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STEP3 2020 -- Pure Mathematics

Exam: STEP3  |  Year: 2020  |  Questions: Q1—Q8  |  Total marks per question: 20

All questions are pure mathematics. Solutions and examiner commentary are included below.

QTopicDifficultyKey Techniques
1Pure MathematicsChallengingIntegration by parts, compound-angle formulae, induction
2Pure MathematicsChallengingImplicit differentiation, discriminants, hyperbolic functions, curve symmetry
3纯数Hard复数指数形式, 旋转公式, 重心公式, 模长计算
4纯数Hard反射矩阵公式, 矩阵方程求解, 旋转矩阵, 变换复合
5Pure MathematicsChallengingPartial fractions, algebraic identities, differentiation, improper-integral limits
6Pure MathematicsHardPolar sketches, small-quantity approximations, polar area formulae, trigonometric substitutions
7Pure MathematicsChallengingReduction of order, integrating factors, parameter matching, initial conditions
8Pure MathematicsHardContradiction, induction, recurrence analysis, construction, Euclidean algorithm

Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

1 For non-negative integers aa and bb, let I(a,b)=0π2cosaxcosbx dx.I(a, b) = \int_{0}^{\frac{\pi}{2}} \cos^{a} x \cos bx \ dx.

(i) Show that for positive integers aa and bb, I(a,b)=aa+bI(a1,b1).I(a, b) = \frac{a}{a + b} I(a - 1, b - 1).

(ii) Prove by induction on nn that for non-negative integers nn and mm, 0π2cosnxcos(n+2m+1)x dx=(1)m2nn!(2m)!(n+m)!m!(2n+2m+1)!.\int_{0}^{\frac{\pi}{2}} \cos^{n} x \cos(n + 2m + 1)x \ dx = (-1)^{m} \frac{2^{n} n! (2m)! (n + m)!}{m! (2n + 2m + 1)!}.

Hint
  1. (i) Integrating by parts,

u=cosaxv=cosbxu = \cos^a x \quad v' = \cos bx u=acosa1xsinxv=1bsinbxu' = -a \cos^{a-1} x \sin x \quad v = \frac{1}{b} \sin bx

I(a,b)=[cosax1bsinbx]0π20π2acosa1xsinx1bsinbx dxI(a, b) = \left[ \cos^a x \frac{1}{b} \sin bx \right]_0^{\frac{\pi}{2}} - \int_0^{\frac{\pi}{2}} -a \cos^{a-1} x \sin x \frac{1}{b} \sin bx \ dx =0+0π2acosa1xsinx1bsinbx dx=ab0π2cosa1xsinxsinbx dx= 0 + \int_0^{\frac{\pi}{2}} a \cos^{a-1} x \sin x \frac{1}{b} \sin bx \ dx = \frac{a}{b} \int_0^{\frac{\pi}{2}} \cos^{a-1} x \sin x \sin bx \ dx

cos(b1)x=cosbxcosx+sinbxsinx\cos(b - 1)x = \cos bx \cos x + \sin bx \sin x

So I(a,b)=ab0π2cosa1x (cos(b1)xcosbxcosx) dxI(a, b) = \frac{a}{b} \int_0^{\frac{\pi}{2}} \cos^{a-1} x \ (\cos(b - 1)x - \cos bx \cos x) \ dx =ab[I(a1,b1)I(a,b)]= \frac{a}{b} [I(a - 1, b - 1) - I(a, b)]

Thus I(a,b)=aa+b I(a1,b1)I(a, b) = \frac{a}{a+b} \ I(a - 1, b - 1) as required.

(ii) Suppose

I(k,k+2m+1)=(1)m2k k! (2m)! (k+m)!m! (2k+2m+1)!I(k, k + 2m + 1) = (-1)^m \frac{2^k \ k! \ (2m)! \ (k + m)!}{m! \ (2k + 2m + 1)!}

Then by (i),

I(k+1,k+2m+2)=k+12k+2m+3I(k,k+2m+1)I(k + 1, k + 2m + 2) = \frac{k + 1}{2k + 2m + 3} I(k, k + 2m + 1)

=k+12k+2m+3 (1)m2k k! (2m)! (k+m)!m! (2k+2m+1)!= \frac{k + 1}{2k + 2m + 3} \ (-1)^m \frac{2^k \ k! \ (2m)! \ (k + m)!}{m! \ (2k + 2m + 1)!}

=k+12k+2m+3 (1)m2k k! (2m)! (k+m)!m! (2k+2m+1)!×2k+2m+22k+2m+2= \frac{k + 1}{2k + 2m + 3} \ (-1)^m \frac{2^k \ k! \ (2m)! \ (k + m)!}{m! \ (2k + 2m + 1)!} \times \frac{2k + 2m + 2}{2k + 2m + 2}

=(1)m2k+1 (k+1)! (2m)! (k+m)!m! (2k+2m+3)!= (-1)^m \frac{2^{k+1} \ (k + 1)! \ (2m)! \ (k + m)!}{m! \ (2k + 2m + 3)!}

=(1)m2k+1 (k+1)! (2m)! ((k+1)+m)!m! (2(k+1)+2m+1)!= (-1)^m \frac{2^{k+1} \ (k + 1)! \ (2m)! \ ((k + 1) + m)!}{m! \ (2(k + 1) + 2m + 1)!}

which is the required result for k+1k + 1

I(0,2m+1)=0π2cos(2m+1)x dx=12m+1[sin(2m+1)x]0π2I(0, 2m + 1) = \int\limits_{0}^{\frac{\pi}{2}} \cos(2m + 1)x \ dx = \frac{1}{2m + 1} \left[ \sin(2m + 1)x \right]_{0}^{\frac{\pi}{2}}

=12m+1 if m is even or =12m+1 if m is odd , or alternatively (1)m12m+1= \frac{1}{2m+1} \text{ if m is even or } = \frac{-1}{2m+1} \text{ if m is odd , or alternatively } (-1)^m \frac{1}{2m+1}

If n=0n = 0,

(1)m2n n! (2m)! (n+m)!m! (2n+2m+1)!=(1)m(2m)! (m)!m! (2m+1)!=(1)m12m+1(-1)^m \frac{2^n \ n! \ (2m)! \ (n + m)!}{m! \ (2n + 2m + 1)!} = (-1)^m \frac{(2m)! \ (m)!}{m! \ (2m + 1)!} = (-1)^m \frac{1}{2m + 1}

so result is true for n=0n = 0.

So by the principle of mathematical induction, the required result is true.

Alternative for (i)

cosaxcosbx=cosa1x[cosxcosbx]\cos^a x \cos bx = \cos^{a-1} x \left[ \cos x \cos bx \right] cosxcosbx=12[cos(b+1)x+cos(b1)x]\cos x \cos bx = \frac{1}{2} [\cos(b + 1)x + \cos(b - 1)x] 2I(a,b)=I(a1,b+1)+I(a1,b1)2I(a, b) = I(a - 1, b + 1) + I(a - 1, b - 1)

Also

sinxsinbx=12[cos(b1)xcos(b+1)x]\sin x \sin bx = \frac{1}{2} [\cos(b - 1)x - \cos(b + 1)x]

so using integration by parts of main scheme,

2I(a,b)=ab[I(a1,b1)I(a1,b+1)]2I(a, b) = \frac{a}{b} [I(a - 1, b - 1) - I(a - 1, b + 1)]

Eliminating I(a1,b+1)I(a - 1, b + 1) between these results gives required result.

Model Solution

Part (i). Integrate by parts, taking

u=cosax,dv=cosbxdx.u=\cos^a x,\qquad dv=\cos bx\,dx.

Then

du=acosa1xsinxdx,v=sinbxb.du=-a\cos^{a-1}x\sin x\,dx,\qquad v=\frac{\sin bx}{b}.

The boundary term is zero, since sinbx=0\sin bx=0 at x=0x=0 and cosax=0\cos^a x=0 at x=π2x=\frac{\pi}{2} for positive aa. Hence

I(a,b)=ab0π/2cosa1xsinxsinbxdx.I(a,b)=\frac{a}{b}\int_0^{\pi/2}\cos^{a-1}x\sin x\sin bx\,dx.

Using

cos(b1)x=cosbxcosx+sinbxsinx,\cos(b-1)x=\cos bx\cos x+\sin bx\sin x,

we get

sinxsinbx=cos(b1)xcosxcosbx.\sin x\sin bx=\cos(b-1)x-\cos x\cos bx.

Therefore

I(a,b)=ab(I(a1,b1)I(a,b)).I(a,b)=\frac{a}{b}\left(I(a-1,b-1)-I(a,b)\right).

Thus

(a+b)I(a,b)=aI(a1,b1),(a+b)I(a,b)=aI(a-1,b-1),

and so

I(a,b)=aa+bI(a1,b1).I(a,b)=\frac{a}{a+b}I(a-1,b-1).

Part (ii). We prove the result by induction on nn, with mm fixed.

For n=0n=0,

0π/2cos(2m+1)xdx=[sin(2m+1)x2m+1]0π/2=(1)m2m+1.\int_0^{\pi/2}\cos(2m+1)x\,dx =\left[\frac{\sin(2m+1)x}{2m+1}\right]_0^{\pi/2} =\frac{(-1)^m}{2m+1}.

The proposed formula gives

(1)m200!(2m)!m!m!(2m+1)!=(1)m2m+1,(-1)^m\frac{2^0\,0!\,(2m)!\,m!}{m!(2m+1)!} =\frac{(-1)^m}{2m+1},

so the base case holds.

Assume the formula holds for n=kn=k, namely

I(k,k+2m+1)=(1)m2kk!(2m)!(k+m)!m!(2k+2m+1)!.I(k,k+2m+1) =(-1)^m\frac{2^k k!(2m)!(k+m)!}{m!(2k+2m+1)!}.

Applying part (i) with a=k+1a=k+1 and b=k+2m+2b=k+2m+2 gives

I(k+1,k+2m+2)=k+12k+2m+3I(k,k+2m+1).I(k+1,k+2m+2) =\frac{k+1}{2k+2m+3}I(k,k+2m+1).

Substituting the induction hypothesis,

I(k+1,k+2m+2)=(1)m(k+1)2kk!(2m)!(k+m)!m!(2k+2m+3)(2k+2m+1)!.I(k+1,k+2m+2) =(-1)^m \frac{(k+1)2^k k!(2m)!(k+m)!}{m!(2k+2m+3)(2k+2m+1)!}.

Since 2k+2m+2=2(k+m+1)2k+2m+2=2(k+m+1), this is

(1)m2k+1(k+1)!(2m)!(k+m+1)!m!(2k+2m+3)!,(-1)^m \frac{2^{k+1}(k+1)!(2m)!(k+m+1)!}{m!(2k+2m+3)!},

which is the required formula with n=k+1n=k+1. By induction, the formula holds for all non-negative integers nn.

Examiner Notes

约70%的考生尝试本题,平均分约63%。第(i)部分常见问题是代数和符号错误,尤其是复合角公式的使用。第(ii)部分的归纳法表述常不够规范:遗漏基例、未明确归纳假设,或没有说明非负整数情形应从 n=0n=0 开始。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

2 The curve CC has equation sinhx+sinhy=2k\sinh x + \sinh y = 2k, where kk is a positive constant.

(i) Show that the curve CC has no stationary points and that d2ydx2=0\frac{d^{2}y}{dx^{2}} = 0 at the point (x,y)(x, y) on the curve if and only if 1+sinhxsinhy=0.1 + \sinh x \sinh y = 0. Find the co-ordinates of the points of inflection on the curve CC, leaving your answers in terms of inverse hyperbolic functions.

(ii) Show that if (x,y)(x, y) lies on the curve CC and on the line x+y=ax + y = a, then e2x(1ea)4kex+(ea1)=0e^{2x}(1 - e^{-a}) - 4ke^{x} + (e^{a} - 1) = 0 and deduce that 1<cosha2k2+11 < \cosh a \leqslant 2k^{2} + 1.

(iii) Sketch the curve CC.

Hint
  1. (i) sinhx+sinhy=2k\sinh x + \sinh y = 2k

Differentiating with respect to xx, coshx+coshydydx=0\cosh x + \cosh y \frac{dy}{dx} = 0

dydx=0    coshx=0\frac{dy}{dx} = 0 \implies \cosh x = 0 which is not possible as coshx1x\cosh x \geq 1 \forall x, so there are no stationary points.

Differentiating again with respect to xx, sinhx+sinhy(dydx)2+coshyd2ydx2=0\sinh x + \sinh y \left(\frac{dy}{dx}\right)^2 + \cosh y \frac{d^2y}{dx^2} = 0

dydx=coshxcoshy\frac{dy}{dx} = \frac{-\cosh x}{\cosh y} and d2ydx2=0\frac{d^2y}{dx^2} = 0 implies sinhx+sinhy(coshxcoshy)2=0\sinh x + \sinh y \left(\frac{-\cosh x}{\cosh y}\right)^2 = 0

cosh2ysinhx+cosh2xsinhy=0\cosh^2 y \sinh x + \cosh^2 x \sinh y = 0

(1+sinh2y)sinhx+(1+sinh2x)sinhy=0(1 + \sinh^2 y) \sinh x + (1 + \sinh^2 x) \sinh y = 0

(sinhx+sinhy)(1+sinhxsinhy)=0(\sinh x + \sinh y)(1 + \sinh x \sinh y) = 0

But sinhx+sinhy=2k>0\sinh x + \sinh y = 2k > 0 so

1+sinhxsinhy=01 + \sinh x \sinh y = 0

as required.

At a point of inflection, d2ydx2=0\frac{d^2y}{dx^2} = 0, so sinhx+sinhy=2k\sinh x + \sinh y = 2k and sinhxsinhy=1\sinh x \sinh y = -1 and thus, sinhx\sinh x (and sinhy\sinh y as well) is a root of λ22kλ1=0\lambda^2 - 2k\lambda - 1 = 0

λ=2k±4k2+42\lambda = \frac{2k \pm \sqrt{4k^2 + 4}}{2}

sinhx=k+k2+1\sinh x = k + \sqrt{k^2 + 1}, sinhy=1k+k2+1=1k+k2+1×kk2+1kk2+1=(kk2+1)k2(k2+1)=kk2+1\sinh y = \frac{-1}{k + \sqrt{k^2 + 1}} = \frac{-1}{k + \sqrt{k^2 + 1}} \times \frac{k - \sqrt{k^2 + 1}}{k - \sqrt{k^2 + 1}} = \frac{-(k - \sqrt{k^2 + 1})}{k^2 - (k^2 + 1)} = k - \sqrt{k^2 + 1} and vice versa.

So the points of inflection are

(sinh1(k+k2+1),sinh1(kk2+1))(\sinh^{-1}(k + \sqrt{k^2 + 1}), \sinh^{-1}(k - \sqrt{k^2 + 1})) and (sinh1(kk2+1),sinh1(k+k2+1))(\sinh^{-1}(k - \sqrt{k^2 + 1}), \sinh^{-1}(k + \sqrt{k^2 + 1}))

(ii) x+y=a    y=axx + y = a \implies y = a - x so as sinhx+sinhy=2k\sinh x + \sinh y = 2k

exex2+eaxexa2=2k\frac{e^x - e^{-x}}{2} + \frac{e^{a-x} - e^{x-a}}{2} = 2k

Multiplying by 2ex2e^x,

e2x1+eae2xea=4kexe^{2x} - 1 + e^a - e^{2x}e^{-a} = 4ke^x

e2x(1ea)4kex+(ea1)=0e^{2x}(1 - e^{-a}) - 4ke^x + (e^a - 1) = 0

As exe^x is real, 'b24ac0b^2 - 4ac \geq 0', so 16k24(1ea)(ea1)016k^2 - 4(1 - e^{-a})(e^a - 1) \geq 0

4k2eaea+204k^2 - e^a - e^{-a} + 2 \geq 0 4k22cosha+204k^2 - 2 \cosh a + 2 \geq 0

So cosha2k2+1\cosh a \leq 2k^2 + 1

If a=0a = 0, then x=yx = -y so sinhx=sinhy\sinh x = -\sinh y and thus sinhx+sinhy=2k=0\sinh x + \sinh y = 2k = 0 but k>0k > 0.

So cosha>1\cosh a > 1 as required.

(iii)

Alternative

(i) dydx=coshxcoshy\frac{dy}{dx} = \frac{-\cosh x}{\cosh y}, d2ydx2={coshysinhxcoshxsinhydydxcosh2y}={cosh2ysinhx+cosh2xsinhycosh3y}\frac{d^2y}{dx^2} = -\left\{ \frac{\cosh y \sinh x - \cosh x \sinh y \frac{dy}{dx}}{\cosh^2 y} \right\} = -\left\{ \frac{\cosh^2 y \sinh x + \cosh^2 x \sinh y}{\cosh^3 y} \right\}

then as before.

(ii) Substituting a=0a = 0 would imply ex=0e^x = 0 which is impossible.

Model Solution

Part (i). Differentiating

sinhx+sinhy=2k\sinh x+\sinh y=2k

with respect to xx gives

coshx+coshydydx=0,\cosh x+\cosh y\,\frac{dy}{dx}=0,

so

dydx=coshxcoshy.\frac{dy}{dx}=-\frac{\cosh x}{\cosh y}.

Since coshx>0\cosh x>0 and coshy>0\cosh y>0, the derivative is never zero. Hence CC has no stationary points.

Differentiating again,

sinhx+sinhy(dydx)2+coshyd2ydx2=0.\sinh x+\sinh y\left(\frac{dy}{dx}\right)^2+\cosh y\,\frac{d^2y}{dx^2}=0.

Thus d2ydx2=0\frac{d^2y}{dx^2}=0 if and only if

sinhx+sinhy(cosh2xcosh2y)=0.\sinh x+\sinh y\left(\frac{\cosh^2x}{\cosh^2y}\right)=0.

Multiplying by cosh2y\cosh^2y and using cosh2t=1+sinh2t\cosh^2t=1+\sinh^2t,

(1+sinh2y)sinhx+(1+sinh2x)sinhy=0.(1+\sinh^2y)\sinh x+(1+\sinh^2x)\sinh y=0.

This factors as

(sinhx+sinhy)(1+sinhxsinhy)=0.(\sinh x+\sinh y)(1+\sinh x\sinh y)=0.

Since sinhx+sinhy=2k>0\sinh x+\sinh y=2k>0, we must have

1+sinhxsinhy=0.1+\sinh x\sinh y=0.

At an inflection point, put X=sinhxX=\sinh x and Y=sinhyY=\sinh y. Then

X+Y=2k,XY=1.X+Y=2k,\qquad XY=-1.

So XX and YY are the roots of

λ22kλ1=0,\lambda^2-2k\lambda-1=0,

namely

λ=k±k2+1.\lambda=k\pm\sqrt{k^2+1}.

The points of inflection are therefore

(sinh1(k+k2+1), sinh1(kk2+1))\left(\sinh^{-1}(k+\sqrt{k^2+1}),\ \sinh^{-1}(k-\sqrt{k^2+1})\right)

and

(sinh1(kk2+1), sinh1(k+k2+1)).\left(\sinh^{-1}(k-\sqrt{k^2+1}),\ \sinh^{-1}(k+\sqrt{k^2+1})\right).

Part (ii). If the point also lies on x+y=ax+y=a, then y=axy=a-x. Substituting into the curve,

exex2+eaxexa2=2k.\frac{e^x-e^{-x}}{2}+\frac{e^{a-x}-e^{x-a}}{2}=2k.

Multiplying by 2ex2e^x gives

e2x1+eae2xa=4kex,e^{2x}-1+e^a-e^{2x-a}=4ke^x,

or

e2x(1ea)4kex+(ea1)=0.e^{2x}(1-e^{-a})-4ke^x+(e^a-1)=0.

This is a quadratic in exe^x, so for a real point of intersection its discriminant must be non-negative:

16k24(1ea)(ea1)0.16k^2-4(1-e^{-a})(e^a-1)\geq 0.

Now

(1ea)(ea1)=ea+ea2=2cosha2.(1-e^{-a})(e^a-1)=e^a+e^{-a}-2=2\cosh a-2.

Hence

16k24(2cosha2)0,16k^2-4(2\cosh a-2)\geq0,

so

cosha2k2+1.\cosh a\leq 2k^2+1.

Also a0a\neq0, because x+y=0x+y=0 would give y=xy=-x and hence sinhx+sinhy=0\sinh x+\sinh y=0, contradicting 2k>02k>0. Therefore cosha>1\cosh a>1, and

1<cosha2k2+1.1<\cosh a\leq 2k^2+1.

Part (iii). The curve is symmetric in xx and yy, hence symmetric about the line y=xy=x. It has no stationary points and has two inflection points found in part (i). Part (ii) shows that a line x+y=ax+y=a can meet the curve only when

1<cosha2k2+1,1<\cosh a\leq2k^2+1,

which gives the limiting range of such diagonal sections. The sketch should show a decreasing curve, symmetric about y=xy=x, passing through the two inflection points and lying in the allowed strip determined by the bounds on x+yx+y.

Examiner Notes

84%的考生尝试本题,平均分约45%。第(i)(ii)部分整体完成较好,但第(ii)部分中严格下界常被忽略。第(iii)部分作图时,很多答案没有充分利用第(ii)部分的边界条件,拐点和截距标注也不完整。曲线关于 y=xy=x 对称以及相关直线边界是作图的关键。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

3 Given distinct points AA and BB in the complex plane, the point GABG_{AB} is defined to be the centroid of the triangle ABKABK, where the point KK is the image of BB under rotation about AA through a clockwise angle of 13π\frac{1}{3}\pi.

Note: if the points PP, QQ and RR are represented in the complex plane by pp, qq and rr, the centroid of triangle PQRPQR is defined to be the point represented by 13(p+q+r)\frac{1}{3}(p + q + r).

(i) If AA, BB and GABG_{AB} are represented in the complex plane by aa, bb and gabg_{ab}, show that

gab=13(ωa+ωb),g_{ab} = \frac{1}{\sqrt{3}}(\omega a + \omega^* b),

where ω=eiπ6\omega = e^{\frac{i\pi}{6}}.

(ii) The quadrilateral Q1Q_1 has vertices AA, BB, CC and DD, in that order, and the quadrilateral Q2Q_2 has vertices GABG_{AB}, GBCG_{BC}, GCDG_{CD} and GDAG_{DA}, in that order. Using the result in part (i), show that Q1Q_1 is a parallelogram if and only if Q2Q_2 is a parallelogram.

(iii) The triangle T1T_1 has vertices AA, BB and CC and the triangle T2T_2 has vertices GABG_{AB}, GBCG_{BC} and GCAG_{CA}. Using the result in part (i), show that T2T_2 is always an equilateral triangle.

Hint
  1. (i)

ka=(ba)eiπ3k - a = (b - a)e^{-\frac{i\pi}{3}}

Therefore,

gAB=13[a+b+(a+(ba)eiπ3)]g_{AB} = \frac{1}{3} \left[ a + b + \left( a + (b - a)e^{-\frac{i\pi}{3}} \right) \right]

=a(2eiπ33)+b(1+eiπ33)= a \left( \frac{2 - e^{-\frac{i\pi}{3}}}{3} \right) + b \left( \frac{1 + e^{-\frac{i\pi}{3}}}{3} \right)

ω=eiπ6=3+i2\omega = e^{\frac{i\pi}{6}} = \frac{\sqrt{3} + i}{2}

and so

ω=3i2\omega^* = \frac{\sqrt{3} - i}{2}

2eiπ33=2(1i32)3=3+i36=133+i2=13ω\frac{2 - e^{-\frac{i\pi}{3}}}{3} = \frac{2 - \left( \frac{1 - i\sqrt{3}}{2} \right)}{3} = \frac{3 + i\sqrt{3}}{6} = \frac{1}{\sqrt{3}} \frac{\sqrt{3} + i}{2} = \frac{1}{\sqrt{3}} \omega

and

1+eiπ33=1+(1i32)3=3i36=13ω\frac{1 + e^{-\frac{i\pi}{3}}}{3} = \frac{1 + \left( \frac{1 - i\sqrt{3}}{2} \right)}{3} = \frac{3 - i\sqrt{3}}{6} = \frac{1}{\sqrt{3}} \omega^*

Thus gAB=13(ωa+ωb)g_{AB} = \frac{1}{\sqrt{3}} (\omega a + \omega^* b) as required.

(ii) gAB=13(ωa+ωb)g_{AB} = \frac{1}{\sqrt{3}} (\omega a + \omega^* b)

gBC=13(ωb+ωc)g_{BC} = \frac{1}{\sqrt{3}} (\omega b + \omega^* c)

gCD=13(ωc+ωd)g_{CD} = \frac{1}{\sqrt{3}} (\omega c + \omega^* d)

gDA=13(ωd+ωa)g_{DA} = \frac{1}{\sqrt{3}} (\omega d + \omega^* a)

Q1Q_1 parallelogram ba=cdda=cb\Rightarrow b - a = c - d \Leftrightarrow d - a = c - b

gBCgAB=13(ω(ba)+ω(cb))=13(ω(cd)+ω(da))=gCDgDAg_{BC} - g_{AB} = \frac{1}{\sqrt{3}} (\omega(b - a) + \omega^*(c - b)) = \frac{1}{\sqrt{3}} (\omega(c - d) + \omega^*(d - a)) = g_{CD} - g_{DA}

Q2\Rightarrow Q_2 parallelogram.

Q2Q_2 parallelogram gBCgAB=gCDgDA\Rightarrow g_{BC} - g_{AB} = g_{CD} - g_{DA}

13{ω[(ba)(cd)]+ω[(cb)(da)]}=0\frac{1}{\sqrt{3}} \{ \omega[(b - a) - (c - d)] + \omega^*[(c - b) - (d - a)] \} = 0

13(ωω)[(ab)(dc)]=0\frac{1}{\sqrt{3}} (\omega^* - \omega) [(a - b) - (d - c)] = 0

As ωω0\omega^* - \omega \neq 0, (ab)(dc)=0(a - b) - (d - c) = 0 and so Q1Q_1 is a parallelogram

(iii) gBCgAB=13(ω(ba)+ω(cb))g_{BC} - g_{AB} = \frac{1}{\sqrt{3}}(\omega(b - a) + \omega^*(c - b)) gCAgAB=13(ω(ca)+ω(ab))(1)g_{CA} - g_{AB} = \frac{1}{\sqrt{3}}(\omega(c - a) + \omega^*(a - b)) \quad (1) ω2(gBCgAB)=13(ω3(ba)+ω(cb))(2)\omega^2(g_{BC} - g_{AB}) = \frac{1}{\sqrt{3}}(\omega^3(b - a) + \omega(c - b)) \quad (2) =13(i(ba)+ω(cb))= \frac{1}{\sqrt{3}}(i(b - a) + \omega(c - b))

The coefficient of 13a\frac{1}{\sqrt{3}}a in (1) is ωω=3i23+i2=i\omega^* - \omega = \frac{\sqrt{3}-i}{2} - \frac{\sqrt{3}+i}{2} = -i The coefficient of 13b\frac{1}{\sqrt{3}}b in (1) is ω=(iω)-\omega^* = (i - \omega) The coefficient of 13c\frac{1}{\sqrt{3}}c in (1) is ω\omega

Thus GABGBCG_{AB}G_{BC} rotated through π3\frac{\pi}{3} is GABGCAG_{AB}G_{CA} which means that GABGBCGCAG_{AB}G_{BC}G_{CA} is an equilateral triangle.

(iii) Alternative

x=gBCgAB=13(ω(ba)+ω(cb))x = g_{BC} - g_{AB} = \frac{1}{\sqrt{3}}(\omega(b - a) + \omega^*(c - b)) y=gCAgAB=13(ω(ca)+ω(ab))y = g_{CA} - g_{AB} = \frac{1}{\sqrt{3}}(\omega(c - a) + \omega^*(a - b)) x=13(eiπ6beiπ6a+eiπ6ceiπ6b)x = \frac{1}{\sqrt{3}}\left(e^{\frac{i\pi}{6}}b - e^{\frac{i\pi}{6}}a + e^{\frac{-i\pi}{6}}c - e^{\frac{-i\pi}{6}}b\right) =13(eiπ2b+eiπ6c+ei7π6a)= \frac{1}{\sqrt{3}}\left(e^{\frac{i\pi}{2}}b + e^{\frac{-i\pi}{6}}c + e^{\frac{i7\pi}{6}}a\right) y=13(eiπ6c+ei3π2a+ei5π6b)y = \frac{1}{\sqrt{3}}\left(e^{\frac{i\pi}{6}}c + e^{\frac{i3\pi}{2}}a + e^{\frac{i5\pi}{6}}b\right) yx=eiπ3\frac{y}{x} = e^{\frac{i\pi}{3}}

eiπ3e^{\frac{i\pi}{3}} means yy is xx rotated through π3\frac{\pi}{3} and thus GABGBCGCAG_{AB}G_{BC}G_{CA} is an equilateral triangle.

[or alternatively

yx=1\left| \frac{y}{x} \right| = 1 and similarly zy=1\left| \frac{z}{y} \right| = 1 and thus all three sides are equal length]

Model Solution

Part (i)

The point KK is obtained by rotating BB about AA through a clockwise angle of π3\frac{\pi}{3}. A clockwise rotation corresponds to multiplication by eiπ/3e^{-i\pi/3} in the complex plane. To rotate BB about AA:

  1. Translate so that AA is at the origin: bab - a.
  2. Apply the rotation: (ba)eiπ/3(b - a)e^{-i\pi/3}.
  3. Translate back: k=a+(ba)eiπ/3k = a + (b - a)e^{-i\pi/3}.

The centroid of triangle ABKABK is:

gab=13(a+b+k)=13(a+b+a+(ba)eiπ/3)g_{ab} = \frac{1}{3}(a + b + k) = \frac{1}{3}\left(a + b + a + (b - a)e^{-i\pi/3}\right) =13(2a+b+(ba)eiπ/3)= \frac{1}{3}\left(2a + b + (b - a)e^{-i\pi/3}\right) =13(a(2eiπ/3)+b(1+eiπ/3))()= \frac{1}{3}\left(a(2 - e^{-i\pi/3}) + b(1 + e^{-i\pi/3})\right) \qquad (*)

Now evaluate the two coefficients. Since eiπ/3=cosπ3isinπ3=1232ie^{-i\pi/3} = \cos\frac{\pi}{3} - i\sin\frac{\pi}{3} = \frac{1}{2} - \frac{\sqrt{3}}{2}i:

2eiπ/3=212+32i=32+32i2 - e^{-i\pi/3} = 2 - \frac{1}{2} + \frac{\sqrt{3}}{2}i = \frac{3}{2} + \frac{\sqrt{3}}{2}i 1+eiπ/3=1+1232i=3232i1 + e^{-i\pi/3} = 1 + \frac{1}{2} - \frac{\sqrt{3}}{2}i = \frac{3}{2} - \frac{\sqrt{3}}{2}i

With ω=eiπ/6=3+i2\omega = e^{i\pi/6} = \frac{\sqrt{3}+i}{2} and ω=3i2\omega^* = \frac{\sqrt{3}-i}{2}:

3ω=33+i2=3+i32=32+32i=2eiπ/3\sqrt{3}\,\omega = \sqrt{3}\cdot\frac{\sqrt{3}+i}{2} = \frac{3+i\sqrt{3}}{2} = \frac{3}{2} + \frac{\sqrt{3}}{2}i = 2 - e^{-i\pi/3} 3ω=33i2=3i32=3232i=1+eiπ/3\sqrt{3}\,\omega^* = \sqrt{3}\cdot\frac{\sqrt{3}-i}{2} = \frac{3-i\sqrt{3}}{2} = \frac{3}{2} - \frac{\sqrt{3}}{2}i = 1 + e^{-i\pi/3}

Substituting into ()(*):

gab=13(3ωa+3ωb)=13(ωa+ωb)g_{ab} = \frac{1}{3}\left(\sqrt{3}\,\omega\cdot a + \sqrt{3}\,\omega^*\cdot b\right) = \frac{1}{\sqrt{3}}(\omega a + \omega^* b)

Part (ii)

From part (i), the four centroid points are:

gAB=13(ωa+ωb),gBC=13(ωb+ωc)g_{AB} = \frac{1}{\sqrt{3}}(\omega a + \omega^* b), \qquad g_{BC} = \frac{1}{\sqrt{3}}(\omega b + \omega^* c) gCD=13(ωc+ωd),gDA=13(ωd+ωa)g_{CD} = \frac{1}{\sqrt{3}}(\omega c + \omega^* d), \qquad g_{DA} = \frac{1}{\sqrt{3}}(\omega d + \omega^* a)

Q1Q_1 is a parallelogram if and only if its opposite sides are equal, i.e. ba=cdb - a = c - d.

Q2Q_2 is a parallelogram if and only if gBCgAB=gCDgDAg_{BC} - g_{AB} = g_{CD} - g_{DA}.

Compute the two sides of Q2Q_2:

gBCgAB=13(ω(ba)+ω(cb))g_{BC} - g_{AB} = \frac{1}{\sqrt{3}}\left(\omega(b - a) + \omega^*(c - b)\right) gCDgDA=13(ω(cd)+ω(da))g_{CD} - g_{DA} = \frac{1}{\sqrt{3}}\left(\omega(c - d) + \omega^*(d - a)\right)

So Q2Q_2 is a parallelogram if and only if:

ω(ba)+ω(cb)=ω(cd)+ω(da)\omega(b - a) + \omega^*(c - b) = \omega(c - d) + \omega^*(d - a)

Rearranging:

ω[(ba)(cd)]+ω[(cb)(da)]=0\omega\left[(b - a) - (c - d)\right] + \omega^*\left[(c - b) - (d - a)\right] = 0

Since (cb)(da)=(cd)(ba)=[(ba)(cd)](c - b) - (d - a) = (c - d) - (b - a) = -\left[(b - a) - (c - d)\right], this becomes:

[ωω][(ba)(cd)]=0\left[\omega - \omega^*\right]\left[(b - a) - (c - d)\right] = 0

Now ωω=3+i23i2=i0\omega - \omega^* = \frac{\sqrt{3}+i}{2} - \frac{\sqrt{3}-i}{2} = i \neq 0, so:

Q2 is a parallelogram    (ba)(cd)=0    ba=cdQ_2 \text{ is a parallelogram} \iff (b - a) - (c - d) = 0 \iff b - a = c - d

This is exactly the condition for Q1Q_1 to be a parallelogram. Therefore Q1Q_1 is a parallelogram if and only if Q2Q_2 is a parallelogram.

Part (iii)

The two side vectors of T2T_2 emanating from GABG_{AB} are:

GBCGAB=13(ω(ba)+ω(cb))(1)G_{BC} - G_{AB} = \frac{1}{\sqrt{3}}\left(\omega(b - a) + \omega^*(c - b)\right) \qquad (1) GABGCA=13(ω(ac)+ω(ba))(2)G_{AB} - G_{CA} = \frac{1}{\sqrt{3}}\left(\omega(a - c) + \omega^*(b - a)\right) \qquad (2)

We show that multiplying (1) by ω2\omega^2 gives (2)-(2), so that the two sides are related by a rotation of π3\frac{\pi}{3}.

Compute ω2\omega^2 times (1):

ω2(GBCGAB)=13(ω3(ba)+ω2ω(cb))\omega^2(G_{BC} - G_{AB}) = \frac{1}{\sqrt{3}}\left(\omega^3(b - a) + \omega^2\omega^*(c - b)\right)

Since ω=1|\omega| = 1 we have ω=ω1\omega^* = \omega^{-1}, so ω2ω=ω\omega^2\omega^* = \omega. Also ω3=eiπ/2=i\omega^3 = e^{i\pi/2} = i. Therefore:

ω2(GBCGAB)=13(i(ba)+ω(cb))(3)\omega^2(G_{BC} - G_{AB}) = \frac{1}{\sqrt{3}}\left(i(b - a) + \omega(c - b)\right) \qquad (3)

Now expand (2):

GABGCA=13(ωaωc+ωbωa)=13((ωω)a+ωbωc)G_{AB} - G_{CA} = \frac{1}{\sqrt{3}}\left(\omega a - \omega c + \omega^* b - \omega^* a\right) = \frac{1}{\sqrt{3}}\left((\omega - \omega^*)a + \omega^* b - \omega c\right)

Since ωω=i\omega - \omega^* = i:

GABGCA=13(ia+ωbωc)(4)G_{AB} - G_{CA} = \frac{1}{\sqrt{3}}\left(ia + \omega^* b - \omega c\right) \qquad (4)

Expand (3):

13(ia+ib+ωcωb)=13(ia+(iω)b+ωc)\frac{1}{\sqrt{3}}\left(-ia + ib + \omega c - \omega b\right) = \frac{1}{\sqrt{3}}\left(-ia + (i - \omega)b + \omega c\right)

We check that iω=ωi - \omega = -\omega^*:

iω=i3+i2=2i3i2=i32=3i2=ωi - \omega = i - \frac{\sqrt{3}+i}{2} = \frac{2i - \sqrt{3} - i}{2} = \frac{i - \sqrt{3}}{2} = -\frac{\sqrt{3}-i}{2} = -\omega^*

So (3) becomes:

ω2(GBCGAB)=13(iaωb+ωc)\omega^2(G_{BC} - G_{AB}) = \frac{1}{\sqrt{3}}\left(-ia - \omega^* b + \omega c\right)

Comparing with (4), every coefficient in (3) is the negative of the corresponding coefficient in (4), so:

ω2(GBCGAB)=(GABGCA)\omega^2(G_{BC} - G_{AB}) = -(G_{AB} - G_{CA})

Rearranging:

GCAGAB=ω2(GBCGAB)G_{CA} - G_{AB} = \omega^2(G_{BC} - G_{AB})

Since ω2=1|\omega^2| = 1 and arg(ω2)=π3\arg(\omega^2) = \frac{\pi}{3}, the vector from GABG_{AB} to GCAG_{CA} is obtained from the vector from GABG_{AB} to GBCG_{BC} by a rotation through π3\frac{\pi}{3}. Therefore:

  • GCAGAB=GBCGAB|G_{CA} - G_{AB}| = |G_{BC} - G_{AB}| (the two sides from vertex GABG_{AB} have equal length);
  • the angle at vertex GABG_{AB} is π3\frac{\pi}{3} (60 degrees).

A triangle with two equal sides and an included angle of 6060^\circ is equilateral (by the cosine rule, the third side equals the other two, and all angles are 6060^\circ). Therefore T2T_2 is always an equilateral triangle.

Examiner Notes

这是较少人选择的纯数题。第(i)部分常见错误是把旋转方向搞反,或遗漏平移项。第(ii)部分中,许多考生试图同时证明两个方向;从 Q2Q_2 出发的证明通常更清楚。第(iii)部分需要用复数计算模长,把相关复数误当作实数是常见错误。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

4 The plane Π\Pi has equation rn=0\mathbf{r} \cdot \mathbf{n} = 0 where n\mathbf{n} is a unit vector. Let PP be a point with position vector x\mathbf{x} which does not lie on the plane Π\Pi. Show that the point QQ with position vector x(xn)n\mathbf{x} - (\mathbf{x} \cdot \mathbf{n})\mathbf{n} lies on Π\Pi and that PQPQ is perpendicular to Π\Pi.

(i) Let transformation TT be a reflection in the plane ax+by+cz=0ax + by + cz = 0, where a2+b2+c2=1a^2 + b^2 + c^2 = 1.

Show that the image of i=(100)\mathbf{i} = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} under TT is (b2+c2a22ab2ac)\begin{pmatrix} b^2 + c^2 - a^2 \\ -2ab \\ -2ac \end{pmatrix}, and find the images of j\mathbf{j} and k\mathbf{k} under TT.

Write down the matrix M\mathbf{M} which represents transformation TT.

(ii) The matrix

(0.640.480.60.480.360.80.60.80)\begin{pmatrix} 0.64 & 0.48 & 0.6 \\ 0.48 & 0.36 & -0.8 \\ 0.6 & -0.8 & 0 \end{pmatrix}

represents a reflection in a plane. Find the cartesian equation of the plane.

(iii) The matrix N\mathbf{N} represents a rotation through angle π\pi about the line through the origin parallel to (abc)\begin{pmatrix} a \\ b \\ c \end{pmatrix}, where a2+b2+c2=1a^2 + b^2 + c^2 = 1. Find the matrix N\mathbf{N}.

(iv) Identify the single transformation which is represented by the matrix NM\mathbf{NM}.

Hint
  1. π\pi has equation r.n=0r.n = 0 so nn is a vector perpendicular to this plane.

QQ lies on π\pi if x(x.n)nx - (x.n)n satisfies r.n=0r.n = 0

(x(x.n)n).n=x.n(x.n)n.n=x.nx.n=0(x - (x.n)n).n = x.n - (x.n)n.n = x.n - x.n = 0 so QQ lies on π\pi as required.

PQ=(x(x.n)n)x=(x.n)nPQ = (x - (x.n)n) - x = -(x.n)n which is parallel to nn and so is perpendicular to π\pi.

(i) The image of a point with position vector xx under TT is x2(x.n)nx - 2(x.n)n, so as n=(abc)n = \begin{pmatrix} a \\ b \\ c \end{pmatrix} and

i=(100)i = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix}, the image of ii under TT is (100)2((100).(abc))(abc)=(100)2a(abc)=(12a22ab2ac)\begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} - 2 \left( \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} . \begin{pmatrix} a \\ b \\ c \end{pmatrix} \right) \begin{pmatrix} a \\ b \\ c \end{pmatrix} = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} - 2a \begin{pmatrix} a \\ b \\ c \end{pmatrix} = \begin{pmatrix} 1 - 2a^2 \\ -2ab \\ -2ac \end{pmatrix}

But a2+b2+c2=1a^2 + b^2 + c^2 = 1 so 12a2=a2+b2+c22a2=b2+c2a21 - 2a^2 = a^2 + b^2 + c^2 - 2a^2 = b^2 + c^2 - a^2

Thus, the image of ii under TT is (b2+c2a22ab2ac)\begin{pmatrix} b^2 + c^2 - a^2 \\ -2ab \\ -2ac \end{pmatrix} as required.

Similarly, the images of jj and kk are (2abc2+a2b22bc)\begin{pmatrix} -2ab \\ c^2 + a^2 - b^2 \\ -2bc \end{pmatrix} and (2ac2bca2+b2c2)\begin{pmatrix} -2ac \\ -2bc \\ a^2 + b^2 - c^2 \end{pmatrix} respectively.

Thus M=(b2+c2a22ab2ac2abc2+a2b22bc2ac2bca2+b2c2)M = \begin{pmatrix} b^2 + c^2 - a^2 & -2ab & -2ac \\ -2ab & c^2 + a^2 - b^2 & -2bc \\ -2ac & -2bc & a^2 + b^2 - c^2 \end{pmatrix}

(ii) 12a2=0.64a=±0.321 - 2a^2 = 0.64 \Rightarrow a = \pm 0.3\sqrt{2} and thus as 2ab=0.48-2ab = 0.48 and 2ac=0.6-2ac = 0.6,

b=0.42b = \mp 0.4\sqrt{2} and c=0.52c = \mp 0.5\sqrt{2} and the plane is 3x4y5z=03x - 4y - 5z = 0 (or 3x+4y+5z=0-3x + 4y + 5z = 0)

(iii) Suppose the position vector of the point QQ on the given line such that PQPQ is perpendicular to that line is yy, then y=λ(abc)y = \lambda \begin{pmatrix} a \\ b \\ c \end{pmatrix} for some λ\lambda and (yx).(abc)=0(y - x) . \begin{pmatrix} a \\ b \\ c \end{pmatrix} = 0

So, y.(abc)x.(abc)=0y . \begin{pmatrix} a \\ b \\ c \end{pmatrix} - x . \begin{pmatrix} a \\ b \\ c \end{pmatrix} = 0, i.e. λ=x.(abc)\lambda = x . \begin{pmatrix} a \\ b \\ c \end{pmatrix}

So, the image of PP under the rotation, is x+2(yx)=2yx=2x.(abc)(abc)xx + 2(y - x) = 2y - x = 2x . \begin{pmatrix} a \\ b \\ c \end{pmatrix} \begin{pmatrix} a \\ b \\ c \end{pmatrix} - x

The image of ii under the rotation is thus (2a212ab2ac)=(a2b2c22ab2ac)\begin{pmatrix} 2a^2 - 1 \\ 2ab \\ 2ac \end{pmatrix} = \begin{pmatrix} a^2 - b^2 - c^2 \\ 2ab \\ 2ac \end{pmatrix}, and of jj and kk are (2abb2c2a22bc)\begin{pmatrix} 2ab \\ b^2 - c^2 - a^2 \\ 2bc \end{pmatrix} and (2ac2bcc2a2b2)\begin{pmatrix} 2ac \\ 2bc \\ c^2 - a^2 - b^2 \end{pmatrix} respectively.

Thus N=(a2b2c22ab2ac2abb2c2a22bc2ac2bcc2a2b2)N = \begin{pmatrix} a^2 - b^2 - c^2 & 2ab & 2ac \\ 2ab & b^2 - c^2 - a^2 & 2bc \\ 2ac & 2bc & c^2 - a^2 - b^2 \end{pmatrix}, which, incidentally =M= -M.

(iv) NM=MM=INM = -MM = -I as MM is self-inverse.

Thus the single transformation is an enlargement, scale factor -1, with centre of enlargement the origin.

alternative for (iii)

x=u+vx = u + v where uΠu \in \Pi and vΠv \perp \Pi

Mv=vMu=uMx=uvMv = -v \qquad Mu = u \qquad Mx = u - v

Nx=vu=MxNx = v - u = -Mx

N=MN = -M

alternative for (ii) the matrix represents a reflection, an invariant point under the reflection lies on the plane of reflection.

Therefore,

(0.640.480.60.480.360.80.60.80)(xyz)=(xyz)\begin{pmatrix} 0.64 & 0.48 & 0.6 \\ 0.48 & 0.36 & -0.8 \\ 0.6 & -0.8 & 0 \end{pmatrix} \begin{pmatrix} x \\ y \\ z \end{pmatrix} = \begin{pmatrix} x \\ y \\ z \end{pmatrix}

Taking the simplest component equation

0.6x0.8y=z0.6x - 0.8y = z

(although the other two give equivalent equations).

This simplifies to

3x4y5z=03x - 4y - 5z = 0

Model Solution

Preliminary

QQ has position vector q=x(xn)n\mathbf{q} = \mathbf{x} - (\mathbf{x} \cdot \mathbf{n})\mathbf{n}.

To show QQ lies on Π\Pi, we verify qn=0\mathbf{q} \cdot \mathbf{n} = 0:

qn=xn(xn)(nn)=xnxn=0\mathbf{q} \cdot \mathbf{n} = \mathbf{x} \cdot \mathbf{n} - (\mathbf{x} \cdot \mathbf{n})(\mathbf{n} \cdot \mathbf{n}) = \mathbf{x} \cdot \mathbf{n} - \mathbf{x} \cdot \mathbf{n} = 0

using nn=1\mathbf{n} \cdot \mathbf{n} = 1 (since n\mathbf{n} is a unit vector). So QQ lies on Π\Pi.

The vector PQ=qx=(xn)n\overrightarrow{PQ} = \mathbf{q} - \mathbf{x} = -(\mathbf{x} \cdot \mathbf{n})\mathbf{n}, which is a scalar multiple of n\mathbf{n}. Since n\mathbf{n} is perpendicular to Π\Pi, the line PQPQ is perpendicular to Π\Pi.

Part (i)

The reflection TT in the plane ax+by+cz=0ax + by + cz = 0 (with n=(a,b,c)T\mathbf{n} = (a, b, c)^T a unit vector) maps a point with position vector r\mathbf{r} to r2(rn)n\mathbf{r} - 2(\mathbf{r} \cdot \mathbf{n})\mathbf{n}. This follows from the preliminary result: the reflection sends PP to the point on the other side of the plane at the same distance, which is Q+PQ=x2(xn)nQ+\overrightarrow{PQ}=\mathbf{x}-2(\mathbf{x}\cdot\mathbf{n})\mathbf{n}.

Image of i\mathbf{i}:

T(i)=(100)2((100)(abc))(abc)=(100)2a(abc)=(12a22ab2ac)T(\mathbf{i}) = \begin{pmatrix}1\\0\\0\end{pmatrix} - 2\left(\begin{pmatrix}1\\0\\0\end{pmatrix}\cdot\begin{pmatrix}a\\b\\c\end{pmatrix}\right)\begin{pmatrix}a\\b\\c\end{pmatrix} = \begin{pmatrix}1\\0\\0\end{pmatrix} - 2a\begin{pmatrix}a\\b\\c\end{pmatrix} = \begin{pmatrix}1-2a^2\\-2ab\\-2ac\end{pmatrix}

Since a2+b2+c2=1a^2 + b^2 + c^2 = 1: 12a2=(a2+b2+c2)2a2=b2+c2a21 - 2a^2 = (a^2 + b^2 + c^2) - 2a^2 = b^2 + c^2 - a^2.

T(i)=(b2+c2a22ab2ac)T(\mathbf{i}) = \begin{pmatrix}b^2+c^2-a^2\\-2ab\\-2ac\end{pmatrix}

Image of j\mathbf{j}:

T(j)=(010)2b(abc)=(2ab12b22bc)=(2aba2+c2b22bc)T(\mathbf{j}) = \begin{pmatrix}0\\1\\0\end{pmatrix} - 2b\begin{pmatrix}a\\b\\c\end{pmatrix} = \begin{pmatrix}-2ab\\1-2b^2\\-2bc\end{pmatrix} = \begin{pmatrix}-2ab\\a^2+c^2-b^2\\-2bc\end{pmatrix}

Image of k\mathbf{k}:

T(k)=(001)2c(abc)=(2ac2bc12c2)=(2ac2bca2+b2c2)T(\mathbf{k}) = \begin{pmatrix}0\\0\\1\end{pmatrix} - 2c\begin{pmatrix}a\\b\\c\end{pmatrix} = \begin{pmatrix}-2ac\\-2bc\\1-2c^2\end{pmatrix} = \begin{pmatrix}-2ac\\-2bc\\a^2+b^2-c^2\end{pmatrix}

The columns of M\mathbf{M} are the images of i\mathbf{i}, j\mathbf{j}, k\mathbf{k}:

M=(b2+c2a22ab2ac2aba2+c2b22bc2ac2bca2+b2c2)\mathbf{M} = \begin{pmatrix}b^2+c^2-a^2 & -2ab & -2ac \\ -2ab & a^2+c^2-b^2 & -2bc \\ -2ac & -2bc & a^2+b^2-c^2\end{pmatrix}

Part (ii)

We match the given matrix entries against M\mathbf{M}.

From the (1,1)(1,1) entry: b2+c2a2=0.64b^2 + c^2 - a^2 = 0.64. Since a2+b2+c2=1a^2 + b^2 + c^2 = 1, we get 12a2=0.641 - 2a^2 = 0.64, so a2=0.18a^2 = 0.18.

From the (1,2)(1,2) entry: 2ab=0.48-2ab = 0.48, so ab=0.24ab = -0.24.

From the (1,3)(1,3) entry: 2ac=0.6-2ac = 0.6, so ac=0.3ac = -0.3.

Taking a2=0.18a^2 = 0.18, so a=±3102=±0.32a = \pm\frac{3}{10}\sqrt{2} = \pm 0.3\sqrt{2}.

Taking a=0.32a = 0.3\sqrt{2}:

b=0.240.32=0.82=0.42b = \frac{-0.24}{0.3\sqrt{2}} = \frac{-0.8}{\sqrt{2}} = -0.4\sqrt{2} c=0.30.32=12=0.52c = \frac{-0.3}{0.3\sqrt{2}} = \frac{-1}{\sqrt{2}} = -0.5\sqrt{2}

Verification: a2+b2+c2=0.18+0.32+0.5=1a^2 + b^2 + c^2 = 0.18 + 0.32 + 0.5 = 1. ✓

Check remaining entries:

  • (2,2)(2,2): a2+c2b2=0.18+0.50.32=0.36a^2 + c^2 - b^2 = 0.18 + 0.5 - 0.32 = 0.36
  • (2,3)(2,3): 2bc=2(0.42)(0.52)=2(0.4)(0.5)(2)=0.8-2bc = -2(-0.4\sqrt{2})(-0.5\sqrt{2}) = -2(0.4)(0.5)(2) = -0.8
  • (3,3)(3,3): a2+b2c2=0.18+0.320.5=0a^2 + b^2 - c^2 = 0.18 + 0.32 - 0.5 = 0

The plane equation is ax+by+cz=0ax + by + cz = 0:

0.32x0.42y0.52z=00.3\sqrt{2}\,x - 0.4\sqrt{2}\,y - 0.5\sqrt{2}\,z = 0

Dividing by 0.120.1\sqrt{2}:

3x4y5z=03x - 4y - 5z = 0

(The alternative sign choice a=0.32a = -0.3\sqrt{2} gives 3x+4y+5z=0-3x + 4y + 5z = 0, which is the same plane.)

Part (iii)

A rotation through angle π\pi about a line through the origin maps each point to its reflection in that line. For a unit direction vector n=(a,b,c)T\mathbf{n} = (a, b, c)^T, the foot of the perpendicular from x\mathbf{x} to the line is (xn)n(\mathbf{x} \cdot \mathbf{n})\mathbf{n}. The image of x\mathbf{x} is the point diametrically opposite across the foot:

T(x)=2(xn)nxT(\mathbf{x}) = 2(\mathbf{x} \cdot \mathbf{n})\mathbf{n} - \mathbf{x}

Image of i\mathbf{i}:

N(i)=2a(abc)(100)=(2a212ab2ac)\mathbf{N}(\mathbf{i}) = 2a\begin{pmatrix}a\\b\\c\end{pmatrix} - \begin{pmatrix}1\\0\\0\end{pmatrix} = \begin{pmatrix}2a^2-1\\2ab\\2ac\end{pmatrix}

Since 2a21=2a2(a2+b2+c2)=a2b2c22a^2 - 1 = 2a^2 - (a^2+b^2+c^2) = a^2 - b^2 - c^2:

N(i)=(a2b2c22ab2ac)\mathbf{N}(\mathbf{i}) = \begin{pmatrix}a^2-b^2-c^2\\2ab\\2ac\end{pmatrix}

Similarly:

N(j)=(2abb2a2c22bc),N(k)=(2ac2bcc2a2b2)\mathbf{N}(\mathbf{j}) = \begin{pmatrix}2ab\\b^2-a^2-c^2\\2bc\end{pmatrix}, \qquad \mathbf{N}(\mathbf{k}) = \begin{pmatrix}2ac\\2bc\\c^2-a^2-b^2\end{pmatrix} N=(a2b2c22ab2ac2abb2a2c22bc2ac2bcc2a2b2)\mathbf{N} = \begin{pmatrix}a^2-b^2-c^2 & 2ab & 2ac \\ 2ab & b^2-a^2-c^2 & 2bc \\ 2ac & 2bc & c^2-a^2-b^2\end{pmatrix}

Comparing with M\mathbf{M}, every entry of N\mathbf{N} is the negative of the corresponding entry of M\mathbf{M}, so N=M\mathbf{N} = -\mathbf{M}.

Part (iv)

NM=(M)M=M2\mathbf{NM} = (-\mathbf{M})\mathbf{M} = -\mathbf{M}^2

Since M\mathbf{M} represents a reflection, it is self-inverse: M1=M\mathbf{M}^{-1} = \mathbf{M}, and since M2=MM1=I\mathbf{M}^2 = \mathbf{M}\mathbf{M}^{-1} = \mathbf{I}:

NM=I\mathbf{NM} = -\mathbf{I}

The matrix I-\mathbf{I} maps every vector x\mathbf{x} to x-\mathbf{x}. This is an enlargement with scale factor 1-1 and centre the origin (equivalently, a point reflection or inversion through the origin).

Examiner Notes

本题不太受欢迎,但尝试者在各小问中的基本思路通常正确。第(i)部分即使没有完全使用题干,多数考生也能用对称性求出 j\mathbf{j}k\mathbf{k} 的像。第(ii)部分方程求解较直接,但计算错误较常见。第(iii)部分需要类比第(i)部分的技术。第(iv)部分描述变换时常见错误是说成“关于原点的旋转”,而没有明确这是半转。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

5 Show that for positive integer nn, xnyn=(xy)r=1nxnryr1x^n - y^n = (x - y) \sum_{r=1}^{n} x^{n-r} y^{r-1}.

(i) Let F be defined by

F(x)=1xn(xk)for x0,kF(x) = \frac{1}{x^n(x - k)} \quad \text{for } x \neq 0, k

where nn is a positive integer and k0k \neq 0.

(a) Given that

F(x)=Axk+f(x)xn,F(x) = \frac{A}{x - k} + \frac{f(x)}{x^n},

where AA is a constant and f(x)f(x) is a polynomial, show that

f(x)=1xk(1(xk)n).f(x) = \frac{1}{x - k} \left( 1 - \left( \frac{x}{k} \right)^n \right).

Deduce that

F(x)=1kn(xk)1kr=1n1knrxr.F(x) = \frac{1}{k^n(x - k)} - \frac{1}{k} \sum_{r=1}^{n} \frac{1}{k^{n-r} x^r}.

(b) By differentiating xnF(x)x^n F(x), prove that

1xn(xk)2=1kn(xk)2nxkn(xk)+r=1nnrkn+1rxr+1.\frac{1}{x^n(x - k)^2} = \frac{1}{k^n(x - k)^2} - \frac{n}{x k^n(x - k)} + \sum_{r=1}^{n} \frac{n - r}{k^{n+1-r} x^{r+1}}.

(ii) Hence evaluate the limit of

2N1x3(x1)2 dx\int_{2}^{N} \frac{1}{x^3(x - 1)^2} \text{ d}x

as NN \to \infty, justifying your answer.

Hint
  1. (xy)(xn1+xn2y++yn1)=xnxn1y+xn1yxn2y++xyn1yn(x - y)(x^{n-1} + x^{n-2}y + \dots + y^{n-1}) = x^n - x^{n-1}y + x^{n-1}y - x^{n-2}y + \dots + xy^{n-1} - y^n

=xnyn= x^n - y^n

as each even numbered term cancels with its subsequent term.

(i) If

F(x)=1xn(xk)=Axk+f(x)xnF(x) = \frac{1}{x^n(x - k)} = \frac{A}{x - k} + \frac{f(x)}{x^n}

then multiplying by xn(xk)x^n(x - k)

1=Axn+(xk)f(x)1 = Ax^n + (x - k)f(x)

x=kA=1knx = k \Rightarrow A = \frac{1}{k^n}

so

1=xnkn+(xk)f(x)1 = \frac{x^n}{k^n} + (x - k)f(x)

and

f(x)=1xk(1(xk)n)f(x) = \frac{1}{x - k} \left( 1 - \left( \frac{x}{k} \right)^n \right)

as required.

Thus

F(x)=1knxk+1xk(1(xk)n)xnF(x) = \frac{\frac{1}{k^n}}{x - k} + \frac{\frac{1}{x - k} \left( 1 - \left( \frac{x}{k} \right)^n \right)}{x^n}

=1kn(xk)xnknknxn(xk)= \frac{1}{k^n(x - k)} - \frac{x^n - k^n}{k^n x^n (x - k)}

and so, by the result of the stem,

F(x)=1kn(xk)1knxnr=1nxnrkr1F(x) = \frac{1}{k^n(x - k)} - \frac{1}{k^n x^n} \sum_{r=1}^{n} x^{n-r} k^{r-1}

=1kn(xk)1kr=1n1knrxr= \frac{1}{k^n(x - k)} - \frac{1}{k} \sum_{r=1}^{n} \frac{1}{k^{n-r} x^r}

(ii) xnF(x)=1xk=xnkn(xk)1kr=1nxnrknrx^n F(x) = \frac{1}{x - k} = \frac{x^n}{k^n(x - k)} - \frac{1}{k} \sum_{r=1}^{n} \frac{x^{n-r}}{k^{n-r}}

Differentiating with respect to xx,

1(xk)2=nxn1kn(xk)xnkn(xk)21kr=1n(nr)xnr1knr\frac{-1}{(x - k)^2} = \frac{nx^{n-1}}{k^n(x - k)} - \frac{x^n}{k^n(x - k)^2} - \frac{1}{k} \sum_{r=1}^{n} \frac{(n - r)x^{n-r-1}}{k^{n-r}}

Multiplying by 1xn\frac{-1}{x^n}

1xn(xk)2=nxkn(xk)+1kn(xk)2+r=1nnrkn+1rxr+1\frac{1}{x^n(x - k)^2} = \frac{-n}{xk^n(x - k)} + \frac{1}{k^n(x - k)^2} + \sum_{r=1}^{n} \frac{n - r}{k^{n+1-r}x^{r+1}}

(iii) 2N1x3(x1)2dx=2N3x(x1)+1(x1)2+r=133rxr+1dx\int_{2}^{N} \frac{1}{x^3(x - 1)^2} dx = \int_{2}^{N} \frac{-3}{x(x - 1)} + \frac{1}{(x - 1)^2} + \sum_{r=1}^{3} \frac{3 - r}{x^{r+1}} dx

=2N3x3(x1)+1(x1)2+r=133rxr+1dx= \int_{2}^{N} \frac{3}{x} - \frac{3}{(x - 1)} + \frac{1}{(x - 1)^2} + \sum_{r=1}^{3} \frac{3 - r}{x^{r+1}} dx

=[3lnx3ln(x1)1x1r=133rrxr]2N= \left[ 3 \ln x - 3 \ln(x - 1) - \frac{1}{x - 1} - \sum_{r=1}^{3} \frac{3 - r}{rx^r} \right]_{2}^{N} =[3ln(xx1)1x1r=133rrxr]2N= \left[ 3 \ln \left( \frac{x}{x - 1} \right) - \frac{1}{x - 1} - \sum_{r=1}^{3} \frac{3 - r}{rx^r} \right]_{2}^{N}

=3ln(NN1)1N1r=133rrNr3ln(2)+1+r=133rr2r= 3 \ln \left( \frac{N}{N - 1} \right) - \frac{1}{N - 1} - \sum_{r=1}^{3} \frac{3 - r}{rN^r} - 3 \ln(2) + 1 + \sum_{r=1}^{3} \frac{3 - r}{r2^r}

As NN \to \infty, (NN1)1\left( \frac{N}{N-1} \right) \to 1, so 3ln(NN1)03 \ln \left( \frac{N}{N-1} \right) \to 0, and 1N10\frac{1}{N-1} \to 0, 1Nr0\frac{1}{N^r} \to 0

So the limit of the integral is,

3ln2+1+22+18=3ln2+178-3 \ln 2 + 1 + \frac{2}{2} + \frac{1}{8} = -3 \ln 2 + \frac{17}{8}

Alternatives for stem using sum of GP or proof by induction

Model Solution

Preliminary result. We show xnyn=(xy)r=1nxnryr1x^n - y^n = (x - y)\sum_{r=1}^{n} x^{n-r} y^{r-1}.

Expanding the right side:

(xy)r=1nxnryr1=r=1nxnr+1yr1r=1nxnryr(x - y)\sum_{r=1}^{n} x^{n-r} y^{r-1} = \sum_{r=1}^{n} x^{n-r+1} y^{r-1} - \sum_{r=1}^{n} x^{n-r} y^{r}

In the first sum, let s=r1s = r - 1: s=0n1xnsys=xn+s=1n1xnsys\sum_{s=0}^{n-1} x^{n-s} y^{s} = x^n + \sum_{s=1}^{n-1} x^{n-s} y^{s}.

In the second sum, let s=rs = r: s=1nxnsys=s=1n1xnsys+yn\sum_{s=1}^{n} x^{n-s} y^{s} = \sum_{s=1}^{n-1} x^{n-s} y^{s} + y^n.

Subtracting, all intermediate terms cancel, leaving xnynx^n - y^n. \qquad \square


Part (i)(a). From F(x)=Axk+f(x)xnF(x) = \frac{A}{x - k} + \frac{f(x)}{x^n}, multiply through by xn(xk)x^n(x - k):

1=Axn+(xk)f(x)1 = Ax^n + (x - k)f(x)

Setting x=kx = k: 1=Akn1 = Ak^n, so A=1knA = \dfrac{1}{k^n}.

Rearranging: (xk)f(x)=1xnkn(x - k)f(x) = 1 - \dfrac{x^n}{k^n}, hence

f(x)=1xk(1(xk)n)f(x) = \frac{1}{x - k}\left(1 - \left(\frac{x}{k}\right)^n\right) \qquad \checkmark

Deduction. We simplify f(x)xn\dfrac{f(x)}{x^n}. Write

f(x)=1xkknxnknf(x) = \frac{1}{x - k} \cdot \frac{k^n - x^n}{k^n}

Applying the preliminary result with kk in place of xx and xx in place of yy:

knxn=(kx)r=1nknrxr1=(xk)r=1nknrxr1k^n - x^n = (k - x)\sum_{r=1}^{n} k^{n-r} x^{r-1} = -(x - k)\sum_{r=1}^{n} k^{n-r} x^{r-1}

So

f(x)=(xk)r=1nknrxr1kn(xk)=r=1nxr1krf(x) = \frac{-(x - k)\sum_{r=1}^{n} k^{n-r} x^{r-1}}{k^n(x - k)} = -\sum_{r=1}^{n} \frac{x^{r-1}}{k^r}

Dividing by xnx^n:

f(x)xn=r=1n1krxnr+1\frac{f(x)}{x^n} = -\sum_{r=1}^{n} \frac{1}{k^r \, x^{n-r+1}}

Reindex with s=n+1rs = n + 1 - r (so r=n+1sr = n + 1 - s, and r:1nr: 1 \to n gives s:n1s: n \to 1):

r=1n1krxn+1r=s=1n1kn+1sxs=1ks=1n1knsxs\sum_{r=1}^{n} \frac{1}{k^r \, x^{n+1-r}} = \sum_{s=1}^{n} \frac{1}{k^{n+1-s} x^s} = \frac{1}{k}\sum_{s=1}^{n} \frac{1}{k^{n-s} x^s}

Therefore

F(x)=1kn(xk)+f(x)xn=1kn(xk)1kr=1n1knrxrF(x) = \frac{1}{k^n(x - k)} + \frac{f(x)}{x^n} = \frac{1}{k^n(x - k)} - \frac{1}{k}\sum_{r=1}^{n} \frac{1}{k^{n-r} x^r} \qquad \square

Part (i)(b). From F(x)=1xn(xk)F(x) = \dfrac{1}{x^n(x - k)}, we have xnF(x)=1xkx^n F(x) = \dfrac{1}{x - k}.

Using the result of (a), multiply through by xnx^n:

xnF(x)=xnkn(xk)1kr=1nxnrknr=xnkn(xk)r=1nxnrknr+1x^n F(x) = \frac{x^n}{k^n(x - k)} - \frac{1}{k}\sum_{r=1}^{n} \frac{x^{n-r}}{k^{n-r}} = \frac{x^n}{k^n(x - k)} - \sum_{r=1}^{n} \frac{x^{n-r}}{k^{n-r+1}}

Differentiate both sides with respect to xx. The left side:

ddx[1xk]=1(xk)2\frac{d}{dx}\left[\frac{1}{x - k}\right] = \frac{-1}{(x - k)^2}

For the right side, use the product rule on xnkn1xk\dfrac{x^n}{k^n} \cdot \dfrac{1}{x - k} and the power rule on each sum term:

ddx[xnkn(xk)]=nxn1kn(xk)xnkn(xk)2\frac{d}{dx}\left[\frac{x^n}{k^n(x - k)}\right] = \frac{nx^{n-1}}{k^n(x - k)} - \frac{x^n}{k^n(x - k)^2} ddx[r=1nxnrknr+1]=r=1n(nr)xnr1knr+1\frac{d}{dx}\left[\sum_{r=1}^{n} \frac{x^{n-r}}{k^{n-r+1}}\right] = \sum_{r=1}^{n} \frac{(n - r)\,x^{n-r-1}}{k^{n-r+1}}

Equating the derivatives:

1(xk)2=nxn1kn(xk)xnkn(xk)2r=1n(nr)xnr1knr+1\frac{-1}{(x - k)^2} = \frac{nx^{n-1}}{k^n(x - k)} - \frac{x^n}{k^n(x - k)^2} - \sum_{r=1}^{n} \frac{(n - r)\,x^{n-r-1}}{k^{n-r+1}}

Multiply both sides by 1xn\dfrac{-1}{x^n}:

1xn(xk)2=1kn(xk)2nxkn(xk)+r=1n(nr)xnr1knr+1xn\frac{1}{x^n(x - k)^2} = \frac{1}{k^n(x - k)^2} - \frac{n}{x\,k^n(x - k)} + \sum_{r=1}^{n} \frac{(n - r)\,x^{n-r-1}}{k^{n-r+1}\,x^n}

Since xnr1xn=1xr+1\dfrac{x^{n-r-1}}{x^n} = \dfrac{1}{x^{r+1}}:

1xn(xk)2=1kn(xk)2nxkn(xk)+r=1nnrkn+1rxr+1\frac{1}{x^n(x - k)^2} = \frac{1}{k^n(x - k)^2} - \frac{n}{x\,k^n(x - k)} + \sum_{r=1}^{n} \frac{n - r}{k^{n+1-r}\,x^{r+1}} \qquad \square

Part (ii). Set n=3n = 3 and k=1k = 1 in the result of (b):

1x3(x1)2=1(x1)23x(x1)+r=133rxr+1\frac{1}{x^3(x - 1)^2} = \frac{1}{(x - 1)^2} - \frac{3}{x(x - 1)} + \sum_{r=1}^{3} \frac{3 - r}{x^{r+1}} =1(x1)23x(x1)+2x2+1x3+0= \frac{1}{(x - 1)^2} - \frac{3}{x(x - 1)} + \frac{2}{x^2} + \frac{1}{x^3} + 0

For the 3x(x1)\dfrac{3}{x(x - 1)} term, use partial fractions:

3x(x1)=Ax+Bx1    3=A(x1)+Bx\frac{3}{x(x - 1)} = \frac{A}{x} + \frac{B}{x - 1} \implies 3 = A(x - 1) + Bx

x=0x = 0: A=3A = -3. \quad x=1x = 1: B=3B = 3. \quad So 3x(x1)=3x13x\dfrac{3}{x(x - 1)} = \dfrac{3}{x - 1} - \dfrac{3}{x}.

Therefore

1x3(x1)2=1(x1)23x1+3x+2x2+1x3\frac{1}{x^3(x - 1)^2} = \frac{1}{(x - 1)^2} - \frac{3}{x - 1} + \frac{3}{x} + \frac{2}{x^2} + \frac{1}{x^3}

Integrating term by term:

dxx3(x1)2=1x13ln(x1)+3lnx2x12x2+C\int \frac{dx}{x^3(x - 1)^2} = -\frac{1}{x - 1} - 3\ln(x - 1) + 3\ln x - \frac{2}{x} - \frac{1}{2x^2} + C =3lnxx11x12x12x2+C= 3\ln\frac{x}{x - 1} - \frac{1}{x - 1} - \frac{2}{x} - \frac{1}{2x^2} + C

Evaluating from 22 to NN:

2N=[3lnxx11x12x12x2]2N\int_2^N = \left[3\ln\frac{x}{x - 1} - \frac{1}{x - 1} - \frac{2}{x} - \frac{1}{2x^2}\right]_2^N

At x=Nx = N:

3lnNN11N12N12N23\ln\frac{N}{N - 1} - \frac{1}{N - 1} - \frac{2}{N} - \frac{1}{2N^2}

At x=2x = 2:

3ln21118=3ln21783\ln 2 - 1 - 1 - \frac{1}{8} = 3\ln 2 - \frac{17}{8}

So

2Ndxx3(x1)2=3lnNN11N12N12N23ln2+178\int_2^N \frac{dx}{x^3(x - 1)^2} = 3\ln\frac{N}{N - 1} - \frac{1}{N - 1} - \frac{2}{N} - \frac{1}{2N^2} - 3\ln 2 + \frac{17}{8}

As NN \to \infty:

  • lnNN1=ln ⁣(11N)0\ln\dfrac{N}{N - 1} = -\ln\!\left(1 - \dfrac{1}{N}\right) \to 0
  • 1N10\dfrac{1}{N - 1} \to 0, 2N0\quad \dfrac{2}{N} \to 0, 12N20\quad \dfrac{1}{2N^2} \to 0

Therefore the limit is

1783ln2\frac{17}{8} - 3\ln 2
Examiner Notes

本题较热门,成功率也较高。第(i)(a)部分主要问题是求 AA 时出错,或忽略 x=kx=k 处未定义。第(i)(b)部分不少考生没有意识到需要两边对 xx 求导,求导错误和变量混淆是主要障碍。第(ii)部分多数考生能使用第(i)(b)部分的结果,但极限中的对数项处理常被遗漏。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

6 (i) Sketch the curve y=cosx+cos2xy = \cos x + \sqrt{\cos 2x} for 14πx14π-\frac{1}{4}\pi \leqslant x \leqslant \frac{1}{4}\pi.

(ii) The equation of curve C1C_1 in polar co-ordinates is

r=cosθ+cos2θ14πθ14π.r = \cos \theta + \sqrt{\cos 2\theta} \quad -\frac{1}{4}\pi \leqslant \theta \leqslant \frac{1}{4}\pi.

Sketch the curve C1C_1.

(iii) The equation of curve C2C_2 in polar co-ordinates is

r22rcosθ+sin2θ=014πθ14π.r^2 - 2r \cos \theta + \sin^2 \theta = 0 \quad -\frac{1}{4}\pi \leqslant \theta \leqslant \frac{1}{4}\pi.

Find the value of rr when θ=±14π\theta = \pm \frac{1}{4}\pi.

Show that, when rr is small, r12θ2r \approx \frac{1}{2}\theta^2.

Sketch the curve C2C_2, indicating clearly the behaviour of the curve near r=0r = 0 and near θ=±14π\theta = \pm \frac{1}{4}\pi.

Show that the area enclosed by curve C2C_2 and above the line θ=0\theta = 0 is π22\frac{\pi}{2\sqrt{2}}.

Hint
  1. (i)

y=cosx+cos2xy = \cos x + \sqrt{\cos 2x}

x=0,y=2x = 0, y = 2 There is symmetry in x=0x = 0 x=±π4,y=12x = \pm \frac{\pi}{4}, y = \frac{1}{\sqrt{2}}

dydx=sinxsin2xcos2xsox=0,dydx=0x>0,dydx<0 and vice versa\frac{dy}{dx} = -\sin x - \frac{\sin 2x}{\sqrt{\cos 2x}} \quad \text{so} \quad x = 0, \frac{dy}{dx} = 0 \quad x > 0, \frac{dy}{dx} < 0 \text{ and vice versa}

as xπ4,dydxx \to \frac{\pi}{4}, \frac{dy}{dx} \to -\infty

(ii)

(iii) θ=±π4,r=12\theta = \pm \frac{\pi}{4}, r = \frac{1}{\sqrt{2}}

r22rcosθ+sin2θ=0r^2 - 2r \cos \theta + \sin^2 \theta = 0

(rcosθ)2=cos2θsin2θ=cos2θ(r - \cos \theta)^2 = \cos^2 \theta - \sin^2 \theta = \cos 2\theta

Therefore, rcosθ=±cos2θr - \cos \theta = \pm \sqrt{\cos 2\theta}, i.e. r=cosθ±cos2θr = \cos \theta \pm \sqrt{\cos 2\theta}

From (i), rr is only small on the branch, r=cosθcos2θr = \cos \theta - \sqrt{\cos 2\theta}. For θ=0,r=0\theta = 0, r = 0

Otherwise, cosθcos2θ=0,cos2θ=cos2θ,2cos2θ1=cos2θ,cosθ=±1\cos \theta - \sqrt{\cos 2\theta} = 0, \cos 2\theta = \cos^2 \theta, 2\cos^2 \theta - 1 = \cos^2 \theta, \cos \theta = \pm 1 so for π4θπ4,θ=0-\frac{\pi}{4} \le \theta \le \frac{\pi}{4}, \theta = 0 is the only value for which r=0r = 0

So rr small implies r=cosθcos2θr = \cos \theta - \sqrt{\cos 2\theta} and θ\theta is small

Thus r1θ22(1(2θ)22)121θ221+θ2=θ22r \approx 1 - \frac{\theta^2}{2} - \left(1 - \frac{(2\theta)^2}{2}\right)^{\frac{1}{2}} \approx 1 - \frac{\theta^2}{2} - 1 + \theta^2 = \frac{\theta^2}{2} as required.

Area required is

120π4(cosθ+cos2θ)2dθ120π4(cosθcos2θ)2dθ\frac{1}{2} \int_{0}^{\frac{\pi}{4}} (\cos \theta + \sqrt{\cos 2\theta})^2 \, d\theta - \frac{1}{2} \int_{0}^{\frac{\pi}{4}} (\cos \theta - \sqrt{\cos 2\theta})^2 \, d\theta

=20π4cosθcos2θdθ= 2 \int_{0}^{\frac{\pi}{4}} \cos \theta \sqrt{\cos 2\theta} \, d\theta

=20π4cosθ12sin2θdθ= 2 \int_{0}^{\frac{\pi}{4}} \cos \theta \sqrt{1 - 2 \sin^2 \theta} \, d\theta

Let 2sinθ=sinu\sqrt{2} \sin \theta = \sin u, then 2cosθdθdu=cosu\sqrt{2} \cos \theta \frac{d\theta}{du} = \cos u,

So the integral becomes

20π2cos2u2 du=20π2cos2u+12 du=2[sin2u4+u2]0π2=π222 \int_{0}^{\frac{\pi}{2}} \frac{\cos^{2} u}{\sqrt{2}} \ du = \sqrt{2} \int_{0}^{\frac{\pi}{2}} \frac{\cos 2u + 1}{2} \ du = \sqrt{2} \left[ \frac{\sin 2u}{4} + \frac{u}{2} \right]_{0}^{\frac{\pi}{2}} = \frac{\pi}{2\sqrt{2}}

(iii) alternative

r12rcosθ+sin2θ0r \ll 1 \Rightarrow -2r \cos \theta + \sin^{2} \theta \approx 0 rsin2θ2cosθ=12sinθtanθθ22r \approx \frac{\sin^{2} \theta}{2 \cos \theta} = \frac{1}{2} \sin \theta \tan \theta \approx \frac{\theta^{2}}{2}

Model Solution

Part (i). Let y=cosx+cos2xy = \cos x + \sqrt{\cos 2x} for π4xπ4-\frac{\pi}{4} \le x \le \frac{\pi}{4}.

Key values:

  • x=0x = 0: y=1+1=2y = 1 + 1 = 2
  • x=±π4x = \pm\dfrac{\pi}{4}: y=12+0=12y = \dfrac{1}{\sqrt{2}} + 0 = \dfrac{1}{\sqrt{2}}

Symmetry: Both cosx\cos x and cos2x\cos 2x are even functions, so y(x)=y(x)y(-x) = y(x). The curve is symmetric about x=0x = 0.

Derivative:

y=sinxsin2xcos2x=sinx2sinxcosxcos2x=sinx(1+2cosxcos2x)y' = -\sin x - \frac{\sin 2x}{\sqrt{\cos 2x}} = -\sin x - \frac{2\sin x \cos x}{\sqrt{\cos 2x}} = -\sin x\left(1 + \frac{2\cos x}{\sqrt{\cos 2x}}\right)

At x=0x = 0: y(0)=0y'(0) = 0 (horizontal tangent at the maximum).

For 0<x<π40 < x < \frac{\pi}{4}: sinx>0\sin x > 0, cosx>0\cos x > 0, cos2x>0\cos 2x > 0, so y<0y' < 0 (decreasing).

As xπ4x \to \frac{\pi}{4}^-: cos2x0+\cos 2x \to 0^+, so sin2xcos2x+\dfrac{\sin 2x}{\sqrt{\cos 2x}} \to +\infty, hence yy' \to -\infty (vertical tangent at both endpoints).

The curve has a maximum of y=2y = 2 at x=0x = 0, decreases to y=12y = \dfrac{1}{\sqrt{2}} at both endpoints with vertical tangents, and is symmetric about the yy-axis.


Part (ii). The polar curve C1C_1 is r=cosθ+cos2θr = \cos\theta + \sqrt{\cos 2\theta} for π4θπ4-\frac{\pi}{4} \le \theta \le \frac{\pi}{4}.

This is the same function as in part (i), now plotted as rr against θ\theta in polar coordinates. Since r>0r > 0 throughout the domain and the endpoint rays are distinct, this is an open polar arc rather than a closed loop:

  • At θ=0\theta = 0: r=2r = 2, so the curve reaches the point (2,0)(2, 0) in Cartesian coordinates.
  • At θ=±π4\theta = \pm\frac{\pi}{4}: r=12r = \frac{1}{\sqrt{2}}, so the curve meets the lines θ=±π4\theta = \pm\frac{\pi}{4} at distance 12\frac{1}{\sqrt{2}} from the origin (Cartesian: (12,±12)\left(\frac{1}{2}, \pm\frac{1}{2}\right)).
  • The curve is symmetric about the initial line θ=0\theta = 0.
  • It forms an arc bulging outward to r=2r = 2 along the positive xx-axis.

Part (iii).

Finding rr when θ=±π4\theta = \pm\frac{\pi}{4}:

r22rcosπ4+sin2π4=0r^2 - 2r\cos\frac{\pi}{4} + \sin^2\frac{\pi}{4} = 0 r22r+12=0r^2 - \sqrt{2}\,r + \frac{1}{2} = 0 (r12)2=0\left(r - \frac{1}{\sqrt{2}}\right)^2 = 0

So r=12r = \dfrac{1}{\sqrt{2}}. \qquad \checkmark


Showing r12θ2r \approx \frac{1}{2}\theta^2 for small rr:

Complete the square in the equation r22rcosθ+sin2θ=0r^2 - 2r\cos\theta + \sin^2\theta = 0:

(rcosθ)2=cos2θsin2θ=cos2θ(r - \cos\theta)^2 = \cos^2\theta - \sin^2\theta = \cos 2\theta

So r=cosθ±cos2θr = \cos\theta \pm \sqrt{\cos 2\theta}.

For small rr, we need the - branch: r=cosθcos2θr = \cos\theta - \sqrt{\cos 2\theta}, since at θ=0\theta = 0 this gives r=11=0r = 1 - 1 = 0. (The ++ branch gives r=2r = 2 at θ=0\theta = 0.)

For small θ\theta, using Taylor expansions:

cosθ1θ22,cos2θ12θ2\cos\theta \approx 1 - \frac{\theta^2}{2}, \qquad \cos 2\theta \approx 1 - 2\theta^2 cos2θ=(12θ2)1/21θ2\sqrt{\cos 2\theta} = (1 - 2\theta^2)^{1/2} \approx 1 - \theta^2

Therefore

r(1θ22)(1θ2)=θ22r \approx \left(1 - \frac{\theta^2}{2}\right) - (1 - \theta^2) = \frac{\theta^2}{2} \qquad \checkmark

Sketch of C2C_2:

The curve C2C_2 consists of two branches meeting at θ=±π4\theta = \pm\frac{\pi}{4}:

  • Outer branch: r=cosθ+cos2θr = \cos\theta + \sqrt{\cos 2\theta} (the same as C1C_1; maximum r=2r = 2 at θ=0\theta = 0).
  • Inner branch: r=cosθcos2θr = \cos\theta - \sqrt{\cos 2\theta} (passes through the origin at θ=0\theta = 0; reaches r=12r = \frac{1}{\sqrt{2}} at θ=±π4\theta = \pm\frac{\pi}{4}).

Near r=0r = 0: the inner branch has rθ22r \approx \frac{\theta^2}{2}, so the curve approaches the origin tangentially to the initial line θ=0\theta = 0 (since r/θ0r/\theta \to 0 as θ0\theta \to 0).

Near θ=±π4\theta = \pm\frac{\pi}{4}: both branches give r=12r = \frac{1}{\sqrt{2}}, and drdθ±\frac{dr}{d\theta} \to \pm\infty on each branch, so the curve has cusps at these junction points.


Area enclosed by C2C_2 above θ=0\theta = 0:

The required area is the region between the two branches for 0θπ40 \le \theta \le \frac{\pi}{4}:

A=120π/4r+2dθ120π/4r2dθA = \frac{1}{2}\int_0^{\pi/4} r_+^2 \, d\theta - \frac{1}{2}\int_0^{\pi/4} r_-^2 \, d\theta

where r±=cosθ±cos2θr_{\pm} = \cos\theta \pm \sqrt{\cos 2\theta}.

Using the difference of squares:

r+2r2=(r++r)(r+r)=(2cosθ)(2cos2θ)=4cosθcos2θr_+^2 - r_-^2 = (r_+ + r_-)(r_+ - r_-) = (2\cos\theta)(2\sqrt{\cos 2\theta}) = 4\cos\theta\sqrt{\cos 2\theta}

So

A=120π/44cosθcos2θdθ=20π/4cosθ12sin2θdθA = \frac{1}{2}\int_0^{\pi/4} 4\cos\theta\sqrt{\cos 2\theta} \, d\theta = 2\int_0^{\pi/4} \cos\theta\sqrt{1 - 2\sin^2\theta} \, d\theta

Substitute 2sinθ=sinϕ\sqrt{2}\sin\theta = \sin\phi. Then 2cosθdθ=cosϕdϕ\sqrt{2}\cos\theta \, d\theta = \cos\phi \, d\phi, so

cosθdθ=cosϕ2dϕ\cos\theta \, d\theta = \frac{\cos\phi}{\sqrt{2}} \, d\phi

When θ=0\theta = 0: ϕ=0\phi = 0. When θ=π4\theta = \frac{\pi}{4}: sinϕ=212=1\sin\phi = \sqrt{2} \cdot \frac{1}{\sqrt{2}} = 1, so ϕ=π2\phi = \frac{\pi}{2}.

12sin2θ=1sin2ϕ=cosϕ(since ϕ[0,π2])\sqrt{1 - 2\sin^2\theta} = \sqrt{1 - \sin^2\phi} = \cos\phi \qquad (\text{since } \phi \in [0, \tfrac{\pi}{2}])

Therefore

A=20π/2cosϕcosϕ2dϕ=220π/2cos2ϕdϕA = 2\int_0^{\pi/2} \cos\phi \cdot \frac{\cos\phi}{\sqrt{2}} \, d\phi = \frac{2}{\sqrt{2}}\int_0^{\pi/2} \cos^2\phi \, d\phi

Using cos2ϕ=12(1+cos2ϕ)\cos^2\phi = \frac{1}{2}(1 + \cos 2\phi):

0π/2cos2ϕdϕ=12[ϕ+sin2ϕ2]0π/2=12π2=π4\int_0^{\pi/2} \cos^2\phi \, d\phi = \frac{1}{2}\left[\phi + \frac{\sin 2\phi}{2}\right]_0^{\pi/2} = \frac{1}{2} \cdot \frac{\pi}{2} = \frac{\pi}{4}

So

A=22π4=2π4=π22A = \frac{2}{\sqrt{2}} \cdot \frac{\pi}{4} = \sqrt{2} \cdot \frac{\pi}{4} = \frac{\pi}{2\sqrt{2}} \qquad \square
Examiner Notes

约70%的考生尝试本题,但平均得分仅约35%。第(i)部分多数考生能完成,但常忽略端点斜率。第(ii)部分作图质量较弱,端点行为处理不好。第(iii)部分的小量近似论证常不完整;很多考生没有发现 C1C_1C2C_2 的一条分支。极坐标面积计算是主要障碍,成功者通常意识到需要取两个极坐标积分之差。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

7 (i) Given that the variables xx, yy and uu are connected by the differential equations

dudx+f(x)u=h(x)anddydx+g(x)y=u,\frac{\mathrm{d}u}{\mathrm{d}x} + \mathrm{f}(x)u = \mathrm{h}(x) \quad \text{and} \quad \frac{\mathrm{d}y}{\mathrm{d}x} + \mathrm{g}(x)y = u,

show that

d2ydx2+(g(x)+f(x))dydx+(g(x)+f(x)g(x))y=h(x).(1)\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + (\mathrm{g}(x) + \mathrm{f}(x))\frac{\mathrm{d}y}{\mathrm{d}x} + (\mathrm{g}'(x) + \mathrm{f}(x)\mathrm{g}(x))y = \mathrm{h}(x). \qquad \text{(1)}

(ii) Given that the differential equation

d2ydx2+(1+4x)dydx+(2x+2x2)y=4x+12(2)\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + \left(1 + \frac{4}{x}\right)\frac{\mathrm{d}y}{\mathrm{d}x} + \left(\frac{2}{x} + \frac{2}{x^2}\right)y = 4x + 12 \qquad \text{(2)}

can be written in the same form as (1), find a first order differential equation which is satisfied by g(x)\mathrm{g}(x).

If g(x)=kxn\mathrm{g}(x) = kx^n, find a possible value of nn and the corresponding value of kk.

Hence find a solution of (2) with y=5y = 5 and dydx=3\frac{\mathrm{d}y}{\mathrm{d}x} = -3 at x=1x = 1.

Hint
  1. (i) u=dydx+g(x)yu = \frac{dy}{dx} + g(x)y

Thus

dudx=d2ydx2+g(x)dydx+g(x)y\frac{du}{dx} = \frac{d^2y}{dx^2} + g(x)\frac{dy}{dx} + g'(x)y

As dudx+f(x)u=h(x)\frac{du}{dx} + f(x)u = h(x)

d2ydx2+g(x)dydx+g(x)y+f(x)(dydx+g(x)y)=h(x)\frac{d^2y}{dx^2} + g(x)\frac{dy}{dx} + g'(x)y + f(x)\left(\frac{dy}{dx} + g(x)y\right) = h(x)

that is

d2ydx2+(g(x)+f(x))dydx+(g(x)+f(x)g(x))y=h(x)\frac{d^2y}{dx^2} + (g(x) + f(x))\frac{dy}{dx} + (g'(x) + f(x)g(x))y = h(x)

as required.

(ii)

g(x)+f(x)=1+4xg(x) + f(x) = 1 + \frac{4}{x}

and so f(x)=1+4xg(x)f(x) = 1 + \frac{4}{x} - g(x)

g(x)+f(x)g(x)=2x+2x2g'(x) + f(x)g(x) = \frac{2}{x} + \frac{2}{x^2}

so

g(x)+(1+4xg(x))g(x)=2x+2x2g'(x) + \left(1 + \frac{4}{x} - g(x)\right)g(x) = \frac{2}{x} + \frac{2}{x^2}

as requested.

If g(x)=kxng(x) = kx^n, g(x)=knxn1g'(x) = knx^{n-1}

knxn1+(1+4xkxn)kxn=2x+2x2knx^{n-1} + \left(1 + \frac{4}{x} - kx^n\right)kx^n = \frac{2}{x} + \frac{2}{x^2}

k2x2n+2+kxn+2+k(n+4)xn+12x2=0-k^2x^{2n+2} + kx^{n+2} + k(n + 4)x^{n+1} - 2x - 2 = 0

Considering the x2n+2x^{2n+2} term,

either it is eliminated by the xn+2x^{n+2} term, in which case, 2n+2=n+22n + 2 = n + 2 and k2+k=0-k^2 + k = 0

which would imply n=0n = 0 and k=0k = 0 or k=1k = 1

k=0k = 0 is not possible (2x2=0)(-2x - 2 = 0); n=0,k=1n = 0, k = 1 would give 4x2x2=04x - 2x - 2 = 0 so not possible

Or it is eliminated by the xn+1x^{n+1} term, in which case, 2n+2=n+12n + 2 = n + 1 which implies n=1n = -1 and thus k2+k(n+4)2=0-k^2 + k(n + 4) - 2 = 0 and considering the other two terms k2=0k - 2 = 0

k=2k = 2 and n=1n = -1 satisfy k2+k(n+4)2=0-k^2 + k(n + 4) - 2 = 0 so these are possible values.

So g(x)=2xg(x) = \frac{2}{x} and as f(x)=1+4xg(x)f(x) = 1 + \frac{4}{x} - g(x), f(x)=1+2xf(x) = 1 + \frac{2}{x} h(x)=4x+12h(x) = 4x + 12

dudx+f(x)u=h(x)\frac{du}{dx} + f(x)u = h(x) is thus dudx+(1+2x)u=4x+12\frac{du}{dx} + \left(1 + \frac{2}{x}\right)u = 4x + 12

The integrating factor is

e(1+2x)dx=ex+2lnx=x2exe^{\int \left(1 + \frac{2}{x}\right) dx} = e^{x + 2 \ln x} = x^2 e^x

Thus

x2exdudx+(x2+2x)exu=(4x+12)x2ex=(4x3+12x2)exx^2 e^x \frac{du}{dx} + (x^2 + 2x)e^x u = (4x + 12)x^2 e^x = (4x^3 + 12x^2)e^x

Integrating with respect to xx

x2exu=(4x3+12x2)exdx=4x3ex+cx^2 e^x u = \int (4x^3 + 12x^2)e^x dx = 4x^3 e^x + c

As u=dydx+g(x)yu = \frac{dy}{dx} + g(x)y, and g(x)=2xg(x) = \frac{2}{x}, when x=1x = 1, y=5y = 5, dydx=3\frac{dy}{dx} = -3, we have u=3+2×5u = -3 + 2 \times 5

That is u=7u = 7, so 7e=4e+c7e = 4e + c, which means c=3ec = 3e

So u=4x+3eexx2u = 4x + 3e \frac{e^{-x}}{x^2}

dydx+2xy=4x+3eexx2\frac{dy}{dx} + \frac{2}{x}y = 4x + 3e \frac{e^{-x}}{x^2}

This has integrating factor

e2xdx=e2lnx=x2e^{\int \frac{2}{x} dx} = e^{2 \ln x} = x^2

So

x2dydx+2xy=4x3+3eexx^2 \frac{dy}{dx} + 2xy = 4x^3 + 3e e^{-x}

Integrating with respect to xx

x2y=4x3+3eexdx=x43eex+cx^2 y = \int 4x^3 + 3e e^{-x} dx = x^4 - 3ee^{-x} + c'

when x=1x = 1, y=5y = 5 so 5=13+c5 = 1 - 3 + c' which means c=7c' = 7

Therefore,

y=x2+7x23ex+1x2y = x^2 + \frac{7}{x^2} - \frac{3e^{-x+1}}{x^2}

Model Solution

Part (i)

From the second equation, u=dydx+g(x)yu = \dfrac{\mathrm{d}y}{\mathrm{d}x} + \mathrm{g}(x)y.

Differentiating both sides with respect to xx using the product rule:

dudx=d2ydx2+g(x)dydx+g(x)y.\frac{\mathrm{d}u}{\mathrm{d}x} = \frac{\mathrm{d}^2y}{\mathrm{d}x^2} + \mathrm{g}(x)\frac{\mathrm{d}y}{\mathrm{d}x} + \mathrm{g}'(x)y.

Substituting into the first equation dudx+f(x)u=h(x)\dfrac{\mathrm{d}u}{\mathrm{d}x} + \mathrm{f}(x)u = \mathrm{h}(x):

d2ydx2+g(x)dydx+g(x)y+f(x) ⁣(dydx+g(x)y)=h(x).\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + \mathrm{g}(x)\frac{\mathrm{d}y}{\mathrm{d}x} + \mathrm{g}'(x)y + \mathrm{f}(x)\!\left(\frac{\mathrm{d}y}{\mathrm{d}x} + \mathrm{g}(x)y\right) = \mathrm{h}(x).

Collecting terms in dydx\dfrac{\mathrm{d}y}{\mathrm{d}x} and yy:

d2ydx2+(g(x)+f(x))dydx+(g(x)+f(x)g(x))y=h(x).(1)\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + \bigl(\mathrm{g}(x) + \mathrm{f}(x)\bigr)\frac{\mathrm{d}y}{\mathrm{d}x} + \bigl(\mathrm{g}'(x) + \mathrm{f}(x)\mathrm{g}(x)\bigr)y = \mathrm{h}(x). \qquad \text{(1)}

Part (ii)

Comparing equation (2) with (1), we identify:

g(x)+f(x)=1+4x,g(x)+f(x)g(x)=2x+2x2.\mathrm{g}(x) + \mathrm{f}(x) = 1 + \frac{4}{x}, \qquad \mathrm{g}'(x) + \mathrm{f}(x)\mathrm{g}(x) = \frac{2}{x} + \frac{2}{x^2}.

From the first relation, f(x)=1+4xg(x)\mathrm{f}(x) = 1 + \dfrac{4}{x} - \mathrm{g}(x). Substituting into the second:

g(x)+(1+4xg(x))g(x)=2x+2x2.\mathrm{g}'(x) + \left(1 + \frac{4}{x} - \mathrm{g}(x)\right)\mathrm{g}(x) = \frac{2}{x} + \frac{2}{x^2}.

This is the required first order ODE for g(x)\mathrm{g}(x).

Now suppose g(x)=kxn\mathrm{g}(x) = kx^n, so g(x)=knxn1\mathrm{g}'(x) = knx^{n-1}. Substituting:

knxn1+(1+4xkxn)kxn=2x+2x2.knx^{n-1} + \left(1 + \frac{4}{x} - kx^n\right)kx^n = \frac{2}{x} + \frac{2}{x^2}.

Expanding the left side:

knxn1+kxn+4kxn1k2x2n=2x+2x2.knx^{n-1} + kx^n + 4kx^{n-1} - k^2x^{2n} = \frac{2}{x} + \frac{2}{x^2}.

k2x2n+kxn+k(n+4)xn1=2x+2x2.-k^2x^{2n} + kx^n + k(n+4)x^{n-1} = \frac{2}{x} + \frac{2}{x^2}.

Multiplying through by x2x^2:

k2x2n+2+kxn+2+k(n+4)xn+1=2x+2.()-k^2x^{2n+2} + kx^{n+2} + k(n+4)x^{n+1} = 2x + 2. \qquad (\ast)

The right side has terms in x1x^1 and x0x^0 only. We try n=1n = -1, which gives:

k2+kx+3k=2x+2.-k^2 + kx + 3k = 2x + 2.

Comparing coefficients of xx: k=2k = 2.

Comparing constant terms: k2+3k=4+6=2-k^2 + 3k = -4 + 6 = 2. This matches.

So n=1n = -1 and k=2k = 2, giving g(x)=2x\mathrm{g}(x) = \dfrac{2}{x}.

It follows that f(x)=1+4x2x=1+2x\mathrm{f}(x) = 1 + \dfrac{4}{x} - \dfrac{2}{x} = 1 + \dfrac{2}{x} and h(x)=4x+12\mathrm{h}(x) = 4x + 12.

Solving for yy:

The first equation for uu is:

dudx+(1+2x)u=4x+12.\frac{\mathrm{d}u}{\mathrm{d}x} + \left(1 + \frac{2}{x}\right)u = 4x + 12.

The integrating factor is e(1+2/x)dx=ex+2lnx=x2exe^{\int(1 + 2/x)\,\mathrm{d}x} = e^{x + 2\ln x} = x^2e^x. Multiplying through:

ddx ⁣(x2exu)=(4x+12)x2ex=(4x3+12x2)ex.\frac{\mathrm{d}}{\mathrm{d}x}\!\left(x^2 e^x u\right) = (4x + 12)x^2 e^x = (4x^3 + 12x^2)e^x.

We evaluate (4x3+12x2)exdx\displaystyle\int(4x^3 + 12x^2)e^x\,\mathrm{d}x by repeated integration by parts:

4x3exdx=4x3ex12x2exdx=4x3ex12x2ex+24xexdx\int 4x^3 e^x\,\mathrm{d}x = 4x^3 e^x - 12\int x^2 e^x\,\mathrm{d}x = 4x^3 e^x - 12x^2 e^x + 24\int x e^x\,\mathrm{d}x =4x3ex12x2ex+24xex24ex.= 4x^3 e^x - 12x^2 e^x + 24xe^x - 24e^x.

12x2exdx=12x2ex24xexdx=12x2ex24xex+24ex.\int 12x^2 e^x\,\mathrm{d}x = 12x^2 e^x - 24\int xe^x\,\mathrm{d}x = 12x^2 e^x - 24xe^x + 24e^x.

Adding:

(4x3+12x2)exdx=4x3ex+C.\int(4x^3 + 12x^2)e^x\,\mathrm{d}x = 4x^3 e^x + C.

So x2exu=4x3ex+Cx^2 e^x u = 4x^3 e^x + C, i.e.\ u=4x+Cex/x2u = 4x + Ce^{-x}/x^2.

From the second equation, u=dydx+2xyu = \dfrac{\mathrm{d}y}{\mathrm{d}x} + \dfrac{2}{x}y. At x=1x = 1: y=5y = 5, dydx=3\dfrac{\mathrm{d}y}{\mathrm{d}x} = -3, so u=3+10=7u = -3 + 10 = 7.

Setting x=1x = 1, u=7u = 7: 7=4+Ce17 = 4 + Ce^{-1}, so C=3eC = 3e.

Thus u=4x+3e1xx2u = 4x + \dfrac{3e^{1-x}}{x^2}.

Now solve dydx+2xy=4x+3e1xx2\dfrac{\mathrm{d}y}{\mathrm{d}x} + \dfrac{2}{x}y = 4x + \dfrac{3e^{1-x}}{x^2}.

The integrating factor is e2/xdx=x2e^{\int 2/x\,\mathrm{d}x} = x^2. Multiplying through:

ddx(x2y)=4x3+3e1x.\frac{\mathrm{d}}{\mathrm{d}x}(x^2 y) = 4x^3 + 3e^{1-x}.

Integrating:

x2y=x43e1x+C.x^2 y = x^4 - 3e^{1-x} + C'.

At x=1x = 1, y=5y = 5: 5=13+C5 = 1 - 3 + C', so C=7C' = 7.

y=x2+7x23e1xx2.y = x^2 + \frac{7}{x^2} - \frac{3e^{1-x}}{x^2}.

Examiner Notes

这是第二热门且最成功的题目,平均得分约65%。第(i)部分几乎所有考生都能完成。第(ii)部分中,找到一阶微分方程通常不是主要问题;许多考生会先猜 n=1n=-1,再验证 k=2k=2。积分因子和积分计算是主要失分点。部分考生使用特解加齐次解的方法,但齐次解常出错。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

8 A sequence uku_k, for integer k1k \geqslant 1, is defined as follows.

u1=1u_1 = 1 u2k=uk for k1u_{2k} = u_k \text{ for } k \geqslant 1 u2k+1=uk+uk+1 for k1u_{2k+1} = u_k + u_{k+1} \text{ for } k \geqslant 1

(i) Show that, for every pair of consecutive terms of this sequence, except the first pair, the term with odd subscript is larger than the term with even subscript.

(ii) Suppose that two consecutive terms in this sequence have a common factor greater than one. Show that there are then two consecutive terms earlier in the sequence which have the same common factor. Deduce that any two consecutive terms in this sequence are co-prime (do not have a common factor greater than one).

(iii) Prove that it is not possible for two positive integers to appear consecutively in the same order in two different places in the sequence.

(iv) Suppose that aa and bb are two co-prime positive integers which do not occur consecutively in the sequence with bb following aa. If a>ba > b, show that aba - b and bb are two co-prime positive integers which do not occur consecutively in the sequence with bb following aba - b, and whose sum is smaller than a+ba + b. Find a similar result for a<ba < b.

(v) For each integer n1n \geqslant 1, define the function f from the positive integers to the positive rational numbers by f(n)=unun+1f(n) = \frac{u_n}{u_{n+1}}. Show that the range of f is all the positive rational numbers, and that f has an inverse.

Hint
  1. (i) All terms of the sequence are positive integers because they are all either equal to a previous term or the sum of two previous terms which are positive integers.

Thus, for k1k \geq 1, as u2k=uku_{2k} = u_k and u2k+1=uk+uk+1u_{2k+1} = u_k + u_{k+1}, u2k+1u2k=uk+11u_{2k+1} - u_{2k} = u_{k+1} \geq 1

Also, u2k+1u2k+2=uk+uk+1uk+1=uk1u_{2k+1} - u_{2k+2} = u_k + u_{k+1} - u_{k+1} = u_k \geq 1. Thus, the required result is proved for terms from the third onwards. (The only terms not included in this proof are the first two, which are in case both equal to 1).

(ii) Suppose that u2k=cu_{2k} = c, and that u2k+1=du_{2k+1} = d, for k1k \geq 1, where d and c share a common factor greater than one, then uk=cu_k = c, as u2k=uku_{2k} = u_k, and uk+1=dc1u_{k+1} = d - c \geq 1 as u2k+1=uk+uk+1u_{2k+1} = u_k + u_{k+1} and using (i). Then as d and c share a common factor greater than one, d-c and c share a common factor greater than one. So, two earlier terms in the sequence do share the same common factor.

Likewise, suppose that u2k+2=cu_{2k+2} = c, and that u2k+1=du_{2k+1} = d, for k1k \geq 1, where d and c share a common factor greater than one, then uk+1=cu_{k+1} = c and uk=dcu_k = d - c giving the same result.

This is true for pairs of consecutive terms from the second term (and third) onwards. Repeating this argument, we find that it would imply that the first two terms would share a common factor greater than one, which is a contradiction. Hence any two consecutive terms are co-prime.

(iii) For k1k \geq 1, and m1m \geq 1 suppose that u2k=cu_{2k} = c and u2k+1=du_{2k+1} = d, and that u2k+m=cu_{2k+m} = c and u2k+m+1=du_{2k+m+1} = d, then as d>cd > c, 2k+m2k + m is even, so mm is even, say 2n2n. Thus, uk=cu_k = c and uk+1=dcu_{k+1} = d - c, and uk+n=cu_{k+n} = c and uk+n+1=dcu_{k+n+1} = d - c. That is, an earlier pair of terms would appear consecutively.

Likewise, if u2k+2=cu_{2k+2} = c and u2k+1=du_{2k+1} = d, and that u2k+m+2=cu_{2k+m+2} = c and u2k+m+1=du_{2k+m+1} = d, the same argument applies.

So the argument can be repeated down to the first two terms, which are of course equal, and it would imply a later pair are likewise which contradicts (i).

(iv) If (a,b)(a, b) does not occur, where aa and bb are coprime and a>ba > b, then there does not exist kk such that u2k+1=au_{2k+1} = a and u2k+2=bu_{2k+2} = b. Therefore there cannot exist a kk such that uk+1=bu_{k+1} = b and uk=abu_k = a - b, the sum of which is aa, which is smaller than a+ba + b.

If (a,b)(a, b) does not occur, where aa and bb are coprime and a<ba < b, then there does not exist kk such that u2k=au_{2k} = a and u2k+1=bu_{2k+1} = b. Therefore there cannot exist a kk such that uk=au_k = a and uk+1=bau_{k+1} = b - a, the sum of which is bb, which is smaller than a+ba + b.

(v) Suppose that there exists an ordered pair of coprime integers (a,b) which does not occur consecutively in the sequence. Then by part (iv) the pair (a-b, b) [if a>b] or (a, b-a) [if b>a] (which has a smaller sum) does not occur. Repeating this means that a coprime pair with sum <3 does not occur. The only coprime pair of integers with sum <3 is (1, 1) which are the first two terms. Contradiction and so every ordered pair of coprime integers occurs in the sequence and by (iii) only occurs once. Therefore, there exists an nn, and that nn is unique such that

q=unun+1q = \frac{u_n}{u_{n+1}}, for any positive rational qq (which is expressed in lowest form). So the inverse of f exists.

Model Solution

First, let us list the first several terms to build intuition:

u1=1,  u2=1,  u3=2,  u4=1,  u5=3,  u6=2,  u7=3,  u8=1,  u9=4,  u10=3,  u11=5,  u12=2,u_1 = 1,\; u_2 = 1,\; u_3 = 2,\; u_4 = 1,\; u_5 = 3,\; u_6 = 2,\; u_7 = 3,\; u_8 = 1,\; u_9 = 4,\; u_{10} = 3,\; u_{11} = 5,\; u_{12} = 2, \ldots

All terms are positive integers, since every term is either equal to a previous term (u2k=uku_{2k} = u_k) or a sum of two previous terms (u2k+1=uk+uk+1u_{2k+1} = u_k + u_{k+1}), with u1=1>0u_1 = 1 > 0.

Part (i)

For k1k \geqslant 1, we compare consecutive pairs (u2k,u2k+1)(u_{2k}, u_{2k+1}) and (u2k+1,u2k+2)(u_{2k+1}, u_{2k+2}).

u2k+1u2k=(uk+uk+1)uk=uk+11.u_{2k+1} - u_{2k} = (u_k + u_{k+1}) - u_k = u_{k+1} \geqslant 1.

u2k+1u2k+2=(uk+uk+1)uk+1=uk1.u_{2k+1} - u_{2k+2} = (u_k + u_{k+1}) - u_{k+1} = u_k \geqslant 1.

So for every pair of consecutive terms from the third term onwards, the odd-subscripted term exceeds the even-subscripted term. The only exception is the first pair (u1,u2)=(1,1)(u_1, u_2) = (1, 1), where both are equal.

Part (ii)

We show that if two consecutive terms share a common factor d>1d > 1, then an earlier consecutive pair also shares the factor dd.

Case 1: Suppose u2ku_{2k} and u2k+1u_{2k+1} share a common factor d>1d > 1 (for k1k \geqslant 1). Then uk=u2ku_k = u_{2k} is divisible by dd, and uk+1=u2k+1uku_{k+1} = u_{2k+1} - u_k is also divisible by dd. So the earlier consecutive pair (uk,uk+1)(u_k, u_{k+1}) shares the factor dd.

Case 2: Suppose u2k+1u_{2k+1} and u2k+2u_{2k+2} share a common factor d>1d > 1 (for k1k \geqslant 1). Then uk+1=u2k+2u_{k+1} = u_{2k+2} is divisible by dd, and uk=u2k+1uk+1u_k = u_{2k+1} - u_{k+1} is also divisible by dd. So the earlier consecutive pair (uk,uk+1)(u_k, u_{k+1}) shares the factor dd.

In either case, we can step back to an earlier consecutive pair sharing the same factor d>1d > 1. Repeating this process, we eventually reach the pair (u1,u2)=(1,1)(u_1, u_2) = (1, 1). But gcd(1,1)=1\gcd(1, 1) = 1, which contradicts the existence of a common factor d>1d > 1.

Therefore, any two consecutive terms in the sequence are coprime.

Part (iii)

Suppose for contradiction that two positive integers a,ba, b appear consecutively in the same order at two different positions: (um,um+1)=(un,un+1)=(a,b)(u_m, u_{m+1}) = (u_n, u_{n+1}) = (a, b) with m<nm < n.

We first establish that the predecessor of any consecutive pair is uniquely determined. Every consecutive pair (uj,uj+1)(u_j, u_{j+1}) for j2j \geqslant 2 arises from an earlier pair (uk,uk+1)(u_k, u_{k+1}) via one of two maps:

(u2k,u2k+1)=(uk,  uk+uk+1)and(u2k+1,u2k+2)=(uk+uk+1,  uk+1).(u_{2k}, u_{2k+1}) = (u_k,\; u_k + u_{k+1}) \qquad \text{and} \qquad (u_{2k+1}, u_{2k+2}) = (u_k + u_{k+1},\; u_{k+1}).

By part (i), if jj is even then uj+1>uju_{j+1} > u_j, and if jj is odd then uj>uj+1u_j > u_{j+1}. So:

  • If jj is even, j=2kj = 2k: (uj,uj+1)=(uk,uk+uk+1)(u_j, u_{j+1}) = (u_k, u_k + u_{k+1}), so the predecessor is (uk,uk+1)=(uj,  uj+1uj)(u_k, u_{k+1}) = (u_j,\; u_{j+1} - u_j).

  • If jj is odd, j=2k+1j = 2k+1: (uj,uj+1)=(uk+uk+1,uk+1)(u_j, u_{j+1}) = (u_k + u_{k+1}, u_{k+1}), so the predecessor is (uk,uk+1)=(ujuj+1,  uj+1)(u_k, u_{k+1}) = (u_j - u_{j+1},\; u_{j+1}).

In both cases, the predecessor pair and its parent index are determined uniquely by the values (uj,uj+1)(u_j,u_{j+1}): if the first entry is smaller, the pair came from an even index 2k2k and has predecessor (uj,uj+1uj)(u_j,u_{j+1}-u_j); if the first entry is larger, it came from an odd index 2k+12k+1 and has predecessor (ujuj+1,uj+1)(u_j-u_{j+1},u_{j+1}). Since (um,um+1)=(un,un+1)(u_m,u_{m+1})=(u_n,u_{n+1}), repeatedly applying this unique reverse step gives equal earlier ancestor pairs at every level.

Continuing the reverse process must eventually reach the initial pair (u1,u2)=(1,1)(u_1,u_2)=(1,1) for both occurrences. The same sequence of parity choices is forced by the pair values at each reverse step, so the binary path back from the root is the same for both positions. Hence the two positions are identical, contradicting m<nm<n.

Therefore, no two positive integers can appear consecutively in the same order at two different positions.

Part (iv)

Case a>ba > b: Suppose (a,b)(a, b) does not occur as a consecutive pair in the sequence. We claim (ab,b)(a - b, b) also does not occur as a consecutive pair with bb following aba - b.

Suppose for contradiction that (ab,b)(a - b, b) does occur, say (uk,uk+1)=(ab,b)(u_k, u_{k+1}) = (a - b, b). Then (u2k+1,u2k+2)=(uk+uk+1,uk+1)=(a,b)(u_{2k+1}, u_{2k+2}) = (u_k + u_{k+1}, u_{k+1}) = (a, b), contradicting our assumption. So (ab,b)(a - b, b) does not occur as a consecutive pair with bb following aba - b.

Furthermore, gcd(ab,b)=gcd(a,b)=1\gcd(a - b, b) = \gcd(a, b) = 1, so aba - b and bb are coprime positive integers (positive since a>ba > b). And (ab)+b=a<a+b(a - b) + b = a < a + b.

Case a<ba < b: By an analogous argument, if (a,b)(a, b) does not occur, then (a,ba)(a, b - a) does not occur as a consecutive pair with bab - a following aa. These are coprime positive integers with sum b<a+bb < a + b.

Explicitly: if (a,ba)=(uk,uk+1)(a, b - a) = (u_k, u_{k+1}), then (u2k,u2k+1)=(uk,uk+uk+1)=(a,b)(u_{2k}, u_{2k+1}) = (u_k, u_k + u_{k+1}) = (a, b), a contradiction.

Part (v)

Surjectivity: Let pq\dfrac{p}{q} be any positive rational number, where p,qp, q are coprime positive integers. We prove by strong induction on p+qp + q that the pair (p,q)(p, q) occurs as consecutive terms (un,un+1)(u_n, u_{n+1}) for some nn.

Base case: p+q=2p + q = 2 gives p=q=1p = q = 1. We have (u1,u2)=(1,1)(u_1, u_2) = (1, 1).

Inductive step: Suppose the result holds for all coprime pairs with sum less than p+qp + q, where p+q>2p + q > 2. Since gcd(p,q)=1\gcd(p, q) = 1 and p+q>2p + q > 2, we cannot have p=qp = q, so either p>qp > q or p<qp < q.

If p>qp > q: consider (pq,q)(p - q, q), which is a coprime pair with sum p<p+qp < p + q. By the inductive hypothesis, (pq,q)=(uk,uk+1)(p - q, q) = (u_k, u_{k+1}) for some kk. Then (u2k+1,u2k+2)=(uk+uk+1,uk+1)=(p,q)(u_{2k+1}, u_{2k+2}) = (u_k + u_{k+1}, u_{k+1}) = (p, q).

If p<qp < q: consider (p,qp)(p, q - p), which is a coprime pair with sum q<p+qq < p + q. By the inductive hypothesis, (p,qp)=(uk,uk+1)(p, q - p) = (u_k, u_{k+1}) for some kk. Then (u2k,u2k+1)=(uk,uk+uk+1)=(p,q)(u_{2k}, u_{2k+1}) = (u_k, u_k + u_{k+1}) = (p, q).

In both cases, (p,q)(p, q) occurs as consecutive terms. So every positive rational pq\dfrac{p}{q} is in the range of ff.

Injectivity: Suppose f(m)=f(n)f(m) = f(n), i.e., umum+1=unun+1\dfrac{u_m}{u_{m+1}} = \dfrac{u_n}{u_{n+1}}. Writing both fractions in lowest terms, we get the same coprime pair (p,q)(p, q). By part (iii), no ordered pair of positive integers appears consecutively at two different positions, so m=nm = n. Thus ff is injective.

Since ff is both surjective and injective, it is a bijection from the positive integers to the positive rationals, and therefore has an inverse.

Examiner Notes

约60%的考生尝试本题,但平均得分仅约33%。第(i)部分常见错误是误认为所有偶数下标项都满足所需性质。第(ii)部分需要分别考虑 (u2k1,u2k)(u_{2k-1},u_{2k})(u2k,u2k+1)(u_{2k},u_{2k+1}) 两种相邻情形。第(iii)部分对 “consecutive” 的理解是关键,很多考生错误地声称重现必定发生在 2nk2^n k 一类位置。第(iv)(v)部分很少有人完成,需要把第(iv)部分的 Euclidean algorithm 思想和第(v)部分的满射性联系起来。