Kvant

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74

  1. Find all values ​​of xx belonging to the interval [−π;π][-\pi; \pi] and satisfying relations

∣sin⁡2x∣=cos⁡4x2−sin⁡4x2.|\sin 2x| = \cos^4 \frac{x}{2} - \sin^4 \frac{x}{2}.

Physics

Oral exam objectives

  1. A bullet flying at a certain speed penetrates into a solid barer to a depth of l=10l=10 cm. How deep into the same barer will a bullet with twice the speed go?

  2. A bus with a mass of m=4m=4 t starts from rest and on a path l=100l=100 m acquires a speed of v=20v=20 m/s. Find the friction coefficient if the traction force is F=10F=10 kN.

  3. A ball flying at a speed of v1=20v_1=20 m/s is thrown back by a racket strike in the opposite direction with a speed of v2=15v_2=15 m/s. Find what the change in momentum of the ball is if the change in its kinetic energy is equal to ΔE=8,75\Delta E=8,75 J.

  4. A car weighing m=2000m=2000 kg slows down and stops after t=4t=4 s, it will travel a distance of l=40l=40 m. What work is done by the traction force?

  5. A cylinder with a volume of V=0,2V=0,2 m³ contains helium under a pressure of p1=105p_1=10^5 Pa at a temperature of t1=17∘Ct_1=17^\circ\text{C}. After pumping helium, the pressure increased to p2=3⋅105p_2=3\cdot10^5 Pa, and the temperature became equal to t2=47∘Ct_2=47^\circ\text{C}. How much has the mass of helium increased? The universal gas constant is R=8,31R=8,31 J/(mol K), the molar mass of helium is =4⋅10−3=4\cdot10^{-3} kg/mol.

  6. It took τ1=15\tau_1=15 min to heat a certain amount of water from 0∘C0^\circ\text{C} to boiling temperature using an electric heater. After this, τ2=1\tau_2=1 hours 20 minutes were required to convert all the water into steam under the same conditions. Using these data, determine the specific heat of vaporization of water. Specific heat of water c=4200c=4200 J/(kg K).

  7. Two identical metal balls with charges q1=9,5⋅10−9q_1=9,5\cdot10^{-9} Kl and q2=54,5×10−9q_2=54,5\times10^{-9} Kl were in the air at some distance from each other. Then they were connected for a while and placed in kerosene in their original place. The force of interaction between the balls did not change. Find the dielectric permeability of kerosene.

  8. A resistor with a resistance of R=6R=6 Ohm is connected to a current source with internal resistance r=0,4r=0,4 Ohm. How many times does the power released in the external circuit change if another identical resistor is connected in series with the first one?

  9. The electric motor of a crane operates under a voltage of U=380U=380 V and consumes a current of I=20I=20 A. What is the efficiency of the motor if the crane lifts a load weighing m=1m=1 t uniformly to a height of h=19h=19 m in a time of t=50t=50 s?

  10. A ray of light falls from a certain liquid onto its interface with a vacuum. Angle of incidence a=30∘a=30^\circ. The reflected and refracted rays redistributed each other. Find the refractive index of this liquid.

Moscow Institute of Electronic Engineering

Mathematics

Written exam
Option 1

  1. Solve the equation

1x+1x−a=1x2−ax.\frac{1}{\sqrt{x}} + \frac{1}{\sqrt{x-a}} = \frac{1}{\sqrt{x^2-ax}}.

  1. Solve the equation

sin⁡x+cos⁡x=1+tgx.\sin x + \cos x = \sqrt{1 + \tg x}.

  1. In a regular quadrangular prism, the side of the base is aa. A plane is drawn through the diagonal of the lower base and the vertex of the upper base, intersecting two mixed side faces recognized as straight lines, the angle between which is equal to aa. Determine the volume of recognition.

  2. Calculate the sum of the roots of the equation

x2+2(a2−3a)x−(6a3−14a2+4)=0x^2 + 2(a^2 - 3a)x - (6a^3 - 14a^2 + 4) = 0

and find the values ​​of aa at which it takes on the most value.

  1. Solve the equation

(x−lg⁡x2)lg⁡22x−lg⁡x5−1=1.\left(x - \lg \frac{x}{2}\right)^{\lg^2 2x - \lg \frac{x}{5}} - 1 = 1.

Option 2

  1. Solve the equation

x+23x−a+3−x3x2+2ax−a2=3x+2x+a.\frac{x + 2}{3x - a} + \frac{3 - x}{3x^2 + 2ax - a^2} = \frac{3x + 2}{x + a}.

  1. Solve the equation

2cos⁡2x+4sin⁡(x+1)=4sin⁡xcos⁡1−sin⁡2x.\sqrt{2\cos^2 x + 4\sin(x + 1)} = \sqrt{4\sin x \cos 1 - \sin 2x}.

  1. Give a definition of the functions y=sin⁡xy = \sin x, explain its properties and the construction of its graph with justification.

  2. For what values ​​of aa is the smallest value of the function y=x2+(a−2)x−ay = x^2 + (a - 2)x - a on the interval [1; 3] equals -4?

  3. a) The side of the trigon is 9, the radius of the inscribed circle is 3, one of the angles is a right angle. Determine the area of ​​the trigon.

  1. The side of the trigon is 9, the radius of the inscribed circle is 3. What is the smallest value that the area of ​​the trigon can take?

The publication was prepared by V. A. Tonin

75

Moscow Institute of Physics and Technology
Matematika
Option 1

  1. 0<x<10 < x < 1.
  2. π4+πk,π6+2πk(k∈Z)\frac{\pi}{4} + \pi k, \frac{\pi}{6} + 2\pi k (k \in \mathbb{Z}).
  3. 73\frac{7}{\sqrt{3}}. Note. Let AK=a,∠KAO=φAK = a, \angle KAO = \varphi, point K′K' be the orthogonal projection of point KK onto line ACAC (Fig. 1). From the conditions of the problem it follows that OK′=1OK' = 1. Then
    {acos⁡φ=3,acos⁡(π3−φ)=2,\begin{cases} a \cos \varphi = 3, \\ a \cos \left(\frac{\pi}{3} - \varphi\right) = 2, \end{cases}
    whence tgφ=133tg \varphi = \frac{1}{3\sqrt{3}} and a=273a = 2\sqrt{\frac{7}{3}}.
  4. (0;52)(0; \frac{5}{2}). Note. The set MM is defined by the system of inequalities
    ∣a∣<1,(3a−4b+15)(7a−24b+35)<0.|a| < 1, \quad (3a - 4b + 15)(7a - 24b + 35) < 0.
    This set is a graption with vertices at points A(1;92),B(1;74),C(−1;76),D(−1;3)A\left(1; \frac{9}{2}\right), B\left(1; \frac{7}{4}\right), C\left(-1; \frac{7}{6}\right), D(-1; 3), and AB+CD=AD+BCAB + CD = AD + BC. Let the ordinate of the center of the circle be bb. Since the radius of the circle is equal to 1 and the straight line ADAD intersects the ordinate axis at the point (0;154)\left(0; \frac{15}{4}\right), then bb is the equation (154−b)cos⁡(arctg34)=1\left(\frac{15}{4} - b\right)\cos \left(\arctg \frac{3}{4}\right) = 1.
  5. 63432\frac{63}{4}\sqrt{\frac{3}{2}}. Solution. In a pentagon KK1K2K3K4KK_1K_2K_3K_4 (Fig. 2) K1K2cos⁡∠KK1M=72cos⁡(arctg55)=7414K_1K_2 \cos \angle KK_1M = \frac{7}{2} \cos (\arctg \sqrt{55}) = \frac{7}{4\sqrt{14}}. Note that KK1−K2K3=7414KK_1 - K_2K_3 = \frac{7}{4\sqrt{14}} is therefore (KK3)⊥(KK1)(KK_3) \perp (KK_1). Let AB=a,∠CKK1=φAB = a, \angle CKK_1 = \varphi, points K2′K'_2 and K3′K'_3 be orthogonal projections onto the plane ABCABC of points K2K_2 and K3K_3 (Fig. 3). Applying the theorem of sines to the triangle KCK1,AK2′K2′,KBK3′KCK_1, AK'_2K'_2, KBK'_3 (taking into account that ∠K1KK3′\angle K_1KK'_3 is a straight line), we obtain:
    142sin⁡(π3+φ)=a2sin⁡π3,\frac{\sqrt{14}}{2} \sin \left(\frac{\pi}{3} + \varphi\right) = \frac{a}{2} \sin \frac{\pi}{3},
    3814sin⁡(π3+φ)=AK2′sin⁡π3,\frac{3}{8} \sqrt{14} \sin \left(\frac{\pi}{3} + \varphi\right) = AK'_2 \sin \frac{\pi}{3},
    a2cos⁡φ=(a−AK2′)sin⁡(π6+φ).\frac{a}{2} \cos \varphi = (a - AK'_2) \sin \left(\frac{\pi}{6} + \varphi\right).
    From (1) and (2) we obtain that AK2′=38aAK'_2 = \frac{3}{8} a, taking this into account from (3) it follows that φ=arctg35\varphi = \arctg \frac{\sqrt{3}}{5}. Next we find a=32,K1K2′=722a = 3\sqrt{2}, K_1K'_2 = \frac{7}{2\sqrt{2}}. The height of the lines is 722\frac{7}{2\sqrt{2}}.
    Option 2
  6. (−1)nπ6+πn,n∈Z(-1)^n \frac{\pi}{6} + \pi n, n \in \mathbb{Z}.
  7. 2302\sqrt{30}. Note. Let AB=aAB = a. Using the bisector property, we obtain KC=713aKC = \frac{7}{13} a. Then KD=23013a,AK=1713aKD = \frac{2\sqrt{30}}{13} a, AK = \frac{17}{13} a.
  8. 4 hours.
  9. p≤2p \leq 2. Note. The tangent drawn to the graph of the function at point (x0;y0),x0≥0(x_0; y_0), x_0 \geq 0 intersects the ordinate axes at point (0;a)(0; a), where a=−3x02+3x02+21p22p+3a = -3x_0^2 + \sqrt{3}x_0^2 + \frac{21p^2}{2^p + 3}. The function a(x0)a(x_0) takes its greatest value at point 36\sqrt{\frac{\sqrt{3}}{6}}, it is equal to 14+21p22p+3\frac{1}{4} + \frac{21p^2}{2^p + 3}.
  10. AB=1013,MN=30AB = 10\sqrt{13}, MN = 30, the distance from point NN to plane ABCDABCD is 10141310\sqrt{\frac{14}{13}}. Solution. Let AB=a,AM=BK=b,∠ABN=φAB = a, AM = BK = b, \angle ABN = \varphi, planes ABCDABCD and KLMN intersect at angle φ\varphi (Fig. 4). We find BN=a2(sin⁡φ+cos⁡φ)BN = \frac{a}{2} (\sin \varphi + \cos \varphi). Then from the condition that the point NN is equidistant from the point BB and CC we obtain

76

Dem

gM=Fmcos⁡α=(2πT)2lcos⁡α≈3,8 m/c2.g_M = \frac{F}{m} \cos \alpha = \left( \frac{2\pi}{T} \right)^2 l \cos \alpha \approx 3,8 \text{ m/c}^2.

  1. The state of 1 mole of an ideal gas on the right side of the vessel at the initial moment is described by the Mendeleev-Clapeyron equation:

p1V1=RT1.p_1 V_1 = RT_1.

Here and henceforth, the index “1” will refer to the gas parameters on the right side of the vessel, and “2” - on the left. When we supply a small amount of heat ΔQ\Delta Q to the right side of the vessel, the parameters of the gas change, but will still satisfy the equation of state:

(p1+Δp1)(V1+ΔV1)=R(T1+ΔT1).(p_1 + \Delta p_1)(V_1 + \Delta V_1) = R(T_1 + \Delta T_1).

Subtracting one equality from the other term by term, we get:

p1ΔV1+V1Δp1+Δp1ΔV1=RΔT1.p_1 \Delta V_1 + V_1 \Delta p_1 + \Delta p_1 \Delta V_1 = R \Delta T_1.

As usual, assuming that in the process we are conducting all gas parameters change by small values ​​(ΔT1≪T1\Delta T_1 \ll T_1, Δp1≪p1\Delta p_1 \ll p_1, ΔV1≪V1\Delta V_1 \ll V_1), we can neglect the small term Δp1ΔV1\Delta p_1 \Delta V_1 compared to the others and write:

p1ΔV1+V1Δp1=RΔT1.p_1 \Delta V_1 + V_1 \Delta p_1 = R \Delta T_1.

We can obtain a similar expression for 1 mole of gas on the left side of the vessel:

p2ΔV2+V2Δp2=0.p_2 \Delta V_2 + V_2 \Delta p_2 = 0.

By definition of heat capacity

C=ΔQΔT.C = \frac{\Delta Q}{\Delta T}.

Using the first law of thermodynamics, for the gas on the right side of the container we can write:

ΔQ=CΔT1=ΔU1+p1ΔV1,\Delta Q = C \Delta T_1 = \Delta U_1 + p_1 \Delta V_1,

or

CΔT1=32RΔT1+p1ΔV1.C \Delta T_1 = \frac{3}{2} R \Delta T_1 + p_1 \Delta V_1.

Since the pressures in both parts of the vessel remain equal all the time: p1=p2=pp_1 = p_2 = p and Δp1=Δp2=Δp\Delta p_1 = \Delta p_2 = \Delta p, and the changes in volumes are related by the estimating relation ΔV1=−ΔV2\Delta V_1 = -\Delta V_2, from equalities (1) and (2) it is easy to obtain that

p1ΔV1=RΔT11+V1/V2,p_1 \Delta V_1 = \frac{R \Delta T_1}{1 + V_1/V_2},

and therefore

C=32R+R1+V1/V2.C = \frac{3}{2} R + \frac{R}{1 + V_1/V_2}.

At the moment when the piston divides the vessel in half, V1=V2V_1 = V_2, from where

78

Interpreting taking into account the initial conditions, we obtain
I=I0−E2Lt=±0,6E1CL−0,8E1Lt,I = I_0 - \frac{\mathcal{E}_2}{L} t = \pm 0,6 \mathcal{E}_1 \sqrt{\frac{C}{L}} - 0,8 \frac{\mathcal{E}_1}{L} t,
from where we find two solutions:

  1. −1,8E1CL=0,6E1CL−0,8E1Lt1⇒t1=3LC;-1,8 \mathcal{E}_1 \sqrt{\frac{C}{L}} = 0,6 \mathcal{E}_1 \sqrt{\frac{C}{L}} - 0,8 \frac{\mathcal{E}_1}{L} t_1 \Rightarrow t_1 = 3 \sqrt{LC};
  2. −1,8E1CL=−0,6E1CL−0,8E1Lt2⇒t2=3/2LC.-1,8 \mathcal{E}_1 \sqrt{\frac{C}{L}} = -0,6 \mathcal{E}_1 \sqrt{\frac{C}{L}} - 0,8 \frac{\mathcal{E}_1}{L} t_2 \Rightarrow t_2 = 3/2 \sqrt{LC}.
  1. The conditions of the problem are met by a system of two intrinsic lenses, each of which produces a real image (Fig. 10). Using the thin lens formula for lens J1J_1, we find f1=F1d1d1−F1f_1 = \frac{F_1 d_1}{d_1 - F_1} and notice
    Γ11=f1d1=F1d1−F1.\Gamma_{11} = \frac{f_1}{d_1} = \frac{F_1}{d_1 - F_1}.
    For lens J2J_2 we get
    d2=L−f1,f2=F2d2d2−F2d_2 = L - f_1, f_2 = \frac{F_2 d_2}{d_2 - F_2}
    and notice
    Γ12=F2d2−F2=F2L−d1F1d1−F1−F2.\Gamma_{12} = \frac{F_2}{d_2 - F_2} = \frac{F_2}{L - \frac{d_1 F_1}{d_1 - F_1} - F_2}.
    The total notification of a two-lens system is
    Γ1=Γ11⋅Γ12=F1d1−F1×F2L−d1F1d1−F1−F2.\Gamma_1 = \Gamma_{11} \cdot \Gamma_{12} = \frac{F_1}{d_1 - F_1} \times \frac{F_2}{L - \frac{d_1 F_1}{d_1 - F_1} - F_2}.
    In our case, it is convenient to rewrite this expression in the form:
    1Γ1=1Γ11⋅1Γ12=d1(L−(F1+F2))+F1F2F1F2−LF2.\frac{1}{\Gamma_1} = \frac{1}{\Gamma_{11}} \cdot \frac{1}{\Gamma_{12}} = \frac{d_1(L - (F_1 + F_2)) + F_1 F_2}{F_1 F_2} - \frac{L}{F_2}.
    After rearranging the lenses, the system notification is given by a similar expression:
    1Γ2=1Γ21⋅1Γ22=d1(L−(F2+F1))+F2F1F2F1−LF1.\frac{1}{\Gamma_2} = \frac{1}{\Gamma_{21}} \cdot \frac{1}{\Gamma_{22}} = \frac{d_1(L - (F_2 + F_1)) + F_2 F_1}{F_2 F_1} - \frac{L}{F_1}.
    From here
    1Γ1−1Γ2=L(1F1−1F2).\frac{1}{\Gamma_1} - \frac{1}{\Gamma_2} = L \left( \frac{1}{F_1} - \frac{1}{F_2} \right).
    Since the optical power of the lens is D=1/FD = 1/F, then
    D2−D1=1L(1Γ1−1Γ2)=3 дитр.D_2 - D_1 = \frac{1}{L} \left( \frac{1}{\Gamma_1} - \frac{1}{\Gamma_2} \right) = 3 \text{ дитр.}
    Moscow State Pedagogical Institute named after. V. I. Lenina
    Matematika
    Option 1
  2. 25 km/h.
  3. x1=π4(4k+1),x2=π(2l+1),x3=π4(8m+3),k,l,m∈Z.x_1 = \frac{\pi}{4} (4k + 1), x_2 = \pi (2l + 1), x_3 = \frac{\pi}{4} (8m + 3), k, l, m \in \mathbb{Z}.
  4. ]−∞;0)∪[1/2;+∞].] - \infty; 0) \cup [^1/2; + \infty].
  5. ymax=79/25.y_{\text{max}} = 79/25.
  6. a2(6+15)/3.a^2(\sqrt{6} + \sqrt{15})/3.
    Option 2
  7. ymax=16;ymin=−4.y_{\text{max}} = 16; y_{\text{min}} = -4.
  8. 5/2, 6, 13/2.
  9. [−2;1].[-2; 1].
  10. (−1;0)∪(4;+∞).(-1; 0) \cup (4; + \infty).
  11. ±π/6;±π/2.\pm \pi/6; \pm \pi/2.
    Physics
  12. l′=4l=40 см.l' = 4l = 40 \text{ см}.
  13. μ=Fmg−v22lg=0,05.\mu = \frac{F}{mg} - \frac{v^2}{2lg} = 0,05.
  14. ΔP=2ΔE/(v1−v2)=3,5 кг⋅м/с.\Delta P = 2\Delta E/(v_1 - v_2) = 3,5 \text{ кг} \cdot \text{м}/\text{с}.
  15. A=2ml2/t2=4⋅105 Дж.A = 2ml^2/t^2 = 4 \cdot 10^5 \text{ Дж}.
  16. Δm=MVR(p2T2−p1T1)=0,06 кг.\Delta m = \frac{MV}{R} \left( \frac{p_2}{T_2} - \frac{p_1}{T_1} \right) = 0,06 \text{ кг}.
  17. r=c(tk−t0)t2/t1≈2,2⋅106 Дж/кгr = c(t_k - t_0)t_2/t_1 \approx 2,2 \cdot 10^6 \text{ Дж}/\text{кг} (here tk=100∘Ct_k = 100^\circ \text{C} is the boiling point, t0=0∘Ct_0 = 0^\circ \text{C} is the initial temperature of water).
  18. ε=(q1+q2)2/(4q1q2)≈2.\varepsilon = (q_1 + q_2)^2/(4q_1q_2) \approx 2.
  19. Power will decrease by n=(r+2R)2/(2(r+R)2)≈1,9 раз.n = (r + 2R)^2/(2(r + R)^2) \approx 1,9 \text{ раз}.
  20. η=mgh/(UIt)≈50%.\eta = mgh/(UIt) \approx 50 \%.
  21. n=ctgα=1,73.n = \text{ctg} \alpha = 1,73.

Moscow Institute of Electronic Engineering
Matematika
Option 1

  1. x=(a+1)2/4 при ∣a∣<1x = (a + 1)^2/4 \text{ при } |a| < 1. For other a there are no roots.
  2. 2πk;π4+2πk;−π4+πk(k∈Z).2\pi k; \frac{\pi}{4} + 2\pi k; -\frac{\pi}{4} + \pi k (k \in \mathbb{Z}).
  3. V=a32cos⁡a/(2sin⁡α2).V = a^3 \sqrt{2\cos a}/(2 \sin \frac{\alpha}{2}).
  4. a=2a = 2. Note. The sum of the roots is 2(3a−a2)2(3a - a^2) subject to D≥0.D \geq 0.
  5. [0,5];5[0, 5]; 5. Note. x−lg⁡x2>1x - \lg \frac{x}{2} > 1 for all x>0x > 0, since the function f(x)=x−lg⁡x2f(x) = x - \lg \frac{x}{2} has a minimum at the point x0=lg⁡ex_0 = \lg e, and f(x0)=lg⁡2elge>1.f(x_0) = \lg \frac{2e}{lg e} > 1.
    Option 2
  6. [−1;+(4a+3)/8][-1; +(4a + 3)/8] at a≠−3,−9/4,−1/4,1;[−9/8]a \neq -3, -9/4, -1/4, 1; [-9/8] at a=−3;[−1]a = -3; [-1] at a=−9/4a = -9/4 and a=−1/4;[7/8]a = -1/4; [7/8] at a=1.a = 1.
  7. π2+2πk(k∈Z)\frac{\pi}{2} + 2\pi k (k \in \mathbb{Z}). Note. After squaring, we obtain after simplifications two equations: cos⁡x=0\cos x = 0 and cos⁡x+sin⁡x=−2sin⁡1\cos x + \sin x = -2 \sin 1; the second of them has no roots, since

80

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Preparation number:
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Registration number:
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