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Entrance written exam in mathematics at the Faculty of Computational Mathematics and Cybernetics of Moscow State University in 1970

Алимов Ш. А., Васильев Ф. П., Моденов В. П.

Rough automatic draft, low quality: expect mistakes and awkward wording. It will be replaced by a better translation. Original →

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Entrance written exam in mathematics at the Faculty of Computational Mathematics and Cybernetics of Moscow State University in 1970

Sh. A. Alimov, F. P. Vasiliev, V. P. Modenov

In the last two decades, the importance of mathematical sciences in the general system of human knowledge has increased immeasurably. The main reason for this is the development of computational mathematics. The creation of electronic computers resulted in a real revolution not only in computing capabilities and methods, but also in the very nature of the application of mathematics. It became clear that the quality and quantity of mathematical machines, their application and management systems are an integral part that determines the scientific and technical level of the country.

In this regard, the need arose to train mathematicians of a new specialization. In 1970, a new faculty was opened at the M.V. Lomonosov Moscow State University - the Faculty of Computational Mathematics and Cybernetics. In the same year, the first admission to this faculty was made.

At the written exam in mathematics, each applicant was given a variant of five problems, the solution of which was given 4 hours. To obtain a satisfactory grade, more than two problems had to be solved. An excellent mark was given for correctly solving all five problems.

As an example, let’s look at a typical version made up of tasks offered in a written exam.

Option 0

  1. Determine all real values ​​of aa, for each of which the equation cos⁡4x−(a−2)cos⁡2x−3(a+1)=0\cos^4 x - (a-2)\cos^2 x - 3(a+1) = 0
    have a solution, and find all these solutions.

  2. Solve the equation
    ∣1+log⁡13x∣=3+∣2−log⁡13x∣.\left| 1 + \log \frac{1}{3} x \right| = 3 + \left| 2 - \log \frac{1}{3} x \right|.

  3. From the city AA to the city BB, located at a distance of 240 km from AA, an autorus leaves at a speed of 40 km/h. At the same time, from BB to AA at a constant speed of vv km/h, the automaton exits. Half an hour after the car meets, before reaching the city AA, it turns back and at the same speed towards BB. Determine all the values ​​of vv at which autoroms come to BB more equally than autorus.

  4. In triangle ABCABC, the length of side BCBC is equal to the arithmetic mean of the lengths of sides ABAB and ACAC. Angle AA is equal to α\alpha. Find the angles BB and CC, assuming that B≥CB \geq C. Investigate at what values ​​of the angle α\alpha the problem has a solution.

  5. In a right circular cone with vertex SS, the angle between the height SOSO and the generator is equal to φ. On the base plane outside the cone, two points AA and BB are chosen so that the lines SASA and SBSB are mutually perpendicular and form angles with a height SOSO corresponding to α\alpha and β\beta. Calculate the angle between the generators along which the lateral surface of the cone intersects the triangles OSAOSA and OSBOSB.

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Analysis of problems

  1. Note that 0≤cos⁡2x≤10 \leq \cos^2 x \leq 1 for all xx. Then, using the substitution cos⁡2x=t\cos^2 x = t, the equation is reduced to the system:

{t2−(a−2)t−3(a+1)=0,0≤t≤1,\begin{cases} t^2 - (a - 2)t - 3(a + 1) = 0, \\ 0 \leq t \leq 1, \end{cases}

which has the solution t=a+1t = a + 1 at −1≤a≤0-1 \leq a \leq 0. Hence,

cos⁡2x=a+1,\cos^2 x = a + 1,

where −1≤a≤0-1 \leq a \leq 0. From here

x=±arccos⁡a+1+πnx = \pm \arccos \sqrt{a + 1} + \pi n

(n=0,±1,±2,… ;−1≤a≤0n = 0, \pm 1, \pm 2, \dots; -1 \leq a \leq 0).

Most of those who applied coped with this task. Some of the applicants incorrectly solved equation (1), mistakenly believing that arccos⁡(−a+1)=arccos⁡a+1\arccos (-\sqrt{a + 1}) = \arccos \sqrt{a + 1}, and lost the solution corresponding to equation cos⁡x=−a+1\cos x = -\sqrt{a + 1}. Some applicants did not indicate all values ​​of aa for which a solution to the problem exists.

  1. Range of acceptable values ​​of the unknown: x>0x > 0. Let’s rewrite the equation in the form

∣1+t∣=3+∣2−t∣,|1 + t| = 3 + |2 - t|,

where t=log⁡13xt = \log \frac{1}{3} x. Sequentially spaced intervals t≤−1,−1<t<2,t≥2t \leq -1, -1 < t < 2, t \geq 2. For t≥2t \geq 2 we have 1+t=3+t−2,1 + t = 3 + t - 2,

that is, equation (1) is then satisfied effectively for all t≥2t \geq 2. Next, we verify that equation (1) for t≤−1t \leq -1 and −1<t<2-1 < t < 2 has no solution. Thus, equation (1) is all t≥2t \geq 2. Hence log⁡13x≥2\log \frac{1}{3} x \geq 2, and taking into account the domain of definition of finding

0<x≤1/9.0 < x \leq 1/9.

Some applicants, noticing the same equation (2), wrote that the equation is then validly satisfied for all tt, without taking into account the constraint t≥2t \geq 2.

  1. Let t(u)t(u) be the time of movement of the automaton before the first meeting with the automaton. Since the automaton and the automaton left at the same time, the equality is true

40t+vt=240.40t + vt = 240.

(1)

The car surfaces through t+12(u)t + \frac{1}{2}(u) after leaving the city BB and therefore returned to BB through 2t+1(u)2t + 1(u). After the first meeting, the bus traveled vt(κm)vt(\kappa m), spending vt40(u)\frac{vt}{40}(u) on this journey. Thus, the Bus needed t+vt40(u)t + \frac{vt}{40}(u) for the entire journey from AA to BB. In order for the car to arrive at BB earlier than the bus, the inequality

2t+1<t+vt40.2t + 1 < t + \frac{vt}{40}.

(2)

According to the conditions of the surface automaton, before reaching the city AA. Since at the moment of the first meeting he is at a distance of 40t(κm)40t(\kappa m) from AA and during the receiving path v2\frac{v}{2}, then this condition comes to the inequality

v2<40t.\frac{v}{2} < 40t.

(3)

Combining (1), (2) and (3), we arrive at the system:

{40t+vt=240,2t+1<t+vt40,v2<40t.\begin{cases} 40t + vt = 240, \\ 2t + 1 < t + \frac{vt}{40}, \\ \frac{v}{2} < 40t. \end{cases}

From equation (1) we find t=240v+40t = \frac{240}{v + 40} and substitute it into inequalities (2) and (3). By jointly solving the resulting inequalities for vv, we find 56<v<12056 < v < 120.

Most applicants were able to complete equation (1) and inequality (2), although some of them replaced the < sign in (2)

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to the ≤ sign. The main share of errors was caused by conditions (3), since many applicants did not understand the need for this requirement and limited themselves to only solving the system obtained from (1) and (2).

  1. According to the condition

BC=AB+AC2.BC = \frac{AB + AC}{2}.

(1)

Using the sine theorem we find

AB=BCsin⁡Csin⁡α,AC=BCsin⁡Bsin⁡αAB = BC \frac{\sin C}{\sin \alpha}, \quad AC = BC \frac{\sin B}{\sin \alpha}

and substitute it into (1). We get

sin⁡B+sin⁡C=2sin⁡α,\sin B + \sin C = 2 \sin \alpha,

sin⁡B+C2cos⁡B−C2=sin⁡α.\sin \frac{B + C}{2} \cos \frac{B - C}{2} = \sin \alpha.

Because

B+C=π−α,B + C = \pi - \alpha,

(2)

then sin⁡B+C2=cos⁡α2,\sin \frac{B + C}{2} = \cos \frac{\alpha}{2}, and

cos⁡B−C2=2sin⁡α2.\cos \frac{B - C}{2} = 2 \sin \frac{\alpha}{2}.

(3)

Since by condition B≥CB \geq C and, in addition, 0<C<π,0<B<π0 < C < \pi, 0 < B < \pi, then

0≤B−C<π.0 \leq B - C < \pi.

(4)

Noting that sin⁡α2>0\sin \frac{\alpha}{2} > 0, from conditions (2), (3), (4) for determining BB and CC we have the system:

{B−C=2arccos⁡(2sin⁡α2),B+C=π−α.\begin{cases} B - C = 2 \arccos \left(2 \sin \frac{\alpha}{2}\right), \\ B + C = \pi - \alpha. \end{cases}

(5)

From (5) there is

{B=π−α2+arccos⁡(2sin⁡α2),C=π−α2−arccos⁡(2sin⁡α2).\begin{cases} B = \frac{\pi - \alpha}{2} + \arccos \left(2 \sin \frac{\alpha}{2}\right), \\ C = \frac{\pi - \alpha}{2} - \arccos \left(2 \sin \frac{\alpha}{2}\right). \end{cases}

Thus, for all values ​​of α\alpha for which there is a triangle ABCABC that satisfies all the conditions of the problem, the values ​​of the angles BB and CC are obtained from formulas (6).

Let us investigate at what values ​​of α\alpha the problem has a solution. From (6) it necessarily follows

∣2sin⁡α2∣≤1.\left| 2 \sin \frac{\alpha}{2} \right| \leq 1.

Since 0<α<π0 < \alpha < \pi, then hence 0<sin⁡α2≤120 < \sin \frac{\alpha}{2} \leq \frac{1}{2} and, therefore, 0<α≤π30 < \alpha \leq \frac{\pi}{3}.

For the found values ​​of α\alpha, the values ​​A=α,BA = \alpha, B and CC, determined by formulas (6), are positive and in total equal to π\pi. To prove this, it is enough to check conditions C>0C > 0 or 0<α≤π30 < \alpha \leq \frac{\pi}{3} and, as follows from (6), B≥C,α+B+C=πB \geq C, \alpha + B + C = \pi.

Let us show that C>0C > 0 or, according to (5),

π−α2>arccos⁡(2sin⁡α2).\frac{\pi - \alpha}{2} > \arccos \left(2 \sin \frac{\alpha}{2}\right).

(7)

Since cos xx monotonically kills on the segment 0≤x≤π0 \leq x \leq \pi, and the quantities π−α2\frac{\pi - \alpha}{2} and arccos (2sin⁡α2)\left(2 \sin \frac{\alpha}{2}\right) belong to this segment, then, calculating the cosine of both sides of inequality (7), we have cos⁡π−α2=sin⁡α2<2sin⁡α2.\cos \frac{\pi - \alpha}{2} = \sin \frac{\alpha}{2} < 2 \sin \frac{\alpha}{2}.

For 0<α<π30 < \alpha < \frac{\pi}{3} this inequality is true.

Repeating our reasoning in reverse order, we are convinced of the validity of the inequality C>0C > 0.

Thus, a triangle ABCABC with angles A=α,B≥CA = \alpha, B \geq C and satisfying the conditions of the problem, the values ​​of angles BB and CC are given by formulas (6), 0<α≤π30 < \alpha \leq \frac{\pi}{3}.

Many applicants, having received a system for determining BB and CC, were unable to solve it, and some wrote the answer in the form (6), but did not investigate at what values ​​of α\alpha the problem has a solution. Some applicants indicated only the case of an equilateral triangle

α=B=C=π3.\alpha = B = C = \frac{\pi}{3}.

  1. Let xx be the exclusive angle between the generators SA1SA_1 and SB1SB_1 along which the lateral surface of the cone intersects the triangles OSAOSA and OSBOSB (see Fig.ok): ⇒ASB=π2,⇒OSA=α,\Rightarrow ASB = \frac{\pi}{2}, \Rightarrow OSA = \alpha,

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Few applicants managed this task.

Note that formulas (1) and (2) express the relationships between the internal two-faceted angle and the flat angles at the vertex of the trihedral angle. In the general case, if A,BA, B and CC are interior two angles, the opposite of the corresponding plane angles α\alpha, β\beta and γ\gamma of a trihedral angle, then the valid formulas are:

cos⁡A=cos⁡α−cos⁡βcos⁡γsin⁡βsin⁡γ,\cos A = \frac{\cos \alpha - \cos \beta \cos \gamma}{\sin \beta \sin \gamma},

cos⁡B=cos⁡β−cos⁡αcos⁡γsin⁡αsin⁡γ,\cos B = \frac{\cos \beta - \cos \alpha \cos \gamma}{\sin \alpha \sin \gamma},

cos⁡C=cos⁡γ−cos⁡αcos⁡βsin⁡αsin⁡β,\cos C = \frac{\cos \gamma - \cos \alpha \cos \beta}{\sin \alpha \sin \beta},

which are derived in the same way as formula (1). These formulas can be useful in solving many stereometric problems.

In conclusion, we suggest that you independently solve the following option offered in the written exam.

Option 1

  1. Determine all real values ​​of aa for each of which the equation cos⁡4x−(a+2)cos⁡2x−(a+3)=0\cos^4 x - (a+2)\cos^2 x - (a+3)=0 has a solution, and find all these solutions.

  2. Solve the equation

∣1−log⁡1x∣+2=∣3−log⁡1x∣.|1 - \log_1 x| + 2 = |3 - \log_1 x|.

  1. From the city AA to the city BB, located at a distance of 105 km from AA, an autorus leaves at a constant speed vv km/h. 30 minutes later, following him out of AA at a speed of 40 km/h, a car leaves, which, having caught up with the bus on the way, turns back and moves at the same speed. Determine all values ​​of vv at which the car returns to AA later than the car arrives to BB.

  2. In triangle ABCABC, side BCBC serves as the base of a semicircle whose area is equal to the area of ​​triangle ABCABC. Angle AA is equal to α\alpha. Find the angles BB and CC, assuming that B≥CB \geq C. Investigate at what values ​​of the angle α\alpha the problem has a solution.

  3. In a right circular cone with vertex SS, the angle between generators SASA and SBSB is equal to α\alpha, and the angle between their projections onto the plane of the base is equal to β\beta. Calculate the angle between the bissertrices of angles OSAOSA and OSBOSB, where point OO is the center of the circle that served as the base of the cone.