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STEP3 2022 -- Pure Mathematics

STEP3 2022 — Section A (Pure Mathematics)

Section titled “STEP3 2022 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2022  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1纯数Standard参数方程代入消元, 韦达定理, 对称多项式化简, 将四次方程倒数变换
2纯数Challenging无穷递降法, 反证法, 模3/模2同余分析, 奇偶性分析, 平方剩余
3纯数Challenging隐函数微分, 驻点条件推导, 四次方程根的分析, 联立方程消元
4纯数Challenging数学归纳法, 麦克劳林展开求极限, 虚数代换, 几何级数指数化简
5纯数Standard换元积分(u=-x), 奇偶函数分解, 微积分基本定理, 函数方程推理
6纯数Hard三角函数小量展开, 参数方程构建, 周期性条件处理, 导数的几何解释
7纯数Challenging向量叉积计算, 单位向量性质利用, Rodrigues旋转公式, 几何直觉与图示
8纯数ChallengingDe Moivre定理, 二项式展开, sec²θ-1=tan²θ代换, 奇偶性分析, 反证法

Topic: 纯数  |  Difficulty: Standard  |  Marks: 20

1 Let C1C_1 be the curve given by the parametric equations

x=ct,y=ctx = ct, \quad y = \frac{c}{t}

where c>0c > 0 and t0t \neq 0, and let C2C_2 be the circle

(xa)2+(yb)2=r2.(x - a)^2 + (y - b)^2 = r^2 .

C1C_1 and C2C_2 intersect at the four points PiP_i (i=1,2,3,4i = 1, 2, 3, 4), and the corresponding values of the parameter tt at these points are tit_i.

(i) Show that tit_i are the roots of the equation

c2t42act3+(a2+b2r2)t22bct+c2=0.()c^2t^4 - 2act^3 + (a^2 + b^2 - r^2)t^2 - 2bct + c^2 = 0 . \quad (*)

(ii) Show that

i=14ti2=2c2(a2b2+r2)\sum_{i=1}^4 t_i^2 = \frac{2}{c^2} (a^2 - b^2 + r^2)

(iii) Show that

the center of the circle C2C_2 lies on the line y=xy = x if and only if t1t2t3t4=1t_1t_2t_3t_4 = 1 and t1+t2+t3+t4=1t1+1t2+1t3+1t4t_1 + t_2 + t_3 + t_4 = \frac{1}{t_1} + \frac{1}{t_2} + \frac{1}{t_3} + \frac{1}{t_4}.

Hint

交点:(cta)2+(ctb)2=r2(ct-a)^2+(\frac{c}{t}-b)^2=r^2。 展开乘 t2t^2c2t42act3+(a2+b2r2)t22bct+c2=0c^2t^4-2act^3+(a^2+b^2-r^2)t^2-2bct+c^2=0

Vieta:ti=2ac\sum t_i=\frac{2a}{c}i<jtitj=a2+b2r2c2\sum_{i<j}t_it_j=\frac{a^2+b^2-r^2}{c^2}ti2=(2ac)22a2+b2r2c2=2c2(a2b2+r2)\sum t_i^2=(\frac{2a}{c})^2-2\cdot\frac{a^2+b^2-r^2}{c^2}=\frac{2}{c^2}(a^2-b^2+r^2)。 交换 aba\leftrightarrow b1ti2=2c2(b2a2+r2)\sum\frac{1}{t_i^2}=\frac{2}{c^2}(b^2-a^2+r^2)

OPi2=(c2ti2+c2ti2)=c2(2c2(a2b2+r2)+2c2(b2a2+r2))=4r2\sum OP_i^2=\sum(c^2t_i^2+\frac{c^2}{t_i^2})=c^2(\frac{2}{c^2}(a^2-b^2+r^2)+\frac{2}{c^2}(b^2-a^2+r^2))=4r^2

两切点     \implies 两对重根 t1=t3,t2=t4t_1=t_3,t_2=t_4t12t22=1    t1t2=±1t_1^2t_2^2=1 \implies t_1t_2=\pm 1。 Vieta:t1+t2=act_1+t_2=\frac{a}{c}t1t2(t1+t2)=bc    ba=±1    a=±bt_1t_2(t_1+t_2)=\frac{b}{c} \implies \frac{b}{a}=\pm 1 \implies a=\pm b。 圆心 (a,±a)(a,\pm a)y=±xy=\pm x 上。

Model Solution

Part (i)

At an intersection point of C1C_1 and C2C_2, the parametric coordinates satisfy the circle equation:

(cta)2+(ctb)2=r2(ct - a)^2 + \left(\frac{c}{t} - b\right)^2 = r^2

Expanding each squared term:

c2t22act+a2+c2t22bct+b2=r2c^2t^2 - 2act + a^2 + \frac{c^2}{t^2} - \frac{2bc}{t} + b^2 = r^2

Multiplying both sides by t2t^2 (valid since t0t \neq 0):

c2t42act3+a2t2+c22bct+b2t2=r2t2c^2t^4 - 2act^3 + a^2t^2 + c^2 - 2bct + b^2t^2 = r^2t^2

Collecting terms by powers of tt:

c2t42act3+(a2+b2r2)t22bct+c2=0()c^2t^4 - 2act^3 + (a^2 + b^2 - r^2)t^2 - 2bct + c^2 = 0 \qquad (*)

Since the four intersection points PiP_i correspond to parameter values tit_i, each tit_i satisfies this equation, so the tit_i are roots of ()(*).

Part (ii)

By Vieta’s formulas applied to the quartic ()(*) with leading coefficient c2c^2:

i=14ti=2ac,1i<j4titj=a2+b2r2c2\sum_{i=1}^4 t_i = \frac{2a}{c}, \qquad \sum_{1 \leqslant i < j \leqslant 4} t_it_j = \frac{a^2 + b^2 - r^2}{c^2}

Using the identity ti2=(ti)22i<jtitj\sum t_i^2 = \left(\sum t_i\right)^2 - 2\sum_{i<j} t_it_j:

i=14ti2=(2ac)22a2+b2r2c2=4a2c22(a2+b2r2)c2\sum_{i=1}^4 t_i^2 = \left(\frac{2a}{c}\right)^2 - 2 \cdot \frac{a^2 + b^2 - r^2}{c^2} = \frac{4a^2}{c^2} - \frac{2(a^2 + b^2 - r^2)}{c^2}

=4a22a22b2+2r2c2=2a22b2+2r2c2=2c2(a2b2+r2)= \frac{4a^2 - 2a^2 - 2b^2 + 2r^2}{c^2} = \frac{2a^2 - 2b^2 + 2r^2}{c^2} = \frac{2}{c^2}(a^2 - b^2 + r^2)

Part (iii)

We need to show that a=ba = b if and only if both conditions hold.

Direction 1: Suppose a=ba = b. Then the center of C2C_2 lies on y=xy = x.

By Vieta’s formulas, the product of all four roots of ()(*) is:

t1t2t3t4=c2c2=1t_1t_2t_3t_4 = \frac{c^2}{c^2} = 1

The sum of the reciprocals is:

i=141ti=i<j<ktitjtkt1t2t3t4=S3S4\sum_{i=1}^4 \frac{1}{t_i} = \frac{\sum_{i<j<k} t_it_jt_k}{t_1t_2t_3t_4} = \frac{S_3}{S_4}

By Vieta’s formulas, S3=2bcc2=2bcS_3 = \frac{2bc}{c^2} = \frac{2b}{c} and S4=1S_4 = 1, so:

i=141ti=2bc\sum_{i=1}^4 \frac{1}{t_i} = \frac{2b}{c}

Since a=ba = b, we have ti=2ac=2bc=1ti\sum t_i = \frac{2a}{c} = \frac{2b}{c} = \sum \frac{1}{t_i}. Both conditions are satisfied.

Direction 2: Suppose t1t2t3t4=1t_1t_2t_3t_4 = 1 and ti=1ti\sum t_i = \sum \frac{1}{t_i}. We show a=ba = b.

From Vieta’s formulas:

t1t2t3t4=c2c2=1t_1t_2t_3t_4 = \frac{c^2}{c^2} = 1

This is automatically true (the constant term and leading coefficient of ()(*) are both c2c^2), so this condition holds regardless of aa and bb.

The condition ti=1ti\sum t_i = \sum \frac{1}{t_i} gives:

2ac=2bc\frac{2a}{c} = \frac{2b}{c}

Therefore a=ba = b, so the center (a,b)(a, b) of C2C_2 lies on y=xy = x.

Examiner Notes

最受欢迎题目(94%考生选择),平均分约14/20。第(i)部分几乎全员正确。第(ii)部分求和符号书写不规范是主要扣分点,更高效的方法是将四次方程除以t⁴后与原方程比较。部分考生从(iii)反推,未获认可。第(iii)部分需注意利用(ii)的结果而非独立推导。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

2 (i) Suppose that there are three non-zero integers aa, bb and cc for which a3+2b3+4c3=0a^3 + 2b^3 + 4c^3 = 0. Explain why there must exist an integer pp, with p<a|p| < |a|, such that 4p3+b3+2c3=04p^3 + b^3 + 2c^3 = 0, and show further that there must exist integers pp, qq and rr, with p<a|p| < |a|, q<b|q| < |b| and r<c|r| < |c|, such that p3+2q3+4r3=0p^3 + 2q^3 + 4r^3 = 0. Deduce that no such integers aa, bb and cc can exist.

(ii) Prove that there are no non-zero integers aa, bb and cc for which 9a3+10b3+6c3=09a^3 + 10b^3 + 6c^3 = 0.

(iii) By considering the expression (3n±1)2(3n \pm 1)^2, prove that, unless an integer is a multiple of three, its square is one more than a multiple of 3. Deduce that the sum of the squares of two integers can only be a multiple of three if each of the integers is a multiple of three.

Hence prove that there are no non-zero integers aa, bb and cc for which a2+b2=3c2a^2 + b^2 = 3c^2.

(iv) Prove that there are no non-zero integers aa, bb and cc for which a2+b2+c2=4abca^2 + b^2 + c^2 = 4abc.

Hint

a3+2b3+4c3=0    aa^3+2b^3+4c^3=0 \implies a 偶数,设 a=2pa=2pp<a|p|<|a|8p3+2b3+4c3=0    4p3+b3+2c3=08p^3+2b^3+4c^3=0 \implies 4p^3+b^3+2c^3=0。 同理 b=2q,c=2rb=2q,c=2r,得 p3+2q3+4r3=0p^3+2q^3+4r^3=0。 无穷递降:不存在非零整数解。

9a3+10b3+6c3=0    3b9a^3+10b^3+6c^3=0 \implies 3|b,设 b=3qb=3q9a3+270q3+6c3=0    3a3+90q3+2c3=0    3c9a^3+270q^3+6c^3=0 \implies 3a^3+90q^3+2c^3=0 \implies 3|c。 同理 3a3|a,设 a=3pa=3p9p3+10q3+6r3=09p^3+10q^3+6r^3=0。无穷递降。

平方模 3:n≢0    n21n\not\equiv 0 \implies n^2\equiv 1a2+b20    a,ba^2+b^2\equiv 0 \implies a,b 均为 3 的倍数。 设 a=3p,b=3qa=3p,b=3q,则 c=3rc=3rp2+q2=3r2p^2+q^2=3r^2。无穷递降。

a2+b2+c2=4abca^2+b^2+c^2=4abc。RHS 0(mod4)    a,b,c\equiv 0 \pmod 4 \implies a,b,c 全偶。 设 a=2p,b=2q,c=2ra=2p,b=2q,c=2rp2+q2+r2=8pqrp^2+q^2+r^2=8pqr。无穷递降。

Model Solution

Part (i)

Suppose for contradiction that non-zero integers a,b,ca, b, c exist with a3+2b3+4c3=0a^3 + 2b^3 + 4c^3 = 0.

Step 1: Show aa is even and produce pp with p<a|p| < |a|.

Since a3+2b3+4c3=0a^3 + 2b^3 + 4c^3 = 0, we have a3=2b34c3=2(b3+2c3)a^3 = -2b^3 - 4c^3 = -2(b^3 + 2c^3). The right side is even, so a3a^3 is even, hence aa is even. Write a=2pa = 2p for some integer pp.

Substituting: (2p)3+2b3+4c3=0(2p)^3 + 2b^3 + 4c^3 = 0, i.e., 8p3+2b3+4c3=08p^3 + 2b^3 + 4c^3 = 0.

Dividing by 2:

4p3+b3+2c3=04p^3 + b^3 + 2c^3 = 0

Since a0a \neq 0, we have p0p \neq 0, and p=a/2<a|p| = |a|/2 < |a| (as a2|a| \geqslant 2).

Step 2: Show bb and cc are also even, producing q,rq, r with q<b|q| < |b|, r<c|r| < |c|.

From 4p3+b3+2c3=04p^3 + b^3 + 2c^3 = 0, we get b3=4p32c3=2(2p3+c3)b^3 = -4p^3 - 2c^3 = -2(2p^3 + c^3), so b3b^3 is even, hence bb is even. Write b=2qb = 2q.

Substituting: 4p3+8q3+2c3=04p^3 + 8q^3 + 2c^3 = 0, dividing by 2: 2p3+4q3+c3=02p^3 + 4q^3 + c^3 = 0.

So c3=2p34q3=2(p3+2q3)c^3 = -2p^3 - 4q^3 = -2(p^3 + 2q^3), hence cc is even. Write c=2rc = 2r.

Substituting: 2p3+4q3+8r3=02p^3 + 4q^3 + 8r^3 = 0, dividing by 2:

p3+2q3+4r3=0p^3 + 2q^3 + 4r^3 = 0

We have p<a|p| < |a|, q<b|q| < |b|, r<c|r| < |c|, and (p,q,r)(p, q, r) satisfies the same equation as (a,b,c)(a, b, c).

Step 3: Deduction by infinite descent.

Starting from any non-zero solution (a,b,c)(a, b, c), we produce a new non-zero solution (p,q,r)(p, q, r) with strictly smaller absolute values. Repeating this process produces an infinite strictly decreasing sequence of positive integers a>p>>0|a| > |p| > \cdots > 0. This is impossible since the positive integers are well-ordered (every non-empty set of positive integers has a least element). Therefore no non-zero integers a,b,ca, b, c with a3+2b3+4c3=0a^3 + 2b^3 + 4c^3 = 0 can exist.

Part (ii)

Suppose for contradiction that non-zero integers a,b,ca, b, c exist with 9a3+10b3+6c3=09a^3 + 10b^3 + 6c^3 = 0.

Step 1: Show 3b3 \mid b.

Reducing modulo 3: 9a3+10b3+6c30+b3+0b3(mod3)9a^3 + 10b^3 + 6c^3 \equiv 0 + b^3 + 0 \equiv b^3 \pmod{3}.

Since the left side equals 0, we need b30(mod3)b^3 \equiv 0 \pmod{3}, so 3b3 \mid b. Write b=3qb = 3q.

Substituting: 9a3+10(27q3)+6c3=09a^3 + 10(27q^3) + 6c^3 = 0, i.e., 9a3+270q3+6c3=09a^3 + 270q^3 + 6c^3 = 0.

Dividing by 3: 3a3+90q3+2c3=03a^3 + 90q^3 + 2c^3 = 0.

Step 2: Show 3c3 \mid c.

Reducing modulo 3: 3a3+90q3+2c30+0+2c32c3(mod3)3a^3 + 90q^3 + 2c^3 \equiv 0 + 0 + 2c^3 \equiv 2c^3 \pmod{3}.

Since the left side equals 0, we need 2c30(mod3)2c^3 \equiv 0 \pmod{3}, hence c30(mod3)c^3 \equiv 0 \pmod{3} (as gcd(2,3)=1\gcd(2, 3) = 1), so 3c3 \mid c. Write c=3rc = 3r.

Substituting: 3a3+90q3+54r3=03a^3 + 90q^3 + 54r^3 = 0. Dividing by 3: a3+30q3+18r3=0a^3 + 30q^3 + 18r^3 = 0.

Step 3: Show 3a3 \mid a.

Reducing modulo 3: a3+30q3+18r3a3(mod3)a^3 + 30q^3 + 18r^3 \equiv a^3 \pmod{3}.

Since the left side equals 0, a30(mod3)a^3 \equiv 0 \pmod{3}, so 3a3 \mid a. Write a=3pa = 3p.

Substituting: 27p3+30q3+18r3=027p^3 + 30q^3 + 18r^3 = 0. Dividing by 3:

9p3+10q3+6r3=09p^3 + 10q^3 + 6r^3 = 0

Step 4: Infinite descent.

We have a new solution (p,q,r)(p, q, r) satisfying the same equation, with p<a|p| < |a|, q<b|q| < |b|, r<c|r| < |c|. By the same infinite descent argument as part (i), no non-zero solution can exist.

Part (iii)

Step 1: Show that if nn is not a multiple of 3, then n21(mod3)n^2 \equiv 1 \pmod{3}.

If nn is not a multiple of 3, then n=3k+1n = 3k + 1 or n=3k1n = 3k - 1 for some integer kk.

Case 1: n=3k+1n = 3k + 1. Then n2=9k2+6k+1=3(3k2+2k)+11(mod3)n^2 = 9k^2 + 6k + 1 = 3(3k^2 + 2k) + 1 \equiv 1 \pmod{3}.

Case 2: n=3k1n = 3k - 1. Then n2=9k26k+1=3(3k22k)+11(mod3)n^2 = 9k^2 - 6k + 1 = 3(3k^2 - 2k) + 1 \equiv 1 \pmod{3}.

In both cases, n2n^2 is one more than a multiple of 3.

Step 2: Deduce that a2+b20(mod3)a^2 + b^2 \equiv 0 \pmod{3} implies 3a3 \mid a and 3b3 \mid b.

The possible values of a2(mod3)a^2 \pmod{3} and b2(mod3)b^2 \pmod{3} are:

  • If 3a3 \mid a: a20(mod3)a^2 \equiv 0 \pmod{3}.
  • If 3a3 \nmid a: a21(mod3)a^2 \equiv 1 \pmod{3} (by Step 1).

So a2+b2(mod3)a^2 + b^2 \pmod{3} can be 00, 11, or 22:

a(mod3)a \pmod{3}b(mod3)b \pmod{3}a2+b2(mod3)a^2 + b^2 \pmod{3}
000000
000\neq 011
0\neq 00011
0\neq 00\neq 022

Therefore a2+b20(mod3)a^2 + b^2 \equiv 0 \pmod{3} only when 3a3 \mid a and 3b3 \mid b.

Step 3: Prove no non-zero integers satisfy a2+b2=3c2a^2 + b^2 = 3c^2.

Suppose for contradiction that non-zero integers a,b,ca, b, c exist with a2+b2=3c2a^2 + b^2 = 3c^2.

Since 3c20(mod3)3c^2 \equiv 0 \pmod{3}, by Step 2, 3a3 \mid a and 3b3 \mid b. Write a=3pa = 3p, b=3qb = 3q.

Substituting: 9p2+9q2=3c29p^2 + 9q^2 = 3c^2, so 3(p2+q2)=c23(p^2 + q^2) = c^2.

This means 3c23 \mid c^2, and since 3 is prime, 3c3 \mid c. Write c=3rc = 3r.

Substituting: 3(p2+q2)=9r23(p^2 + q^2) = 9r^2, so p2+q2=3r2p^2 + q^2 = 3r^2.

We have a new solution (p,q,r)(p, q, r) satisfying the same equation, with p<a|p| < |a|, q<b|q| < |b|, r<c|r| < |c|. By infinite descent, no non-zero solution can exist.

Part (iv)

Suppose for contradiction that non-zero integers a,b,ca, b, c exist with a2+b2+c2=4abca^2 + b^2 + c^2 = 4abc.

Step 1: Show a,b,ca, b, c are all even.

Since 4abc4abc is divisible by 4, we need a2+b2+c20(mod4)a^2 + b^2 + c^2 \equiv 0 \pmod{4}.

The square of any integer satisfies (2k)2=4k20(mod4)(2k)^2 = 4k^2 \equiv 0 \pmod{4} and (2k+1)2=4k2+4k+11(mod4)(2k+1)^2 = 4k^2 + 4k + 1 \equiv 1 \pmod{4}. So a2+b2+c2(mod4)a^2 + b^2 + c^2 \pmod{4} equals the number of odd values among a,b,ca, b, c.

We check each case:

  • All three odd: a2+b2+c23(mod4)a^2 + b^2 + c^2 \equiv 3 \pmod{4}. But 4abc0(mod4)4abc \equiv 0 \pmod{4}. So 30(mod4)3 \equiv 0 \pmod{4}, contradiction.

  • Exactly two odd: a2+b2+c22(mod4)a^2 + b^2 + c^2 \equiv 2 \pmod{4}. But 4abc4abc is divisible by 4. So 20(mod4)2 \equiv 0 \pmod{4}, contradiction.

  • Exactly one odd: a2+b2+c21(mod4)a^2 + b^2 + c^2 \equiv 1 \pmod{4}. But 4abc0(mod4)4abc \equiv 0 \pmod{4}. So 10(mod4)1 \equiv 0 \pmod{4}, contradiction.

  • All three even: a2+b2+c20(mod4)a^2 + b^2 + c^2 \equiv 0 \pmod{4}. This is consistent.

Therefore a,b,ca, b, c must all be even.

Step 2: Infinite descent.

Write a=2pa = 2p, b=2qb = 2q, c=2rc = 2r. Substituting:

4p2+4q2+4r2=4(2p)(2q)(2r)=32pqr4p^2 + 4q^2 + 4r^2 = 4(2p)(2q)(2r) = 32pqr

Dividing by 4:

p2+q2+r2=8pqrp^2 + q^2 + r^2 = 8pqr

This equation has the same form as the original (a sum of three squares equals a constant times the product). We have p<a|p| < |a|, q<b|q| < |b|, r<c|r| < |c|.

By the same infinite descent argument, no non-zero solution can exist. \blacksquare

Examiner Notes

仅约半数考生尝试,平均分9/20。主要问题在于逻辑表述不清——“可以无限继续”或”模不断减小”的论述不够严谨,必须明确解释为什么整数性导致矛盾。第(ii)部分关键是利用模3分析。第(iv)部分出乎意料地需要更精巧的论证(非简单复制(i)的结构),许多考生在此受阻。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

3 (i) The curve C1C_1 has equation ax2+bxy+cy2=1ax^2 + bxy + cy^2 = 1 where abc0abc \neq 0 and a>0a > 0.

Show that, if the curve has two stationary points, then b2<4acb^2 < 4ac.

(ii) The curve C2C_2 has equation ay3+bx2y+cx=1ay^3 + bx^2y + cx = 1 where abc0abc \neq 0 and b>0b > 0.

Show that the xx-coordinates of stationary points on this curve satisfy 4cb3x48b3x3ac3=0.4cb^3x^4 - 8b^3x^3 - ac^3 = 0. Show that, if the curve has two stationary points, then 4ac6+27b3>04ac^6 + 27b^3 > 0.

(iii) Consider the simultaneous equations ay3+bx2y+cx=1ay^3 + bx^2y + cx = 1 2bxy+c=02bxy + c = 0 3ay2+bx2=03ay^2 + bx^2 = 0 where abc0abc \neq 0 and b>0b > 0.

Show that, if these simultaneous equations have a solution, then 4ac6+27b3=04ac^6 + 27b^3 = 0.

Hint

ax2+bxy+cy2=1ax^2+bxy+cy^2=1。隐函数求导:2ax+by+bxy+2cyy=02ax+by+bx y'+2cy y'=0。 驻点 y=0    by=2axy'=0 \implies by=-2ax。 原方程乘 b2b^2ab2x2+b3xy+b2cy2=b2ab^2x^2+b^3xy+b^2cy^2=b^2。 代入 by=2axby=-2axab2x22ab2x2+4a2cx2=b2    a(4acb2)x2=b2ab^2x^2-2ab^2x^2+4a^2cx^2=b^2 \implies a(4ac-b^2)x^2=b^2b2>0,a>0    4acb2>0    b2<4acb^2>0,a>0 \implies 4ac-b^2>0 \implies b^2<4ac

ay3+bx2y+cx=1ay^3+bx^2y+cx=13ay2y+2bxy+bx2y+c=03ay^2 y'+2bxy+bx^2 y'+c=0。 驻点 2bxy=c2bxy=-c。 原方程乘 8b3x38b^3x^38ab3x3y3+8b4x5y+8b3cx4=8b3x38ab^3x^3y^3+8b^4x^5y+8b^3cx^4=8b^3x^3(2bxy)3=c3    ac34cb3x4+8cb3x4=8b3x3    4cb3x48b3x3ac3=0(2bxy)^3=-c^3 \implies -ac^3-4cb^3x^4+8cb^3x^4=8b^3x^3 \implies 4cb^3x^4-8b^3x^3-ac^3=0f(x)=8b3x2(2cx3)=0f'(x)=8b^3x^2(2cx-3)=0,极值 x=32cx=\frac{3}{2c}f(32c)<0f(\frac{3}{2c})<0(或 >0>0    4ac6+27b3>0\implies 4ac^6+27b^3>0

联立三方程。3ay2+bx2=0    a<03ay^2+bx^2=0 \implies a<02bxy=c2bxy=-c,乘 4by24by^212aby4+c2=0    y4=c212ab12aby^4+c^2=0 \implies y^4=\frac{-c^2}{12ab}。 原方程乘 yyay4+bx2y2+cxy=yay^4+bx^2y^2+cxy=yay4=c212bay^4=\frac{-c^2}{12b}bx2y2=c24bbx^2y^2=\frac{c^2}{4b}cxy=c22bcxy=\frac{-c^2}{2b}y=c23by=\frac{-c^2}{3b}y4=(c23b)4=c212ab    4ac6+27b3=0y^4=(\frac{-c^2}{3b})^4=\frac{-c^2}{12ab} \implies 4ac^6+27b^3=0

Model Solution

Part (i)

We differentiate ax2+bxy+cy2=1ax^2 + bxy + cy^2 = 1 implicitly with respect to xx:

2ax+by+bxdydx+2cydydx=02ax + by + bx\frac{dy}{dx} + 2cy\frac{dy}{dx} = 0

At a stationary point, dydx=0\frac{dy}{dx} = 0, so:

2ax+by=0i.e.by=2ax()2ax + by = 0 \qquad \text{i.e.} \quad by = -2ax \qquad \cdots (*)

We substitute by=2axby = -2ax into the original equation. Multiply the original equation by b2b^2:

ab2x2+b3xy+b2cy2=b2ab^2x^2 + b^3xy + b^2cy^2 = b^2

Using by=2axby = -2ax, we get b3xy=b2(bxy)=b2(2ax2)=2ab2x2b^3xy = b^2(bxy) = b^2(-2ax^2) = -2ab^2x^2 and b2cy2=c(by)2=c4a2x2=4a2cx2b^2cy^2 = c(by)^2 = c \cdot 4a^2x^2 = 4a^2cx^2. Substituting:

ab2x22ab2x2+4a2cx2=b2ab^2x^2 - 2ab^2x^2 + 4a^2cx^2 = b^2

a(4acb2)x2=b2()a(4ac - b^2)x^2 = b^2 \qquad \cdots (**)

Since a>0a > 0 and b2>0b^2 > 0, equation ()(**) requires 4acb2>04ac - b^2 > 0 for real solutions xx to exist. If 4acb204ac - b^2 \leq 0, the left-hand side is non-positive while the right-hand side is positive, a contradiction.

Therefore, if the curve has stationary points, b2<4acb^2 < 4ac. \blacksquare

Part (ii)

We differentiate ay3+bx2y+cx=1ay^3 + bx^2y + cx = 1 implicitly:

3ay2dydx+2bxy+bx2dydx+c=03ay^2\frac{dy}{dx} + 2bxy + bx^2\frac{dy}{dx} + c = 0

At a stationary point, dydx=0\frac{dy}{dx} = 0:

2bxy+c=0()2bxy + c = 0 \qquad \cdots (*)

From ()(*): y=c2bxy = \frac{-c}{2bx} (note x0x \neq 0 since c0c \neq 0). Substituting into the original equation ay3+bx2y+cx=1ay^3 + bx^2y + cx = 1:

a(c2bx)3+bx2c2bx+cx=1a\left(\frac{-c}{2bx}\right)^3 + bx^2 \cdot \frac{-c}{2bx} + cx = 1

ac38b3x3cx2+cx=1\frac{-ac^3}{8b^3x^3} - \frac{cx}{2} + cx = 1

ac38b3x3+cx2=1\frac{-ac^3}{8b^3x^3} + \frac{cx}{2} = 1

Multiply through by 8b3x38b^3x^3:

ac3+4cb3x4=8b3x3-ac^3 + 4cb^3x^4 = 8b^3x^3

4cb3x48b3x3ac3=04cb^3x^4 - 8b^3x^3 - ac^3 = 0 \qquad \blacksquare

Now we show that if the curve has two stationary points, then 4ac6+27b3>04ac^6 + 27b^3 > 0.

Let f(x)=4cb3x48b3x3ac3f(x) = 4cb^3x^4 - 8b^3x^3 - ac^3. The stationary points of the curve correspond to roots of f(x)=0f(x) = 0.

Compute f(x)=16cb3x324b3x2=8b3x2(2cx3)f'(x) = 16cb^3x^3 - 24b^3x^2 = 8b^3x^2(2cx - 3).

Since b>0b > 0, f(x)=0f'(x) = 0 at x=0x = 0 (double root) and x=32cx = \frac{3}{2c}.

Because x=0x = 0 is a double root of ff', it is an inflection point of ff, not a local extremum. The only extremum of ff is at x=32cx = \frac{3}{2c}.

Evaluate:

f ⁣(32c)=4cb38116c48b3278c3ac3=81b34c327b3c3ac3=(4ac6+27b3)4c3f\!\left(\frac{3}{2c}\right) = 4cb^3 \cdot \frac{81}{16c^4} - 8b^3 \cdot \frac{27}{8c^3} - ac^3 = \frac{81b^3}{4c^3} - \frac{27b^3}{c^3} - ac^3 = \frac{-(4ac^6 + 27b^3)}{4c^3}

Also f(0)=ac3f(0) = -ac^3. The leading coefficient of ff is 4cb34cb^3, so f(x)+f(x) \to +\infty as x±x \to \pm\infty when c>0c > 0, and f(x)f(x) \to -\infty as x±x \to \pm\infty when c<0c < 0.

For f(x)=0f(x) = 0 to have exactly two real roots (corresponding to two stationary points), the unique extremum must be on the opposite side of the xx-axis from the end behaviour.

  • If c>0c > 0: f+f \to +\infty at both ends. Two roots requires f ⁣(32c)<0f\!\left(\frac{3}{2c}\right) < 0, i.e. (4ac6+27b3)4c3<0\frac{-(4ac^6 + 27b^3)}{4c^3} < 0. Since 4c3>04c^3 > 0, this gives 4ac6+27b3>04ac^6 + 27b^3 > 0.

  • If c<0c < 0: ff \to -\infty at both ends. Two roots requires f ⁣(32c)>0f\!\left(\frac{3}{2c}\right) > 0, i.e. (4ac6+27b3)4c3>0\frac{-(4ac^6 + 27b^3)}{4c^3} > 0. Since 4c3<04c^3 < 0, we need (4ac6+27b3)<0-(4ac^6 + 27b^3) < 0, which again gives 4ac6+27b3>04ac^6 + 27b^3 > 0.

In both cases, two stationary points requires 4ac6+27b3>04ac^6 + 27b^3 > 0. \blacksquare

Part (iii)

We have the simultaneous equations:

ay3+bx2y+cx=1(1)ay^3 + bx^2y + cx = 1 \qquad \cdots (1) 2bxy+c=0(2)2bxy + c = 0 \qquad \cdots (2) 3ay2+bx2=0(3)3ay^2 + bx^2 = 0 \qquad \cdots (3)

From (3)(3): bx2=3ay2bx^2 = -3ay^2. Since b>0b > 0, this requires a<0a < 0.

From (2)(2): x=c2byx = \frac{-c}{2by}. Squaring: x2=c24b2y2x^2 = \frac{c^2}{4b^2y^2}. Substituting into (3)(3):

3ay2+c24by2=03ay^2 + \frac{c^2}{4by^2} = 0

Multiply by 4by24by^2:

12aby4+c2=0(4)12aby^4 + c^2 = 0 \qquad \cdots (4)

Now multiply equation (1)(1) by yy:

ay4+bx2y2+cxy=yay^4 + bx^2y^2 + cxy = y

Using bx2=3ay2bx^2 = -3ay^2 (from (3)(3)), we get bx2y2=3ay4bx^2y^2 = -3ay^4.

From (2)(2): 2bxy=c2bxy = -c, so cxy=cc2b=c22bcxy = c \cdot \frac{-c}{2b} = \frac{-c^2}{2b}.

Substituting:

ay43ay4c22b=yay^4 - 3ay^4 - \frac{c^2}{2b} = y

2ay4c22b=y-2ay^4 - \frac{c^2}{2b} = y

From (4)(4): ay4=c212bay^4 = \frac{-c^2}{12b}, so 2ay4=c26b-2ay^4 = \frac{c^2}{6b}.

c26bc22b=y\frac{c^2}{6b} - \frac{c^2}{2b} = y

y=c23c26b=c23b(5)y = \frac{c^2 - 3c^2}{6b} = \frac{-c^2}{3b} \qquad \cdots (5)

Substitute (5)(5) into (4)(4):

12ab(c23b)4+c2=012ab \cdot \left(\frac{-c^2}{3b}\right)^4 + c^2 = 0

12abc881b4+c2=012ab \cdot \frac{c^8}{81b^4} + c^2 = 0

4ac827b3+c2=0\frac{4ac^8}{27b^3} + c^2 = 0

Divide by c2c^2 (valid since c0c \neq 0):

4ac627b3+1=0\frac{4ac^6}{27b^3} + 1 = 0

4ac6+27b3=04ac^6 + 27b^3 = 0 \qquad \blacksquare

Examiner Notes

超过90%考生尝试但平均分仅约5.5/20,是高尝试率中得分最低的题目。常见错误:错误假设两个驻点是重根、未考虑c<0的情况、对四次方程在驻点处取值符号的错误断言。值得注意的是,第(iii)部分通过直接消元求解方程组的考生反而比试图联系(ii)结果的考生表现更好。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

4 You may assume that all infinite sums and products in this question converge.

(i) Prove by induction that for all positive integers nn,

sinhx=2ncosh(x2)cosh(x4)cosh(x2n)sinh(x2n)\sinh x = 2^n \cosh \left( \frac{x}{2} \right) \cosh \left( \frac{x}{4} \right) \cdots \cosh \left( \frac{x}{2^n} \right) \sinh \left( \frac{x}{2^n} \right)

and deduce that, for x0x \neq 0,

sinhxxx2nsinh(x2n)=cosh(x2)cosh(x4)cosh(x2n).\frac{\sinh x}{x} \frac{\frac{x}{2^n}}{\sinh \left( \frac{x}{2^n} \right)} = \cosh \left( \frac{x}{2} \right) \cosh \left( \frac{x}{4} \right) \cdots \cosh \left( \frac{x}{2^n} \right) .

(ii) You are given that the Maclaurin series for sinhx\sinh x is

sinhx=r=0x2r+1(2r+1)!.\sinh x = \sum_{r=0}^{\infty} \frac{x^{2r+1}}{(2r+1)!} .

Use this result to show that, as yy tends to 0, ysinhy\frac{y}{\sinh y} tends to 1.

Deduce that, for x0x \neq 0,

sinhxx=cosh(x2)cosh(x4)cosh(x2n).\frac{\sinh x}{x} = \cosh \left( \frac{x}{2} \right) \cosh \left( \frac{x}{4} \right) \cdots \cosh \left( \frac{x}{2^n} \right) \cdots .

(iii) Let x=ln2x = \ln 2. Evaluate cosh(x2)\cosh \left( \frac{x}{2} \right) and show that

cosh(x4)=1+2122×214.\cosh \left( \frac{x}{4} \right) = \frac{1 + 2^{\frac{1}{2}}}{2 \times 2^{\frac{1}{4}}} .

Use part (ii) to show that

1ln2=1+2122×1+2142×1+2182.\frac{1}{\ln 2} = \frac{1 + 2^{\frac{1}{2}}}{2} \times \frac{1 + 2^{\frac{1}{4}}}{2} \times \frac{1 + 2^{\frac{1}{8}}}{2} \cdots .

(iv) Show that

2π=22×2+22×2+2+22.\frac{2}{\pi} = \frac{\sqrt{2}}{2} \times \frac{\sqrt{2 + \sqrt{2}}}{2} \times \frac{\sqrt{2 + \sqrt{2 + \sqrt{2}}}}{2} \cdots .

Hint

n=1n=1sinhx=2coshx2sinhx2\sinh x=2\cosh\frac{x}{2}\sinh\frac{x}{2}。 归纳:2k+1sinhx2k+1=2sinhxcoshx2k+1sinhx2k+1sinhx2k=sinhx2^{k+1}\cdots\sinh\frac{x}{2^{k+1}}=2\sinh x\cdot\frac{\cosh\frac{x}{2^{k+1}}\sinh\frac{x}{2^{k+1}}}{\sinh\frac{x}{2^k}}=\sinh x。 推论:两边除 xx 整理即得。

ysinhy1\frac{y}{\sinh y}\to 1y0y\to 0)。令 nn\to\inftysinhxx=n=1coshx2n\frac{\sinh x}{x}=\prod_{n=1}^{\infty}\cosh\frac{x}{2^n}

x=ln2x=\ln 2sinh(ln2)=34\sinh(\ln 2)=\frac{3}{4}coshln22=322\cosh\frac{\ln 2}{2}=\frac{3}{2\sqrt{2}}1ln2=1+22×1+242×=n=11+21/2n2\frac{1}{\ln 2}=\frac{1+\sqrt{2}}{2}\times\frac{1+\sqrt[4]{2}}{2}\times\cdots=\prod_{n=1}^{\infty}\frac{1+2^{1/2^n}}{2}

x=iπ2x=\frac{i\pi}{2}sinh(iπ/2)iπ/2=2π\frac{\sinh(i\pi/2)}{i\pi/2}=\frac{2}{\pi}cosπ4=22\cos\frac{\pi}{4}=\frac{\sqrt{2}}{2}cosπ8=2+22\cos\frac{\pi}{8}=\frac{\sqrt{2+\sqrt{2}}}{2}2π=22×2+22×\frac{2}{\pi}=\frac{\sqrt{2}}{2}\times\frac{\sqrt{2+\sqrt{2}}}{2}\times\cdots(Vieta 公式)。

Model Solution

Part (i)

We prove by induction on nn that:

sinhx=2ncosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)sinh ⁣(x2n)P(n)\sinh x = 2^n \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \sinh\!\left(\frac{x}{2^n}\right) \qquad \text{P}(n)

Base case (n=1n = 1): We need sinhx=2cosh ⁣(x2)sinh ⁣(x2)\sinh x = 2\cosh\!\left(\frac{x}{2}\right)\sinh\!\left(\frac{x}{2}\right).

Using the identity sinhx=sinh ⁣(2x2)=2sinh ⁣(x2)cosh ⁣(x2)\sinh x = \sinh\!\left(2 \cdot \frac{x}{2}\right) = 2\sinh\!\left(\frac{x}{2}\right)\cosh\!\left(\frac{x}{2}\right), the base case holds. (This follows from sinh2θ=2sinhθcoshθ\sinh 2\theta = 2\sinh\theta\cosh\theta, which is the hyperbolic analogue of sin2θ=2sinθcosθ\sin 2\theta = 2\sin\theta\cos\theta.)

Inductive step: Assume P(k)(k) holds for some positive integer kk, i.e.:

sinhx=2kcosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2k)sinh ⁣(x2k)\sinh x = 2^k \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^k}\right) \sinh\!\left(\frac{x}{2^k}\right)

We need to show P(k+1)(k+1): sinhx=2k+1cosh ⁣(x2)cosh ⁣(x2k+1)sinh ⁣(x2k+1)\sinh x = 2^{k+1} \cosh\!\left(\frac{x}{2}\right) \cdots \cosh\!\left(\frac{x}{2^{k+1}}\right) \sinh\!\left(\frac{x}{2^{k+1}}\right).

Applying sinhθ=2sinh ⁣(θ2)cosh ⁣(θ2)\sinh\theta = 2\sinh\!\left(\frac{\theta}{2}\right)\cosh\!\left(\frac{\theta}{2}\right) with θ=x2k\theta = \frac{x}{2^k}:

sinh ⁣(x2k)=2sinh ⁣(x2k+1)cosh ⁣(x2k+1)\sinh\!\left(\frac{x}{2^k}\right) = 2\sinh\!\left(\frac{x}{2^{k+1}}\right)\cosh\!\left(\frac{x}{2^{k+1}}\right)

Substituting into the inductive hypothesis:

sinhx=2kcosh ⁣(x2)cosh ⁣(x2k)2sinh ⁣(x2k+1)cosh ⁣(x2k+1)\sinh x = 2^k \cosh\!\left(\frac{x}{2}\right) \cdots \cosh\!\left(\frac{x}{2^k}\right) \cdot 2\sinh\!\left(\frac{x}{2^{k+1}}\right)\cosh\!\left(\frac{x}{2^{k+1}}\right)

=2k+1cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2k+1)sinh ⁣(x2k+1)= 2^{k+1} \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^{k+1}}\right) \sinh\!\left(\frac{x}{2^{k+1}}\right)

This is P(k+1)(k+1). By induction, P(n)(n) holds for all positive integers nn. \blacksquare

Deduction: For x0x \neq 0, divide both sides of P(n)(n) by xx:

sinhxx=2ncosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)sinh ⁣(x2n)x2n2n111\frac{\sinh x}{x} = 2^n \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \cdot \frac{\sinh\!\left(\frac{x}{2^n}\right)}{\frac{x}{2^n} \cdot \frac{2^n}{1}} \cdot \frac{1}{1}

More directly, rewrite P(n)(n) as:

sinhx=cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)2nsinh ⁣(x2n)1\sinh x = \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \cdot \frac{2^n \sinh\!\left(\frac{x}{2^n}\right)}{1}

Divide both sides by xx:

sinhxx=cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)2nsinh ⁣(x2n)x\frac{\sinh x}{x} = \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \cdot \frac{2^n \sinh\!\left(\frac{x}{2^n}\right)}{x}

Since x=2nx2nx = 2^n \cdot \frac{x}{2^n}:

sinhxx=cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)sinh ⁣(x2n)x2n\frac{\sinh x}{x} = \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \cdot \frac{\sinh\!\left(\frac{x}{2^n}\right)}{\frac{x}{2^n}}

Rearranging:

sinhxxx2nsinh ⁣(x2n)=cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)\frac{\sinh x}{x} \cdot \frac{\frac{x}{2^n}}{\sinh\!\left(\frac{x}{2^n}\right)} = \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) \qquad \blacksquare

Part (ii)

Show that ysinhy1\frac{y}{\sinh y} \to 1 as y0y \to 0.

From the Maclaurin series:

sinhy=y+y33!+y55!+=y(1+y26+y4120+)\sinh y = y + \frac{y^3}{3!} + \frac{y^5}{5!} + \cdots = y\left(1 + \frac{y^2}{6} + \frac{y^4}{120} + \cdots\right)

So:

ysinhy=11+y26+y4120+\frac{y}{\sinh y} = \frac{1}{1 + \frac{y^2}{6} + \frac{y^4}{120} + \cdots}

As y0y \to 0, the terms y26,y4120,\frac{y^2}{6}, \frac{y^4}{120}, \ldots all tend to 00, so:

limy0ysinhy=11+0=1\lim_{y \to 0} \frac{y}{\sinh y} = \frac{1}{1 + 0} = 1 \qquad \blacksquare

Deduction: From Part (i), for any fixed x0x \neq 0 and all nn:

sinhxxx2nsinh ⁣(x2n)=cosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)\frac{\sinh x}{x} \cdot \frac{\frac{x}{2^n}}{\sinh\!\left(\frac{x}{2^n}\right)} = \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right)

As nn \to \infty, x2n0\frac{x}{2^n} \to 0, so x2nsinh ⁣(x2n)1\frac{\frac{x}{2^n}}{\sinh\!\left(\frac{x}{2^n}\right)} \to 1. Therefore:

sinhxx=limncosh ⁣(x2)cosh ⁣(x4)cosh ⁣(x2n)=m=1cosh ⁣(x2m)\frac{\sinh x}{x} = \lim_{n \to \infty} \cosh\!\left(\frac{x}{2}\right) \cosh\!\left(\frac{x}{4}\right) \cdots \cosh\!\left(\frac{x}{2^n}\right) = \prod_{m=1}^{\infty} \cosh\!\left(\frac{x}{2^m}\right) \qquad \blacksquare

Part (iii)

Let x=ln2x = \ln 2.

Evaluate cosh ⁣(x2)\cosh\!\left(\frac{x}{2}\right):

sinh(ln2)=eln2eln22=2122=34\sinh(\ln 2) = \frac{e^{\ln 2} - e^{-\ln 2}}{2} = \frac{2 - \frac{1}{2}}{2} = \frac{3}{4}

Using sinhx=2sinh ⁣(x2)cosh ⁣(x2)\sinh x = 2\sinh\!\left(\frac{x}{2}\right)\cosh\!\left(\frac{x}{2}\right) and cosh2 ⁣(x2)sinh2 ⁣(x2)=1\cosh^2\!\left(\frac{x}{2}\right) - \sinh^2\!\left(\frac{x}{2}\right) = 1:

sinh(ln2)=2sinh ⁣(ln22)cosh ⁣(ln22)=34\sinh(\ln 2) = 2\sinh\!\left(\frac{\ln 2}{2}\right)\cosh\!\left(\frac{\ln 2}{2}\right) = \frac{3}{4}

Alternatively, compute directly:

cosh ⁣(ln22)=eln2/2+eln2/22=2+122=2+222=3222=322\cosh\!\left(\frac{\ln 2}{2}\right) = \frac{e^{\ln 2/2} + e^{-\ln 2/2}}{2} = \frac{\sqrt{2} + \frac{1}{\sqrt{2}}}{2} = \frac{\sqrt{2} + \frac{\sqrt{2}}{2}}{2} = \frac{\frac{3\sqrt{2}}{2}}{2} = \frac{3}{2\sqrt{2}}

So cosh ⁣(x2)=322\cosh\!\left(\frac{x}{2}\right) = \frac{3}{2\sqrt{2}}. Note that 322=3221/2=1+2221/2=1+21/2221/2\frac{3}{2\sqrt{2}} = \frac{3}{2 \cdot 2^{1/2}} = \frac{1 + 2}{2 \cdot 2^{1/2}} = \frac{1 + 2^{1/2}}{2 \cdot 2^{1/2}} … Actually, let me write this differently.

322=323/2=3221/2\frac{3}{2\sqrt{2}} = \frac{3}{2^{3/2}} = \frac{3}{2 \cdot 2^{1/2}}

We can verify: 1+21/2221/4\frac{1 + 2^{1/2}}{2 \cdot 2^{1/4}} … hmm, let me check the pattern the question wants.

Actually, cosh ⁣(x2)=322\cosh\!\left(\frac{x}{2}\right) = \frac{3}{2\sqrt{2}}, and note:

322=32222=324\frac{3}{2\sqrt{2}} = \frac{3}{2\sqrt{2}} \cdot \frac{\sqrt{2}}{\sqrt{2}} = \frac{3\sqrt{2}}{4}

But let’s think about the pattern more carefully. We have ex/2=21/2e^{x/2} = 2^{1/2}, so:

cosh ⁣(x2)=21/2+21/22=21/2(1+21)2=21/2322=323/2\cosh\!\left(\frac{x}{2}\right) = \frac{2^{1/2} + 2^{-1/2}}{2} = \frac{2^{1/2}(1 + 2^{-1})}{2} = \frac{2^{1/2} \cdot \frac{3}{2}}{2} = \frac{3}{2^{3/2}}

More usefully: 21/2+21/22=12(21/2+21/2)\frac{2^{1/2} + 2^{-1/2}}{2} = \frac{1}{2}(2^{1/2} + 2^{-1/2}).

Show cosh ⁣(x4)=1+21/22×21/4\cosh\!\left(\frac{x}{4}\right) = \frac{1 + 2^{1/2}}{2 \times 2^{1/4}}:

cosh ⁣(x4)=ex/4+ex/42=21/4+21/42\cosh\!\left(\frac{x}{4}\right) = \frac{e^{x/4} + e^{-x/4}}{2} = \frac{2^{1/4} + 2^{-1/4}}{2}

Now 21/4=121/42^{-1/4} = \frac{1}{2^{1/4}}, so:

cosh ⁣(x4)=21/4+121/42=21/2+1221/4=1+21/22×21/4\cosh\!\left(\frac{x}{4}\right) = \frac{2^{1/4} + \frac{1}{2^{1/4}}}{2} = \frac{2^{1/2} + 1}{2 \cdot 2^{1/4}} = \frac{1 + 2^{1/2}}{2 \times 2^{1/4}} \qquad \blacksquare

General pattern: For any m1m \geq 1:

cosh ⁣(x2m)=21/2m+21/2m2=21/2m+1+21/2m+1221/2m+121/2m+1\cosh\!\left(\frac{x}{2^m}\right) = \frac{2^{1/2^m} + 2^{-1/2^m}}{2} = \frac{2^{1/2^{m+1}} + 2^{-1/2^{m+1}}}{2} \cdot \frac{2^{1/2^{m+1}}}{2^{1/2^{m+1}}}

Actually, let me just compute each factor directly. For m1m \geq 1, ex/2m=21/2me^{x/2^m} = 2^{1/2^m}:

cosh ⁣(x2m)=21/2m+21/2m2\cosh\!\left(\frac{x}{2^m}\right) = \frac{2^{1/2^m} + 2^{-1/2^m}}{2}

Note that 21/2m+21/2m=21/2m(22/2m+1)=21/2m(1+21/2m1)2^{1/2^m} + 2^{-1/2^m} = 2^{-1/2^m}(2^{2/2^m} + 1) = 2^{-1/2^m}(1 + 2^{1/2^{m-1}}). So:

cosh ⁣(x2m)=1+21/2m1221/2m\cosh\!\left(\frac{x}{2^m}\right) = \frac{1 + 2^{1/2^{m-1}}}{2 \cdot 2^{1/2^m}}

For m=1m = 1: cosh ⁣(x2)=1+21/1221/2=322\cosh\!\left(\frac{x}{2}\right) = \frac{1 + 2^{1/1}}{2 \cdot 2^{1/2}} = \frac{3}{2\sqrt{2}}.

For m=2m = 2: cosh ⁣(x4)=1+21/2221/4\cosh\!\left(\frac{x}{4}\right) = \frac{1 + 2^{1/2}}{2 \cdot 2^{1/4}}.

For general mm: cosh ⁣(x2m)=1+21/2m1221/2m\cosh\!\left(\frac{x}{2^m}\right) = \frac{1 + 2^{1/2^{m-1}}}{2 \cdot 2^{1/2^m}}.

Deduction using Part (ii): From Part (ii), sinhxx=m=1cosh ⁣(x2m)\frac{\sinh x}{x} = \prod_{m=1}^{\infty} \cosh\!\left(\frac{x}{2^m}\right). With x=ln2x = \ln 2:

sinh(ln2)ln2=3/4ln2=34ln2\frac{\sinh(\ln 2)}{\ln 2} = \frac{3/4}{\ln 2} = \frac{3}{4\ln 2}

And:

m=1cosh ⁣(ln22m)=m=11+21/2m1221/2m\prod_{m=1}^{\infty} \cosh\!\left(\frac{\ln 2}{2^m}\right) = \prod_{m=1}^{\infty} \frac{1 + 2^{1/2^{m-1}}}{2 \cdot 2^{1/2^m}}

So:

34ln2=m=11+21/2m1221/2m\frac{3}{4\ln 2} = \prod_{m=1}^{\infty} \frac{1 + 2^{1/2^{m-1}}}{2 \cdot 2^{1/2^m}}

We need to show this gives 1ln2=m=11+21/2m2\frac{1}{\ln 2} = \prod_{m=1}^{\infty} \frac{1 + 2^{1/2^m}}{2}.

Let’s compute the partial products. Let Pn=m=1ncosh ⁣(ln22m)P_n = \prod_{m=1}^{n} \cosh\!\left(\frac{\ln 2}{2^m}\right).

From Part (i): Pn=sinh(ln2)ln2ln2/2nsinh(ln2/2n)=34ln2ln2/2nsinh(ln2/2n)P_n = \frac{\sinh(\ln 2)}{\ln 2} \cdot \frac{\ln 2 / 2^n}{\sinh(\ln 2 / 2^n)} = \frac{3}{4\ln 2} \cdot \frac{\ln 2 / 2^n}{\sinh(\ln 2 / 2^n)}.

As nn \to \infty: ln2/2nsinh(ln2/2n)1\frac{\ln 2 / 2^n}{\sinh(\ln 2 / 2^n)} \to 1, so Pn34ln2P_n \to \frac{3}{4\ln 2}.

Now compute PnP_n directly:

Pn=m=1n21/2m+21/2m2P_n = \prod_{m=1}^{n} \frac{2^{1/2^m} + 2^{-1/2^m}}{2}

Let am=21/2ma_m = 2^{1/2^m}. Then cosh ⁣(ln22m)=am+am12=am2+12am\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{a_m + a_m^{-1}}{2} = \frac{a_m^2 + 1}{2a_m}.

Note am2=21/2m1=am1a_m^2 = 2^{1/2^{m-1}} = a_{m-1} (where a0=2a_0 = 2). So cosh ⁣(ln22m)=am1+12am\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{a_{m-1} + 1}{2a_m}.

Pn=m=1nam1+12am=m=1n(am1+1)2nm=1namP_n = \prod_{m=1}^{n} \frac{a_{m-1} + 1}{2a_m} = \frac{\prod_{m=1}^{n}(a_{m-1} + 1)}{2^n \prod_{m=1}^{n} a_m}

The denominator: m=1nam=21/221/421/2n=2m=1n1/2m=211/2n\prod_{m=1}^{n} a_m = 2^{1/2} \cdot 2^{1/4} \cdots 2^{1/2^n} = 2^{\sum_{m=1}^{n} 1/2^m} = 2^{1 - 1/2^n}.

So 2n211/2n=2n+11/2n2^n \cdot 2^{1-1/2^n} = 2^{n+1-1/2^n}.

The numerator: m=1n(am1+1)=(a0+1)(a1+1)(an1+1)=3(1+2)(1+21/4)(1+21/2n1)\prod_{m=1}^{n}(a_{m-1} + 1) = (a_0 + 1)(a_1 + 1) \cdots (a_{n-1} + 1) = 3 \cdot (1 + \sqrt{2}) \cdot (1 + 2^{1/4}) \cdots (1 + 2^{1/2^{n-1}}).

Hmm, this is getting complicated. Let me try a telescoping approach instead.

Note that am1+12am=am1+12am\frac{a_{m-1}+1}{2a_m} = \frac{a_{m-1}+1}{2a_m}. Since am1=am2a_{m-1} = a_m^2:

am2+12am=(am+1)22am2am\frac{a_m^2 + 1}{2a_m} = \frac{(a_m+1)^2 - 2a_m}{2a_m}

That doesn’t telescope nicely either. Let me try yet another approach.

Actually, let’s just use the result from Part (ii) directly. We have sinhxx=m=1cosh ⁣(x2m)\frac{\sinh x}{x} = \prod_{m=1}^{\infty} \cosh\!\left(\frac{x}{2^m}\right), so:

1ln2=1sinh(ln2)sinh(ln2)ln2=43m=1cosh ⁣(ln22m)\frac{1}{\ln 2} = \frac{1}{\sinh(\ln 2)} \cdot \frac{\sinh(\ln 2)}{\ln 2} = \frac{4}{3} \cdot \prod_{m=1}^{\infty} \cosh\!\left(\frac{\ln 2}{2^m}\right)

Wait, sinh(ln2)=3/4\sinh(\ln 2) = 3/4, so sinh(ln2)ln2=34ln2\frac{\sinh(\ln 2)}{\ln 2} = \frac{3}{4\ln 2}, giving 1ln2=4334ln2=1ln2\frac{1}{\ln 2} = \frac{4}{3} \cdot \frac{3}{4\ln 2} = \frac{1}{\ln 2}. That’s circular.

Let me think about this differently. We need to show:

1ln2=1+21/221+21/421+21/82\frac{1}{\ln 2} = \frac{1 + 2^{1/2}}{2} \cdot \frac{1 + 2^{1/4}}{2} \cdot \frac{1 + 2^{1/8}}{2} \cdots

Let me define bm=1+21/2m2b_m = \frac{1 + 2^{1/2^m}}{2} for m=1,2,3,m = 1, 2, 3, \ldots

So the right side is m=1bm\prod_{m=1}^{\infty} b_m.

Now, cosh ⁣(ln22m)=21/2m+21/2m2\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{2^{1/2^m} + 2^{-1/2^m}}{2}. We showed this equals 1+21/2m1221/2m=bm121/2m\frac{1 + 2^{1/2^{m-1}}}{2 \cdot 2^{1/2^m}} = \frac{b_{m-1}}{2^{1/2^m}} (for m2m \geq 2, and cosh ⁣(ln22)=322\cosh\!\left(\frac{\ln 2}{2}\right) = \frac{3}{2\sqrt{2}}).

Hmm wait, let me be more careful. We have:

cosh ⁣(ln22m)=21/2m+21/2m2\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{2^{1/2^m} + 2^{-1/2^m}}{2}

Let t=21/2mt = 2^{1/2^m}. Then cosh=t+t12=t2+12t\cosh = \frac{t + t^{-1}}{2} = \frac{t^2 + 1}{2t}.

Now t2=21/2m1t^2 = 2^{1/2^{m-1}}, so t2+1=1+21/2m1t^2 + 1 = 1 + 2^{1/2^{m-1}}.

And 2t=221/2m=21+1/2m2t = 2 \cdot 2^{1/2^m} = 2^{1 + 1/2^m}.

So cosh ⁣(ln22m)=1+21/2m121+1/2m\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{1 + 2^{1/2^{m-1}}}{2^{1+1/2^m}}.

For m=1m = 1: cosh ⁣(ln22)=1+221+1/2=323/2=322\cosh\!\left(\frac{\ln 2}{2}\right) = \frac{1 + 2}{2^{1+1/2}} = \frac{3}{2^{3/2}} = \frac{3}{2\sqrt{2}}. Correct.

For m2m \geq 2: cosh ⁣(ln22m)=1+21/2m121+1/2m=bm121/2m11=2bm1221/2m\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{1 + 2^{1/2^{m-1}}}{2^{1+1/2^m}} = \frac{b_{m-1}}{2^{1/2^m}} \cdot \frac{1}{1} = \frac{2 \cdot b_{m-1}}{2 \cdot 2^{1/2^m}}

Actually bm1=1+21/2m12b_{m-1} = \frac{1 + 2^{1/2^{m-1}}}{2}, so 1+21/2m1=2bm11 + 2^{1/2^{m-1}} = 2b_{m-1}.

Therefore cosh ⁣(ln22m)=2bm121+1/2m=bm121/2m\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{2b_{m-1}}{2^{1+1/2^m}} = \frac{b_{m-1}}{2^{1/2^m}}.

So for m2m \geq 2:

cosh ⁣(ln22m)=bm121/2m\cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{b_{m-1}}{2^{1/2^m}}

And cosh ⁣(ln22)=322=323/2\cosh\!\left(\frac{\ln 2}{2}\right) = \frac{3}{2\sqrt{2}} = \frac{3}{2^{3/2}}.

Now:

m=1cosh ⁣(ln22m)=323/2m=2bm121/2m=323/2m=1bmm=221/2m\prod_{m=1}^{\infty} \cosh\!\left(\frac{\ln 2}{2^m}\right) = \frac{3}{2^{3/2}} \cdot \prod_{m=2}^{\infty} \frac{b_{m-1}}{2^{1/2^m}} = \frac{3}{2^{3/2}} \cdot \frac{\prod_{m=1}^{\infty} b_m}{\prod_{m=2}^{\infty} 2^{1/2^m}}

Now m=221/2m=2m=21/2m=21/2\prod_{m=2}^{\infty} 2^{1/2^m} = 2^{\sum_{m=2}^{\infty} 1/2^m} = 2^{1/2}.

Also b1=1+22b_1 = \frac{1 + \sqrt{2}}{2}, and 323/2=322\frac{3}{2^{3/2}} = \frac{3}{2\sqrt{2}}.

So:

34ln2=323/2m=1bm21/2=323/221/2m=1bm=34m=1bm\frac{3}{4\ln 2} = \frac{3}{2^{3/2}} \cdot \frac{\prod_{m=1}^{\infty} b_m}{2^{1/2}} = \frac{3}{2^{3/2} \cdot 2^{1/2}} \cdot \prod_{m=1}^{\infty} b_m = \frac{3}{4} \cdot \prod_{m=1}^{\infty} b_m

Therefore:

1ln2=m=1bm=1+21/221+21/421+21/82\frac{1}{\ln 2} = \prod_{m=1}^{\infty} b_m = \frac{1 + 2^{1/2}}{2} \cdot \frac{1 + 2^{1/4}}{2} \cdot \frac{1 + 2^{1/8}}{2} \cdots \qquad \blacksquare

Part (iv)

We substitute x=iπ2x = \frac{i\pi}{2} into the result of Part (ii): sinhxx=m=1cosh ⁣(x2m)\frac{\sinh x}{x} = \prod_{m=1}^{\infty} \cosh\!\left(\frac{x}{2^m}\right).

Left side: Using sinh(iθ)=isinθ\sinh(i\theta) = i\sin\theta:

sinh ⁣(iπ2)iπ2=isin ⁣(π2)iπ2=1π2=2π\frac{\sinh\!\left(\frac{i\pi}{2}\right)}{\frac{i\pi}{2}} = \frac{i\sin\!\left(\frac{\pi}{2}\right)}{\frac{i\pi}{2}} = \frac{1}{\frac{\pi}{2}} = \frac{2}{\pi}

Right side: Using cosh(iθ)=cosθ\cosh(i\theta) = \cos\theta:

cosh ⁣(iπ22m)=cos ⁣(π2m+1)\cosh\!\left(\frac{i\pi}{2 \cdot 2^m}\right) = \cos\!\left(\frac{\pi}{2^{m+1}}\right)

So:

2π=m=1cos ⁣(π2m+1)=cos ⁣(π4)cos ⁣(π8)cos ⁣(π16)\frac{2}{\pi} = \prod_{m=1}^{\infty} \cos\!\left(\frac{\pi}{2^{m+1}}\right) = \cos\!\left(\frac{\pi}{4}\right) \cos\!\left(\frac{\pi}{8}\right) \cos\!\left(\frac{\pi}{16}\right) \cdots

Now we evaluate each factor.

cos ⁣(π4)=22\cos\!\left(\frac{\pi}{4}\right) = \frac{\sqrt{2}}{2}

For cos ⁣(π8)\cos\!\left(\frac{\pi}{8}\right), use the half-angle formula cos ⁣(θ2)=1+cosθ2\cos\!\left(\frac{\theta}{2}\right) = \sqrt{\frac{1 + \cos\theta}{2}} with θ=π4\theta = \frac{\pi}{4}:

cos ⁣(π8)=1+cos(π/4)2=1+222=2+24=2+22\cos\!\left(\frac{\pi}{8}\right) = \sqrt{\frac{1 + \cos(\pi/4)}{2}} = \sqrt{\frac{1 + \frac{\sqrt{2}}{2}}{2}} = \sqrt{\frac{2 + \sqrt{2}}{4}} = \frac{\sqrt{2 + \sqrt{2}}}{2}

For cos ⁣(π16)\cos\!\left(\frac{\pi}{16}\right), apply the half-angle formula again with θ=π8\theta = \frac{\pi}{8}:

cos ⁣(π16)=1+cos(π/8)2=1+2+222=2+2+22\cos\!\left(\frac{\pi}{16}\right) = \sqrt{\frac{1 + \cos(\pi/8)}{2}} = \sqrt{\frac{1 + \frac{\sqrt{2+\sqrt{2}}}{2}}{2}} = \frac{\sqrt{2 + \sqrt{2 + \sqrt{2}}}}{2}

In general, defining c1=2c_1 = \sqrt{2} and ck+1=2+ckc_{k+1} = \sqrt{2 + c_k}, we get cos ⁣(π2m+1)=cm2\cos\!\left(\frac{\pi}{2^{m+1}}\right) = \frac{c_m}{2}.

Therefore:

2π=222+222+2+22\frac{2}{\pi} = \frac{\sqrt{2}}{2} \cdot \frac{\sqrt{2 + \sqrt{2}}}{2} \cdot \frac{\sqrt{2 + \sqrt{2 + \sqrt{2}}}}{2} \cdots \qquad \blacksquare

Examiner Notes

第四受欢迎题目(80%+考生尝试),平均分9/20。归纳法中逻辑流向不规范和未讨论除零问题是常见扣分点。第(ii)部分许多考生误用洛必达法则而非题目要求的麦克劳林级数。第(iv)部分最佳方法是虚数代换(令x=iπ/2),但许多考生试图使用Osborn法则却未充分论证。


Topic: 纯数  |  Difficulty: Standard  |  Marks: 20

5 (i) Show that aa11+exdx=a for all a0.\int_{-a}^{a} \frac{1}{1+e^{x}} dx = a \text{ for all } a \geqslant 0.

(ii) Explain why, if gg is a continuous function and 0ag(x)dx=0 for all a0,\int_{0}^{a} g(x) dx = 0 \text{ for all } a \geqslant 0, then g(x)=0g(x) = 0 for all x0x \geqslant 0.

Let ff be a continuous function with f(x)0f(x) \geqslant 0 for all xx. Show that aa11+f(x)dx=a for all a0\int_{-a}^{a} \frac{1}{1+f(x)} dx = a \text{ for all } a \geqslant 0 if and only if 11+f(x)+11+f(x)1=0 for all x0,\frac{1}{1+f(x)} + \frac{1}{1+f(-x)} - 1 = 0 \text{ for all } x \geqslant 0, and hence if and only if f(x)f(x)=1f(x)f(-x) = 1 for all xx.

(iii) Let ff be a continuous function such that, for all xx, f(x)0f(x) \geqslant 0 and f(x)f(x)=1f(x)f(-x) = 1. Show that, if hh is a continuous function with h(x)=h(x)h(x) = h(-x) for all xx, then aah(x)1+f(x)dx=0ah(x)dx.\int_{-a}^{a} \frac{h(x)}{1+f(x)} dx = \int_{0}^{a} h(x) dx .

(iv) Hence find the exact value of 12π12πexcosxcoshxdx.\int_{-\frac{1}{2}\pi}^{\frac{1}{2}\pi} \frac{e^{-x} \cos x}{\cosh x} dx .

Hint

解题思路

本题围绕积分对称性展开,四个部分层层递进:

  • Part (i) 通过具体函数 1/(1+e^x) 建立一个积分恒等式
  • Part (ii) 利用微积分基本定理推广到一般函数,建立充要条件
  • Part (iii) 将结论推广到含偶函数 h(x) 的被积函数
  • Part (iv) 将理论应用于具体积分求值

Part (i):证明 ∫_{-a}^{a} 1/(1+e^x) dx = a(a ≥ 0)

方法一(分子分母同乘 e^{-x}): ∫{-a}^{a} 1/(1+e^x) dx = ∫{-a}^{a} e^{-x}/(e^{-x}+1) dx = [-ln(e^{-x}+1)]_{-a}^{a} = ln((e^a+1)/(e^{-a}+1)) = ln(e^a) = a

方法二(拆项法): 1/(1+e^x) + 1/(1+e^{-x}) = 1/(1+e^x) + e^x/(1+e^x) = 1 因此 ∫_{-a}^{a} 1/(1+e^x) dx = ∫_0^a 1 dx = a。

Part (ii) 第一部分:若 g 连续且 ∫_0^a g(x) dx = 0 对所有 a ≥ 0,则 g(x) = 0(x ≥ 0)

由微积分基本定理(FTC),设 G(a) = ∫_0^a g(x) dx,则 G(a) = 0 对所有 a ≥ 0,故 G’(a) = g(a) = 0 对所有 a ≥ 0。

Part (ii) 第二部分:证明充要条件

必要性(⇒): ∫{-a}^{a} 1/(1+f(x)) dx = a ⇔ ∫{-a}^{0} 1/(1+f(x)) dx + ∫{0}^{a} 1/(1+f(x)) dx = a 对第一项作 x → -x 代换: ⇔ ∫{0}^{a} 1/(1+f(-x)) dx + ∫{0}^{a} 1/(1+f(x)) dx = a ⇔ ∫{0}^{a} [1/(1+f(-x)) + 1/(1+f(x)) - 1] dx = 0 由第一部分结论,被积函数恒为零: 1/(1+f(-x)) + 1/(1+f(x)) - 1 = 0 ∀ x ≥ 0

充分性(⇐):反向推导同样成立。

化简得 f(x)f(-x) = 1: 1/(1+f(x)) + 1/(1+f(-x)) = 1 ⇔ 1+f(-x) + 1+f(x) = (1+f(x))(1+f(-x)) ⇔ 2 + f(x) + f(-x) = 1 + f(x) + f(-x) + f(x)f(-x) ⇔ f(x)f(-x) = 1

Part (iii):设 f(x) ≥ 0,f(x)f(-x) = 1,h 连续且 h(x) = h(-x),证明 ∫_{-a}^{a} h(x)/(1+f(x)) dx = ∫_0^a h(x) dx

{-a}^{a} h(x)/(1+f(x)) dx = ∫{-a}^{0} h(x)/(1+f(x)) dx + ∫_{0}^{a} h(x)/(1+f(x)) dx

对第一项作 x → -x 代换,利用 h(-x) = h(x): = ∫{0}^{a} h(x)/(1+f(-x)) dx + ∫{0}^{a} h(x)/(1+f(x)) dx = ∫_0^a h(x)[1/(1+f(-x)) + 1/(1+f(x))] dx

由 Part (ii) 的结论 1/(1+f(-x)) + 1/(1+f(x)) = 1: = ∫_0^a h(x) dx

Part (iv):求 ∫_{-π/2}^{π/2} (e^{-x} cos x)/cosh x dx

第一步:化简被积函数 (e^{-x} cos x)/cosh x = (e^{-x} cos x)/((e^x + e^{-x})/2) = (2 cos x)/(e^{2x} + 1) = (2 cos x)/(1 + e^{2x})

第二步:验证条件

  • h(x) = cos x:连续且 h(-x) = cos(-x) = cos x = h(x)(偶函数)✓
  • f(x) = e^{2x}:连续,f(x) > 0,f(x)f(-x) = e^{2x} · e^{-2x} = 1 ✓

第三步:应用 Part (iii) 结论 ∫_{-π/2}^{π/2} (2 cos x)/(1+e^{2x}) dx = 2∫_0^{π/2} cos x dx = 2[sin x]_0^{π/2} = 2(1 - 0) = 2

常见错误(Examiner Notes)

  1. Part (i):积分 ∫ 1/(1+e^x) dx 错误地算成 ln(1+e^x)
  2. Part (ii):直接从 ∫_{-a}^{a} g(x) dx = 0 推出 g(x) = 0,这是错误推理
  3. Part (ii):使用 u = -x 代换时未展示充分的推导步骤
  4. Part (iii):未意识到 h(x) = h(-x) 即使题目已给出此条件
  5. Part (iv):未验证 cos x 和 e^{2x} 满足 Part (iii) 的条件;遗漏因子 2
Model Solution

Part (i)

Let I=aa11+exdxI = \int_{-a}^{a} \frac{1}{1+e^{x}} dx.

Using the substitution u=xu = -x (so du=dxdu = -dx), when x=ax = -a, u=au = a; when x=ax = a, u=au = -a. Thus

I=aa11+eu(du)=aa11+eudu.I = \int_{a}^{-a} \frac{1}{1+e^{-u}} (-du) = \int_{-a}^{a} \frac{1}{1+e^{-u}} du.

Since 11+eu=eueu+1\frac{1}{1+e^{-u}} = \frac{e^{u}}{e^{u}+1}, renaming the dummy variable back to xx:

I=aaex1+exdx.I = \int_{-a}^{a} \frac{e^{x}}{1+e^{x}} dx.

Adding the two expressions for II:

2I=aa11+exdx+aaex1+exdx=aa1+ex1+exdx=aa1dx=2a.2I = \int_{-a}^{a} \frac{1}{1+e^{x}} dx + \int_{-a}^{a} \frac{e^{x}}{1+e^{x}} dx = \int_{-a}^{a} \frac{1+e^{x}}{1+e^{x}} dx = \int_{-a}^{a} 1 \, dx = 2a.

Therefore I=aI = a.

Part (ii)

First we show that if gg is continuous and 0ag(x)dx=0\int_{0}^{a} g(x) dx = 0 for all a0a \geqslant 0, then g(x)=0g(x) = 0 for all x0x \geqslant 0.

Define G(a)=0ag(x)dxG(a) = \int_{0}^{a} g(x) dx. By hypothesis, G(a)=0G(a) = 0 for all a0a \geqslant 0. Since gg is continuous, by the Fundamental Theorem of Calculus, GG is differentiable and G(a)=g(a)G'(a) = g(a) for all a>0a > 0. But G(a)=0G(a) = 0 for all a0a \geqslant 0 implies G(a)=0G'(a) = 0 for all a>0a > 0. Hence g(x)=0g(x) = 0 for all x>0x > 0. By continuity of gg, g(0)=limx0+g(x)=0g(0) = \lim_{x \to 0^+} g(x) = 0. So g(x)=0g(x) = 0 for all x0x \geqslant 0.

Now let ff be continuous with f(x)0f(x) \geqslant 0 for all xx. We show that aa11+f(x)dx=a\int_{-a}^{a} \frac{1}{1+f(x)} dx = a for all a0a \geqslant 0 if and only if 11+f(x)+11+f(x)1=0\frac{1}{1+f(x)} + \frac{1}{1+f(-x)} - 1 = 0 for all x0x \geqslant 0.

Forward direction (\Rightarrow): Suppose aa11+f(x)dx=a\int_{-a}^{a} \frac{1}{1+f(x)} dx = a for all a0a \geqslant 0. Split the integral:

a011+f(x)dx+0a11+f(x)dx=a.\int_{-a}^{0} \frac{1}{1+f(x)} dx + \int_{0}^{a} \frac{1}{1+f(x)} dx = a.

In the first integral, substitute u=xu = -x (so du=dxdu = -dx):

a011+f(x)dx=a011+f(u)(du)=0a11+f(u)du.\int_{-a}^{0} \frac{1}{1+f(x)} dx = \int_{a}^{0} \frac{1}{1+f(-u)} (-du) = \int_{0}^{a} \frac{1}{1+f(-u)} du.

Renaming uu to xx:

0a11+f(x)dx+0a11+f(x)dx=a.\int_{0}^{a} \frac{1}{1+f(-x)} dx + \int_{0}^{a} \frac{1}{1+f(x)} dx = a.

Combining:

0a[11+f(x)+11+f(x)]dx=a=0a1dx.\int_{0}^{a} \left[ \frac{1}{1+f(-x)} + \frac{1}{1+f(x)} \right] dx = a = \int_{0}^{a} 1 \, dx.

Therefore:

0a[11+f(x)+11+f(x)1]dx=0for all a0.\int_{0}^{a} \left[ \frac{1}{1+f(-x)} + \frac{1}{1+f(x)} - 1 \right] dx = 0 \quad \text{for all } a \geqslant 0.

Since ff is continuous, the integrand g(x)=11+f(x)+11+f(x)1g(x) = \frac{1}{1+f(-x)} + \frac{1}{1+f(x)} - 1 is continuous. By the result just proved, g(x)=0g(x) = 0 for all x0x \geqslant 0, i.e.,

11+f(x)+11+f(x)1=0for all x0.\frac{1}{1+f(x)} + \frac{1}{1+f(-x)} - 1 = 0 \quad \text{for all } x \geqslant 0.

Backward direction (\Leftarrow): Suppose 11+f(x)+11+f(x)1=0\frac{1}{1+f(x)} + \frac{1}{1+f(-x)} - 1 = 0 for all x0x \geqslant 0. Then for all a0a \geqslant 0:

0a[11+f(x)+11+f(x)1]dx=0,\int_{0}^{a} \left[ \frac{1}{1+f(x)} + \frac{1}{1+f(-x)} - 1 \right] dx = 0,

so 0a[11+f(x)+11+f(x)]dx=a\int_{0}^{a} \left[ \frac{1}{1+f(x)} + \frac{1}{1+f(-x)} \right] dx = a. Reversing the substitution u=xu = -x on the second integral:

0a11+f(x)dx=a011+f(x)dx.\int_{0}^{a} \frac{1}{1+f(-x)} dx = \int_{-a}^{0} \frac{1}{1+f(x)} dx.

Therefore aa11+f(x)dx=a\int_{-a}^{a} \frac{1}{1+f(x)} dx = a.

Showing the equivalence with f(x)f(x)=1f(x)f(-x) = 1: Starting from 11+f(x)+11+f(x)=1\frac{1}{1+f(x)} + \frac{1}{1+f(-x)} = 1, multiply both sides by (1+f(x))(1+f(x))(1+f(x))(1+f(-x)):

(1+f(x))+(1+f(x))=(1+f(x))(1+f(x)).(1+f(-x)) + (1+f(x)) = (1+f(x))(1+f(-x)).

Expanding the right side:

2+f(x)+f(x)=1+f(x)+f(x)+f(x)f(x).2 + f(x) + f(-x) = 1 + f(x) + f(-x) + f(x)f(-x).

Cancelling f(x)+f(x)f(x) + f(-x) from both sides:

2=1+f(x)f(x),2 = 1 + f(x)f(-x),

hence f(x)f(x)=1f(x)f(-x) = 1 for all xx.

Part (iii)

Let ff be continuous with f(x)0f(x) \geqslant 0 and f(x)f(x)=1f(x)f(-x) = 1 for all xx, and let hh be continuous with h(x)=h(x)h(x) = h(-x) for all xx. We show aah(x)1+f(x)dx=0ah(x)dx\int_{-a}^{a} \frac{h(x)}{1+f(x)} dx = \int_{0}^{a} h(x) dx.

Split the integral:

aah(x)1+f(x)dx=a0h(x)1+f(x)dx+0ah(x)1+f(x)dx.\int_{-a}^{a} \frac{h(x)}{1+f(x)} dx = \int_{-a}^{0} \frac{h(x)}{1+f(x)} dx + \int_{0}^{a} \frac{h(x)}{1+f(x)} dx.

In the first integral, substitute u=xu = -x:

a0h(x)1+f(x)dx=a0h(u)1+f(u)(du)=0ah(u)1+f(u)du.\int_{-a}^{0} \frac{h(x)}{1+f(x)} dx = \int_{a}^{0} \frac{h(-u)}{1+f(-u)} (-du) = \int_{0}^{a} \frac{h(-u)}{1+f(-u)} du.

Since h(u)=h(u)h(-u) = h(u), this equals 0ah(u)1+f(u)du\int_{0}^{a} \frac{h(u)}{1+f(-u)} du. Renaming uu to xx and combining:

aah(x)1+f(x)dx=0ah(x)[11+f(x)+11+f(x)]dx.\int_{-a}^{a} \frac{h(x)}{1+f(x)} dx = \int_{0}^{a} h(x) \left[ \frac{1}{1+f(-x)} + \frac{1}{1+f(x)} \right] dx.

By Part (ii), since f(x)f(x)=1f(x)f(-x) = 1 for all xx (and f(x)0f(x) \geqslant 0), we have 11+f(x)+11+f(x)=1\frac{1}{1+f(-x)} + \frac{1}{1+f(x)} = 1 for all x0x \geqslant 0. Therefore:

aah(x)1+f(x)dx=0ah(x)1dx=0ah(x)dx.\int_{-a}^{a} \frac{h(x)}{1+f(x)} dx = \int_{0}^{a} h(x) \cdot 1 \, dx = \int_{0}^{a} h(x) dx.

Part (iv)

We evaluate 12π12πexcosxcoshxdx\int_{-\frac{1}{2}\pi}^{\frac{1}{2}\pi} \frac{e^{-x} \cos x}{\cosh x} dx.

First, rewrite the integrand using coshx=ex+ex2\cosh x = \frac{e^{x} + e^{-x}}{2}:

excosxcoshx=excosxex+ex2=2excosxex+ex.\frac{e^{-x} \cos x}{\cosh x} = \frac{e^{-x} \cos x}{\frac{e^{x} + e^{-x}}{2}} = \frac{2e^{-x} \cos x}{e^{x} + e^{-x}}.

Multiplying numerator and denominator by exe^{x}:

2excosxex+exexex=2cosxe2x+1=2cosx1+e2x.\frac{2e^{-x} \cos x}{e^{x} + e^{-x}} \cdot \frac{e^{x}}{e^{x}} = \frac{2 \cos x}{e^{2x} + 1} = \frac{2\cos x}{1 + e^{2x}}.

We identify h(x)=2cosxh(x) = 2\cos x and f(x)=e2xf(x) = e^{2x}, and verify the conditions of Part (iii):

  • f(x)=e2x>0f(x) = e^{2x} > 0 for all xx, so f(x)0f(x) \geqslant 0.
  • f(x)f(x)=e2xe2x=1f(x)f(-x) = e^{2x} \cdot e^{-2x} = 1 for all xx.
  • h(x)=2cosxh(x) = 2\cos x is continuous and h(x)=2cos(x)=2cosx=h(x)h(-x) = 2\cos(-x) = 2\cos x = h(x), so hh is even.

All conditions are satisfied. Applying Part (iii) with a=π2a = \frac{\pi}{2}:

π2π22cosx1+e2xdx=0π22cosxdx=2[sinx]0π2=2(10)=2.\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \frac{2\cos x}{1 + e^{2x}} dx = \int_{0}^{\frac{\pi}{2}} 2\cos x \, dx = 2[\sin x]_{0}^{\frac{\pi}{2}} = 2(1 - 0) = 2.

Therefore:

12π12πexcosxcoshxdx=2.\int_{-\frac{1}{2}\pi}^{\frac{1}{2}\pi} \frac{e^{-x} \cos x}{\cosh x} dx = 2.

Examiner Notes

第三成功题目,平均分接近满分的一半。第(i)部分常见错误是积分∫1/(1+eˣ)dx直接得到ln(1+eˣ)而非正确简化,以及推导步骤不充分。第(ii)部分最难,关键错误警示:∫₋ₐᵃg(x)dx=0不能直接推出g(x)=0(g(x)=sin x是反例),必须使用微积分基本定理。第(iv)部分必须使用前面部分的结果(题目要求”hence”),否则不给分。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

6 (i) Show that when α\alpha is small, cos(θ+α)cosθαsinθ12α2cosθ\cos(\theta + \alpha) - \cos \theta \approx -\alpha \sin \theta - \frac{1}{2} \alpha^2 \cos \theta.

Find the limit as α0\alpha \to 0 of sin(θ+α)sinθcos(θ+α)cosθ(*)\frac{\sin(\theta + \alpha) - \sin \theta}{\cos(\theta + \alpha) - \cos \theta} \qquad \text{(*)}

in the case sinθ0\sin \theta \neq 0.

In the case sinθ=0\sin \theta = 0, what happens to the value of expression (*) when α0\alpha \to 0?

(ii) A circle C1C_1 of radius aa rolls without slipping in an anti-clockwise direction on a fixed circle C2C_2 with centre at the origin OO and radius (n1)a(n - 1)a, where nn is an integer greater than 2. The point PP is fixed on C1C_1. Initially the centre of C1C_1 is at (na,0)(na, 0) and PP is at ((n+1)a,0)((n + 1)a, 0).

(a) Let QQ be the point of contact of C1C_1 and C2C_2 at any time in the rolling motion. Show that when OQOQ makes an angle θ\theta, measured anticlockwise, with the positive xx-axis, the xx-coordinate of PP is x(θ)=a(ncosθ+cosnθ)x(\theta) = a(n \cos \theta + \cos n\theta), and find the corresponding expression for the yy-coordinate, y(θ)y(\theta), of PP.

(b) Find the values of θ\theta for which the distance OPOP is (n1)a(n - 1)a.

(c) Let θ0=1n1π\theta_0 = \frac{1}{n - 1} \pi. Find the limit as α0\alpha \to 0 of y(θ0+α)y(θ0)x(θ0+α)x(θ0).\frac{y(\theta_0 + \alpha) - y(\theta_0)}{x(\theta_0 + \alpha) - x(\theta_0)}.

Hence show that, at the point (x(θ0),y(θ0))(x(\theta_0), y(\theta_0)), the tangent to the curve traced out by PP is parallel to OPOP.

Hint

解题思路概述: 本题分为两部分:(i) 小量近似与三角函数极限;(ii) 滚动圆的参数方程(外摆线),涉及几何推理、代数化简和极限计算。

Part (i) 第一问(Show that): 利用展开 cos(θ + α) = cos θ cos α - sin θ sin α,取小量近似 cos α ≈ 1 - α²/2,sin α ≈ α: cos(θ + α) - cos θ ≈ cos θ(1 - α²/2) - sin θ · α - cos θ = -α sin θ - (α²/2) cos θ

Part (i) 第二问(sin θ ≠ 0 的情况): 类似地,sin(θ + α) - sin θ ≈ α cos θ - (α²/2) sin θ。 lim_{α→0} [sin(θ+α)-sinθ]/[cos(θ+α)-cosθ] = lim_{α→0} [α cos θ - (α²/2) sin θ]/[-α sin θ - (α²/2) cos θ] = lim_{α→0} [cos θ - (α/2) sin θ]/[-sin θ - (α/2) cos θ] = -cot θ

(替代方法:L’Hôpital 法则直接求导得 cos(θ+α)/(-sin(θ+α)) → -cot θ)

Part (i) 第三问(sin θ = 0 的情况): 当 sin θ = 0 时,分子的 α cos θ 项不为零,分母 -α sin θ 为零: lim_{α→0} (α cos θ)/(-(α²/2) cos θ) = lim_{α→0} (-2)/α 因此当 α → +0 时趋向 -∞,当 α → -0 时趋向 +∞。

Part (ii)(a): C₂ 上初始接触点 Q₀,当 OQ 转过角度 θ 时,弧 Q₀Q 在 C₂ 上的长度为 (n-1)aθ。由于无滑动滚动,C₁ 上滚过的弧长也等于 (n-1)aθ。在 C₁ 上这对应角度 (n-1)aθ/a = (n-1)θ。

C₁ 的中心 T 的位置为 T = (na cos θ, na sin θ)。P 相对于 T 的方向角为 θ + (n-1)θ = nθ。 x(θ) = na cos θ + a cos nθ = a(n cos θ + cos nθ) y(θ) = na sin θ + a sin nθ = a(n sin θ + sin nθ)

Part (ii)(b): OP = (n-1)a 要求: (n cos θ + cos nθ)² + (n sin θ + sin nθ)² = (n-1)² 展开得 n² + 1 + 2n cos(n-1)θ = n² - 2n + 1,即 cos(n-1)θ = -1。

因此 (n-1)θ = (2r+1)π,r = 0, 1, 2, … θ = (2r+1)π/(n-1),r = 0, 1, 2, …

Part (ii)(c): 设 θ₀ = π/(n-1),需要求: lim_{α→0} [y(θ₀+α) - y(θ₀)]/[x(θ₀+α) - x(θ₀)]

利用小量展开,分子和分母分别化为: [cos θ₀ + cos nθ₀ - (α/2)(sin θ₀ + n sin nθ₀)]/[-(sin θ₀ + sin nθ₀) - (α/2)(cos θ₀ + n cos nθ₀)]

关键观察:因为 (n-1)θ₀ = π,利用和差化积:

  • cos θ₀ + cos nθ₀ = 2cos((n+1)θ₀/2)cos((n-1)θ₀/2) = 2cos((n+1)θ₀/2)cos(π/2) = 0
  • sin θ₀ + sin nθ₀ = 2sin((n+1)θ₀/2)cos((n-1)θ₀/2) = 0

利用加法公式 cos nθ₀ = cos((n-1)θ₀ + θ₀) = -cos θ₀,sin nθ₀ = -sin θ₀:

  • sin θ₀ + n sin nθ₀ = (1-n) sin θ₀
  • cos θ₀ + n cos nθ₀ = (1-n) cos θ₀

因此极限为:[(1-n) sin θ₀]/[(1-n) cos θ₀] = tan θ₀

这表明在点 (x(θ₀), y(θ₀)) 处,曲线的切线与 OP 平行。

常见错误(来自 Examiner Report):

  • Part (i):除以一个未必非零的量。
  • Part (ii):缺少图示或图示过小;未说明 x(θ) 中第二项 cos nθ 的来源。
  • Part (ii)(b):得出 cos(n-1)θ = -1 后忘记考虑周期性。
  • Part (ii)(c):错误地将极限当作 0/0 直接计算 cotangent。
Model Solution

Part (i)

Show that cos(θ+α)cosθαsinθ12α2cosθ\cos(\theta + \alpha) - \cos\theta \approx -\alpha\sin\theta - \frac{1}{2}\alpha^2\cos\theta when α\alpha is small.

Using the addition formula cos(θ+α)=cosθcosαsinθsinα\cos(\theta + \alpha) = \cos\theta\cos\alpha - \sin\theta\sin\alpha, and the small-angle approximations cosα1α22\cos\alpha \approx 1 - \frac{\alpha^2}{2}, sinαα\sin\alpha \approx \alpha:

cos(θ+α)cosθcosθ(1α22)sinθαcosθ=αsinθ12α2cosθ.\cos(\theta + \alpha) - \cos\theta \approx \cos\theta\left(1 - \frac{\alpha^2}{2}\right) - \sin\theta \cdot \alpha - \cos\theta = -\alpha\sin\theta - \frac{1}{2}\alpha^2\cos\theta.

Find the limit when sinθ0\sin\theta \neq 0.

Similarly, sin(θ+α)=sinθcosα+cosθsinα\sin(\theta + \alpha) = \sin\theta\cos\alpha + \cos\theta\sin\alpha, so:

sin(θ+α)sinθsinθ(1α22)+cosθαsinθ=αcosθ12α2sinθ.\sin(\theta + \alpha) - \sin\theta \approx \sin\theta\left(1 - \frac{\alpha^2}{2}\right) + \cos\theta \cdot \alpha - \sin\theta = \alpha\cos\theta - \frac{1}{2}\alpha^2\sin\theta.

Therefore:

sin(θ+α)sinθcos(θ+α)cosθαcosθ12α2sinθαsinθ12α2cosθ.\frac{\sin(\theta+\alpha) - \sin\theta}{\cos(\theta+\alpha) - \cos\theta} \approx \frac{\alpha\cos\theta - \frac{1}{2}\alpha^2\sin\theta}{-\alpha\sin\theta - \frac{1}{2}\alpha^2\cos\theta}.

Dividing numerator and denominator by α\alpha (valid since α0\alpha \neq 0):

cosθα2sinθsinθα2cosθ.\frac{\cos\theta - \frac{\alpha}{2}\sin\theta}{-\sin\theta - \frac{\alpha}{2}\cos\theta}.

Taking α0\alpha \to 0:

limα0sin(θ+α)sinθcos(θ+α)cosθ=cosθsinθ=cotθ.\lim_{\alpha \to 0} \frac{\sin(\theta+\alpha) - \sin\theta}{\cos(\theta+\alpha) - \cos\theta} = \frac{\cos\theta}{-\sin\theta} = -\cot\theta.

When sinθ=0\sin\theta = 0:

In this case cosθ=±1\cos\theta = \pm 1 (so cosθ0\cos\theta \neq 0). The numerator is αcosθ12α2sinθ=αcosθ\alpha\cos\theta - \frac{1}{2}\alpha^2\sin\theta = \alpha\cos\theta (first-order in α\alpha), while the denominator is αsinθ12α2cosθ=12α2cosθ-\alpha\sin\theta - \frac{1}{2}\alpha^2\cos\theta = -\frac{1}{2}\alpha^2\cos\theta (second-order in α\alpha). Thus:

sin(θ+α)sinθcos(θ+α)cosθαcosθ12α2cosθ=2α.\frac{\sin(\theta+\alpha) - \sin\theta}{\cos(\theta+\alpha) - \cos\theta} \approx \frac{\alpha\cos\theta}{-\frac{1}{2}\alpha^2\cos\theta} = \frac{-2}{\alpha}.

As α0+\alpha \to 0^+, this tends to -\infty; as α0\alpha \to 0^-, this tends to ++\infty. The expression has no finite limit.

Part (ii)(a)

When the rolling circle C1C_1 has rolled so that the contact point QQ on C2C_2 is at angle θ\theta from the positive xx-axis, the arc from the initial contact point to QQ on C2C_2 has length (n1)aθ(n-1)a\theta. By the no-slip condition, this equals the arc rolled on C1C_1, which subtends angle (n1)aθa=(n1)θ\frac{(n-1)a\theta}{a} = (n-1)\theta at the centre of C1C_1.

The centre TT of C1C_1 is at distance nana from OO (since the radii of C1C_1 and C2C_2 are aa and (n1)a(n-1)a respectively), so T=(nacosθ,nasinθ)T = (na\cos\theta, \, na\sin\theta).

Initially, PP was on the positive xx-side of TT. After rolling, PP has rotated by angle (n1)θ(n-1)\theta relative to TT in the same direction as the rolling. The direction from TT to PP relative to the positive xx-axis is θ+(n1)θ=nθ\theta + (n-1)\theta = n\theta. Therefore:

x(θ)=nacosθ+acos(nθ)=a(ncosθ+cosnθ),x(\theta) = na\cos\theta + a\cos(n\theta) = a(n\cos\theta + \cos n\theta),

y(θ)=nasinθ+asin(nθ)=a(nsinθ+sinnθ).y(\theta) = na\sin\theta + a\sin(n\theta) = a(n\sin\theta + \sin n\theta).

Part (ii)(b)

We need OP=(n1)aOP = (n-1)a, i.e., x(θ)2+y(θ)2=(n1)2a2x(\theta)^2 + y(\theta)^2 = (n-1)^2 a^2. Dividing by a2a^2:

(ncosθ+cosnθ)2+(nsinθ+sinnθ)2=(n1)2.(n\cos\theta + \cos n\theta)^2 + (n\sin\theta + \sin n\theta)^2 = (n-1)^2.

Expanding the left side:

n2cos2θ+2ncosθcosnθ+cos2nθ+n2sin2θ+2nsinθsinnθ+sin2nθn^2\cos^2\theta + 2n\cos\theta\cos n\theta + \cos^2 n\theta + n^2\sin^2\theta + 2n\sin\theta\sin n\theta + \sin^2 n\theta

=n2+1+2n(cosθcosnθ+sinθsinnθ)=n2+1+2ncos(n1)θ.= n^2 + 1 + 2n(\cos\theta\cos n\theta + \sin\theta\sin n\theta) = n^2 + 1 + 2n\cos(n-1)\theta.

Setting this equal to (n1)2=n22n+1(n-1)^2 = n^2 - 2n + 1:

n2+1+2ncos(n1)θ=n22n+1,n^2 + 1 + 2n\cos(n-1)\theta = n^2 - 2n + 1,

2ncos(n1)θ=2n,2n\cos(n-1)\theta = -2n,

cos(n1)θ=1.\cos(n-1)\theta = -1.

Therefore (n1)θ=(2r+1)π(n-1)\theta = (2r+1)\pi for integer rr, giving:

θ=(2r+1)πn1,r=0,1,2,\theta = \frac{(2r+1)\pi}{n-1}, \qquad r = 0, 1, 2, \ldots

Part (ii)(c)

Let θ0=πn1\theta_0 = \frac{\pi}{n-1}, so (n1)θ0=π(n-1)\theta_0 = \pi. We first compute x(θ0)x(\theta_0) and y(θ0)y(\theta_0).

Since (n1)θ0=π(n-1)\theta_0 = \pi, we have nθ0=π+θ0n\theta_0 = \pi + \theta_0, so cosnθ0=cos(π+θ0)=cosθ0\cos n\theta_0 = \cos(\pi + \theta_0) = -\cos\theta_0 and sinnθ0=sin(π+θ0)=sinθ0\sin n\theta_0 = \sin(\pi + \theta_0) = -\sin\theta_0. Therefore:

x(θ0)=a(ncosθ0cosθ0)=a(n1)cosθ0,x(\theta_0) = a(n\cos\theta_0 - \cos\theta_0) = a(n-1)\cos\theta_0,

y(θ0)=a(nsinθ0sinθ0)=a(n1)sinθ0.y(\theta_0) = a(n\sin\theta_0 - \sin\theta_0) = a(n-1)\sin\theta_0.

Now we expand x(θ0+α)x(\theta_0 + \alpha) and y(θ0+α)y(\theta_0 + \alpha) for small α\alpha.

Using cos(θ0+α)=cosθ0cosαsinθ0sinα\cos(\theta_0 + \alpha) = \cos\theta_0\cos\alpha - \sin\theta_0\sin\alpha and cos(nθ0+nα)=cosnθ0cosnαsinnθ0sinnα=cosθ0cosnα+sinθ0sinnα\cos(n\theta_0 + n\alpha) = \cos n\theta_0\cos n\alpha - \sin n\theta_0\sin n\alpha = -\cos\theta_0\cos n\alpha + \sin\theta_0\sin n\alpha:

x(θ0+α)=a[n(cosθ0cosαsinθ0sinα)+(cosθ0cosnα+sinθ0sinnα)]x(\theta_0 + \alpha) = a\bigl[n(\cos\theta_0\cos\alpha - \sin\theta_0\sin\alpha) + (-\cos\theta_0\cos n\alpha + \sin\theta_0\sin n\alpha)\bigr]

=a[cosθ0(ncosαcosnα)sinθ0(nsinαsinnα)].= a\bigl[\cos\theta_0(n\cos\alpha - \cos n\alpha) - \sin\theta_0(n\sin\alpha - \sin n\alpha)\bigr].

Similarly, using sin(θ0+α)=sinθ0cosα+cosθ0sinα\sin(\theta_0 + \alpha) = \sin\theta_0\cos\alpha + \cos\theta_0\sin\alpha and sinnθ0=sinθ0\sin n\theta_0 = -\sin\theta_0:

y(θ0+α)=a[sinθ0(ncosαcosnα)+cosθ0(nsinαsinnα)].y(\theta_0 + \alpha) = a\bigl[\sin\theta_0(n\cos\alpha - \cos n\alpha) + \cos\theta_0(n\sin\alpha - \sin n\alpha)\bigr].

The differences from the values at θ0\theta_0 are:

x(θ0+α)x(θ0)=a[cosθ0(ncosαcosnα(n1))sinθ0(nsinαsinnα)],x(\theta_0 + \alpha) - x(\theta_0) = a\bigl[\cos\theta_0(n\cos\alpha - \cos n\alpha - (n-1)) - \sin\theta_0(n\sin\alpha - \sin n\alpha)\bigr],

y(θ0+α)y(θ0)=a[sinθ0(ncosαcosnα(n1))+cosθ0(nsinαsinnα)].y(\theta_0 + \alpha) - y(\theta_0) = a\bigl[\sin\theta_0(n\cos\alpha - \cos n\alpha - (n-1)) + \cos\theta_0(n\sin\alpha - \sin n\alpha)\bigr].

For small α\alpha: cosα1α22\cos\alpha \approx 1 - \frac{\alpha^2}{2}, sinαα\sin\alpha \approx \alpha, cosnα1n2α22\cos n\alpha \approx 1 - \frac{n^2\alpha^2}{2}, sinnαnα\sin n\alpha \approx n\alpha. So:

ncosαcosnα(n1)n(1α22)(1n2α22)(n1)=n(n1)α22,n\cos\alpha - \cos n\alpha - (n-1) \approx n\left(1 - \frac{\alpha^2}{2}\right) - \left(1 - \frac{n^2\alpha^2}{2}\right) - (n-1) = \frac{n(n-1)\alpha^2}{2},

nsinαsinnαnαnα=0.n\sin\alpha - \sin n\alpha \approx n\alpha - n\alpha = 0.

The second expression vanishes to first order; more precisely, nsinαsinnα=nαnα36nα+n3α36+=n(n21)α36+n\sin\alpha - \sin n\alpha = n\alpha - \frac{n\alpha^3}{6} - n\alpha + \frac{n^3\alpha^3}{6} + \cdots = \frac{n(n^2-1)\alpha^3}{6} + \cdots, which is third-order. So the dominant contributions come from the α2\alpha^2 terms:

x(θ0+α)x(θ0)acosθ0n(n1)α22,x(\theta_0 + \alpha) - x(\theta_0) \approx a \cdot \cos\theta_0 \cdot \frac{n(n-1)\alpha^2}{2},

y(θ0+α)y(θ0)asinθ0n(n1)α22.y(\theta_0 + \alpha) - y(\theta_0) \approx a \cdot \sin\theta_0 \cdot \frac{n(n-1)\alpha^2}{2}.

Taking the ratio:

limα0y(θ0+α)y(θ0)x(θ0+α)x(θ0)=sinθ0cosθ0=tanθ0.\lim_{\alpha \to 0} \frac{y(\theta_0 + \alpha) - y(\theta_0)}{x(\theta_0 + \alpha) - x(\theta_0)} = \frac{\sin\theta_0}{\cos\theta_0} = \tan\theta_0.

Showing the tangent is parallel to OPOP:

At θ=θ0\theta = \theta_0, the point on the curve is P=(a(n1)cosθ0,a(n1)sinθ0)P = (a(n-1)\cos\theta_0, \, a(n-1)\sin\theta_0). The vector OPOP has direction (cosθ0,sinθ0)(\cos\theta_0, \sin\theta_0), so the slope of OPOP is sinθ0cosθ0=tanθ0\frac{\sin\theta_0}{\cos\theta_0} = \tan\theta_0.

The limit computed above is the slope of the tangent to the curve at this point, which also equals tanθ0\tan\theta_0. Since both slopes are equal, the tangent to the curve at (x(θ0),y(θ0))(x(\theta_0), y(\theta_0)) is parallel to OPOP.

Examiner Notes

约半数考生尝试,是得分最低的题目之一(平均分约1/4)。常见问题:图形缺失或过小且遗漏关键细节、未说明参数方程第二项的来源、第(b)部分忘记处理周期性(加2kπ)、第(c)部分错误地对0/0型极限直接求值后声称余切是答案。部分考生能正确识别零点并有效处理三角函数。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

7 Let n be a vector of unit length in three dimensions. For each vector r, f(r) is defined by f(r) = n × r.

(i) Given that

n=(abc) and r=(xyz),\mathbf{n} = \begin{pmatrix} a \\ b \\ c \end{pmatrix} \text{ and } \mathbf{r} = \begin{pmatrix} x \\ y \\ z \end{pmatrix},

show that the xx-component of f(f(r)) is x(b2+c2)+aby+acz-x(b^2 + c^2) + aby + acz. Show further that

f(f(r))=(nr)nr.\text{f(f}(\mathbf{r})) = (\mathbf{n} \cdot \mathbf{r})\mathbf{n} - \mathbf{r}.

Explain, by means of a diagram, how f(f(r)) is related to n and r.

(ii) Let RR be the point with position vector r and PP be the point with position vector g(r), where g is defined by

g(s)=s+sinθf(s)+(1cosθ)f(f(s)).\text{g}(\mathbf{s}) = \mathbf{s} + \sin \theta \, \text{f}(\mathbf{s}) + (1 - \cos \theta) \, \text{f(f}(\mathbf{s})).

By considering g(n) and g(r) when r is perpendicular to n, state, with justification, the geometric transformation which maps RR onto PP.

(iii) Let RR be the point with position vector r and QQ be the point with position vector h(r), where h is defined by

h(s)=s2f(f(s)).\text{h}(\mathbf{s}) = -\mathbf{s} - 2 \, \text{f(f}(\mathbf{s})).

State, with justification, the geometric transformation which maps RR onto QQ.

Hint

解题思路: 本题考察向量叉积的性质、Rodrigues 旋转公式和反射变换。核心恒等式是 n × (n × r) = (n·r)n − r(当 |n|=1 时)。

Part (i):证明 f(f(r)) = (n·r)n − r 并用图解释

步骤1:计算 f(r) = n × r f(r) = (a, b, c)ᵀ × (x, y, z)ᵀ = (bz − cy, cx − az, ay − bx)ᵀ

步骤2:计算 f(f(r)) 的 x 分量 f(f(r)) 的 x 分量 = b(ay − bx) − c(cx − az) = −x(b² + c²) + aby + acz

步骤3:利用 |n|=1 简化 由于 a² + b² + c² = 1: −x(b² + c²) + aby + acz = −x(a² + b² + c²) + a(ax + by + cz) = −x + a(n·r)

同理 y 分量为 −y + b(n·r),z 分量为 −z + c(n·r)。

因此 f(f(r)) = −r + (n·r)n = (n·r)n − r ✓

几何解释:r 可分解为平行于 n 的分量 (n·r)n 和垂直于 n 的分量 r − (n·r)n。f(f(r)) = (n·r)n − r = −(r − (n·r)n),即 r 的垂直分量取反。

Part (ii):旋转

步骤1:计算 g(n) g(n) = n + sin θ(n × n) + (1 − cos θ)((n·n)n − n) = n + 0 + (1 − cos θ)(n − n) = n → n 方向的向量在变换下不变。

步骤2:计算 g(r),其中 r ⊥ n 当 r ⊥ n 时,n·r = 0,所以 f(f(r)) = −r。 g(r) = r + sin θ(n × r) + (1 − cos θ)(−r) = r cos θ + sin θ(n × r)

步骤3:判断几何变换 r、n×r 都垂直于 n,且 |r| = |n×r|(因为 |n|=1),两者夹角为 θ。因此 g(r) 是将 r 绕 n 轴逆时针旋转角度 θ。

结论:g 表示绕 n 轴逆时针旋转角度 θ 的旋转变换。

Part (iii):反射

步骤1:化简 h(s) h(s) = −s − 2f(f(s)) = −s − 2((n·s)n − s) = s − 2(n·s)n

步骤2:验证变换性质

  • h(n) = n − 2(n·n)n = n − 2n = −n(n 方向反向)
  • 若 r ⊥ n,则 h(r) = r − 2(n·r)n = r(垂直分量不变)
  • h(n × r) = n × r − 2(n·(n × r))n = n × r(不变)

结论:h 表示关于过原点且垂直于 n 的平面的反射变换。

常见错误(来自 Examiner Report):

  1. Part (i):向量叉积计算错误,尤其是符号。
  2. Part (ii):未能正确解释 g 的几何意义。
  3. Part (iii):未能将 h 与反射联系起来。
Model Solution

Part (i)

We compute f(r) = n x r using the determinant formula:

n×r=ijkabcxyz=(bzcycxazaybx)\mathbf{n} \times \mathbf{r} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ a & b & c \\ x & y & z \end{vmatrix} = \begin{pmatrix} bz - cy \\ cx - az \\ ay - bx \end{pmatrix}

Now we compute f(f(r)) = n x (f(r)). The xx-component is:

b(aybx)c(cxaz)=abyb2xc2x+acz=x(b2+c2)+aby+aczb(ay - bx) - c(cx - az) = aby - b^2 x - c^2 x + acz = -x(b^2 + c^2) + aby + acz

This establishes the first result. Now we use n=1|\mathbf{n}| = 1, i.e., a2+b2+c2=1a^2 + b^2 + c^2 = 1, so b2+c2=1a2b^2 + c^2 = 1 - a^2. The xx-component becomes:

x(1a2)+a(by+cz)=x+a2x+aby+acz=x+a(ax+by+cz)=x+a(nr)-x(1 - a^2) + a(by + cz) = -x + a^2 x + aby + acz = -x + a(ax + by + cz) = -x + a(\mathbf{n} \cdot \mathbf{r})

By identical reasoning (cyclic permutation of components), the yy-component is y+b(nr)-y + b(\mathbf{n} \cdot \mathbf{r}) and the zz-component is z+c(nr)-z + c(\mathbf{n} \cdot \mathbf{r}). Therefore:

f(f(r))=r+(nr)n=(nr)nr(*)\text{f(f}(\mathbf{r})) = -\mathbf{r} + (\mathbf{n} \cdot \mathbf{r})\mathbf{n} = (\mathbf{n} \cdot \mathbf{r})\mathbf{n} - \mathbf{r} \qquad \text{(*)}

Diagram and geometric interpretation:

Any vector r can be decomposed into a component parallel to n and a component perpendicular to n:

r=(nr)ncomponent parallel to n+(r(nr)n)component perpendicular to n\mathbf{r} = \underbrace{(\mathbf{n} \cdot \mathbf{r})\mathbf{n}}_{\text{component parallel to } \mathbf{n}} + \underbrace{(\mathbf{r} - (\mathbf{n} \cdot \mathbf{r})\mathbf{n})}_{\text{component perpendicular to } \mathbf{n}}

From (*), f(f(r)) = (n . r)n - r = -(r - (n . r)n). This means f(f(r)) is the vector obtained by negating the perpendicular component of r while leaving the parallel component unchanged. In other words, f(f(r)) is the reflection of r through the line spanned by n (equivalently, the reflection in the direction perpendicular to n).

Diagrammatically, if we draw r, its component (nr)n(\mathbf{n} \cdot \mathbf{r})\mathbf{n} along n, and the perpendicular residual r(nr)n\mathbf{r} - (\mathbf{n} \cdot \mathbf{r})\mathbf{n}, then f(f(r)) has the same component along n but the perpendicular residual is flipped.

Part (ii)

We examine g in two special cases.

Case 1: s = n. Since n x n = 0, we have f(n) = 0 and f(f(n)) = (n . n)n - n = n - n = 0. Therefore:

g(n)=n+0+0=n\text{g}(\mathbf{n}) = \mathbf{n} + \mathbf{0} + \mathbf{0} = \mathbf{n}

So points along the n-axis are unchanged by g.

Case 2: s = r where r is perpendicular to n (i.e., n . r = 0).

Since n . r = 0, we get f(f(r)) = -r from (*). Therefore:

g(r)=r+sinθ(n×r)+(1cosθ)(r)=rcosθ+sinθ(n×r)\text{g}(\mathbf{r}) = \mathbf{r} + \sin\theta \, (\mathbf{n} \times \mathbf{r}) + (1 - \cos\theta)(-\mathbf{r}) = \mathbf{r}\cos\theta + \sin\theta \, (\mathbf{n} \times \mathbf{r})

Since |n| = 1 and r is perpendicular to n, we have |n x r| = |r|. The vectors r and n x r are both perpendicular to n and perpendicular to each other, with equal magnitudes. The expression rcosθ+(n×r)sinθ\mathbf{r}\cos\theta + (\mathbf{n} \times \mathbf{r})\sin\theta is a rotation of r by angle θ\theta within the plane perpendicular to n, in the direction from r towards n x r (which is the right-hand rule / anticlockwise direction about n).

Since any vector s can be decomposed as s=(ns)n+(s(ns)n)\mathbf{s} = (\mathbf{n} \cdot \mathbf{s})\mathbf{n} + (\mathbf{s} - (\mathbf{n} \cdot \mathbf{s})\mathbf{n}), and g fixes the parallel component (by Case 1) and rotates the perpendicular component by θ\theta (by Case 2), the transformation g is a rotation through angle θ\theta about the axis through the origin in the direction of n, in the anticlockwise sense (right-hand rule). This is precisely the Rodrigues rotation formula.

Part (iii)

We simplify h(s):

h(s)=s2f(f(s))=s2((ns)ns)=s2(ns)n\text{h}(\mathbf{s}) = -\mathbf{s} - 2\,\text{f(f}(\mathbf{s})) = -\mathbf{s} - 2((\mathbf{n} \cdot \mathbf{s})\mathbf{n} - \mathbf{s}) = \mathbf{s} - 2(\mathbf{n} \cdot \mathbf{s})\mathbf{n}

We verify the key properties:

  • h(n) = n - 2(n . n)n = n - 2n = -n. So the component along n is negated.
  • If r is perpendicular to n (i.e., n . r = 0), then h(r) = r. So the perpendicular component is unchanged.

Therefore h reflects each vector through the plane through the origin that is perpendicular to n: the component along n is negated, while all components in the plane perpendicular to n are preserved. This is precisely the reflection in the plane through OO perpendicular to n.

Examiner Notes

约三分之一考生尝试,略优于Q3和Q6。第(i)部分第一问通常正确,但许多考生忽略了n是单位向量的条件导致第二问推导困难。图形绘制是主要失分点——未能理解三个向量的大小关系和垂直关系。第(ii)(iii)部分少数考生能准确识别并论证变换,但多数虽有大致想法却无法精确定义和论证结论。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

8 (i) Use De Moivre’s theorem to prove that for any positive integer k>1k > 1,

sin(kθ)=sinθcosk1θ(k(k3)(sec2θ1)+(k5)(sec2θ1)2)\sin(k\theta) = \sin \theta \cos^{k-1} \theta \left( k - \binom{k}{3}(\sec^2 \theta - 1) + \binom{k}{5}(\sec^2 \theta - 1)^2 - \cdots \right)

and find a similar expression for cos(kθ)\cos(k\theta).

(ii) Let θ=cos1(1a)\theta = \cos^{-1}(\frac{1}{a}), where θ\theta is measured in degrees, and aa is an odd integer greater than 1.

Suppose that there is a positive integer kk such that sin(kθ)=0\sin(k\theta) = 0 and sin(mθ)0\sin(m\theta) \neq 0 for all integers mm with 0<m<k0 < m < k.

Show that it would be necessary to have kk even and cos(12kθ)=0\cos(\frac{1}{2}k\theta) = 0.

Deduce that θ\theta is irrational.

(iii) Show that if ϕ=cot1(1b)\phi = \cot^{-1}(\frac{1}{b}), where ϕ\phi is measured in degrees, and bb is an even integer greater than 1, then ϕ\phi is irrational.

Hint

解题思路: 本题以 De Moivre 定理为核心工具,通过分析 sin(kθ) 展开式中各项的奇偶性来证明角度的无理性。核心技巧是:将 sec²θ - 1 替换为 tan²θ = (a²-1),利用 a 为奇数时 a²-1 为偶数这一数论性质,证明展开式中括号内的值恒为奇数(从而非零),导出矛盾。

Part (i):用 De Moivre 定理展开 sin(kθ) 和 cos(kθ)

由 De Moivre 定理:cos(kθ) + i sin(kθ) = (cos θ + i sin θ)^k

用二项式展开右边,分别取虚部和实部:

sin(kθ) 的展开: sin(kθ) = C(k,1)cos^{k-1}θ sin θ - C(k,3)cos^{k-3}θ sin³θ + C(k,5)cos^{k-5}θ sin⁵θ - …

提取公因子 sin θ cos^{k-1}θ,并用 tan²θ = sec²θ - 1: sin(kθ) = sin θ cos^{k-1}θ [k - C(k,3)(sec²θ - 1) + C(k,5)(sec²θ - 1)² - …]

cos(kθ) 的类似表达式: cos(kθ) = cos^k θ [1 - C(k,2)(sec²θ - 1) + C(k,4)(sec²θ - 1)² - …]

Part (ii):证明 k 必须为偶数,并推导 θ 为无理数

设 θ = cos⁻¹(1/a),其中 a 为大于 1 的奇数。

第一步:证明 k 必须为偶数。

假设 k 为奇数。代入 sec θ = a,sin(kθ) = 0 意味着: sin θ · (1/a^{k-1}) [k - C(k,3)(a²-1) + C(k,5)(a²-1)² - … + (-1)^{(k-1)/2}(a²-1)^{(k-1)/2}] = 0

由于 a 为奇数,a² - 1 为偶数。括号内各项中:

  • 第一项 k 为奇数
  • 其余各项都包含 (a²-1) 的幂次,因此都是偶数 所以括号内 = 奇数 + 偶数之和 = 奇数 ≠ 0。

又 sin θ ≠ 0,1/a^{k-1} ≠ 0。三个因子均非零,矛盾!故 k 必须为偶数。

第二步:证明 cos(kθ/2) = 0。

k 为偶数时,sin(kθ) = 2 sin(kθ/2) cos(kθ/2) = 0。由于 k/2 < k,由题设 sin(kθ/2) ≠ 0,故必有 cos(kθ/2) = 0。

第三步:导出矛盾,证明 θ 为无理数。

设 n = k/2。由 Part (i) 的 cos 展开: cos(nθ) = (1/a^n)[1 - C(n,2)(a²-1) + C(n,4)(a²-1)² - …]

括号内第一项为 1(奇数),其余各项含 (a²-1) 的幂次(偶数),故括号内为奇数 ≠ 0。因此 cos(nθ) ≠ 0,与 cos(nθ) = 0 矛盾!

这说明不存在最小的正整数 k 使得 sin(kθ) = 0。若 θ 为有理数,则 θ = 180p/k,此时 sin(kθ) = sin(180p) = 0,矛盾。故 θ 为无理数。

Part (iii):证明 φ = cot⁻¹(1/b) 为无理数

设 b 为大于 1 的偶数,φ = cot⁻¹(1/b),即 tan φ = b。

假设存在最小的奇数 k 使得 sin(kφ) = 0。由 Part (i): sin(kφ) = sin φ cos^{k-1}φ [k - C(k,3)b² + C(k,5)b⁴ - …] = 0

括号内第一项 k 为奇数,其余各项含 b²(偶数,因为 b 为偶数),故括号内为奇数 ≠ 0。又 sin φ ≠ 0,cos φ ≠ 0,矛盾。故 k 不能为奇数。

若 k 为偶数,同 Part (ii) 论证,cos(kφ/2) = 0。设 n = k/2: cos(nφ) = cos^n φ [1 - C(n,2)b² + C(n,4)b⁴ - …]

括号内为奇数 ≠ 0,cos φ ≠ 0,故 cos(nφ) ≠ 0,矛盾。

因此不存在 k 使得 sin(kφ) = 0,故 φ 为无理数。

常见错误(来自 Examiner Report):

  1. 混淆度与弧度:题目明确说 θ 以度为单位,但有考生错误地引用 π 的无理性来论证。
  2. Part (ii) 不完整:大多数考生能代入 sec θ = a 得到展开式,但难以完成”k 必须为偶数”的论证。
  3. 忽视结果的意义:部分考生能证明 cos(kθ/2) = 0,但未能认识到它与无理性论证的关系。
  4. Part (i) 工作不足:少数考生未给出充分的推导过程。
Model Solution

Part (i)

By De Moivre’s theorem, cos(kθ)+isin(kθ)=(cosθ+isinθ)k\cos(k\theta) + i\sin(k\theta) = (\cos\theta + i\sin\theta)^k. We expand the right side using the binomial theorem:

(cosθ+isinθ)k=r=0k(kr)coskrθ(isinθ)r(\cos\theta + i\sin\theta)^k = \sum_{r=0}^{k} \binom{k}{r} \cos^{k-r}\theta \, (i\sin\theta)^r

Taking the imaginary part to obtain sin(kθ)\sin(k\theta), only odd powers of isinθi\sin\theta contribute (since i2m+1i^{2m+1} is purely imaginary):

sin(kθ)=(k1)cosk1θsinθ(k3)cosk3θsin3θ+(k5)cosk5θsin5θ\sin(k\theta) = \binom{k}{1}\cos^{k-1}\theta\sin\theta - \binom{k}{3}\cos^{k-3}\theta\sin^3\theta + \binom{k}{5}\cos^{k-5}\theta\sin^5\theta - \cdots

We factor out sinθcosk1θ\sin\theta\cos^{k-1}\theta from every term. The general term (k2j+1)cosk(2j+1)θsin2j+1θ\binom{k}{2j+1}\cos^{k-(2j+1)}\theta\sin^{2j+1}\theta becomes (k2j+1)cosk1θsinθsin2jθcos2jθ=(k2j+1)cosk1θsinθtan2jθ\binom{k}{2j+1}\cos^{k-1}\theta\sin\theta \cdot \frac{\sin^{2j}\theta}{\cos^{2j}\theta} = \binom{k}{2j+1}\cos^{k-1}\theta\sin\theta \cdot \tan^{2j}\theta.

Since tan2θ=sec2θ1\tan^2\theta = \sec^2\theta - 1, we obtain:

sin(kθ)=sinθcosk1θ(k(k3)(sec2θ1)+(k5)(sec2θ1)2)(*)\sin(k\theta) = \sin\theta\cos^{k-1}\theta\left(k - \binom{k}{3}(\sec^2\theta - 1) + \binom{k}{5}(\sec^2\theta - 1)^2 - \cdots\right) \qquad \text{(*)}

where the signs alternate and the powers of (sec2θ1)(\sec^2\theta - 1) increase by 1 at each step.

Taking the real part to obtain cos(kθ)\cos(k\theta), only even powers contribute:

cos(kθ)=(k0)coskθ(k2)cosk2θsin2θ+(k4)cosk4θsin4θ\cos(k\theta) = \binom{k}{0}\cos^k\theta - \binom{k}{2}\cos^{k-2}\theta\sin^2\theta + \binom{k}{4}\cos^{k-4}\theta\sin^4\theta - \cdots

Factoring out coskθ\cos^k\theta and using sin2jθ/cos2jθ=tan2jθ=(sec2θ1)j\sin^{2j}\theta/\cos^{2j}\theta = \tan^{2j}\theta = (\sec^2\theta - 1)^j:

cos(kθ)=coskθ(1(k2)(sec2θ1)+(k4)(sec2θ1)2)(**)\cos(k\theta) = \cos^k\theta\left(1 - \binom{k}{2}(\sec^2\theta - 1) + \binom{k}{4}(\sec^2\theta - 1)^2 - \cdots\right) \qquad \text{(**)}

Part (ii)

Let θ=cos1(1/a)\theta = \cos^{-1}(1/a) where aa is an odd integer greater than 1, so secθ=a\sec\theta = a. Suppose kk is the smallest positive integer with sin(kθ)=0\sin(k\theta) = 0.

Step 1: kk must be even.

Suppose for contradiction that kk is odd. Substituting secθ=a\sec\theta = a into (*):

sin(kθ)=sinθ1ak1[k(k3)(a21)+(k5)(a21)2+(1)(k1)/2(kk)(a21)(k1)/2]\sin(k\theta) = \sin\theta \cdot \frac{1}{a^{k-1}} \left[k - \binom{k}{3}(a^2 - 1) + \binom{k}{5}(a^2 - 1)^2 - \cdots + (-1)^{(k-1)/2}\binom{k}{k}(a^2 - 1)^{(k-1)/2}\right]

Since aa is an odd integer, a21a^2 - 1 is even. In the bracket:

  • The first term kk is odd (since kk is odd).
  • Every other term contains a positive power of (a21)(a^2 - 1), so each is even.

Therefore the bracket equals (odd) + (sum of evens) = odd, and in particular the bracket is non-zero.

Since θ=cos1(1/a)\theta = \cos^{-1}(1/a) with a>1a > 1, we have sinθ0\sin\theta \neq 0 and 1/ak101/a^{k-1} \neq 0. The product of three non-zero factors is non-zero, contradicting sin(kθ)=0\sin(k\theta) = 0. Hence kk must be even.

Step 2: cos(12kθ)=0\cos(\tfrac{1}{2}k\theta) = 0.

Since kk is even, write k=2nk = 2n where nn is a positive integer. Then:

sin(kθ)=sin(2nθ)=2sin(nθ)cos(nθ)=0\sin(k\theta) = \sin(2n\theta) = 2\sin(n\theta)\cos(n\theta) = 0

Since n=k/2<kn = k/2 < k, by the minimality of kk we have sin(nθ)0\sin(n\theta) \neq 0. Therefore cos(nθ)=0\cos(n\theta) = 0, i.e., cos(12kθ)=0\cos(\tfrac{1}{2}k\theta) = 0.

Step 3: Deduce that θ\theta is irrational.

We apply (**) with n=k/2n = k/2 and secθ=a\sec\theta = a:

cos(nθ)=1an[1(n2)(a21)+(n4)(a21)2]\cos(n\theta) = \frac{1}{a^n}\left[1 - \binom{n}{2}(a^2 - 1) + \binom{n}{4}(a^2 - 1)^2 - \cdots\right]

In the bracket, the first term is 1 (odd), and every other term contains a positive power of (a21)(a^2-1) (which is even), so each is even. The bracket is (odd) + (sum of evens) = odd, hence non-zero. Since 1/an01/a^n \neq 0, we conclude cos(nθ)0\cos(n\theta) \neq 0, contradicting Step 2.

This contradiction shows that no such smallest positive integer kk can exist. Now suppose θ\theta is rational, say θ=180p/q\theta = 180p/q degrees where p,qp, q are positive integers with gcd(p,q)=1\gcd(p, q) = 1. Then sin(qθ)=sin(180p)=0\sin(q\theta) = \sin(180p) = 0, so there exists a positive integer kqk \leq q with sin(kθ)=0\sin(k\theta) = 0. By the argument above, no such kk exists. This is a contradiction, so θ\theta must be irrational.

Part (iii)

Let ϕ=cot1(1/b)\phi = \cot^{-1}(1/b) where bb is an even integer greater than 1, so tanϕ=b\tan\phi = b (equivalently sec2ϕ=1+b2\sec^2\phi = 1 + b^2). We show ϕ\phi is irrational by the same strategy.

Suppose for contradiction that there exists a smallest positive integer kk with sin(kϕ)=0\sin(k\phi) = 0. We use the expansion (*) with sec2ϕ1=tan2ϕ=b2\sec^2\phi - 1 = \tan^2\phi = b^2:

sin(kϕ)=sinϕcosk1ϕ(k(k3)b2+(k5)b4)\sin(k\phi) = \sin\phi\cos^{k-1}\phi\left(k - \binom{k}{3}b^2 + \binom{k}{5}b^4 - \cdots\right)

Since bb is even, b2b^2 is even, and every positive power of b2b^2 is even.

Case 1: kk is odd. The bracket is k(even)+(even)=k+(even sum)k - (\text{even}) + (\text{even}) - \cdots = k + (\text{even sum}). Since kk is odd, the bracket is odd, hence non-zero. Since ϕ=cot1(1/b)\phi = \cot^{-1}(1/b) with b>1b > 1, we have sinϕ0\sin\phi \neq 0 and cosϕ0\cos\phi \neq 0. Three non-zero factors give sin(kϕ)0\sin(k\phi) \neq 0, a contradiction.

Case 2: kk is even. Write k=2nk = 2n. As before, sin(2nϕ)=2sin(nϕ)cos(nϕ)=0\sin(2n\phi) = 2\sin(n\phi)\cos(n\phi) = 0 with sin(nϕ)0\sin(n\phi) \neq 0 (by minimality of kk), so cos(nϕ)=0\cos(n\phi) = 0.

Now apply (**) with sec2ϕ1=b2\sec^2\phi - 1 = b^2:

cos(nϕ)=cosnϕ(1(n2)b2+(n4)b4)\cos(n\phi) = \cos^n\phi\left(1 - \binom{n}{2}b^2 + \binom{n}{4}b^4 - \cdots\right)

The bracket is 1+(sum of evens)=odd01 + (\text{sum of evens}) = \text{odd} \neq 0, and cosϕ0\cos\phi \neq 0, so cos(nϕ)0\cos(n\phi) \neq 0. This contradicts cos(nϕ)=0\cos(n\phi) = 0.

In both cases we reach a contradiction, so no such kk exists. If ϕ\phi were rational, say ϕ=180p/q\phi = 180p/q degrees, then sin(qϕ)=0\sin(q\phi) = 0, giving such a kk. This is impossible, so ϕ\phi is irrational.

Examiner Notes

最不受欢迎的纯数题(略少于Q7),平均分6/20。第(i)部分通常正确但推导过程常不充分。第(ii)部分超过半数考生止步于此,主要困难在于证明k必须为偶数。严重错误警示:部分考生引用π的无理性来证明(题目明确θ以度为单位,π的无理性与此无关)。能完成(ii)的考生通常也能完成(iii)。