Kvant
University Applicant's Workshop

Written exam in mathematics at the Faculty of Mechanics and Mathematics of Moscow State University in 1970

Колесников Н. Н.

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

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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

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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.