Kvant
Kvant 1970, No. 8

Kvant 1970, No. 8 · Pages

Sheet 10

p. 8Transcribed from the scan · Rough draft translation, low quality

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Problem 6. Prove that the vertices of a polyorganic can be divided into black and white poppies so that no two vertices of a monozoche tsempa are adjacent moeda and molko moeda, when each face of the polyorganic has an even number of sides.

e is also indicated. To prove it, it is enough to take any vertex and declare it white, its neighbors black, etc. It is necessary to prove that no contradictions arise in this case, i.e., that in every closed broken line composed of the edges of a polyorganic there is an even number of links.

Let’s return to the polyorganic MM with colored vertices. Since MM three faces converge at each vertex, the number of white vertices is equal to the number of black vertices. Let us select some of its black vertices (one, two or all) and cut them off using planes. Each vertex is a segment of one plane, intersecting only those edges that emanate from this vertex, and not containing any vertices MM. We denote the resulting polyorganic by M′M'. It differs from MM in that it has, together with some black vertices, triangular faces. Let us prove that the polyorganic M′M' is absolutely indescribable.

Let us assume that the polyorganic M′M' or another polyorganic having the same structure is inscribed in a sphere. Let us select three faces that correspond to those faces of the polyorganic MM that converge at one trimmed vertex. These three faces are pairwise adjacent, the vertex of the truncated trihedral angle obviously lies outside the sphere, since the polyorganic is inscribed, therefore the sum of the relative angles for them is less than l. Let us assign to each edge of the polyorganic MM a relative angle with the corresponding edge of the polyorganic M′M'. Then the sum of these assigned angles for all white and all unselected black vertices is equal to l, and for selected black vertices it is strictly less than l. As in the proof of Steinitz’s theorem, we write out these equalities and inequalities, multiply the sums corresponding to the white vertices by -1 and add them. The result should be strict inequality. However, on the left side we get zero, or each of the assigned angles is included in the sum once for a white vertex, and once for a black one. On the right side we will also get zero, since the number of white vertices is equal to the number of black ones. The resulting contradiction (0<00<0) proves our statement.

Exactly the same reasoning can be verified if the marked vertices are defined not by one, but by several planes, as long as the faces converging in them remain pairwise adjacent and do not converge at one vertex.

This method can also obtain other sufficient conditions. Now some necessary conditions have become known for a polyorganic to be absolutely indescribable, but in general the problem has not yet been solved.

The relative angle method allows us to solve other interesting problems.

Problem 7. Let three faces converge at each vertex of the polyorganic MM, and let each face have the same number of sides. Prove that if all but one of the vertices of the polyorganic MM lie on the sphere, then the polyorganic MM is inscribed.

Indicated and e. Use problem 6. Do not miss this unpleasant possibility: edges emanating from a vertex that does not lie on the sphere touch the sphere.

Similar, but more complex.

Problem 8. Let all the vertices of the polyorganic MM be divided into black and white, as described in Problem 5, and the number of black vertices is equal to the number of white ones. Prove that if all but one of the vertices of the polyorganic MM lie on the sphere, then the polyorganic MM is inscribed.

Thus, if the vertices can be divided into black and white, as described in task 5, then either the polyorganic is absolutely indescribable or satisfies task 8, i.e.

Sheet 17

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First, the entire first row and first two columns are filled. Further filling of the table is carried out according to the following scheme:

| an−2a_{n-2} | an−1a_{n-1} | ana_n |
| :— | :— | :— |
| pn−2p_{n-2} | pn−1p_{n-1} | |

  1. column ∣pn−1qn−1∣\left| \frac{p_{n-1}}{q_{n-1}} \right| multiplied by ana_n,

  2. add the previous one to the resulting column.

The same scheme is recommended to be used if you need to calculate the value of the entire continued fraction: the last column ∣psqs∣\left| \frac{p_s}{q_s} \right| will provide a sufficient answer.

Practice filling out the table for the continued fraction [0; 3, 14, 1, 2, 5]

| 0 | 3 | 14 | 1 | 2 | 5 |
| :— | :— | :— | :— | :— | :— |
| 0 | 1 | 14 | 15 | 44 | 235 |
| 1 | 3 | 43 | 46 | 135 | 721 |

  1. Difference of adjacent suitable fractions. The step from the nnth suitable fraction to the next one is represented by the nnth fraction and is designated Δn\Delta_n:

Δn=pn+1qn+1−pnqn=pn+1qn−pnqn+1qnqn+1=Dnqnqn+1,\Delta_n = \frac{p_{n+1}}{q_{n+1}} - \frac{p_n}{q_n} = \frac{p_{n+1} q_n - p_n q_{n+1}}{q_n q_{n+1}} = \frac{D_n}{q_n q_{n+1}},

where DnD_n denotes numeric

Dn=pn+1qn−pnqn+1.D_n = p_{n+1} q_n - p_n q_{n+1}.

Let us lower the indices yy pn+1p_{n+1} and qn+1q_{n+1} according to formulas (3.2):

Dn=(pnan+1+pn−1)qn−pn(qnan+1+qn−1)=−(pnqn−1−pn−1qn).D_n = \left( p_n a_{n+1} + p_{n-1} \right) q_n - p_n \left( q_n a_{n+1} + q_{n-1} \right) = -\left( p_n q_{n-1} - p_{n-1} q_n \right).

The expression in parentheses is the same type as (**), but all indices are by one

less. So it represents Dn−1D_{n-1}:

Dn=−Dn−1.D_n = -D_{n-1}.

This recurrence relationship allows you to lower the index to zero:

Dn=−Dn−1=Dn−2=−Dn−3=⋯=(−1)nD0.D_n = -D_{n-1} = D_{n-2} = -D_{n-3} = \dots = (-1)^n D_0.

For complete success, all that remains is to directly calculate D0D_0:

D0=p1q0−p0q1=(a1a0+1)⋅1−a0a1=1.D_0 = p_1 q_0 - p_0 q_1 = (a_1 a_0 + 1) \cdot 1 - a_0 a_1 = 1.

Hence,

Dn=pn+1qn−pnqn+1=(−1)n,D_n = p_{n+1} q_n - p_n q_{n+1} = (-1)^n,

(4.1) and by formula (*)

Δn=pn+1qn+1−pnqn=(−1)nqnqn+1.\Delta_n = \frac{p_{n+1}}{q_{n+1}} - \frac{p_n}{q_n} = \frac{(-1)^n}{q_n q_{n+1}}.

  1. Comparing the one with the odd number greater than the neighboring fractions (previous and subsequent). What suitable odd-numbered fraction is smaller than its neighboring fractions.

When applying this formulation to the zero and last suitable fractions, we must take into account that each of them has only one neighboring fraction.

The validity of this property is immediately clear from formula (4.2).

Property 1 means that successive suitable fractions are alternately greater and lesser.

Property 2. Differences between adjacent fractions in abscimal values ​​cancel out (meaning: as the number increases).

Let’s compare:

∣Δn∣=1qnqn+1,|\Delta_n| = \frac{1}{q_n q_{n+1}},

∣Δn+1∣=1qn+1qn+2.|\Delta_{n+1}| = \frac{1}{q_n+1 q_{n+2}}.

We have qn+2>qnq_{n+2} > q_n. This means that the second fraction has a larger denominator, but it itself is smaller:

∣Δn+1∣<∣Δn∣.|\Delta_{n+1}| < |\Delta_n|.

  1. Irreducibility of suitable fractions. All suitable fractions are irreducible.

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Recall that the numerators and denominators of suitable fractions are formed according to formulas (3.1). Let us assume that the fraction pnqn\frac{p_n}{q_n} is reducible, i.e. its numerator and denominator have a common factor λ\lambda, different from one:

pn=λpn′,qn=λqn′.p_n = \lambda p_n', \quad q_n = \lambda q_n'.

Then formula (4.1) gives

λ(pn+1qn′−pn′qn+1)=(−1)n.\lambda (p_{n+1} q_n' - p_n' q_{n+1}) = (-1)^n.

We are stuck with an absurd equality: the left side is divisible by λ\lambda, but the right is not. This means that the fraction pnqn\frac{p_n}{q_n} is irreducible.

III. Introduction of infinite fractions

  1. The meaning of an infinite continued fraction. The principle of nested segments will serve us as a key that will open the meaning of an infinite continued fraction. Let us recall a similar situation: how to extrude an infinite decimal fraction? An infinite decimal fraction can be considered as a shorthand notation of a sequence of nested segments: successive roundings with a deficit give the left ends of these segments, and with an excess - the right ones. What is the meaning of the statement that 2\sqrt{2} is expressed as an infinite decimal fraction

2=1,4142...?\sqrt{2} = 1,4142...?

This means that

1<2<2,1 < \sqrt{2} < 2,

1,4<2<1,5,1,4 < \sqrt{2} < 1,5,

1,41<2<1,42,1,41 < \sqrt{2} < 1,42,

There is a single number that satisfies all these inequalities at once. This is 2\sqrt{2}.

Having symbolic infinite continued fractions

[a0;a1,a2,… ],[a_0; a_1, a_2, \dots],

it is possible to form an infinite sequence of finite continued fractions

a0,[a0;a1],[a0;a1,a2],…,a_0, [a_0; a_1], [a_0; a_1, a_2], \dots,

[a0;a1,a2,…,an],…,[a_0; a_1, a_2, \dots, a_n], \dots,

(**)

which can be written as suitable fractions

p0q0,p1q1,p2q2,…,pnqn,…\frac{p_0}{q_0}, \frac{p_1}{q_1}, \frac{p_2}{q_2}, \dots, \frac{p_n}{q_n}, \dots

(***)

These suitable fractions determine the sequence of nested segments

[p0q0,p1q1],[p2q2,p1q1],[p2q2,p3q3],\left[ \frac{p_0}{q_0}, \frac{p_1}{q_1} \right], \left[ \frac{p_2}{q_2}, \frac{p_1}{q_1} \right], \left[ \frac{p_2}{q_2}, \frac{p_3}{q_3} \right],

[p4q4,p3q3],…\left[ \frac{p_4}{q_4}, \frac{p_3}{q_3} \right], \dots

Each next segment is in the previous one (Fig. 4) and their lengths tend to zero (see formulas (4.2)). Therefore, there is a number α\alpha that belongs to all segments. It belongs to the value of an infinite continued fraction**).

This definition can be expressed in another way. Here are two options.

  1. The value of an infinite continued fraction lies between any two adjacent suitable fractions.

  2. The value of a .befinite continued fraction is greater than the doi of a suitable fraction

(*) Marks 0, 1, 2, … on figure 4 read the numbers of suitable fractions.

**) This defines the term “fitting fraction”, it “fits” closer and closer to the point α\alpha.

Sheet 19

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bi with an even number and less than every suitable fraction with an odd number (all this is clearly visible on figure 5).

It is important to understand that any of these formulations define a singular number.

It is easy to show (do this) that if the irrational number α\alpha is decomposed into an integer fraction, then successive suitable fractions are alternately smaller and larger than α\alpha. It follows that this number α\alpha is the value that is now assigned to the infinite whole fraction (the unity of the point belonging to all segments!). Others are allowed to write

α=[a0;a1,a2,… ].\alpha = [a_0; a_1, a_2, \dots].

It is now clear that each suitable fraction can be considered an approximation of the whole fraction. The larger the number, the more accurate the approximation.

Almost the same thing was said about the approximation of a finite integer fraction by suitable fractions. The only difference is that in the case of an infinite whole fraction, there is no last good fraction, and significant, no good fraction gives the powerful value of the whole fraction.

For infinite integer fractions, the sign of equality is preserved («Kvant», No. 1, p. 22). Let’s formulate it like this:

  1. Two infinite integer fractions [a0;a1,a2,…,an,… ][a_0; a_1, a_2, \dots, a_n, \dots] and [b0;b1,b2,…,bn,… ][b_0; b_1, b_2, \dots, b_n, \dots] are equal to each other if and only if their corresponding elements coincide, i.e. an=bna_n = b_n with n=0,1,2,…n=0, 1, 2, \dots.

  2. An infinite whole fraction cannot be equal to a finite fraction.

  1. And the approximation of a suitable fraction and fractions. Does the reader remember when we set out on this long voyage? We are looking for an advantageous way to approximate real numbers (including rational numbers) to rational ones.

What’s happened! Is this a typo? Is it possible to approximate rational numbers by rational numbers?

Can. For example,

61877425≈56.\frac{6187}{7425} \approx \frac{5}{6}.

In this example, we replace a cumbersome rational number with a simpler one.

Once we’ve become familiar with whole fractions, a natural project that comes up is to factor the number α\alpha into a whole fraction and count successive suitable fractions as approximations of that number. In other words, truncate the whole fraction, discarding all elements starting from some, and take the remaining truncated fraction as an approximate value of the full whole fraction. This is exactly what we do by truncating the decimal fraction and leaving only the desired number of francs after the decimal point.

In order to accept or reject this project, we need to find out what kind of error we allow by replacing the number α\alpha with a suitable fraction, i.e., assuming

α≈pnqn.\alpha \approx \frac{p_n}{q_n}.

In all further reasoning it is assumed that the fraction pnqn\frac{p_n}{q_n} is not zero and not the last. For n=0n=0 the use of whole fractions does not provide anything new compared to the use of decimals, and the case n=sn=s is uninteresting since we get α=α\alpha=\alpha and the error is zero.

Sheet 21

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cutting is ∣Δn∣=1qnqn+1|\Delta_n| = \frac{1}{q_n q_{n+1}}. The point α\alpha may be an interior point of that segment, or may be the same as pn+1qn+1\frac{p_{n+1}}{q_{n+1}} (if α\alpha is rational and pn+1qn+1\frac{p_{n+1}}{q_{n+1}} is the last matching fraction). Thus,

∣α−pnqn∣⩽∣Δn∣.(10.1)\left| \alpha - \frac{p_n}{q_n} \right| \leqslant |\Delta_n|. \tag{10.1}

Let pq−какая-нибудь дробь\frac{p}{q} - \text{какая-нибудь дробь}, whose denominator is less than qnq_n and thereby less than qn+1q_{n+1}:

q<qn<qn+1.(10.2)q < q_n < q_{n+1}. \tag{10.2}

Since the suitable fractions are irreducible, it follows from inequalities (10.2) that

pq≠pnqn,pq≠pn+1qn+1.\frac{p}{q} \neq \frac{p_n}{q_n}, \quad \frac{p}{q} \neq \frac{p_{n+1}}{q_{n+1}}.

It’s clear that

∣pq−pnqn∣=∣pqn−pn∣qqn⩾1qqn,\left| \frac{p}{q} - \frac{p_n}{q_n} \right| = \frac{|pq_n - p_n|}{qq_n} \geqslant \frac{1}{qq_n},

∣pq−pn+1qn+1∣=∣pqn+1−pn+1∣qqn+1⩾1qqn+1.\left| \frac{p}{q} - \frac{p_{n+1}}{q_{n+1}} \right| = \frac{|pq_{n+1} - p_{n+1}|}{qq_{n+1}} \geqslant \frac{1}{qq_{n+1}}.

These inequalities are still successful if we replace qq with the greater value of qn+1q_{n+1} or qnq_n:

∣pq−pnqn∣>1qn+1qn=∣Δn∣,\left| \frac{p}{q} - \frac{p_n}{q_n} \right| > \frac{1}{q_{n+1} q_n} = |\Delta_n|,

∣pq−pn+1qn+1∣>1qnqn+1=∣Δn∣.\left| \frac{p}{q} - \frac{p_{n+1}}{q_{n+1}} \right| > \frac{1}{q_n q_{n+1}} = |\Delta_n|.

The meaning of the last two inequalities is as follows: the fraction pq\frac{p}{q} is removed from each end of the segment [pnqn,pn+1qn+1]\left[ \frac{p_n}{q_n}, \frac{p_{n+1}}{q_{n+1}} \right] at a distance greater than the length of this segment ∣Δn∣|\Delta_n|. Delaying the segment ∣Δn∣|\Delta_n| (Fig. 6) from points pnqn\frac{p_n}{q_n} and pn+1qn+1\frac{p_{n+1}}{q_{n+1}} to the left and right, we obtain a forbidden zone ABAB, in which the fraction pq\frac{p}{q} cannot be located (points AA and BB are also forbidden). It is now clear that pq\frac{p}{q} is a worse approximation for the number α\alpha than pnqn\frac{p_n}{q_n}. In fact,

∣α−pnqn∣⩽∣Δn∣,\left| \alpha - \frac{p_n}{q_n} \right| \leqslant |\Delta_n|,

∣α−pq∣>∣Δn∣.\left| \alpha - \frac{p}{q} \right| > |\Delta_n|.

Note that the converse theorem is not true, i.e., there are fractions that do not serve as suitable ones and yet give a better approximation for the number α\alpha than any fraction with a smaller value. For example, from the table on page 18 («Kvant», No. 1) it is clear that the approximations of the numbers 19/619/6, 165\frac{16}{5} and 134\frac{13}{4} have this property. Therefore, the theorem proved does not mean that suitable fractions are better than others for approximating real numbers. But here are two horizontal strong theorems, which we will present without proof.

For a suitable fraction, the benefit coefficient ∗^*) λ=12∣qnα−pn∣\lambda = \frac{1}{2|q_n \alpha - p_n|} is greater than for any other fraction with a smaller value.

Finally, the most surprising thing: the converse theorem is also true, i.e. it has such a large coefficient of profitability ∗^*) «Kvant», No. 1, p. 18.

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SUBSCRIBE TO THE MAGAZINE ANNOUNCED
“QUANT” FOR 1971

«Kvant» is a popular science physics and mathematics journal of the USSR Academy of Sciences and the USSR Academy of Pedagogical Sciences. It is intended primarily for schoolchildren in grades 8–10. Among its readers are many teachers, especially those who teach clubs or elective classes in physics and mathematics, as well as students of pedagogical institutes. Older physics and mathematics lovers also read it with interest.

«Kvant» publishes articles and notes devoted to modern problems of science, as well as many different materials that expand and deepen school courses in physics and mathematics.

It contains a wealth of information for those preparing to enter college.

The regular sections of the magazine - “Quent’s Problem Book”, “Quant’s Laboratory”, “Applicant’s Workshop” - contain many interesting tasks and home experiments.

«Kvant» provides its readers with regular information about new books, about the work of physics and mathematics schools and clubs.

Among our authors are famous Soviet and foreign scientists, young scientists, and teachers. Schoolchildren can also report on their first discoveries, laboratory work or independently constructed devices on the pages of our magazine.

Subscription starts on September 1st. The price of the room is 30 kopecks. The cost of an annual subscription is 3 rubles 60 kopecks. Subscription index 70465.

Sheet 35

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One inductive method for proving inequalities

S. T. Berkolaiko,
S. B. Skating rink

The arithmetic mean and geometric mean theorem, which states that for any positive x1,x2,…,xnx_1, x_2, \dots, x_n the inequality

1n(x1+x2+⋯+xn)≥x1x2…xn,\frac{1}{n} (x_1 + x_2 + \dots + x_n) \geq \sqrt{x_1 x_2 \dots x_n},

is one of those mathematical facts whose proofs are less known than their formulations. (Other examples of this kind: in arithmetic - the only factorization of a number into prime factors; in geometry - the theorem that the altitudes of a triangle intersect at one point.) Meanwhile, there are many different ways to prove this remarkable inequality, including elementary ones (for example, in [1] (solution to problem 268) 3 elementary proofs are given, and at the beginning of [5] 12 different proofs are proposed). This note provides another short proof by induction, which also works for other positive inequalities.

We must prove that

x1+⋯+xn≥n(x1…xn)1nx_1 + \dots + x_n \geq n (x_1 \dots x_n)^{\frac{1}{n}}

(1)

for all integers n≥2n \geq 2 and positive x1,…,xnx_1, \dots, x_n.

For n=2n=2 this inequality looks like this:

x1+x2≥2(x1x2)12x_1 + x_2 \geq 2 (x_1 x_2)^{\frac{1}{2}}

(2)

and immediately follows from the obvious inequality

(x112−x212)2≥0.(x_1^{\frac{1}{2}} - x_2^{\frac{1}{2}})^2 \geq 0.

Let us assume that inequality (1) is true for n=kn=k and prove it for n=k+1n=k+1.

To do this, consider the following expression:

x1+x2+⋯+xk+xk+1+(k−1)(x1x2…xk+1)1k+1.x_1 + x_2 + \dots + x_k + x_{k+1} + (k-1) (x_1 x_2 \dots x_{k+1})^{\frac{1}{k+1}}.

Divide this sum into two, kk terms, and estimate which of them, applying inequality (1) for n=kn=k:

x1+x2+⋯+xk≥k(x1…xk)1k,x_1 + x_2 + \dots + x_k \geq k (x_1 \dots x_k)^{\frac{1}{k}},

xk+1+(k−1)(x1…xk+1)1k+1≥k(xk+1x1k−1k+1…xk+1k−1k+1)1k.x_{k+1} + (k-1) (x_1 \dots x_{k+1})^{\frac{1}{k+1}} \geq k (x_{k+1} x_1^{\frac{k-1}{k+1}} \dots x_{k+1}^{\frac{k-1}{k+1}})^{\frac{1}{k}}.

We consider (k−1)(x1x2…xk+1)1k+1(k-1) (x_1 x_2 \dots x_{k+1})^{\frac{1}{k+1}} as the sum of (k−1)(k-1) identical terms (x1x2…xk+1)1k+1(x_1 x_2 \dots x_{k+1})^{\frac{1}{k+1}}.

Sheet 38

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In words, prove the required inequality only for n=2n=2.

And if we prove the upward convexity of the function lg⁡x\lg x (which is evidence of the proof of inequality (2)), then from our theorem, as one of the special cases, we obtain a theorem about the arithmetic mean and the geometric mean:

lg⁡(x1+…+xnn)≤lg⁡x1+…+lg⁡xnn,\lg \left( \frac{x_1 + \ldots + x_n}{n} \right) \leq \frac{\lg x_1 + \ldots + \lg x_n}{n},

i.e.

lg⁡(x1+…+xnn)≤lg⁡(x1…xn)1n,1n(x1+…+xn)≤(x1…xn)1n.\lg \left( \frac{x_1 + \ldots + x_n}{n} \right) \leq \lg \left( x_1 \ldots x_n \right)^{\frac{1}{n}}, \quad \frac{1}{n} \left( x_1 + \ldots + x_n \right) \leq \left( x_1 \ldots x_n \right)^{\frac{1}{n}}.

In conclusion, we will provide a list of books in which you can read other proofs of the arithmetic mean and geometric mean theorem.

[1] D. O. Shklyarsky, N. N. Chentsov, I. M. Yaglom, Selected problems and theorems of elementary mathematics, Part I, M., “Nauka”, 1965.

Consider the first of three proofs given in this book (“By Reverse Indication”).

[2] Kretschmar, Algebra Problem Book. M., “Science”, 1968.

[3] E. Beckenbach and R. Belman, Introduction to Inequalities, M., “Mir”, 1965.

[4] G. G. Hardy, D. E. Littelwood, G. Polyana, Inequalities, IL, 1948.

[5] E. Beckenbach and R. Belman, Inequalities, M., “World”, 1965.

Exercises

  1. What inequality results if we apply the theorem to the function y=x2y=x^2? Try to prove this inequality directly.

  2. Derive from the general theorem inequalities a)-e). What functions need to be proven to be convex for this?

  3. Come up with a few more examples of convex functions and write down the inequality that follows from Theorem 1 when applied to these functions.

  4. The function ff is defined on the interval [a,b][a, b] and has an inverse**) function gg. Prove that if ff is convex upward, then gg is convex downward, and vice versa.

  5. The function f(x)f(x), defined on the interval [a,b][a, b], is convex upward. Prove that for any points x1,…,xnx_1, \ldots, x_n lying on the segment [a,b][a, b] and any positive points a1,…,ana_1, \ldots, a_n the following inequality holds:

a1f(x1)+…+anf(xn)a1+…+an≤f((a1x1+…+anxn)a1+…+an).\frac{a_1 f(x_1) + \ldots + a_n f(x_n)}{a_1 + \ldots + a_n} \leq f\left(\frac{(a_1 x_1 + \ldots + a_n x_n)}{a_1 + \ldots + a_n}\right).

(Note that this problem is a generalization of the previously proven theorem, which is obtained for a1=a2=…=an=1a_1=a_2=\ldots=a_n=1.)

Note. To solve this problem, you can use the same technique that we use when proving the theorem.

*) You can take the logarithm to any base greater than one.
**) See «Kvant», No. 1, page 22.

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ka 9 will be inside the ball. The electrode ball is connected to the brush with a bolt and secured by ball 11, which has a threaded hole.

The lower roller, and therefore the tape, can be turned by hand. But we use an asynchronous single-digit electric motor from an electric player 12 and connected it to the lower roller with a clutch 13.

The electric motor is turned on, the tape runs along the rollers. Along the way, from friction with brush 8, it picked up and deposited electric charges on the ball conductor. The more the tape has to rotate, the higher the potential of the ball will be. But there is a limit here. The fact is that at high electric field strength near the ball, the impact becomes electrically conductive, and charges begin to drain from the ball. The ball’s potential stops growing.

We can calculate to what potential we can charge the ball. The field voltage on the surface of the ball is calculated by the formula E=VRE = \frac{V}{R}, where VV is the potential of the ball, and RR is its radius. If R=5R = 5 cm, and EE for exposure at atmospheric pressure is equal to 30 kV/cm, then the ball can be charged up to 150 thousand volts.

This calculation is correct only for an ideal smooth ball, located very far from all other conducting objects. Therefore, the voltage created by our generator will be lower than the calculated one.

If you manage to make a larger ball, then you can charge it to a higher potential. Above only means that the ball should be very smooth and even.

Now do some experiments with the model.

First of all, determine the sign of the ball’s charge. How to do this is clear. You just have to remember that an ebonite rod rubbed against fur is electrified negatively, and a glass rod rubbed against silk is positively electrified.

Determine how many full revolutions the tape must make in order for the high-voltage electrode to be fully charged. To do this, place a clearly visible mark on the tape and count how many full revolutions the tape makes until the electrode potential increases to its maximum value. Please note that the “generator performance” depends significantly on the position of the upper brush.

If the brush is positioned so that it is close to the place where the tape enters the ball, then the charges from the tape will not be completely removed, and you will have to wait a long time until the high-voltage electrode is charged. By changing the position of the upper brush, find one in which the high-voltage electrode will be fully charged at a minimum number of revolutions of the belt.

Our model uses nylon tape. And Van de Graaff used silk. In the electrostatic generator of the Kharkov Institute, the charging tape was made of rubberized fabric. Try making a charging tape from a different material.

Our charging brush is made from a polystyrene plate; it can be made from limited stack or copper. If you use a wire brush, ground it. The generator begins to work better. Why?

Don’t despair if you fail at first. Remember that even the best existing electrostatic generators produce voltages that are only a third of what they are designed for. All the reasons for this are not yet clear. So there is something to think about and something to invent.

For those who want to learn more about electrostatic generators, we recommend reading the book “Electrostatic accelerators of charged particles”, Gosatomizdat, 1963.

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PROBLEM WORKER

Chapter 1

Fig. 1.

F42. The rope will be thrown over the block, with part of the rope lying on the table and part on the floor. After the rope was released, it began to move. Find the speed of steady uniform motion of the rope. The height of the table is h.

F43. Find the pressure at the center of a liquid of radius R if the liquid is incompressible and has a density ρ.

Weighted Physics Olympiad, 1969

F44. Two dolphins swim towards each other. One of them makes a sound of frequency ω. What frequency does the other dolphin hear if the speeds of the dolphins relative to the water are the same and equal to v? Speed ​​of sound in water and.

Weighted Physics Olympiad, 1968

F45. A spherical capacitor filled with a dielectric and charged to a certain potential difference is discharged through its dielectric. What will be the magnetic field of the discharge currents in the space between the spheres?

F46. A cube falls onto a ball from a height of 1 m, and then jumps almost 1 m. To what height does the ball jump? To what height will the ball jump if exactly the same ball falls on it from a height of 1 m?

G. L. Komkin

F47. If the ABC process (Fig. 1) is performed on an ideal gas, then the amount of heat Q is imparted to it. What amount of heat is imparted to the gas during the ADC process?

Moscow City Physical Olympiad, 1970

M36. Prove that it is impossible to arrange seven lines and seven points on a plane so that three lines pass through each point and three points lie on each line.

M37. A certain number is inscribed in each cell of an infinite sheet of checkered paper so that the sum of the numbers in any square (the sides of which follow the grid lines) does not exceed one in absolute value. Prove that then there exists a number c such that the sum of the numbers in any rectangle (whose sides go along the lines

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mesh) no more than cc; in other words, that the sums of numbers in all rectangular iks are limited. Prove that it is possible to take c=4c=4. Perhaps you can incriminate this estimate (for example, prove that our statement is true for c=3c=3 or even for c=2c=2)?
Yu. I. Ionin

M38. A circle constructed at the height ADAD of a right triangle ABCABC as a diameter intersects leg ABAB at point KK, and leg ACAC at point MM. Line segment KMKM intersects height ADAD at point LL. It is known that the segments AKAK, ALAL and AMAM form a geometric progression (i.e. AK/AL=AL/AMAK/AL=AL/AM). Find the acute angles of triangle ABCABC (Fig. 2).
L. M. Lopovok

Fig. 2.

M39. Prove that non-negative integers x,yx, y satisfy the equation
x2−mxy+y2=1x^2 - mxy + y^2 = 1
(where mm is a given integer greater than one) if and only if xx and yy are adjacent numbers of the sequence

φ0=0,φ1=1,φ2=m,\varphi_0 = 0, \quad \varphi_1 = 1, \quad \varphi_2 = m,
φ3=m2−1,φ4=m3−2m,\varphi_3 = m^2 - 1, \quad \varphi_4 = m^3 - 2m,
φ5=m4−3m2+1,…,\varphi_5 = m^4 - 3m^2 + 1, \quad \dots,
in which φk+1=mφk−φk−1\varphi_{k+1} = m\varphi_k - \varphi_{k-1} for all k⩾1k \geqslant 1.

For example, all solutions to the equation x2−3xy+y2=1x^2 - 3xy + y^2 = 1 for the number 0⩽x<y0 \leqslant x < y are pairs (0,1)(0, 1); (1,3)(1, 3); (3,8)(3, 8); (8,21)(8, 21) adjacent members of the sequence 0,1,3,8,21,55,…0, 1, 3, 8, 21, 55, \dots defined by the conditions φ0=0,φ1=1,φk+1=3φk−φk−1\varphi_0 = 0, \quad \varphi_1 = 1, \quad \varphi_{k+1} = 3\varphi_k - \varphi_{k-1} for all k⩾1k \geqslant 1. (This red fact was used in the work of Yu. Matiyasevich related to Hilbert’s 10th problem, which was discussed in the previous issue «Kvant».)

M40. Find the amount
1⋅n+2⋅(n−1)+3⋅(n−2)+…1 \cdot n + 2 \cdot (n - 1) + 3 \cdot (n - 2) + \dots
⋯+(n−1)⋅2+n⋅1.\dots + (n - 1) \cdot 2 + n \cdot 1.

Try solving the following, more general problem: find the sum
Sn,k=[1⋅2…k]×S_n, k = [1 \cdot 2 \dots k] \times
×[n(n−1)…(n−k+1)]+\times [n(n - 1) \dots (n - k + 1)] +
+[2⋅3…(k+1)]×+ [2 \cdot 3 \dots (k + 1)] \times
×[(n−1)(n−2)…(n−k)]+\times [(n - 1)(n - 2) \dots (n - k)] +
+[3⋅4…(k+2)]×+ [3 \cdot 4 \dots (k + 2)] \times
×[(n−2)(n−1)…(n−k−1)]+…\times [(n - 2)(n - 1) \dots (n - k - 1)] + \dots
⋯+[(n−k)(n−k+1)…(n−1)]×\dots + [(n - k)(n - k + 1) \dots (n - 1)] \times
×[(k+1)k…2]+\times [(k + 1)k \dots 2] +
+[(n−k+1)(n−k+2)…n]×+ [(n - k + 1)(n - k + 2) \dots n] \times
×[k(k−1)…1].\times [k(k - 1) \dots 1].

V. N. Berezin

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M3. (a) On figure 1, and the plane is covered with heel squares of flowers. The centers of squares of the same color are located at the vertices of the square grid. With what number of colors is a similar filling of the plane possible?

(b) On figure 1, b the plane is covered with hexagons of families and colors so that the centers of hexagons of the same color form the vertices of a lattice of identical regular triangles. With what number of colors is a similar construction possible?

Notes. In the first problem, the number of colors can be one (all squares are the same color) or two (like on a chessboard). In the second problem you can easily find solutions with one color and with a third color. It is advisable to give a complete solution to the problems, i.e., describe all colorings that satisfy the specified conditions. However, please send incomplete solutions if they seem interesting to you. Think, for example, is there a solution with thirteen colors in the second problem?

Solution*)

Now we will consider correct only such filling of the plane with squares (or hexagons) in which the grid corresponding to any one color has the same dimensions and directions of the sides of the squares (or triangles) as the grid corresponding to any other color. In other words, all meshes must be obtained from each other in parallel. Of course, different meshes cannot be painted with the same color. The solution to the problem for general cases (squares and hexagons) is similar, and we will consider both cases at once.

  1. Let us first prove that if the filling plane is in the indicated way, then the number of colors is equal to k2+l2k^2 + l^2 in the case of squares and k2+kl+l2k^2 + kl + l^2 in the case of hexagons, where k,lk, l are non-negative integers (but not equal to zero at the same time)**).

*) For the beginning of solving this problem, see «Kvant» No. 7, page 54.
**) There are other formulas that represent the same sets of numbers, for example, k2−kl+l2k^2 - kl + l^2 for hexagons,

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The unit of length is the distance between the centers of two adjacent squares or hexagons.

Let’s draw a grid with thick black lines passing through the centers of squares or hexagons of the same color, say, red (Fig. 2, 3).

In the case of hexagons, we will draw lines in only two directions, so that the grid will not consist of regular triangles, but of rhombuses.

Let ABCDABCD be one square or one diamond of the grid. Let us derive a formula for its area.

In the case of a square, we draw straight lines through the points AA and BB, parallel to the sides of the surrounded squares, and denote the point of their intersection as MM. The lengths AM=kAM=k and BM=lBM=l are integers (one of them can be zero). On figure 1 k=3k=3, l=2l=2. Then AB=k2+l2AB=\sqrt{k^2+l^2} and the area of ​​ABCDABCD is k2+l2k^2+l^2.

In the case of a rhombus, we draw straight lines through the points AA and BB, parallel to the apsphemas of the hexagons, and denote the point of their intersection as MM. Angle AMBAMB may turn out to be equal to 120∘120^\circ or 60∘60^\circ. Let’s draw straight lines so that it is equal to 120∘120^\circ. The lengths AM=kAM=k and BM=lBM=l are integers (one of them can be zero). On figure 2 k=1k=1, l=2l=2. Then AB=k2+kl+l2AB=\sqrt{k^2+kl+l^2}, and the area of ​​the rhombus is 32(k2+kl+l2)\frac{\sqrt{3}}{2}(k^2+kl+l^2).

We will prove that the number of colors participating in the coloring is equal to the ratio of the area ABCDABCD to the area of ​​one circumferential square (case (a)) or hexagon (case (6)) and is therefore equal to:

in the case of squares k2+l2k^2+l^2,

in case of hexagons k2+kl+l2k^2+kl+l^2

(since the area of ​​one hexagon is 32\frac{\sqrt{3}}{2}).

This follows immediately from the next lemma.

Main lemma. Part ABCDABCD, painted with whatever color is involved in the coloring, either represents one square (in case (a)), corresponding to a hexagon (in case (6)), or consists of pieces (for red - four, for other colors - two), from which the same square or hexagon can be folded.

The proof of the lemma is not difficult, and we invite the reader to carry out

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Fig. 4. The plane is filled with identical figures with an area of ​​13 squares. Try to find an “elementary” piece of a plane filled in this way and glue a torus from it, as we did with a square.

Note. You need to select 13 figures, from them you need to form a polygon that will not be a square, but nevertheless can easily be glued into a torus. This should be done with a sheet of glue paper.

It’s on its own. Let us only note that the coloring of all squares (rhombuses) of the bold grid is the same, that is, if you cut out a square (rhombus) ABCDABCD from the plane and superimpose it, say, on an adjacent square (rhombus), then part ABCDABCD, painted with any color, will exactly match the part of the neighboring square (rhombus), painted with the same color.

There is another way to present this proof, more beautiful, but requiring some imagination. Let us first restrict ourselves to the case of a square grid. Let us express a square ABCDABCD from the plane and make a tube from it - a cylinder, the colored side on the outside, compatible from the sides ABAB and DCDC. This tube is delimited by two circles derived from sides ABAB and DCDC. Let’s glue these circles together (by combining point A=DA=D with point B=CB=C). For this, the paper tube will have to be solidified, but we still consider its entire painted surface as a single whole, not divided into parts by folds. The surface area of ​​the resulting figure is k2+l2k^2+l^2, and the part of it painted with any of the coloring colors is a square of size 1×11 \times 1. We advise you to do all this practically with a square sheet of paper, coloring it with a fifth or more colors.

In the case of hexagons, we will arrive at a similar result if we mark a rectangle in the same way, having one side common with the rhombus ABCDABCD and the other equal to the height of the rhombus.

You can fill the plane with other equal figures in which the areas shaded with different colors are equal. For example, in the solution to problem (a), sent from Kyiv (Belinsky lane 8, apt. 32, the author’s last name is not indicated), it is proposed to fill the plane with figures made up of two squares on the sides kk and ll. Let’s say for k=2k=2 and l=3l=3 (13 colors) the figure will be the same as in figure 4.

II. Now let us be given the number m=k2+l2m=k^2+l^2 or n=k2+kl+l2n=k^2+kl+l^2. Let us show that the plane can be filled in accordance with the conditions with squares of mm colors or hexagons of nn colors.

Let’s fill the plane with equal squares or regular hexagons and start cutting them out as follows.

Let’s paint one of them red. Let’s count kk squares (hexagons) from it in one direction, then turn it by 90∘90^\circ for squares and 60∘60^\circ for hexagons and count ll squares (hexagons) in a new direction, and we will also paint the square (hexagon) in which we arrive in red. On the segment connecting the centers of two red squares (hexagons), as on the side, we will construct a square (a) or a regular triangle (6). By attaching equal squares (regular triangles) to it, we get the centers of all squares (hexagons), which must be painted red; moving all the soybeans in parallel

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A collection of red squares (hexagons), each time we will get a new collection of unpainted squares (hexagons) and paint it with a new color until we have painted the entire plane. According to what was proven above, the number of colors will be equal to k2+l2k^2+l^2 in case (a) and k2+kl+l2k^2+kl+l^2 in case (b).

III. What natural numbers can be represented as k2+l2k^2+l^2 or k2+kl+l2k^2+kl+l^2? To write down the first few of these numbers, it is convenient to create two tables: table 1 for k2+l2k^2+l^2, table 2 for k2+kl+l2k^2+kl+l^2.

The numbers below the diagonal repeat those already written and do not need to be written. Some numbers appear in the table twice; the corresponding cells are highlighted. This means that with such a number of colors there are two significantly different ways of filling the plane. Now it’s easy to find and write these numbers in ascending order.

First table: 1, 2, 4, 5, 8, 9, 10, 13, 16, 17, 18, 20, 25, 26, …
Second table: 1, 3, 4, 7, 9, 12, 13, 16, 19, 21, 25, 27, 28, …

Suppose we have already written down these numbers to some point and are looking for the next largest number.

The red lines drawn on the first table help to do this. To explain how they are carried out, we note that in the first table each number is equal to the square of the distance from the center of the cell in which it stands to point 0 in the upper left corner (we take the side of the cell as a unit of length). Therefore, if we draw several circles with center 0, then they will divide our numbers (that is, the centers of the cells in which they stand) into groups in ascending order. If you try to draw similar lines in the second table by hand, it may seem that they are straight. But this, of course, is not true. In fact, these graphs correspond to the form

k2+kl+l2=c=constk^2+kl+l^2=c=\text{const}

in a coordinate system with origin 0 and axes going: axis kk - to the right, axis ll - down. Moving on to another pair of variables: x=k+lx=k+l, y=k−ly=k-l, you can see that these are ellipses elongated in the direction of the y∗y^* axis).

In a sense, we have the answer, but perhaps it can be simplified. For example, if in some other problem we get the answer: all numbers of the form k2+l2+m2+n2k^2+l^2+m^2+n^2, two kk, ll, mm, nn are integers, then it can be rewritten as follows: any non-negative integer, since all natural numbers can be represented in this form. It may be in our sequence

*) Those who read the book by N.B. Vasiliev and V.L. Gutenmacher “Straights and Curves”, of course, noticed that the red lines are the level lines of the functions k2+l2k^2+l^2 and k2+kl+l2k^2+kl+l^2 on the plane (k,l)(k, l).

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Are all natural numbers included, starting from a certain place? To prove that this is not so, you can use the dotted line system.

Let us draw a red circle with center 0 of radius nn in the first table. The centers of all cells containing numbers less than or equal to n2n^2 lie inside or on the edge of a sector of this circle with a central angle of 45∘45^\circ. Therefore, all such cells lie inside the figure; they are obtained from this sector if we add to it a strip of width 1 bordering it. The area of ​​this figure is less than πn28+3n+4\frac{\pi n^2}{8} + 3n + 4.

Hence, among the first n2n^2 natural numbers there are πn28+3n+4\frac{\pi n^2}{8} + 3n + 4, representable as k2+l2k^2 + l^2. For large nn the second number of the first is approximately π8\frac{\pi}{8}. In fact, since some numbers in the table are equal, there are even fewer numbers of the form k2+l2k^2 + l^2. It is easy to see that the fraction of numbers representable as k2+kl+l2k^2 + kl + l^2 is even smaller.

M4. Given the segment ABAB. Find points CC on the plane of the set such that in triangle ABCABC the median drawn from vertex AA is equal to the altitude drawn from vertex BB.

Solution

The editors have received many letters with solutions to this problem, but almost all of them are incomplete. Many readers have forgotten that when finding the geometric locus of points (GLP), it is necessary to clearly verify two things: 1) all points of the found set satisfy the conditions; 2) all points satisfying the conditions belong to the found set. Requirement 1) a lot of things were not taught. We will present two solutions to the problem: one is purely geometric, the second is using the coordinate method.

First decision. Let’s start with 2). Let us be given a segment ABAB and a path CC—a point satisfying the conditions, ADAD—the median of triangle ABCABC. Let us complete the triangle to a parallelogram by extending the median ADAD to the point EE so that AD=DEAD=DE. There are two possible cases here: the angle AEBAEB is acute or obtuse.

(a) Let the angle AEBAEB be acute (Fig. 5, a). Let’s draw BF⊥ACBF \perp AC, AK∥BFAK \parallel BF, then in the right triangle AEKAEK the leg AKAK is equal to half the hypotenuse AEAE, therefore ∠AEB=30∘\angle AEB=30^\circ.

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(6) Let angle AEB be of type (Fig. 5, 6). Carrying out BF ⊥ AC, AK || BF, we obtain, similarly to case (a), that ∠AEK=30°, therefore ∠AEB=150° (the difference from case (a) is that now points K and B lie on opposite sides of E).

So, if C is the desired point, then segment AB is visible from point E at an angle of 30° or 150°. As is known, all such points E are located on two circles O₁ and O₂, which are divided by the chord AB into arcs of 300° and 60° (Fig. 6, a), and, therefore, all points C are on the same circles O’₁ and O’₂, obtained from O₁ and O₂ by parallel transfer to the segment l=AB in the direction from B to A (Fig. 6, 6).

Now we prove that any point M of circles O’₁ and O’₂ belongs to the required set of points. Let M be an arbitrary point of one of these circles; then by drawing MK=AB, MK||AB, we get point K on one of the circles O₁ or O₂ (Fig. 7, a, 6). On figure 7, a’ BF ⊥ MA, AL||BF, AL=BF, then (from ΔAKL) AL=1/2 AK, i.e. the point M satisfies the conditions. Similarly on figure 7, 6 BF ⊥ MA, AL=BF, AL||BF, ∠AKB=150°, ∠AKL=180°−∠AKB=30°, i.e. AL=1/2 AK, and point M also satisfies the conditions. So, all points O’₁ and O’₂, except points N and A, satisfy the conditions.

Note that many readers who solved the geometric problem received parts of circles O’₁ and O’₂ as an answer. (Figure 8, a was obtained, for example, by V. Mashanov from the city of Grodno, figure 8, 6 by S. Ivanenko from the city of Fedosia and figure 8, by A. Alyaeva from the Penza region.) The correct solution (although slightly different from the one given here) was added by L. Stolyarov from the city of Penza.

Second solution. (A slight simplification of the solution sent by A. Grishkov from Tomsk.) Let us introduce a rectangular coordinate system with the origin at point A, let point B have coordinates (2; 0), and the desired point C have coordinates (x; y). Let AF be the median in triangle ABC, BK ⊥ AC (Fig. 9). It is easy to show that point F has coordinates (x+2/2; y/2). Then AF²=(x+2/2)²+y²/4. According to the conditions BK²=AF², therefore

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Fig. 8, a. Fig. 8, b. Fig. 8, p.

from the similarity of triangles AKB and ACD it follows that BK2AK2=CD2AD2\frac{BK^2}{AK^2} = \frac{CD^2}{AD^2} or
(x+22)2+y244−[(x+22)2+y24]=y2x2.\frac{\left(\frac{x+2}{2}\right)^2 + \frac{y^2}{4}}{4 - \left[\left(\frac{x+2}{2}\right)^2 + \frac{y^2}{4}\right]} = \frac{y^2}{x^2}.

Transforming (1), we get
y4+(2x2+4x−12)y2+(2x+x2)2=0.y^4 + (2x^2 + 4x - 12)y^2 + (2x + x^2)^2 = 0.

This is the equation connecting the coordinates of the required points. Some readers further wrote that it defines a fourth-order curve, which is quite difficult to draw.

In fact, it turns out that the left side of equation (2) is factorized:
[(x+1)2+(y+3)2−4][(x+1)2+(y−3)2−4]=0.[(x+1)^2 + (y+\sqrt{3})^2 - 4] [(x+1)^2 + (y-\sqrt{3})^2 - 4] = 0.

Fig. 9. Fig. 10.

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You can guess about it, for example, like this.

Let us introduce the notation: y2=zy^2 = z. Then (2) is a quadratic equation with respect to zz. Let’s factorize its left-hand side. To do this, let’s find roots (2).

z1,2=12−2x2−4x±(12−2x2−4x)2−4(2x+x2)22=z_{1,2} = \frac{12 - 2x^2 - 4x \pm \sqrt{(12 - 2x^2 - 4x)^2 - 4(2x + x^2)^2}}{2} =

=12−2x2−4x±48(3−x2−2x)2=6−x2−2x±23(3−x2−2x)== \frac{12 - 2x^2 - 4x \pm \sqrt{48(3 - x^2 - 2x)}}{2} = 6 - x^2 - 2x \pm 2\sqrt{3(3 - x^2 - 2x)} =

=(3−x2−2x±3)2.= (\sqrt{3 - x^2 - 2x} \pm \sqrt{3})^2.

Equation (2) can now be represented as follows:

∣z−(3−x2−2x+3)∣∣z−3−x2−2x−3∣2=0\left| z - (\sqrt{3 - x^2 - 2x} + \sqrt{3}) \right| \left| z - \sqrt{3 - x^2 - 2x} - \sqrt{3} \right|^2 = 0

or

∣y2−(4−(x+1)2+3)∣∣y2−(4−(x+1)2−3)∣2=0.\left| y^2 - (\sqrt{4 - (x + 1)^2} + \sqrt{3}) \right| \left| y^2 - (\sqrt{4 - (x + 1)^2} - \sqrt{3}) \right|^2 = 0.

(see figure 10, where one of these sets is red and the other is green).

Let us transform (4) further:

∣y−4−(x+1)2+3∣∣y+4−(x+1)2−3∣[… ][… ]=0;\left| y - \sqrt{4 - (x + 1)^2} + \sqrt{3} \right| \left| y + \sqrt{4 - (x + 1)^2} - \sqrt{3} \right| [\dots] [\dots] = 0;

hence we get (3)*.

Ninth-grader P. Kriksunov from Kiev and some other readers who wrote us solutions to this problem noticed that the following more general problem can be solved in a similar way: find a set of points CC such that in triangle ABCABC the ratio of medians ADAD to height BFBF is equal to the given number kk (either of the two solution methods described above is suitable).

M5. In the set EE, consisting of nn elements, mm different subsets (different from EE itself) are identified so that for every two elements from EE there is exactly one of the given subsets that contains both of these elements.

Prove that m≥nm \geq n. In what cases is a solution possible?

Solution

From readers’ letters one can judge that this task is extremely difficult, but interesting. Strictly speaking, here we are dealing with two problems: 1) prove that m≥nm \geq n, 2) in what cases is a solution possible?

As for the first problem, only AA solved it completely. Creatures from Leningrad. His proof is based on one of the basic theorems of linear algebra, which states that if there are more nn-vectors than nn, then they are linearly dependent.

For those who are familiar with this concept, it will be interesting to come up with such a proof. As for the second problem, it is shown, and this is not surprising, since it will be shown below that it is related to one known, but unsolved mathematical probleme.

For ease of presentation, some readers suggested other formulations of the problem. Here are two of them.

*) Equation (x−a)2+(y−b)2=c2(x - a)^2 + (y - b)^2 = c^2 defines a circle with center at point (a;b)(a; b) of radius cc (see, for example, I. M. Gelfand, E. G. Glagoleva, A. A. Kirr ilov, Method of coordinates, “Nauka”, 1968).

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Fig. 11.

a) Students from the same school often gather in groups and go out to eat ice cream. After such a visit, they quarrel so much that no two of them eat ice cream together after that. By the end of the year, they found out that in the future they could only go to the ice cream parlor one by one. Prove that if the number of students visited by this time was more than 1, then it is not less than the number of students in the school.

  1. Let there be nn points. Through every two points there is exactly one straight line, and each straight line contains no more than (n−1)(n-1) points. We need to prove that the number of lines is at least nn.

Are these tasks equivalent to the original one?

In any case, it is convenient, when thinking about this problem, to imagine the elements as “points”, and the bases as “lines”, passing through these points and doing for yourself figure like our figure 11 and 12. (In general, it is impossible not to ensure that all the lines are straight; as problem M36, figure 12 shows, it is impossible to correct it so that the red line is straight, so the problem 6) is not equivalent to the original one.)

Next, we present the solution to the problem, following the instructions of the author of the problem, N. Bourbaki*), and also, for convenience, we rewrite the conditions of the problem.

Given nn different elements and has a system mm of sets composed of these elements, and:

  1. no set of our system contains all the elements at once;
  2. every two of the given nn elements occur in one of the set of the system;
  3. if two elements occur in one of the sets, then they do not appear together in any of the other sets of the system.

Let us prove that m≥nm \geq n.

Let us give some example of such arrangement of elements. Let n=5n=5 and there be elements: a,b,c,d,ea, b, c, d, e. Let’s create such a system of a set of these elements;

(a,b),(a,c,e,),(b,e),(b,c),(b,d),(a,d),(d,e),(c,d)(a, b), (a, c, e,), (b, e), (b, c), (b, d), (a, d), (d, e), (c, d).

Obviously, it satisfies conditions 1), 2), 3). Here m=8m=8, and by the way 8≥58 \geq 5.

To make the proof more clear, we will sometimes refer to this example.

Proof. Note that n>2n>2 and that it is sufficient to prove the inequality m≥nm \geq n for a system of sets containing at least two elements.

  1. The system consists of at least two sets, then by condition 2) this set would contain all the elements at once, which contradicts conditions 1).

*) See N. Bourbaki, Set Theory, Mir, M., 1965, p. 220.

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  1. Each element is included in at least two sets of the system. If an element were included in only one set, then by virtue of 2) it must contain all nn elements, which contradicts 1).

  2. One and the same element cannot be included in all sets of the system at once. Let some element, call it xx, be included in all sets of the system. Then, by condition 3), no two sets contain identical elements, with the exception of the element xx. Therefore, no two elements other than xx occur in any of the set, but this contradicts 2).

  3. Let us associate each element with the number of the set of the system in which it is included, that is, we count how many times it is repeated in this system. In the example, the element aa is mapped to the number 3, the element bb to 4, etc.

What set of the system is comparable to the number of elements it contains? In the example of the first set the number 2 is associated, the second set is associated with 3, etc.

The sum of all numbers corresponding to elements is equal to the sum of all numbers corresponding to sets. In the example 3+4+3+4=2+3+2+2+2+2+2+2=173+4+3+4=2+3+2+2+2+2+2+2=17.

In fact, if we consider two elements to be different when they are included in different sets, then both sum to the number of elements of all sets of the system.

  1. Notation. Let’s take one of those elements that correspond to the smallest number, i.e., which is included in the smallest number of the set of the system. In the example, we can take either aa, or cc, or ee; let’s take aa. Let us denote this element by ana_n, and the number of the set in which it is included by knk_n. In the example a5=aa_5=a, k5=3k_5=3. By virtue of paragraphs. 2 and 3 we have 2⩽kn<m2 \leqslant k_n < m.

The sets that include ana_n will be denoted in some order by A1A_1, A2A_2, …, AknA_{k_n}, and the rest by Akn+1A_{k_n+1}, …, AmA_m. In the example A1=(a,b)A_1=(a, b), A2=(a,c,e)A_2=(a, c, e), A3=(a,d)A_3=(a, d), A4=(b,e)A_4=(b, e), …, A8=(c,d)A_8=(c, d).

Consider the first knk_n sets A1A_1, A2A_2, …, AknA_{k_n}. Reasoning in the same way as in point 3, we see that no two of them contain the same elements, with the exception of a˙n\dot{a}_n. Therefore, we can take one element from each of these sets and denote them respectively by a1a_1, a2a_2, …, akna_{k_n}. We denote the remaining elements in some order by akn+1a_{k_n+1}, akn+2a_{k_n+2}, …, ana_n. In the example a1=ba_1=b, a2=ca_2=c, a3=da_3=d, a4=ea_4=e; then A1=(a1,a5)A_1=(a_1, a_5), A2=(a2,a4,a5)A_2=(a_2, a_4, a_5), A3=(a3,a5)A_3=(a_3, a_5), A4=(a1,a4)A_4=(a_1, a_4), A5=(a1,a2)A_5=(a_1, a_2), A6=(a1,a3)A_6=(a_1, a_3), A7=(a3,a4)A_7=(a_3, a_4), A8=(a2,a3)A_8=(a_2, a_3).

Now let us denote the numbers corresponding to the elements a1a_1, a2a_2, …, akna_{k_n}, …, an−1a_{n-1} in the same order by k1k_1, k2k_2, …, kn−1k_{n-1}. For example, that the element ana_n corresponds to the number knk_n, and it is the smallest of all the numbers k1k_1, k2k_2, …, kn−1k_{n-1}, knk_n.

Finally, let us denote the numbers corresponding to the sets A1A_1, A2A_2, …, AmA_m in the same order by s1s_1, s2s_2, …, skns_{k_n}, …, sms_m.

Let us once again pay attention to how we numbered the elements and sets.

First, knk_n is the smallest of the numbers k1,k2,...,kn−1k_1, k_2, ..., k_{n-1}.

Secondly, knk_n is the number of the last of the sets that contain the element ana_n, and, thus, the element ana_n is not included in the sets Akn+1A_{k_n+1}, …, AmA_m.

The set AiA_i contains the element aia_i, but does not contain the elements aja_j if 1⩽i⩽kn1 \leqslant i \leqslant k_n, 1⩽j⩽kn1 \leqslant j \leqslant k_n and i≠ji \neq j. In addition, according to paragraph 4, k1+⋯+kn=s1+⋯+smk_1 + \dots + k_n = s_1 + \dots + s_m.

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  1. If the element aia_i does not belong to some set AjA_j, then ki⩾sjk_i \geqslant s_j. Indeed, let the set AjA_j not contain the element aia_i and consist of sjs_j different elements. then the element aia_i must occur with each of these elements in some of the remaining sets of the system. On the other hand, no two of these elements can ever occur in these sets, since they have already occurred in AjA_j. Therefore, the number of sets in which the element aia_i is not less than sjs_j.

  2. Consider the first knk_n set A1,A2,…,AknA_1, A_2, \dots, A_{k_n} and the first knk_n elements of a1,a2,…,akna_1, a_2, \dots, a_{k_n}. They are chosen in such a way that each set AiA_i contains an element aia_i with the same number, but does not contain elements with other numbers, then, according to paragraph 6, s1⩽k2,s2⩽k1s_1 \leqslant k_2, s_2 \leqslant k_1 if kn=2k_n = 2 and

s1⩽k2,s2⩽k1,…,skn⩽k1,s1⩽kkn,s2⩽kkn,…,skn⩽kkn−1,\begin{align*} s_1 &\leqslant k_2, \quad s_2 \leqslant k_1, \quad \dots, s_{k_n} \leqslant k_1, \\ s_1 &\leqslant k_{k_n}, \quad s_2 \leqslant k_{k_n}, \quad \dots, s_{k_n} \leqslant k_{k_n-1}, \end{align*}

if kn>2k_n > 2.

In the example kn=3k_n = 3 and

2=s1⩽k2=3,3=s2⩽k1=4,3=s3⩽k1=4,2=s1⩽k3=4,3=s2⩽k3=4,3=s3⩽k2=3.\begin{align*} 2 &= s_1 \leqslant k_2 = 3, \quad 3 &= s_2 \leqslant k_1 = 4, \quad 3 &= s_3 \leqslant k_1 = 4, \\ 2 &= s_1 \leqslant k_3 = 4, \quad 3 &= s_2 \leqslant k_3 = 4, \quad 3 &= s_3 \leqslant k_2 = 3. \end{align*}

  1. Adding up all the inequalities, we get that

(kn−1)(s1+s2+⋯+skn)⩽(kn−1)(k1+⋯+kkn)(k_n - 1)(s_1 + s_2 + \dots + s_{k_n}) \leqslant (k_n - 1)(k_1 + \dots + k_{k_n})

or

s1+s2+⋯+skn⩽k1+⋯+kn.s_1 + s_2 + \dots + s_{k_n} \leqslant k_1 + \dots + k_{n}.

  1. Teller we can prove the inequality m⩾nm \geqslant n required in the problem. Let’s assume that m<nm < n. Let’s compare two amounts

S=(s1+s2+⋯+skn)+skn+1+⋯+smS = (s_1 + s_2 + \dots + s_{k_n}) + s_{k_n+1} + \dots + s_m

And

K=(k1+k2+⋯+kn)+kkn+1+⋯+kn.K = (k_1 + k_2 + \dots + k_n) + k_{k_n+1} + \dots + k_n.

Note that we have renumbered the set in such a way that the element ana_n does not belong to the set Akn+1,…,AmA_{k_n+1}, \dots, A_m; this means skn+1⩽kn,…,sm⩽kns_{k_n+1} \leqslant k_n, \dots, s_m \leqslant k_n and even more so skn+1⩽kkn+1,…,sm⩽kms_{k_n+1} \leqslant k_{k_n+1}, \dots, s_m \leqslant k_m, since knk_n is the smallest of all numbers kik_i. In this case, since m<nm < n, we get: kkn+1+⋯+kn>skn+1+⋯+smk_{k_n+1} + \dots + k_n > s_{k_n+1} + \dots + s_m, but then S<KS < K, and this contradicts item 4.

The proof that m⩾nm \geqslant n is complete.

  1. Let’s try to find out in what cases equality is possible. If m=nm = n, then from items 8, 9 and 4 it follows:

k1+⋯+kkn+⋯+kn=s1+⋯+skn+⋯+sn.k_1 + \dots + k_{k_n} + \dots + k_n = s_1 + \dots + s_{k_n} + \dots + s_n.

Obviously, for this it is necessary that the equality

k1+⋯+kkn=s1+⋯+sknk_1 + \dots + k_{k_n} = s_1 + \dots + s_{k_n}

and all the inequalities from paragraph 8 were reduced to equalities. Since knk_n is the smallest of kik_i, we have

skn+1=⋯=sn=kkn+1+⋯+kn.s_{k_n+1} = \dots = s_n = k_{k_n+1} + \dots + k_n.

Next we consider two cases.

(a) kn=2k_n = 2. In this case, as is easy to see, the following set system is possible (Fig. 9): (an,a1),(an,a2,a3,…,an−1),(a1,a2),(a1,a3),…,(a1,an−1)(a_n, a_1), (a_n, a_2, a_3, \dots, a_{n-1}), (a_1, a_2), (a_1, a_3), \dots, (a_1, a_{n-1}). For any nn it satisfies the conditions of the problem.

(b) kn>2k_n > 2. In this case, we obtain that all inequalities in paragraph 7 must be

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rushes into equality. Comparing all these equalities, we obtain that s1=s2=⋯=skn=k1=k2=⋯=kkns_1=s_2=\dots=s_{k_n}=k_1=k_2=\dots=k_{k_n}.

And the same as for case (a): skn+1=⋯=sn=kkn+1=⋯=kn−1=kns_{k_n+1}=\dots=s_n=k_{k_n+1}=\dots=k_{n-1}=k_n.
It is obvious that one of the numbers s1,s2,…,skns_1, s_2, \dots, s_{k_n} is at most one of the numbers kkn+1,…,kn−1k_{k_n+1},\dots,k_{n-1} and, therefore, s1=s2=⋯=sn=k1=k2=⋯=kn=l>2s_1=s_2=\dots=s_n=k_1=k_2=\dots=k_n=l>2.

As a result, we find that in this case the following condition is satisfied:

  1. which set contains exactly ll distinct elements and which element is included in exactly ll distinct sets.

For this it is necessary that n=l(l−1)+1n=l(l-1)+1. Indeed, consider some element xx. It must appear exactly in the ll set, therefore all these sets contain all nn elements just as xx must occur with all elements. In addition, they cannot contain the same elements, since they all contain the element xx. From here we obtain the required equality.

For l=3l=3, i.e. n=7n=7, it is easy to construct the required set system (Fig. 10). But the question of for which nn type l2−l+1l^2-l+1 a set of nn elements there is a subset system that satisfies conditions 1), 2), 3) and 4) turns out to be very difficult.

Such a system has a special name: a finite projective plane of order l−1l-1. (On Fig. 12 a projective plane of order 2 is depicted, consisting of 7 points and 7 lines.) It is easy to prove that for any finite projective plane the following property is also satisfied, “dual” to property 2):

  1. Any two sets from our system have a common element (obviously only one); in other words, which two lines intersect at one point.

Let us show how to construct a finite projective plane of order pp (with n=p2−p+1n=p^2-p+1), where pp is a prime number. To do this, you need to use “numbers” from pp-arthmetic (see the article “Comparisons modulo and remainder arithmetic”, «Kvant» No. 5, pp. 27-33) - arthmetic of remainders modulo pp. In this kind of mathematics, if pp is prime, you can divide any “number” by any other non-zero number. Let us use a point to define the triple “number” (x1,x2,x3)(x_1, x_2, x_3), considered up to proportionality (i.e., the triples (x1,x2,x3)(x_1, x_2, x_3) and (kx1,kx2,kx3)(kx_1, kx_2, kx_3) define the same point). Let’s agree that the three (0,0,0)(0, 0, 0) should not be considered a dot.

The straight line is given by a triple of numbers (a1,a2,a3)(a_1, a_2, a_3) (except for the triple (0,0,0)(0, 0, 0)), considered up to proportionality. The point (x1,x2,x3)(x_1, x_2, x_3) accepts a straight line (a1,a2,a3)(a_1, a_2, a_3) if and only if a1x1+a2x2+a3x3=0a_1x_1+a_2x_2+a_3x_3=0.

Check that for such specific lines and points all conditions 1)–5) are met. Make sure that for p=2p=2 you get exactly the example of a projective plane of order 2 that is chosen for figure 12.

Similarly, we can prove that there exists a projective plane of order pkp^k, where pp is a prime and kk is any natural number. It is proven that projective planes of order NN do not exist for an infinite number of NN (in particular, for N=6N=6, N=14N=14). But for N=10N=10 it is unknown whether a projective plane of order NN exists or not: no computer can simply enumerate all possible combinations.

You can read about the theory of finite projective planes and related problem combinators in the book “Combinatorial Mathematics” by G. J. Reiser (“Mir”, 1966, series “Matematika Collection Library”).

A. Toom, J. Rabbot, W. Gutenacher

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“Mathematics” is a magazine for secondary school students of the People’s Republic of Bulgaria, published by the Central Committee of the Dmitrov Communist Youth Union and the Ministry of Public Education. High school students in Bulgaria, who are more interested in mathematics, receive 6 books of the magazine every day with a volume of 48 pages. The magazine is very popular - its circulation exceeds 50 thousand copies. The editorial board of “Mathematics” includes a number of famous Bulgarian mathematicians, who devoted a lot of time and effort to promoting mathematics among young people.

The traditional magazine is a systematic publication of stories about outstanding mathematicians, popular science articles on the development of mathematical science and its applications. From issue to issue, the magazine publishes small materials on mathematical problems accessible to high school students, introduces its readers to a modern presentation of a number of issues in elementary mathematics, to such branches of science as set theory, group theory, etc. It is especially pleasant to note that all the articles are written in an accessible, engaging and vivid manner. Among the journal’s materials there are translations of articles by foreign, in particular, Soviet mathematicians.

A significant place in the magazine is devoted to the task, recommended for those finishing school, for those entering college and technical education. A special section is devoted to more difficult problems: the reader is invited to participate in a competition to solve them. The last few pages of the magazine contain entertaining and humorous questions.

In this issue «Kvant» we will introduce our readers to several materials translated from the magazine “Mathematics”.

Editorial
magazine «Kvant»

The editors of the journal “Mathematics” received the first issues of the journal «Kvant».

On behalf of our many readers and on behalf of the editors, we cordially congratulate you on the creation of the Vashcheyo magazine and wish you fruitful and successful work. The journal “Mathematics,” which has been published for nine years, is «Kvant»’s brother. And we will be very happy if both journals further establish a theoretical one.

With another greeting, “Mathematics” magazine
Ch. editor prof. A. Mateev

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About two actions
with real numbers
Kiril Chimev

The operations of addition and multiplication of real numbers are subject to a number of laws. Let’s recall some of them:

  1. Commutativity of addition: a+b=b+aa+b=b+a.
  2. Addition associativity: (a+b)+c=a+(b+c)(a+b)+c=a+(b+c)
  3. Commutativity of multiplication: ab=baab=ba.
  4. Multiplication associativity: (ab)c=a(bc)(ab)c=a(bc).
  5. Distributivity of multiplication relative to addition:
    (a+b)c=ac+bc(a+b)c=ac+bc

It is curious, however, that these laws remain valid in some other cases, when “addition” and “multiplication” are understood as other operations that differ from the addition and multiplication of real numbers that are familiar to us.

By “sum”*) of two real numbers aa and bb we agree to understand max (a,b)(a, b), that is, the largest of the numbers aa and bb, if a≠ba \neq b, and any of them, if a=ba=b. The operation of “addition,” which assigns any two real numbers aa and bb their “sum,” will be denoted by the sign ⊕\oplus, so
a⊕b=max⁡(a,b).a \oplus b=\max(a, b).

For example:
(−3)⊕2=2,(-3) \oplus 2=2,
0⊕(−2)=0,0 \oplus (-\sqrt{2})=0,
π⊕π=π.\pi \oplus \pi=\pi.

Commutativity of “addition”
a⊕b=b⊕aa \oplus b=b \oplus a
obvious because
max⁡(a,b)=max⁡(b,a).\max(a, b)=\max(b, a).

By the “product” of two real numbers aa and bb we agree to understand the number min (a,b)(a, b), that is, the largest of the numbers aa and bb, if a≠ba \neq b, and any of them, if a=ba=b. The operation of “multiplication”, which assigns any two real numbers aa and bb their “product”, will be denoted by the sign ⊗\otimes, so that
a⊗b=min⁡(a,b).a \otimes b=\min(a, b).

For example:
(−3)⊗2=−3,(-3) \otimes 2=-3,
0⊗(−2)=−2,0 \otimes (-\sqrt{2})=-\sqrt{2},
π⊗π=π.\pi \otimes \pi=\pi.

Commutativity of “multiplication”
a⊗b=b⊗aa \otimes b=b \otimes a
obvious because
min⁡(a,b)=min⁡(b,a).\min(a, b)=\min(b, a).

In order to establish the associativity of “addition”
(a⊕b)⊕c=a⊕(b⊕c),(a \oplus b) \oplus c=a \oplus (b \oplus c),
(1)
we must make sure that equality is fair
max⁡(max⁡(a,b),c)=max⁡(a,max⁡(b,c).\max(\max(a, b), c)=\max(a, \max(b, c).
To do this, let’s draw up table 1. Its left column lists all possible arrangements of the three real numbers a,b,ca, b, c in ascending order, and in the following columns for each of the locations

*) We put quotation marks to avoid confusion with familiar arithmetic operations.

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quantities a⊕ba \oplus b, (a⊕b)⊕c(a \oplus b) \oplus c, b⊕cb \oplus c, a⊕(b⊕c)a \oplus (b \oplus c). From this table it is clear that equality (1) is valid for any real numbers a,b,ca, b, c.

Thus we can talk about the “sum” of three real numbers a⊕b⊕ca \oplus b \oplus c, defined as a⊕(b⊕c)a \oplus (b \oplus c) or, equivalently, as (a⊕b)⊕c(a \oplus b) \oplus c. A closer look at this Table 1 leads us to the conclusion that a⊕b⊕c=max⁡(a,b,c)a \oplus b \oplus c = \max(a, b, c).

Associativity of “multiplication”, i.e. valid for any real a,b,ca, b, c equalities

(a⊗b)⊗c=a⊗(b⊗c)(a \otimes b) \otimes c = a \otimes (b \otimes c)

or, what is the same, the reader will check the equalities min (min⁡(a,b),c)=min⁡(a,min⁡(b,c))(\min(a, b), c) = \min(a, \min(b, c)) independently in the same way as we were convinced of the associativity of “addition”.

Let us now establish the distributivity of “multiplication” relative to “addition”:

(a⊕b)⊗c=(a⊗c)⊕(b⊗c),(a \oplus b) \otimes c = (a \otimes c) \oplus (b \otimes c),

(2) which can be written in the form

min⁡(max⁡(a,b),c)=max⁡(min⁡(a,c),min⁡(b,c))\min(\max(a, b), c) = \max(\min(a, c), \min(b, c)).

To do this, it is enough to compile Table 2, from which it is clear that equality (2) is indeed true for any three real numbers a,b,ca, b, c.

As is known, for ordinary arithmetic operations the distributivity of addition with respect to multiplication does not apply: the equality (ab)+c=(a+c)×(b+c)(ab) + c = (a + c) \times (b + c) is not true for all real numbers. But for the operations “addition” and “multiplication” we introduced, this distributivity is also true:

(a⊗b)⊕c=(a⊕c)⊗(b⊕c).(a \otimes b) \oplus c = (a \oplus c) \otimes (b \oplus c).

The reader will be convinced of this by checking that max (min⁡(a,b),c)=min⁡(max⁡(a,c),max⁡(b,c))(\min(a, b), c) = \min(\max(a, c), \max(b, c)) for any real numbers a,b,ca, b, c.

Interestingly, “addition” and “multiplication” also have other properties that are not observed in ordinary real number arithmetic:

a⊕a=a,a⊗a=a;a \oplus a = a, a \otimes a = a;

a⊗(a⊕b)=a,a⊕(a⊗b)=a.a \otimes (a \oplus b) = a, a \oplus (a \otimes b) = a.

These relations directly follow from the definitions of the operations ⊕\oplus and ⊗\otimes.

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Everyone knows that every real number aa can be assigned an opposite number, that is, the number −a-a. We condition the number opposite aa to be denoted by the symbol aa. For example: 2,5‾=−2,5;−V2‾=2;0‾=0\overline{2,5} = -2,5; \overline{-V^2} = \sqrt{2}; \overline{0} = 0.

It is curious that the operations of “addition” and “multiplication” turn out to be connected with the operation of taking the opposite number:

a⊕b‾=a‾⊗b‾;a⊗b‾=a‾⊕b‾\overline{a \oplus b} = \overline{a} \otimes \overline{b}; \overline{a \otimes b} = \overline{a} \oplus \overline{b}

(6) (in general arithmetic the formulas are also incorrect!).

Prove these formulas yourself.

In conclusion, try to solve the following problems yourself:

  1. Verify that for n≥2n \geq 2 arbitrary real numbers a1,…,ana_1, \ldots, a_n
    a1⊕…⊕an=max⁡(a1,…,an),a1⊗…⊗an=min⁡(a1,…,an)a_1 \oplus \ldots \oplus a_n = \max(a_1, \ldots, a_n), a_1 \otimes \ldots \otimes a_n = \min(a_1, \ldots, a_n).

  2. Are the matches correct?
    c⊗(a⊕b)=(c⊗a)⊕(c⊗b),c⊕(a⊗b)=(c⊕a)⊗(c⊕b)?c \otimes (a \oplus b) = (c \otimes a) \oplus (c \otimes b), c \oplus (a \otimes b) = (c \oplus a) \otimes (c \oplus b)?

  3. Prove that for any real numbers a,b,ca, b, c the equality
    min⁡[min⁡(a,c),min⁡(max⁡(a,b),c)]=min⁡(a,c)\min [\min(a, c), \min(\max(a, b), c)] = \min(a, c) and write it using the operations ⊕\oplus and ⊗\otimes. How can you immediately be convinced of its validity after this?

  4. Let a,b,ca, b, c be arbitrary real numbers. Find a simple expression for the quantity
    min⁡[a,−max⁡(min⁡(a,b),max⁡(a,c))]\min[a, -\max(\min(a, b), \max(a, c))].

  5. For any real numbers a,b,ca, b, c is the equality true
    (a⊕b)⊗(a⊕b⊕c)=a⊗[c⊗(c⊕b)]?(a \oplus b) \otimes (a \oplus b \oplus c) = a \otimes [c \otimes (c \oplus b)]?

  6. Is it possible to find a real number xx such that
    max⁡[min⁡(a,max⁡(a,b),x)]=b\max [\min(a, \max(a, b), x)] = b?

Below are several problems taken from the competition section of the Matematika magazine.

  1. In some kingdoms, in some states there are several cities, and the distances between them are all different in pairs. On one morning, one plane takes off from each city and is used in the nearest neighboring city.

Can there be more than one heel of planes in any city?

  1. prove; that if a,b,ca, b, c are the lengths of the sides of the triangle, and la,lb,lcl_a, l_b, l_c are the lengths of the bisectors of the internal angles drawn to them, then
    laa+lbb+lcc≤p22S\frac{l_a}{a} + \frac{l_b}{b} + \frac{l_c}{c} \leq \frac{p^2}{2S}

where pp is the half-perimeter, and SS is the area of ​​the triangle; the equal sign is achieved only for an equilateral triangle.

A. Mameev

  1. Prove that if the real number aa is the root of the equation
    2(x2+x)sin⁡2x+(2x+2−x3)cos⁡2x=x3+2x+22(x^2 + x)\sin 2x + (2x + 2 - x^3)\cos 2x = x^3 + 2x + 2,
    then this number satisfies the inequality ∣a∣<1|a| < 1.

B. Petkov

  1. Let there be a point in the plane of a convex polygon that has the property that any line drawn through this point divides the polygon into two equal parts. Prove that then this polygon is centrally symmetric.

P. Grozdanov

  1. The fly, without stopping, will climb in one direction at a constant speed along the circumference of the upper base of a cylindrical tin can, the height of which is 4 times the diameter 2r2r of the base. At some point, from the point of the jar’s surface farthest from the husband, the flour begins to follow the path, and it climbs along the surface of the jar at a constant speed equal to the speed of the flour (and also does not stop). Find the length of the shortest path along which the path can overtake the flour.

I. Dimovski

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1970 is the year of the Great Jubilee, the 100th anniversary of the birth of V.I. Lenin, whose name is given to awards for the most outstanding research and achievements in the field of science and technology. It is gratifying to note that the majority of the anniversary year prizes went to physiomathematical research. This is convincing evidence of the successful development of modern physics and mathematics, which occupy the forefront of world science. Next, a short story about the works awarded the Lenin Prize will, of necessity, take up several pages in our magazine.

A team of employees from four leading scientific institutes - the Institute of Experimental and Theoretical Physics, the Radio Engineering Institute, the Institute of High Energy Physics and the Research Institute of Electrophysical Equipment - includes Corresponding Member of the USSR Academy of Sciences V.V. Vladimirsky, D.G. Koshkarev, A.A. Kuzmin, Corresponding Member of the USSR Academy of Sciences A.A. Logunov, R.M. Sulyaev, I.F. Malysheva was awarded the Lenin Prize for the development and commissioning of the promon synchropron of the Institute of High Energy Physics for an energy of 70 GeV.

The main experimental tool for studying the wonderful world of elementary particles is the loaded particle accelerator. By accelerating particles to gigantic energies, it makes it possible to study the interaction of accelerated particles with matter, from the various features of which one can judge the nature of the forces acting between particles. With such interactions, new elementary particles are born that do not exist under normal conditions.

The largest accelerator in the world is the Soviet proton synchrotron, recently built in the young science city of Protvino near Serpukhov. It accelerates the atomic nuclei of hydrogen - protons - to an energy of 70 billion electron volts (70 GeV; 1 electron volt equals energy

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gini, which acquires an electron by passing through an electron potential difference of one volt). Left behind are the recent record holders—the proton intensifier of the European Atomic Center in Geneva at 28 Gsv and a similar American accelerator at Brookhaven National Laboratory at 33 Gsv. It should be noted that in a number of experiments, the energy of protons achieved in Protvino turned out to be higher than the design one and amounted to 76 Gsv.

The main part of the accelerator is the pressing chamber - a giant underground ring 1480 m long. The chamber is located in a magnetic field formed by 120 magnetic sections weighing 200 tons, between which 54 accelerating devices (resonance) are placed. The creator of the accelerator had to offer enormous difficulties associated with unusually strict requirements for the characteristics of the magnetic field and the arrangement of the blocks. It is enough to indicate that the deviation of any block from the specified position by more than 0.1 mm disrupts the operation of the accelerator!

The accelerated particles make about 400,000 revolutions in 2.6 seconds and reach speeds very close to the speed of light in vacuum. When they hit targets, they generate streams of secondary particles (mesons, antiprotons, neutrinos, etc.), which are sorted by special separators into different channels for further research.

During the short period of operation of the accelerator in Protvino, a number of unique experiments have already been performed on it. One of them was devoted to the Japanese so-called “quarks” (hypothetical elemental particles with fractional values ​​of electron charges), the other ended with the creation of atomic nuclei of the anti-helement - antihelium with a mass of 3. They will consist of two antiprotons and one antineutron. There is no doubt that the new record-breaking Soviet accelerator can wrest more secrets of the microworld from nature.

A team of employees of the Evvan Physical Institute, the Institute of Physics of the Academy of Sciences of the Georgian SSR and the Moscow Engineering Physics Institute - corresponding member of the USSR Academy of Sciences A. I. Alikhanyan, T. L. Asatini, G. E. Chikovani, V. N. Roinishvili, B. A. Dolgoshen, B. I. Luchkov - received a premio for the creation of a new means of observing elementary particles - preque art cameras.

Research on elementary particles requires not only accelerators capable of creating such particles, but also special methods for recording traces of these particles. There are few such methods, and each of them brings fundamental discoveries to science. A track spark chamber is one of the best modern methods for recording elementary particles. It consists of several electrodes (plates or wires) connected to a high voltage source and placed in a vessel filled with a neutral gas. Passing through the gas gaps between the electrodes, a rapidly charged particle destroys gas atoms. A track appears - a visible trace of a particle formed by a chain of bright sparks. The design of the cameras is such that they are capable of recording particles for very short periods of time, amounting to millionths of a second. This allows experimenters to target the camera to record specific types of particle elements and their characteristic interactions. Track spark chambers have helped make important discoveries, for example, the discovery of the existence of two types of special particle elements - neutrinos, one of which is associated with the birth of electrons,

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and the other - we will generate mesons.

Professor of the Faculty of Physics of Moscow University A. A. Vlasov was awarded the Lenin Prize for a series of works on the theory of plasma, containing a fundamental method for studying its properties.

Plasma is an inoculated gas consisting of a huge number of loaded particles. We will encounter it in various electronic devices. It forms the upper layers of the earth’s atmosphere and fills outer space. The behavior of plasma is very different from the behavior of an ordinary gas consisting of neutral particles. In an ordinary gas, the main role is played by direct collisions of its particles. The behavior of such a gas is described by the Boltzmann equation. A. A. Vlasov was the first to show that in plasma such collisions play practically no role, since the electrostatic response does not allow the particles to come close to each other. Therefore, in his equation for plasma, Vlasov excluded the classical term that takes into account the direct abundances of particles, and introduced a term that takes into account the collective influence of loaded neighbors on the behavior of individual particles. This is how the famous “Vlasov equation” was obtained, which formed the basis of plasma theory.

The method of plasma research developed by A. A. Vlasov is used in work on the creation of controlled thermonuclear reactions, in the study of the propagation of radio waves in the atmosphere and outer space, as well as in a vast new field of physics, the so-called magnetic hydrodynamics, associated in part with methods of direct conversion of thermal energy into electrical energy.

Corresponding Member of the USSR Academy of Sciences R.V. Khokhlov and Professor S.A. Akhmanov, working at the Faculty of Physics of Moscow University, were awarded a prize for the study of nonlinear co-ferential interactions in optics.

Object optics deals with processes in which the intensity of light is insufficient to change the physical properties of the medium through which the light passes. The emergence of powerful sources of light beams - lasers - makes it possible to create new optics, so-called nonlinear. She studies the numerous changes in the physical characteristics of the environment under the influence of the passage of light. The foundations of this area of ​​physics were laid by R.V. Khokhlov and S.A. Akhmanov. However, one of the most important achievements of these scientists was the creation of lasers with varying wavelengths of radiation. Typically, each laser has its own strictly fixed wavelength of emitted radiation, its own color. It is determined by natural radiatingweise. The range of possible wavelengths for different lasers is quite poor; it does not contain many tricks needed for physics, chemistry and biological sciences. R.V. Khokhlov and S.A. Akhmanov developed new principles that allowed less colorization of the laser in a very wide range of wavelengths. For example, using their methods, a laser operating on invisible infrared waves can be made to emit ultraviolet rays. Such lasers have many important practical applications. They greatly expanded the possibilities of studying the nature of substances.

The fifth Lenin Prize in Physics was awarded to Yu. N. Denisyuk, an employee of the State Optical Institute, for a series of works “Holeraphy with recording in a three-dimensional environment.”

Objects give us a flat image of the objects imprinted on them. And in the mirror we see a three-dimensional image - the object appears to be located in the depths of the mirror. Of course, what we see behind the mirror is not really there. The image is created by light waves incident on the mirror and reflected from it. Is it not possible

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make sure that the three-dimensional picture that we see in the mirror does not disappear even after removing the mirror?
In other words, is it possible to capture a three-dimensional image of opaque objects in the same way that regular photographic film does with a flat image? This problem was solved by Yu. N. Denisok (before him, a similar problem of obtaining a volumetric image of solid bodies was solved by the English physicist Gabor). It turns out that for this it is necessary to record in a special transparent fine-grained emulsion the distribution of light waves near the object under consideration (as they say, to obtain a hologram of the object). If you develop the resulting “photograph,” it will be completely different from the object depicted. However, having illuminated the developed plate with white light, we will see close to it a magnificent three-dimensional image of the object photographed in this way.

If you insert a mirror and take a photo in the usual way, you will get a circle with light reflections. If you get a hologram of such a mirror, then the image created with its help will be so real that it can focus the light falling on it like a real mirror.

A new method for obtaining three-dimensional images, created by Yu. N. Denisok, opens up the possibility of creating color three-dimensional cinema and television, improving radar and sonar.

In the field of mathematics, the Lenin Prize was awarded to a team of Leningrad scientists - academician Yu. V. Linnik, corresponding member of the USSR Academy of Sciences Yu. V. Prozhorov, professor I. A. Ibragimov and Yu. A. Rozanov for a series of works on limit methods of probability techniques. In these works, the most important patterns of a number of complex random processes that play a major role in many areas of science and technology were found. The patterns found greatly facilitate the study of random processes that are widespread in nature and society.

The Central Committee of the CPSU and the Council of Ministers of the USSR also decided to award the 1970 Lenin Prizes in the field of science and technology to a large group of scientists, designers and industrial workers for the following works:

— a set of scientific and technical work carried out with the aim of creating an experimental orbital station and implementing it during launches of the Soyuz rocket and space system;

— creation of automatic mechanical stations “Venera-4”, “Venera-5”, “Venera-6” and a complex of scientific research to determine the physical parameters and chemical composition of the atmosphere of the planet Venus;

  • the creation of a meteorological system that, with the help of artificial Earth satellites “Meteor”, provides the receipt and prompt processing of global meteorological information for those in need of addressing these complex scientific and technical problems, a great contribution was made by Soviet mathematicians and physicists.

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To the article “Non-hanging polyhedra”

  1. Let us show that from each face of an arbitrary convex polyhedron one can go to any other, moving from funny face to funny face. To do this, take two arbitrary faces and select a point in them that does not lie on the boundary. Let’s connect the selected points with a segment. This segment does not intersect the planes of the faces of the polyhedron, or the polyhedron is convex. Let us draw a plane through this segment that does not contain the vertices of the polyhedron: this is possible, since the polyhedron has only a finite number of vertices. The drawn plane carves two broken lines on the surface of the polyhedron. They do not pass through the vertices of the polyhedron, i.e., moving along them, we will move from one adjacent face to another and pass from the vertex face to the second. Telerfficium some face of a polyhedron, say Γ1\Gamma_1, and two points O1O_1 and O2O_2, distant rhr_h from all its vertices. Let us assume for simplicity that three faces converge at all vertices of the polyhedron; In general, the essence of the matter remains unchanged. the vertices of any face adjacent to Γ1\Gamma_1 are removed by rhr_h either from O1O_1 or from O2O_2, but not from both, or all points equidistant from O1O_1 and O2O_2 lie in the plane of face Γ1\Gamma_1. Let us assume that there are also faces Γ2\Gamma_2 and Γ3\Gamma_3, that the vertices of the first lie at a distance rhr_h from O1O_1, and the vertices of the second lie at a distance O2O_2. It is clear that then there are two such faces that converge at one vertex, and therefore, by virtue of an additional assumption, are adjacent. Then the second end of their common edge is equal to O2O_2 and O1O_1, which contradicts the convexity of the polyhedron.

So, the vertices of all faces adjacent to Γ1\Gamma_1 are equal to the same point, for example, O1O_1. This is also true for the vertices of faces adjacent to Γ2\Gamma_2 or Γ3\Gamma_3, etc., i.e., for all vertices of the polyhedron. The opposite statement is obvious.

  1. Let us show that if all arc boundaries and angles of the constructed polyhedron are less than l, then it is convex. Let us take a plane polyhedron of its faces. All faces adjacent to it lie on one side of this plane, which means that on the same side lies the entire triangular paramid containing the extended face, and three other paramids that have a common edge with the first. Consequently, on the same side lie two faces of the octahedron, containing one of the edges of the vertex, and therefore the octahedron itself and the remaining paramides. To complete the proof, it is enough to calculate the arc boundary angle of the octahedron.

  2. Proceeding as in the proof of Steinitz’s theorem, it is easy to see that the sum in the first part is strictly greater than 0 (and not greater than 0).

  3. In the example based on Steinitz’s theorem, it is necessary to glue only part of the amdd.

  4. The proof coincides exactly with the proof that if kk faces converge at each vertex of a polyhedron, then it does not completely satisfy Steinitz’s theorem.

  5. Let us show that any closed broken line composed of edges of a polyhedron is even-linked. It is clear that it is sufficient to prove this for broken lines without self-intersection.

Let us consider some broken line that does not contain self-intersection and cut the polyhedron along this broken line. Let there be KK faces in one part, and LL and L≤KL \leq K in the other. The integer LL is called the girth of the broken line. If the girth is equal to 1, then the statement we prove follows from the conditions of the problem. Let us apply induction, let the problem be solved for broken girths less than LL. Let us choose a face Γ\Gamma whose edge belongs to the broken line and which lies in that part of the polyhedron where there are fewer faces. Let P1,P2,…,PkP_1, P_2, \dots, P_k be the edges of the polyline that are the edges of the face Γ\Gamma and Pk+1,…,PsP_{k+1}, \dots, P_s the remaining edges of the face Γ\Gamma. Let’s move on to a new broken line, which is obtained from the original by replacing the edges P1,…,PkP_1, \dots, P_k with Pk+1,…,PsP_{k+1}, \dots, P_s. It is possible that the new broken line has self-intersections and even consists of several unconnected pieces, but the girth of each of its non-self-intersecting parts is certainly less than LL, which means that the new broken line is even-linked. Let’s assume that it has 2N2N ringing. The face chosen at the beginning of the proof has 2Q=s2Q = s lines, then the number of links in the original broken line is 2N+2Q−2K2N+2Q-2K—an even number (Fig. 1).

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  1. We will present the solution to Problem 8, from which Problem 7 follows easily. Consider a kk-faceted angle whose vertex does not lie on the sphere. Let us draw a ray ll, entirely contained by the rutri (but not on the boundary) of the angle. Let the vertex initially lie outside the ball. Each circle divides the sphere into two “hats”. Let’s consider the circles - the intersections of the edges of the angle with the sphere and choose for each of them the cap that does not contain the point AA and BB - the points of intersection of the ray ll with the sphere. Consider a step-afficient projection onto a plane with the center of the projection at point AA. The fixed kk caps do not intersect at one point, which means that the projection will produce a picture similar to figure 2.

Fig. 2.
B′B' is the image of point BB under projection. The sum of the angles of a polygon A1,…,AkA_1, \dots, A_k is strictly greater than the sum of the relative angles. We do not know whether it is convex, but it is clear that the straight segments connecting the point B′B' with the points AiA_i belong entirely to it. This follows from the definition of ray ll. Due to this, A1+⋯+Ak=π(k−2)A_1 + \dots + A_k = \pi(k-2) and the sum of relative angles is less than π(k−2)\pi(k-2).

If the vertex lies inside the ball, then we prove in exactly the same way that the sum of the relative angles is greater than π(k−2)\pi(k-2).

Let’s move directly to solving the problem. Let B1B_1 be a vertex whose position is undefined. Let’s divide the vertices, as described in task 6, into black and white. Let B1B_1 be white. It is easy to see that if the vertex of a kk-faceted angle lies on the sphere and all its edges intersect the sphere except one edge tangent to the sphere, then the sum of the relative angles is equal to π(k−2)\pi(k-2).

Now let’s move on to the external relative angles and calculate their sums at each vertex. For all vertices except B1B_1, these sums are obviously equal to 2π. If B1B_1 does not lie on the sphere, then the sum under it is not equal to 2π. Let’s add the equalities for white vertices, subtract from them the equalities for black and

As a result, we get that 0≠00 \neq 0. Thus, B1B_1 lies on the sphere.

  1. Let’s assume the opposite. Let us connect the point of contact of each face with the vertices of the face by segments and consider the angle between two segments, which rests on some edge of the polygon (Fig. 3). The magnitude of this angle does not depend on the choice of one of the faces containing the edge. ΔO′B1B2=ΔO′′B1B2\Delta O'B_1B_2 = \Delta O''B_1B_2 (according to the sides), which means <B1O′B2=<B1O′′B2<B_1O'B_2 = <B_1O''B_2.

We assign to each edge the value of the angle resting on it. Let us denote the angle assigned to the edge PkP_k by βk\beta_k. The sum of the angles assigned by the edge of each face is 2π.

Further proof comes from

Fig. 3.
proof of Steinitz’s theorem by replacing the word vertex with the words edge.

  1. ab=[1;1,2,1,2,… ]\frac{a}{b} = [1; 1, 2, 1, 2, \dots].
  2. [1;1,1,… ]=5+12[1; 1, 1, \dots] = \frac{\sqrt{5}+1}{2};
    a10=R5−12;sin⁡18∘=5−14a_{10} = R \frac{\sqrt{5}-1}{2}; \sin 18^\circ = \frac{\sqrt{5}-1}{4}.
  3. [0;1,1,… ]=5−12[0; 1, 1, \dots] = \frac{\sqrt{5}-1}{2};
    a10=R5−12;sin⁡18∘=5−14a_{10} = R \frac{\sqrt{5}-1}{2}; \sin 18^\circ = \frac{\sqrt{5}-1}{4}.
  4. If a0≠0a_0 \neq 0, then move the entire “comb” one step to the right, and put a zero in place of the integers. If a0=0a_0 = 0, then move the entire comb one step to the right. For example:
    α=[3;1,2,5],1α=[0;3,1,2,5]\alpha = [3; 1, 2, 5], \frac{1}{\alpha} = [0; 3, 1, 2, 5],
    β=[0;2,2,… ],1β=[2;2,2,… ].\beta = [0; 2, 2, \dots], \frac{1}{\beta} = [2; 2, 2, \dots].

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  1. Yes, with the only difference that the ≤ sign will be one step to the right, i.e.

p0<p1≤p2<p3<…p_0 < p_1 \leq p_2 < p_3 < \dots

To the article “Alice through the Looking Glass”

  1. 4 fum.
  2. 2 fum; 6 inch
  3. 60 fum; 3 inch; 3 inch; 4.
  4. 2.6 inch; 6 inch
  5. 0,25; 1/4=(1/2)21/4 = (1/2)^2.
  6. A truncated paramid measuring about 1/2×1/2×1/41/2 \times 1/2 \times 1/4 inch.
  7. 3 inches wide; 3/83/8 inch thick.
  8. She will be too thin.
  9. a) ordinary; 6) oval dial; when expressed, the arrows lengthen and shorten.
  10. The same as with the clock in Exercise 11, 6.
  11. In the direction 63∘50′63^\circ 50' northeast.
  12. No.

To the article “On one inductive method for proving inequalities”

  1. a) f(x)=xpf(x) = x^p; to prove the inequality for n−2n - 2 it is convenient to introduce the notations x=x1+x22x = \frac{x_1 + x_2}{2} and d=x2−x12d = \frac{x_2 - x_1}{2} and replace that if (x+d)p=Cp0xp+Cp1xp−1d+Cp2xp−2d2+Cp3xp−3d3+⋯+Cppdp(x + d)^p = C_p^0 x^p + C_p^1 x^{p-1} d + C_p^2 x^{p-2} d^2 + C_p^3 x^{p-3} d^3 + \dots + C_p^p d^p, where Cp0,Cp1,Cp2,…C_p^0, C_p^1, C_p^2, \dots are the coefficients of the polynomial (x+d)p(x + d)^p, then (x−d)p=Cp0xp−Cp1xp−1d+Cp2xp−2d2−Cp3xp−3d3+⋯+(−1)pCpp(x - d)^p = C_p^0 x^p - C_p^1 x^{p-1} d + C_p^2 x^{p-2} d^2 - C_p^3 x^{p-3} d^3 + \dots + (-1)^p C_p^p

c) f(α)=lg⁡sin⁡α;0<α<π2f(\alpha) = \lg \sin \alpha; \quad 0 < \alpha < \frac{\pi}{2}.

e) f(x)=lg⁡(1+10x),−∞<x<∞f(x) = \lg (1 + 10^x), -\infty < x < \infty; in the resulting inequality put xh=lg⁡bhahx_h = \lg \frac{b_h}{a_h},

To the article “An endless work”

First, let’s make sure that we get a geometric progression:

(1+x+x2+⋯+x9)×(1+x10+x20+⋯+x90)×(1+x100+x200+⋯+x900)⋯=1+x+x2+x3+x4+…(1 + x + x^2 + \dots + x^9) \times (1 + x^{10} + x^{20} + \dots + x^{90}) \times (1 + x^{100} + x^{200} + \dots + x^{900}) \dots = 1 + x + x^2 + x^3 + x^4 + \dots

Indeed, xanan−1…a0x^{a_n a_{n-1} \dots a_0} (where anan−1…a0=a0+10a1+⋯+10nana_n a_{n-1} \dots a_0 = a_0 + 10a_1 + \dots + 10^n a_n is the decimal notation of any non-negative integer) must necessarily appear in the process of multiplying parentheses and, moreover,

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Crossword

Vertical:

  1. Orthodromic referral.
  2. Concept from mechanics.
  3. Obstacle reflecting rays.
  4. Illustration for mathematical reasoning.
  5. Side of the world.
  6. Obstacle.
  7. Premise.
  8. Specialization in one of the applied objects of physics.
  9. Coordinate.
  10. A phenomenon that serves as the basis for another phenomenon.
  11. Way.
  12. Argument.
  13. Working conditions.
  14. Device for sighting.
  15. The number that turns the equation into equality.
  16. Mechanism.
  17. Research method.
  18. Research method.
  19. The number in the ancient Slavic numbering, about which it was said “and most of all there is something

the human mind can understand.”
30. Part of the table.

Horizontal:
7. Real number.
8. The path of movement of a celestial body.
9. Number.
11. A phenomenon accompanying the transfer of a body.
13. Unit for ancient mathematicians.
16. A measure of the integrity of fluid flow.
18. The place occupied by a digit in the notation of a natural number.
20. One of the characteristics of a triangle.
21. Angular motion of a satellite or aircraft.
22. A mechanism that transmits rotational motion.
25. Part of a telephone set.
26. Abrupt change in function behavior.
28. System of fastened rods.
31. One of the first geometers known to us.
32. Sample.
33. Soviet physician involved in cybernetics and its popularization.

Answer to the task “Three Magic Squares”, published in No. 7 (see figure).

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