangle”.

Let now a battery with negligible small internal resistance and e.m. be connected to points A and B. With. E=1 in. We need to find the current through section CB.

The circuit must be transformed so that the resistance CB of interest to us is not affected. The transformation we did earlier (Fig. 4) will do.

Using that RAB=1311 омаR_{AB} = \frac{13}{11} \text{ ома} we get I=ERAB=1113aI = \frac{E}{R_{AB}} = \frac{11}{13} a. After branching, the points are added in the ratio inverse to the resistances of the branches:

I1I2=74.\frac{I_1}{I_2} = \frac{7}{4}.

At the same time I1+I2=II_1 + I_2 = I. (I is the current before the branching, I1I_1 is the current in the upper branch, I2I_2 is the current in the lower branch).

From here

I1=713aI_1 = \frac{7}{13} a

It would be a little more difficult to find the current flowing through the CD section. To do this we would still have to find a current,

Sheet 15

p. 13Transcribed from the scan · Rough draft translation, low quality

13

Fig. 6.

potentiometer. Moreover, the sum of resistance 5r+R15r+R_1 and 7r+R27r+R_2 remains constant. Let’s see what they should be so that the total resistance is maximum. We denote 5r+R15r+R_1 by r1r_1 and 7r+R27r+R_2 by r2r_2. Then the total resistance of the parts of the circuit connected in parallel is r0=r1r2r1+r2r_0 = \frac{r_1 r_2}{r_1 + r_2}. If we take into account that r1+r2=const=cr_1+r_2 = const = c, then the resistance r0r_0 will be expressed as follows: r1(c−r1)c\frac{r_1 (c-r_1)}{c}. This expression is maximum when the number of slipels is maximum. But y=(cr1−r12)y = (cr_1-r_1^2) is the equation of a parabola (Fig. 7), the branches of which intersect the x-axis at points OO and cc. Therefore, the numerical fraction is greatest at r1=c2r_1 = \frac{c}{2}. Since r1+r2=cr_1+r_2 = c, this means that the resistance between points AA and BB is maximum if r1=r2r_1=r_2, that is 5r+R1=7r+R25r+R_1=7r+R_2, or R1−R2=2rR_1-R_2=2r.

It is clear that this is only possible if the resistance of the entire potentiometer R=R1+R2R=R_1+R_2 is not less than 2r2r. Otherwise, the maximum resistance between points AA and BB is achieved when the potentiometer slider is in its extreme position.

So the answer is: R≤2rR \leq 2r.

The method we have described is very convenient for sequentially transforming a complex diagram into a simple form. It allows you to calculate practically any complex target consisting of resistances.

This method can be applied to circuits containing more than just resistances.

Please note that we did not talk anywhere about physical processes in the circuit, but only used the formal expression for Ohm’s law: U=r⋅IU=r \cdot I. It follows from it that when connected in series, their values ​​are added, and when connected in parallel, the values ​​reciprocal to resistance (1r06π=1r1+1r2)\left(\frac{1}{r_{06\pi}} = \frac{1}{r_1} + \frac{1}{r_2}\right) are added. It is clear that if any other physical quantities are related by a law similar to Ohm’s law, then all our conclusions are valid for them.

As an example, consider a circuit with a capacitor (Fig. 8). We know that Q=C⋅UQ=C \cdot U, or U=1CQU = \frac{1}{C} Q.

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p. 14Transcribed from the scan · Rough draft translation, low quality

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Fig. 9.

Let’s compare this with the expression for Ohm’s law U=r⋅IU=r \cdot I.

It can be seen that the laws of positivity, only then together there is a charge, and together with resistance there are quantities, the inverse capacitance. This means that in order to find, say, charges on capacitors, you can do this. Instead of a circuit containing capacitors, draw a target containing resistances, and replace the capacitor with a capacitance of xx farads with a resistance r=1x omr = \frac{1}{x} \text{ om}. After we calculate the current in a circuit of resistances, we can immediately write what the charges are on the capacitors: if a current of I=yI=y amers flows through the resistance, then the corresponding capacitor will have a charge of Q=yQ=y coulombs.

E.m.f. The batteries remain unchanged during this transformation. But, of course, in a circuit with capacitors, the internal resistance of the batteries does not affect the result. Therefore, the goal changes, we will have to deprive the batteries of their internal resistances.

Let, for example, you need to find the charge on a capacitor with capacity 10 мкф10 \text{ мкф} (Fig. 9). To the capacitor

Sheet 17

p. 15Transcribed from the scan · Rough draft translation, low quality

15

DO YOU LIKE FUCKING?
WITH WHOLE NUMBERS?

M. I. Bashmakov

Several schoolchildren were asked to answer the following question:
Find out whether the equality 3100+7100=81003^{100} + 7^{100} = 8^{100} is true or false.
After a few minutes they all replied that this equation was false.
Here are the most typical obligations.

  1. Let’s look at the last digit of the numbers on the right and left. 3 squared is 9, 3 cubed ends in 7, in the fourth power ends in 1, in the fifth power ends in 3, in the sixth power ends in 9, etc. After four powers, the last digit is repeated, so the number 31003^{100} has the same last digit as 343^4, that is, 1. In the same way, it is easy to assume that the last digit of 71007^{100} is also 1, and 81008^{100} is 6. So, the last digit of the number is 2, and the last digit on the right is 6. Therefore, the numbers on the left and right are different.

  2. 3+73 + 7 is greater than 8. But 32+72=583^2 + 7^2 = 58 is less than 82=648^2 = 64. Next, 3100+7100=(32)50+(72)50<(32+72)50=5850<6450=81003^{100} + 7^{100} = (3^2)^{50} + (7^2)^{50} < (3^2 + 7^2)^{50} = 58^{50} < 64^{50} = 8^{100}. We found that the number on the left is less than on the right.

  3. The number on the left is divisible by 2, but not divisible by 4. Indeed, any odd number squared gives a remainder of one when divided by 4: (2n+1)2=4n2+4n+1(2n + 1)^2 = 4n^2 + 4n + 1. The sum of two such numbers (350)2+(750)2(3^{50})^2 + (7^{50})^2 gives a remainder of 2. On the right is a number divisible by 4.

Is the evidence given similar to each other? It is easy to notice the similarity of the first and third: in both, the remainders from division by some integer are compared, in one - by 10 (the last digit), and in the other - by 4. But finding an analogy between this proof and the second is not at all so easy. We will try to calculate it at the end of this article. For now, let’s learn how to apply the first method of reasoning to some other problems.

Computations “modulo”

Problem a 1. Prove that the equation x3=2+3y2x^3 = 2 + 3 y^2 has no solutions in integers.

Let us consider this equation “modulo 9”, that is, up to terms that are multiples of division *). Since each integer xx has the form 3n3n, 3n−13n - 1 or 3n+13n + 1, where nn is an integer, a(3n±1)3=27n3±27n2+9n±1=9k±1a(3n \pm 1)^3 = 27n^3 \pm 27n^2 + 9n \pm 1 = 9k \pm 1, where kk is an integer, then any number cubed is either divisible by 9, or leaves a remainder of 1 or 8 when divided by 9.

*) In general, two integers aa and bb are said to be comparable modulo kk if the difference a−ba - b is divisible by kk. For those who are not familiar with this concept, we advise you to look at the article by A. A. Egorov “Arithmetic of remainders” in «Kvant» No. 5, 1970.

Likewise, since 3(3n±1)2=27n2±18n+33(3n \pm 1)^2 = 27n^2 \pm 18n + 3,

3y23y^2 gives a remainder of 0 or 3 when divided by 9. So, the right side of our equation modulo 9 can only equal 2 or 5, and the left side can only equal 0, 1 or 8, so they cannot coincide for any purpose. The modulo calculations themselves are easy to do. Let us formulate the basic rule of these calculations: if, when adding (or multiplying), we replace numbers comparable to them in terms of

Sheet 18

p. 16Transcribed from the scan · Rough draft translation, low quality

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modulo kk, then we obtain a number comparable to the sum (or product) modulo kk. In other words, in an equality in which the operations of addition and multiplication function, we can replace numbers with modulo kk comparable to them whenever in the answer we are interested only in the remainder of division by kk.

The fact that aa and bb are comparable modulo kk is written as follows: a≡b(modk)a \equiv b \pmod{k}. The rules for operations on comparisons can be written as follows:

если {a≡b(modk),c≡d(modk),\text{если } \begin{cases} a \equiv b \pmod{k}, \\ c \equiv d \pmod{k}, \end{cases}

то {a+c≡b+d(modk),ac≡bd(modk).\text{то } \begin{cases} a + c \equiv b + d \pmod{k}, \\ ac \equiv bd \pmod{k}. \end{cases}

Recall that by definition, a≡b(modk)a \equiv b \pmod{k} means that a−b=k⋅q∗a - b = k \cdot q^*.

Will engage in such a rather artificial task.

Task 2. Prove that the equality 115360+21160=27027⋅100x+21153^{60} + 211^{60} = 27027 \cdot 100^x + 2 is impossible for any integer xx.

It is clear that if for some modulus we do not obtain equality, then it cannot exist in the general sense. Modulo 2 there is no contradiction - there are even numbers on the right (zeros modulo 2). Will work on module 3. 1153≡1(mod3)=115360≡1(mod3)1153 \equiv 1 \pmod{3} = 1153^{60} \equiv 1 \pmod{3}; 211≡1(mod3)=21160≡1(mod3)211 \equiv 1 \pmod{3} = 211^{60} \equiv 1 \pmod{3}. On the right is 27027≡0(mod3)27027 \equiv 0 \pmod{3}. Therefore, the entire right-hand side gives a remainder of 2. Again, we do not obtain a contradiction. If you have enough patience, make sure that modulo all numbers up to 16 inclusive, the written equality is true. (You’ll notice that 27027⋅100x,x≥227027 \cdot 100^x, x \geq 2 is divided by each of these numbers, leaving a remainder of 2.)

*) Be careful with division comparisons. If ac≡bc(modk)ac \equiv bc \pmod{k}, then it is not necessarily true that a≡b(modk)a \equiv b \pmod{k}. For example, 27≡3(mod6)27 \equiv 3 \pmod{6} but 9≠1(mod6)9 \neq 1 \pmod{6}. However, if cc is coprime with the modulus kk, then it is possible to cancel by cc. This is a consequence of such a gentle and not simply provable fact: if cc is coprime with kk, then there is a number xx such that cx≡1(modk)cx \equiv 1 \pmod{k}.

If you are consistent, then modulo 17 you will get the following equalities: (−3)(−2)x+2≡0(mod17)(-3)(-2)^x + 2 \equiv 0 \pmod{17}. By going through the values ​​of xx in a row (the cycle here will be of length 8), you will never get the desired equality. A contradiction will be found.

The calculations done will immediately raise many questions:

(1) If the equality is false, can this be detected by any modulus?

(2) Is it possible to somehow indicate those modules for which contradictions are more likely to be obtained?

(3) Is the behavior of equality across different modules related?

If we are talking about some specific numerical equality (as was the case in our very first example), then, of course, there is always a number comparable in modulus to which we find a contradiction (for example, we can take a number greater than the common parts of the equality). Equalities in which there are variables are much more interesting (this was the case in the last two examples). For equations in integers, each of the three questions posed is interesting and not always fully explored.

A little unproven

The first equations in integers that pose serious difficulties in solving are quadratic equations*. Mathematicians have long been interested in questions of this kind: can a given number be represented as the sum of two squares? It turned out that the solvability of equations of the form x2+y2=ax^2 + y^2 = a and other more general ones, given by polynomials of the second degree, is evidence for checking the solvability of comparison (positive

*) The theory of linear integer equations is quite simple. At the same time, it contains a number of interesting tasks that are close to elementary, and deserves a separate stat.

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researching questions concerning objective numbers: pose these questions “modulo pp”, and then draw general conclusions from the behavior of all pp. This method of strangeness was called the “Minkowski-Hasse principle.” There have been and continue to be problems for which it gives the result: a problem has a solution in terms of numbers if and only if it is solvable in any modulus. It was all the more disappointing to find examples where this principle does not work. One of the first examples of this kind (but not the very first chronologically) was an example found by the Norwegian mathematician Selmer. The equation 3x3+4y3+5z3=03x^3+4y^3+5z^3=0 turned out to be solvable in any modulus (and, of course, in real numbers), but unsolvable in terms of numbers (other than zero). This example served as the starting point for much research on Diophantine equations (that is, equations in numerical terms) over the past 15 years. It should only be said that during this time the number of unclear questions and hypotheses has greatly increased, and the true roots of what will actually happen have not become clear.

Distances between rational numbers

The most important modern development in number theory is the new understanding of “modulo calculations”. For simplicity, let’s move on from whole numbers to rational ones. (This transition is often made painlessly - for example, the solutions to the equation xn+yn=znx^n+y^n=z^n in terms of numbers are very closely related to the solutions to the equation xn+yn=1x^n+y^n=1 in rational numbers.) It is clear that if we want to solve an equation in rational numbers, we must find out whether it can be solved in real numbers. This solvability is much easier to check: you can extract various roots, take logarithms, write inequalities, etc.

But let’s remember how we got real numbers from rational numbers? One of the points of view is this: we can consider sequences of rational numbers, the distance between neighboring terms of which decreases without limit. For example, 1; 1.4; 1.41; 1.4142; … Such a sequence (which can be imagined as a sequence of changes with age-related accuracy) determines a real number. How does the deviation of neighboring members of the sequence from each other change? If the sequence is written like this: a1;a2;a3;...a_1; a_2; a_3; ..., then the distance between the terms is written as ∣am−an∣|a_m-a_n|. Thus, the basis for obtaining real numbers from rational numbers is the distance, defined as the absolute value of the difference. Let’s denote the distance between two numbers as follows: d(a,b)=∣b−a∣d(a, b) = |b-a|. Try displaying the following distance properties*:

  1. d(a,b)≥0d(a, b) \geq 0, with d(a,b)=0⇒a=bd(a, b) = 0 \Rightarrow a=b;
  2. d(a,b)=d(b,a)d(a, b) = d(b, a);
  3. d(a,c)≤d(a,b)+d(b,c)d(a, c) \leq d(a, b) + d(b, c) (triangle inequality);
  4. d(a+c,b+c)=d(a,b)d(a+c, b+c) = d(a, b);
  5. d(ab,0)=d(a,0)⋅d(b,0)d(ab, 0) = d(a, 0) \cdot d(b, 0).

It turned out that, in addition to the general absolute value, rational numbers have many other distances that have the 1-5 property. Let us fix an arbitrary prime number pp. Any rational number aa (except zero) can be represented as a=pv⋅ra=p^v \cdot r, where v=v(a)v=v(a) is an integer, and the rational number r=r(a)r=r(a) is such that when written in

*) The first three of these properties are the main ones that satisfy the general distance on the plane and in space; these are aximons that any “metric” must satisfy (see the article by N.B. Vasiliev “Metric spaces” in «Kvant» No. 10, 1970). The fourth and fifth properties of real distance with the operations of addition and multiplication of numbers. A metric that satisfies them is said to be a field metric (for example, d(b,a)=∣b−a∣d(b, a) = |b-a| is the metric of the field of real numbers).

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in the form of an irreducible fraction, pp is not included in either the numerator or the denominator. (Note that v(a)v(a) can be either zero or a negative integer. For example, if p=3p=3, a=73324=3−4⋅734a=\frac{73}{324}=3^{-4}\cdot\frac{73}{4}, then v(a)=−4v(a)=-4.) Now take an arbitrary positive number λ<1\lambda<1. Let’s define the distance dpd_p as follows: dp(a,b)=λv(a−b)d_p(a,b)=\lambda v(a-b), if a≠ba\neq b, and dp(a,a)=0d_p(a,a)=0. It is easy to check (try it yourself) that all distance properties will be satisfied.

Since there is a new distance, we can try to obtain new numbers by constructing sequences of rational numbers a1,a2,…a_1, a_2, \ldots, so that the distances between neighboring ones decrease. This means that λv(an+1−an)\lambda v(a_{n+1}-a_n) as nn increases should become smaller and smaller and tend to zero, and then v(an+1−an)v(a_{n+1}-a_n) should increase.

As a result, we obtain new numbers, which are called pp-adic ∗^*. They are very similar to real ones. Just as easily as for real numbers, questions can be explored when it is possible to take the root, logarithm, and perform other operations on pp-adic numbers. The problem of the solvability of an equation according to the power model of a given prime number will be replaced by the problem of its solvability in pp-adic numbers.

The question arises whether we have found all the distances between rational numbers. It turns out that yes. There is Ostrovsky’s denominator theorem (you can find it in the book on number theory cited above), which shows that all distances are exhausted by a common absolute value and the pp-adic distances introduced by us for each prime pp.

We have, as it were, equalized the behavior of an equation based on the model of a single prime number and its power, on the one hand, and its behavior in ordinary real numbers

∗)^*) It is easy to prove that the choice of λ\lambda does not affect the forgiveness and properties of pp-adic numbers. One can, if one likes, assume everywhere that λ=12\lambda=\frac{1}{2} or λ=1p\lambda=\frac{1}{p}.

numbers - on the other. In both cases, numbers are compared by their distance from each other, but these distances are chosen differently. (Then we see how the second and third solutions to the problem with which our article began are similar.)

Understanding of this fact greatly enriched number theory, again brought into it powerful methods of function theory and geometry, previously developed for general real numbers, but successfully used for pp-adic numbers, making this sum the ancient branch of modern mathematics one of the most flourishing.)

Exercises

  1. Prove that none of the equations a) x2+y2=1971x^2+y^2=1971, b) 19x3−17y3=5019x^3-17y^3=50, b) 3x2−y2=5z3x^2-y^2=5^z, r) x3+y3+7z=3x^3+y^3+7z=3 has integer solutions.

  2. Prove that from the numbers 1, 2, 3, 4, 5, 6, 7 it is impossible to form two different seven-digit numbers, one of which is divisible by the other. (All digits must be used in each digit.)

  3. Prove that a number whose decimal notation consists of thirty ones, some zeros, and some nines is not a perfect square.

  4. Find the 5-adic distance (that is, the distance d5d_5) between the numbers: a) 0 and 25\frac{2}{5}; b) 131451\frac{31}{45} and 62156\frac{2}{15}; b) 6 and 631.

  5. Prove that for 3-adic numbers the equality is true

1+3+9+27+…=−121+3+9+27+\ldots=-\frac{1}{2}

(in other words, a sequence of distances

αn=d3(1+3+…+3n,−12)\alpha_n=d_3\left(1+3+\ldots+3^n,-\frac{1}{2}\right)

tends to zero).

What is the sum of 1+32+34+36+…1+3^2+3^4+3^6+\ldots?

Sheet 23

p. 21Transcribed from the scan · Rough draft translation, low quality

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The board moves on round rollers. At the same time, it maintains a horizontal position and remains at the same height. Why is this happening? Yes, because the circle has the same width no matter how it turns.

Will the dock move the same way if you use non-circular rollers? At the first moment it seems that this is impossible. Let’s not rush, however. It turns out that there are curves that, like a circle, have the same width in all directions. They are called lines of the same width.

One of the simplest curves of this kind is shown in figure 1. It consists of two A1B1,A2B2,A3B3A_1B_1, A_2B_2, A_3B_3 of radius rr and two B1A3,B3A2,B2A1B_1A_3, B_3A_2, B_2A_1 of radius RR, the centers of which are located at the vertices of a regular triangle O1O2O3O_1O_2O_3. It is easy to see that the width of this curve is the same in all directions and is equal to R+rR+r. Consequently, rollers whose profiles are sequential along such curves will work no worse than round ones (Fig. 2).

The curve shown at figure 1 can be obtained as follows. Let’s take the segment A1B3A_1B_3 and rotate it by 60∘60^\circ around the point O1O_1 and move it to position B1A2B_1A_2. Then, rotate the segment B1A2B_1A_2 by 60∘60^\circ around the point O2O_2, we get the segment A3B2A_3B_2 and, finally, rotate the segment A3B2A_3B_2 by 60∘60^\circ around the point O3O_3, again we arrive at the segment A1B3A_1B_3. In the process of these turns, one end of the segment is considered, arcs A1B1A3B3A_1B_1A_3B_3, and the other - arcs B3A2B2A1B_3A_2B_2A_1. Therefore, the curve shown in figure 1 can be considered as a trajectory described by the ends of some

Sheet 24

p. 22Transcribed from the scan · Rough draft translation, low quality

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Fig. 3.

The width of all these curves is constructed and is equal to the length of the rotated segment. You can rotate a segment around one of its ends. This way we get the simplest curve of equal width, different from a circle (Fig. 4). In this case, the segment ABAB rotates first around the point AA, moving to the position AB′AB', then around the point B′B', passing into the segment B′BB'B, and, finally, around the point BB, closing the curve.

Let us now consider the non-actor segment ABAB. Let it roll without sliding along the SS curve. Then in every

Fig. 4.

In a separate moment, such movement can be considered as rotation of a segment relative to the point of contact. The tangent point about which the rotation is currently being made is called the instantaneous center of rotation (for example, point CC on figure 5).

The idea of ​​an instantaneous center of rotation makes it easy to calculate the velocities of various points on the segment ABAB. For example, for the speed of points AA and BB we have

vA=ω⋅CA,v_A = \omega \cdot CA,
vB=ω⋅CB,v_B = \omega \cdot CB,

where ω\omega is the angular velocity of the segment ABAB in its “instantaneous” rotation around the center CC. In this case, the velocities of the points under consideration will be perpendicular to the corresponding radius of rotation, that is, the segments CACA and CBCB. In this way, you can calculate the speed of any point lying on this segment or rigidly connected with this segment. If, for example, a non-actor figure is rigidly connected to the segment ABAB, then the speed of any point PP is equal to the product ω⋅CP\omega \cdot CP.

Let us now return to the constructed width curves. Let the segment ABAB roll along the curve SS. Since the velocities vAv_A and vBv_B are perpendicular to the radii CACA and CBCB, they are parallel to each other. But the speed vAv_A is directional

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p. 23Transcribed from the scan · Rough draft translation, low quality

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Fig. 6.

line is tangent to the trajectory of point AA, and speed vBv_B is tangent to the trajectory of point BB. Therefore, these tangents are parallel to each other, and the distance between them remains equal to ABAB all the time. But this means that the trajectories A1A2A_1A_2 and B1B2B_1B_2 can be considered as parts of some curve of constant cyrin.

However, we need to construct not two sections, but just this curve. If we want to do this using the described operation, we must choose the line SSSS so that, by drawing it, the segment ABAB rotates to 180∘180^\circ, that is, so that the point AA comes to the position BB, and the point BB to the position AA. However, of such lines - PQRPPQRP - is shown on figure 6. Let us trace in more detail how the segment ABAB describes it.

First it rolls along area PQPQ and comes to position A′B′A'B'. Moreover, its ends describe the arcs AA′AA' and BB′BB'. Then it rolls along the section QRQR, and its ends describe the arcs A′A′′A'A'' and B′B′′B'B''. Finally, it marks the part RPRP, and its ends move along the arcs A′′BA''B and B′′AB''A. As a result, point AA comes to position BB, and point BB to position AA, and the curve of the constructed cirina is closed. In this case, arcs PQPQ, QRQR

and RPRP can have any shape and do not have to be the same. The only thing that is required of them is that they be convex and touch each other as shown in figure. As for the segments APAP and PBPB, their length cannot be arbitrary, or then the arc described by the point AA will not “join” the arc described by the point BB. Here you can build as follows. Let us draw a straight line through the point PP, tangent to the arc PQPQ, and place the point AA on it. Let us now force this straight line to line PQRPPQRP. Then the end of the arc, which will cover the point AA, determines the position of the point BB.

Line PQRPPQRP, shown in figure 6, consists of three arcs. But the number of arcs may be greater. For example, on figure 7 the curve of the constructed tsirina is shown, obtained by drawing the line PQRSTPPQRSTP, consisting of the heel of the arcs.

The curves of the constructed cirina have one more property that makes them similar to the circle. They are expressed by the following theorem:

The perimeter of the curve of the constructed cirina is l=πDl=\pi D, where DD is the width of this curve.

Let’s prove this theorem.

Sheet 26

p. 24Transcribed from the scan · Rough draft translation, low quality

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Fig. 8.

Let the horizontal straight line PQPQ be moved using rollers of constant width (Fig. 8). In the distance is one of these skating rinks, for example the left one. Let its width be DD and its perimeter be ll. When the straight line PQPQ moves so much that this roller makes one revolution, it moves relative to the straight line MNMN by a distance ll to the right. But since it rolls not only along the straight line MNMN, but also along the straight line PQPQ, then after one revolution it turns out to be folded relative to the straight line PQPQ by a distance ll to the left. Consequently, the displacement of straight line PQPQ relative to straight line MNMN will be equal to 2l2l.

But since this same mixing is equal to vtvt, where tt is the time during which the roller makes one revolution, then

2l=vt.(1)2l = vt. \tag{1}

(We assume that straight line PQPQ moves at a constant speed.) The instantaneous center of rotation of the roller is at point AA, which means that the speed of movement

v=ω⋅AB=ωD,v = \omega \cdot AB = \omega D,

where ω\omega is the angular speed of the roller. Substituting this expression into equality (1), we obtain

2l=ωDt.(2)2l = \omega Dt. \tag{2}

But ωt\omega t is the angle of rotation of the roller per revolution. Hence,

ωt=2π,\omega t = 2\pi,

and equality (2) takes the form

2l=2πD,2l = 2\pi D,

where

l=πD.l = \pi D.

Thus, the perimeter of a constant width curve is calculated in the same way as the perimeter of a circle. What is the area enclosed by a curve of constant width? Can it be calculated in the same way as the area of ​​a circle? It turns out not. However, the area of ​​a scapula of constant width can be calculated as the area of ​​the scapula between two concentric circles. More precisely this means the following.

Consider a curve of constant width (Fig. 9). Through an arbitrary point CC we draw a normal on it (a straight line perpendicular to the tangent is normally called) and plot a segment CC′CC' of a given length dd along it. By setting aside such segments from each point of a given curve, we obtain a new curve, which is the geometric locus of the ends of the delayed segments. Obviously, it will also have a constant width. If we now denote by SS the area enclosed between these curves, then the equality will be true

S=πD224−πD124,S = \frac{\pi D_2^2}{4} - \frac{\pi D_1^2}{4},

where D1D_1 is the width of the inner curve, and D2D_2 is the width of the outer one.

Try to prove it yourself.

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SEMI-CORRECT

L. M. Lopovok POLYGONS

By definition, a convex polygon is called regular if it is equiangular and equilateral. However, there is an interesting class of figures that do not possess these two properties at the same time. We will call half-right and the following polygons:

a) equiangular, in which the sides are equal through one;
b) equilateral, in which the angles are equal through one.

An example of a semi-right polygon of the first kind is a rectangle, and an example of the second is a rhombus. From the description of half-right polygons it is clear that each of them has an even number of vertices; let’s denote it by 2n2n.

Properties of half-right equiangular polygons

  1. Opposite sides of an equiangular polygon are parallel.

Indeed, when traversing the polygon, we replace that each side is rotated relative to the previous one by an external angle, that is, by 180∘n\frac{180^\circ}{n} (Fig. 1). Therefore, side An+1An+2A_{n+1}A_{n+2} is rotated relative to side A1A2A_1A_2 by the amount of nn external angles, that is, by 180∘180^\circ.

  1. If you connect the vertices of a half-right equiangular polygon through one (all odd or all even vertices), you get a regular polygon (Fig. 1).

The proof is not difficult: the triangles A1A2A3A_1A_2A_3, A3A4A5A_3A_4A_5, A5A6A7A_5A_6A_7, … are equal according to the first criterion, which means A1A3=A3A5=…A_1A_3=A_3A_5=\dots. On the other hand, from the equality of triangles it follows that their corresponding angles are equal. Let us denote the interior angle of an equal 2n2n-gon by α2n\alpha_{2n}. We find the interior angles of our best polygon: they are equal

α2n−(β+γ)=α2n−(180∘−α2n)=\alpha_{2n} - (\beta + \gamma) = \alpha_{2n} - (180^\circ - \alpha_{2n}) =

=2α2n−180∘=2⋅180∘(1−1n)−= 2\alpha_{2n} - 180^\circ = 2 \cdot 180^\circ \left( 1 - \frac{1}{n} \right) -

−180∘=180∘(1−2n),- 180^\circ = 180^\circ \left( 1 - \frac{2}{n} \right),

Fig. 1.

  1. Quantum No. 3

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as it should be for a regular nn-gon.

  1. A circle can be described around a semi-regular equiangular polygon.

Let us describe a circle around the regular nn-gon A1A3A5…A_1A_3A_5\dots (Fig. 2). The interior angle of an equiangular 2n2n-gon is 180∘(1−1n)180^\circ \left(1 - \frac{1}{n}\right). It is easy to calculate that ⇒A1A2A3\Rightarrow A_1A_2A_3 is half the degree value of the arc A3A5A1A_3A_5A_1, which means that point A2A_2 lies on the constructed circle. This also applies to other vertices: A4A_4, A6A_6,…

Property 3 is based on two methods for constructing semiregular equiangular polygons.

a) Construct a regular nn-gon A1A3A5…A2n−1A_1A_3A_5\dots A_{2n-1} and describe a circle around it. Then we find (using a compass) on the circle the points A2A_2, A4A_4, A6A_6,…, A2nA_{2n}, located at the same distance from the corresponding vertices of the nn-gon: A1A2=A3A4=..A_1A_2=A_3A_4=..

b) We construct a triangle A1A2A3A_1A_2A_3 using two sides (of arbitrary length) and a known angle between them, and describe a circle around this triangle. Then, knowing the sizes of all sides, we successively find the remaining vertices using the notches of a compass.

  1. If the number of vertices of a semiregular equiangular polygon is a multiple of 4, then more diagonals intersect at one point and bisect it.

To prove use 2: these diagonals are also the diagonals of a regular polygon with side four, so they intersect at one point—the center of the polygon’s circumscribed circle—and are bisected by that point.

If the number of vertices of a semiregular equiangular polygon is not a multiple of 4, then it is not difficult to construct an example (Fig. 3), when more diagonals intersect at several points.

  1. The center of a circle circumscribed about a semiregular equiangular 4n4n-gon is its symmetrical center.

From property 4 it follows that with central symmetry with respect to the circle, the vertices of the polygon transform into vertices; therefore, the parties also change sides.

  1. The straight line passing through the midpoints of two parallel sides of a semiregular equiangular polygon is its symmetrical axis.

According to the property of parallel chords of a circle, this straight line passes through the center of the circumscribed circle. From the equality of the corresponding chords on both sides of the line, the symmetry of the corresponding vertices follows

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A polygon with respect to a drawn line (see further Fig. 6).

  1. Let a semiregular equiangular polygon have 2n vertices, then the center of the circle circumscribed around it is its symmetric center of order n.

This means that when rotated around the center of the circle by an angle that is a multiple of 360∘n\frac{360^\circ}{n}, the polygon aligns with itself. This follows from properties 2 and 3.

  1. The sum of the distances from the interior point to the sides (or their extensions) of a semi-regular equiangular polygon is constructed.

As is known, a semiregular polygon has this property.

If you connect the interior point of the equigon with the vertices, then the sum of the areas of the resulting triangles is equal to the area of ​​the polygon. Denoting the side of the polygon by aa, and the distance to the side by x0,x1,x2,x3,…x_0, x_1, x_2, x_3, \dots, we obtain

S=ax02+ax12+ax22+ax32+… ;S = \frac{ax_0}{2} + \frac{ax_1}{2} + \frac{ax_2}{2} + \frac{ax_3}{2} + \dots;

x0+x1+x2+x3+⋯=2Sa=const.x_0 + x_1 + x_2 + x_3 + \dots = \frac{2S}{a} = \text{const.}

Let the side A1A2A_1A_2 be larger than the side A2A3A_2A_3 in a given polygon. Let us construct a regular 2n-gon (Fig. 4) on A1A2A_1A_2. Then all the sides of the original polygon (except three) are respectively parallel to the sides of the regular polygon, and three (A1A2A_1A_2 and funny with it) lie on the sides of the regular polygon. Therefore, the distances from the internal point MM to the side of the correct polygon are as follows:

x0=y0, x1=y1, x2=y2, x3=y3+b1,x_0 = y_0, \ x_1 = y_1, \ x_2 = y_2, \ x_3 = y_3 + b_1,

x4=y4+b2, x5=y5+b3,…,x_4 = y_4 + b_2, \ x_5 = y_5 + b_3, \dots,

where b1,b2,b3b_1, b_2, b_3 are constant, and the required sum

y0+y1+y2+y3+y4+⋯=(x0+x1+x2+x3+x4+… )−(b1+b2+… )=const.y_0 + y_1 + y_2 + y_3 + y_4 + \dots = (x_0 + x_1 + x_2 + x_3 + x_4 + \dots) - (b_1 + b_2 + \dots) = \text{const.}

  1. If you connect the sides of an equiangular equilateral polygon in series, you get a semi-regular equilateral polygon.

Indeed, by Property 2, all small diagonals of a semiregular equiangular polygon are equal to each other. The sides of the equigon (Fig. 5) are half the size of these diagonals, since it is the average of the linear triangles A1A2A3,A2A3A4,A3A4A5,…A_1A_2A_3, A_2A_3A_4, A_3A_4A_5, \dots. Using property 7, it is easy to install

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TASKS

M71. A rectangular table of mm rows and nn columns is filled with numbers. Let’s rearrange the numbers in each line in ascending order. Prove that if you then rearrange the numbers in each column in ascending order, then in each row they will still appear in ascending order.

Think about what will happen if you act in a different order: in the original table, first rearrange the numbers in ascending order in the columns, and then in the rows: will the result be the same table as in the first case, or a different one?

M72. Solve the equation

1−x3+1+x3=p,\sqrt[3]{1-x} + \sqrt[3]{1+x} = p,

where pp is an arbitrary real number.

Yu. I. Ionin

M73. On a game ticket you need to mark 8 cells out of 64. What is the probability that after a drawing in which 8 of some cells out of 64 are also chosen (and we consider all such possibilities to be equally probable), it turns out that exactly 4 cells were guessed? 5 cells?…all 8 cells?

M74. The polynomial pp has the following property: for some number aa

p(x)=p(a−x).p(x) = p(a-x).

Prove that p(x)p(x) can be represented as a polynomial in (x−a2)2\left(x - \frac{a}{2}\right)^2. For example, if p(x)=x5+(1−x)5p(x) = x^5 + (1-x)^5, then obviously p(x)=p(1−x)p(x) = p(1-x) and, as is not difficult to check,

p(x)=5y2+52y+116,p(x) = 5y^2 + \frac{5}{2}y + \frac{1}{16},

where y=(x−12)2y = \left(x - \frac{1}{2}\right)^2.

M75. a) Prove that in any convex polyhedron the sum of the lengths of all edges is greater than triple the diameter. (The diameter of a polyhedron is the longest of the lengths of all possible segments with ends at the vertices of the polyhedron.)

  1. Prove that for any two vertices AA and BB the convex polyhedron will find three broken lines, each of which goes along the edges of the polyhedron from AA to BB and no two go along the same edge.

b) Prove that if two edges are cut in a convex polyhedron, then for any two of its vertices AA and BB there is a broken line going from AA to BB along the remaining edges.

d) Prove that in problem 6) it is possible to choose three broken lines that pairwise do not have common vertices, with the exception of the ends AA and BB.

A. G. Kushinirenko

F83. A board of mass mm and length ll lies on a horizontal floor. The friction coefficient of the board on the floor is kk. How much work must be done in order to rotate the board in a horizontal plane through a small angle α\alpha around one of its ends?

F84. A “black box” (a box with an unknown circuit inside) has two pairs of terminals. If voltage UU is applied to terminals I, then

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Fig. 1.

a voltmeter with very high internal resistance connected to terminals II will show a voltage of U2\frac{U}{2}. If you apply voltage UU to terminals II, then the voltmeter connected to terminals I will show UU. What electrical circuit is in the “box”?

S. G. Semenchinsky

F85. Is it possible to test a closed process (cycle) with an ideal gas so that points AA and BB (Fig. 1) lie on the same isotherm?

The temperatures T1T_1 and T2T_2, which correspond to the isotherms drawn at Fig. 1, ​​the volume V1V_1 (or V3V_3) are given.

B. B. Bukhovtsev

F86. In Millikan’s experiment, the position of a droplet weighing 10−510^{-5} e is determined by a microscope with an accuracy of 10 μm. What is the uncertainty in determining its speed?

F87. The source of spherical waves moves along the surface of the water with a speed of uu. Draw pictures of a wave on the surface of the water when the wave speed is higher and lower than the speed of the source.

L. G. Aslamaov

FROM THE HISTORY OF PHYSICS

The first electromagnets appeared shortly after Christan Oersted discovered the magnetic effect of electric current in 1820. Already in the autumn of the same 1820, Ampere came up with an iron-free electromagnet - solenoid (the name of this was also introduced by Ampere). Three years later, a small English physics teacher, Sturgeon, invented, manufactured and shows in his lectures the first real electromagnet in the form of a varnished iron rod (see Fig.) with a wire wound on it.
dragging The varnish served as electrical insulation. As the achievement progressed, it was possible to hold several tens of grams of iron with this electromagnet. Sturgeon also made the first horseshoe-shaped electromagnet, which could hold a load of more than 4 kg.
(Ends on page 44.)

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SOLUTIONS

M26

Let’s assume that in each issue of our magazine there will be five mathematics problems in the “Kvata” task. Let us denote by f(x,y)f(x, y) the number of the first of the tasks of the xx-th issue of the journal for the yy year (for example, f(6,1970)=26f(6, 1970) = 26). Write the general formula for f(x,y)f(x, y) for all x,yx, y (1≤x≤12,y≥19701 \leq x \leq 12, y \geq 1970). Solve equation f(x,y)=yf(x, y) = y.

The function ff satisfies the following conditions:

  1. f(1,1970)=1f(1, 1970) = 1;
  2. f(x+1,y)=f(x,y)+5f(x + 1, y) = f(x, y) + 5 (1≤x<121 \leq x < 12) - for each month f(x,y)f(x, y) increases by 5;
  3. f(1,y+1)=f(1,y)+60f(1, y + 1) = f(1, y) + 60 - for each year f(x,y)f(x, y) increases by 60.

It is clear that the function is uniquely determined by these conditions; it can be specified, for example, with the following formula:

f(x,y)=5x+60(y−1970)−4.f(x, y) = 5x + 60(y - 1970) - 4.

It is easy to verify that f(5,2003)=2001f(5, 2003) = 2001; f(6,2003)=2006f(6, 2003) = 2006. Therefore, equation f(x,y)=yf(x, y) = y has no solutions.

The correct solutions were sent by E. Orlok from Zhitomir, N. Ilyin from the village of Zakhar, Irkutsk region, M. Perelmuter from Kyiv and other readers.

From the above, it is clear that if we also introduced the following function: f(k,x,y)f(k, x, y) is the number of the kkth problem of the xxth issue of the journal for the yyth year (1≤k≤5,1≤x≤12,y≥19701 \leq k \leq 5, 1 \leq x \leq 12, y \geq 1970), then the equation f(k,x,y)=yf(k, x, y) = y would be the only solution k=3,x=5,y=2003k = 3, x = 5, y = 2003 - in other words, if our system remains unchanged until then (still in each issue there will be five problems in mathematics), then the third problem in the “Kvata” task No. 5 for 2003 will have the number M2003. The general formula for f(k,x,y)f(k, x, y) is also:

f(k,x,y)=k+5x+60(y−1970)−5.f(k, x, y) = k + 5x + 60(y - 1970) - 5.

For readers, please, more useful are the formulas given by the inverse function, which by the given number nn allows you to find the year yy and the journal number xx in which this problem was proposed.

To do this, it is convenient to use the following notations: [a][a] is the integer part of the number aa (the largest integer not exceeding aa) and {a}=a−[a]\{a\} = a - [a] is the fractional part of the number aa.

Check that

x=[12{n−160}]+1,y=[n−160]+1970.x = \left[ 12 \left\{ \frac{n - 1}{60} \right\} \right] + 1, y = \left[ \frac{n - 1}{60} \right] + 1970.

M27

Prove that if ab−c+bc−a+ca−b=0\frac{a}{b - c} + \frac{b}{c - a} + \frac{c}{a - b} = 0 then a(b−c)2+b(c−a)2+c(a−b)2=0\frac{a}{(b - c)^2} + \frac{b}{(c - a)^2} + \frac{c}{(a - b)^2} = 0.

This statement follows from this lie:

(ab−c+bc−a+ca−b)(1b−c+1c−a+1a−b)=a(b−c)2+b(c−a)2+c(a−b)2.\left( \frac{a}{b - c} + \frac{b}{c - a} + \frac{c}{a - b} \right)\left( \frac{1}{b - c} + \frac{1}{c - a} + \frac{1}{a - b} \right) = \frac{a}{(b - c)^2} + \frac{b}{(c - a)^2} + \frac{c}{(a - b)^2}.

To prove it, it is enough to multiply the two sums on the left side of the lie, term by term, and take into account that the sum of three fractions

ab−c(1c−a+1a−b)=ca−ab(a−b)(b−c)(c−a),\frac{a}{b - c}\left( \frac{1}{c - a} + \frac{1}{a - b} \right) = \frac{ca - ab}{(a - b)(b - c)(c - a)},

bc−a(1b−c+1a−b)=ab−bc(a−b)(b−c)(c−a),\frac{b}{c - a}\left( \frac{1}{b - c} + \frac{1}{a - b} \right) = \frac{ab - bc}{(a - b)(b - c)(c - a)},

ca−b(1b−c+1c−a)=bc−ca(a−b)(b−c)(c−a)\frac{c}{a - b}\left( \frac{1}{b - c} + \frac{1}{c - a} \right) = \frac{bc - ca}{(a - b)(b - c)(c - a)}

equal to zero.

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This decision was sent by A. Shilitum from Tashkent. Less clear, but also correct solutions were sent by B. Paiss from Novomoskovsk, Tula region, and A. Izbitsky from Malorita, Brest region.

After reading such an artificial solution, of course, a reasonable question may arise: what is the agreement that the given expression must be multiplied by 1b−c+1c−a+1a−b\frac{1}{b-c} + \frac{1}{c-a} + \frac{1}{a-b}? Is it possible to come up with a general method of calculation that allows solving such problems?

It would be more natural to solve this problem this way. Let’s write these expressions as a ratio of two polynomials:

ab−c+bc−a+ca−b=p(a,b,c)(a−b)(b−c)(c−a),\frac{a}{b-c} + \frac{b}{c-a} + \frac{c}{a-b} = \frac{p(a,b,c)}{(a-b)(b-c)(c-a)},

a(b−c)2+b(c−a)2+c(a−b)2=q(a,b,c)(a−b)2(b−c)2(c−a)2\frac{a}{(b-c)^2} + \frac{b}{(c-a)^2} + \frac{c}{(a-b)^2} = \frac{q(a,b,c)}{(a-b)^2(b-c)^2(c-a)^2}

(pp will be a third-degree polynomial, and qq will be a fifth-degree polynomial). We must prove that if p(a,b,c)=0p(a,b,c) = 0 then also q(a,b,c)=0q(a,b,c) = 0. It is natural to try to prove that the polynomial qq is divisible by the polynomial pp, that is, to find a polynomial r=r(a,b,c)r=r(a,b,c) such that q=prq=pr (you can prove a general theorem for polynomials in any number of variables: if qq is equal to zero for all those values of the variables for which pp is equal to zero, and at the same time the polynomial pp is continuous, that is, it cannot be factorized—and in this case it is—then qq must be divisible by pp). You can divide polynomials in the usual way - with a “corner”, considering them polynomials in one variable aa (the coefficients of which include the letters bb and cc); for example, pp would be written like this:

p(a,b,c)=−a3+p1(b,c)a2+p2(b,c)a+p3(b,c).p(a,b,c) = -a^3 + p_1(b,c)a^2 + p_2(b,c)a + p_3(b,c).

As a result, we would, of course, get q=prq=pr, where

r(a,b,c)=(a−b)(b−c)(c−a)(1a−b+1b−c+1c−a)=−a2+ab+ac+bc−b2−c2.r(a,b,c) = (a-b)(b-c)(c-a)\left(\frac{1}{a-b} + \frac{1}{b-c} + \frac{1}{c-a}\right) = -a^2 + ab + ac + bc - b^2 - c^2.

In this example, the implementation of this solution plan involves very difficult calculations (in the polynomial q(a,b,c)q(a,b,c) even after reducing similar terms to the remaining 21 terms!), but we strongly advise readers to consider all the details of this solution, which applies to many others.

N. B. Vasiliev

M28

a) Of the 19 balls, 2 are radioactive. For any pile of balls, in one check you can find out whether it contains at least one radioactive ball or not (but you cannot find out how many such balls are in the pile). Prove that in 8 tests it is possible to isolate both radioactive balls.

b) Of the 11 balls, 2 are radioactive. Prove that in less than 7 checks it is impossible to guarantee the release of both radioactive balls.

Let’s start with a similar, but simpler task. Let nn balls be given, one of which is radioactive; How many checks can it take to identify it? It is easy to indicate a method that allows you to select one of the n=2kn=2^k balls in kk checks: first, we divide all the balls into two equal piles of 2k−12^{k-1} balls in each, we check one of them and thereby determine which of them contains the radioactive ball, then we divide this pile of 2k−12^{k-1} balls into halves again, etc. - with each check the number the balls are halved, and after kk checks we will find the radioactive ball. It is clear that if n<2kn<2^k, then kk checks are also sufficient. So, in order to isolate one radioactive ball from nn, it is enough to perform f1(n)f_1(n) tests, where f1(n)f_1(n) is the smallest integer kk for which n≤2kn\leq 2^k (in other words, f1(n)f_1(n) is the smallest integer greater than or equal to log⁡2n\log_2 n). Below we will see that less than the number of checks completed is not enough.

Now let’s move directly to solving our problem. Here it was no longer possible to obtain an exact result immediately for any member of the remaining 21 members!, but we strongly advise readers to consider all the details of this solution, which applies to many others.

N. B. Vasiliev

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Fig. 1. This figure presents a method that allows you to select 2 radioactive balls from 7 in 5 checks. We consider that the balls are numbered 1, 2, …, 7, and in each cell we write a bunch of balls that are subject to verification (sometimes the pile consists of one ball). For example, the first one to check is a pile of three balls {1, 2, 3}.
Each check has two possible outcomes: “there is radioactivity” - then you need to follow the red arrow, and “there is no radioactivity” - then you need to follow the black arrow. If the cell is shaded, then no further checks are needed. For each path descending along the arrows from top to bottom, as a result of all the checks performed along this path, it is possible to determine which pair of balls is radioactive (it is indicated under the lowest arrow). Make sure of it!

but we are interested in how many checks can be used to identify radioactive balls for sure, regardless of any option for their location, even the most unfavorable one for us. In the same way, checking the balls one after another, you can select two balls from 4 in 3 checks, from 5 - in 4, from 6 - in 5, from 7 - in 6, etc. However, for n=7n=7 you can bypass the fifth one with checks. Before reading the solution further, try to prove this, that is, find an appropriate way to lower radioactive balls. However, this method (there are several of them) is indicated in figure 1.

This figure helps us understand what we mean by the words “method of dropping balls”: to specify a method, you need to indicate the pile of balls that is checked first, and also indicate which pile to check after each of the possible outcomes of the next test for radioactivity; in other words, you need to measure a diagram from straight

mogol cells and arrows - the same as on figure 1, only, if necessary, with a different number of kk checks - and write some numbers of balls in each cell.

Now we will try to answer two related questions: how to find a way to find two balls among nn, consisting of kk checks, if such a method exists; if it does not exist, then how to prove it?

In principle, for any specific nn and kk these questions can be solved by “exhaustive search”: try one after another all possible ways to fill the cells of the diagram corresponding to kk checks with subsets of nn balls (after all, there are a finite number of such methods!) and for each of these methods check whether it allows you to isolate radioactive balls or not (that is, whether there will be a different assumption: which pair balls are radioactive - match different paths using the arrows from top to bottom). But the number of such methods, even with small nn and kk, is so great that it is practically impossible to do a “full search” even with the help of a computer (for example, with n=11n=11 and k=7k=7 you can fill the cells of the diagram with piles

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more than 1040010^{400} different ways!). We will now show how this search can be greatly reduced.

Let’s return again to figure 1. From the lowest row of cells, corresponding to the last, fifth check, 25=322^5=32 arrows extend. In general, for kk checks, there will be 2k2^k. If the ponska method, written on the diagram, guarantees the isolation of radioactive balls, then each of these arrows corresponds to only one of the possible answer options: which two balls are radioactive (but, perhaps, different arrows correspond to the same option). Therefore, the number of different possible answer options depends on no more than the number of the arrow, that is, no more than 2k2^k.

Let’s formulate this main message like this:

If the number of possible options is greater than 2k2^k, then there is no way to select one of these options in kk checks.

The same can be said like this:

If there is a way that allows you to select one option from NN possible in kk checks, then N≤2kN \leq 2^k.

(The last inequality can also be written as follows: k≥f1(N)k \geq f_1(N).)

Of course, this rule applies to any problem where you need to select one option from NN based on the results of several checks; the only important thing is that each check has two possible initial ones: “there is radioactivity” and “there is no radioactivity”).

In particular, it follows from this rule that it is impossible to select one and 同一 radioactive ball from nn in less than f1(n)f_1(n) checks: if f1(n)=kf_1(n) = k, then 2k−1<n2^{k-1} < n, and there are nn different options in this problem (the 1st ball is radioactive, the 2nd ball is radioactive, …, the nnth is radioactive ball).

Let’s return again to the problem where there are two radioactive balls. How many different options are there? At figure 1, where we choose 2 balls from 7, the number of options is 21. In general, there are Cn2=n(n−1)2C_n^2 = \frac{n(n-1)}{2} options to choose 2 balls from nn. From our basic rule, printed above on a pink background, it follows that if in kk checks it is possible to select 2 balls from nn, then n(n−1)2≤2k\frac{n(n-1)}{2} \leq 2^k.

Conditions denote the smallest number of checks required to select 2 balls from nn, through f2(n)f_2(n). Then the last inequality can be written as follows:

f2(n)≥f1(n(n−1)2).f_2(n) \geq f_1\left(\frac{n(n-1)}{2}\right).

It is clear from the table that for some nn (for example, for n=6n=6, n=8n=8) a strict inequality is possible here. Indeed, in order for kk checks to be able to find 2 radioactive balls among nn, it is not enough that inequality n(n−1)2≤2k\frac{n(n-1)}{2} \leq 2^k be satisfied. It is also necessary that such options for which the first check should result in “+” (natural radioactivity) should be no more than 2k−12^{k-1} and those for which the result should be “-” (no radioactivity) should also be no more than 2k−12^{k-1} - because otherwise, according to the basic rule, we will not be able to choose one of these options during the k−1k-1 check! In the same way, each of the outcomes “++” (1st check “+”, 2nd check “+”), “+—”, “+—”, “—” should correspond to no more than 2k−22^{k-2} options, etc.

We will return to solving this problem in the next issue of the journal.

A. N. Vilenkin

Sheet 39

p. 37Transcribed from the scan · Rough draft translation, low quality

37

Fig. 3.

where nжсn_{жс} is the refractive index of a light ray when passing from liquid to glass.

With total internal reflection of light at the glass-liquid interface α=90∘\alpha = 90^\circ, and therefore sin⁡β0=nжс\sin \beta_0 = n_{жс}, where β0\beta_0 is the angle of incidence of the beam at which total internal reflection is observed. Similarly, for the total internal reflection of light at the glass-air interface, we can write sin⁡δ0=1nc\sin \delta_0 = \frac{1}{n_c}, where ncn_c is the refractive index of glass. From these two formulas, taking into account that nжс=nжсncn_{жс} = \frac{n_{жс}}{n_c}, we find

nжc=sin⁡β0sin⁡δ0.n_{жc} = \frac{\sin \beta_0}{\sin \delta_0}.

Fig. 4.

Now we need to determine the refractive index of a light beam so that it can only be observed by correcting the total internal reflection at the glass-liquid interface. This we will define the angle β0\beta_0. Then we define the angle δ0\delta_0 in exactly the same way. After this, calculating the refractive index of a light beam is not difficult. The fact that the beam does not undergo refraction at the spherical boundary of glass and air will help to carry out the experiments, since it falls perpendicular to the surface of the glass. This makes it easy to determine the direction of the beam incident on the flat boundary of the plate.

F37

In two vertical cylinders with cross-sectional areas S1S_1 and S2S_2 there are two irreversible pistons connected by a thin irreversible thread of length ll (Fig. 4). The space between the pistons is filled with water. Find the tension in the thread if the ends of the vessels are open to the atmosphere. Density of water ρρ.

If the fluid pressure on a large piston (with an area S1S_1) is pp, and the atmospheric pressure is p0p_0, then the pressure force F1=S1pF_1 = S_1p acts upward on the piston, and the tension force TT of the thread and the atmospheric pressure force F1′=p0⋅S1F'_1 = p_0 \cdot S_1 acts downward on the piston. Since the piston is in equilibrium, then

S1p=S1p0+T.S_1p = S_1p_0 + T.

A similar equation can be drawn up for the lower piston: the thread tension force TT and the atmospheric pressure force F2′=p0S2F'_2 = p_0S_2 act upward on it, and the water pressure force F1=p′S2F_1 = p'S_2 acts downwards on it. Moreover, the pressure p′p' of water on the lower piston is ρgl\rho gl greater than on the upper one. Since the piston is in equilibrium, then

T+p0S2=(p+ρgl)S2.T + p_0S_2 = (p + \rho gl)S_2.

Solving both equations together, we find

T=ρglS1S2S1−S2.T = \rho gl \frac{S_1S_2}{S_1 - S_2}.

Sheet 40

p. 38Transcribed from the scan · Rough draft translation, low quality

38

We usually check the answer by using it at the extreme values ​​of the parameters. We will assume that S2→S1S_2 \rightarrow S_1. In this case T→∞T \rightarrow \infty. This is understandable. The entire system maintains balance thanks to the water pressure on the stake with an area of ​​S1−S2S_1 - S_2 on the upper piston. If S1→S2S_1 \rightarrow S_2, then the pressure on this stake should tend to infinity. In this case, the tension force of the thread should also tend to infinity.

For S1=S2S_1 = S_2 we get that TT is infinite. However, this is no longer true. Such a limiting transition is impossible. When solving the problem, we assumed that the system is in equilibrium. However, at S1=S2S_1 = S_2 equilibrium is impossible and the system of pistons will fall equal to the acceleration of free fall gg. The thread tension in this case should be zero. This example shows how carefully one must approach passages to the limit in physics. It is necessary to ensure that this phenomenon does not become completely different.

This solution was sent by N. Fedin from Omsk, tenth-class student M. Fedorov from Moscow, A. Ratzozin from Izhevsk.

An interesting solution was proposed by A. Zhukov from Kirovsk, Donetsk region. He used the method of virtual change. Although such a discussion about this method requires a special long article, the solution will be clear anyway.

Let the thread decrease by Δl\Delta l, and the upper piston moves to Δl1\Delta l_1, and the lower one to Δl2\Delta l_2. Since the volume of water between the pistons has not changed, both pistons should move in the same direction (lower), and in such a way that

Δl1S1=Δl2S2 и Δl2−Δl1=Δl\Delta l_1 S_1 = \Delta l_2 S_2 \text{ и } \Delta l_2 - \Delta l_1 = \Delta l
(Δl2>Δl1\Delta l_2 > \Delta l_1).

Solving these equations together, we find

Δl1=ΔlS2S1−S2 и Δl2=ΔlS1S1−S2.\Delta l_1 = \Delta l \frac{S_2}{S_1 - S_2} \text{ и } \Delta l_2 = \Delta l \frac{S_1}{S_1 - S_2}.

The change in the potential energy of the system when moving the volume of water ρS1Δl1\rho S_1 \Delta l_1 (or ρS2Δl2\rho S_2 \Delta l_2) by ll must be equal to the work done by the tension force of the thread. Therefore we can write,

p+Δp=p+ρgh,p + \Delta p = p + \rho gh,

Sheet 41

p. 39Transcribed from the scan · Rough draft translation, low quality

39

where hh is the difference in fluid levels in the elbows (Fig. 5). From this equation we find that h=Δpρgh = \frac{\Delta p}{\rho g}. We see that hh does not depend on the areas of the pressure gauge elbows. This means that the accuracy of measurements when connecting a vessel to both a wide and a narrow elbow is the same.

The correct solution was sent by A. Zhukov and the memoirs of S. Pastmukhov from Sverdlovsk.

F39

A planet of radius rr and mass MM is surrounded by an equally dense atmosphere consisting of gas with molecular weight μ\mu. What is the temperature of the atmosphere on the surface of the planet if the height of the atmosphere is hh?

Let us write the equation of the gas state for the volume of gas VV with mass mm (Mendeleev-Clapeyron equation):

PV=mμRT;PV = \frac{m}{\mu} RT;

PP is pressure, VV is gas volume, RR is gas constant and TT is temperature. Since mV=ρ\frac{m}{V} = \rho, where ρ\rho is the gas density, we can rewrite this equation in the form P=ρμRTP = \frac{\rho}{\mu} RT.

Hence T=PμρRT = \frac{P\mu}{\rho R}.

It is clear that in order to find the temperature on the surface of a planet, we need to find the pressure on its surface. If ρ=const\rho = \text{const}, then P=ρghP = \rho gh, where gg is the acceleration of free pressure on a given planet. Let’s find him.

For a body of mass mm located on the surface of the planet, the force of attraction is equal to mgmg. On the other hand, according to the law of universal gravitation, it is equal to γmMr2\gamma \frac{mM}{r^2}. Therefore we can write that mg=γmMr2mg = \gamma \frac{mM}{r^2}.

Hence g=γMr2g = \gamma \frac{M}{r^2} and P=ργMr2hP = \rho \gamma \frac{M}{r^2} h.

Substituting this expression for PP into the equation for temperature, we obtain

T=γMμhr2R.T = \frac{\gamma M\mu h}{r^2 R}.

The correct solution to the problem was sent by V. Malkov from Orsha and A. Proskuryakov from Moscow.

F40

At what potential difference between the electrodes does a neon lamp light up if the energy of neon is I=21,5I = 21,5 eV, and the average distance between two successive collisions of the electrode with gas atoms is l=0,4l = 0,4 mm? The electrodes are in the form of large flat plates located at a distance of d=3d = 3 mm from each other.

If the potential difference between the electrodes is UU, then the direction of the electric field between them is E=UdE = \frac{U}{d}. In this field, the electron is acted upon by a force F=E⋅eF = E \cdot e (e is the charge of the electron), imparting to it an acceleration a=Fm=Eem=Uedma = \frac{F}{m} = \frac{Ee}{m} = \frac{Ue}{dm}, where mm is the mass of the electrode.

When an electron collides with an atom of a gas, it transfers its energy to it and is abandoned (we assume that the collision is inelastic). The mass of the atom is greater than the mass of the electrode. Therefore, during a collision, an atom of a gas is transferred energy mv22\frac{mv^2}{2}, acquired by an electron between its successive stolnovs. This energy must be equal to the gas nomization energy II:

mv22=I.\frac{mv^2}{2} = I.

Let us now find the speed acquired by the electron. If the flare time is tt, then we can write that v=aτ=Uemdtv = a\tau = \frac{Ue}{md} t and l=aτ22=Ueτ22mdl = \frac{a\tau^2}{2} = \frac{Ue\tau^2}{2md}. From these equations we find that

v=2Uelmd.v = \sqrt{\frac{2Uel}{md}}.

Substituting this expression for vv equation (*), we obtain

Ueld=I.\frac{Uel}{d} = I.

Hence U=Idel≈160θU = \frac{Id}{el} \approx 160\theta.

Sheet 42

p. 40Transcribed from the scan · Rough draft translation, low quality

40

Exponential equations are usually called equations in which the unknown quantity is contained in the exponent (but the bases do not contain it).

Solving exponential equations is based on the following power property:

if two powers with the same positive base different from one are equal, then their exponents are equal.

According to this property, the simplest exponential equation

ax=b(a>0,a≠1,b>0)a^x = b \quad (a > 0, a \neq 1, b > 0)

is solved as follows:

ax=alog⁡ab,x=log⁡ab.a^x = a^{\log_a b}, \quad x = \log_a b.

The difficulty in solving exponential equations is often that you need to be able to see the common basis of the left and right sides of the equation. If in Eq.

(49)x⋅(278)x−1=23\left(\frac{4}{9}\right)^x \cdot \left(\frac{27}{8}\right)^{x-1} = \frac{2}{3}

the common base 23\frac{2}{3} (or 32\frac{3}{2}) of the left and right sides immediately catches the eye, then in the equations

(0,4)x−1=(6,25)6x−5(0,4)^{x-1} = (6,25)^{6x-5}

To find the common base 25\frac{2}{5} (or 52\frac{5}{2}), you must first convert the decimal fractions to ordinary ones. (Complete the solutions to the given examples; in equation (1) you will receive the answer x=2x=2, and in equation (2) x=1113x = \frac{11}{13}.)

To reduce many exponential equations to the simplest, the following formula is often useful:

ap⋅bp=(ab)p.a^p \cdot b^p = (ab)^p.

Example 1: Solve the equation

3x⋅5x=225.\sqrt{3^x} \cdot \sqrt{5^x} = 225.

Solution e. We write the equation in the form

3x⋅5x=225.3^x \cdot 5^x = 225.

Using formula (3), we get

15x=152,15^x = 15^2,

where do we find x=4x=4.

Example 2: Solve the equation

23x⋅5x=1600.2^3x \cdot 5^x = 1600.

Solution e. We have the following integer equivalent equations:

(23)x⋅5x=1600,8x⋅5x=1600,40x=402,x=2.(2^3)x \cdot 5^x = 1600, \quad 8^x \cdot 5^x = 1600, \quad 40^x = 40^2, \quad x=2.

It is easy to reduce to the simplest equation the form

aφ(x)=1(a>0,a≠1).a^{\varphi(x)} = 1 \quad (a > 0, a \neq 1).

To do this, it is enough to represent one as aa to the zeroth power: 1=a01 = a^0.

Example 3: Solve the equation

5x2+x−2=1.5^{x^2+x-2} = 1.

Solution e. We successively find

5x2+x−2=50,x2+x−2=0,x1=−2,x2=1.5^{x^2+x-2} = 5^0, \quad x^2+x-2=0, \quad x_1=-2, \quad x_2=1.

Sheet 44

p. 42Transcribed from the scan · Rough draft translation, low quality

42

Example 9. Solve the equation
3⋅16x+36x=2⋅81x.3 \cdot 16^x + 36^x = 2 \cdot 81^x.
Solved and e. We see that in this equation the bases 16, 36, 81 form a geometric progression and are raised to the same power xx. To solve, divide both sides of the equation by 81x81^x. We get
3⋅(49)2x+(49)x=2.3 \cdot \left(\frac{4}{9}\right)^{2x} + \left(\frac{4}{9}\right)^x = 2.
Denoting (49)x\left(\frac{4}{9}\right)^x by yy, we arrive at the quadratic equation 3y2+y−2=03y^2 + y - 2 = 0 with roots y1=−1,y2=23y_1 = -1, y_2 = \frac{2}{3}. We consider two cases:
a) (49)x=−1\left(\frac{4}{9}\right)^x = -1 (no solutions);
b) (49)x=23,(23)2x=(23)1,2x=1,x=12\left(\frac{4}{9}\right)^x = \frac{2}{3}, \left(\frac{2}{3}\right)^{2x} = \left(\frac{2}{3}\right)^1, 2x = 1, x = \frac{1}{2}.
Example 10. Solve the equation
27x+12x=2⋅8x.27^x + 12^x = 2 \cdot 8^x.
This equation is close to the one just considered: the exponent of the bases is the same, but bases 27, 12 and 8 do not form a geometric progression. The numbers 27, 18, 12, and 8 form a geometric progression—we can assume that the term containing 18x18^x enters the equation with a coefficient of zero.

Solved and e. Delimm all terms on 8x8^x, we get
(32)3x+(32)x=2.\left(\frac{3}{2}\right)^{3x} + \left(\frac{3}{2}\right)^x = 2.
Denoting (32)x\left(\frac{3}{2}\right)^x by yy, we arrive at the cubic equation
y3+y−2=0,y^3 + y - 2 = 0,
the left side of which can be easily factorized:
(y3−1)+(y−1)=0,(y^3 - 1) + (y - 1) = 0,
(y−1)(y2+y+2)=0.(y - 1)(y^2 + y + 2) = 0.

The only real root of this equation y=1y = 1 leads to the equation (32)x=1\left(\frac{3}{2}\right)^x = 1, from which we find x=0x = 0.

Example 11. Solve the equation
5⋅23x−3−3⋅25−3x+7=0.5 \cdot 2^{3x - 3} - 3 \cdot 2^{5 - 3x} + 7 = 0.
Solved and e. Let us rewrite the equation in the form
58⋅23x−9623x+7=0.\frac{5}{8} \cdot 2^{3x} - \frac{96}{2^{3x}} + 7 = 0.
Let’s denote 23x2^{3x} by yy, then we get:
58y−96y+7=0,\frac{5}{8} y - \frac{96}{y} + 7 = 0,
5y2+56y−768=0,5y^2 + 56y - 768 = 0,
y1=−19,2;y2=8.y_1 = -19,2; y_2 = 8.
a) 23x=−19,22^{3x} = -19,2 - the equation has no solution.
b) 23x=8,23x=23,3x=3,x=1.2^{3x} = 8, 2^{3x} = 2^3, 3x = 3, x = 1.
In the example above, the product of the bases is equal to one, and this is immediately noticeable; in the following example this fact is not so easy to notice *).

Example 12. Solve the equation
(5+26)x+(5−26)x=10.\left(\sqrt{5 + 2\sqrt{6}}\right)^x + \left(\sqrt{5 - 2\sqrt{6}}\right)^x = 10.
Solved and e. Multiply the bases:
5+26⋅5−26=25−24=1.\sqrt{5 + 2\sqrt{6}} \cdot \sqrt{5 - 2\sqrt{6}} = \sqrt{25 - 24} = 1.
If we denote (5+26)x\left(\sqrt{5 + 2\sqrt{6}}\right)^x by yy, then (5−26)x=1(5+26)x=1y\left(\sqrt{5 - 2\sqrt{6}}\right)^x = \frac{1}{\left(\sqrt{5 + 2\sqrt{6}}\right)^x} = \frac{1}{y}. Hence
*) Note that the equations analyzed in examples 11 and 12 can be attributed to the same type as the equations in examples 9 and 10: the bases of the degree 2, 1, 12\frac{1}{2} and 5+26\sqrt{5 + 2\sqrt{6}}, 1, 5−26\sqrt{5 - 2\sqrt{6}} form a geometric progression and are raised to the same dependence on the xx degree.

Sheet 46

p. 44Transcribed from the scan · Rough draft translation, low quality

44

  1. 4x−3x−12=3x+12−22x−14^x - 3^{x-\frac{1}{2}} = 3^{x+\frac{1}{2}} - 2^{2x-1}.
  2. 3⋅2x+2⋅3x=2x+3+3x−23 \cdot 2^x + 2 \cdot 3^x = 2^{x+3} + 3^{x-2}.
  3. 9x−2x+12=2x+72−32x−19^x - 2^{x+\frac{1}{2}} = 2^{x+\frac{7}{2}} - 3^{2x-1}.
  4. 3x+1+3x−1+3x−2=5x+5x−1+5x−23^{x+1} + 3^{x-1} + 3^{x-2} = 5^x + 5^{x-1} + 5^{x-2}.
  5. 9x−1+3x=2⋅31,5x9^{x-1} + 3^x = 2 \cdot 3^1, 5^x.
  6. 4x+x2−2−5⋅2x−1+x2−2=64^x + \sqrt{x^2-2} - 5 \cdot 2^{x-1} + \sqrt{x^2-2} = 6.
  7. 8x+18x=2⋅27x8^x + 18^x = 2 \cdot 27^x.
  8. 31−x−31+x+9x+9−x=63^{1-x} - 3^{1+x} + 9^x + 9^{-x} = 6.
  9. (23)3x−(32)3x−23x+32x=3\sqrt[x]{\left(\frac{2}{3}\right)^3} - \sqrt[x]{\left(\frac{3}{2}\right)^3} - \sqrt[x]{\frac{2}{3}} + \sqrt[x]{\frac{3}{2}} = 3.
  10. 69x−136x+64x=06 \sqrt[x]{9} - 13 \sqrt[x]{6} + 6 \sqrt[x]{4} = 0.
  11. 4x=2⋅14x+3⋅49x4^x = 2 \cdot 14^x + 3 \cdot 49^x.
  12. (a+a2−1)x+(a−a2−1)x=2a(\sqrt{a + \sqrt{a^2-1}})^x + (\sqrt{a - \sqrt{a^2-1}})^x = 2a (a>1a > 1).

Check that the equation of Example 12 is obtained from this equation at a=5a = 5. Write what form this equation takes at a=2,3,2,3,4,6a = \sqrt{2}, \sqrt{3}, 2, 3, 4, 6.

  1. 2x−3x2=12^x - 3^{\frac{x}{2}} = 1.
  2. (sin⁡1)x+(cos⁡1)x=1(\sin 1)^x + (\cos 1)^x = 1.
  3. 3x−1+5x−1=343^{x-1} + 5^{x-1} = 34.
  4. 5x+12x=13x5^{\sqrt{x}} + 12^{\sqrt{x}} = 13^{\sqrt{x}}.
  5. 10x2=2⋅100x10^{x^2} = 2 \cdot 100^x.
  6. 2x+3−3x2−2=3x2+1−2x−12^{x+3} - 3^{x^2} - 2 = 3^{x^2} + 1 - 2^{x-1}.
  7. 3x2+4x2=5x23^{x^2} + 4^{x^2} = 5^{x^2}.
  8. xx=(x)xx^{\sqrt{x}} = (\sqrt{x})^x.
  9. xx2=(x)xx^{\sqrt{x^2}} = (\sqrt{x})^x.
  10. 8x+9⋅2x+2=2088^x + 9 \cdot 2^{x+2} = 208.

(For a start, see page 31.)

The next important step in the assimilation of electromagnets was made by the American physicist Joeph Henry in 1827. He is the first to contract for an iron core, not just one, but many layers of wiring, and the turns themselves are laid close to each other. It is possible that this would have been allowed by others, but at that time there was no wiring covered with insulation. Henry was the first to do such wiring. Insulated wires were not on sale then, and much later, of course. According to Henry’s employee, the inventor of the telephone, F. Morse, even in 1837, only … milliners used non-bare wires to make the frames of ladies’ hats. Henry made the wires covered with insulation himself. As an insulating material, he used strips of silk cut from … his wife’s outfits (in those days, women wore long and fluffy clothes). This is how insulated wires first appeared and were used. Judging by Henry’s electromagnets preserved in the museum, he had to wind silk strips around a lot of the wiring. But already in 1831 he could report that his largest electromagnet was capable of holding a load of 930 kilograms!

Sheet 47

p. 45Transcribed from the scan · Rough draft translation, low quality

45

WRITTEN EXAM
IN MATHEMATICS
AT MSU MEKHMAT IN 1970

N. N. Kolesnikov

In «Kvant» No. 2 for 1970, an article by N. S. Bakhvalov and N. N. Kuznetsov about the written exam in mathematics at the mexmate of Moscow State University in 1969 was published. Without repeating the comments made there about the nature of this exam, I would like to emphasize some of its features in 1970.

The tasks proposed to applicants once again confirm the position that their successful solution was achieved by any applicant, according to the conditions of the school program, and not just by a graduate of mathematics schools. You will see that these problems do not contain “pitfalls” or “traps”, but require a clear understanding of the main sections of the mathematics program for applicants to universities and certain skills in technical calculations and solving simple equations, inequalities and geometric problems.

Naturally, such “standardization” of problems implies increased requirements for the evaluation of their solutions, requirements for the ability to bring a solution to the end, and not limit oneself to hints at a solution. A satisfactory mark (tri) was given in 1970 for completing the correct solution of any two or three problems, good (four) for any four problems, excellent (five) for five problems. 4 astronomical hours were allotted to solve the problem (a set of five problems - variants).

Let’s move on to analyzing one of the options for the written exam in mathematics, briefly focusing on the most typical errors encountered in the works of those admitted to the Faculty of Mechanics and Mathematics.

Option 1

  1. Solve inequality
    −log⁡2(1+cos⁡3x)≤2+log⁡2(14−cos⁡x).-\log_2(1 + \cos 3x) \leq 2 + \log_2\left(\frac{1}{4} - \cos x\right).

  2. Find all valid solutions of the system
    {y2−∣xy∣+2=0,8−x2=(x+2y)2.\begin{cases} y^2 - |xy| + 2 = 0, \\ 8 - x^2 = (x + 2y)^2. \end{cases}

  3. Three racers A, B and C, starting at the same time, move at constant speeds in one direction along a ring road. At the start, racer B is in front of racer A at a distance of 1/31/3 the length of the highway, and racer C is in front of racer B at the same distance. Racer A first caught up with B at the moment when B finished his first lap, and 10 minutes later A caught up with racer C for the first time. Racer B spends 2.5 minutes less per lap than C. How much time does racer A spend on a lap?

  4. On the diagonal AC of the convex plane ABCD there is the center of a circle of radius r tangent to sides AB, AD and BC. On the diagonal BD is the center of a circle of the same radius r, touching sides BC, CD and AD. Find the area of ​​four (circle ABCD), knowing that the indicated circles touch each other externally.

  5. A ball of radius r touches plane P at point A. Line l forms with plane P

Sheet 49

p. 47Transcribed from the scan · Rough draft translation, low quality

47

includes the product of unknowns module, consider two cases.

a) Let xy≥0xy \geq 0. In this case, the conditions of the system have the form

{y2−xy+2=0,8−x2=(x+2y)2,y2−xy+2=0,−8+2x2+4xy+4y2=0.\begin{cases} y^2 - xy + 2 = 0, \\ 8 - x^2 = (x + 2y)^2, \\ y^2 - xy + 2 = 0, \\ -8 + 2x^2 + 4xy + 4y^2 = 0. \end{cases}

Multiplying the first equation by 4 and adding it with the second, we get 2x2+8y2=02x^2 + 8y^2 = 0, which is only possible for real x=y=0x = y = 0. But these values ​​of unknowns to the system under consideration are unsatisfactory.

b) Let now xy<0xy < 0. The original system will take the form

{y2+xy+2=0,8−x2=(x+2y)2y2+xy+2=0,2x2+4xy+4y2−8=0.\begin{cases} y^2 + xy + 2 = 0, \\ 8 - x^2 = (x + 2y)^2 \\ y^2 + xy + 2 = 0, \\ 2x^2 + 4xy + 4y^2 - 8 = 0. \end{cases}

Multiplying the first equation again by 4 and subtracting it from the second, we get x2=8x^2 = 8, that is, x=±22x = \pm 2\sqrt{2}. Now from the first equation it is easy to find y:(y±2)2=0y: (y \pm \sqrt{2})^2 = 0, hence y=∓2y = \mp \sqrt{2}.

According to assumption xy<0xy < 0. Taking this into account, we find the answer:

x=22,y=−2x = 2\sqrt{2}, y = -\sqrt{2}

or

x=−22,y=2x = -2\sqrt{2}, y = \sqrt{2}

The check confirms that both pairs of numbers are roots.

This example also does not contain any tricks or tricks. It is designed for schoolchildren with a normal mathematical background. The mistakes made when solving this example were associated with a unclear idea of ​​the absolute value (modulus) of a function and the inability to correctly write down the answer. In this case, either two cases were not considered, and the equation with the model was simply replaced by one or another equation without it, or the resulting set of values ​​xx and yy did not agree with the conditions xy<0xy < 0, and unnecessary answers appeared.

  1. This problem can be solved in different ways by introducing certain unknowns.

Let tA,tBt_A, t_B and tCt_C be the times that racers AA, BB and CC spend on a lap, respectively (we take the length of the path to be one). Then the speeds of each of them will be 1tA,1tB,1tC\frac{1}{t_A}, \frac{1}{t_B}, \frac{1}{t_C}.

Note that at any but identical absolute speeds, the distance between the riders would remain unchanged throughout the entire movement. The distance between the racers is reduced due to the excess speed of one over the speed of the other. The speed of the racer AA relative to BB is 1tA−1tB\frac{1}{t_A} - \frac{1}{t_B}, AA relative to CC is 1tA−1tC\frac{1}{t_A} - \frac{1}{t_C}, and the speed of BB relative to CC is 1tB−1tC\frac{1}{t_B} - \frac{1}{t_C}.

Now it is easy to translate the conditions of the problem into equation language. Since the rider AA first agreed to BB when the latter completed his first lap, then AA agreed to BB in tBt_B hours. But for this AA to cover 1/31/3 of the circle with a relative speed of 1tA−1tB\frac{1}{t_A} - \frac{1}{t_B}, this gives the equation

(1tA−1tB)tB=13.\left(\frac{1}{t_A} - \frac{1}{t_B}\right)t_B = \frac{1}{3}.

The initial distance between racers AA and CC was 2/32/3, racer AA covered it at a relative speed of 1tA−1tC\frac{1}{t_A} - \frac{1}{t_C} in tB+16t_B + \frac{1}{6} hours; we got the second equation:

(1tA−1tC)(tB+16)=23.\left(\frac{1}{t_A} - \frac{1}{t_C}\right)\left(t_B + \frac{1}{6}\right) = \frac{2}{3}.

In addition, it is known that

tB+124=tC.t_B + \frac{1}{24} = t_C.

From equation (1) it immediately follows that tB=43tAt_B = \frac{4}{3}t_A, and from equation (3) tC=43tA+124t_C = \frac{4}{3}t_A + \frac{1}{24}. Excluding now from

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Fig. 2.

equation (2) tBt_B and tCt_C, we obtain an equation containing only tAt_A:

(1tA−2432tA+1)(43tA+16)=23,\left( \frac{1}{t_A} - \frac{24}{32t_A + 1} \right) \left( \frac{4}{3} t_A + \frac{1}{6} \right) = \frac{2}{3},

or

64tA2−12tA−1=0.(4)64t_A^2 - 12t_A - 1 = 0. \quad (4)

Discarding the negative solution of the quadratic equation (4), which is unsuitable for the purpose of the problem, we obtain the answer: tA=14t_A = \frac{1}{4}.

Most of the applicants who did not fully solve this problem did not show decent skills in solving logical problems: they either made mistakes when composing the equation, or could not accurately solve the resulting system.

  1. Let ABCDABCD (Fig. 2) be the given quadrilateral, O1O_1 and O2O_2 the centers of the indicated circles lying on the diagonals ACAC and DBDB. Points K1,L1,M1K_1, L_1, M_1 are the tangent points of the circle centered at O1O_1 from the side AD,AB,BCAD, AB, BC, respectively, and K2,L2,M2K_2, L_2, M_2 are the tangent points of the circle centered at O2O_2 from the side AD,CD,BCAD, CD, BC. Let B′B' be the base of the height dropped from BB to ADAD.

According to the conditions, the circles are equal and touch each other, which implies the parallelism of their common tangents: BCBC and ADAD. Now we replace that ⇒BCA=⇒CAD\Rightarrow BCA = \Rightarrow CAD, as crosswise angles, and ⇒CAD=⇒BAC\Rightarrow CAD = \Rightarrow BAC, since ACAC is a bisector (ABAB and ADAD are tangents, and ACAC passes through the center of the circle). Therefore, ⇒BAC=⇒CAD\Rightarrow BAC = \Rightarrow CAD is demanding, ⇒ABC\Rightarrow ABC is equilateral and AB=BCAB=BC.

So, our quadrilateral has BC∥AD,AB=CDBC \parallel AD, AB=CD, therefore, it is either a trapezoid, and an equilateral one, or a parallelogram.

The parallelogram is not suitable, since the centers O1O_1 and O2O_2 must lie on the midline of the quadrilateral, but in a parallelogram the diagonals, intersecting each other, are divided in half, that is, the centers of the circles would have to coincide, which contradicts the conditions. We follow the new figure (Fig. 3).

Let BM1=M2C=xBM_1=M_2C=x. Then AB=BC=2r+2xAB=BC=2r+2x. But BM1=BL1BM_1=BL_1, as segments of tangents drawn to a circle from one point, and then AL1=AK1=2r+xAL_1=AK_1=2r+x.

By construction, B′K1=xB'K_1=x, therefore, AB′=2r=BB′AB'=2r=BB', the triangle AB′BAB'B is equilateral and right-angled, that is

⇒A=⇒ABB′=π4иD=π4.\Rightarrow A = \Rightarrow ABB' = \frac{\pi}{4} \quad \text{и} \quad D = \frac{\pi}{4}.

Now it’s easy to get the answer. Required area

S=BB′BC+AD2,BB′=2r,S = BB' \frac{BC+AD}{2}, \quad BB' = 2r,

BC=AB=22r,BC = AB = 2\sqrt{2}r,

AD=BC+2AB′=22r+4r,AD = BC + 2AB' = 2\sqrt{2}r + 4r,

S=2r⋅22r+(22r+4r)2=4(2+1)r2.S = 2r \cdot \frac{2\sqrt{2}r + (2\sqrt{2}r + 4r)}{2} = 4(\sqrt{2} + 1)r^2.

A typical mistake made when solving this problem was

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Fig. 4.

low excessive enthusiasm for the “obviousness” of some logical expressions, carelessness in intermediate reasoning. Thus, many wrote without any evidence that ABCDABCD is an equilateral trapezoid; other possibilities were not explored. There have been cases when the proof that ABCDABCD can only be a trapezoid was … a drawing and words that to fulfill the conditions of the problem, a quadrilateral cannot be drawn in any other way.

  1. Let B′B' be the base of the perpendicular dropped from the point BB to the plane PP (Fig. 4). According to the conditions

⇒BCB′=φ,OB=OA=r,CA=2r,⇒CBO=π2.\Rightarrow BCB' = \varphi, OB = OA = r, CA = 2r, \\ \Rightarrow CBO = \frac{\pi}{2}.

Finding the length of the segment ABAB can be found, for example, from the right triangle AB′BAB'B, the sides of which are easy to calculate. Note that CB=CA=2rCB = CA = 2r are segments of tangents to the ball drawn from one point. It follows that

BB′=CBsin⁡φ=2rsin⁡φ.BB' = CB \sin \varphi = 2r \sin \varphi.

Side AB′AB' of triangle AB′BAB'B is equal to the perpendicular OO′OO' dropped from OO to BB′BB' (OA∥BB′OA \parallel BB', as perpendiculars to one plane; BB′⊥AB′BB' \perp AB' since AB′AB' lies in the plane PP, perpendicular to BB′BB'; OO′⊥BB′OO' \perp BB' by construction; therefore OO′B′AOO'B'A is straight). OO′OO' is from right triangle OO′B′OO'B':

OO′=r2−(BO′)2,OO' = \sqrt{r^2 - (BO')^2},

BO′=∣BB′−B′O′∣=∣BB′−OA∣=∣2rsin⁡φ−r∣,BO' = |BB' - B'O'| = |BB' - OA| = |2r \sin \varphi - r|,

OO′=AB′=sin⁡φ−sin⁡2φ⋅2r.OO' = AB' = \sqrt{\sin \varphi - \sin^2 \varphi} \cdot 2r.

Finally, ABAB is found from triangle AB′BAB'B:

AB=(AB′)2+(B′B)2=2rsin⁡φ.AB = \sqrt{(AB')^2 + (B'B)^2} = 2r \sqrt{\sin \varphi}.

We are now convinced that the difficulties in solving this stereometric problem (as well as others proposed in 1970) do not exceed those encountered in solving school problems. However, every year a lot of applicants for the written exam in mathematics simply do not attend to solving stereometric problems, apparently believing that they are inherently impossible to solve.

Among the errors encountered in the work of the applicants, it should be noted that it is not clear what an angle of a straight line with a plane is. Thus, in the problem analyzed, this angle is often taken to be ⇒BCA\Rightarrow BCA.

It is also common when deciding to use the conditions that ⇒CB′A\Rightarrow CB'A is direct, although in the general case this is not at all true.

In conclusion, we offer readers of the magazine, for their own decision, another version of a written work in mathematics, proposing the mechanism of Moscow State University in 1970.

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Option 2

  1. Solve inequality
    log⁡2(1+cos⁡4x)≤1+log⁡2sin⁡x.\log_2(1 + \cos 4x) \leq 1 + \log_{\sqrt{2}} \sin x.

  2. Find all valid solutions of the system
    {∣xy−2∣=6−x2,2+3y2=2xy.\begin{cases} |xy - 2| = 6 - x^2, \\ 2 + 3y^2 = 2xy. \end{cases}

  3. Three racers (AA, then BB and then CC) start with an interval of 1 minute from one point on the track highway and move in the same direction at constant speeds. Each racer spends more than two minutes on a lap. Having made three laps, the racer AA will finish BB for the first time at the starting point, and after another 3 minutes he will overtake CC for the second time. Racer BB agreed for the first time CC also at the starting point, having completed 4 laps. How many minutes does a racer AA spend on a lap?

  4. A convex quadrilateral ABCDABCD contains two circles of the same radius rr, externally touching each other. The center of the first circle is on the segment connecting vertex AA with the midpoint FF of side CDCD, and the center of the second circle is on the segment connecting vertex CC with the midpoint EE of side ABAB. The first circle touches sides ABAB, ADAD and CDCD; the second circle touches sides ABAB, BCBC and CDCD. Find ACAC.

  5. The length of each edge of the triangular pyramid SABCSABC is equal to 1. BDBD is the height of triangle ABCABC. The equilateral triangle BDEBDE lies in the plane forming an angle φ with the edge ACAC, and the points SS and EE lie on the same side of the plane ABCABC. Find the distance between points SS and EE.

Sweeping. In problem 2, the system can be solved differently: from the first equation, express xx through yy and substitute it into the second. Try this solution method.

Figure 3 is symmetrical, therefore BM1=M2CBM_1 = M_2C, which are used in the solution of problem 4. One can, however, deduce this equality from the equality of the corresponding triangles.

In problem 5
In the solution to Problem 5, the model signs in BO′BO' are placed because the point BB can lie lower than the point O′O'.

Physics questions

  1. Is the power of a hydroelectric power plant sufficient to evaporate the water passing through the turbines?

  2. What gets cold faster under the same conditions: broth or tea? Why?

  3. The terminal rod is suspended on light threads (see Fig. 1). Where is its center of gravity?

  4. Two identical boas begin to simultaneously swallow each other from the tail and do this at a constant speed until each of them passes the other’s body completely (but without heads). Draw a diagram of how it all ends.

  5. Fill a 2 liter saucepan to the top with water. A thin-walled pan with a capacity of 1.5 liters and a weight of 0.6 kg (Fig. 2.) is placed in it. How much water will come out?

  6. Pure water is used for light. Why is fog, which is small drops of water, opaque?

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51

WRITTEN EXAM
IN PHYSICS AT MOSCOW ROAD ROAD INSTITUTE

A. N. Ageev, Yu. G. Rudoy

This year, a written exam in physics was held for the first time at the Moscow Automobile and Road Institute. Each ticket consists of a theoretical question on one of the sections of the program and four tasks designed to cover all sections of the program.

When answering a theoretical question and solving problems, applicants had to show both the meaning of physical laws and the ability to apply them in a particular physical situation, as well as the meaning of units of measurement of physical quantities and correctness in calculations. Therefore, all problems had to be solved first in general form, and then a numerical answer was obtained.

As the exams showed, answering the theoretical question did not cause any difficulties and the overwhelming majority of applicants answered them well. The tasks were, as a rule, more difficult.

Let us give, as an example, several problems proposed in the exam papers and, describing their solutions, let us briefly dwell on some characteristics of construction errors. For convenience, we have divided these tasks into traditional sections.

In problems on mechanics, errors were mainly due to the fact that the examinee was not always able to identify all the forces that control movement and correctly determine their point of application and direction. This is where the equation of motion is drawn up incorrectly. For example, in this problem:

Task 1 (variant No. 26). Two bodies with masses m1=50m_1=50 e and m2=100m_2=100 e, connected incredibly by a thread, lie on a smooth horizontal surface. A force F=300ΓF=300\Gamma is applied to the first body, directed along the plane. Find the tension of the bottom when the bodies move. Will the force change if the same force is applied to the second mass? Neglect friction on the surface (Fig. 1).

The acceleration of the system in the first and second cases is the same. Indeed, applying Newton’s 2nd law to the entire system, we obtain:

in case a) F=(m1+m2)a1F=(m_1+m_2)a_1,
in case b) F=(m1+m2)a2F=(m_1+m_2)a_2.

From here

a1=a2=a=Fm1+m2.a_1=a_2=a=\frac{F}{m_1+m_2}.

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Fig. 2.

The thread tensions, however, are different: the force T1T_1 imparts an acceleration aa to a body with mass m1m_1, and therefore

T1=m1a=m1m1+m2⋅F=100Γ,T_1 = m_1 a = \frac{m_1}{m_1 + m_2} \cdot F = 100 \Gamma,

and the force T2T_2 imparts this acceleration to a body with mass m2m_2, and therefore

T2=m2a=m2m1+m2⋅F=200Γ.T_2 = m_2 a = \frac{m_2}{m_1 + m_2} \cdot F = 200 \Gamma.

There were many errors in this task:

Problem 2 (varnant No. 16). A load with a mass of m=140m=140 kg lying on the floor of the lowering elevator car presses on the floor with a force of N=147N=147 kg. Determine the magnitude and direction of the elevator acceleration.

Let us assume that the acceleration is directed upward (Fig. 2). Then, based on Newton’s 2nd law, we can write F−P=maF-P=ma (F is the support reaction force).

From here

a=gF−PP.a = g \frac{F-P}{P}.

According to Newton’s 3rd law F=NF=N. That’s why

a=gN−PP=0,05g.a = g \frac{N-P}{P} = 0,05g.

So, the acceleration is directed upward and is equal to 0.05 g.

Quite a large number of applicants confuse rest training and sliding training. The resting force is always equal to the tg force, and the sliding force is equal to kNkN, where NN is the normal pressure force. If you attach a diameter gauge to a beam lying on a horizontal surface and slowly increase

Fig. 3.

Liquify the friction until the block begins to slide along the surface, then the dependence of the friction on the friction will be graphically depicted as shown in figure 3. Point AA corresponds to the beginning of the movement.

There were many mistakes associated with the insufficient importance of conservation laws and the inability to use these extremely powerful methods for solving problems.

In cases where the application of the laws of conservation of energy and implyvas allows one to obtain a simple and elegant solution, applicants usually chose a relatively long solution path using the laws of motion. Let us present for use a problem from the 2nd round of the Physics Olympiad, which was held at MADI in 1970.

Problem 3. A puck of mass mm moves horizontally with a speed v0v_0, hits the platform of mass MM and continues to move along its surface. Determine the speed

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53

the growth of the platform by the time the puck stops on it. The friction coefficient between the washer and the platform is kk. The platform can roll on the rails without friction.

Let us first solve this problem using the laws of motion.

A friction force equal to kmgkmg acts on the washer and platform in the horizontal direction, under the influence of which the platform and washer move with accelerations aππa_{\pi\pi} and aπa_{\pi} relative to the ground. The directions of acceleration are shown in figure, and their magnitudes are determined by Newton’s 2nd law:

maπ=kmg,и поэтому aπ=kg,ma_{\pi}=kmg, \quad \text{и поэтому } a_{\pi}=kg,
Maππ=kmg,и поэтому aππ=kgmM.Ma_{\pi\pi}=kmg, \quad \text{и поэтому } a_{\pi\pi}=kg\frac{m}{M}.

The acceleration of the puck relative to the platform is

a⃗=aπ−aππ⃗,или a=aπ+aππ=\vec{a}=a_{\pi}-\vec{a_{\pi\pi}}, \quad \text{или } a=a_{\pi}+a_{\pi\pi}=
=kg(1+mM).=kg\left(1+\frac{m}{M}\right).

Since the speed of the puck relative to the platform decreases with time according to the law v=v0−atv=v_0-at, then v=0v=0 (that is, the puck will stop) after time

t=v0a=v0kg(1+mM).t=\frac{v_0}{a}=\frac{v_0}{kg\left(1+\frac{m}{M}\right)}.

By this time the speed of the platform becomes equal

vππ=aππt=kgmM⋅v0kg(1+mM)=v_{\pi\pi}=a_{\pi\pi}t=kg\frac{m}{M}\cdot\frac{v_0}{kg\left(1+\frac{m}{M}\right)}=
=mv0m+M.=\frac{mv_0}{m+M}.

A significant solution to this problem is to use the law of conservation of momentum. Indeed, the frictional force between the puck and the platform is an internal force, and therefore it cannot change the overall momentum of the system. At the same time, external forces in the horizontal direction do not act on the platform-puck system (recall that the platform rolls on rails without friction). Equating them

the pulse of the system at the initial moment, when the platform is still finished, its pulse at the moment when the puck stops on the platform, we get

mv0=(m+M)vππ.mv_0=(m+M)v_{\pi\pi}.

From here

vππ=mv0m+M.v_{\pi\pi}=\frac{mv_0}{m+M}.

There were many mistakes when solving the gas laws problem. Here, applicants quite easily coped with those tasks for which only formal knowledge of the laws was sufficient, but in those cases where the solution required somehow transforming the notation of laws or simply consistently applying gas laws for various elementary processes, much was lost. Let’s give an example.

Task 4 (varnant No. 26). Gaz eradicated from volume V1=8λV_1=8\lambda to volume V2=6λV_2=6\lambda. The pressure increased by Δp=4⋅103μM2\Delta p=4\cdot10^3\frac{\mu}{M^2}.

What was the initial pressure?

To solve it, it is enough to write the Boyle-Mariotte law in the following form:

V1−V2V2=P2−P1P1.\frac{V_1-V_2}{V_2}=\frac{P_2-P_1}{P_1}.

From here

P1=ΔPV2ΔV=12⋅103μM2.P_1=\Delta P\frac{V_2}{\Delta V}=12\cdot10^3\frac{\mu}{M^2}.

The exams showed that applicants were weak in diagrammatic representations of various processes. Therefore, few people correctly solve problems of the following type.

Fig. 5.

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Fig. 9.

Errors in problems of determining the work of moving a charge are mainly associated with a flat polyman of the physical meaning of such a characteristic of the electric field as potential. Many have tried to find work using the formula A=F⋅SA = F \cdot S, whereas in a non-uniform field the force acting on the charge changes as it moves and this formula cannot be used. To solve such problems it is necessary to apply the concept of potential difference. Let’s take the following problem as an example.

Task 7 (varnant 24). What work must be done to move the exact charge q=20q = 20 units. SGSE from infinity to point AA, located at a distance of L=10L = 10 cm from the surface of the metal ball (Fig. 9)? The potential of the ball is φ0=200\varphi_0 = 200 θ\theta, the radius of the ball is R=2R = 2 cm. The ball is in the air (Fig. 11).

By definition, the potential at point AA is numerically equal to the work of moving a unit positive charge from infinity to a given point. Therefore, the original work W=q⋅φAW = q \cdot \varphi_A. Since the field of a charged sphere coincides with the field of an exact charge equal to the charge of the sphere and is located at the center of the sphere, the potential at point AA is equal to φA=QR+L\varphi_A = \frac{Q}{R + L}. Next, since

φ0=QR,то φA=φ0⋅RR+Lи\varphi_0 = \frac{Q}{R}, \quad \text{то } \varphi_A = \varphi_0 \cdot \frac{R}{R + L} \quad \text{и}
W=q⋅φA=q⋅φ0⋅RR+L=2,2 эрэ.W = q \cdot \varphi_A = q \cdot \varphi_0 \cdot \frac{R}{R + L} = 2,2 \text{ эрэ}.

Fig. 10.

In the “Constant Current” section, the greatest difficulty was caused by the tasks of calculating the circuit when charging the battery. Let’s consider, for example, the following problem.

Task 8 (varnant 52). The battery, discharged to 12θ12\theta, is connected for charging to a network with voltage 15θ15\theta (Fig. 10). What additional resistance RR must be connected to the circuit so that the charging current does not exceed 1α1\alpha? Internal battery resistance r=2Ωr = 2\Omega.

In the case when the battery operates as a current source and is connected to the load RR, the current is determined by Ohm’s law for the complete circuit:

I0=ER+r.I_0 = \frac{E}{R + r}.

Inside the source, this current is directed from the negative electrode to the positive one (Fig. 10). When charging a battery, the current in it has the opposite direction, that is, from the positive electrode to the negative. If the battery is positively discharged, then the charging current is determined by the formula I3=UcR+rI_3 = \frac{U_c}{R + r}, where UcU_c is the network voltage.

In the case when the battery is not completely discharged, as is the case in our case, the total current can be represented as the difference

I=I3−I0=UcR+r−ER+r,I = I_3 - I_0 = \frac{U_c}{R + r} - \frac{E}{R + r}, where EE is the value of e. d. c. discharged battery.

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Fig. 11.

Thus, Uc=I(R+r)+EU_c = I(R + r) + E. From here
R=Uc−E−IrI=1 ом.R = \frac{U_c - E - Ir}{I} = 1 \text{ ом}.

In the last section of the Optics program, as a rule, problems of constructing an image in lenses were not solved in cases where it was necessary to use a clear focal plane and secondary focus. Let us give examples of such problems.

Task 9 (varnant 78). Find by construction the path of the beam ABAB after the collecting line (Fig. 11).

Let us draw a secondary optical axis parallel to ABAB and intersecting the focal plane. The point of intersection of the secondary axis with the focal plane (F′F') is the secondary focus at which all rays parallel to this axis are collected. Consequently, the ray ABAB after the refraction of the line must pass through the point F′F' (Fig. 12).

The same problem with a scattering line is solved in a similar way. You just need to remember that the tricks in this case are minimal (Fig. 13).

Fig. 12.

Fig. 13.

In conclusion, we present one of the ticket options that were offered during the entrance exams.

Option 47

  1. Magnetic interaction of conductors with current. The concept of magnetic field, induction and lines of force (using the example of direct and circular current).
  2. A car weighing P=1 tP = 1 \text{ t} and developing 60 hp climbs a hill at a speed of v=36 km/часv = 36 \text{ km/час}. Determine the angle of inclination of the mountain α\alpha. Friction is not taken into account.
  3. In 480 e water at a temperature of −8∘C-8^\circ \text{C}. What is the temperature of the mixture if ice is dropped at 56 e? Ud. The heat capacity of ice is 0.5 cal/e deg, the specific heat of fusion is 80 cal/e.
  4. What speed does an electron acquire when it passes through a uniform electric field with a strength of 0.01 CGSE units along a field line at a distance of 2 cm?
  5. Construct an image of the segment ABAB in the collecting line (Fig. 14).

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PHYSICS NEWS

A new type of radioactivity - proton radioactivity

Until now, four types of radioactive decay have been known. β - decay occurs with the emission of electrons (β⁻-decay) or positrons (β⁺-decay); α - decay that occurs with the radiation of α - particles and γ - decay - the radiation of light quanta with high energy. Here we can also add nuclear fission (spontaneous - as they say, spontaneous), discovered in 1940 by Soviet physicists Flerov and Petrzhak, in which a heavy nucleus (uranium, plutonium, etc.) breaks into two.

At the end of 1970, another type of decay was discovered—proton radioactivity, the existence of which was predicted by corresponding member of the USSR Academy of Sciences V. I. Goldansky. Proton activity was discovered by Czerny and a group of English and American physicists.

The cobalt isotope with a mass number of 53 turned out to be proton-active. The nucleus of this isotope contains 27 protons and 26 neutrons. The decaying isotope is in the resulting state - its energy is approximately 3 MeV more than normal (1 MeV = 1 million electron volts = 1.6 10⁻⁶ere = 1.6 10⁻¹³ J).

53 Co decays, turns into an isotope of iron with mass number 52: 53Co→52Fe+proton

53Co(m)beech m means that cobalt arose and is in a metal-stable state) lives on average about 0.3 seconds. A proton-active isotope of cobalt is obtained as a result of the shelling of oxygen nuclei from calcium mines:

40Ca+16O=53Co+2 neutrons +1 proton

and as a result of the bombardment of iron protons

54Fe+p=53Co+2 neutrons The energy of the emitted protons is 1.6 MeV.

Reviews, bibliography

If you need to calculate something…

In our country, such a need may arise quite often and it is not always necessary to turn to the help of electronic computers. But if you have to count yourself, you will definitely come across tables.

You can be sure that in almost all cases, for calculations it will be enough to use “Four-digit mathematical tables” by L. S. Khrenov, published as a manual for teachers by the publishing house “Prosveshchenie” in 1967.

In addition to numerical tables, the author gives a brief formulation of the “Rules of Approximate Calculations.” They provide basic definitions, rules for operating with approximate numbers and interpolation, and recommendations regarding the order of calculations. As difficult as it may be, the author managed to be concise, precise and clear here at the same time. The “Explanations for the Tables” are also well written.

The main content of the book is the clear values ​​of the table of basic elementary functions that are well known to secondary school students and are often encountered in calculations. The book also contains a small table of prime numbers, a table of biominal coefficients and representations of irreducible fractions in the form of decimals.

L. S. Khrenov’s tables can be fully recommended both as a textbook for schoolchildren and as a tool for mass computing.

R. S. Guter

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58

Sorcerer
from Putapova street

G. I. Mishkevich

A post of mathematics, a bard of physics, a herald of astronomy—that was rightfully Yakov Isidorovich Perelman. His fascinating books on mathematics (arithmetic, algebra, geometry), physics (mechanics, acoustics, optics), astronomy and mechanical travel have sold millions of copies all over the world. The name of Ya. I. Perelman is associated with an entire era of Russian and especially Soviet popular science literature and its specific direction, which is called entertaining.

Yakov Isidorovich Perelman was born in Bialystok in 1882. His father was an accountant, his mother a schoolteacher.

He published his fascinating “intriguing” work back in 1899, while a student at the Bialystok real estate school. It was an essay “About the expected fiery rain”, published in the “Grodno Provincial Gazette”. The essay exposed in vivid form the changes in the churchmen’s views about the “coming end of the world.” Already in this youthful work, the tasks of the future talented popularizer are clearly visible.

I asked Yakov Isidorovich about how he became a popularizer, and Perelman responded like this:

“I owe this to my teachers and books. They taught me not only to love mathematics and physics, but also to think paradoxically. I began to look for an intriguing beginning everywhere, even where it seemed there was no trace of it.”

Later, Yakov Isidorovich, in the article “On the Methodology of Scientific Popularization,” writes: “Not everyone is able to find something new in the old, and not everyone is inclined to think deeply about what is constantly happening before their eyes.

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zami. To draw attention to offended phenomena, it is necessary to show new, unexpected sides to them.”
In another article, “What is Entertaining Science,” Perelman puts surprise in the first place: “We early cease to be surprised, early we lose the precious ability that prompts interest in things that do not directly affect our existence.”
Ya. I. Perelman perfectly mastered the art of surprising, knew how to intrigue, and touch the reader’s heartstrings. He expected the dry dogmas of school wisdom, turning them into a fascinating subject.
At the beginning of this century, Ya. I. Perelman moved to St. Petersburg and began to engage in literary activity, at the same time indicating a precious ability that encourages interest in things that do not directly affect our existence.”
Here he proposed moving the clocks forward an hour to save fuel for lighting. This proposal has received the force of law.)
When Perelman was studying at the Forestry Institute, Professor A. S. Domogarov drew attention to his mathematical abilities. It was he who instilled in his student a love of the ability to find what is necessary in the general.
While studying at the Forestry Institute, Yakov Isidorovich worked as a proofreader for the book distributor P. P. Soykin. Then he edited the magazines “Nature and People”, “In the Workshop of Nature”, and was published in the “World of Adventures”. Stats signed “I. Lesnoy", “P. Silvestrov”, “Ya. P.”, gained more and more sympathy. Here, in Soikin’s book assignment, Perelman began to seriously concern himself with the problems of an engaging presentation of science, primarily physics. Yakov Isidorovich considered the basis of such a presentation to be the ability to arouse keen interest in the subject. Only interest can facilitate understanding and, consequently, give rise to a conscious and lasting assimilation of the basic sciences.
Ya. I. Perelman’s first book, “Entertaining Physics,” was published in 1913. And its first reader and reader was the famous physicist teacher, professor at St. Petersburg University, Orest Danilovich Khvolson. He invited Perelman to his apartment, and the following conversation took place between them, as Yakov Isidorovich said:
— I read your book with satisfaction, it is excellent. But I haven’t seen your name among physicists. Where would you like to finish your course?
“I am a scientific forester, this is my knowledge…” Perelman became embarrassed.
“Well, I’ll tell you what,” Khvolson answered. “Even without you, we have scientists who are foresters, like trees in the forest, but we don’t have any physicists who could write like you.” Keep writing books like this in the future…
“Entertaining Physics” was followed by a whole series of entertaining books written by Yakov Isidorovich. Yes, Khvolson was right when he dissuaded Perelman from taking up forestry.
Perelman’s teachers, who shaped his art as a popularizer, were also books. He read a lot, systematically and with good pedagogy. His pedagogy was expressed in the fact that Yakov Isidorovich scrupulously kept a card index of what he read and made thousands of extracts. I remember well the racks of neat brown boxes filled with cards covered in caligraphic handwriting. Shelving takes up an entire wall in his spacious office.
Yakov Isidorovich loved to repeat Pascal’s aphorism: “The subject of mathematics is so heartfelt that one must not miss the opportunity to make it a little intriguing”—and he did this with amazing brilliance. Not only in application to mathematics, but also to the general class of physical sciences.

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To contradict A.P. Chekhov (already with his “entertaining” positions), Perelman finds in the story “Tutor” a problem that the merchant Udodov solved instantly on office accounts - much faster than his son’s tutor did. Yakov Isidorovich openly and fascinatingly reveals the mathematical sum of the merchant’s method of solving the problem. L. N. Tolstoy’s story “How a house was repaired in the city of Paris” gives Perelman a reason to comment on the phenomenon of thermal expansion of metals. In “Scenes from Times of Knighthood” by A. S. Pushkin, the dreamer Berthold hopes to discover “perpetual motion.” Perelman introduces Pushkin’s text with a corresponding scientific interpretation into his “Entertaining Physics”.

Perelman’s works are populated by heroes of novels, novels, short stories, and essays - from Servant’s Don Quixote to the Soviet parachute of Kaytanov, a master of exciting jumps.

Ya. I. Perelman analyzes the science fiction works of such royal genre figures as Jules Verne and Herbert Wells. Without in any way detracting from the complex and literary merits, Yakov Isidorovich shows on what scientific “thread” the entire work is held. In August 1934, a group of Leningrad writers and popular scientists met at the Astoria Hotel with the English writer Herbert Wells, who was then in Leningrad.

In the ensuing conversation, Wells, among other things, asked:

Aren’t you the same Jacob Perelman whose column uniquely interpreted my works? I read your “Amazing Physics” - that’s what it’s called in the English translation.

“The same one,” Perelman answered, smiling.

-… and who so kindly exposed my “Invisible Man”, pointing out that he must be blind, like a newborn puppy… And Mr. Cavor for the invention of a substance that is free from the effects of gravity…

— Yes, I wrote about this back in 1915. But that doesn’t make your novels any worse, does it?

“And I must admit, I tried so hard to hide these vulnerable spots from the reader’s eyes!”

His talent was that he could read.

Hundreds of letters were sent from everywhere to Plutalova Street. Many people needed Yakov Isidorovich: workers waited for him in the red corners of the workshops to listen to a lecture on space travel; schoolchildren tried to get him into their science clubs; Lawyers also needed him as a knowledgeable person, an expert on issues related to the scientific interpretation of any controversial fact. (There is a well-known case when Yakov Isidorovich spoke in court in the case of a driver accused of negligence. Perelman explained and proved to the court that the driver was not guilty - the reason was that the formation of the train was incorrect.) Yakov Isidorovich willingly shared his knowledge. Not wanting strength, he patiently “chipped off” capable people everywhere. The writer L.V. Uspensky said about him extremely accurately and aptly: “The bacillus carrier of the missing perelmanitis”!

In Nikolaev, Perelman found industrial engineer V.V. Ryumin, and the author of “Entertaining Chemistry” and “Entertaining Technicalities at a Construction Site” was born. In Moscow, professor of physics A.V. Tsinger was “discovered” - a passionate collector of herbariums. Thanks to Perelman, the physicist Tsinger became the author of the academic book “Entertaining Botany”.

“Entertaining meteorology” comes out with the light hand of Perelman

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D. O. Svyatsky and T. N. Klado, “Entertaining world studies” by V. O. Pryanishchinkov, “Entertaining statistics” by E. E. Svyatlovsky.

The appearance of “Entertaining Mineralogy” and “Entertaining Geochemistry” by Academician A. E. Fersman, “Entertaining Geology” by Academician V. A. Obruchev and “Entertaining Geography” by L. V. Uspensky also owes a lot to Perelman.

Geography, geology, geochemistry, mineralogy, statistics, meteorology, even military science (meaning Colonel V.P. Vnukov’s book “Physics and National Defense”) are included in the orbit of educational literature.

In 1935, Yakov Isidorovich with his team - V. A. Kamsky, A. Ya. Malkov, V. O. Pryanishchinkov, L. V. Uspensky - founded the House of Educational Science (DZN) in Leningrad. It was a genuine cabinet of curiosities for educational sciences: physics, mathematics, astronomy, geography, geology, meteorology. In 1939, there were more than 100 large exhibits in the Leningrad Science Museum, grouped in four departments: Astronomy, Geography (with the Geology Hall), Mathematics, and Physics (with the Optics Hall). In addition, an Electricity Department was created.

Everything in this house was exciting, but everything was strictly justified. Moving from room to room, from exhibit to exhibit, the visitor became convinced that the simple, boring school-truths are not so simple. Here people see the mediocre as entertaining and the boring as exciting and interesting.

Here, for example, is “Galton’s Board”. It was a very simple exhibit - an inclined board studded with steel pins. Millet was poured into the funnel. Hitting the stuffed needles, the grains were placed on an inclined board, always following the same curved line.

This was how the mathematical law of normal distribution was demonstrated - Gauss’s law. Gauss and… wheat!

DZN was not a cultural and educational “eatery”. Entertaining was not an end in itself, but a means of promoting science.

During this period of his activity, Perelman actively collaborated with such luminaries of accounting package science and technology as K. E. Tsiolkovsky, F. A. Tsander, S. P. Korolev, N. A. Rynin and others. He met with him through work at LenGIRD and carried on extensive correspondence.

In memory of the merits of Yakov Isidorovich Perelman, one of the craters on the far side of the Moon, first formed by the Soviet automatic international station “Luna-3” on October 7, 1959, is named after him. The Ya. I. Perelman crater has a diameter of 95 kilometers and is located at a point with lunar coordinates β = +16°30′ and λ = −160°.

The name of Ya. I. Perelman is immortalized on the Moon… It’s a shame that this has not been done on Earth. Plutalova Street, where Perelman lived, did not become Perelman’s street, and there is not even a memorial plaque on house No. 12. The House of Educational Science has not been revived either. …


We have tried to sketch a portrait of a person whose name is widely known throughout the world. Let us add that Yakov Isidorovich Perelman was a true patriot. When the Great Patriotic War began, he found himself evacuated from Leningrad. In the very first weeks, his only son Mikhail died at the front. His wife, a doctor, soon died of hunger. On April 3, 1942, Yakov Isidorovich Perelman died of exhaustion in besieged Leningrad.

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To the article “Conversion of electrical circuits”

  1. Let’s transform the “star” r1=r2=r3r_1 = r_2 = r_3 into a triangle (see Fig.). It is not difficult to find points passing through resistances R12R_{12}, R13R_{13} and R23:I12=1θ+2θR12=1a;I13=13a;I23=23aR_{23}: I_{12} = \frac{1\theta + 2\theta}{R_{12}} = 1a; I_{13} = \frac{1}{3}a; I_{23} = \frac{2}{3}a. This means that battery E1E_1 carries current I1=43aI_1 = \frac{4}{3}a, and battery E2E_2 carries current I2=53aI_2 = \frac{5}{3}a. This means that current I=13aI = \frac{1}{3}a flows through resistance r3r_3 in the original circuit.

  2. When the switch is open, the total capacitance of the capacitor system is C1=C2+C⋅2C3C=76CC_1 = \frac{C}{2} + \frac{C \cdot 2C}{3C} = \frac{7}{6}C. When the key is closed, it is equal to C2=1311CC_2 = \frac{13}{11}C. Pozotomu

ΔQ=E(C2−C1)=EC(1311−76)=166EC.\Delta Q = E(C_2 - C_1) = EC \left( \frac{13}{11} - \frac{7}{6} \right) = \frac{1}{66}EC.

To the article “Do you like tinkering with integers?”

  1. Consider these equations using models: a) 4; b) 9; b) 8; d) 7.

  2. Use that any such number has a remainder of 1 when divided by 9.

  3. This number is divisible by 3 and not divisible by 9.

  4. a) λ−1\lambda^{-1}; b) λ\lambda because 6215−13145=89⋅56 \frac{2}{15} - 1 \frac{31}{45} = \frac{8}{9} \cdot 5; b) λ4\lambda^4.

  5. 1+3+32+⋯+3n=−12+12⋅3n+11 + 3 + 3^2 + \dots + 3^n = -\frac{1}{2} + \frac{1}{2} \cdot 3^{n+1}, therefore αn=d3(12⋅3n+1,0)=λn+1\alpha_n = d_3 \left( \frac{1}{2} \cdot 3^{n+1}, 0 \right) = \lambda^{n+1}. Search λ<1\lambda < 1, then this sequence tends to 0.

Note that the geometric progression 1, 3, 3², …, 3ⁿ, … is infinitely decreasing in terms of the distance d3d_3: d3(3n+1,0)=λn+1d_3 (3^{n+1}, 0) = \lambda^{n+1}, so it is not surprising that its sum can be found using the general formula

1+3+32+⋯=11−3=−12.1 + 3 + 3^2 + \dots = \frac{1}{1-3} = -\frac{1}{2}.

  1. 41481=⟨11,0112⟩;14181=⟨1,1112⟩;d3(41481,14181)=λ−1.4 \frac{14}{81} = \langle 11,0112 \rangle; 1 \frac{41}{81} = \langle 1,1112 \rangle; d_3 \left( 4 \frac{14}{81}, 1 \frac{41}{81} \right) = \lambda^{-1}.

  2. −1=⟨...22222⟩;12=(−12)+1=⟨...11112⟩;25=⟨...121012101211⟩-1 = \langle ... 22222 \rangle; \frac{1}{2} = \left( -\frac{1}{2} \right) + 1 = \langle ... 11112 \rangle; \frac{2}{5} = \langle ... 121012101211 \rangle (you can use the fact that 25=481−81+1\frac{2}{5} = \frac{48}{1-81} + 1); 245=⟨...1210121012,11⟩\frac{2}{45} = \langle ... 1210121012, 11 \rangle.

To the article “Exponential Equations”

  1. x=9x=9.
  2. x=4x=4.
  3. x=3x=3.
  4. x=32x=\frac{3}{2}.
  5. x=lg⁡45−lg⁡17lg⁡3−lg⁡2x = \frac{\lg 45 - \lg 17}{\lg 3 - \lg 2}.
  6. x=32x=\frac{3}{2}.
  7. x=2x=2.
  8. x1,2=2lg⁡(9±72)lg⁡3x_{1,2} = \frac{2 \lg (9 \pm \sqrt{72})}{\lg 3}.
  9. x=32x=\frac{3}{2}.
  10. x=0x=0.
  11. x1=log⁡3(2+5);x2=log⁡35−12x_1 = \log_3 (2 + \sqrt{5}); x_2 = \log_3 \frac{\sqrt{5} - 1}{2}.

Hint: Denote 3x−3−x3^x - 3^{-x} by yy and show that 9x+9−x=y2+29^x + 9^{-x} = y^2 + 2.

  1. x=lg⁡2−lg⁡3lg⁡(1+5)−lg⁡2x = \frac{\lg 2 - \lg 3}{\lg (1 + \sqrt{5}) - \lg 2}.

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and e: enter the notation (23)1x−(23)−1x=y\left(\frac{2}{3}\right)^{\frac{1}{x}} - \left(\frac{2}{3}\right)^{-\frac{1}{x}} = y and check that (23)3x−(23)−3x=y3+3y\left(\frac{2}{3}\right)^{\frac{3}{x}} - \left(\frac{2}{3}\right)^{-\frac{3}{x}} = y^3 + 3y.

  1. x1=1;x2=−1x_1 = 1; x_2 = -1.

  2. x=lg⁡3lg⁡2−lg⁡7x = \frac{\lg 3}{\lg 2 - \lg 7}.

  3. x=2x = 2.

  4. x=2x = 2. Hint: Reduce the equation to the form (12)x+(32)x=1\left(\frac{1}{2}\right)^x + \left(\frac{\sqrt{3}}{2}\right)^x = 1.

  5. x=2x = 2.

  6. x=3x = 3.

  7. x=4x = 4.

  8. x1,2=1±1+lg⁡2x_{1,2} = 1 \pm \sqrt{1 + \lg 2}. Hint: prodogarnified general partial equation in base 10.

  9. x1,2=12(log⁡32±log⁡322−4log⁡356153)x_{1,2} = \frac{1}{2} \left(\log_3 2 \pm \sqrt{\log_3^2 2 - 4 \log_3 \frac{56}{153}}\right). Instructions: Reduce the equation to the form 3x2=2x⋅153563^{x^2} = 2^x \cdot \frac{153}{56} and the pro-garnified general partial equation to base 3.

  10. x=±2x = \pm \sqrt{2}.

  11. x1=1,x2=4x_1 = 1, x_2 = 4.

  12. x1=1,x2=8x_1 = 1, x_2 = 8.

  13. x=2x = 2.

To the article “Written exam in mathematics at the mechanics of Moscow State University in 1970”

  1. π6+2πn⩽x⩽5π6+2πn\frac{\pi}{6} + 2\pi n \leqslant x \leqslant \frac{5\pi}{6} + 2\pi n, where x≠π4+2πn,x≠34π+2πnx \neq \frac{\pi}{4} + 2\pi n, x \neq \frac{3}{4} \pi + 2\pi n (n=0,±1,±2,…n = 0, \pm 1, \pm 2, \dots).

  2. x1=6,y1=63;x2=−6,y2=−63x_1 = \sqrt{6}, y_1 = \frac{\sqrt{6}}{3}; x_2 = -\sqrt{6}, y_2 = -\frac{\sqrt{6}}{3}.

  3. 3 min.

  4. AC=25rAC = 2\sqrt{5} r.

  5. SE=125−26sin⁡φSE = \frac{1}{2} \sqrt{5 - 2\sqrt{6}} \sin \varphi.

To the article “Written exam in physics at the Moscow Road Transport Institute”

Option No. 47

  1. sin⁡α=0,3\sin \alpha = 0, 3.

  2. θ=12∘C\theta = 12^\circ \text{C}.

  3. v=1,5⋅106 m/secv = 1, 5 \cdot 10^6 \text{ m/sec}.

To the article “Kinematika and connections” («Kvant» No. 2) *

  1. At point A, the projections of the velocities of the cylinder vAΥv_{A\Upsilon} and rod vACv_{AC} onto the direction AO′AO' (AO′⊥OAAO' \perp OA) coincide. The meaning is that the instantaneous axis of rotation of the cylinder passes through point BB. Therefore, vAΥv_{A\Upsilon} is directed perpendicular to ABAB and is equal to Ω⋅AB\Omega \cdot AB, where Ω\Omega is the angular velocity of rotation of the cylinder. Since

Ω=vr и AB=2rcos⁡α2, получим\Omega = \frac{v}{r} \text{ и } AB = 2r \cos \frac{\alpha}{2}, \text{ получим}

vAΥ=vr⋅2rcos⁡α2=2vcos⁡α2v_{A\Upsilon} = \frac{v}{r} \cdot 2r \cos \frac{\alpha}{2} = 2v \cos \frac{\alpha}{2}.

From the condition of equality of projections we have

vAC=vAΥcos⁡(π−α2)v_{AC} = v_{A\Upsilon} \cos \left(\pi - \frac{\alpha}{2}\right)

or

ωrcos⁡α2=2vcos⁡α2sin⁡α2,\omega r \cos \frac{\alpha}{2} = 2v \cos \frac{\alpha}{2} \sin \frac{\alpha}{2},

where

ωr2sin⁡2α2=ωr1−cos⁡α\frac{\omega r}{2 \sin^2 \frac{\alpha}{2}} = \frac{\omega r}{1 - \cos \alpha}.

  1. Since the speeds of the ends of the shatur are in the direction ABAB, we obtain (vA=ωrv_A = \omega r):

vcos⁡α=ωrcos⁡(π−α−β),v \cos \alpha = \omega r \cos (\pi - \alpha - \beta),

or

v=ωrsin⁡(α+β)cos⁡αv = \omega r \sin (\alpha + \beta) \cos \alpha.

Using the theorem of sines

sin⁡α=sin⁡β/l\sin \alpha = \sin \beta / l,

can be found

v=ωr1−(lrsin⁡α)2+lrsin⁡α=ωl⋅tgα×((rl)2−sin⁡2α+cos⁡α)v = \omega r \sqrt{1 - \left(\frac{l}{r} \sin \alpha\right)^2} + \frac{l}{r} \sin \alpha = \omega l \cdot tg \alpha \times \left(\sqrt{\left(\frac{r}{l}\right)^2 - \sin^2 \alpha} + \cos \alpha\right).

*) At figure to this problem in «Kvant» No. 2 the velocity vector vAΥv_{A\Upsilon} should be directed at an angle α2\frac{\alpha}{2} to the rod.

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Stamps, tying to N. E. Zhukovsky

The father of Russian aviation - this is how Vladimir Ilyich Lenin called the Russian scientist, founder of modern hydro- and aeromechanics Nikolai Egorovich Zhukovsky.

A number of Soviet stamps are associated with this scientist.

The first series of three stamps, bound to N. E. Zhukovsky, was issued in 1941 on the 20th anniversary of his death. On the first stamp of this series (by the artist P. Platonov) a portrait of the scientist is reproduced, and a vise of a smolet is depicted, since Zhukovsky associated a number of his works with the study of propeller thrust.

The second stamp (by artist R. Porshyan) reproduces a portrait of N. E. Zhukovsky against the background of the military academy that bears his name. The third stamp of the series (artist P. Platonov) depicts the scientist and his formula for determining the magnitude of the lifting force, published in 1906 in the work “On the addition of vinryakh”.

In January 1947, for the 100th anniversary of the birth of N. E. Zhukovsky, two stamps with his portrait (artist V. Zavyalov) were issued.

In August 1963, a series of stamps was issued related to domestic aviation parts. On one of the stamps in this series, a portrait of N. E. Zhukovsky is reproduced. On the initiative and under the leadership of Zhukovsky, one of the first wind tunnels in the world was built, and the artist V. Pimenov depicted a cross-section of the wind tunnel on the stamp next to the portrait of the scientist.

In his speech “On Aeronautics”, delivered in 1898, that is, long before the advent of the airplane, Zhukovsky said: “A man does not have wings and, in the ratio of the weight of his body to the weight of his muscles, is 72 times weaker than a bird…, but I think that he will win, relying not on the strength of his muscles, but on the strength of his size.” These words of the great scientist are shown on the postal block (artist A. Aksamit), which depicts the world’s first passenger supersonic aircraft TU-144. The block was issued in December 1969 in a series of stamps dedicated to the development of civil aviation.

The department is led by A. V. Altyks

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11

  1. A caterpillar is crawling along a tree. During the day it rises by 6 meters, and at night it drops by 4 meters. How many days will it take her to crawl to the top if the tree is 14 meters high?

  2. Out of 15 coins that look identical, one is counterfeit. It is unknown whether it is heavier or lighter than the others. How can you find out by doing no more than two weighings on a cup scale without mushrooms?

  3. The numbers 9 and 9 are cubes of integers. Which ones?

  4. Six matches lie on the table as shown in figure 1. You need to change their places, adhering to the following rules: a match can only be moved in the direction of its head to a free space, either by simply moving it or re-sticking it through no more than one match.

  5. Given a square sheet of paper. How can we cut it into four parts with straight lines (Fig. 2) so that they can be used to form a triangular paramid, no edges of which are equal (Fig. 3)?

The editor-in-chief is academician I.K. Kikoin.
The first deputy editor is Academician A. N. Kolmogorov.
Editorial collection: L. A. Artsimovich; M. I. Bashmakov; V. G. Boltyansky; I. N. Bronstein; N. B. Vasiliev; I. F. Ginzburg; V. G. Zubov; P. L. Kapitsa; V. A. Kirillin; V. A. Leshkovtsev (deputy editor-in-chief); V. P. Lishevsky; A. I. Markushevich; M. D. Millionshchikov; N. A. Patrieeva; N. Kh. Rozov; A. P. Savin; I. Sh. Slobodetsky; M. L. Smolyansky (deputy editor-in-chief); Y. A. Smorodinsky; V. A. Fabrikant.

Editorial Head L. V. Chernova
Chief artist A. I. Klimanov
Art editor T. M. Makarova
Technical editor G. N. Dyachenko
Proofreader M. L. Medvedskaya
Publishing house “Science”
Main editorial office of physical and mathematical literature
Tel. 234-08-11

Delivered on November 24, 1970.
Signed for publication on January 28, 1971.
Paper 70×100¹/₁₆. Phys. oven l. 4.
Condition-bake l. 5.20. Academic ed. l. 5.54. Type. 283,700.
T-02151
Price 30 kopecks. Order 1993.
Chekhov printing plant of the Glavpolinggrafprom of the Printing Committee under the Council of Ministers of the USSR, Chekhov, Moscow region.

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CROSSWORD

Horizontal:

  1. Characteristics of alternating current. 4. Location installation. 7. Unit of radioactivity. 9. Ice crust. 10. French mathematician. 11. An ancient Greek sage who discovered several geometric theorems. 13. Purposeful activity. 15. Measure of interaction between two bodies. 17. Limitation of the degree of freedom. 18. Actions part. 20. Thin layer. 22. Closed space. 23. Persuasion. 25. Geometic body. 27. Product of force and distance traveled. 31. Movement of electrons. 33. Repeatable process step. 34. Part of the day. 35. Mineral. 36. Stage in development. 38. Infinite amount. 41. Luminary. 43. Permissible deviation. 45. Outstanding French mathematician of the 18th - 19th centuries. 47. German mathematician, fruitfully working in the field of number theory. 49. Queue. 50. Operating conditions of the mechanism. 51. One of the founders of the theory of logarithms. 52. Development. 55. Closed convex line. 57. Instruction. 58. Hole for light. 59. Measuring device. 60. Beam. 61. Quantum of light. 62. Gas movement in the chimney.

Verticals:

  1. To get together is truly a work. 2. Electrode. 3. Frame. 5. Fractional part. 6. The subject of the science of glasiology. 7. Direction of movement. 8. Itchy object. 11. Exact science. 12. Part of a circle. 14. Switch. 15. Constellation. 17. Sound accompanying rubbing. 19. View of the cart. 21. Object in space. 24. Description of sea birches and currents. 25. Demonstration of the exhibit. 26. System of rules. 28. French physicist and astronomer of the 19th century. 29. International children’s camp. 30. Part of a jet engine. 31. Geometric body. 32. List of notation conditions. 37. Three of coordinate vectors. 39. Part of an atom. 40. Sound amplifier. 42. Auxiliary part of the word. 43. Flaw. 44. Physicist who first used mathematics to prove the rotation of the Earth. 46. ​​Line segment. 48. Elastic substance. 49. One of the founders of celestial mechanics. 52. Unit of division of the compass card. 53. Rope. 54. The set of rays of the visible spectrum. 55. Experiment. 56. Magnifying glass.