OCR (Cambridge University Press & Assessment) · United Kingdom
STEP 3 2018
2018
3h
13 questions worth 120 marks in total. Each part is annotated: check the hint if you are stuck, or reveal the worked solution once you have committed to an approach.
The function f is given by f(β)=β−β1−β21(β=0). Find the stationary point of the curve y=f(β) and sketch the curve.
Sketch also the curve y=g(β), where g(β)=β+β3−β21(β=0).
Let u and v be the roots of the equation x2+αx+β=0, where β=0. Obtain expressions in terms of α and β for u+v+uv1 and u1+v1+uv.
Given that u+v+uv1=−1, and that u and v are real, show that u1+v1+uv⩽−1.
Given instead that u+v+uv1=3, and that u and v are real, find the greatest value of u1+v1+uv.
Differentiation
The sequence of functions y0, y1, y2, … is defined by y0=1 and, for n⩾1, yn=(−1)nz1dxndnz, where z=e−x2.
Show that dxdyn=2xyn−yn+1 for n⩾1.
Prove by induction that, for n⩾1, yn+1=2xyn−2nyn−1. Deduce that, for n⩾1, yn+12−y2nynn+2=2n(yn2−ynn−1y2n+1)+2yn2.
Hence show that yn2−y2n−1y2n+1>0 for n⩾1.
Sequences & Series
Show that the second-order differential equation x2y′′+(1−2p)xy′+(p2−q2)y=f(x), where p and q are constants, can be written in the form xa(xb(xcy)′)′=f(x),(*) where a, b and c are constants.
Use (∗) to derive the general solution of the equation x2y′′+(1−2p)xy′+(p2−q2)y=0 in the different cases that arise according to the values of p and q.
Use (∗) to derive the general solution of the equation x2y′′+(1−2p)xy′+p2y=xn in the different cases that arise according to the values of p and n.
Differential Equations
The point P(asecθ,btanθ) lies on the hyperbola a2x2−b2y2=1, where a>b>0. Show that the equation of the tangent to the hyperbola at P can be written as bx−aysinθ=abcosθ.
This tangent meets the lines ax=by and ax=−by at S and T, respectively.
How is the mid-point of ST related to P?
The point Q(asecϕ,btanϕ) also lies on the hyperbola and the tangents to the hyperbola at P and Q are perpendicular. These two tangents intersect at (x,y).
Obtain expressions for x2 and y2 in terms of a, θ and ϕ.
Hence, or otherwise, show that x2+y2=a2−b2.
Coordinate Geometry & Conics
The real numbers a1, a2, a3, … are all positive. For each positive integer n, An and Gn are defined by An=na1+a2+⋯+anand Gn=(a1a2⋯an)1/n.
Show that, for any given positive integer k, (k+1)(Ak+1−Gk+1)⩾k(Ak−Gk) if and only if λkk+1−(k+1)λk+k⩾0, where λk=(Gkak+1)k+11.
Let f(x)=xk+1−(k+1)x+k, where x>0 and k is a positive integer. Show that f(x)⩾0 and that f(x)=0 if and only if x=1.
Deduce that:
(a)An⩾Gn for all n;
(b) if An=Gn for some n, then a1=a2=⋯=an.
Proof & Number Theory
The distinct points A, Q and C lie on a straight line in the Argand diagram, and represent the distinct complex numbers a, q and c, respectively. Show that c−aq−a is real and hence that (c−a)(q∗−a∗)=(c∗−a∗)(q−a).
Given that aa∗=cc∗=1, show further that q+acq∗=a+c.
The distinct points A, B, C and D lie, in anticlockwise order, on the circle of unit radius with centre at the origin
(so that, for example, aa∗=1). The lines AC and BD meet at Q. Show that (ac−bd)q∗=(a+c)−(b+d), where b and d are complex numbers represented by the points B and D respectively, and show further that (ac−bd)(q+q∗)=(a−b)(1+cd)+(c−d)(1+ab).
The lines AB and CD meet at P, which represents the complex number p. Given that p is real, show that p(1+ab)=a+b. Given further that ac−bd=0, show that p(q+q∗)=2.
Complex Numbers
Use De Moivre's theorem to show that, if sinθ=0, then 2i(cotθ+i)2n+1−(cotθ−i)2n+1=sin2n+1θsin(2n+1)θ, for any positive integer n.
Deduce that the solutions of the equation (12n+1)xn−(32n+1)xn−1+⋯+(−1)n=0 are x=cot2(2n+1mπ) where m=1, 2, … , n.
Hence show that m=1∑ncot2(2n+1mπ)=3n(2n−1).
Given that 0<sinθ<θ<tanθ for 0<θ<21π, show that cot2θ<θ21<1+cot2θ. Hence show that m=1∑∞m21=6π2.
Complex Numbers
In this question, you should ignore issues of convergence.
Let I=∫011+xf(x−1)dx, where f(x) is a function for which the integral exists.
Show that I=n=1∑∞∫nn+1y(1+y)f(y)dy and deduce that, if f(x)=f(x+1) for all x, then I=∫011+xf(x)dx.
The fractional part, {x}, of a real number x is defined to be x−⌊x⌋ where ⌊x⌋ is the largest integer less than or equal to x. For example {3.2}=0.2 and {3}=0.
Use the result of part (i) to evaluate ∫011+x{x−1}dx and ∫011+x{2x−1}dx.
Integration
A particle P of mass m is projected with speed u0 along a smooth horizontal floor directly towards a wall. It collides with a particle Q of mass km which is moving directly away from the wall with speed v0. In the subsequent motion, Q collides alternately with the wall and with P. The coefficient of restitution between Q and P is e, and the coefficient of restitution between Q and the wall is 1.
Let un and vn be the velocities of P and Q, respectively, towards the wall after the nth collision between P and Q.
Show that, for n⩾2, (1+k)un−(1−k)(1+e)un−1+e(1+k)un−2=0.(*)
You are now given that e=21 and k=341, and that the solution of (∗) is of the form (n⩾0)un=A(107)n+B(75)n(n⩾0), where A and B are independent of n. Find expressions for A and B in terms of u0 and v0.
Show that, if 0<6u0<v0, then un will be negative for large n.
Mechanics
A uniform disc with centre O and radius a is suspended from a point A on its circumference, so that it can swing freely about a horizontal axis L through A. The plane of the disc is perpendicular to L. A particle P is attached to a point on the circumference of the disc. The mass of the disc is M and the mass of the particle is m.
In equilibrium, the disc hangs with OP horizontal, and the angle between AO and the downward vertical through A is β. Find sinβ in terms of M and m and show that aAP=M+m2M.The disc is rotated about L and then released. At later time t, the angle between OP and the horizontal is θ; when P is higher than O, θ is positive and when P is lower than O, θ is negative. Show that 21Iθ˙2+(1−sinβ)ma2θ˙2+(m+M)gacosβ(1−cosθ) is constant during the motion, where I is the moment of inertia of the disc about L.
Given that m=23M and that I=23Ma2, show that the period of small oscillations is 3π5g3a.
Mechanics
A particle is attached to one end of a light inextensible string of length b. The other end of the string is attached to a fixed point O. Initially the particle hangs vertically below O. The particle then receives a horizontal impulse.
The particle moves in a circular arc with the string taut until the acute angle between the string and the upward vertical is α, at which time it becomes slack. Express V, the speed of the particle when the string becomes slack, in terms of b, g and α.
Show that the string becomes taut again a time T later, where gT=4Vsinα, and that just before this time the trajectory of the particle makes an angle β with the horizontal where tanβ=3tanα.
When the string becomes taut, the momentum of the particle in the direction of the string is destroyed. Show that the particle comes instantaneously to rest at this time if and only if sin2α=41+3.
Mechanics
A random process generates, independently, n numbers each of which is drawn from a uniform (rectangular) distribution on the interval 0 to 1. The random variable Yk is defined to be the kth smallest number (so there are k−1 smaller numbers).
Show that, for 0⩽y⩽1, P(Yk⩽y)=m=k∑n(mn)ym(1−y)n−m.(*)
Show that m(mn)=n(m−1n−1) and obtain a similar expression for (n−m)(mn).
Starting from (∗), show that the probability density function of Yk is n(k−1n−1)yk−1(1−y)n−k. Deduce an expression for ∫01yk−1(1−y)n−kdy.
Find E(Yk) in terms of n and k.
Probability & Statistics
The random variable X takes only non-negative integer values and has probability generating function G(t). Show that P(X=0 or 2 or 4 or 6…)=21(G(1)+G(−1)).You are now given that X has a Poisson distribution with mean λ. Show that G(t)=e−λ(1−t).
The random variable Y is defined by P(Y=r)={kP(X=r)0if r=0,2,4,6,…otherwise,
where k is an appropriate constant.
Show that
the probability generating function of Y is coshλcoshλt.
Deduce that
\text{E(Y)<λ}
for λ>0.
The random variable Z is defined by
P(Z=r)={cP(X=r)0if r=0,4,8,12,…otherwise, where c is an appropriate constant.
Is E(Z)<λ for all positive values of λ?