olymmath

Putnam 1946

William Lowell Putnam Mathematical Competition 1946.

Session A

A1

  • Session A

Suppose that the function f(x)=ax2+bx+cf(x)=a x^2 +bx+c , where a,b,ca,b,c are real, satisfies the condition ∣f(x)∣≤1|f(x)|\leq 1 for ∣x∣≤1|x|\leq1 . Prove that ∣f′(x)∣≤4|f'(x)|\leq 4 for ∣x∣≤1|x|\leq1 .

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A2

  • Session A

If a(x),b(x),c(x)a(x), b(x), c(x) and d(x)d(x) are polynomials in xx , show that ∫1xa(x)c(x)dx⋅∫1xb(x)d(x)dx−∫1xa(x)d(x)dx⋅∫1xb(x)c(x)dx\int_{1}^{x} a(x) c(x) dx \cdot \int_{1}^{x} b(x) d(x) dx - \int_{1}^{x} a(x) d(x) dx \cdot \int_{1}^{x} b(x) c(x) dx is divisible by (x−1)4.(x-1)^4.

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A3

  • Session A

A projectile in flight is observed simultaneously from four radio stations which are situated at the corners of a square of side bb . The distances of the projectile from the four stations, taken in order around the square, are found to be R1,R2,R3R_1 , R_2 , R_3 and R4R_4 . Show that R12+R32=R22+R42.R_{1}^{2}+ R_{3}^{2}= R_{2}^{2}+ R_{4}^{2}. Show also that the height hh of the projectile above the ground is given by h2=−12b2+14(R12+R22+R32+R42)−18b2(R14+R24+R34+R44−2R12R32−2R22R42).h^{2}=- \frac{1}{2} b^2 +\frac{1}{4}(R_{1}^{2}+R_{2}^{2}+R_{3}^{2}+R_{4}^{2}) -\frac{1}{8 b^{2}}(R_{1}^{4}+R_{2}^{4}+R_{3}^{4}+R_{4}^{4}- 2 R_{1}^{2}R_{3}^{2} -2 R_{2}^{2} R_{4}^{2}).

Answer, solutions and source

A4

  • Session A

Let g(x)g(x) be a function that has a continuous first derivative g′(x)g'(x) . Suppose that g(0)=0g(0)=0 and ∣g′(x)∣≤∣g(x)∣|g'(x)| \leq |g(x)| for all values of x.x. Prove that g(x)g(x) vanishes identically.

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A5

  • Session A

Find the smallest volume bounded by the coordinate planes and by a tangent plane to the ellipsoid x2a2+y2b2+z2c2=1.\frac{x^{2}}{a^{2}}+\frac{y^{2}}{b^{2}}+\frac{z^{2}}{c^{2}}=1.

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A6

  • Session A

A particle of unit mass moves on a straight line under the action of a force which is a function f(v)f(v) of the velocity vv of the particle, but the form of the function is not known. A motion is observed, and the distance xx covered in time tt satisfies the formula x=at2+bt+cx= at^2 + bt+c , where a,b,ca,b,c have numerical values determined by observation of the motion. Find the function f(v)f(v) for the range of vv covered by the experiment.

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Session B

B1

  • Session B

Let KK denote the circumference of a circular disk of radius 11 , and let kk denote a circular arc that joins two points a,ba,b on KK and lies otherwise in the given circular disc. Suppose that kk divides the circular disk into two parts of equal area. Prove that the length of kk exceeds 2.2.

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B2

  • Session B

Let A,BA, B be two variable points on a parabola P0P_{0} , such that the tangents at AA and BB are perpendicular to each other. Show that the locus of the centroid of the triangle formed by A,BA,B and the vertex of P0P_0 is a parabola P1.P_1 . Apply the same process to P1P_1 and repeat the process, obtaining the sequence of parabolas P1,P2,…,PnP_1, P_2 , \ldots, P_n . If the equation of P0P_0 is y=mx2y=m x^2 , find the equation of Pn.P_n .

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B3

  • Session B

In a solid sphere of radius RR the density ρ\rho is a function of rr , the distance from the center of the sphere. If the magnitude of the gravitational force of attraction due to the sphere at any point inside the sphere is kr2k r^2 , where kk is a constant, find ρ\rho as a function of r.r. Find also the magnitude of the force of attraction at a point outside the sphere at a distance rr from the center.

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B4

  • Session B

For each positive integer nn , put pn=(1+1n)n,Pn=(1+1n)n+1,hn=2pnPnpn+Pn.p_n =\left(1+\frac{1}{n}\right)^{n}, P_n =\left(1+\frac{1}{n}\right)^{n+1}, h_n = \frac{2 p_n P_{n}}{ p_n + P_n }. Prove that h1<h2<h3<…h_1 < h_2 < h_3 <\ldots

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B5

  • Session B

Show that ⌈(3+1)2n)⌉\lceil (\sqrt{3}+1)^{2n})\rceil is divisible by 2n+1.2^{n+1}.

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B6

  • Session B

A particle moves on a circle with center OO , starting from rest at a point PP and coming to rest again at a point QQ , without coming to rest at any intermediate point. Prove that the acceleration vector of the particle does not vanish at any point between PP and QQ and that, at some point RR between PP and QQ , the acceleration vector points in along the radius RO.RO.

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