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STEP3 2015 -- Pure Mathematics

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STEP3 2015 — Section A (Pure Mathematics)

Section titled “STEP3 2015 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2015  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1积分学 (Integral Calculus)Challenging分部积分, 换元积分 u=xx1u=x-x^{-1}, 递推公式推导, 对称性
2数列与不等式 (Sequences and Inequalities)Challenging反例构造, 数学归纳法, 不等式放缩, 序关系的传递性
3极坐标 (Polar Coordinates)Hard极坐标方程分析, 分情况讨论, 三角函数积分, 蚌线的几何性质
4复数 (Complex Numbers)Challenging中间值定理, 韦达定理, 棣莫弗定理, 复数的实部虚部分析
5数论 (Number Theory)Challenging反证法, 最小元原理, 等价命题证明, 集合论方法
6纯数 (Pure Mathematics)Challenging联立方程求解,判别式分析,反例构造,实数与复数条件
7纯数 (Pure Mathematics)Challenging数学归纳法,微分算子运算,二项式展开,x=1代入法
8纯数 (Pure Mathematics)Hard极坐标变换,链式法则,分离变量,部分分式积分,解曲线分类讨论

Topic: 积分学 (Integral Calculus)  |  Difficulty: Challenging  |  Marks: 20

1 (i) Let In=01(1+u2)ndu,I_n = \int_0^\infty \frac{1}{(1 + u^2)^n} \, du \, , where nn is a positive integer. Show that InIn+1=12nInI_n - I_{n+1} = \frac{1}{2n} I_n and deduce that In+1=(2n)!π22n+1(n!)2.I_{n+1} = \frac{(2n)! \, \pi}{2^{2n+1}(n!)^2} \, .

(ii) Let J=0f((xx1)2)dx,J = \int_0^\infty f((x - x^{-1})^2) \, dx \, , where ff is any function for which the integral exists. Show that J=0x2f((xx1)2)dx=120(1+x2)f((xx1)2)dx=0f(u2)du.J = \int_0^\infty x^{-2}f((x - x^{-1})^2) \, dx = \frac{1}{2} \int_0^\infty (1 + x^{-2})f((x - x^{-1})^2) \, dx = \int_0^\infty f(u^2) \, du \, .

(iii) Hence evaluate 0x2n2(x4x2+1)ndx,\int_0^\infty \frac{x^{2n-2}}{(x^4 - x^2 + 1)^n} \, dx \, , where nn is a positive integer.

Hint

The first result can be obtained by simplifying the LHS and then writing it as 0uu(1+u2)n+1du\int_{0}^{\infty} u \frac{u}{(1+u^2)^{n+1}} du and integrating this by parts. To obtain the evaluation of In+1I_{n+1}, the first result can be re-arranged to make In+1I_{n+1} the subject, and then iterating the result to express it in terms of I1I_1 which is a standard integral. The expression can be tidied by multiplying numerator and denominator by (2n)(2n2)(2)(2n)(2n-2) \dots (2). The first result for (ii) is obtained by means of the substitution u=x1u = x^{-1}, the second by adding the two versions of JJ, and the third by the substitution u=xx1u = x - x^{-1}, being careful with limits of integration and employing symmetry. Part (iii) is solved by expressing the integrand as x2((xx1)2+1)n\frac{x^{-2}}{((x-x^{-1})^2+1)^n} and then employing first part (ii) then part (i) to obtain InI_n, which is (2n2)!π22n1((n1)!)2\frac{(2n-2)!\pi}{2^{2n-1}((n-1)!)^2}.

Model Solution

Part (i)

We have

InIn+1=01(1+u2)ndu01(1+u2)n+1du=0(1+u2)1(1+u2)n+1du=0u2(1+u2)n+1du.I_n - I_{n+1} = \int_0^\infty \frac{1}{(1+u^2)^n} \, du - \int_0^\infty \frac{1}{(1+u^2)^{n+1}} \, du = \int_0^\infty \frac{(1+u^2) - 1}{(1+u^2)^{n+1}} \, du = \int_0^\infty \frac{u^2}{(1+u^2)^{n+1}} \, du.

We rewrite this as 0uu(1+u2)n+1du\int_0^\infty u \cdot \frac{u}{(1+u^2)^{n+1}} \, du and integrate by parts with

p=u,dqdu=u(1+u2)n+1.p = u, \qquad \frac{dq}{du} = \frac{u}{(1+u^2)^{n+1}}.

Then dpdu=1\frac{dp}{du} = 1 and q=12n(1+u2)nq = -\frac{1}{2n(1+u^2)^n} (found by substituting w=1+u2w = 1 + u^2). So

0u2(1+u2)n+1du=[u2n(1+u2)n]0+012n(1+u2)ndu.\int_0^\infty \frac{u^2}{(1+u^2)^{n+1}} \, du = \left[-\frac{u}{2n(1+u^2)^n}\right]_0^\infty + \int_0^\infty \frac{1}{2n(1+u^2)^n} \, du.

The boundary term vanishes: at u=0u = 0 the numerator is 00, and as uu \to \infty the power (1+u2)n(1+u^2)^n in the denominator dominates. Therefore

InIn+1=0+12nIn,I_n - I_{n+1} = 0 + \frac{1}{2n} I_n \, ,

as required.

Rearranging: In+1=In12nIn=2n12nInI_{n+1} = I_n - \frac{1}{2n} I_n = \frac{2n-1}{2n} I_n.

We now iterate this recurrence starting from I1=0du1+u2=[arctanu]0=π2I_1 = \int_0^\infty \frac{du}{1+u^2} = \left[\arctan u\right]_0^\infty = \frac{\pi}{2}.

I2=12π2,I3=3412π2,I_2 = \frac{1}{2} \cdot \frac{\pi}{2}, \qquad I_3 = \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2}, \qquad \ldots

In general, for n1n \geq 1:

In+1=1234562n12nπ2=135(2n1)246(2n)π2.I_{n+1} = \frac{1}{2} \cdot \frac{3}{4} \cdot \frac{5}{6} \cdots \frac{2n-1}{2n} \cdot \frac{\pi}{2} = \frac{1 \cdot 3 \cdot 5 \cdots (2n-1)}{2 \cdot 4 \cdot 6 \cdots (2n)} \cdot \frac{\pi}{2}.

To simplify the numerator, multiply top and bottom by 246(2n)=2nn!2 \cdot 4 \cdot 6 \cdots (2n) = 2^n \cdot n!:

135(2n1)=(2n)!2nn!.1 \cdot 3 \cdot 5 \cdots (2n-1) = \frac{(2n)!}{2^n \cdot n!}.

The denominator is 2nn!2^n \cdot n!. Therefore

In+1=(2n)!2nn!2nn!π2=(2n)!π22n+1(n!)2.I_{n+1} = \frac{(2n)!}{2^n \cdot n! \cdot 2^n \cdot n!} \cdot \frac{\pi}{2} = \frac{(2n)! \, \pi}{2^{2n+1} (n!)^2}.

Part (ii)

Let J=0f((xx1)2)dxJ = \int_0^\infty f((x - x^{-1})^2) \, dx.

First, we show J=0x2f((xx1)2)dxJ = \int_0^\infty x^{-2} f((x - x^{-1})^2) \, dx.

Substitute x=u1x = u^{-1}, so dx=u2dudx = -u^{-2} \, du. When x=0x = 0, uu \to \infty; when xx \to \infty, u=0u = 0. Also (xx1)2=(u1u)2=(uu1)2(x - x^{-1})^2 = (u^{-1} - u)^2 = (u - u^{-1})^2. So

J=0f((uu1)2)(u2)du=0u2f((uu1)2)du.J = \int_\infty^0 f((u - u^{-1})^2) \left(-u^{-2}\right) du = \int_0^\infty u^{-2} f((u - u^{-1})^2) \, du.

Renaming the dummy variable uu back to xx gives J=0x2f((xx1)2)dxJ = \int_0^\infty x^{-2} f((x-x^{-1})^2) \, dx.

Next, adding this to the original JJ:

2J=0(1+x2)f((xx1)2)dx,2J = \int_0^\infty (1 + x^{-2}) f((x - x^{-1})^2) \, dx,

so J=120(1+x2)f((xx1)2)dxJ = \frac{1}{2} \int_0^\infty (1 + x^{-2}) f((x - x^{-1})^2) \, dx.

Finally, substitute u=xx1u = x - x^{-1}. Then du=(1+x2)dxdu = (1 + x^{-2}) \, dx. As x0+x \to 0^+, uu \to -\infty; as xx \to \infty, u+u \to +\infty. So

J=12f(u2)du.J = \frac{1}{2} \int_{-\infty}^{\infty} f(u^2) \, du.

Since f(u2)f(u^2) is an even function of uu, this equals 0f(u2)du\int_0^\infty f(u^2) \, du.

Part (iii)

We evaluate 0x2n2(x4x2+1)ndx\int_0^\infty \frac{x^{2n-2}}{(x^4 - x^2 + 1)^n} \, dx.

Divide numerator and denominator by x2nx^{2n}:

x2n2(x4x2+1)n=x2(x21+x2)n.\frac{x^{2n-2}}{(x^4 - x^2 + 1)^n} = \frac{x^{-2}}{\left(x^2 - 1 + x^{-2}\right)^n}.

Using (xx1)2=x22+x2(x - x^{-1})^2 = x^2 - 2 + x^{-2}, we get x21+x2=(xx1)2+1x^2 - 1 + x^{-2} = (x - x^{-1})^2 + 1. So the integral becomes

0x2((xx1)2+1)ndx.\int_0^\infty \frac{x^{-2}}{\left((x - x^{-1})^2 + 1\right)^n} \, dx.

Set f(t)=(t+1)nf(t) = (t + 1)^{-n}, so the integrand is x2f((xx1)2)x^{-2} f((x - x^{-1})^2). By the result of part (ii),

0x2f((xx1)2)dx=0f(u2)du=0du(u2+1)n=In.\int_0^\infty x^{-2} f((x-x^{-1})^2) \, dx = \int_0^\infty f(u^2) \, du = \int_0^\infty \frac{du}{(u^2 + 1)^n} = I_n.

Using the formula from part (i) (replacing n+1n+1 by nn, i.e., replacing nn by n1n-1):

In=(2n2)!π22n1((n1)!)2.I_n = \frac{(2n-2)! \, \pi}{2^{2n-1} ((n-1)!)^2}.

Examiner Notes

This was the most popular question, being attempted by 85% of candidates, it was however only moderately successful although a number achieved full marks. Quite often, candidates ignored the helpful approach suggested by the LHS of the first required result, though, of course, it was possible to start from the first defined integral and achieve the same result. Many needlessly lost marks through omitting fairly straightforward steps such as the final evaluation in the last part of the question and failing to substantiate the simplified form of the result of part (i). Some got very carried away with tan or sinh substitutions in part (i), usually unsuccessfully and leading to monstrous amounts of algebraic working. A few failed to change the limits of integration in part (ii).


Topic: 数列与不等式 (Sequences and Inequalities)  |  Difficulty: Challenging  |  Marks: 20

2 If s1,s2,s3,s_1, s_2, s_3, \dots and t1,t2,t3,t_1, t_2, t_3, \dots are sequences of positive numbers, we write

(sn)(tn)(s_n) \leqslant (t_n)

to mean

“there exists a positive integer mm such that sntns_n \leqslant t_n whenever nmn \geqslant m”.

Determine whether each of the following statements is true or false. In the case of a true statement, you should give a proof which includes an explicit determination of an appropriate mm; in the case of a false statement, you should give a counterexample.

(i) (1000n)(n2)(1000n) \leqslant (n^2).

(ii) If it is not the case that (sn)(tn)(s_n) \leqslant (t_n), then it is the case that (tn)(sn)(t_n) \leqslant (s_n).

(iii) If (sn)(tn)(s_n) \leqslant (t_n) and (tn)(un)(t_n) \leqslant (u_n), then (sn)(un)(s_n) \leqslant (u_n).

(iv) (n2)(2n)(n^2) \leqslant (2^n).

Hint

Part (ii) is the only false statement, and a simple counter-example is sn=1s_n = 1 and tn=2t_n = 2 for nn odd, and sn=2s_n = 2 and tn=1t_n = 1 for nn even. Part (i) m=1000m = 1000 is a suitable value, then 1000n1000 \le n and as nn is positive, the inequality can be multiplied by it giving the required result. Part (iii) requires the use of the definition twice with values m1m_1 and m2m_2 say, and then using m=max(m1,m2)m = \max(m_1, m_2). For part (iv), we can choose m=4m = 4, and an inductive argument such as

(k+1)2=(1+1k)2k2(1+14)2k2<2k22×2k=2k+1(k+1)^2 = \left(1 + \frac{1}{k}\right)^2 k^2 \le \left(1 + \frac{1}{4}\right)^2 k^2 < 2k^2 \le 2 \times 2^k = 2^{k+1} works.

Model Solution

Part (i) (TRUE)

We need 1000nn21000n \leq n^2 for all nmn \geq m. Choose m=1000m = 1000. For n1000n \geq 1000, since n>0n > 0 we may divide both sides by nn to get 1000n1000 \leq n, which holds by our choice of mm. Multiplying back by n>0n > 0 gives 1000nn21000n \leq n^2. \blacksquare

Part (ii) (FALSE)

The statement says: if it is not the case that (sn)(tn)(s_n) \leq (t_n), then (tn)(sn)(t_n) \leq (s_n).

Counterexample: Define sn=1s_n = 1 for all nn, and tn=(1)n+1t_n = (-1)^n + 1 (so tn=2t_n = 2 for even nn and tn=0t_n = 0 for odd nn). Both are sequences of positive numbers… Actually, tn=0t_n = 0 for odd nn is not positive. Let me adjust.

Set sn=1s_n = 1 and tn=2t_n = 2 when nn is odd, and sn=2s_n = 2 and tn=1t_n = 1 when nn is even. Both sequences consist of positive numbers.

We check: (sn)(tn)(s_n) \leq (t_n) requires some mm such that sntns_n \leq t_n for all nmn \geq m. But for any mm, there exists an even nmn \geq m where sn=2>1=tns_n = 2 > 1 = t_n. So (sn)(tn)(s_n) \leq (t_n) fails.

Similarly, (tn)(sn)(t_n) \leq (s_n) requires some mm such that tnsnt_n \leq s_n for all nmn \geq m. But for any mm, there exists an odd nmn \geq m where tn=2>1=snt_n = 2 > 1 = s_n. So (tn)(sn)(t_n) \leq (s_n) also fails.

Since neither relation holds, the statement is false. \blacksquare

Part (iii) (TRUE)

Suppose (sn)(tn)(s_n) \leq (t_n) and (tn)(un)(t_n) \leq (u_n). By definition, there exist positive integers m1m_1 and m2m_2 such that

sntnfor all nm1,tnunfor all nm2.s_n \leq t_n \quad \text{for all } n \geq m_1, \qquad t_n \leq u_n \quad \text{for all } n \geq m_2.

Let m=max(m1,m2)m = \max(m_1, m_2). For all nmn \geq m, both inequalities hold, so sntnuns_n \leq t_n \leq u_n, giving snuns_n \leq u_n. Therefore (sn)(un)(s_n) \leq (u_n) with this mm. \blacksquare

Part (iv) (TRUE)

We prove by induction that n22nn^2 \leq 2^n for all n4n \geq 4 (taking m=4m = 4).

Base case: n=4n = 4. We have 16=1616 = 16, so 42=244^2 = 2^4. The inequality holds.

Inductive step: Suppose k22kk^2 \leq 2^k for some k4k \geq 4. We need (k+1)22k+1(k+1)^2 \leq 2^{k+1}.

Write

(k+1)2=k2(1+1k)2.(k+1)^2 = k^2 \left(1 + \frac{1}{k}\right)^2.

Since k4k \geq 4, we have 1+1k1+14=541 + \frac{1}{k} \leq 1 + \frac{1}{4} = \frac{5}{4}, so (1+1k)22516<2\left(1 + \frac{1}{k}\right)^2 \leq \frac{25}{16} < 2.

Therefore (k+1)2<2k2(k+1)^2 < 2k^2. By the inductive hypothesis k22kk^2 \leq 2^k, so

(k+1)2<22k=2k+1.(k+1)^2 < 2 \cdot 2^k = 2^{k+1}.

By induction, n22nn^2 \leq 2^n for all n4n \geq 4. We can take m=4m = 4. \blacksquare

Examiner Notes

Nearly three quarters attempted this, though again with moderate success as the main feature of the question was proof, and this was frequently handled cavalierly. Whilst it was not a crucial aspect of the question, ignoring the fact that the question deals with sequences of positive numbers was careless. Answers to the first part suffered at times from lack of argument or backwards logic. Part (ii) was generally well answered, although there were some silly counter-examples. This part suffered from those who completely missed the point of what the question was all about, forgetting the initial definition. Whilst most appreciated that part (iv) was true, there were many different methods used to attempt to prove it, and often unsuccessfully. Whilst induction using algebra is fairly straightforward, differentiation with or without logarithms and graphical methods frequently came to grief.


Topic: 极坐标 (Polar Coordinates)  |  Difficulty: Hard  |  Marks: 20

3 In this question, rr and θ\theta are polar coordinates with r0r \geqslant 0 and π<θπ-\pi < \theta \leqslant \pi, and aa and bb are positive constants.

Let LL be a fixed line and let AA be a fixed point not lying on LL. Then the locus of points that are a fixed distance (call it dd) from LL measured along lines through AA is called a conchoid of Nicomedes.

(i) Show that if

rasecθ=b,(*)|r - a \sec \theta| = b, \qquad \text{(*)}

where a>ba > b, then secθ>0\sec \theta > 0. Show that all points with coordinates satisfying ()(\ast) lie on a certain conchoid of Nicomedes (you should identify LL, dd and AA). Sketch the locus of these points.

(ii) In the case a<ba < b, sketch the curve (including the loop for which secθ<0\sec \theta < 0) given by

rasecθ=b.|r - a \sec \theta| = b.

Find the area of the loop in the case a=1a = 1 and b=2b = 2.

[Note: secθdθ=lnsecθ+tanθ+C\int \sec \theta \, \mathrm{d}\theta = \ln |\sec \theta + \tan \theta| + C.]

Hint

The part (i) inequality for secθ\sec \theta can be obtained by making rr the subject of the formula as r=asecθ±br = a \sec \theta \pm b and invoking a>ba > b remembering that r<0r < 0 is not permitted.

Then the points lie on a conchoid of Nicomedes with A being the pole (origin), d being bb, and L being the line r=asecθr = a \sec \theta ("x=ax = a").

In part (ii), the extra feature is the loop as specified with end-points at the pole corresponding to secθ=ba\sec \theta = \frac{-b}{a}.

So in the given case, the area is given by 2×122π3π(secθ+2)2dθ2 \times \frac{1}{2} \int_{\frac{2\pi}{3}}^{\pi} (\sec \theta + 2)^2 d\theta which is 4π3+34ln2+3\frac{4\pi}{3} + \sqrt{3} - 4 \ln |2 + \sqrt{3}|.

Model Solution

Part (i)

Showing secθ>0\sec\theta > 0:

The equation rasecθ=b|r - a\sec\theta| = b gives two cases:

r=asecθ+borr=asecθbr = a\sec\theta + b \qquad \text{or} \qquad r = a\sec\theta - b

Since r0r \geq 0:

For r=asecθbr = a\sec\theta - b: we need asecθba\sec\theta \geq b, so secθba>0\sec\theta \geq \frac{b}{a} > 0. Thus secθ>0\sec\theta > 0 immediately.

For r=asecθ+br = a\sec\theta + b: we need asecθba\sec\theta \geq -b, so secθba\sec\theta \geq -\frac{b}{a}. Suppose for contradiction that secθ<0\sec\theta < 0. Then secθ1|\sec\theta| \geq 1 (since cosθ1|\cos\theta| \leq 1), giving secθ1\sec\theta \leq -1. But a>b>0a > b > 0 implies ba>1-\frac{b}{a} > -1, so secθ1<ba\sec\theta \leq -1 < -\frac{b}{a}, contradicting secθba\sec\theta \geq -\frac{b}{a}. Therefore secθ>0\sec\theta > 0.

So in both cases, secθ>0\sec\theta > 0. \blacksquare

Identifying the conchoid:

Since secθ>0\sec\theta > 0, we have cosθ>0\cos\theta > 0, and the polar equation becomes r=asecθ±br = a\sec\theta \pm b.

The line r=asecθr = a\sec\theta is equivalent to rcosθ=ar\cos\theta = a, i.e., the vertical line x=ax = a in Cartesian coordinates. For a ray from the origin (the pole) at angle θ\theta, the point where this ray meets x=ax = a is at distance asecθa\sec\theta from the origin. Points satisfying rasecθ=b|r - a\sec\theta| = b are at distance bb from this intersection point, measured along the ray.

This is the conchoid of Nicomedes with:

  • AA = the pole (origin)
  • LL = the line x=ax = a
  • d=bd = b

Sketch:

The curve has two branches, with x=ax = a as a common vertical asymptote:

  • Outer branch (r=asecθ+br = a\sec\theta + b): lies to the right of x=ax = a, since x=rcosθ=a+bcosθ>ax = r\cos\theta = a + b\cos\theta > a. Passes through (a+b,0)(a+b, 0) at θ=0\theta = 0.
  • Inner branch (r=asecθbr = a\sec\theta - b): lies to the left of x=ax = a, since x=rcosθ=abcosθ<ax = r\cos\theta = a - b\cos\theta < a (but x>ab>0x > a - b > 0). Passes through (ab,0)(a-b, 0) at θ=0\theta = 0.

Both branches extend to infinity as θ±π2\theta \to \pm\frac{\pi}{2}, approaching the asymptote x=ax = a. Both are symmetric about the xx-axis.

Part (ii)

When a<ba < b, the equation rasecθ=b|r - a\sec\theta| = b again gives r=asecθ+br = a\sec\theta + b or r=asecθbr = a\sec\theta - b.

For r=asecθb0r = a\sec\theta - b \geq 0: secθba>1\sec\theta \geq \frac{b}{a} > 1, so θ(π2,arccosab][arccosab,π2)\theta \in \left(-\frac{\pi}{2}, -\arccos\frac{a}{b}\right] \cup \left[\arccos\frac{a}{b}, \frac{\pi}{2}\right). This branch starts at the origin (where r=0r = 0) and extends to infinity as θπ2|\theta| \to \frac{\pi}{2}.

For r=asecθ+br = a\sec\theta + b:

  • When secθ>0\sec\theta > 0 (i.e., θ(π2,π2)\theta \in (-\frac{\pi}{2}, \frac{\pi}{2})): r>0r > 0 always, giving a branch on the right similar to part (i).
  • When secθ<0\sec\theta < 0: r0r \geq 0 requires secθba\sec\theta \geq -\frac{b}{a}. Since a<ba < b, we have ba<1-\frac{b}{a} < -1. With secθ<0\sec\theta < 0 and secθba\sec\theta \geq -\frac{b}{a}, we get cosθab\cos\theta \leq -\frac{a}{b} (and cosθ<0\cos\theta < 0). So

θ[πarccosab,π][π,π+arccosab].\theta \in \left[\pi - \arccos\frac{a}{b},\, \pi\right] \cup \left[-\pi,\, -\pi + \arccos\frac{a}{b}\right].

This last piece forms a loop. At the endpoints θ=±(πarccosab)\theta = \pm\left(\pi - \arccos\frac{a}{b}\right):

r=a(ba)+b=0r = a\left(-\frac{b}{a}\right) + b = 0

so the loop passes through the origin. At θ=±π\theta = \pm\pi: r=a+b=ba>0r = -a + b = b - a > 0, giving the Cartesian point (ab,0)(a-b, 0) on the negative xx-axis (since a<ba < b).

Area of the loop for a=1a = 1, b=2b = 2:

Here arccosab=arccos12=π3\arccos\frac{a}{b} = \arccos\frac{1}{2} = \frac{\pi}{3}, so the loop is traced by r=secθ+2r = \sec\theta + 2 for θ[2π3,π][π,2π3]\theta \in \left[\frac{2\pi}{3},\, \pi\right] \cup \left[-\pi,\, -\frac{2\pi}{3}\right].

By symmetry of the integrand (since secθ\sec\theta is even, (secθ+2)2(\sec\theta + 2)^2 is even):

A=2×122π/3π(secθ+2)2dθ=2π/3π(secθ+2)2dθA = 2 \times \frac{1}{2}\int_{2\pi/3}^{\pi} (\sec\theta + 2)^2 \, d\theta = \int_{2\pi/3}^{\pi} (\sec\theta + 2)^2 \, d\theta

Expanding:

A=2π/3πsec2θdθ+42π/3πsecθdθ+42π/3πdθA = \int_{2\pi/3}^{\pi} \sec^2\theta \, d\theta + 4\int_{2\pi/3}^{\pi} \sec\theta \, d\theta + 4\int_{2\pi/3}^{\pi} d\theta

First integral:

2π/3πsec2θdθ=[tanθ]2π/3π=tanπtan2π3=0(3)=3\int_{2\pi/3}^{\pi} \sec^2\theta \, d\theta = \left[\tan\theta\right]_{2\pi/3}^{\pi} = \tan\pi - \tan\frac{2\pi}{3} = 0 - (-\sqrt{3}) = \sqrt{3}

Second integral (using the given antiderivative):

2π/3πsecθdθ=[lnsecθ+tanθ]2π/3π\int_{2\pi/3}^{\pi} \sec\theta \, d\theta = \left[\ln|\sec\theta + \tan\theta|\right]_{2\pi/3}^{\pi}

At θ=π\theta = \pi: secπ=1\sec\pi = -1, tanπ=0\tan\pi = 0, so ln1+0=ln1=0\ln|-1 + 0| = \ln 1 = 0.

At θ=2π3\theta = \frac{2\pi}{3}: sec2π3=2\sec\frac{2\pi}{3} = -2, tan2π3=3\tan\frac{2\pi}{3} = -\sqrt{3}, so ln2+(3)=ln(2+3)\ln|-2 + (-\sqrt{3})| = \ln(2 + \sqrt{3}).

Therefore the integral is 0ln(2+3)=ln(2+3)0 - \ln(2 + \sqrt{3}) = -\ln(2 + \sqrt{3}).

Third integral:

2π/3πdθ=π2π3=π3\int_{2\pi/3}^{\pi} d\theta = \pi - \frac{2\pi}{3} = \frac{\pi}{3}

Combining:

A=3+4(ln(2+3))+4π3=4π3+34ln(2+3)A = \sqrt{3} + 4\bigl(-\ln(2 + \sqrt{3})\bigr) + 4 \cdot \frac{\pi}{3} = \frac{4\pi}{3} + \sqrt{3} - 4\ln(2 + \sqrt{3})

\blacksquare

Examiner Notes

Under 20% attempted this, making it the least popular Pure question on the paper, and it was the least successfully attempted of all questions on the paper. Candidates seemed to find it intimidating, and many gave up before part (ii). They often got confused when dealing with separate cases and did not seem to understand what was required to show secθ>0\sec \theta > 0 in part (i). Those that did make a stab at (ii) usually omitted a factor of two and most failed to find the correct limit to use.


Topic: 复数 (Complex Numbers)  |  Difficulty: Challenging  |  Marks: 20

4 (i) If aa, bb and cc are all real, show that the equation

z3+az2+bz+c=0(*)z^3 + az^2 + bz + c = 0 \qquad \text{(*)}

has at least one real root.

(ii) Let

S1=z1+z2+z3,S2=z12+z22+z32,S3=z13+z23+z33,S_1 = z_1 + z_2 + z_3, \quad S_2 = z_1^2 + z_2^2 + z_3^2, \quad S_3 = z_1^3 + z_2^3 + z_3^3,

where z1z_1, z2z_2 and z3z_3 are the roots of the equation (*). Express aa and bb in terms of S1S_1 and S2S_2, and show that

6c=S13+3S1S22S3.6c = -S_1^3 + 3S_1S_2 - 2S_3.

(iii) The six real numbers rkr_k and θk\theta_k (k=1,2,3k = 1, 2, 3), where rk>0r_k > 0 and π<θk<π-\pi < \theta_k < \pi, satisfy

k=13rksin(θk)=0,k=13rk2sin(2θk)=0,k=13rk3sin(3θk)=0.\sum_{k=1}^3 r_k \sin(\theta_k) = 0, \quad \sum_{k=1}^3 r_k^2 \sin(2\theta_k) = 0, \quad \sum_{k=1}^3 r_k^3 \sin(3\theta_k) = 0.

Show that θk=0\theta_k = 0 for at least one value of kk.

Show further that if θ1=0\theta_1 = 0 then θ2=θ3\theta_2 = -\theta_3.

Hint

Part (i) is simply shown by considering the image of the function f(z)=z3+az2+bz+cf(z) = z^3 + az^2 + bz + c as z±z \rightarrow \pm\infty and then observing that the function is continuous and exhibits a sign-change. Part (ii) can be approached by writing z3+az2+bz+c=(zz1)(zz2)(zz3)z^3 + az^2 + bz + c = (z - z_1)(z - z_2)(z - z_3) giving a=S1a = -S_1, b=S12S22b = \frac{S_1^2 - S_2}{2}, which can be obtained by considering (z1+z2+z3)2(z_1 + z_2 + z_3)^2 and the required result for 6c6c which can be neatly obtained by considering f(z1)+f(z2)+f(z3)=0f(z_1) + f(z_2) + f(z_3) = 0.

Writing zk=rk(cosθk+isinθk)z_k = r_k(\cos \theta_k + i \sin \theta_k) for k=1,2,3k = 1, 2, 3, employing de Moivre’s theorem, the three sums imply the reality of S1S_1, S2S_2, and S3S_3, and hence aa, bb, and cc which by virtue of the result of part (i) yields the reality of z1z_1, z2z_2, or z3z_3 and hence the required result. The final result can be considered as two cases, the trivial one of all three roots being real, and the one where the other two are complex. The latter can be shown to give the required result by considering the real and imaginary parts of the roots of a real quadratic.

Model Solution

Part (i)

Let f(z)=z3+az2+bz+cf(z) = z^3 + az^2 + bz + c. Since a,b,cRa, b, c \in \mathbb{R}, ff is a continuous real-valued function on R\mathbb{R}.

As z+z \to +\infty: the leading term z3z^3 dominates, so f(z)+f(z) \to +\infty. As zz \to -\infty: the leading term z3z^3 dominates, so f(z)f(z) \to -\infty.

By the Intermediate Value Theorem, there exists at least one z0Rz_0 \in \mathbb{R} such that f(z0)=0f(z_0) = 0. Therefore the equation has at least one real root. \blacksquare

Part (ii)

Since z1,z2,z3z_1, z_2, z_3 are roots of z3+az2+bz+c=0z^3 + az^2 + bz + c = 0:

z3+az2+bz+c=(zz1)(zz2)(zz3)z^3 + az^2 + bz + c = (z - z_1)(z - z_2)(z - z_3)

Expanding the right side:

(zz1)(zz2)(zz3)=z3(z1+z2+z3)z2+(z1z2+z1z3+z2z3)zz1z2z3(z - z_1)(z - z_2)(z - z_3) = z^3 - (z_1 + z_2 + z_3)z^2 + (z_1z_2 + z_1z_3 + z_2z_3)z - z_1z_2z_3

Comparing coefficients of z2z^2:

a=(z1+z2+z3)=S1a = -(z_1 + z_2 + z_3) = -S_1

For bb, expand S12S_1^2:

S12=(z1+z2+z3)2=z12+z22+z32+2(z1z2+z1z3+z2z3)=S2+2bS_1^2 = (z_1 + z_2 + z_3)^2 = z_1^2 + z_2^2 + z_3^2 + 2(z_1z_2 + z_1z_3 + z_2z_3) = S_2 + 2b

Solving for bb:

b=S12S22b = \frac{S_1^2 - S_2}{2}

For cc: since zkz_k satisfies zk3+azk2+bzk+c=0z_k^3 + az_k^2 + bz_k + c = 0 for each k=1,2,3k = 1, 2, 3, summing these three equations:

(z13+z23+z33)+a(z12+z22+z32)+b(z1+z2+z3)+3c=0(z_1^3 + z_2^3 + z_3^3) + a(z_1^2 + z_2^2 + z_3^2) + b(z_1 + z_2 + z_3) + 3c = 0

S3+aS2+bS1+3c=0S_3 + aS_2 + bS_1 + 3c = 0

Substituting a=S1a = -S_1 and b=S12S22b = \frac{S_1^2 - S_2}{2}:

S3S1S2+S12S22S1+3c=0S_3 - S_1 S_2 + \frac{S_1^2 - S_2}{2} \cdot S_1 + 3c = 0

S3S1S2+S13S1S22+3c=0S_3 - S_1 S_2 + \frac{S_1^3 - S_1 S_2}{2} + 3c = 0

Combining the S1S2S_1 S_2 terms (writing S1S2=2S1S22-S_1 S_2 = -\frac{2S_1 S_2}{2}):

S3+S132S1S2S1S22+3c=0S_3 + \frac{S_1^3 - 2S_1 S_2 - S_1 S_2}{2} + 3c = 0

S3+S133S1S22+3c=0S_3 + \frac{S_1^3 - 3S_1 S_2}{2} + 3c = 0

3c=S3S133S1S22=2S3S13+3S1S223c = -S_3 - \frac{S_1^3 - 3S_1 S_2}{2} = \frac{-2S_3 - S_1^3 + 3S_1 S_2}{2}

Multiplying both sides by 2:

6c=S13+3S1S22S36c = -S_1^3 + 3S_1 S_2 - 2S_3

\blacksquare

Part (iii)

Define zk=rkeiθk=rk(cosθk+isinθk)z_k = r_k e^{i\theta_k} = r_k(\cos\theta_k + i\sin\theta_k) for k=1,2,3k = 1, 2, 3.

By de Moivre’s theorem, zkn=rkn(cos(nθk)+isin(nθk))z_k^n = r_k^n(\cos(n\theta_k) + i\sin(n\theta_k)).

Step 1: Show S1,S2,S3S_1, S_2, S_3 are real.

S1=k=13zk=k=13rkcosθk+ik=13rksinθk=k=13rkcosθkS_1 = \sum_{k=1}^3 z_k = \sum_{k=1}^3 r_k\cos\theta_k + i\sum_{k=1}^3 r_k\sin\theta_k = \sum_{k=1}^3 r_k\cos\theta_k

since rksinθk=0\sum r_k\sin\theta_k = 0. So S1RS_1 \in \mathbb{R}.

S2=k=13zk2=k=13rk2cos(2θk)+ik=13rk2sin(2θk)=k=13rk2cos(2θk)S_2 = \sum_{k=1}^3 z_k^2 = \sum_{k=1}^3 r_k^2\cos(2\theta_k) + i\sum_{k=1}^3 r_k^2\sin(2\theta_k) = \sum_{k=1}^3 r_k^2\cos(2\theta_k)

since rk2sin(2θk)=0\sum r_k^2\sin(2\theta_k) = 0. So S2RS_2 \in \mathbb{R}.

S3=k=13zk3=k=13rk3cos(3θk)+ik=13rk3sin(3θk)=k=13rk3cos(3θk)S_3 = \sum_{k=1}^3 z_k^3 = \sum_{k=1}^3 r_k^3\cos(3\theta_k) + i\sum_{k=1}^3 r_k^3\sin(3\theta_k) = \sum_{k=1}^3 r_k^3\cos(3\theta_k)

since rk3sin(3θk)=0\sum r_k^3\sin(3\theta_k) = 0. So S3RS_3 \in \mathbb{R}.

Step 2: Construct a cubic with real coefficients having z1,z2,z3z_1, z_2, z_3 as roots.

Since S1,S2,S3S_1, S_2, S_3 are real, define:

a=S1,b=S12S22,6c=S13+3S1S22S3a = -S_1, \qquad b = \frac{S_1^2 - S_2}{2}, \qquad 6c = -S_1^3 + 3S_1 S_2 - 2S_3

These are all real. We verify that z1,z2,z3z_1, z_2, z_3 are roots of z3+az2+bz+c=0z^3 + az^2 + bz + c = 0 by checking the Vieta relations:

  • z1+z2+z3=S1=az_1 + z_2 + z_3 = S_1 = -a \checkmark
  • z1z2+z1z3+z2z3=S12S22=bz_1z_2 + z_1z_3 + z_2z_3 = \frac{S_1^2 - S_2}{2} = b \checkmark (since S12=S2+2(z1z2+z1z3+z2z3)S_1^2 = S_2 + 2(z_1z_2 + z_1z_3 + z_2z_3))
  • z1z2z3=cz_1z_2z_3 = -c \checkmark (from 6c=S13+3S1S22S3=6z1z2z36c = -S_1^3 + 3S_1S_2 - 2S_3 = -6z_1z_2z_3, verified by expanding S13S_1^3 and S1S2S_1S_2)

Step 3: Apply part (i).

By part (i), this cubic with real coefficients has at least one real root, which must be one of z1,z2,z3z_1, z_2, z_3. If zkz_k is real and rk>0r_k > 0, then zk=rk(cosθk+isinθk)Rz_k = r_k(\cos\theta_k + i\sin\theta_k) \in \mathbb{R} requires sinθk=0\sin\theta_k = 0. Since π<θk<π-\pi < \theta_k < \pi, this gives θk=0\theta_k = 0.

Therefore θk=0\theta_k = 0 for at least one value of kk. \blacksquare

Showing θ2=θ3\theta_2 = -\theta_3 when θ1=0\theta_1 = 0:

If θ1=0\theta_1 = 0, then z1=r1>0z_1 = r_1 > 0 is real. Factor the cubic:

z3+az2+bz+c=(zz1)(z2+αz+β)z^3 + az^2 + bz + c = (z - z_1)(z^2 + \alpha z + \beta)

where α=a+z1\alpha = a + z_1 and β=b+z1(a+z1)\beta = b + z_1(a + z_1) are real (since a,b,z1a, b, z_1 are all real). The remaining roots z2,z3z_2, z_3 satisfy z2+αz+β=0z^2 + \alpha z + \beta = 0, a quadratic with real coefficients.

Case 1: The discriminant α24β0\alpha^2 - 4\beta \geq 0. Then z2,z3z_2, z_3 are both real, so θ2=θ3=0\theta_2 = \theta_3 = 0, giving θ2=θ3=0\theta_2 = -\theta_3 = 0.

Case 2: The discriminant α24β<0\alpha^2 - 4\beta < 0. Then z2,z3z_2, z_3 are complex conjugates: z2=z3z_2 = \overline{z_3}. Writing zk=rkeiθkz_k = r_k e^{i\theta_k}:

r2eiθ2=r3eiθ3r_2 e^{i\theta_2} = r_3 e^{-i\theta_3}

Taking moduli: r2=r3r_2 = r_3. Then eiθ2=eiθ3e^{i\theta_2} = e^{-i\theta_3}, so θ2=θ3+2nπ\theta_2 = -\theta_3 + 2n\pi for some integer nn. Since π<θ2,θ3<π-\pi < \theta_2, \theta_3 < \pi, we must have n=0n = 0, giving θ2=θ3\theta_2 = -\theta_3.

In both cases, θ2=θ3\theta_2 = -\theta_3. \blacksquare

Examiner Notes

Along with questions 5 and 7, attempted by just over three quarters, this was the third most popular question, though a little less successful than the most popular question 1. The first part was frequently not well attempted, but the second part was usually mastered. Attempts at the third part suffered from arguments with poor logical structure, though many did not get a start on this part.


Topic: 数论 (Number Theory)  |  Difficulty: Challenging  |  Marks: 20

5 (i) In the following argument to show that 2\sqrt{2} is irrational, give proofs appropriate for steps 3, 5 and 6.

  1. Assume that 2\sqrt{2} is rational.

  2. Define the set SS to be the set of positive integers with the following property:

nn is in SS if and only if n2n\sqrt{2} is an integer.

  1. Show that the set SS contains at least one positive integer.

  2. Define the integer kk to be the smallest positive integer in SS.

  3. Show that (21)k(\sqrt{2} - 1)k is in SS.

  4. Show that steps 4 and 5 are contradictory and hence that 2\sqrt{2} is irrational.

(ii) Prove that 2132^{\frac{1}{3}} is rational if and only if 2232^{\frac{2}{3}} is rational.

Use an argument similar to that of part (i) to prove that 2132^{\frac{1}{3}} and 2232^{\frac{2}{3}} are irrational.

Hint

(i) Step 3 is straightforward on the basis of steps 1 and 2, noting that no lowest terms restriction need be made in part 1. Step 5 requires that the given expression is a positive integer as well as well as being integer when multiplied by root two. Step 6 requires justification that 21<1\sqrt{2} - 1 < 1.

(ii) The rationality of 22/32^{2/3} on the basis of 21/32^{1/3} being rational is simply obtained by squaring the latter, and the opposite implication can be made by squaring the former or dividing 2 by the former. To construct the similar argument, let the set TT be the set of positive integers with the following property: nn is in TT if and only if n21/3n2^{1/3} and n22/3n2^{2/3} are integers, and taking tt to be the smallest positive integer in that set, consider t(22/31)t(2^{2/3} - 1) to produce the argument.

Model Solution

Part (i)

Step 3: Show that SS contains at least one positive integer.

By Step 1, 2\sqrt{2} is rational, so we can write 2=pq\sqrt{2} = \frac{p}{q} where pp and qq are positive integers. Then

q2=qpq=p,q\sqrt{2} = q \cdot \frac{p}{q} = p,

which is a positive integer. Therefore qq is a positive integer with q2Zq\sqrt{2} \in \mathbb{Z}, so qSq \in S. In particular, SS is non-empty. \blacksquare

Step 5: Show that (21)k(\sqrt{2} - 1)k is in SS.

We need to show two things: (a) (21)k(\sqrt{2} - 1)k is a positive integer, and (b) (21)k2(\sqrt{2} - 1)k \cdot \sqrt{2} is an integer.

For (a): Since 1<2<21 < \sqrt{2} < 2, we have 0<21<10 < \sqrt{2} - 1 < 1. As kk is a positive integer, (21)k>0(\sqrt{2} - 1)k > 0. Also, (21)k<k(\sqrt{2} - 1)k < k, so (21)k(\sqrt{2} - 1)k is a positive real number less than kk.

Now, since kSk \in S, the number k2k\sqrt{2} is an integer. Therefore

(21)k=k2k(\sqrt{2} - 1)k = k\sqrt{2} - k

is the difference of two integers, hence an integer. Combined with (21)k>0(\sqrt{2} - 1)k > 0, this is a positive integer.

For (b): We compute

(21)k2=k(22)=2kk2.(\sqrt{2} - 1)k \cdot \sqrt{2} = k(2 - \sqrt{2}) = 2k - k\sqrt{2}.

Since kk and k2k\sqrt{2} are both integers, this is an integer.

Therefore (21)k(\sqrt{2} - 1)k is a positive integer whose product with 2\sqrt{2} is an integer, so (21)kS(\sqrt{2} - 1)k \in S. \blacksquare

Step 6: Show that Steps 4 and 5 are contradictory.

From Step 5, (21)kS(\sqrt{2} - 1)k \in S, and from the analysis above, 0<(21)k<k0 < (\sqrt{2} - 1)k < k. But Step 4 defines kk as the smallest positive integer in SS. This is a contradiction: (21)k(\sqrt{2} - 1)k is a positive integer in SS that is strictly smaller than kk.

The contradiction arose from the assumption in Step 1 that 2\sqrt{2} is rational. Therefore 2\sqrt{2} is irrational. \blacksquare

Part (ii)

First, prove the equivalence: 21/32^{1/3} is rational if and only if 22/32^{2/3} is rational.

()(\Rightarrow): If 21/32^{1/3} is rational, then 22/3=(21/3)22^{2/3} = (2^{1/3})^2 is the square of a rational number, hence rational.

()(\Leftarrow): If 22/32^{2/3} is rational, then 21/3=222/32^{1/3} = \frac{2}{2^{2/3}} is the quotient of two rational numbers (with non-zero denominator), hence rational. \blacksquare

Now prove that 21/32^{1/3} and 22/32^{2/3} are irrational, using an argument similar to part (i).

Suppose for contradiction that 21/32^{1/3} is rational (equivalently, 22/32^{2/3} is rational, by the result above). Define the set

T={nZ+:n21/3Z and n22/3Z}.T = \{n \in \mathbb{Z}^+ : n \cdot 2^{1/3} \in \mathbb{Z} \text{ and } n \cdot 2^{2/3} \in \mathbb{Z}\}.

Since 21/32^{1/3} is rational, say 21/3=p/q2^{1/3} = p/q for positive integers p,qp, q, then 22/3=p2/q22^{2/3} = p^2/q^2. Choose n=q2n = q^2. Then n21/3=q2p/q=qpZn \cdot 2^{1/3} = q^2 \cdot p/q = qp \in \mathbb{Z} and n22/3=q2p2/q2=p2Zn \cdot 2^{2/3} = q^2 \cdot p^2/q^2 = p^2 \in \mathbb{Z}. So q2Tq^2 \in T, and TT is non-empty.

Since TT is a non-empty set of positive integers, by the well-ordering principle it has a smallest element; call it tt.

Now consider t(22/31)t(2^{2/3} - 1).

(a) We show t(22/31)t(2^{2/3} - 1) is a positive integer. Since 13=1<4=221^3 = 1 < 4 = 2^2 and 23=8>4=222^3 = 8 > 4 = 2^2, we have 1<22/3<21 < 2^{2/3} < 2, so 0<22/31<10 < 2^{2/3} - 1 < 1. Now

t(22/31)=t22/3t.t(2^{2/3} - 1) = t \cdot 2^{2/3} - t.

Since tTt \in T, the number t22/3t \cdot 2^{2/3} is an integer, so t22/3tt \cdot 2^{2/3} - t is an integer. Since t22/3>tt \cdot 2^{2/3} > t (because 22/3>12^{2/3} > 1), this integer is positive. Since 22/31<12^{2/3} - 1 < 1, we also have t(22/31)<tt(2^{2/3} - 1) < t.

(b) We show t(22/31)21/3t(2^{2/3} - 1) \cdot 2^{1/3} is an integer:

t(22/31)21/3=t(221/3)=2tt21/3.t(2^{2/3} - 1) \cdot 2^{1/3} = t(2 - 2^{1/3}) = 2t - t \cdot 2^{1/3}.

Since tTt \in T, the number t21/3t \cdot 2^{1/3} is an integer, so 2tt21/32t - t \cdot 2^{1/3} is an integer.

(c) We show t(22/31)22/3t(2^{2/3} - 1) \cdot 2^{2/3} is an integer:

t(22/31)22/3=t(24/322/3)=t(221/322/3)=2(t21/3)t22/3.t(2^{2/3} - 1) \cdot 2^{2/3} = t(2^{4/3} - 2^{2/3}) = t(2 \cdot 2^{1/3} - 2^{2/3}) = 2(t \cdot 2^{1/3}) - t \cdot 2^{2/3}.

Since tTt \in T, both t21/3t \cdot 2^{1/3} and t22/3t \cdot 2^{2/3} are integers, so this is an integer.

Therefore t(22/31)t(2^{2/3} - 1) is a positive integer in TT with t(22/31)<tt(2^{2/3} - 1) < t, contradicting the minimality of tt.

The contradiction shows that 21/32^{1/3} (and hence 22/32^{2/3}) is irrational. \blacksquare

Examiner Notes

Marginally less successful than question 2, a lot of candidates earned about half of the marks. Unfortunately, many candidates approached this on the basis of their knowledge of the standard irrationality proof for root two employing rational numbers expressed in lowest terms rather than observing the specified argument. In part (i), proving step 5 was frequently beset with omissions, and simple steps like 0<21<10 < \sqrt{2} - 1 < 1 were not acknowledged let alone justified. The first result of part (ii) caused few problems except to those that did not appreciate ‘if and only if’, but defining a suitable set in order to construct a similar argument to prove the irrationality of the cube roots of 2 and 2 squared was beyond most leading to mostly spurious logic.


Topic: 纯数 (Pure Mathematics)  |  Difficulty: Challenging  |  Marks: 20

6 (i) Let ww and zz be complex numbers, and let u=w+zu = w + z and v=w2+z2v = w^2 + z^2. Prove that ww and zz are real if and only if uu and vv are real and u22vu^2 \leqslant 2v.

**(ii)** The complex numbers $u$, $w$ and $z$ satisfy the equations
w+zu=0w2+z2u2=23w3+z3λu=λ\begin{aligned} w + z - u &= 0 \\ w^2 + z^2 - u^2 &= -\frac{2}{3} \\ w^3 + z^3 - \lambda u &= -\lambda \end{aligned}
where $\lambda$ is a positive real number. Show that for all values of $\lambda$ except one (which you should find) there are three possible values of $u$, all real.
Are $w$ and $z$ necessarily real? Give a proof or counterexample.
Hint

Treating the equations for uu and vv as simultaneous equations for ww and zz, one finds that w=u±2vu22w = \frac{u \pm \sqrt{2v - u^2}}{2} and z=u2vu22z = \frac{u \mp \sqrt{2v - u^2}}{2} which demonstrates that if uRu \in \mathbb{R} and u22vu^2 \le 2v, i.e. vRv \in \mathbb{R}, ww and zz are real. If ww and zz are real, then uu and vv are (trivially) and 2vu2=(wz)202v - u^2 = (w - z)^2 \ge 0.

In (ii), the first two equations yield 3wz=13wz = 1, making it possible to write the third equation as u(u21)=λ(u1)u(u^2 - 1) = \lambda(u - 1) which has an obvious factor of (u1)(u - 1) leading to u=1u = 1 or u=1±1+4λ2u = \frac{-1 \pm \sqrt{1 + 4\lambda}}{2} from the quadratic equation. If one of the solutions of the quadratic equation gives the same root u=1u = 1, then there are not three possible values, i.e. if λ=2\lambda = 2. From the first part of the question, for ww and zz to be real, we would want uu to be real, u223u^2 - \frac{2}{3} to be real, and u22(u223)u^2 \le 2(u^2 - \frac{2}{3}), in other words u243u^2 \geq \frac{4}{3}. So a counter-example could be u=1u = 1 giving 2w22w+23=02w^2 - 2w + \frac{2}{3} = 0 which has a negative discriminant.

Model Solution

Part (i)

We prove both directions.

()(\Rightarrow) Suppose ww and zz are real. Then u=w+zu = w + z and v=w2+z2v = w^2 + z^2 are clearly real. Moreover,

2vu2=2(w2+z2)(w+z)2=2w2+2z2w22wzz2=w22wz+z2=(wz)20,2v - u^2 = 2(w^2 + z^2) - (w + z)^2 = 2w^2 + 2z^2 - w^2 - 2wz - z^2 = w^2 - 2wz + z^2 = (w - z)^2 \geqslant 0,

so u22vu^2 \leqslant 2v. \blacksquare

()(\Leftarrow) Suppose uu and vv are real with u22vu^2 \leqslant 2v. Since w+z=uw + z = u and w2+z2=vw^2 + z^2 = v, we can find wzwz:

(w+z)2=w2+2wz+z2=v+2wz,(w + z)^2 = w^2 + 2wz + z^2 = v + 2wz,

so u2=v+2wzu^2 = v + 2wz, giving wz=u2v2wz = \frac{u^2 - v}{2}, which is real.

Now ww and zz are roots of the quadratic

t2(w+z)t+wz=t2ut+u2v2=0.t^2 - (w+z)t + wz = t^2 - ut + \frac{u^2 - v}{2} = 0.

The discriminant is

Δ=u24u2v2=u22(u2v)=2vu2.\Delta = u^2 - 4 \cdot \frac{u^2 - v}{2} = u^2 - 2(u^2 - v) = 2v - u^2.

Since u22vu^2 \leqslant 2v, we have Δ=2vu20\Delta = 2v - u^2 \geqslant 0, so the quadratic has real roots. Therefore ww and zz are real. \blacksquare

Part (ii)

From the first equation: w+z=uw + z = u.

From the second equation: w2+z2=u223w^2 + z^2 = u^2 - \frac{2}{3}.

Using (w+z)2=w2+2wz+z2(w + z)^2 = w^2 + 2wz + z^2:

u2=(u223)+2wz    wz=13.u^2 = \left(u^2 - \frac{2}{3}\right) + 2wz \implies wz = \frac{1}{3}.

For the third equation, we use the identity

w3+z3=(w+z)(w2wz+z2)=(w+z)((w2+z2)wz).w^3 + z^3 = (w + z)(w^2 - wz + z^2) = (w + z)\left((w^2 + z^2) - wz\right).

Substituting:

w3+z3=u((u223)13)=u(u21).w^3 + z^3 = u\left(\left(u^2 - \frac{2}{3}\right) - \frac{1}{3}\right) = u(u^2 - 1).

The third equation w3+z3λu=λw^3 + z^3 - \lambda u = -\lambda becomes

u(u21)λu=λ.u(u^2 - 1) - \lambda u = -\lambda.

Rearranging:

u3uλu+λ=0    u3(1+λ)u+λ=0.u^3 - u - \lambda u + \lambda = 0 \implies u^3 - (1 + \lambda)u + \lambda = 0.

We observe that u=1u = 1 is a root: 1(1+λ)+λ=01 - (1 + \lambda) + \lambda = 0. Factoring out (u1)(u - 1):

u3(1+λ)u+λ=(u1)(u2+uλ)=0.u^3 - (1 + \lambda)u + \lambda = (u - 1)(u^2 + u - \lambda) = 0.

The quadratic u2+uλ=0u^2 + u - \lambda = 0 has solutions

u=1±1+4λ2.u = \frac{-1 \pm \sqrt{1 + 4\lambda}}{2}.

Since λ>0\lambda > 0, we have 1+4λ>1>01 + 4\lambda > 1 > 0, so these are real and distinct. They are also distinct from u=1u = 1 unless u=1u = 1 satisfies u2+uλ=0u^2 + u - \lambda = 0, i.e., 1+1λ=01 + 1 - \lambda = 0, giving λ=2\lambda = 2.

Therefore: for all positive real λ\lambda except λ=2\lambda = 2, there are three distinct real values of uu. When λ=2\lambda = 2, the values u=1u = 1 coincide and there are only two distinct values: u=1u = 1 and u=2u = -2.

Are ww and zz necessarily real?

No. We use part (i): ww and zz are real if and only if uu and v=u223v = u^2 - \frac{2}{3} are real and u22vu^2 \leqslant 2v, i.e.,

u22(u223)=2u243    u243.u^2 \leqslant 2\left(u^2 - \frac{2}{3}\right) = 2u^2 - \frac{4}{3} \implies u^2 \geqslant \frac{4}{3}.

For the root u=1u = 1 (which exists for every positive λ\lambda): u2=1<43u^2 = 1 < \frac{4}{3}, so the condition fails, and w,zw, z need not be real.

Counterexample: Take λ=1\lambda = 1 and u=1u = 1. Then w+z=1w + z = 1 and wz=13wz = \frac{1}{3}, so ww and zz are roots of

t2t+13=0    t=1±1432=1±132=12±i23.t^2 - t + \frac{1}{3} = 0 \implies t = \frac{1 \pm \sqrt{1 - \frac{4}{3}}}{2} = \frac{1 \pm \sqrt{-\frac{1}{3}}}{2} = \frac{1}{2} \pm \frac{i}{2\sqrt{3}}.

These are not real. We verify all three equations:

  • w+z=1=uw + z = 1 = u. \checkmark
  • w2+z2=(w+z)22wz=123=13=u223w^2 + z^2 = (w + z)^2 - 2wz = 1 - \frac{2}{3} = \frac{1}{3} = u^2 - \frac{2}{3}. \checkmark
  • w3+z3=(w+z)33wz(w+z)=13131=0w^3 + z^3 = (w + z)^3 - 3wz(w + z) = 1 - 3 \cdot \frac{1}{3} \cdot 1 = 0, and λuλ=111=0\lambda u - \lambda = 1 \cdot 1 - 1 = 0. \checkmark

Therefore ww and zz are not necessarily real. \blacksquare

Examiner Notes

约 3/5 的考生尝试此题但成功率不高。(i) 部分需要证明双向蕴含(if and only if),难倒许多考生;(ii) 第一小题得分机会较好,但当 lambda=2 时无法产生三个不同 u 值的情况需注意;反例部分需明确展示其确实为反例。


Topic: 纯数 (Pure Mathematics)  |  Difficulty: Challenging  |  Marks: 20

7 An operator D is defined, for any function ff, by

Df(x)=xdf(x)dx.Df(x) = x \frac{df(x)}{dx} .

The notation $D^n$ means that D is applied $n$ times; for example

D2f(x)=xddx(xdf(x)dx).D^2f(x) = x \frac{d}{dx} \left( x \frac{df(x)}{dx} \right) .

Show that, for any constant $a$, $D^2x^a = a^2x^a$.
**(i)** Show that if $P(x)$ is a polynomial of degree $r$ (where $r \geqslant 1$) then, for any positive integer $n$, $D^nP(x)$ is also a polynomial of degree $r$.
**(ii)** Show that if $n$ and $m$ are positive integers with $n < m$, then $D^n(1 - x)^m$ is divisible by $(1 - x)^{m-n}$.
**(iii)** Deduce that, if $m$ and $n$ are positive integers with $n < m$, then

r=0m(1)r(mr)rn=0.\sum_{r=0}^{m} (-1)^r \binom{m}{r} r^n = 0 .

Hint

The opening result is simply achieved by following the given explanation for D2f(x)D^2 f(x) with f(x)=xaf(x) = x^a. Parts (i) and (ii) can both be shown using the principle of mathematical induction with initial statements

“Suppose DkP(x)D^k P(x) is a polynomial of degree rr i.e. DkP(x)=arxr+ar1xr1++a0D^k P(x) = a_r x^r + a_{r-1} x^{r-1} + \dots + a_0 for some integer kk.” and “Suppose Dk(1x)mD^k (1 - x)^m is divisible by (1x)mk(1 - x)^{m-k} i.e. Dk(1x)m=f(x)(1x)mkD^k (1 - x)^m = f(x)(1 - x)^{m-k} for some integer kk, with k<m1k < m - 1.” Part (iii) is obtained by expressing (1x)m(1 - x)^m in sigma notation (by the binomial theorem), then carrying out Dn(1x)mD^n (1 - x)^m using the idea in the stem, and finally invoking the result of part (ii) and then substituting x=1x = 1.

Model Solution

We first show D2xa=a2xaD^2 x^a = a^2 x^a.

D(xa)=xaxa1=axa.D(x^a) = x \cdot ax^{a-1} = ax^a.

D2(xa)=D(axa)=xddx(axa)=xa2xa1=a2xa.D^2(x^a) = D(ax^a) = x \cdot \frac{d}{dx}(ax^a) = x \cdot a^2 x^{a-1} = a^2 x^a.

More generally, by induction one can show Dnxa=anxaD^n x^a = a^n x^a for any positive integer nn.

Part (i)

We prove by induction on nn that if P(x)P(x) is a polynomial of degree r1r \geq 1, then DnP(x)D^n P(x) is a polynomial of degree rr.

Base case (n=1n = 1): Let P(x)=arxr+ar1xr1++a0P(x) = a_r x^r + a_{r-1} x^{r-1} + \cdots + a_0 with ar0a_r \neq 0. Then

DP(x)=xP(x)=x(rarxr1+(r1)ar1xr2++a1)=rarxr+(r1)ar1xr1++a1x.DP(x) = x \cdot P'(x) = x(ra_r x^{r-1} + (r-1)a_{r-1} x^{r-2} + \cdots + a_1) = ra_r x^r + (r-1)a_{r-1} x^{r-1} + \cdots + a_1 x.

Since r1r \geq 1 and ar0a_r \neq 0, the leading coefficient rar0ra_r \neq 0, so DP(x)DP(x) is a polynomial of degree rr.

Inductive step: Suppose DkP(x)D^k P(x) is a polynomial of degree rr for some positive integer kk. Write DkP(x)=brxr+br1xr1++b0D^k P(x) = b_r x^r + b_{r-1} x^{r-1} + \cdots + b_0 with br0b_r \neq 0. Then by the same argument as the base case, Dk+1P(x)=D(DkP(x))D^{k+1} P(x) = D(D^k P(x)) is a polynomial of degree rr with leading coefficient rbr0rb_r \neq 0.

By induction, DnP(x)D^n P(x) is a polynomial of degree rr for all positive integers nn. \blacksquare

Part (ii)

We prove by induction on nn that if nn and mm are positive integers with n<mn < m, then Dn(1x)mD^n(1-x)^m is divisible by (1x)mn(1-x)^{m-n}.

Base case (n=0n = 0): D0(1x)m=(1x)mD^0(1-x)^m = (1-x)^m, which is divisible by (1x)m0=(1x)m(1-x)^{m-0} = (1-x)^m. \checkmark

Inductive step: Suppose Dk(1x)m=g(x)(1x)mkD^k(1-x)^m = g(x)(1-x)^{m-k} for some polynomial g(x)g(x) and some non-negative integer k<mk < m. Then

Dk+1(1x)m=D(g(x)(1x)mk)=xddx(g(x)(1x)mk).D^{k+1}(1-x)^m = D\bigl(g(x)(1-x)^{m-k}\bigr) = x \frac{d}{dx}\bigl(g(x)(1-x)^{m-k}\bigr).

Using the product rule:

ddx(g(x)(1x)mk)=g(x)(1x)mk+g(x)(mk)(1x)mk1(1).\frac{d}{dx}\bigl(g(x)(1-x)^{m-k}\bigr) = g'(x)(1-x)^{m-k} + g(x)(m-k)(1-x)^{m-k-1}(-1).

So

Dk+1(1x)m=x[g(x)(1x)mk(mk)g(x)(1x)mk1]D^{k+1}(1-x)^m = x\bigl[g'(x)(1-x)^{m-k} - (m-k)g(x)(1-x)^{m-k-1}\bigr] =x(1x)mk1[g(x)(1x)(mk)g(x)].= x(1-x)^{m-k-1}\bigl[g'(x)(1-x) - (m-k)g(x)\bigr].

The bracketed expression is a polynomial in xx, and the power of (1x)(1-x) is mk1=m(k+1)m - k - 1 = m - (k+1). Since k+1mk + 1 \leq m (as k<mk < m), this is non-negative, so Dk+1(1x)mD^{k+1}(1-x)^m is divisible by (1x)m(k+1)(1-x)^{m-(k+1)}.

By induction, Dn(1x)mD^n(1-x)^m is divisible by (1x)mn(1-x)^{m-n} for all positive integers n<mn < m. \blacksquare

Part (iii)

By the binomial theorem:

(1x)m=r=0m(mr)(x)r=r=0m(1)r(mr)xr.(1-x)^m = \sum_{r=0}^{m} \binom{m}{r}(-x)^r = \sum_{r=0}^{m} (-1)^r \binom{m}{r} x^r.

We compute Dn(1x)mD^n(1-x)^m by applying DnD^n to this sum. Since D(xr)=rxrD(x^r) = r \cdot x^r (as shown in the stem), repeated application gives Dn(xr)=rnxrD^n(x^r) = r^n x^r. Therefore

Dn(1x)m=Dn(r=0m(1)r(mr)xr)=r=0m(1)r(mr)rnxr.D^n(1-x)^m = D^n\left(\sum_{r=0}^{m} (-1)^r \binom{m}{r} x^r\right) = \sum_{r=0}^{m} (-1)^r \binom{m}{r} r^n x^r.

By part (ii), Dn(1x)mD^n(1-x)^m is divisible by (1x)mn(1-x)^{m-n}. Since n<mn < m, we have mn1m - n \geq 1, which means Dn(1x)mD^n(1-x)^m has a factor of (1x)(1-x) and therefore vanishes at x=1x = 1:

Dn(1x)mx=1=0.D^n(1-x)^m\Big|_{x=1} = 0.

Substituting x=1x = 1 into the sum expression:

r=0m(1)r(mr)rn1r=r=0m(1)r(mr)rn=0.\sum_{r=0}^{m} (-1)^r \binom{m}{r} r^n \cdot 1^r = \sum_{r=0}^{m} (-1)^r \binom{m}{r} r^n = 0.

\blacksquare

Examiner Notes

与 Q2 并列第三受欢迎和第二成功。(i) 部分存在许多缺陷,很多考生无法进行正确的形式归纳;(ii) 部分一些考生认为 x 与 d/dx 可交换,经常从前几项推断出错误的 D^n(1-x)^m 公式。不令人意外地,朝给定结果推导时很多人通过错误的步骤(如在使用微分算子之前先将 x=1 代入 (1-x)^m)得到正确答案。


Topic: 纯数 (Pure Mathematics)  |  Difficulty: Hard  |  Marks: 20

8 (i) Show that under the changes of variable x=rcosθx = r \cos \theta and y=rsinθy = r \sin \theta, where rr is a function of θ\theta with r>0r > 0, the differential equation

(y+x)dydx=yx(y + x) \frac{dy}{dx} = y - x

becomes

drdθ+r=0.\frac{dr}{d\theta} + r = 0 \, .

Sketch a solution in the xx-yy plane.

(ii) Show that the solutions of

(y+xx(x2+y2))dydx=yxy(x2+y2)(y + x - x(x^2 + y^2)) \frac{dy}{dx} = y - x - y(x^2 + y^2)

can be written in the form

r2=11+Ae2θr^2 = \frac{1}{1 + Ae^{2\theta}}

and sketch the different forms of solution that arise according to the value of AA.

Hint

Transforming the differential equation in part (i) is made by substituting for xx and yy as given, for dydx\frac{dy}{dx} using dydθ=rcosθ+drdθsinθ\frac{dy}{d\theta} = r \cos \theta + \frac{dr}{d\theta} \sin \theta and a similar result for dxdθ\frac{dx}{d\theta}, and then simplifying the algebra by multiplying out and collecting like terms bearing in mind that a factor rr can be cancelled as r0r \neq 0. The transformed equation can be solved by separating variables or using an integrating factor, to give r=keθr = k e^{-\theta}, the sketch of which is a logarithmic spiral.

The same techniques for part (ii) yields a differential equation rr3+drdθ=0r - r^3 + \frac{dr}{d\theta} = 0 which is solved by separating the variables and then employing partial fractions giving a variety of possible solution sketches depending on the value of AA.

Model Solution

Part (i)

We substitute x=rcosθx = r\cos\theta and y=rsinθy = r\sin\theta into (y+x)dydx=yx(y+x)\frac{dy}{dx} = y - x, where r=r(θ)r = r(\theta).

First, compute the derivatives using the chain rule. Since rr is a function of θ\theta:

dxdθ=drdθcosθrsinθ,dydθ=drdθsinθ+rcosθ.\frac{dx}{d\theta} = \frac{dr}{d\theta}\cos\theta - r\sin\theta, \qquad \frac{dy}{d\theta} = \frac{dr}{d\theta}\sin\theta + r\cos\theta.

Therefore

dydx=dy/dθdx/dθ=drdθsinθ+rcosθdrdθcosθrsinθ.\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta} = \frac{\frac{dr}{d\theta}\sin\theta + r\cos\theta}{\frac{dr}{d\theta}\cos\theta - r\sin\theta}.

Substituting into the ODE (y+x)dydx=yx(y+x)\frac{dy}{dx} = y - x:

(rsinθ+rcosθ)drdθsinθ+rcosθdrdθcosθrsinθ=rsinθrcosθ.(r\sin\theta + r\cos\theta) \cdot \frac{\frac{dr}{d\theta}\sin\theta + r\cos\theta}{\frac{dr}{d\theta}\cos\theta - r\sin\theta} = r\sin\theta - r\cos\theta.

Since r>0r > 0, we cancel rr from both sides:

(sinθ+cosθ)drdθsinθ+rcosθdrdθcosθrsinθ=sinθcosθ.(\sin\theta + \cos\theta) \cdot \frac{\frac{dr}{d\theta}\sin\theta + r\cos\theta}{\frac{dr}{d\theta}\cos\theta - r\sin\theta} = \sin\theta - \cos\theta.

Cross-multiplying (assuming the denominator drdθcosθrsinθ0\frac{dr}{d\theta}\cos\theta - r\sin\theta \neq 0):

(\sin\theta + \cos\theta)\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta) = (\sin\theta - \cos\theta)\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

Expand the left side:

drdθsin2θ+rsinθcosθ+drdθsinθcosθ+rcos2θ\frac{dr}{d\theta}\sin^2\theta + r\sin\theta\cos\theta + \frac{dr}{d\theta}\sin\theta\cos\theta + r\cos^2\theta =drdθ(sin2θ+sinθcosθ)+r(sinθcosθ+cos2θ).= \frac{dr}{d\theta}(\sin^2\theta + \sin\theta\cos\theta) + r(\sin\theta\cos\theta + \cos^2\theta).

Expand the right side:

drdθsinθcosθrsin2θdrdθcos2θ+rsinθcosθ\frac{dr}{d\theta}\sin\theta\cos\theta - r\sin^2\theta - \frac{dr}{d\theta}\cos^2\theta + r\sin\theta\cos\theta =drdθ(sinθcosθcos2θ)+r(sin2θ+sinθcosθ).= \frac{dr}{d\theta}(\sin\theta\cos\theta - \cos^2\theta) + r(-\sin^2\theta + \sin\theta\cos\theta).

Setting left = right and collecting terms with drdθ\frac{dr}{d\theta} on one side:

drdθ[(sin2θ+sinθcosθ)(sinθcosθcos2θ)]=r[(sin2θ+sinθcosθ)(sinθcosθ+cos2θ)].\frac{dr}{d\theta}\bigl[(\sin^2\theta + \sin\theta\cos\theta) - (\sin\theta\cos\theta - \cos^2\theta)\bigr] = r\bigl[(-\sin^2\theta + \sin\theta\cos\theta) - (\sin\theta\cos\theta + \cos^2\theta)\bigr].

Simplifying the brackets:

drdθ(sin2θ+cos2θ)=r(sin2θcos2θ).\frac{dr}{d\theta}(\sin^2\theta + \cos^2\theta) = r(-\sin^2\theta - \cos^2\theta).

Since sin2θ+cos2θ=1\sin^2\theta + \cos^2\theta = 1:

drdθ=r,\frac{dr}{d\theta} = -r,

that is,

drdθ+r=0.\frac{dr}{d\theta} + r = 0.

\blacksquare

Sketch: This ODE has solution r=Ceθr = Ce^{-\theta} for a constant C>0C > 0. This is a logarithmic spiral: as θ\theta increases, rr decreases exponentially, and the curve spirals inwards toward the origin. The curve winds around the origin infinitely many times, getting closer and closer without ever reaching it.

Part (ii)

We substitute x=rcosθx = r\cos\theta, y=rsinθy = r\sin\theta into

(y+xx(x2+y2))dydx=yxy(x2+y2).(y + x - x(x^2 + y^2))\frac{dy}{dx} = y - x - y(x^2 + y^2).

Note that x2+y2=r2x^2 + y^2 = r^2, so x(x2+y2)=r3cosθx(x^2+y^2) = r^3\cos\theta and y(x2+y2)=r3sinθy(x^2+y^2) = r^3\sin\theta. The ODE becomes:

(rsinθ+rcosθr3cosθ)dydx=rsinθrcosθr3sinθ.(r\sin\theta + r\cos\theta - r^3\cos\theta)\frac{dy}{dx} = r\sin\theta - r\cos\theta - r^3\sin\theta.

Factor out rr (using r>0r > 0):

(sinθ+cosθr2cosθ)dydx=sinθcosθr2sinθ.(\sin\theta + \cos\theta - r^2\cos\theta)\frac{dy}{dx} = \sin\theta - \cos\theta - r^2\sin\theta.

Using the expression for dydx\frac{dy}{dx} from part (i):

(sinθ+cosθr2cosθ)drdθsinθ+rcosθdrdθcosθrsinθ=sinθcosθr2sinθ.(\sin\theta + \cos\theta - r^2\cos\theta) \cdot \frac{\frac{dr}{d\theta}\sin\theta + r\cos\theta}{\frac{dr}{d\theta}\cos\theta - r\sin\theta} = \sin\theta - \cos\theta - r^2\sin\theta.

Cross-multiplying:

(sinθ+cosθr2cosθ)(drdθsinθ+rcosθ)(\sin\theta + \cos\theta - r^2\cos\theta)\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right) =(sinθcosθr2sinθ)(drdθcosθrsinθ).= (\sin\theta - \cos\theta - r^2\sin\theta)\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

We can shortcut this algebra by noticing that the part (i) calculation is embedded here. Write the equation as

(sinθ+cosθr2cosθ)dydx=(sinθcosθr2sinθ).(\sin\theta + \cos\theta - r^2\cos\theta)\frac{dy}{dx} = (\sin\theta - \cos\theta - r^2\sin\theta).

This equals the part (i) equation with an extra "r2cosθ-r^2\cos\theta" on the left and "r2sinθ-r^2\sin\theta" on the right. So we can write

[(sinθ+cosθ)r2cosθ]dydx=(sinθcosθ)r2sinθ.\bigl[(\sin\theta + \cos\theta) - r^2\cos\theta\bigr]\frac{dy}{dx} = (\sin\theta - \cos\theta) - r^2\sin\theta.

Following the same algebraic steps as in part (i), the (sinθ+cosθ)dydx=sinθcosθ(\sin\theta + \cos\theta)\frac{dy}{dx} = \sin\theta - \cos\theta part yields drdθ=r\frac{dr}{d\theta} = -r as before. The extra terms contribute additional pieces. Let us work through this systematically.

From the cross-multiplied equation, expand both sides. The left side is:

[(sinθ+cosθ)r2cosθ](drdθsinθ+rcosθ)\left[(\sin\theta + \cos\theta) - r^2\cos\theta\right]\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right)

=(sinθ+cosθ)(drdθsinθ+rcosθ)r2cosθ(drdθsinθ+rcosθ).= (\sin\theta + \cos\theta)\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right) - r^2\cos\theta\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right).

The right side is:

[(sinθcosθ)r2sinθ](drdθcosθrsinθ)\left[(\sin\theta - \cos\theta) - r^2\sin\theta\right]\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right)

=(sinθcosθ)(drdθcosθrsinθ)r2sinθ(drdθcosθrsinθ).= (\sin\theta - \cos\theta)\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right) - r^2\sin\theta\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

From part (i), the first terms on each side are equal (both equal drdθ\frac{dr}{d\theta} after simplification). So we are left with:

r2cosθ(drdθsinθ+rcosθ)=r2sinθ(drdθcosθrsinθ).-r^2\cos\theta\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right) = -r^2\sin\theta\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

Dividing by r2-r^2 (valid since r>0r > 0):

cosθ(drdθsinθ+rcosθ)=sinθ(drdθcosθrsinθ).\cos\theta\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right) = \sin\theta\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

Expanding:

drdθsinθcosθ+rcos2θ=drdθsinθcosθrsin2θ.\frac{dr}{d\theta}\sin\theta\cos\theta + r\cos^2\theta = \frac{dr}{d\theta}\sin\theta\cos\theta - r\sin^2\theta.

The drdθsinθcosθ\frac{dr}{d\theta}\sin\theta\cos\theta terms cancel, leaving:

rcos2θ=rsin2θr(cos2θ+sin2θ)=0r=0.r\cos^2\theta = -r\sin^2\theta \qquad \Longrightarrow \qquad r(\cos^2\theta + \sin^2\theta) = 0 \qquad \Longrightarrow \qquad r = 0.

But r>0r > 0, so this seems contradictory. We need to be more careful: the part (i) simplification and the extra terms do not decouple in this way because drdθ\frac{dr}{d\theta} appears in the extra terms too.

Let us redo the full expansion properly. The cross-multiplied equation is:

LHS=(sinθ+cosθr2cosθ)(drdθsinθ+rcosθ),LHS = (\sin\theta + \cos\theta - r^2\cos\theta)\left(\frac{dr}{d\theta}\sin\theta + r\cos\theta\right),

RHS=(sinθcosθr2sinθ)(drdθcosθrsinθ).RHS = (\sin\theta - \cos\theta - r^2\sin\theta)\left(\frac{dr}{d\theta}\cos\theta - r\sin\theta\right).

Expanding LHSLHS:

=drdθsin2θ+rsinθcosθ+drdθsinθcosθ+rcos2θr2drdθsinθcosθr3cos2θ.= \frac{dr}{d\theta}\sin^2\theta + r\sin\theta\cos\theta + \frac{dr}{d\theta}\sin\theta\cos\theta + r\cos^2\theta - r^2\frac{dr}{d\theta}\sin\theta\cos\theta - r^3\cos^2\theta.

Expanding RHSRHS:

=drdθsinθcosθrsin2θdrdθcos2θ+rsinθcosθr2drdθsinθcosθ+r3sin2θ.= \frac{dr}{d\theta}\sin\theta\cos\theta - r\sin^2\theta - \frac{dr}{d\theta}\cos^2\theta + r\sin\theta\cos\theta - r^2\frac{dr}{d\theta}\sin\theta\cos\theta + r^3\sin^2\theta.

Setting LHS=RHSLHS = RHS and moving everything to the left:

drdθsin2θ+rsinθcosθ+drdθsinθcosθ+rcos2θr2drdθsinθcosθr3cos2θ\frac{dr}{d\theta}\sin^2\theta + r\sin\theta\cos\theta + \frac{dr}{d\theta}\sin\theta\cos\theta + r\cos^2\theta - r^2\frac{dr}{d\theta}\sin\theta\cos\theta - r^3\cos^2\theta drdθsinθcosθ+rsin2θ+drdθcos2θrsinθcosθ+r2drdθsinθcosθr3sin2θ=0.- \frac{dr}{d\theta}\sin\theta\cos\theta + r\sin^2\theta + \frac{dr}{d\theta}\cos^2\theta - r\sin\theta\cos\theta + r^2\frac{dr}{d\theta}\sin\theta\cos\theta - r^3\sin^2\theta = 0.

Collect drdθ\frac{dr}{d\theta} terms:

drdθ[sin2θ+sinθcosθ+cos2θsinθcosθsinθcosθ+cos2θ]\frac{dr}{d\theta}\bigl[\sin^2\theta + \sin\theta\cos\theta + \cos^2\theta - \sin\theta\cos\theta - \sin\theta\cos\theta + \cos^2\theta\bigr]

Wait, let me be more careful. The drdθ\frac{dr}{d\theta} terms from LHSLHS are: sin2θ+sinθcosθr2sinθcosθ\sin^2\theta + \sin\theta\cos\theta - r^2\sin\theta\cos\theta. From RHS-RHS: sinθcosθ+cos2θ+r2sinθcosθ-\sin\theta\cos\theta + \cos^2\theta + r^2\sin\theta\cos\theta. So the coefficient of drdθ\frac{dr}{d\theta} is:

sin2θ+sinθcosθr2sinθcosθsinθcosθ+cos2θ+r2sinθcosθ=sin2θ+cos2θ=1.\sin^2\theta + \sin\theta\cos\theta - r^2\sin\theta\cos\theta - \sin\theta\cos\theta + \cos^2\theta + r^2\sin\theta\cos\theta = \sin^2\theta + \cos^2\theta = 1.

Collect rr terms (without drdθ\frac{dr}{d\theta}):

From LHSLHS: sinθcosθ+cos2θr3cos2θ\sin\theta\cos\theta + \cos^2\theta - r^3\cos^2\theta. From RHS-RHS: sin2θsinθcosθr3sin2θ\sin^2\theta - \sin\theta\cos\theta - r^3\sin^2\theta.

The coefficient of rr is sinθcosθ+cos2θ+sin2θsinθcosθ=1\sin\theta\cos\theta + \cos^2\theta + \sin^2\theta - \sin\theta\cos\theta = 1.

The coefficient of r3r^3 is cos2θsin2θ=1-\cos^2\theta - \sin^2\theta = -1.

So the equation simplifies to:

drdθ+rr3=0,\frac{dr}{d\theta} + r - r^3 = 0,

that is,

drdθ=r3r=r(r21).\frac{dr}{d\theta} = r^3 - r = r(r^2 - 1).

\blacksquare

Solving by separation of variables:

drr(r21)=dθ.\frac{dr}{r(r^2 - 1)} = d\theta.

Using partial fractions:

1r(r21)=1r(r1)(r+1)=Ar+Br1+Cr+1.\frac{1}{r(r^2-1)} = \frac{1}{r(r-1)(r+1)} = \frac{A}{r} + \frac{B}{r-1} + \frac{C}{r+1}.

Multiplying through: 1=A(r1)(r+1)+Br(r+1)+Cr(r1)1 = A(r-1)(r+1) + Br(r+1) + Cr(r-1).

Setting r=0r = 0: 1=A(1)(1)1 = A(-1)(1), so A=1A = -1.

Setting r=1r = 1: 1=B(1)(2)1 = B(1)(2), so B=12B = \frac{1}{2}.

Setting r=1r = -1: 1=C(1)(2)1 = C(-1)(-2), so C=12C = \frac{1}{2}.

Therefore

(1r+1/2r1+1/2r+1)dr=dθ,\int\left(\frac{-1}{r} + \frac{1/2}{r-1} + \frac{1/2}{r+1}\right) dr = \int d\theta,

lnr+12lnr1+12lnr+1=θ+const,-\ln r + \frac{1}{2}\ln|r-1| + \frac{1}{2}\ln|r+1| = \theta + \text{const},

12lnr21lnr=θ+const,\frac{1}{2}\ln|r^2 - 1| - \ln r = \theta + \text{const},

lnr21r2=2θ+const,\ln\frac{|r^2 - 1|}{r^2} = 2\theta + \text{const},

r21r2=±e2θ+const=Be2θ\frac{r^2 - 1}{r^2} = \pm e^{2\theta + \text{const}} = Be^{2\theta}

where BB is a non-zero constant (absorbing the ±\pm into the constant, and noting BB can be positive or negative; also B=0B = 0 corresponds to r2=1r^2 = 1, i.e., the unit circle r=1r = 1).

Solving for r2r^2:

11r2=Be2θ1r2=1Be2θr2=11Be2θ.1 - \frac{1}{r^2} = Be^{2\theta} \qquad \Longrightarrow \qquad \frac{1}{r^2} = 1 - Be^{2\theta} \qquad \Longrightarrow \qquad r^2 = \frac{1}{1 - Be^{2\theta}}.

Writing A=BA = -B (so AA is an arbitrary real constant):

r2=11+Ae2θ.r^2 = \frac{1}{1 + Ae^{2\theta}}.

\blacksquare

Sketch of solutions according to the value of AA:

The solutions are r2=11+Ae2θr^2 = \frac{1}{1 + Ae^{2\theta}}. Since r2>0r^2 > 0, we need 1+Ae2θ>01 + Ae^{2\theta} > 0.

A=0A = 0: r2=1r^2 = 1, i.e., r=1r = 1. The solution is the unit circle.

A>0A > 0: As θ\theta \to -\infty, Ae2θ0Ae^{2\theta} \to 0, so r21r^2 \to 1. As θ\theta increases, Ae2θAe^{2\theta} grows, so r2r^2 decreases toward 00. The curve starts near the unit circle for large negative θ\theta and spirals inward, reaching r=0r = 0 when Ae2θAe^{2\theta} \to \infty, i.e., as θ\theta \to \infty. These are spirals that start near the unit circle and spiral in to the origin.

A<0A < 0: Write A=AA = -|A|. Then r2=11Ae2θr^2 = \frac{1}{1 - |A|e^{2\theta}}. We need 1Ae2θ>01 - |A|e^{2\theta} > 0, i.e., e2θ<1Ae^{2\theta} < \frac{1}{|A|}, i.e., θ<12lnA\theta < -\frac{1}{2}\ln|A|.

  • If A<1|A| < 1: The curve exists for θ<12lnA>0\theta < -\frac{1}{2}\ln|A| > 0. As θ\theta \to -\infty, r1r \to 1 again. As θ\theta increases toward 12lnA-\frac{1}{2}\ln|A|, the denominator 1Ae2θ0+1 - |A|e^{2\theta} \to 0^+, so r2r^2 \to \infty. These are spirals that start near the unit circle and spiral outward to infinity.

  • If A=1|A| = 1: The curve exists for θ<0\theta < 0. As θ0\theta \to 0^-, rr \to \infty. This is a spiral from the unit circle outward to infinity, defined for negative θ\theta.

  • If A>1|A| > 1: The curve exists for θ<12lnA<0\theta < -\frac{1}{2}\ln|A| < 0. Same qualitative behaviour as above but defined on a shorter interval.

In all cases with A<0A < 0, the solutions spiral outward from the unit circle to infinity (over a finite range of θ\theta).

For A>0A > 0, the solutions spiral inward from the unit circle to the origin. For A=0A = 0, the solution is the unit circle itself. The unit circle acts as a separatrix between the inward-spiralling and outward-spiralling families.

Examiner Notes

超过 80% 的考生尝试此题,是得分最高的题目。(i) 部分许多考生未意识到 r 是 theta 的函数;(ii) 部分变换后的微分方程通常正确,但分离变量后正确使用部分分式积分的频率低于预期。令人惊讶的是,尽管其余部分做得很好或完美,很多人没有尝试画任何解的图。没有人意识到常数 A 在 (ii) 中是真正任意的(因为积分中的对数项有绝对值)。解曲线的绘制考查了最优秀的学生。