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STEP2 2001 -- Pure Mathematics

Exam: STEP2  |  Year: 2001  |  Questions: Q1—Q8  |  Total marks per question: 20

All questions are pure mathematics. Model solutions are included below.

QTopicDifficultyKey Techniques
1二项式展开 Binomial ExpansionRoutine二项式定理,级数截断,误差分析
2取整函数与级数 Floor Function and SeriesStandard取整函数,分段分析,几何级数求和,极限
3立体几何 Solid GeometryStandard向量点积,立体几何,不等式证明
4三角方程 Trigonometric EquationsChallenging三角恒等式,因式分解,判别式分析
5微积分 CalculusStandard积分,驻点判断,曲线草图,指数函数
6积分 IntegrationChallenging多项式长除法,分部积分,换元积分
7复数 Complex NumbersChallenging复数几何表示,旋转,圆的方程求解
8微分方程 Differential EquationsChallenging周期函数性质,分离变量法,指数衰减

Topic: 二项式展开 Binomial Expansion  |  Difficulty: Routine  |  Marks: 20

1 Use the binomial expansion to obtain a polynomial of degree 2 which is a good approximation to (1−x)\sqrt{(1 - x)} when xx is small.

(i) By taking x=1/100x = 1/100, show that (11)≈79599/24000\sqrt{(11)} \approx 79599/24000, and estimate, correct to 1 significant figure, the error in this approximation. (You may assume that the error is given approximately by the first neglected term in the binomial expansion.)

(ii) Find a rational number which approximates (1111)\sqrt{(1111)} with an error of about 2×10−122 \times 10^{-12}.

Model Solution

Binomial expansion. We expand (1−x)1/2(1 - x)^{1/2} using the generalised binomial theorem:

(1−x)1/2=1+(1/21)(−x)+(1/22)(−x)2+⋯(1 - x)^{1/2} = 1 + \binom{1/2}{1}(-x) + \binom{1/2}{2}(-x)^2 + \cdots

Computing the binomial coefficients:

(1/21)=12,(1/22)=12⋅(−12)2!=−18\binom{1/2}{1} = \frac{1}{2}, \qquad \binom{1/2}{2} = \frac{\frac{1}{2} \cdot (-\frac{1}{2})}{2!} = -\frac{1}{8}

So the degree 2 approximation is:

1−x≈1−x2−x28(∗)\sqrt{1 - x} \approx 1 - \frac{x}{2} - \frac{x^2}{8} \qquad (*)

Part (i)

We write 11=1399\sqrt{11} = \frac{1}{3}\sqrt{99}. Since 99=100(1−1/100)99 = 100(1 - 1/100):

99=101−1100\sqrt{99} = 10\sqrt{1 - \tfrac{1}{100}}

and so

11=1031−1100.\sqrt{11} = \frac{10}{3}\sqrt{1 - \tfrac{1}{100}}.

Setting x=1/100x = 1/100 in the approximation:

1−1100≈1−1200−180000.\sqrt{1 - \tfrac{1}{100}} \approx 1 - \frac{1}{200} - \frac{1}{80000}.

Therefore:

11≈103(1−1200−180000)=103−10600−10240000.\sqrt{11} \approx \frac{10}{3}\left(1 - \frac{1}{200} - \frac{1}{80000}\right) = \frac{10}{3} - \frac{10}{600} - \frac{10}{240000}.

Simplifying each term with common denominator 240000240000:

103=800000240000,10600=4000240000,10240000=10240000.\frac{10}{3} = \frac{800000}{240000}, \qquad \frac{10}{600} = \frac{4000}{240000}, \qquad \frac{10}{240000} = \frac{10}{240000}. 11≈800000−4000−10240000=795990240000=7959924000.\sqrt{11} \approx \frac{800000 - 4000 - 10}{240000} = \frac{795990}{240000} = \frac{79599}{24000}.

Error estimate. The first neglected term in the binomial expansion is the k=3k = 3 term:

(1/23)(−x)3=12⋅(−12)⋅(−32)3!(−x3)=−x316.\binom{1/2}{3}(-x)^3 = \frac{\frac{1}{2} \cdot (-\frac{1}{2}) \cdot (-\frac{3}{2})}{3!}(-x^3) = -\frac{x^3}{16}.

With x=1/100x = 1/100:

∣−116×106∣=116 000 000≈6×10−8.\left|-\frac{1}{16 \times 10^6}\right| = \frac{1}{16\,000\,000} \approx 6 \times 10^{-8}.

Multiplying by 10/310/3 (the factor relating 11\sqrt{11} to 1−1/100\sqrt{1 - 1/100}):

Error≈103×6×10−8≈2×10−7.\text{Error} \approx \frac{10}{3} \times 6 \times 10^{-8} \approx 2 \times 10^{-7}.

To 1 significant figure, the error is 2×10−7\mathbf{2 \times 10^{-7}}.

Part (ii)

We write 1111=139999\sqrt{1111} = \frac{1}{3}\sqrt{9999}. Since 9999=10000(1−10−4)9999 = 10000(1 - 10^{-4}):

9999=1001−10−4,1111=10031−10−4.\sqrt{9999} = 100\sqrt{1 - 10^{-4}}, \qquad \sqrt{1111} = \frac{100}{3}\sqrt{1 - 10^{-4}}.

Setting x=10−4x = 10^{-4} in the degree 2 binomial approximation:

1−10−4≈1−10−42−10−88.\sqrt{1 - 10^{-4}} \approx 1 - \frac{10^{-4}}{2} - \frac{10^{-8}}{8}.

Therefore:

1111≈1003−1003⋅10−42−1003⋅10−88=1003−1600−124 000 000.\sqrt{1111} \approx \frac{100}{3} - \frac{100}{3} \cdot \frac{10^{-4}}{2} - \frac{100}{3} \cdot \frac{10^{-8}}{8} = \frac{100}{3} - \frac{1}{600} - \frac{1}{24\,000\,000}.

Combining over the common denominator 24 000 00024\,000\,000:

1003=800 000 00024 000 000,1600=40 00024 000 000,124 000 000=124 000 000.\frac{100}{3} = \frac{800\,000\,000}{24\,000\,000}, \qquad \frac{1}{600} = \frac{40\,000}{24\,000\,000}, \qquad \frac{1}{24\,000\,000} = \frac{1}{24\,000\,000}. 1111≈800 000 000−40 000−124 000 000=799 959 99924 000 000.\sqrt{1111} \approx \frac{800\,000\,000 - 40\,000 - 1}{24\,000\,000} = \frac{799\,959\,999}{24\,000\,000}.

Error check. The first neglected (k=3k = 3) term gives:

Error≈1003×(10−4)316=1003×10−1216≈2×10−12.\text{Error} \approx \frac{100}{3} \times \frac{(10^{-4})^3}{16} = \frac{100}{3} \times \frac{10^{-12}}{16} \approx 2 \times 10^{-12}.

This confirms the approximation 799 959 99924 000 000\dfrac{799\,959\,999}{24\,000\,000} has an error of about 2×10−122 \times 10^{-12}. ■\blacksquare


Topic: 取整函数与级数 Floor Function and Series  |  Difficulty: Standard  |  Marks: 20

2 Sketch the graph of the function [x/N][x/N], for 0<x<2N0 < x < 2N, where the notation [y][y] means the integer part of yy. (Thus [2.9]=2[2.9] = 2, [4]=4[4] = 4.)

(i) Prove that ∑k=12N(−1)[k/N]k=2N−N2.\sum_{k=1}^{2N} (-1)^{[k/N]}k = 2N - N^2.

(ii) Let SN=∑k=12N(−1)[k/N]2−k.S_N = \sum_{k=1}^{2N} (-1)^{[k/N]}2^{-k}. Find SNS_N in terms of NN and determine the limit of SNS_N as N→∞N \to \infty.

Model Solution

Graph of [x/N][x/N]. For 0<x<2N0 < x < 2N:

  • When 0<x<N0 < x < N: 0<x/N<10 < x/N < 1, so [x/N]=0[x/N] = 0.
  • When N≤x<2NN \le x < 2N: 1≤x/N<21 \le x/N < 2, so [x/N]=1[x/N] = 1.

The graph is a step function: value 00 on (0,N)(0, N), jumping to value 11 on [N,2N)[N, 2N).

Part (i)

We split the sum according to the value of [k/N][k/N]:

  • k=1,…,N−1k = 1, \ldots, N - 1: [k/N]=0[k/N] = 0, so (−1)[k/N]=+1(-1)^{[k/N]} = +1.
  • k=N,…,2N−1k = N, \ldots, 2N - 1: [k/N]=1[k/N] = 1, so (−1)[k/N]=−1(-1)^{[k/N]} = -1.
  • k=2Nk = 2N: [k/N]=2[k/N] = 2, so (−1)[k/N]=+1(-1)^{[k/N]} = +1.

Therefore:

∑k=12N(−1)[k/N]k=∑k=1N−1k  −  ∑k=N2N−1k  +  2N.\sum_{k=1}^{2N} (-1)^{[k/N]}k = \sum_{k=1}^{N-1} k \;-\; \sum_{k=N}^{2N-1} k \;+\; 2N.

Using ∑k=1mk=m(m+1)2\displaystyle\sum_{k=1}^{m} k = \frac{m(m+1)}{2}:

∑k=1N−1k=(N−1)N2=N2−N2.\sum_{k=1}^{N-1} k = \frac{(N-1)N}{2} = \frac{N^2 - N}{2}.

For the middle sum:

∑k=N2N−1k=∑k=12N−1k−∑k=1N−1k=(2N−1)(2N)2−(N−1)N2=2N(2N−1)−N(N−1)2.\sum_{k=N}^{2N-1} k = \sum_{k=1}^{2N-1} k - \sum_{k=1}^{N-1} k = \frac{(2N-1)(2N)}{2} - \frac{(N-1)N}{2} = \frac{2N(2N-1) - N(N-1)}{2}.

Expanding:

2N(2N−1)=4N2−2N,N(N−1)=N2−N.2N(2N-1) = 4N^2 - 2N, \qquad N(N-1) = N^2 - N. ∑k=N2N−1k=4N2−2N−N2+N2=3N2−N2.\sum_{k=N}^{2N-1} k = \frac{4N^2 - 2N - N^2 + N}{2} = \frac{3N^2 - N}{2}.

Substituting back:

∑k=12N(−1)[k/N]k=N2−N2−3N2−N2+2N=N2−N−3N2+N2+2N\sum_{k=1}^{2N} (-1)^{[k/N]}k = \frac{N^2 - N}{2} - \frac{3N^2 - N}{2} + 2N = \frac{N^2 - N - 3N^2 + N}{2} + 2N =−2N22+2N=−N2+2N=2N−N2.■= \frac{-2N^2}{2} + 2N = -N^2 + 2N = 2N - N^2. \qquad \blacksquare

Part (ii)

We split SN=∑k=12N(−1)[k/N]2−kS_N = \sum_{k=1}^{2N} (-1)^{[k/N]}2^{-k} using the same three ranges:

SN=∑k=1N−12−k⏟positive  −  ∑k=N2N−12−k⏟negative  +  2−2N.S_N = \underbrace{\sum_{k=1}^{N-1} 2^{-k}}_{\text{positive}} \;-\; \underbrace{\sum_{k=N}^{2N-1} 2^{-k}}_{\text{negative}} \;+\; 2^{-2N}.

Positive sum. This is a geometric series with first term 1/21/2, common ratio 1/21/2, and N−1N - 1 terms:

∑k=1N−12−k=12(1−(12)N−1)1−12=1−21−N.\sum_{k=1}^{N-1} 2^{-k} = \frac{\frac{1}{2}(1 - (\frac{1}{2})^{N-1})}{1 - \frac{1}{2}} = 1 - 2^{1-N}.

(When N=1N = 1 this sum is empty and equals 00, which the formula also gives since 20=12^{0} = 1.)

Negative sum. This is a geometric series with first term 2−N2^{-N}, common ratio 1/21/2, and NN terms:

∑k=N2N−12−k=2−N(1−2−N)1−12=2⋅2−N(1−2−N)=21−N(1−2−N).\sum_{k=N}^{2N-1} 2^{-k} = \frac{2^{-N}(1 - 2^{-N})}{1 - \frac{1}{2}} = 2 \cdot 2^{-N}(1 - 2^{-N}) = 2^{1-N}(1 - 2^{-N}).

Combining. Let u=2−Nu = 2^{-N}. Then 21−N=2u2^{1-N} = 2u and 2−2N=u22^{-2N} = u^2, so:

SN=(1−2u)−2u(1−u)+u2=1−2u−2u+2u2+u2=1−4u+3u2.S_N = (1 - 2u) - 2u(1 - u) + u^2 = 1 - 2u - 2u + 2u^2 + u^2 = 1 - 4u + 3u^2.

Factorising:

SN=(1−u)(1−3u)=(1−2−N)(1−3⋅2−N).S_N = (1 - u)(1 - 3u) = (1 - 2^{-N})(1 - 3 \cdot 2^{-N}).

Verification. For N=1N = 1: S1=(1−12)(1−32)=12⋅(−12)=−14S_1 = (1 - \frac{1}{2})(1 - \frac{3}{2}) = \frac{1}{2} \cdot (-\frac{1}{2}) = -\frac{1}{4}.

Directly: (−1)1⋅2−1+(−1)2⋅2−2=−12+14=−14(-1)^1 \cdot 2^{-1} + (-1)^2 \cdot 2^{-2} = -\frac{1}{2} + \frac{1}{4} = -\frac{1}{4}. Correct.

Limit. As N→∞N \to \infty, u=2−N→0u = 2^{-N} \to 0, so:

lim⁡N→∞SN=(1−0)(1−0)=1.\lim_{N \to \infty} S_N = (1 - 0)(1 - 0) = 1.

■\blacksquare


Topic: 立体几何 Solid Geometry  |  Difficulty: Standard  |  Marks: 20

3 The cuboid ABCDEFGHABCDEFGH is such AE,BF,CG,DHAE, BF, CG, DH are perpendicular to the opposite faces ABCDABCD and EFGHEFGH, and AB=2,BC=1,AE=λAB = 2, BC = 1, AE = \lambda. Show that if α\alpha is the acute angle between the diagonals AGAG and BHBH then cos⁡α=∣3−λ25+λ2∣\cos \alpha = \left| \frac{3 - \lambda^2}{5 + \lambda^2} \right|

Let RR be the ratio of the volume of the cuboid to its surface area. Show that R<1/3R < 1/3 for all possible values of λ\lambda.

Prove that, if R⩾1/4R \geqslant 1/4, then α⩽arccos⁡(1/9)\alpha \leqslant \arccos(1/9).

Model Solution

Part (i): Finding cos⁡α\cos\alpha

Set up coordinates with AA at the origin. Let AB⃗\vec{AB} point along the xx-axis, AD⃗\vec{AD} along the yy-axis, and AE⃗\vec{AE} along the zz-axis. Then:

A=(0,0,0),B=(2,0,0),C=(2,1,0),D=(0,1,0)A = (0,0,0),\quad B = (2,0,0),\quad C = (2,1,0),\quad D = (0,1,0) E=(0,0,λ),F=(2,0,λ),G=(2,1,λ),H=(0,1,λ)E = (0,0,\lambda),\quad F = (2,0,\lambda),\quad G = (2,1,\lambda),\quad H = (0,1,\lambda)

The two diagonals are:

AG⃗=(2, 1, λ),BH⃗=(−2, 1, λ)\vec{AG} = (2,\, 1,\, \lambda), \qquad \vec{BH} = (-2,\, 1,\, \lambda)

The dot product is:

AG⃗⋅BH⃗=(2)(−2)+(1)(1)+(λ)(λ)=−4+1+λ2=λ2−3\vec{AG} \cdot \vec{BH} = (2)(-2) + (1)(1) + (\lambda)(\lambda) = -4 + 1 + \lambda^2 = \lambda^2 - 3

The magnitudes are:

∣AG⃗∣=4+1+λ2=5+λ2,∣BH⃗∣=4+1+λ2=5+λ2|\vec{AG}| = \sqrt{4 + 1 + \lambda^2} = \sqrt{5 + \lambda^2}, \qquad |\vec{BH}| = \sqrt{4 + 1 + \lambda^2} = \sqrt{5 + \lambda^2}

The angle θ\theta between the two vectors satisfies:

cos⁡θ=AG⃗⋅BH⃗∣AG⃗∣∣BH⃗∣=λ2−35+λ2\cos\theta = \frac{\vec{AG} \cdot \vec{BH}}{|\vec{AG}||\vec{BH}|} = \frac{\lambda^2 - 3}{5 + \lambda^2}

Since α\alpha is the acute angle between the diagonals, we require cos⁡α≥0\cos\alpha \geq 0, so:

cos⁡α=∣λ2−35+λ2∣=∣3−λ25+λ2∣■\cos\alpha = \left| \frac{\lambda^2 - 3}{5 + \lambda^2} \right| = \left| \frac{3 - \lambda^2}{5 + \lambda^2} \right| \qquad \blacksquare

Part (ii): Showing R<1/3R < 1/3

The volume is:

V=AB×BC×AE=2×1×λ=2λV = AB \times BC \times AE = 2 \times 1 \times \lambda = 2\lambda

The surface area is:

S=2(AB⋅BC)+2(BC⋅AE)+2(AB⋅AE)=2(2)+2(λ)+2(2λ)=4+6λS = 2(AB \cdot BC) + 2(BC \cdot AE) + 2(AB \cdot AE) = 2(2) + 2(\lambda) + 2(2\lambda) = 4 + 6\lambda

The ratio is:

R=VS=2λ4+6λ=λ2+3λR = \frac{V}{S} = \frac{2\lambda}{4 + 6\lambda} = \frac{\lambda}{2 + 3\lambda}

We show R<1/3R < 1/3, i.e. λ2+3λ<13\dfrac{\lambda}{2 + 3\lambda} < \dfrac{1}{3}.

Since λ>0\lambda > 0, the denominator 2+3λ>02 + 3\lambda > 0, so cross-multiplying:

3λ<2+3λ  ⟹  0<23\lambda < 2 + 3\lambda \implies 0 < 2

This holds for all λ>0\lambda > 0, so R<1/3R < 1/3 for all possible values of λ\lambda. ■\qquad \blacksquare

Part (iii): If R≥1/4R \geq 1/4 then α≤arccos⁡(1/9)\alpha \leq \arccos(1/9)

First, find the constraint on λ\lambda from R≥1/4R \geq 1/4:

λ2+3λ≥14\frac{\lambda}{2 + 3\lambda} \geq \frac{1}{4}

Since 2+3λ>02 + 3\lambda > 0:

4λ≥2+3λ  ⟹  λ≥24\lambda \geq 2 + 3\lambda \implies \lambda \geq 2

Now, α≤arccos⁡(1/9)\alpha \leq \arccos(1/9) is equivalent to cos⁡α≥1/9\cos\alpha \geq 1/9 (since arccos⁡\arccos is a decreasing function and α\alpha is acute so cos⁡α≥0\cos\alpha \geq 0).

When λ≥2\lambda \geq 2: λ2≥4>3\lambda^2 \geq 4 > 3, so 3−λ2<03 - \lambda^2 < 0 and

cos⁡α=λ2−35+λ2\cos\alpha = \frac{\lambda^2 - 3}{5 + \lambda^2}

We show λ2−35+λ2≥19\dfrac{\lambda^2 - 3}{5 + \lambda^2} \geq \dfrac{1}{9}. Since 5+λ2>05 + \lambda^2 > 0:

9(λ2−3)≥5+λ29(\lambda^2 - 3) \geq 5 + \lambda^2 9λ2−27≥5+λ29\lambda^2 - 27 \geq 5 + \lambda^2 8λ2≥328\lambda^2 \geq 32 λ2≥4\lambda^2 \geq 4 λ≥2(since λ>0)\lambda \geq 2 \quad (\text{since } \lambda > 0)

This is precisely the condition from R≥1/4R \geq 1/4. Therefore, if R≥1/4R \geq 1/4 then λ≥2\lambda \geq 2, which gives cos⁡α≥1/9\cos\alpha \geq 1/9, i.e. α≤arccos⁡(1/9)\alpha \leq \arccos(1/9). ■\qquad \blacksquare


Topic: 三角方程 Trigonometric Equations  |  Difficulty: Challenging  |  Marks: 20

4 Let f(x)=Psin⁡x+Qsin⁡2x+Rsin⁡3x.f(x) = P \sin x + Q \sin 2x + R \sin 3x . Show that if Q2<4R(P−R)Q^2 < 4R(P - R), then the only values of xx for which f(x)=0f(x) = 0 are given by x=mπx = m\pi, where mm is an integer. [You may assume that sin⁡3x=sin⁡x(4cos⁡2x−1)\sin 3x = \sin x(4 \cos^2 x - 1).]

Now let g(x)=sin⁡2nx+sin⁡4nx−sin⁡6nx,g(x) = \sin 2nx + \sin 4nx - \sin 6nx, where nn is a positive integer and 0<x<π/20 < x < \pi/2. Find an expression for the largest root of the equation g(x)=0g(x) = 0, distinguishing between the cases where nn is even and nn is odd.

Model Solution

Part (i): Showing that Q2<4R(P−R)Q^2 < 4R(P-R) implies f(x)=0f(x) = 0 only when x=mπx = m\pi

We are given:

f(x)=Psin⁡x+Qsin⁡2x+Rsin⁡3xf(x) = P\sin x + Q\sin 2x + R\sin 3x

and the identity sin⁡3x=sin⁡x(4cos⁡2x−1)\sin 3x = \sin x(4\cos^2 x - 1).

We also need sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x\cos x. Factor out sin⁡x\sin x:

f(x)=sin⁡x[P+2Qcos⁡x+R(4cos⁡2x−1)]f(x) = \sin x \bigl[P + 2Q\cos x + R(4\cos^2 x - 1)\bigr]

=sin⁡x[4Rcos⁡2x+2Qcos⁡x+(P−R)]= \sin x \bigl[4R\cos^2 x + 2Q\cos x + (P - R)\bigr]

So f(x)=0f(x) = 0 when either:

  • sin⁡x=0\sin x = 0, which gives x=mπx = m\pi for integer mm; or
  • 4Rcos⁡2x+2Qcos⁡x+(P−R)=04R\cos^2 x + 2Q\cos x + (P - R) = 0.

Let t=cos⁡xt = \cos x. The second equation becomes the quadratic:

4Rt2+2Qt+(P−R)=04Rt^2 + 2Qt + (P - R) = 0

We compute the discriminant:

Δ=(2Q)2−4(4R)(P−R)=4Q2−16R(P−R)=4[Q2−4R(P−R)]\Delta = (2Q)^2 - 4(4R)(P - R) = 4Q^2 - 16R(P - R) = 4\bigl[Q^2 - 4R(P - R)\bigr]

The condition Q2<4R(P−R)Q^2 < 4R(P - R) is equivalent to Δ<0\Delta < 0.

When Δ<0\Delta < 0, the quadratic 4Rt2+2Qt+(P−R)=04Rt^2 + 2Qt + (P - R) = 0 has no real roots in tt, and hence there is no real value of cos⁡x\cos x satisfying it. (Note: we also need 4R>04R > 0, i.e. R>0R > 0, for the quadratic to open upward and be strictly positive everywhere when Δ<0\Delta < 0. If R>0R > 0 and Δ<0\Delta < 0, the quadratic is always positive, so it is never zero.)

Therefore, when Q2<4R(P−R)Q^2 < 4R(P - R) (and R>0R > 0), the only solutions come from sin⁡x=0\sin x = 0, giving x=mπx = m\pi for integer mm. ■\qquad \blacksquare


Part (ii): Largest root of g(x)=0g(x) = 0 for 0<x<π/20 < x < \pi/2

We have:

g(x)=sin⁡2nx+sin⁡4nx−sin⁡6nxg(x) = \sin 2nx + \sin 4nx - \sin 6nx

Using the sum-to-product formula sin⁡A+sin⁡B=2sin⁡ ⁣(A+B2)cos⁡ ⁣(A−B2)\sin A + \sin B = 2\sin\!\left(\frac{A+B}{2}\right)\cos\!\left(\frac{A-B}{2}\right) on the first two terms:

sin⁡2nx+sin⁡4nx=2sin⁡3nxcos⁡nx\sin 2nx + \sin 4nx = 2\sin 3nx \cos nx

Also, by the double angle formula:

sin⁡6nx=2sin⁡3nxcos⁡3nx\sin 6nx = 2\sin 3nx \cos 3nx

So:

g(x)=2sin⁡3nxcos⁡nx−2sin⁡3nxcos⁡3nx=2sin⁡3nx(cos⁡nx−cos⁡3nx)g(x) = 2\sin 3nx \cos nx - 2\sin 3nx \cos 3nx = 2\sin 3nx(\cos nx - \cos 3nx)

Now apply the identity cos⁡A−cos⁡B=−2sin⁡ ⁣(A+B2)sin⁡ ⁣(A−B2)\cos A - \cos B = -2\sin\!\left(\frac{A+B}{2}\right)\sin\!\left(\frac{A-B}{2}\right):

cos⁡nx−cos⁡3nx=−2sin⁡2nxsin⁡(−nx)=2sin⁡2nxsin⁡nx\cos nx - \cos 3nx = -2\sin 2nx \sin(-nx) = 2\sin 2nx \sin nx

Therefore:

g(x)=2sin⁡3nx⋅2sin⁡2nxsin⁡nx=4sin⁡nxsin⁡2nxsin⁡3nxg(x) = 2\sin 3nx \cdot 2\sin 2nx \sin nx = 4\sin nx \sin 2nx \sin 3nx

So g(x)=0g(x) = 0 when sin⁡nx=0\sin nx = 0, sin⁡2nx=0\sin 2nx = 0, or sin⁡3nx=0\sin 3nx = 0.

For 0<x<π/20 < x < \pi/2:

  • sin⁡nx=0  ⟹  nx=kπ  ⟹  x=kπn\sin nx = 0 \implies nx = k\pi \implies x = \dfrac{k\pi}{n}, for k=1,2,…,n−1k = 1, 2, \ldots, n-1 (since 0<kπ/n<π/20 < k\pi/n < \pi/2 requires k<n/2k < n/2, i.e. k=1,…,⌊(n−1)/2⌋k = 1, \ldots, \lfloor(n-1)/2\rfloor).

  • sin⁡2nx=0  ⟹  2nx=kπ  ⟹  x=kπ2n\sin 2nx = 0 \implies 2nx = k\pi \implies x = \dfrac{k\pi}{2n}, for k=1,…,n−1k = 1, \ldots, n-1.

  • sin⁡3nx=0  ⟹  3nx=kπ  ⟹  x=kπ3n\sin 3nx = 0 \implies 3nx = k\pi \implies x = \dfrac{k\pi}{3n}, for k=1,…,⌊(3n−1)/2⌋k = 1, \ldots, \lfloor(3n-1)/2\rfloor.

The roots from sin⁡nx=0\sin nx = 0 are a subset of the roots from sin⁡2nx=0\sin 2nx = 0 (since kπ/n=2kπ/2nk\pi/n = 2k\pi/2n), which are in turn a subset of the roots from sin⁡3nx=0\sin 3nx = 0 (since kπ/2n=3kπ/6nk\pi/2n = 3k\pi/6n). So the complete set of roots is:

x=kπ3n,k=1,2,…,⌊3n−12⌋x = \frac{k\pi}{3n}, \qquad k = 1, 2, \ldots, \left\lfloor \frac{3n-1}{2} \right\rfloor

(The condition x<π/2x < \pi/2 gives kπ/3n<π/2k\pi/3n < \pi/2, so k<3n/2k < 3n/2, i.e. k≤⌊(3n−1)/2⌋k \leq \lfloor(3n-1)/2\rfloor.)

The largest root corresponds to k=⌊(3n−1)/2⌋k = \lfloor(3n-1)/2\rfloor.

Case 1: nn is even. Write n=2mn = 2m. Then 3n/2=3m3n/2 = 3m is an integer, and k<3mk < 3m gives kmax⁡=3m−1=3n2−1=3n−22k_{\max} = 3m - 1 = \frac{3n}{2} - 1 = \frac{3n - 2}{2}.

xmax⁡=(3n−2)π2⋅3n=(3n−2)π6nx_{\max} = \frac{(3n - 2)\pi}{2 \cdot 3n} = \frac{(3n-2)\pi}{6n}

Check: ⌊(3n−1)/2⌋=⌊3m−1/2⌋=3m−1=(3n−2)/2\lfloor(3n-1)/2\rfloor = \lfloor 3m - 1/2\rfloor = 3m - 1 = (3n-2)/2. Correct.

Case 2: nn is odd. Write n=2m+1n = 2m + 1. Then 3n/2=3m+3/23n/2 = 3m + 3/2 is not an integer, and k<3m+3/2k < 3m + 3/2 gives kmax⁡=3m+1=3(n−1)2+1=3n−12k_{\max} = 3m + 1 = \frac{3(n-1)}{2} + 1 = \frac{3n - 1}{2}.

xmax⁡=(3n−1)π2⋅3n=(3n−1)π6nx_{\max} = \frac{(3n-1)\pi}{2 \cdot 3n} = \frac{(3n-1)\pi}{6n}

Check: ⌊(3n−1)/2⌋=⌊3m+1⌋=3m+1=(3n−1)/2\lfloor(3n-1)/2\rfloor = \lfloor 3m + 1\rfloor = 3m + 1 = (3n-1)/2. Correct.

Summary. The largest root of g(x)=0g(x) = 0 in (0,π/2)(0, \pi/2) is:

xmax⁡={(3n−1)π6nif n is odd(3n−2)π6nif n is evenx_{\max} = \begin{cases} \dfrac{(3n-1)\pi}{6n} & \text{if } n \text{ is odd} \\[8pt] \dfrac{(3n-2)\pi}{6n} & \text{if } n \text{ is even} \end{cases}


Topic: 微积分 Calculus  |  Difficulty: Standard  |  Marks: 20

5 The curve C1C_1 passes through the origin in the xx–yy plane and its gradient is given by dydx=x(1−x2)e−x2.\frac{dy}{dx} = x(1 - x^2)e^{-x^2}. Show that C1C_1 has a minimum point at the origin and a maximum point at (1,12e−1)(1, \frac{1}{2}e^{-1}). Find the coordinates of the other stationary point. Give a rough sketch of C1C_1.

The curve C2C_2 passes through the origin and its gradient is given by dydx=x(1−x2)e−x3.\frac{dy}{dx} = x(1 - x^2)e^{-x^3}. Show that C2C_2 has a minimum point at the origin and a maximum point at (1,k)(1, k), where k>12e−1k > \frac{1}{2}e^{-1}. (You need not find kk.)

Model Solution

Finding y(x)y(x) for C1C_1.

We integrate dydx=x(1−x2)e−x2=(x−x3)e−x2\dfrac{dy}{dx} = x(1 - x^2)e^{-x^2} = (x - x^3)e^{-x^2}.

For ∫x e−x2 dx\int x\,e^{-x^2}\,dx: set u=x2u = x^2, du=2x dxdu = 2x\,dx, so ∫x e−x2 dx=12∫e−u du=−12e−x2+C.\int x\,e^{-x^2}\,dx = \tfrac{1}{2}\int e^{-u}\,du = -\tfrac{1}{2}e^{-x^2} + C.

For ∫x3e−x2 dx\int x^3 e^{-x^2}\,dx: set u=x2u = x^2, du=2x dxdu = 2x\,dx, so ∫x3e−x2 dx=12∫u e−u du.\int x^3 e^{-x^2}\,dx = \tfrac{1}{2}\int u\,e^{-u}\,du. Integrate by parts with a=ua = u, db=e−u dudb = e^{-u}\,du: ∫u e−u du=−u e−u+∫e−u du=−u e−u−e−u=−(u+1)e−u.\int u\,e^{-u}\,du = -u\,e^{-u} + \int e^{-u}\,du = -u\,e^{-u} - e^{-u} = -(u+1)e^{-u}. So ∫x3e−x2 dx=−12(x2+1)e−x2+C.\int x^3 e^{-x^2}\,dx = -\tfrac{1}{2}(x^2 + 1)e^{-x^2} + C.

Combining: y=−12e−x2+12(x2+1)e−x2+C=12x2e−x2+C.y = -\tfrac{1}{2}e^{-x^2} + \tfrac{1}{2}(x^2 + 1)e^{-x^2} + C = \tfrac{1}{2}x^2 e^{-x^2} + C.

Since C1C_1 passes through the origin, y(0)=0y(0) = 0, giving C=0C = 0. Therefore y=12x2e−x2.y = \tfrac{1}{2}x^2 e^{-x^2}.

Stationary points. Setting dydx=0\dfrac{dy}{dx} = 0: since e−x2≠0e^{-x^2} \neq 0, we need x(1−x2)=0x(1 - x^2) = 0, giving x=0,  x=1,  x=−1x = 0,\; x = 1,\; x = -1.

At x=0x = 0: y=0y = 0, so the point is (0,0)(0, 0).

At x=1x = 1: y=12e−1y = \tfrac{1}{2}e^{-1}, so the point is (1,12e−1)(1, \tfrac{1}{2}e^{-1}).

At x=−1x = -1: y=12e−1y = \tfrac{1}{2}e^{-1}, so the point is (−1,12e−1)(-1, \tfrac{1}{2}e^{-1}).

Second derivative test. We differentiate the gradient: d2ydx2=ddx[(x−x3)e−x2]=(1−3x2)e−x2+(x−x3)(−2x)e−x2\frac{d^2 y}{dx^2} = \frac{d}{dx}\bigl[(x - x^3)e^{-x^2}\bigr] = (1 - 3x^2)e^{-x^2} + (x - x^3)(-2x)e^{-x^2} =e−x2[(1−3x2)−2x2(1−x2)]=e−x2(1−5x2+2x4).= e^{-x^2}\bigl[(1 - 3x^2) - 2x^2(1 - x^2)\bigr] = e^{-x^2}(1 - 5x^2 + 2x^4).

At x=0x = 0: d2ydx2=1>0\dfrac{d^2y}{dx^2} = 1 > 0, so (0,0)(0, 0) is a minimum point.

At x=1x = 1: d2ydx2=e−1(1−5+2)=−2e−1<0\dfrac{d^2y}{dx^2} = e^{-1}(1 - 5 + 2) = -2e^{-1} < 0, so (1,12e−1)(1, \tfrac{1}{2}e^{-1}) is a maximum point.

The other stationary point is (−1,  12e−1)\mathbf{(-1,\;\tfrac{1}{2}e^{-1})}.

Sketch of C1C_1. The curve passes through the origin (minimum), rises to a maximum at (1,12e−1)(1, \tfrac{1}{2}e^{-1}), and by symmetry about the yy-axis (since y=12x2e−x2y = \tfrac{1}{2}x^2 e^{-x^2} is an even function) also has a maximum at (−1,12e−1)(-1, \tfrac{1}{2}e^{-1}). As x→±∞x \to \pm\infty, y→0+y \to 0^+. The curve has a characteristic bell-shaped hump centred on the yy-axis.


Curve C2C_2.

C2C_2 passes through the origin with dydx=x(1−x2)e−x3\dfrac{dy}{dx} = x(1 - x^2)e^{-x^3}.

Stationary points. Setting dydx=0\dfrac{dy}{dx} = 0: since e−x3≠0e^{-x^3} \neq 0, we again need x(1−x2)=0x(1 - x^2) = 0, giving x=0,±1x = 0, \pm 1.

Second derivative. Differentiating the gradient: d2ydx2=ddx[(x−x3)e−x3]=(1−3x2)e−x3+(x−x3)(−3x2)e−x3\frac{d^2y}{dx^2} = \frac{d}{dx}\bigl[(x - x^3)e^{-x^3}\bigr] = (1 - 3x^2)e^{-x^3} + (x - x^3)(-3x^2)e^{-x^3} =e−x3[(1−3x2)−3x2(1−x2)(x)]=e−x3(1−3x2−3x3+3x5).= e^{-x^3}\bigl[(1 - 3x^2) - 3x^2(1 - x^2)(x)\bigr] = e^{-x^3}(1 - 3x^2 - 3x^3 + 3x^5).

At x=0x = 0: d2ydx2=1>0\dfrac{d^2y}{dx^2} = 1 > 0, so (0,0)(0, 0) is a minimum point.

At x=1x = 1: d2ydx2=e−1(1−3−3+3)=−2e−1<0\dfrac{d^2y}{dx^2} = e^{-1}(1 - 3 - 3 + 3) = -2e^{-1} < 0, so (1,k)(1, k) is a maximum point.

Showing k>12e−1k > \frac{1}{2}e^{-1}. Since C2C_2 passes through the origin, the yy-value at the maximum is k=∫01x(1−x2)e−x3 dx.k = \int_0^1 x(1 - x^2)e^{-x^3}\,dx.

For C1C_1, the yy-value at its maximum is 12e−1=∫01x(1−x2)e−x2 dx\tfrac{1}{2}e^{-1} = \int_0^1 x(1 - x^2)e^{-x^2}\,dx which we can verify: ∫01(x−x3)e−x2 dx=[12x2e−x2]01=12e−1\int_0^1 (x - x^3)e^{-x^2}\,dx = \bigl[\tfrac{1}{2}x^2 e^{-x^2}\bigr]_0^1 = \tfrac{1}{2}e^{-1}.

For 0<x<10 < x < 1: x3<x2x^3 < x^2, so −x3>−x2-x^3 > -x^2, giving e−x3>e−x2e^{-x^3} > e^{-x^2}. Also x(1−x2)>0x(1 - x^2) > 0 for 0<x<10 < x < 1.

Therefore x(1−x2)e−x3>x(1−x2)e−x2x(1 - x^2)e^{-x^3} > x(1 - x^2)e^{-x^2} for all x∈(0,1)x \in (0, 1), and since the integrands are continuous and agree at the endpoints, we conclude k=∫01x(1−x2)e−x3 dx>∫01x(1−x2)e−x2 dx=12e−1.k = \int_0^1 x(1 - x^2)e^{-x^3}\,dx > \int_0^1 x(1 - x^2)e^{-x^2}\,dx = \tfrac{1}{2}e^{-1}.


Topic: 积分 Integration  |  Difficulty: Challenging  |  Marks: 20

6 Show that ∫01x41+x2 dx=π4−23.\int_0^1 \frac{x^4}{1 + x^2} \text{ d}x = \frac{\pi}{4} - \frac{2}{3} . Determine the values of (i) ∫01x3tan⁡−1(1−x1+x) dx\int_0^1 x^3 \tan^{-1} \left( \frac{1 - x}{1 + x} \right) \text{ d}x , (ii) ∫01(1−y)3(1+y)5tan⁡−1y dy\int_0^1 \frac{(1 - y)^3}{(1 + y)^5} \tan^{-1} y \text{ d}y .

Model Solution

Preliminary result.

Perform polynomial long division: x41+x2=x2−1+11+x2\frac{x^4}{1 + x^2} = x^2 - 1 + \frac{1}{1 + x^2} since x4=(x2−1)(x2+1)+1x^4 = (x^2 - 1)(x^2 + 1) + 1.

Therefore ∫01x41+x2 dx=∫01(x2−1) dx+∫0111+x2 dx=[x33−x]01+[tan⁡−1x]01\int_0^1 \frac{x^4}{1 + x^2}\,dx = \int_0^1 (x^2 - 1)\,dx + \int_0^1 \frac{1}{1 + x^2}\,dx = \left[\frac{x^3}{3} - x\right]_0^1 + \left[\tan^{-1}x\right]_0^1 =(13−1)+π4=π4−23.✓= \left(\frac{1}{3} - 1\right) + \frac{\pi}{4} = \frac{\pi}{4} - \frac{2}{3}. \qquad \checkmark


Part (i).

We use integration by parts. First we compute the derivative of tan⁡−1 ⁣(1−x1+x)\tan^{-1}\!\left(\dfrac{1-x}{1+x}\right).

Set u=1−x1+xu = \dfrac{1-x}{1+x}, so dudx=−(1+x)−(1−x)(1+x)2=−2(1+x)2\dfrac{du}{dx} = \dfrac{-(1+x) - (1-x)}{(1+x)^2} = \dfrac{-2}{(1+x)^2}.

1+u2=1+(1−x)2(1+x)2=(1+x)2+(1−x)2(1+x)2=2+2x2(1+x)2=2(1+x2)(1+x)2.1 + u^2 = 1 + \frac{(1-x)^2}{(1+x)^2} = \frac{(1+x)^2 + (1-x)^2}{(1+x)^2} = \frac{2 + 2x^2}{(1+x)^2} = \frac{2(1+x^2)}{(1+x)^2}.

By the chain rule: ddxtan⁡−1 ⁣(1−x1+x)=11+u2⋅dudx=(1+x)22(1+x2)⋅−2(1+x)2=−11+x2.\frac{d}{dx}\tan^{-1}\!\left(\frac{1-x}{1+x}\right) = \frac{1}{1 + u^2}\cdot\frac{du}{dx} = \frac{(1+x)^2}{2(1+x^2)}\cdot\frac{-2}{(1+x)^2} = \frac{-1}{1+x^2}.

Now integrate by parts with U=tan⁡−1 ⁣(1−x1+x)U = \tan^{-1}\!\left(\dfrac{1-x}{1+x}\right) and dV=x3 dxdV = x^3\,dx: dU=−11+x2 dx,V=x44.dU = \frac{-1}{1+x^2}\,dx, \qquad V = \frac{x^4}{4}.

∫01x3tan⁡−1 ⁣(1−x1+x)dx=[x44tan⁡−1 ⁣(1−x1+x)]01−∫01x44⋅−11+x2 dx\int_0^1 x^3 \tan^{-1}\!\left(\frac{1-x}{1+x}\right)dx = \left[\frac{x^4}{4}\tan^{-1}\!\left(\frac{1-x}{1+x}\right)\right]_0^1 - \int_0^1 \frac{x^4}{4}\cdot\frac{-1}{1+x^2}\,dx =[x44tan⁡−1 ⁣(1−x1+x)]01+14∫01x41+x2 dx.= \left[\frac{x^4}{4}\tan^{-1}\!\left(\frac{1-x}{1+x}\right)\right]_0^1 + \frac{1}{4}\int_0^1 \frac{x^4}{1+x^2}\,dx.

Evaluating the boundary term:

  • At x=1x = 1: 14tan⁡−1(0)=0\dfrac{1}{4}\tan^{-1}(0) = 0.
  • At x=0x = 0: 0⋅tan⁡−1(1)=00 \cdot \tan^{-1}(1) = 0.

So the boundary term vanishes, and ∫01x3tan⁡−1 ⁣(1−x1+x)dx=14∫01x41+x2 dx=14(π4−23)=3π−848.\int_0^1 x^3 \tan^{-1}\!\left(\frac{1-x}{1+x}\right)dx = \frac{1}{4}\int_0^1 \frac{x^4}{1+x^2}\,dx = \frac{1}{4}\left(\frac{\pi}{4} - \frac{2}{3}\right) = \frac{3\pi - 8}{48}.


Part (ii).

Use the substitution y=1−t1+ty = \dfrac{1-t}{1+t}, so t=1−y1+yt = \dfrac{1-y}{1+y}.

When y=0y = 0: t=1t = 1. When y=1y = 1: t=0t = 0.

dydt=−(1+t)−(1−t)(1+t)2=−2(1+t)2.\frac{dy}{dt} = \frac{-(1+t) - (1-t)}{(1+t)^2} = \frac{-2}{(1+t)^2}.

We compute the key building blocks: 1+y=1+1−t1+t=(1+t)+(1−t)1+t=21+t,1 + y = 1 + \frac{1-t}{1+t} = \frac{(1+t) + (1-t)}{1+t} = \frac{2}{1+t}, 1−y=1−1−t1+t=(1+t)−(1−t)1+t=2t1+t.1 - y = 1 - \frac{1-t}{1+t} = \frac{(1+t) - (1-t)}{1+t} = \frac{2t}{1+t}.

Therefore (1−y)3(1+y)5=[2t/(1+t)]3[2/(1+t)]5=8t3/(1+t)332/(1+t)5=t3(1+t)24.\frac{(1-y)^3}{(1+y)^5} = \frac{[2t/(1+t)]^3}{[2/(1+t)]^5} = \frac{8t^3/(1+t)^3}{32/(1+t)^5} = \frac{t^3(1+t)^2}{4}.

Also tan⁡−1y=tan⁡−1 ⁣(1−t1+t)\tan^{-1}y = \tan^{-1}\!\left(\dfrac{1-t}{1+t}\right).

Substituting into the integral (and reversing limits to absorb the negative sign from dy/dtdy/dt): ∫01(1−y)3(1+y)5tan⁡−1y dy=∫10t3(1+t)24tan⁡−1 ⁣(1−t1+t)⋅−2(1+t)2 dt\int_0^1 \frac{(1-y)^3}{(1+y)^5}\tan^{-1}y\,dy = \int_1^0 \frac{t^3(1+t)^2}{4}\tan^{-1}\!\left(\frac{1-t}{1+t}\right)\cdot\frac{-2}{(1+t)^2}\,dt =12∫01t3tan⁡−1 ⁣(1−t1+t)dt.= \frac{1}{2}\int_0^1 t^3\tan^{-1}\!\left(\frac{1-t}{1+t}\right)dt.

This is exactly 12\dfrac{1}{2} times the integral evaluated in part (i). Therefore

∫01(1−y)3(1+y)5tan⁡−1y dy=12⋅3π−848=3π−896.\int_0^1 \frac{(1-y)^3}{(1+y)^5}\tan^{-1}y\,dy = \frac{1}{2}\cdot\frac{3\pi - 8}{48} = \frac{3\pi - 8}{96}.


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

7 In an Argand diagram, OO is the origin and PP is the point 2+0i2 + 0i. The points QQ, RR and SS are such that the lengths OPOP, PQPQ, QRQR and RSRS are all equal, and the angles OPQOPQ, PQRPQR and QRSQRS are all equal to 5π/65\pi/6, so that the points OO, PP, QQ, RR and SS are five vertices of a regular 12-sided polygon lying in the upper half of the Argand diagram. Show that QQ is the point 2+3+i2 + \sqrt{3} + i and find SS.

The point CC is the centre of the circle that passes through the points OO, PP and QQ. Show that, if the polygon is rotated anticlockwise about OO until CC first lies on the real axis, the new position of SS is −12(32+6)(3−i).-\frac{1}{2}(3\sqrt{2} + \sqrt{6})(\sqrt{3} - i) .

Model Solution

Setting up the geometry.

The five points O,P,Q,R,SO, P, Q, R, S are consecutive vertices of a regular 12-gon in the upper half-plane. The interior angle of a regular 12-gon is 5π/65\pi/6 (since each exterior angle is π/6\pi/6). Each side has length ∣OP∣=2|OP| = 2.

Finding QQ.

Starting from P=2P = 2, the vector PQ⃗\vec{PQ} has length 2 and makes an angle of π−5π/6=π/6\pi - 5\pi/6 = \pi/6 with the positive real axis (the interior angle OPQ=5π/6OPQ = 5\pi/6 means PQPQ turns by π/6\pi/6 from the direction POPO).

So PQ⃗=2(cos⁡(π/6)+isin⁡(π/6))=2(32+i2)=3+i\vec{PQ} = 2(\cos(\pi/6) + i\sin(\pi/6)) = 2\left(\frac{\sqrt{3}}{2} + \frac{i}{2}\right) = \sqrt{3} + i.

Q=P+PQ⃗=2+3+i■Q = P + \vec{PQ} = 2 + \sqrt{3} + i \qquad \blacksquare

Finding SS.

Each step rotates by −π/6-\pi/6 (turning left by the exterior angle π/6\pi/6) in the complex plane. We can express each successive vertex by multiplying by eiπ/6e^{i\pi/6} (rotating by π/6\pi/6) and scaling.

Alternatively, in the regular 12-gon centred at some point, each vertex is obtained from the previous by rotation through 2π/12=π/62\pi/12 = \pi/6. Let us use the multiplicative structure directly.

The vector from OO to PP is 22. The vector from PP to QQ is 3+i=2eiπ/6\sqrt{3} + i = 2e^{i\pi/6}. Each successive side is obtained by rotating the previous side by eiπ/6e^{i\pi/6}:

  • OP⃗=2\vec{OP} = 2
  • PQ⃗=2eiπ/6\vec{PQ} = 2e^{i\pi/6}
  • QR⃗=2eiπ/3\vec{QR} = 2e^{i\pi/3}
  • RS⃗=2eiπ/2=2i\vec{RS} = 2e^{i\pi/2} = 2i

So: Q=2+2eiπ/6=2+3+iQ = 2 + 2e^{i\pi/6} = 2 + \sqrt{3} + i R=Q+2eiπ/3=(2+3+i)+(1+i3)=3+3+i(1+3)R = Q + 2e^{i\pi/3} = (2 + \sqrt{3} + i) + (1 + i\sqrt{3}) = 3 + \sqrt{3} + i(1 + \sqrt{3}) S=R+2i=3+3+i(3+3)S = R + 2i = 3 + \sqrt{3} + i(3 + \sqrt{3})

Therefore:

S=(3+3)(1+i)S = (3 + \sqrt{3})(1 + i)


Finding the centre CC of the circle through OO, PP, QQ.

The circumcircle of triangle OPQOPQ has centre CC equidistant from OO, PP, and QQ.

Let C=a+biC = a + bi. Then:

From ∣CO∣=∣CP∣|CO| = |CP|:

a2+b2=(a−2)2+b2  ⟹  a2=a2−4a+4  ⟹  4a=4  ⟹  a=1a^2 + b^2 = (a - 2)^2 + b^2 \implies a^2 = a^2 - 4a + 4 \implies 4a = 4 \implies a = 1

From ∣CO∣=∣CQ∣|CO| = |CQ| with Q=2+3+iQ = 2 + \sqrt{3} + i:

1+b2=(1−2−3)2+(b−1)21 + b^2 = (1 - 2 - \sqrt{3})^2 + (b - 1)^2 1+b2=(1+3)2+b2−2b+11 + b^2 = (1 + \sqrt{3})^2 + b^2 - 2b + 1 1=1+23+3−2b+11 = 1 + 2\sqrt{3} + 3 - 2b + 1 1=5+23−2b1 = 5 + 2\sqrt{3} - 2b 2b=4+232b = 4 + 2\sqrt{3} b=2+3b = 2 + \sqrt{3}

So C=1+(2+3)iC = 1 + (2 + \sqrt{3})i.

Rotating until CC lies on the real axis.

When we rotate anticlockwise about OO by angle ϕ\phi, the new position of CC is CeiϕCe^{i\phi}. We need Im(Ceiϕ)=0\text{Im}(Ce^{i\phi}) = 0 and ϕ>0\phi > 0 minimal.

Write C=1+(2+3)iC = 1 + (2 + \sqrt{3})i. In polar form:

∣C∣=1+(2+3)2=1+4+43+3=8+43|C| = \sqrt{1 + (2 + \sqrt{3})^2} = \sqrt{1 + 4 + 4\sqrt{3} + 3} = \sqrt{8 + 4\sqrt{3}}

The argument of CC is θC=tan⁡−1(2+3)\theta_C = \tan^{-1}(2 + \sqrt{3}).

We note that tan⁡(5π/12)=tan⁡75∘=2+3\tan(5\pi/12) = \tan 75^\circ = 2 + \sqrt{3}, so θC=5π/12\theta_C = 5\pi/12.

To bring CC onto the real axis, we rotate by ϕ=−θC\phi = -\theta_C (clockwise, which is negative anticlockwise) to land on the positive real axis, or by ϕ=π−θC\phi = \pi - \theta_C to land on the negative real axis. The question asks for the first time CC lands on the real axis as we rotate anticlockwise (positive ϕ\phi), so:

  • ϕ=2π−5π/12=19π/12\phi = 2\pi - 5\pi/12 = 19\pi/12 lands on the positive real axis (large rotation).
  • ϕ=π−5π/12=7π/12\phi = \pi - 5\pi/12 = 7\pi/12 lands on the negative real axis (smaller rotation).

The first (smallest positive) rotation is ϕ=7π/12\phi = 7\pi/12.

New position of SS.

The rotated position of SS is:

S′=S⋅ei⋅7π/12S' = S \cdot e^{i \cdot 7\pi/12}

We have S=(3+3)(1+i)S = (3 + \sqrt{3})(1 + i).

Write 1+i=2 eiπ/41 + i = \sqrt{2}\,e^{i\pi/4}, so:

S′=(3+3)2 ei(π/4+7π/12)=(3+3)2 ei⋅10π/12=(3+3)2 ei⋅5π/6S' = (3 + \sqrt{3})\sqrt{2}\,e^{i(\pi/4 + 7\pi/12)} = (3 + \sqrt{3})\sqrt{2}\,e^{i \cdot 10\pi/12} = (3 + \sqrt{3})\sqrt{2}\,e^{i \cdot 5\pi/6}

Now ei⋅5π/6=cos⁡(5π/6)+isin⁡(5π/6)=−32+i2=12(−3+i)e^{i \cdot 5\pi/6} = \cos(5\pi/6) + i\sin(5\pi/6) = -\frac{\sqrt{3}}{2} + \frac{i}{2} = \frac{1}{2}(-\sqrt{3} + i).

So:

S′=(3+3)2⋅12(−3+i)=(3+3)22(−3+i)S' = (3 + \sqrt{3})\sqrt{2} \cdot \frac{1}{2}(-\sqrt{3} + i) = \frac{(3 + \sqrt{3})\sqrt{2}}{2}(-\sqrt{3} + i)

We simplify (3+3)2(3 + \sqrt{3})\sqrt{2}:

(3+3)2=32+6(3 + \sqrt{3})\sqrt{2} = 3\sqrt{2} + \sqrt{6}

Therefore:

S′=32+62(−3+i)=−12(32+6)(3−i)■S' = \frac{3\sqrt{2} + \sqrt{6}}{2}(-\sqrt{3} + i) = -\frac{1}{2}(3\sqrt{2} + \sqrt{6})(\sqrt{3} - i) \qquad \blacksquare


Topic: 微分方程 Differential Equations  |  Difficulty: Challenging  |  Marks: 20

8 The function ff satisfies f(x+1)=f(x)f(x + 1) = f(x) and f(x)>0f(x) > 0 for all xx.

(i) Give an example of such a function.

(ii) The function FF satisfies dFdx=f(x)\frac{\mathrm{d}F}{\mathrm{d}x} = f(x) and F(0)=0F(0) = 0. Show that F(n)=nF(1)F(n) = nF(1), for any positive integer nn.

(iii) Let yy be the solution of the differential equation dydx+f(x)y=0\frac{\mathrm{d}y}{\mathrm{d}x} + f(x)y = 0 that satisfies y=1y = 1 when x=0x = 0. Show that y(n)→0y(n) \to 0 as n→∞n \to \infty, where n=1,2,3,…n = 1, 2, 3, \dots

Model Solution

Part (i): Example

f(x)=2+sin⁡2πxf(x) = 2 + \sin 2\pi x satisfies f(x+1)=2+sin⁡2π(x+1)=2+sin⁡(2πx+2π)=2+sin⁡2πx=f(x)f(x+1) = 2 + \sin 2\pi(x+1) = 2 + \sin(2\pi x + 2\pi) = 2 + \sin 2\pi x = f(x), and f(x)≥2−1=1>0f(x) \geq 2 - 1 = 1 > 0 for all xx. ■\qquad \blacksquare

(Any positive periodic function with period 1 works, e.g. f(x)=2+cos⁡2πxf(x) = 2 + \cos 2\pi x.)


Part (ii): Showing F(n)=nF(1)F(n) = nF(1)

Since F′(x)=f(x)F'(x) = f(x) and F(0)=0F(0) = 0:

F(n)=∫0nf(x) dxF(n) = \int_0^n f(x)\,dx

Split the integral into unit intervals:

F(n)=∫01f(x) dx+∫12f(x) dx+⋯+∫n−1nf(x) dx=∑k=0n−1∫kk+1f(x) dxF(n) = \int_0^1 f(x)\,dx + \int_1^2 f(x)\,dx + \cdots + \int_{n-1}^n f(x)\,dx = \sum_{k=0}^{n-1} \int_k^{k+1} f(x)\,dx

In each integral ∫kk+1f(x) dx\int_k^{k+1} f(x)\,dx, substitute x=t+kx = t + k:

∫kk+1f(x) dx=∫01f(t+k) dt=∫01f(t) dt=F(1)−F(0)=F(1)\int_k^{k+1} f(x)\,dx = \int_0^1 f(t + k)\,dt = \int_0^1 f(t)\,dt = F(1) - F(0) = F(1)

where we used f(t+k)=f(t)f(t + k) = f(t) (since ff has period 1 and kk is an integer).

Therefore:

F(n)=∑k=0n−1F(1)=nF(1)■F(n) = \sum_{k=0}^{n-1} F(1) = nF(1) \qquad \blacksquare


Part (iii): Showing y(n)→0y(n) \to 0 as n→∞n \to \infty

The differential equation is:

dydx+f(x)y=0  ⟹  dydx=−f(x)y\frac{dy}{dx} + f(x)y = 0 \implies \frac{dy}{dx} = -f(x)y

This is separable:

dyy=−f(x) dx\frac{dy}{y} = -f(x)\,dx

Integrating from 00 to xx:

ln⁡∣y(x)∣−ln⁡∣y(0)∣=−∫0xf(t) dt=−F(x)\ln|y(x)| - \ln|y(0)| = -\int_0^x f(t)\,dt = -F(x)

Since y(0)=1y(0) = 1:

ln⁡y(x)=−F(x)  ⟹  y(x)=e−F(x)\ln y(x) = -F(x) \implies y(x) = e^{-F(x)}

(We can drop the absolute value since y(0)=1>0y(0) = 1 > 0 and yy is continuous, so y>0y > 0 everywhere.)

At x=nx = n:

y(n)=e−F(n)=e−nF(1)y(n) = e^{-F(n)} = e^{-nF(1)}

From part (ii). Since f(x)>0f(x) > 0 for all xx, we have F(1)=∫01f(x) dx>0F(1) = \int_0^1 f(x)\,dx > 0.

Therefore nF(1)→∞nF(1) \to \infty as n→∞n \to \infty, and:

y(n)=e−nF(1)→0as n→∞■y(n) = e^{-nF(1)} \to 0 \quad \text{as } n \to \infty \qquad \blacksquare