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STEP3 1999 -- Pure Mathematics

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STEP3 1999 — Section A (Pure Mathematics)

Section titled “STEP3 1999 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 1999  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1代数 AlgebraStandard韦达定理,多项式根与系数关系,等比数列性质
2分析 AnalysisChallenging求导判断单调性,函数图像分析,分段讨论参数范围
3微积分 CalculusStandard黎曼和转化为定积分,极限与积分的联系
4几何 GeometryStandard欧拉公式V-E+F=2,面与顶点的计数关系,整数约束分析
5数列与递推 Sequences and RecurrenceChallenging数学归纳法,递推关系代换,代数恒等式变形
6参数方程与曲线面积 (Parametric Curves and Area)Challenging三角参数化,格林面积公式,贝塔函数积分
7抽象代数/群论 (Abstract Algebra/Group Theory)Challenging结合律直接验证,单位元与逆元求解,子群构造
8常微分方程 (Ordinary Differential Equations)Challenging二阶常系数ODE,分段拼接,连续性匹配,无穷级数求和

Topic: 代数 Algebra  |  Difficulty: Standard  |  Marks: 20

1 Consider the cubic equation x3px2+qxr=0,x^3 - px^2 + qx - r = 0 , where p0p \neq 0 and r0r \neq 0.

(i) If the three roots can be written in the form ak1ak^{-1}, aa and akak for some constants aa and kk, show that one root is q/pq/p and that q3rp3=0q^3 - rp^3 = 0.

(ii) If r=q3/p3r = q^3/p^3, show that q/pq/p is a root and that the product of the other two roots is (q/p)2(q/p)^2. Deduce that the roots are in geometric progression.

(iii) Find a necessary and sufficient condition involving pp, qq and rr for the roots to be in arithmetic progression.

Model Solution

Part (i) Show that one root is q/pq/p and that q3rp3=0q^3 - rp^3 = 0.

Let the three roots be ak1ak^{-1}, aa, and akak. By Vieta’s formulas for x3px2+qxr=0x^3 - px^2 + qx - r = 0:

p=ak1+a+ak=a(k1+1+k),(...1)p = ak^{-1} + a + ak = a(k^{-1} + 1 + k), \qquad \text{(...1)}

q=(ak1)(a)+(ak1)(ak)+(a)(ak)=a2(k1+1+k),(...2)q = (ak^{-1})(a) + (ak^{-1})(ak) + (a)(ak) = a^2(k^{-1} + 1 + k), \qquad \text{(...2)}

r=(ak1)(a)(ak)=a3.(...3)r = (ak^{-1})(a)(ak) = a^3. \qquad \text{(...3)}

From (1) and (2), dividing qq by pp:

qp=a2(k1+1+k)a(k1+1+k)=a.\frac{q}{p} = \frac{a^2(k^{-1} + 1 + k)}{a(k^{-1} + 1 + k)} = a.

So a=q/pa = q/p is one of the three roots, as required.

From (3), r=a3=(q/p)3r = a^3 = (q/p)^3, hence rp3=q3rp^3 = q^3, i.e.

q3rp3=0.q^3 - rp^3 = 0. \qquad \blacksquare

Part (ii) Show that q/pq/p is a root and the product of the other two roots is (q/p)2(q/p)^2; deduce the roots are in GP.

Suppose r=q3/p3r = q^3/p^3. We check that x=q/px = q/p is a root:

(qp)3p(qp)2+q(qp)r=q3p3q2p+q2pq3p3=0.\left(\frac{q}{p}\right)^3 - p\left(\frac{q}{p}\right)^2 + q\left(\frac{q}{p}\right) - r = \frac{q^3}{p^3} - \frac{q^2}{p} + \frac{q^2}{p} - \frac{q^3}{p^3} = 0. \checkmark

So q/pq/p is a root. Let the other two roots be α\alpha and β\beta. By Vieta’s formulas:

qp+α+β=p,qpαβ=r=q3p3.\frac{q}{p} + \alpha + \beta = p, \qquad \frac{q}{p} \cdot \alpha\beta = r = \frac{q^3}{p^3}.

From the second relation:

αβ=q3p3pq=q2p2=(qp)2.\alpha\beta = \frac{q^3}{p^3} \cdot \frac{p}{q} = \frac{q^2}{p^2} = \left(\frac{q}{p}\right)^2.

Now α+β=pq/p\alpha + \beta = p - q/p and αβ=(q/p)2\alpha\beta = (q/p)^2. The roots α,β\alpha, \beta satisfy

x2(pqp)x+(qp)2=0.x^2 - \left(p - \frac{q}{p}\right)x + \left(\frac{q}{p}\right)^2 = 0.

The three roots are q/pq/p, α\alpha, β\beta with αβ=(q/p)2\alpha\beta = (q/p)^2. Since the product of all three roots is r=(q/p)3r = (q/p)^3 and one root is q/pq/p, the remaining product is (q/p)2(q/p)^2, meaning

αβ=(qp)2.\alpha \cdot \beta = \left(\frac{q}{p}\right)^2.

If β=(q/p)2α\beta = \frac{(q/p)^2}{\alpha}, then the three roots q/pq/p, α\alpha, (q/p)2α\frac{(q/p)^2}{\alpha} are in geometric progression with common ratio αq/p=pαq\frac{\alpha}{q/p} = \frac{p\alpha}{q}. Indeed, (q/p)2α=q/pα/(q/p)\frac{(q/p)^2}{\alpha} = \frac{q/p}{\alpha/(q/p)} confirms the GP structure. \blacksquare

Part (iii) Necessary and sufficient condition for roots in arithmetic progression.

Let the three roots be ada - d, aa, a+da + d (common difference dd). By Vieta’s:

p=(ad)+a+(a+d)=3a,so a=p3.p = (a-d) + a + (a+d) = 3a, \qquad \text{so } a = \frac{p}{3}.

q=(ad)a+(ad)(a+d)+a(a+d)=a2ad+a2d2+a2+ad=3a2d2.q = (a-d)a + (a-d)(a+d) + a(a+d) = a^2 - ad + a^2 - d^2 + a^2 + ad = 3a^2 - d^2.

r=(ad)a(a+d)=a(a2d2).r = (a-d) \cdot a \cdot (a+d) = a(a^2 - d^2).

From q=3a2d2q = 3a^2 - d^2 we get d2=3a2qd^2 = 3a^2 - q. Substituting into rr:

r=a(3a2d2(3a2d2)+d2)wait, let me redo this cleanly.r = a(3a^2 - d^2 - (3a^2 - d^2) + d^2) \quad \text{wait, let me redo this cleanly.}

r=a(a2d2)=aq2a3+a3no.r = a(a^2 - d^2) = a \cdot q - 2a^3 + a^3 \quad \text{no.}

We have d2=3a2qd^2 = 3a^2 - q and r=a(a2d2)=a(a23a2+q)=a(q2a2)r = a(a^2 - d^2) = a(a^2 - 3a^2 + q) = a(q - 2a^2).

With a=p/3a = p/3:

r=p3(q2p29)=pq32p327.r = \frac{p}{3}\left(q - \frac{2p^2}{9}\right) = \frac{pq}{3} - \frac{2p^3}{27}.

Multiplying through by 27:

27r=9pq2p3.27r = 9pq - 2p^3.

Rearranging:

2p39pq+27r=0.2p^3 - 9pq + 27r = 0.

This is the necessary and sufficient condition for the roots to be in arithmetic progression.

Verification of sufficiency: If 2p39pq+27r=02p^3 - 9pq + 27r = 0, then r=9pq2p327=p3(q2p29)r = \frac{9pq - 2p^3}{27} = \frac{p}{3}(q - \frac{2p^2}{9}), and setting a=p/3a = p/3, d2=3a2q=p23qd^2 = 3a^2 - q = \frac{p^2}{3} - q, the cubic factors as (xa+d)(xa)(xa+d)(x - a + d)(x - a)(x - a + d), giving three real roots in AP (when d20d^2 \geq 0, i.e. qp2/3q \leq p^2/3, the roots are distinct or repeated).

2p39pq+27r=02p^3 - 9pq + 27r = 0 \qquad \blacksquare


Topic: 分析 Analysis  |  Difficulty: Challenging  |  Marks: 20

2 (i) Let f(x)=(1+x2)exf(x) = (1 + x^2)e^x. Show that f(x)0f'(x) \geqslant 0 and sketch the graph of f(x)f(x). Hence, or otherwise, show that the equation (1+x2)ex=k,(1 + x^2)e^x = k, where kk is a constant, has exactly one real root if k>0k > 0 and no real roots if k0k \leqslant 0.

(ii) Determine the number of real roots of the equation (ex1)ktan1x=0(e^x - 1) - k \tan^{-1} x = 0 in the cases (a) 0<k2/π0 < k \leqslant 2/\pi and (b) 2/π<k<12/\pi < k < 1.

Model Solution

Part (i) Show f(x)0f'(x) \geq 0, sketch ff, and determine roots of (1+x2)ex=k(1+x^2)e^x = k.

Let f(x)=(1+x2)exf(x) = (1 + x^2)e^x. Differentiating:

f(x)=2xex+(1+x2)ex=ex(1+2x+x2)=ex(1+x)2.f'(x) = 2xe^x + (1 + x^2)e^x = e^x(1 + 2x + x^2) = e^x(1 + x)^2.

Since ex>0e^x > 0 for all xx and (1+x)20(1+x)^2 \geq 0 for all xx, we have f(x)0f'(x) \geq 0 for all xx, with equality only at x=1x = -1.

Therefore ff is non-decreasing (strictly increasing except at x=1x = -1 where it has a stationary inflection point).

Key features of the graph:

  • f(0)=1f(0) = 1, f(1)=2e1=2/ef(-1) = 2e^{-1} = 2/e.
  • As x+x \to +\infty: f(x)+f(x) \to +\infty (exponential growth dominates).
  • As xx \to -\infty: f(x)0+f(x) \to 0^+ (since ex0e^x \to 0 and 1+x21 + x^2 grows polynomially, but exe^x decays faster).

Since ff is non-decreasing with limxf(x)=0\lim_{x\to-\infty} f(x) = 0 and limx+f(x)=+\lim_{x\to+\infty} f(x) = +\infty, the range of ff is (0,+)(0, +\infty).

For k>0k > 0: the horizontal line y=ky = k crosses the graph of ff exactly once (since ff is non-decreasing and its range is (0,+)(0, +\infty)), so the equation has exactly one real root.

For k0k \leq 0: since f(x)=(1+x2)ex>0f(x) = (1+x^2)e^x > 0 for all xx (as 1+x2>01+x^2 > 0 and ex>0e^x > 0), the equation has no real roots.

Part (ii) Determine the number of real roots of (ex1)karctanx=0(e^x - 1) - k\arctan x = 0.

Let g(x)=ex1karctanxg(x) = e^x - 1 - k\arctan x. Note g(0)=0g(0) = 0, so x=0x = 0 is always a root. We need to determine if there are other roots.

g(x)=exk1+x2.g'(x) = e^x - \frac{k}{1 + x^2}.

Case (a): 0<k2/π0 < k \leq 2/\pi.

We claim g(x)<0g(x) < 0 for x<0x < 0 and g(x)>0g(x) > 0 for x>0x > 0, so x=0x = 0 is the only root.

For x>0x > 0: We show ex1>karctanxe^x - 1 > k\arctan x. Since ex>1+xe^x > 1 + x for x>0x > 0 (standard inequality from the Taylor series), and arctanx<x\arctan x < x for x>0x > 0:

ex1>x>kx(we need a tighter bound).e^x - 1 > x > k \cdot \frac{x}{\text{(we need a tighter bound)}}.

Better approach: consider h(x)=ex1arctanxh(x) = \frac{e^x - 1}{\arctan x} for x>0x > 0. We need h(x)>kh(x) > k. As x0+x \to 0^+, by L’Hopital:

limx0+h(x)=limx0+ex1/(1+x2)=1.\lim_{x \to 0^+} h(x) = \lim_{x \to 0^+} \frac{e^x}{1/(1+x^2)} = 1.

As x+x \to +\infty: h(x)exπ/2+h(x) \approx \frac{e^x}{\pi/2} \to +\infty.

We compute h(x)h'(x) to check monotonicity. Actually, let us instead check g(x)>0g'(x) > 0 for all x>0x > 0, which would mean gg is strictly increasing on (0,)(0, \infty) and hence g(x)>g(0)=0g(x) > g(0) = 0 for x>0x > 0.

g(x)=exk1+x2.g'(x) = e^x - \frac{k}{1+x^2}.

For x>0x > 0: ex>1e^x > 1 and k1+x2<k2π<1\frac{k}{1+x^2} < k \leq \frac{2}{\pi} < 1. So g(x)>0g'(x) > 0 for all x>0x > 0.

Hence gg is strictly increasing on (0,)(0, \infty), giving g(x)>0g(x) > 0 for x>0x > 0.

For x<0x < 0: We need g(x)<0g(x) < 0, i.e. ex1<karctanxe^x - 1 < k\arctan x. Note both sides are negative for x<0x < 0. Rearranging: 1ex>karctanx1 - e^x > k|\arctan x| (both sides positive).

Consider g(x)=exk1+x2g'(x) = e^x - \frac{k}{1+x^2} for x<0x < 0. We have ex<1e^x < 1 and k1+x2k1+x2\frac{k}{1+x^2} \geq \frac{k}{1+x^2}. At x1x \leq -1: exe10.37e^x \leq e^{-1} \approx 0.37 and k1+x2k1+x2\frac{k}{1+x^2} \geq \frac{k}{1+x^2}; we need more care.

Let us check g(x)g'(x) for x<0x < 0. We have g(0)=1k>0g'(0) = 1 - k > 0 (since k2/π<1k \leq 2/\pi < 1). Also g(x)00=0g'(x) \to 0 - 0 = 0 as xx \to -\infty (wait, ex0e^x \to 0 and k1+x20\frac{k}{1+x^2} \to 0, so g(x)0g'(x) \to 0).

Actually, let’s verify g(x)<0g'(x) < 0 is impossible for x<0x < 0 when k2/πk \leq 2/\pi. We need ex<k1+x2e^x < \frac{k}{1+x^2}, i.e. (1+x2)ex<k2/π(1+x^2)e^x < k \leq 2/\pi.

From Part (i), f(x)=(1+x2)exf(x) = (1+x^2)e^x is non-decreasing with minimum value approaching 0. So for xx very negative, f(x)<2/πf(x) < 2/\pi, meaning g(x)<0g'(x) < 0 is possible there. But this just means gg decreases before it increases.

The key insight: g(x)1k(π/2)=1+kπ/2g(x) \to -1 - k(-\pi/2) = -1 + k\pi/2 as xx \to -\infty. For k2/πk \leq 2/\pi: 1+kπ/21+1=0-1 + k\pi/2 \leq -1 + 1 = 0. So g(x)0g(x) \leq 0 as xx \to -\infty, with equality only when k=2/πk = 2/\pi.

For k<2/πk < 2/\pi: g(x)1+kπ/2<0g(x) \to -1 + k\pi/2 < 0 as xx \to -\infty. Since g(0)=0g(0) = 0 and gg is continuous, if gg had a root at some x0<0x_0 < 0 with g(x0)=0g(x_0) = 0, then between -\infty and x0x_0 or between x0x_0 and 00, gg would need to cross zero. Since g(x)<0g'(x) < 0 for very negative xx (where (1+x2)ex(1+x^2)e^x is small), gg is decreasing there. Then gg' changes sign at most once (since (1+x2)ex(1+x^2)e^x is non-decreasing), so gg has at most one local minimum. If gg goes from negative values, reaches a minimum, then increases to g(0)=0g(0) = 0, it stays negative for all x<0x < 0.

For k=2/πk = 2/\pi: g(x)0g(x) \to 0 as xx \to -\infty. Since gg is negative for large negative xx (it approaches 0 from below, because exe^x approaches 0 faster than karctanxk\arctan x approaches kπ/2-k\pi/2, making ex11e^x - 1 \approx -1 while karctanx1k\arctan x \approx -1, but ex1<1+kπ/2=0e^x - 1 < -1 + k\pi/2 = 0 for any finite xx), the same argument gives no additional roots.

Conclusion for case (a): The only real root is x=0x = 0.

Case (b): 2/π<k<12/\pi < k < 1.

Now g(x)1+kπ/2>0g(x) \to -1 + k\pi/2 > 0 as xx \to -\infty. Since g(0)=0g(0) = 0 and gg is continuous, gg must cross zero at least once for x<0x < 0 (since it starts positive and reaches 0).

More precisely: g()=kπ/21>0g(-\infty) = k\pi/2 - 1 > 0 and g(0)=0g(0) = 0. If gg stayed positive on (,0)(-\infty, 0), it would need g(0)0g'(0) \leq 0, but g(0)=1k>0g'(0) = 1 - k > 0. So gg must go below zero somewhere in (,0)(-\infty, 0), meaning it crosses zero at least twice on (,0)(-\infty, 0) (once going down, once coming back up to g(0)=0g(0) = 0).

To count precisely, consider g(x)=exk1+x2g'(x) = e^x - \frac{k}{1+x^2}. Let ϕ(x)=(1+x2)ex\phi(x) = (1+x^2)e^x. Then g(x)=0g'(x) = 0 iff ϕ(x)=k\phi(x) = k. From Part (i), ϕ(x)=k>0\phi(x) = k > 0 has exactly one real root x0x_0. Since k<1=ϕ(0)k < 1 = \phi(0), we have x0<0x_0 < 0.

So g(x)<0g'(x) < 0 for x<x0x < x_0 and g(x)>0g'(x) > 0 for x>x0x > x_0. This means gg decreases on (,x0)(-\infty, x_0) and increases on (x0,)(x_0, \infty), with a unique minimum at x0x_0.

Since g()=kπ/21>0g(-\infty) = k\pi/2 - 1 > 0, gg decreases from positive values to g(x0)g(x_0), then increases to g(0)=0g(0) = 0 and beyond (since g(0)>0g'(0) > 0, gg is increasing at 0, so g(x)>0g(x) > 0 for x>0x > 0).

If g(x0)<0g(x_0) < 0: gg crosses zero once on (,x0)(-\infty, x_0) and once on (x0,0)(x_0, 0), giving 2 negative roots plus x=0x = 0, total 3 roots.

If g(x0)=0g(x_0) = 0: gg touches zero at x0x_0 and at 0, total 2 roots.

If g(x0)>0g(x_0) > 0: gg never crosses zero on (,0)(-\infty, 0) except at x=0x = 0 where it reaches 0 from above. But g(0)=1k>0g'(0) = 1 - k > 0 means gg is increasing at 0, so g(x)<0g(x) < 0 just to the left of 0. This contradicts g(x0)>0g(x_0) > 0 and gg being increasing on (x0,0)(x_0, 0).

Wait, let me reconsider. gg is increasing on (x0,0)(x_0, 0) with g(0)=0g(0) = 0. If g(x0)>0g(x_0) > 0, then gg would decrease from g()>0g(-\infty) > 0 to g(x0)>0g(x_0) > 0 (never crossing zero), then increase from g(x0)>0g(x_0) > 0 to g(0)=0g(0) = 0… but gg increasing on (x0,0)(x_0, 0) with g(0)=0g(0) = 0 requires g(x0)<0g(x_0) < 0. Contradiction.

So g(x0)<0g(x_0) < 0 is forced. Therefore gg crosses zero exactly once on (,x0)(-\infty, x_0) and exactly once on (x0,0)(x_0, 0) (since gg is monotone on each interval).

Conclusion for case (b): There are exactly 3 real roots: one negative (left of x0x_0), one negative (between x0x_0 and 00), and x=0x = 0.

Hmm, wait. Let me recount. gg starts at kπ/21>0k\pi/2 - 1 > 0 as xx \to -\infty, decreases to g(x0)<0g(x_0) < 0, then increases to g(0)=0g(0) = 0. So gg crosses zero exactly once on (,x0)(-\infty, x_0) (from positive to negative). On (x0,0)(x_0, 0), gg increases from negative to 0, so g(x)<0g(x) < 0 on (x0,0)(x_0, 0) and g(0)=0g(0) = 0. So the only crossing is one root in (,x0)(-\infty, x_0), plus x=0x = 0.

For x>0x > 0: g(x)>0g'(x) > 0 and g(0)=0g(0) = 0, so g(x)>0g(x) > 0 for x>0x > 0, no additional roots.

Conclusion for case (b): There are exactly 2 real roots: one negative root and x=0x = 0.


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

3 Justify, by means of a sketch, the formula limn{1nm=1nf(1+m/n)}=12f(x)dx.\lim_{n \to \infty} \left\{ \frac{1}{n} \sum_{m=1}^{n} f(1 + m/n) \right\} = \int_{1}^{2} f(x) \, dx . Show that limn{1n+1+1n+2++1n+n}=ln2.\lim_{n \to \infty} \left\{ \frac{1}{n + 1} + \frac{1}{n + 2} + \dots + \frac{1}{n + n} \right\} = \ln 2 . Evaluate limn{nn2+1+nn2+4++nn2+n2}.\lim_{n \to \infty} \left\{ \frac{n}{n^2 + 1} + \frac{n}{n^2 + 4} + \dots + \frac{n}{n^2 + n^2} \right\} .

Model Solution

Part (i): Justifying the Riemann sum formula

Consider the integral 12f(x)dx\int_1^2 f(x) \, dx. We partition the interval [1,2][1, 2] into nn equal sub-intervals, each of width Δx=21n=1n\Delta x = \frac{2 - 1}{n} = \frac{1}{n}.

The partition points are x0=1,  x1=1+1n,  x2=1+2n,  ,  xn=2x_0 = 1, \; x_1 = 1 + \tfrac{1}{n}, \; x_2 = 1 + \tfrac{2}{n}, \; \ldots, \; x_n = 2.

The right-hand Riemann sum uses the value of ff at the right endpoint of each sub-interval:

m=1nf(xm)Δx=m=1nf ⁣(1+mn)1n=1nm=1nf ⁣(1+mn).\sum_{m=1}^{n} f(x_m) \, \Delta x = \sum_{m=1}^{n} f\!\left(1 + \tfrac{m}{n}\right) \cdot \frac{1}{n} = \frac{1}{n} \sum_{m=1}^{n} f\!\left(1 + \tfrac{m}{n}\right).

Sketch: For a continuous function ff on [1,2][1, 2], the Riemann sum represents the total area of nn rectangles of width 1n\frac{1}{n}, where the mm-th rectangle has height f(1+m/n)f(1 + m/n). As nn \to \infty, these rectangles fill the region under the curve y=f(x)y = f(x) from x=1x = 1 to x=2x = 2 more and more precisely, so the sum converges to the definite integral. Hence

limn{1nm=1nf ⁣(1+mn)}=12f(x)dx.\lim_{n \to \infty} \left\{ \frac{1}{n} \sum_{m=1}^{n} f\!\left(1 + \tfrac{m}{n}\right) \right\} = \int_1^2 f(x) \, dx.

Part (ii): Showing the limit equals ln2\ln 2

We rewrite the sum by dividing numerator and denominator of each term by nn:

1n+1+1n+2++1n+n=m=1n1n+m=m=1n1n ⁣(1+m/n)=1nm=1n11+m/n.\frac{1}{n+1} + \frac{1}{n+2} + \cdots + \frac{1}{n+n} = \sum_{m=1}^{n} \frac{1}{n+m} = \sum_{m=1}^{n} \frac{1}{n\!\left(1 + m/n\right)} = \frac{1}{n} \sum_{m=1}^{n} \frac{1}{1 + m/n}.

This is exactly the Riemann sum from Part (i) with f(x)=1xf(x) = \frac{1}{x}. Therefore

limn{1n+1+1n+2++12n}=121xdx=[lnx]12=ln2ln1=ln2.\lim_{n \to \infty} \left\{ \frac{1}{n+1} + \frac{1}{n+2} + \cdots + \frac{1}{2n} \right\} = \int_1^2 \frac{1}{x} \, dx = \Big[\ln x\Big]_1^2 = \ln 2 - \ln 1 = \ln 2.

Part (iii): Evaluating the second limit

We rewrite each term by dividing numerator and denominator by n2n^2:

nn2+m2=nn2 ⁣(1+m2/n2)=1n11+(m/n)2.\frac{n}{n^2 + m^2} = \frac{n}{n^2\!\left(1 + m^2/n^2\right)} = \frac{1}{n} \cdot \frac{1}{1 + (m/n)^2}.

So the full sum becomes

m=1nnn2+m2=1nm=1n11+(m/n)2.\sum_{m=1}^{n} \frac{n}{n^2 + m^2} = \frac{1}{n} \sum_{m=1}^{n} \frac{1}{1 + (m/n)^2}.

This is the Riemann sum from Part (i) with f(x)=11+x2f(x) = \frac{1}{1 + x^2}. Therefore

limn{nn2+1+nn2+4++nn2+n2}=1211+x2dx=[arctanx]12=arctan2arctan1.\lim_{n \to \infty} \left\{ \frac{n}{n^2+1} + \frac{n}{n^2+4} + \cdots + \frac{n}{n^2+n^2} \right\} = \int_1^2 \frac{1}{1+x^2} \, dx = \Big[\arctan x\Big]_1^2 = \arctan 2 - \arctan 1.

Since arctan1=π4\arctan 1 = \frac{\pi}{4}, the limit is

arctan2π4.\arctan 2 - \frac{\pi}{4}.


Topic: 几何 Geometry  |  Difficulty: Standard  |  Marks: 20

4 A polyhedron is a solid bounded by FF plane faces, which meet in EE edges and VV vertices. You may assume Euler’s formula, that VE+F=2V - E + F = 2.

In a regular polyhedron the faces are equal regular mm-sided polygons, nn of which meet at each vertex. Show that F=4nh,F = \frac{4n}{h}, where h=4(n2)(m2)h = 4 - (n - 2)(m - 2).

By considering the possible values of hh, or otherwise, prove that there are only five regular polyhedra, and find VV, EE and FF for each.

Model Solution

Part (i): Deriving the formula F=4nhF = \frac{4n}{h}

Each face is a regular mm-gon, so each face has mm edges. Since every edge is shared by exactly two faces, counting edge-face incidences gives

2E=mF,soE=mF2....(1)2E = mF, \qquad \text{so} \qquad E = \frac{mF}{2}. \qquad \text{...(1)}

At each vertex exactly nn faces meet, and each face has mm vertices. Counting vertex-face incidences gives

nV=mF,soV=mFn....(2)nV = mF, \qquad \text{so} \qquad V = \frac{mF}{n}. \qquad \text{...(2)}

Substituting (1) and (2) into Euler’s formula VE+F=2V - E + F = 2:

mFnmF2+F=2.\frac{mF}{n} - \frac{mF}{2} + F = 2.

Factor out FF:

F ⁣(mnm2+1)=2.F\!\left(\frac{m}{n} - \frac{m}{2} + 1\right) = 2.

Multiply through by 2n2n:

F(2mmn+2n)=4n.F(2m - mn + 2n) = 4n.

Now expand h=4(n2)(m2)h = 4 - (n-2)(m-2):

h=4(nm2n2m+4)=4nm+2n+2m4=2m+2nmn.h = 4 - (nm - 2n - 2m + 4) = 4 - nm + 2n + 2m - 4 = 2m + 2n - mn.

So 2mmn+2n=h2m - mn + 2n = h, and therefore

Fh=4n,i.e.F=4nh.Fh = 4n, \qquad \text{i.e.} \qquad F = \frac{4n}{h}. \qquad \blacksquare

Part (ii): Proving there are exactly five regular polyhedra

Since F4F \geqslant 4 (a polyhedron has at least 4 faces), we need F=4nh>0F = \frac{4n}{h} > 0. With n3n \geqslant 3 (at least 3 faces meet at each vertex) and m3m \geqslant 3 (each face is at least a triangle), we need h>0h > 0, i.e.

4(n2)(m2)>0(n2)(m2)<4.4 - (n-2)(m-2) > 0 \qquad \Longrightarrow \qquad (n-2)(m-2) < 4.

Since n3n \geqslant 3 and m3m \geqslant 3, we have n21n - 2 \geqslant 1 and m21m - 2 \geqslant 1. The product of two positive integers being less than 4 gives only these cases:

mmnn(n2)(m2)(n-2)(m-2)hhF=4nhF = \frac{4n}{h}E=mF2E = \frac{mF}{2}V=mFnV = \frac{mF}{n}Polyhedron
3313464Tetrahedron
34228126Octahedron
3531203012Icosahedron
43226128Cube
5331123020Dodecahedron

For m6m \geqslant 6, we have m24m - 2 \geqslant 4, so (n2)(m2)4(n-2)(m-2) \geqslant 4 for any n3n \geqslant 3, which violates h>0h > 0. Similarly for n6n \geqslant 6.

Therefore only five pairs (m,n)(m, n) are possible, corresponding to exactly five regular polyhedra. \blacksquare

Summary of the five regular polyhedra:

PolyhedronmmnnFFEEVV
Tetrahedron33464
Cube436128
Octahedron348126
Dodecahedron53123020
Icosahedron35203012

Topic: 数列与递推 Sequences and Recurrence  |  Difficulty: Challenging  |  Marks: 20

5 The sequence u0,u1,u2,u_0, u_1, u_2, \dots is defined by u0=1,u1=1,un+1=un+un1for n1.u_0 = 1, \quad u_1 = 1, \quad u_{n+1} = u_n + u_{n-1} \quad \text{for } n \geqslant 1.

Prove that un+22+un12=2(un+12+un2).u_{n+2}^2 + u_{n-1}^2 = 2(u_{n+1}^2 + u_n^2).

Using induction, or otherwise, prove the following result: u2n=un2+un12andu2n+1=un+12un12u_{2n} = u_n^2 + u_{n-1}^2 \quad \text{and} \quad u_{2n+1} = u_{n+1}^2 - u_{n-1}^2 for any positive integer nn.

Model Solution

Part (i): Prove that un+22+un12=2(un+12+un2)u_{n+2}^2 + u_{n-1}^2 = 2(u_{n+1}^2 + u_n^2)

We start by expanding un+22u_{n+2}^2 using the recurrence un+2=un+1+unu_{n+2} = u_{n+1} + u_n:

un+22=(un+1+un)2=un+12+2un+1un+un2.u_{n+2}^2 = (u_{n+1} + u_n)^2 = u_{n+1}^2 + 2u_{n+1}u_n + u_n^2.

Therefore

un+22+un12=un+12+2un+1un+un2+un12.(...)u_{n+2}^2 + u_{n-1}^2 = u_{n+1}^2 + 2u_{n+1}u_n + u_n^2 + u_{n-1}^2. \qquad \text{(...)}

From the recurrence un+1=un+un1u_{n+1} = u_n + u_{n-1}, we have un1=un+1unu_{n-1} = u_{n+1} - u_n. Substituting into un12u_{n-1}^2:

un12=(un+1un)2=un+122un+1un+un2.u_{n-1}^2 = (u_{n+1} - u_n)^2 = u_{n+1}^2 - 2u_{n+1}u_n + u_n^2.

Substituting this back into (...)(...):

un+22+un12=un+12+2un+1un+un2+un+122un+1un+un2=2un+12+2un2=2(un+12+un2).u_{n+2}^2 + u_{n-1}^2 = u_{n+1}^2 + 2u_{n+1}u_n + u_n^2 + u_{n+1}^2 - 2u_{n+1}u_n + u_n^2 = 2u_{n+1}^2 + 2u_n^2 = 2(u_{n+1}^2 + u_n^2).

This completes the proof. \blacksquare

Part (ii): Prove by induction that u2n=un2+un12u_{2n} = u_n^2 + u_{n-1}^2 and u2n+1=un+12un12u_{2n+1} = u_{n+1}^2 - u_{n-1}^2 for all positive integers nn

Base case (n=1)(n = 1): We have u0=1u_0 = 1, u1=1u_1 = 1, u2=u1+u0=2u_2 = u_1 + u_0 = 2, u3=u2+u1=3u_3 = u_2 + u_1 = 3.

First identity: u2=2=1+1=u12+u02u_2 = 2 = 1 + 1 = u_1^2 + u_0^2. Confirmed.

Second identity: u3=3=41=u22u02u_3 = 3 = 4 - 1 = u_2^2 - u_0^2. Confirmed.

Inductive step: Suppose both identities hold for some positive integer nn, i.e.

u2n=un2+un12,u2n+1=un+12un12.(**)u_{2n} = u_n^2 + u_{n-1}^2, \qquad u_{2n+1} = u_{n+1}^2 - u_{n-1}^2. \qquad \text{(**)}

We prove both identities for n+1n + 1.

First identity for n+1n + 1: We need u2(n+1)=un+12+un2u_{2(n+1)} = u_{n+1}^2 + u_n^2.

u2n+2=u2n+1+u2n=(un+12un12)+(un2+un12)=un+12+un2.u_{2n+2} = u_{2n+1} + u_{2n} = (u_{n+1}^2 - u_{n-1}^2) + (u_n^2 + u_{n-1}^2) = u_{n+1}^2 + u_n^2.

This confirms the first identity for n+1n + 1.

Second identity for n+1n + 1: We need u2n+3=un+22un2u_{2n+3} = u_{n+2}^2 - u_n^2.

u2n+3=u2n+2+u2n+1=(un+12+un2)+(un+12un12)=2un+12+un2un12.u_{2n+3} = u_{2n+2} + u_{2n+1} = (u_{n+1}^2 + u_n^2) + (u_{n+1}^2 - u_{n-1}^2) = 2u_{n+1}^2 + u_n^2 - u_{n-1}^2.

Using un1=un+1unu_{n-1} = u_{n+1} - u_n:

un12=un+122un+1un+un2.u_{n-1}^2 = u_{n+1}^2 - 2u_{n+1}u_n + u_n^2.

Substituting:

u2n+3=2un+12+un2un+12+2un+1unun2=un+12+2un+1un=un+1(un+1+2un).u_{2n+3} = 2u_{n+1}^2 + u_n^2 - u_{n+1}^2 + 2u_{n+1}u_n - u_n^2 = u_{n+1}^2 + 2u_{n+1}u_n = u_{n+1}(u_{n+1} + 2u_n).

Now, un+2un=(un+1+un)un=un+1u_{n+2} - u_n = (u_{n+1} + u_n) - u_n = u_{n+1}, so by the difference of squares:

un+22un2=(un+2un)(un+2+un)=un+1(un+2+un).u_{n+2}^2 - u_n^2 = (u_{n+2} - u_n)(u_{n+2} + u_n) = u_{n+1}(u_{n+2} + u_n).

It remains to show un+1+2un=un+2+unu_{n+1} + 2u_n = u_{n+2} + u_n. Since un+2=un+1+unu_{n+2} = u_{n+1} + u_n:

un+2+un=un+1+un+un=un+1+2un.u_{n+2} + u_n = u_{n+1} + u_n + u_n = u_{n+1} + 2u_n. \checkmark

Therefore u2n+3=un+1(un+2+un)=un+22un2u_{2n+3} = u_{n+1}(u_{n+2} + u_n) = u_{n+2}^2 - u_n^2, confirming the second identity for n+1n + 1.

By induction, both identities hold for all positive integers nn. \blacksquare


Topic: 参数方程与曲线面积 (Parametric Curves and Area)  |  Difficulty: Challenging  |  Marks: 20

6 A closed curve is given by the equation x2/n+y2/n=a2/n(*)x^{2/n} + y^{2/n} = a^{2/n} \qquad \text{(*)} where nn is an odd integer and aa is a positive constant. Find a parametrization x=x(t)x = x(t), y=y(t)y = y(t) which describes the curve anticlockwise as tt ranges from 00 to 2π2\pi.

Sketch the curve in the case n=3n = 3, justifying the main features of your sketch.

The area AA enclosed by such a curve is given by the formula A=1202π[x(t)dy(t)dty(t)dx(t)dt]dt.A = \frac{1}{2} \int_0^{2\pi} \left[ x(t) \frac{dy(t)}{dt} - y(t) \frac{dx(t)}{dt} \right] \, dt.

Use this result to find the area enclosed by (*) for n=3n = 3.

Model Solution

Part (i): Parametrization

The curve is x2/n+y2/n=a2/nx^{2/n} + y^{2/n} = a^{2/n} where nn is odd. We seek a parametrization that traces the curve anticlockwise for t[0,2π]t \in [0, 2\pi].

Set

x=acosnt,y=asinnt.x = a\cos^n t, \qquad y = a\sin^n t.

Since nn is odd, the nn-th root of a negative number is well-defined and real, so xx and yy take all real values as required. We verify:

x2/n+y2/n=(acosnt)2/n+(asinnt)2/n=a2/ncos2t+a2/nsin2t=a2/n(cos2t+sin2t)=a2/n.x^{2/n} + y^{2/n} = (a\cos^n t)^{2/n} + (a\sin^n t)^{2/n} = a^{2/n}\cos^2 t + a^{2/n}\sin^2 t = a^{2/n}(\cos^2 t + \sin^2 t) = a^{2/n}. \checkmark

As tt increases from 00 to 2π2\pi, the point (x,y)(x,y) traces anticlockwise: at t=0t = 0 we have (a,0)(a, 0); at t=π/2t = \pi/2 we have (0,a)(0, a); at t=πt = \pi we have (a,0)(-a, 0); at t=3π/2t = 3\pi/2 we have (0,a)(0, -a).

Part (ii): Sketch for n=3n = 3

The curve x2/3+y2/3=a2/3x^{2/3} + y^{2/3} = a^{2/3} is called an astroid (or tetracuspid hypocycloid). Its key features are:

  • Intercepts: (±a,0)(\pm a, 0) and (0,±a)(0, \pm a).
  • Symmetry: symmetric about both axes (replacing xxx \to -x or yyy \to -y leaves the equation unchanged).
  • Cusps: at each intercept, the curve has a cusp (pointed corner). To see why, note that dydx\frac{dy}{dx} at, say, (a,0)(a, 0) corresponds to t=0t = 0, where dy/dtdx/dt=3asin2tcost3acos2tsint=sintcostt=0=0\frac{dy/dt}{dx/dt} = \frac{3a\sin^2 t\cos t}{-3a\cos^2 t\sin t} = \frac{-\sin t}{\cos t}\big|_{t=0} = 0 from the yy-side, but the tangent direction is degenerate at the cusp.
  • Shape: the curve bulges inward between the axes, forming a concave shape somewhat like a rounded square. This is because when, say, t=π/4t = \pi/4, we have x=y=a(22)3=a22x = y = a(\frac{\sqrt{2}}{2})^3 = \frac{a}{2\sqrt{2}}, which lies well inside the square with vertices (±a,±a)(\pm a, \pm a).

Part (iii): Area for n=3n = 3

With x=acos3tx = a\cos^3 t and y=asin3ty = a\sin^3 t:

dxdt=3acos2tsint,dydt=3asin2tcost.\frac{dx}{dt} = -3a\cos^2 t \sin t, \qquad \frac{dy}{dt} = 3a\sin^2 t \cos t.

Compute the integrand xdydtydxdtx\frac{dy}{dt} - y\frac{dx}{dt}:

xdydt=acos3t3asin2tcost=3a2sin2tcos4t,x\frac{dy}{dt} = a\cos^3 t \cdot 3a\sin^2 t\cos t = 3a^2\sin^2 t\cos^4 t,

ydxdt=asin3t(3acos2tsint)=3a2sin4tcos2t.y\frac{dx}{dt} = a\sin^3 t \cdot (-3a\cos^2 t\sin t) = -3a^2\sin^4 t\cos^2 t.

Therefore

xdydtydxdt=3a2sin2tcos4t+3a2sin4tcos2t=3a2sin2tcos2t(cos2t+sin2t)=3a2sin2tcos2t.x\frac{dy}{dt} - y\frac{dx}{dt} = 3a^2\sin^2 t\cos^4 t + 3a^2\sin^4 t\cos^2 t = 3a^2\sin^2 t\cos^2 t(\cos^2 t + \sin^2 t) = 3a^2\sin^2 t\cos^2 t.

Using the double angle identity sintcost=12sin2t\sin t\cos t = \frac{1}{2}\sin 2t:

sin2tcos2t=14sin22t.\sin^2 t\cos^2 t = \frac{1}{4}\sin^2 2t.

So the area is

A=1202π3a214sin22tdt=3a2802πsin22tdt.A = \frac{1}{2}\int_0^{2\pi} 3a^2 \cdot \frac{1}{4}\sin^2 2t \, dt = \frac{3a^2}{8}\int_0^{2\pi}\sin^2 2t \, dt.

Using sin22t=1cos4t2\sin^2 2t = \frac{1 - \cos 4t}{2}:

02πsin22tdt=02π1cos4t2dt=12[tsin4t4]02π=12(2π00+0)=π.\int_0^{2\pi}\sin^2 2t \, dt = \int_0^{2\pi}\frac{1 - \cos 4t}{2} \, dt = \frac{1}{2}\left[t - \frac{\sin 4t}{4}\right]_0^{2\pi} = \frac{1}{2}(2\pi - 0 - 0 + 0) = \pi.

Therefore

A=3a28π=3πa28.A = \frac{3a^2}{8} \cdot \pi = \frac{3\pi a^2}{8}.


Topic: 抽象代数/群论 (Abstract Algebra/Group Theory)  |  Difficulty: Challenging  |  Marks: 20

7 Let aa be a non-zero real number and define a binary operation on the set of real numbers by

xy=x+y+axy.x * y = x + y + axy .

Show that the operation * is associative.

Show that (G,)(G, *) is a group, where GG is the set of all real numbers except for one number which you should identify.

Find a subgroup of (G,)(G, *) which has exactly 2 elements.

Model Solution

Associativity

We compute (xy)z(x * y) * z and x(yz)x * (y * z) and show they are equal.

(xy)z=(x+y+axy)z=(x+y+axy)+z+a(x+y+axy)z(x * y) * z = (x + y + axy) * z = (x + y + axy) + z + a(x + y + axy)z

=x+y+axy+z+axz+ayz+a2xyz= x + y + axy + z + axz + ayz + a^2xyz

=x+y+z+axy+axz+ayz+a2xyz(... 1)= x + y + z + axy + axz + ayz + a^2xyz \qquad \text{(... 1)}

x(yz)=x(y+z+ayz)=x+(y+z+ayz)+ax(y+z+ayz)x * (y * z) = x * (y + z + ayz) = x + (y + z + ayz) + ax(y + z + ayz)

=x+y+z+ayz+axy+axz+a2xyz= x + y + z + ayz + axy + axz + a^2xyz

=x+y+z+axy+axz+ayz+a2xyz(... 2)= x + y + z + axy + axz + ayz + a^2xyz \qquad \text{(... 2)}

Since (1) and (2) are identical, (xy)z=x(yz)(x * y) * z = x * (y * z) for all real x,y,zx, y, z. The operation * is associative.

Identifying GG and showing it is a group

Identity element. We need ee such that xe=xx * e = x for all xGx \in G:

x+e+axe=x    e(1+ax)=0.x + e + axe = x \implies e(1 + ax) = 0.

For this to hold for all xGx \in G, we need e=0e = 0. Check: x0=x+0+0=xx * 0 = x + 0 + 0 = x and 0x=0+x+0=x0 * x = 0 + x + 0 = x. So the identity is 00.

Inverse element. Given xGx \in G, we need xGx' \in G with xx=0x * x' = 0:

x+x+axx=0    x(1+ax)=x    x=x1+ax.x + x' + axx' = 0 \implies x'(1 + ax) = -x \implies x' = \frac{-x}{1 + ax}.

This expression is defined provided 1+ax01 + ax \neq 0, i.e. x1ax \neq -\frac{1}{a}. Therefore the element that must be excluded from GG is 1a\boxed{-\dfrac{1}{a}}, giving

G=R{1a}.G = \mathbb{R} \setminus \left\{ -\frac{1}{a} \right\}.

We verify that xGx' \in G: if x=1ax' = -\frac{1}{a}, then x1+ax=1a\frac{-x}{1+ax} = -\frac{1}{a}, giving ax=1+axax = 1 + ax, hence 0=10 = 1, a contradiction. So xGx' \in G whenever xGx \in G.

Closure. We must check that xyGx * y \in G whenever x,yGx, y \in G. Suppose for contradiction that xy=1ax * y = -\frac{1}{a}:

x+y+axy=1a    a(x+y+axy)=1    ax+ay+a2xy+1=0.x + y + axy = -\frac{1}{a} \implies a(x + y + axy) = -1 \implies ax + ay + a^2xy + 1 = 0.

Factorising: (1+ax)(1+ay)=0(1 + ax)(1 + ay) = 0, so x=1ax = -\frac{1}{a} or y=1ay = -\frac{1}{a}. This contradicts x,yGx, y \in G. Hence xyGx * y \in G.

Summary. The set G=R{1/a}G = \mathbb{R} \setminus \{-1/a\} with the operation * satisfies all four group axioms: closure, associativity (proved above), identity (e=0e = 0), and inverses (x1=x1+ax)\left(x^{-1} = -\frac{x}{1+ax}\right). Therefore (G,)(G, *) is a group.

A subgroup with exactly 2 elements

A subgroup of order 2 has the form {0,g}\{0, g\} where g0g \neq 0 and gg=0g * g = 0 (the identity). We solve:

g+g+ag2=0    g(2+ag)=0.g + g + ag^2 = 0 \implies g(2 + ag) = 0.

Since g0g \neq 0: 2+ag=02 + ag = 0, giving g=2ag = -\frac{2}{a}.

Check: g=2a1ag = -\frac{2}{a} \neq -\frac{1}{a} (since a0a \neq 0), so gGg \in G.

Verify closure: gg=2a+(2a)+a4a2=4a+4a=0Gg * g = -\frac{2}{a} + \left(-\frac{2}{a}\right) + a \cdot \frac{4}{a^2} = -\frac{4}{a} + \frac{4}{a} = 0 \in G.

The subgroup is {0,2a}\left\{ 0, \, -\dfrac{2}{a} \right\}.


Topic: 常微分方程 (Ordinary Differential Equations)  |  Difficulty: Challenging  |  Marks: 20

8 The function y(x)y(x) is defined for x0x \geqslant 0 and satisfies the conditions

y=0anddydx=1at x=0.y = 0 \quad \text{and} \quad \frac{dy}{dx} = 1 \quad \text{at } x = 0.

When xx is in the range 2(n1)π<x<2nπ2(n - 1)\pi < x < 2n\pi, where nn is a positive integer, y(t)y(t) satisfies the differential equation

d2ydx2+n2y=0.\frac{d^2y}{dx^2} + n^2y = 0.

Both yy and dydx\frac{dy}{dx} are continuous at x=2nπx = 2n\pi for n=0,1,2,n = 0, 1, 2, \dots.

(i) Find y(x)y(x) for 0x2π0 \leqslant x \leqslant 2\pi.

(ii) Show that y(x)=12sin2xy(x) = \frac{1}{2} \sin 2x for 2πx4π2\pi \leqslant x \leqslant 4\pi, and find y(x)y(x) for all x0x \geqslant 0.

(iii) Show that

0y2dx=πn=11n2.\int_{0}^{\infty} y^2 dx = \pi \sum_{n=1}^{\infty} \frac{1}{n^2} .

Model Solution

Part (i) Find y(x)y(x) for 0x2π0 \leqslant x \leqslant 2\pi.

On the interval 0<x<2π0 < x < 2\pi (corresponding to n=1n = 1), the ODE is

d2ydx2+y=0.\frac{d^2y}{dx^2} + y = 0.

The general solution is y=Acosx+Bsinxy = A\cos x + B\sin x.

Applying the initial conditions at x=0x = 0:

y(0)=0    A=0.y(0) = 0 \implies A = 0.

y(0)=1    B=1.y'(0) = 1 \implies B = 1.

Therefore y(x)=sinxy(x) = \sin x for 0x2π0 \leqslant x \leqslant 2\pi.

We note the boundary values at x=2πx = 2\pi that will be needed for continuity matching:

y(2π)=sin2π=0,y(2π)=cos2π=1.y(2\pi) = \sin 2\pi = 0, \qquad y'(2\pi) = \cos 2\pi = 1.

Part (ii) Show that y(x)=12sin2xy(x) = \frac{1}{2}\sin 2x for 2πx4π2\pi \leqslant x \leqslant 4\pi, and find y(x)y(x) for all x0x \geqslant 0.

On the interval 2π<x<4π2\pi < x < 4\pi (corresponding to n=2n = 2), the ODE is

d2ydx2+4y=0.\frac{d^2y}{dx^2} + 4y = 0.

The general solution is y=Ccos2x+Dsin2xy = C\cos 2x + D\sin 2x.

Using continuity at x=2πx = 2\pi:

y(2π)=0    Ccos4π+Dsin4π=0    C=0.y(2\pi) = 0 \implies C\cos 4\pi + D\sin 4\pi = 0 \implies C = 0.

y(2π)=1    2Dcos4π=1    2D=1    D=12.y'(2\pi) = 1 \implies 2D\cos 4\pi = 1 \implies 2D = 1 \implies D = \frac{1}{2}.

Therefore y(x)=12sin2xy(x) = \frac{1}{2}\sin 2x for 2πx4π2\pi \leqslant x \leqslant 4\pi.

General formula. On the interval 2(n1)π<x<2nπ2(n-1)\pi < x < 2n\pi, the ODE is y+n2y=0y'' + n^2y = 0 with general solution

y=Ancos(nx)+Bnsin(nx).y = A_n\cos(nx) + B_n\sin(nx).

We claim y(x)=1nsin(nx)y(x) = \frac{1}{n}\sin(nx), i.e. An=0A_n = 0 and Bn=1nB_n = \frac{1}{n} for all n1n \geqslant 1, and prove this by induction.

Base case n=1n = 1: confirmed above, y=sinxy = \sin x.

Inductive step. Suppose y=1nsin(nx)y = \frac{1}{n}\sin(nx) on [2(n1)π,2nπ][2(n-1)\pi, 2n\pi]. At x=2nπx = 2n\pi:

y(2nπ)=1nsin(2n2π)=0,y(2n\pi) = \frac{1}{n}\sin(2n^2\pi) = 0,

y(2nπ)=cos(2n2π)=1.y'(2n\pi) = \cos(2n^2\pi) = 1.

On the next interval [2nπ,2(n+1)π][2n\pi, 2(n+1)\pi] with the ODE y+(n+1)2y=0y'' + (n+1)^2y = 0, the general solution is y=An+1cos((n+1)x)+Bn+1sin((n+1)x)y = A_{n+1}\cos((n+1)x) + B_{n+1}\sin((n+1)x).

y(2nπ)=0    An+1cos(2n(n+1)π)+Bn+1sin(2n(n+1)π)=0.y(2n\pi) = 0 \implies A_{n+1}\cos(2n(n+1)\pi) + B_{n+1}\sin(2n(n+1)\pi) = 0.

Since 2n(n+1)2n(n+1) is an even integer, cos(2n(n+1)π)=1\cos(2n(n+1)\pi) = 1 and sin(2n(n+1)π)=0\sin(2n(n+1)\pi) = 0, so An+1=0A_{n+1} = 0.

y(2nπ)=1    (n+1)Bn+1cos(2n(n+1)π)=1    (n+1)Bn+1=1    Bn+1=1n+1.y'(2n\pi) = 1 \implies (n+1)B_{n+1}\cos(2n(n+1)\pi) = 1 \implies (n+1)B_{n+1} = 1 \implies B_{n+1} = \frac{1}{n+1}.

This completes the induction. Therefore for all x0x \geqslant 0:

y(x)=1nsin(nx)for 2(n1)πx2nπ,n=1,2,3,y(x) = \frac{1}{n}\sin(nx) \qquad \text{for } 2(n-1)\pi \leqslant x \leqslant 2n\pi, \quad n = 1, 2, 3, \dots

Part (iii) Show that 0y2dx=πn=11n2\int_{0}^{\infty} y^2 \, dx = \pi \sum_{n=1}^{\infty} \frac{1}{n^2}.

We split the integral over the intervals [2(n1)π,2nπ][2(n-1)\pi, 2n\pi]:

0y2dx=n=12(n1)π2nπ1n2sin2(nx)dx.\int_{0}^{\infty} y^2 \, dx = \sum_{n=1}^{\infty} \int_{2(n-1)\pi}^{2n\pi} \frac{1}{n^2}\sin^2(nx) \, dx.

For each term, substitute u=nxu = nx (so dx=dundx = \frac{du}{n}):

2(n1)π2nπ1n2sin2(nx)dx=1n32n(n1)π2n2πsin2udu.\int_{2(n-1)\pi}^{2n\pi} \frac{1}{n^2}\sin^2(nx) \, dx = \frac{1}{n^3} \int_{2n(n-1)\pi}^{2n^2\pi} \sin^2 u \, du.

The interval of integration has length 2n2π2n(n1)π=2nπ2n^2\pi - 2n(n-1)\pi = 2n\pi. Since sin2u\sin^2 u has period π\pi, this interval contains exactly 2n2n complete periods. Over each period [kπ,(k+1)π][k\pi, (k+1)\pi]:

kπ(k+1)πsin2udu=π2.\int_{k\pi}^{(k+1)\pi} \sin^2 u \, du = \frac{\pi}{2}.

Therefore:

2n(n1)π2n2πsin2udu=2nπ2=nπ.\int_{2n(n-1)\pi}^{2n^2\pi} \sin^2 u \, du = 2n \cdot \frac{\pi}{2} = n\pi.

Substituting back:

2(n1)π2nπ1n2sin2(nx)dx=1n3nπ=πn2.\int_{2(n-1)\pi}^{2n\pi} \frac{1}{n^2}\sin^2(nx) \, dx = \frac{1}{n^3} \cdot n\pi = \frac{\pi}{n^2}.

Summing over all nn:

0y2dx=n=1πn2=πn=11n2.\int_{0}^{\infty} y^2 \, dx = \sum_{n=1}^{\infty} \frac{\pi}{n^2} = \pi \sum_{n=1}^{\infty} \frac{1}{n^2}. \qquad \blacksquare

(Using the Basel series n=11n2=π26\sum_{n=1}^{\infty} \frac{1}{n^2} = \frac{\pi^2}{6}, the integral evaluates to π36\frac{\pi^3}{6}.)