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STEP3 2002 -- Pure Mathematics

Exam: STEP3  |  Year: 2002  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1微积分 CalculusChallenging换元积分,分部积分,旋转体体积公式,广义积分
2级数与数列 Sequences and SeriesHard数学归纳法,反正切加法公式,裂项相消,级数求和
3函数与方程 Functions and EquationsChallenging根式函数分析,函数图像描绘,不等式分析,代数方程求解
4数论 Number TheoryHard不等式放缩,反证法,因式分解,整数分析
5代数 AlgebraChallenging配方法,待定系数法,多项式恒等式,因式分解
6微分方程 Differential EquationsChallenging可分离变量法,分情况讨论,解曲线作图
7三角学与坐标几何 Trigonometry and Coordinate GeometryChallenging三角恒等式,坐标法,代数恒等变换,不等式放缩
8复数 Complex NumbersHard复数辐角计算,模的运算,几何解释,Ptolemy定理

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

1 Find the area of the region between the curve y=ln⁡xxy = \frac{\ln x}{x} and the xx-axis, for 1⩽x⩽a1 \leqslant x \leqslant a. What happens to this area as aa tends to infinity?

Find the volume of the solid obtained when the region between the curve y=ln⁡xxy = \frac{\ln x}{x} and the xx-axis, for 1⩽x⩽a1 \leqslant x \leqslant a, is rotated through 2π2\pi radians about the xx-axis. What happens to this volume as aa tends to infinity?

Model Solution

Part (i): Area

The area is

A=∫1aln⁡xx dx=[(ln⁡x)22]1a=(ln⁡a)22.A = \int_1^a \frac{\ln x}{x}\, dx = \left[\frac{(\ln x)^2}{2}\right]_1^a = \frac{(\ln a)^2}{2}.

As a→∞a \to \infty, ln⁡a→∞\ln a \to \infty, so A→∞A \to \infty. The area diverges.

Part (ii): Volume of revolution

The volume obtained by rotating about the xx-axis is

V=π∫1a(ln⁡xx)2dx=π∫1a(ln⁡x)2x2 dx.V = \pi \int_1^a \left(\frac{\ln x}{x}\right)^2 dx = \pi \int_1^a \frac{(\ln x)^2}{x^2}\, dx.

We evaluate this by parts. Let u=(ln⁡x)2u = (\ln x)^2, dv=x−2 dxdv = x^{-2}\, dx, so du=2ln⁡xx dxdu = \frac{2\ln x}{x}\, dx, v=−1xv = -\frac{1}{x}. Then

∫1a(ln⁡x)2x2 dx=[−(ln⁡x)2x]1a+∫1a2ln⁡xx2 dx=−(ln⁡a)2a+2∫1aln⁡xx2 dx.\int_1^a \frac{(\ln x)^2}{x^2}\, dx = \left[-\frac{(\ln x)^2}{x}\right]_1^a + \int_1^a \frac{2\ln x}{x^2}\, dx = -\frac{(\ln a)^2}{a} + 2\int_1^a \frac{\ln x}{x^2}\, dx.

For the remaining integral, let u=ln⁡xu = \ln x, dv=x−2 dxdv = x^{-2}\, dx, so du=1x dxdu = \frac{1}{x}\, dx, v=−1xv = -\frac{1}{x}:

∫1aln⁡xx2 dx=[−ln⁡xx]1a+∫1a1x2 dx=−ln⁡aa+[−1x]1a=−ln⁡aa+1−1a.\int_1^a \frac{\ln x}{x^2}\, dx = \left[-\frac{\ln x}{x}\right]_1^a + \int_1^a \frac{1}{x^2}\, dx = -\frac{\ln a}{a} + \left[-\frac{1}{x}\right]_1^a = -\frac{\ln a}{a} + 1 - \frac{1}{a}.

Combining:

∫1a(ln⁡x)2x2 dx=−(ln⁡a)2a−2ln⁡aa+2−2a=2−(ln⁡a)2+2ln⁡a+2a.\int_1^a \frac{(\ln x)^2}{x^2}\, dx = -\frac{(\ln a)^2}{a} - \frac{2\ln a}{a} + 2 - \frac{2}{a} = 2 - \frac{(\ln a)^2 + 2\ln a + 2}{a}.

Therefore

V=π[2−(ln⁡a)2+2ln⁡a+2a].V = \pi\left[2 - \frac{(\ln a)^2 + 2\ln a + 2}{a}\right].

As a→∞a \to \infty, the fraction (ln⁡a)2+2ln⁡a+2a→0\frac{(\ln a)^2 + 2\ln a + 2}{a} \to 0 (since polynomial growth of ln⁡a\ln a is slower than linear growth of aa), so V→2πV \to 2\pi.


Topic: 级数与数列 Sequences and Series  |  Difficulty: Hard  |  Marks: 20

2 Prove that arctan⁡a+arctan⁡b=arctan⁡(a+b1−ab)\arctan a + \arctan b = \arctan \left( \frac{a + b}{1 - ab} \right) when 0<a<10 < a < 1 and 0<b<10 < b < 1.

Prove by induction that, for n⩾1n \geqslant 1,

∑r=1narctan⁡(1r2+r+1)=arctan⁡(nn+2)\sum_{r=1}^{n} \arctan \left( \frac{1}{r^2 + r + 1} \right) = \arctan \left( \frac{n}{n + 2} \right)

and hence find

∑r=1∞arctan⁡(1r2+r+1).\sum_{r=1}^{\infty} \arctan \left( \frac{1}{r^2 + r + 1} \right) .

Hence prove that

∑r=1∞arctan⁡(1r2−r+1)=π2.\sum_{r=1}^{\infty} \arctan \left( \frac{1}{r^2 - r + 1} \right) = \frac{\pi}{2} .

Model Solution

Part (i): The addition formula

Let α=arctan⁡a\alpha = \arctan a and β=arctan⁡b\beta = \arctan b, so tan⁡α=a\tan\alpha = a and tan⁡β=b\tan\beta = b. Since 0<a<10 < a < 1 and 0<b<10 < b < 1, we have 0<α<π/40 < \alpha < \pi/4 and 0<β<π/40 < \beta < \pi/4, so 0<α+β<π/20 < \alpha + \beta < \pi/2.

Using the tangent addition formula:

tan⁡(α+β)=tan⁡α+tan⁡β1−tan⁡αtan⁡β=a+b1−ab.\tan(\alpha + \beta) = \frac{\tan\alpha + \tan\beta}{1 - \tan\alpha\tan\beta} = \frac{a + b}{1 - ab}.

Since 0<a,b<10 < a, b < 1, we have ab<1ab < 1, so 1−ab>01 - ab > 0 and a+b1−ab>0\frac{a+b}{1-ab} > 0. Also α+β∈(0,π/2)\alpha + \beta \in (0, \pi/2), so

α+β=arctan⁡(a+b1−ab).■\alpha + \beta = \arctan\left(\frac{a + b}{1 - ab}\right). \qquad \blacksquare

Part (ii): Induction proof

Base case (n=1n = 1): arctan⁡ ⁣(11+1+1)=arctan⁡ ⁣(13)=arctan⁡ ⁣(11+2)\arctan\!\left(\frac{1}{1+1+1}\right) = \arctan\!\left(\frac{1}{3}\right) = \arctan\!\left(\frac{1}{1+2}\right), as required.

Inductive step: Assume ∑r=1narctan⁡ ⁣(1r2+r+1)=arctan⁡ ⁣(nn+2)\sum_{r=1}^{n} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n}{n+2}\right). Then

∑r=1n+1arctan⁡ ⁣(1r2+r+1)=arctan⁡ ⁣(nn+2)+arctan⁡ ⁣(1(n+1)2+(n+1)+1).\sum_{r=1}^{n+1} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n}{n+2}\right) + \arctan\!\left(\frac{1}{(n+1)^2+(n+1)+1}\right).

We have (n+1)2+(n+1)+1=n2+3n+3(n+1)^2 + (n+1) + 1 = n^2 + 3n + 3, so we need to compute

arctan⁡ ⁣(nn+2)+arctan⁡ ⁣(1n2+3n+3).\arctan\!\left(\frac{n}{n+2}\right) + \arctan\!\left(\frac{1}{n^2+3n+3}\right).

Since 0<nn+2<10 < \frac{n}{n+2} < 1 and 0<1n2+3n+3<10 < \frac{1}{n^2+3n+3} < 1, we apply the addition formula:

nn+2+1n2+3n+31−n(n+2)(n2+3n+3)=n(n2+3n+3)+(n+2)(n+2)(n2+3n+3)−n.\frac{\frac{n}{n+2} + \frac{1}{n^2+3n+3}}{1 - \frac{n}{(n+2)(n^2+3n+3)}} = \frac{n(n^2+3n+3) + (n+2)}{(n+2)(n^2+3n+3) - n}.

Numerator: n3+3n2+3n+n+2=n3+3n2+4n+2n^3 + 3n^2 + 3n + n + 2 = n^3 + 3n^2 + 4n + 2.

Denominator: n3+3n2+3n+2n2+6n+6−n=n3+5n2+8n+6n^3 + 3n^2 + 3n + 2n^2 + 6n + 6 - n = n^3 + 5n^2 + 8n + 6.

We can verify that n3+3n2+4n+2n3+5n2+8n+6=n+1n+3\frac{n^3 + 3n^2 + 4n + 2}{n^3 + 5n^2 + 8n + 6} = \frac{n+1}{n+3} by cross-multiplying:

(n+1)(n3+5n2+8n+6)=n4+6n3+13n2+14n+6(n+1)(n^3 + 5n^2 + 8n + 6) = n^4 + 6n^3 + 13n^2 + 14n + 6.

(n+3)(n3+3n2+4n+2)=n4+6n3+13n2+14n+6(n+3)(n^3 + 3n^2 + 4n + 2) = n^4 + 6n^3 + 13n^2 + 14n + 6, as required.

Therefore ∑r=1n+1arctan⁡ ⁣(1r2+r+1)=arctan⁡ ⁣(n+1n+3)\sum_{r=1}^{n+1} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n+1}{n+3}\right), completing the induction. ■\qquad \blacksquare

Part (iii): The infinite sum

∑r=1∞arctan⁡ ⁣(1r2+r+1)=lim⁡n→∞arctan⁡ ⁣(nn+2)=arctan⁡(1)=π4.\sum_{r=1}^{\infty} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \lim_{n\to\infty} \arctan\!\left(\frac{n}{n+2}\right) = \arctan(1) = \frac{\pi}{4}.

Part (iv): The second identity

Note that 1r2−r+1=1(r−1)2+(r−1)+1\frac{1}{r^2 - r + 1} = \frac{1}{(r-1)^2 + (r-1) + 1}. Substituting s=r−1s = r - 1:

∑r=1∞arctan⁡ ⁣(1r2−r+1)=∑s=0∞arctan⁡ ⁣(1s2+s+1)=arctan⁡ ⁣(10+0+1)+∑s=1∞arctan⁡ ⁣(1s2+s+1)\sum_{r=1}^{\infty} \arctan\!\left(\frac{1}{r^2-r+1}\right) = \sum_{s=0}^{\infty} \arctan\!\left(\frac{1}{s^2+s+1}\right) = \arctan\!\left(\frac{1}{0+0+1}\right) + \sum_{s=1}^{\infty} \arctan\!\left(\frac{1}{s^2+s+1}\right)

=arctan⁡(1)+π4=π4+π4=π2.■= \arctan(1) + \frac{\pi}{4} = \frac{\pi}{4} + \frac{\pi}{4} = \frac{\pi}{2}. \qquad \blacksquare


Topic: 函数与方程 Functions and Equations  |  Difficulty: Challenging  |  Marks: 20

3 Let

f(x)=ax−x−b,f(x) = a\sqrt{x} - \sqrt{x - b} ,

where x⩾b>0x \geqslant b > 0 and a>1a > 1. Sketch the graph of f(x)f(x). Hence show that the equation f(x)=cf(x) = c, where c>0c > 0, has no solution when c2<b(a2−1)c^2 < b \left( a^2 - 1 \right). Find conditions on c2c^2 in terms of aa and bb for the equation to have exactly one or exactly two solutions.

Solve the equations (i) 3x−x−2=43\sqrt{x} - \sqrt{x - 2} = 4 and (ii) 3x−x−3=53\sqrt{x} - \sqrt{x - 3} = 5.

Model Solution

Part (i): Sketch and analysis

We have f(x)=ax−x−bf(x) = a\sqrt{x} - \sqrt{x-b} for x⩾b>0x \geqslant b > 0, a>1a > 1.

At x=bx = b: f(b)=abf(b) = a\sqrt{b}.

As x→∞x \to \infty: f(x)=x(a−1−b/x)→∞f(x) = \sqrt{x}(a - \sqrt{1 - b/x}) \to \infty since a>1a > 1.

Derivative:

f′(x)=a2x−12x−b=ax−b−x2xx−b.f'(x) = \frac{a}{2\sqrt{x}} - \frac{1}{2\sqrt{x-b}} = \frac{a\sqrt{x-b} - \sqrt{x}}{2\sqrt{x}\sqrt{x-b}}.

Setting f′(x)=0f'(x) = 0: ax−b=xa\sqrt{x-b} = \sqrt{x}, so a2(x−b)=xa^2(x-b) = x, giving x=a2ba2−1x = \frac{a^2 b}{a^2 - 1}.

Since a>1a > 1, we have a2a2−1>1\frac{a^2}{a^2-1} > 1, so xc=a2ba2−1>bx_c = \frac{a^2 b}{a^2-1} > b. This critical point lies in the domain.

For b⩽x<xcb \leqslant x < x_c: f′(x)<0f'(x) < 0 (decreasing). For x>xcx > x_c: f′(x)>0f'(x) > 0 (increasing).

The minimum value is

f(xc)=aa2ba2−1−a2ba2−1−b=a2ba2−1−ba2−1=(a2−1)ba2−1=b(a2−1).f(x_c) = a\sqrt{\frac{a^2 b}{a^2-1}} - \sqrt{\frac{a^2 b}{a^2-1} - b} = \frac{a^2\sqrt{b}}{\sqrt{a^2-1}} - \frac{\sqrt{b}}{\sqrt{a^2-1}} = \frac{(a^2-1)\sqrt{b}}{\sqrt{a^2-1}} = \sqrt{b(a^2-1)}.

The graph starts at (b,ab)(b, a\sqrt{b}), decreases to a minimum at xcx_c with value b(a2−1)\sqrt{b(a^2-1)}, then increases to infinity.

Part (ii): Conditions on cc

The equation f(x)=cf(x) = c with c>0c > 0:

  • No solution when c<b(a2−1)c < \sqrt{b(a^2-1)}, i.e. c2<b(a2−1)c^2 < b(a^2-1).
  • Exactly one solution when c=b(a2−1)c = \sqrt{b(a^2-1)} (at the minimum).
  • Exactly two solutions when b(a2−1)<c≤ab\sqrt{b(a^2-1)} < c \leq a\sqrt{b}, i.e. b(a2−1)<c2≤a2bb(a^2-1) < c^2 \leq a^2 b. At the endpoint c=abc=a\sqrt b, the two solutions are x=bx=b and a second point on the increasing branch.
  • Exactly one solution when c>abc > a\sqrt{b}, i.e. c2>a2bc^2 > a^2 b.

Part (iii): Solving (i) 3x−x−2=43\sqrt{x} - \sqrt{x-2} = 4

Here a=3a = 3, b=2b = 2, c=4c = 4. We have f(2)=32≈4.24f(2) = 3\sqrt{2} \approx 4.24 and b(a2−1)=16=4\sqrt{b(a^2-1)} = \sqrt{16} = 4.

Since c=4=b(a2−1)c = 4 = \sqrt{b(a^2-1)}, the equation has exactly one solution (at the minimum).

Rearranging: 3x=4+x−23\sqrt{x} = 4 + \sqrt{x-2}. Squaring:

9x=16+8x−2+x−2  ⟹  8x−14=8x−2  ⟹  4x−7=4x−2.9x = 16 + 8\sqrt{x-2} + x - 2 \implies 8x - 14 = 8\sqrt{x-2} \implies 4x - 7 = 4\sqrt{x-2}.

Squaring again: 16x2−56x+49=16(x−2)=16x−3216x^2 - 56x + 49 = 16(x-2) = 16x - 32, so 16x2−72x+81=016x^2 - 72x + 81 = 0.

Discriminant: 722−4(16)(81)=5184−5184=072^2 - 4(16)(81) = 5184 - 5184 = 0, so x=7232=94x = \frac{72}{32} = \frac{9}{4}.

Substitution confirms 39/4−9/4−2=3⋅32−14=92−12=43\sqrt{9/4} - \sqrt{9/4 - 2} = 3 \cdot \frac{3}{2} - \sqrt{\frac{1}{4}} = \frac{9}{2} - \frac{1}{2} = 4.

The unique solution is x=94x = \dfrac{9}{4}.

Part (iv): Solving (ii) 3x−x−3=53\sqrt{x} - \sqrt{x-3} = 5

Here a=3a = 3, b=3b = 3, c=5c = 5. We have f(3)=33≈5.20f(3) = 3\sqrt{3} \approx 5.20 and b(a2−1)=24=26≈4.90\sqrt{b(a^2-1)} = \sqrt{24} = 2\sqrt{6} \approx 4.90.

Since 26<5<332\sqrt{6} < 5 < 3\sqrt{3}, the equation has exactly two solutions.

Rearranging: 3x=5+x−33\sqrt{x} = 5 + \sqrt{x-3}. Squaring:

9x=25+10x−3+x−3  ⟹  8x−22=10x−3  ⟹  4x−11=5x−3.9x = 25 + 10\sqrt{x-3} + x - 3 \implies 8x - 22 = 10\sqrt{x-3} \implies 4x - 11 = 5\sqrt{x-3}.

Note: we need 4x−11⩾04x - 11 \geqslant 0, i.e. x⩾11/4x \geqslant 11/4.

Squaring again: 16x2−88x+121=25(x−3)=25x−7516x^2 - 88x + 121 = 25(x-3) = 25x - 75, so 16x2−113x+196=016x^2 - 113x + 196 = 0.

Discriminant: 1132−4(16)(196)=12769−12544=225=152113^2 - 4(16)(196) = 12769 - 12544 = 225 = 15^2.

x=113±1532  ⟹  x=4orx=4916.x = \frac{113 \pm 15}{32} \implies x = 4 \quad \text{or} \quad x = \frac{49}{16}.

Substitution gives 34−1=6−1=53\sqrt{4} - \sqrt{1} = 6 - 1 = 5.

Similarly, 349/16−49/16−3=214−116=214−14=53\sqrt{49/16} - \sqrt{49/16 - 3} = \frac{21}{4} - \sqrt{\frac{1}{16}} = \frac{21}{4} - \frac{1}{4} = 5.

The solutions are x=4916x = \dfrac{49}{16} and x=4x = 4.


Topic: 数论 Number Theory  |  Difficulty: Hard  |  Marks: 20

4 Show that if xx and yy are positive and x3+x2=y3−y2x^3 + x^2 = y^3 - y^2 then x<yx < y.

Show further that if 0<x⩽y−10 < x \leqslant y - 1, then x3+x2<y3−y2x^3 + x^2 < y^3 - y^2.

Prove that there does not exist a pair of positive integers such that the difference of their cubes is equal to the sum of their squares.

Find all the pairs of integers such that the difference of their cubes is equal to the sum of their squares.

Model Solution

Part (i): Show that x<yx < y

Suppose for contradiction that x⩾yx \geqslant y. If x=yx = y, then x3+x2=x3−x2x^3 + x^2 = x^3 - x^2, giving 2x2=02x^2 = 0, so x=0x = 0, contradicting x>0x > 0.

If x>y>0x > y > 0, then x3>y3x^3 > y^3 and x2>y2x^2 > y^2, so x3+x2>y3+y2>y3−y2x^3 + x^2 > y^3 + y^2 > y^3 - y^2 (since y2>0y^2 > 0). This contradicts x3+x2=y3−y2x^3 + x^2 = y^3 - y^2.

Therefore x<yx < y. ■\qquad \blacksquare

Part (ii): Show that 0<x⩽y−10 < x \leqslant y-1 implies x3+x2<y3−y2x^3 + x^2 < y^3 - y^2

Since x⩽y−1x \leqslant y - 1, we have x+1⩽yx + 1 \leqslant y, so

x3+x2=x2(x+1)⩽x2y.x^3 + x^2 = x^2(x+1) \leqslant x^2 y.

Also y3−y2=y2(y−1)⩾y2xy^3 - y^2 = y^2(y-1) \geqslant y^2 x (since y−1⩾xy - 1 \geqslant x).

So x3+x2⩽x2yx^3 + x^2 \leqslant x^2 y and y3−y2⩾xy2y^3 - y^2 \geqslant xy^2. We need x2y<xy2x^2 y < xy^2, i.e. xy(y−x)>0xy(y - x) > 0, which holds since x,y>0x, y > 0 and y>xy > x.

But we need strict inequality throughout. Since x⩽y−1x \leqslant y-1 and x>0x > 0, we have y>1y > 1, so y−1>0y - 1 > 0. Also x<yx < y (from Part (i) or directly from x⩽y−1x \leqslant y-1).

More precisely: x2(x+1)⩽x2yx^2(x+1) \leqslant x^2 y with equality iff x+1=yx + 1 = y. And y2(y−1)⩾xy2y^2(y-1) \geqslant xy^2 with equality iff x=y−1x = y - 1. Even if x=y−1x = y - 1, we get x2yx^2 y vs xy2xy^2, and x2y<xy2x^2 y < xy^2 since x<yx < y. Therefore x3+x2<y3−y2x^3 + x^2 < y^3 - y^2. ■\qquad \blacksquare

Part (iii): No pair of positive integers

Suppose m,nm, n are positive integers with m3−n3=m2+n2m^3 - n^3 = m^2 + n^2. Since m3−n3=(m−n)(m2+mn+n2)>0m^3 - n^3 = (m-n)(m^2 + mn + n^2) > 0 and m2+n2>0m^2 + n^2 > 0, we need m>nm > n, so m⩾n+1m \geqslant n + 1.

Setting x=nx = n and y=my = m in Part (ii): since 0<n⩽m−10 < n \leqslant m - 1, we have n3+n2<m3−m2n^3 + n^2 < m^3 - m^2.

But we need m3−n3=m2+n2m^3 - n^3 = m^2 + n^2, i.e. n3+n2=m3−m2n^3 + n^2 = m^3 - m^2. This contradicts n3+n2<m3−m2n^3 + n^2 < m^3 - m^2.

Therefore no such pair exists. ■\qquad \blacksquare

Part (iv): Find all integer pairs

The equation is y3−x3=y2+x2y^3 - x^3 = y^2 + x^2, i.e. y3−y2=x3+x2y^3 - y^2 = x^3 + x^2, which gives

(y−x)(y2+xy+x2)=x2+y2.(⋆)(y - x)(y^2 + xy + x^2) = x^2 + y^2. \qquad (\star)

Case 1: x=0x = 0. Then y3=y2y^3 = y^2, so y=0y = 0 or y=1y = 1. Solutions: (0,0)(0, 0) and (0,1)(0, 1).

Case 2: y=0y = 0. Then −x3=x2-x^3 = x^2, so x=0x = 0 or x=−1x = -1. Solution: (−1,0)(-1, 0).

Case 3: x>0x > 0. If y<0y<0, then y3−x3<0y^3-x^3<0 while x2+y2>0x^2+y^2>0, which is impossible. If y>0y>0, Part (iii) shows that no positive integer pair exists.

Case 4: x<0x < 0, y>0y > 0. Let x=−px = -p with p⩾1p \geqslant 1. Then (⋆)(\star) becomes

(y+p)(y2−py+p2)=p2+y2.(y + p)(y^2 - py + p^2) = p^2 + y^2.

The left side equals y3+p3y^3+p^3. For p≥2p\geq2 and y≥2y\geq2, we have p3>p2p^3>p^2 and y3>y2y^3>y^2, so p3+y3>p2+y2p^3+y^3>p^2+y^2. Thus only the cases with p=1p=1 or y=1y=1 can remain.

p=1,y=1p = 1, y = 1: (1+1)(1−1+1)=2(1+1)(1-1+1) = 2 and 1+1=21 + 1 = 2. This gives the solution (−1,1)(-1,1).

p=1,y⩾2p = 1, y \geqslant 2: (y+1)(y2−y+1)=y3+1>y2+1(y+1)(y^2 - y + 1) = y^3 + 1 > y^2 + 1. No solution.

p=2,y=1p = 2, y = 1: (3)(4−2+1)=9(3)(4-2+1) = 9 and 4+1=54 + 1 = 5. No solution.

p⩾2,y=1p \geqslant 2, y = 1: (1+p)(1−p+p2)=1+p3⩾9>p2+1(1+p)(1-p+p^2) = 1 + p^3 \geqslant 9 > p^2 + 1. No solution.

Case 5: x<0x < 0, y<0y < 0. Let x=−p,y=−qx = -p, y = -q with p,q⩾1p, q \geqslant 1. Then

(−q+p)(q2−pq+p2)=p2+q2,i.e.(p−q)(p2−pq+q2)=p2+q2.(-q+p)(q^2 - pq + p^2) = p^2 + q^2, \quad \text{i.e.} \quad (p-q)(p^2 - pq + q^2) = p^2 + q^2.

This is p3−q3=p2+q2p^3 - q^3 = p^2 + q^2. If p=qp = q: 0=2p20 = 2p^2, impossible. If p>qp > q: by Part (iii) applied to positive integers q,pq, p with p3−q3=p2+q2p^3 - q^3 = p^2 + q^2, no solution exists (same argument). If p<qp < q: left side is negative, right side is positive. No solution.

Case 6: x<0x < 0, y=0y = 0. Already covered in Case 2.

Therefore the complete set of integer solutions is

(x,y)∈{(0,0), (0,1), (−1,0), (−1,1)}.(x, y) \in \{(0, 0),\ (0, 1),\ (-1, 0),\ (-1, 1)\}.


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

5 Give a condition that must be satisfied by pp, qq and rr for it to be possible to write the quadratic polynomial px2+qx+rpx^2 + qx + r in the form p(x+h)2p(x + h)^2, for some hh.

Obtain an equation, which you need not simplify, that must be satisfied by tt if it is possible to write (x2+12bx+t)2−(x4+bx3+cx2+dx+e)\left(x^2 + \frac{1}{2}bx + t\right)^2 - \left(x^4 + bx^3 + cx^2 + dx + e\right) in the form k(x+h)2k(x + h)^2, for some kk and hh.

Hence, or otherwise, write x4+6x3+9x2−2x−7x^4 + 6x^3 + 9x^2 - 2x - 7 as a product of two quadratic factors.

Model Solution

Part (i): Condition for px2+qx+r=p(x+h)2px^2 + qx + r = p(x+h)^2

Expanding: p(x+h)2=px2+2phx+ph2p(x+h)^2 = px^2 + 2phx + ph^2. Comparing coefficients with px2+qx+rpx^2 + qx + r:

q=2ph,r=ph2.q = 2ph, \qquad r = ph^2.

From the first equation h=q/(2p)h = q/(2p), so r=p⋅q2/(4p2)=q2/(4p)r = p \cdot q^2/(4p^2) = q^2/(4p).

The necessary and sufficient condition is q2=4prq^2 = 4pr, i.e. the discriminant is zero. ■\qquad \blacksquare

Part (ii): Equation for tt

We want

(x2+12bx+t)2−(x4+bx3+cx2+dx+e)=k(x+h)2.\left(x^2 + \tfrac{1}{2}bx + t\right)^2 - \left(x^4 + bx^3 + cx^2 + dx + e\right) = k(x+h)^2.

The left side must be a perfect square (as a quadratic in xx). Expanding the square:

(x2+12bx+t)2=x4+bx3+(14b2+2t)x2+btx+t2.\left(x^2 + \tfrac{1}{2}bx + t\right)^2 = x^4 + bx^3 + \left(\tfrac{1}{4}b^2 + 2t\right)x^2 + btx + t^2.

Subtracting:

(14b2+2t−c)x2+(bt−d)x+(t2−e)=k(x+h)2.\left(\tfrac{1}{4}b^2 + 2t - c\right)x^2 + (bt - d)x + (t^2 - e) = k(x+h)^2.

From Part (i), the condition for this quadratic Ax2+Bx+CAx^2 + Bx + C to be a perfect square is B2=4ACB^2 = 4AC:

(bt−d)2=4(14b2+2t−c)(t2−e).■(bt - d)^2 = 4\left(\tfrac{1}{4}b^2 + 2t - c\right)(t^2 - e). \qquad \blacksquare

Part (iii): Factorizing x4+6x3+9x2−2x−7x^4 + 6x^3 + 9x^2 - 2x - 7

Here b=6b = 6, c=9c = 9, d=−2d = -2, e=−7e = -7. The condition becomes

(6t+2)2=4(9+2t−9)(t2+7)=4⋅2t⋅(t2+7).(6t + 2)^2 = 4(9 + 2t - 9)(t^2 + 7) = 4 \cdot 2t \cdot (t^2 + 7).

Simplifying: (3t+1)2=2t(t2+7)(3t+1)^2 = 2t(t^2 + 7), i.e. 9t2+6t+1=2t3+14t9t^2 + 6t + 1 = 2t^3 + 14t.

2t3−9t2+8t−1=0.2t^3 - 9t^2 + 8t - 1 = 0.

Testing t=1t = 1 gives 2−9+8−1=02 - 9 + 8 - 1 = 0, so we may take t=1t = 1. Then

(x2+3x+1)2−(x4+6x3+9x2−2x−7)=2x2+8x+8=2(x+2)2.\left(x^2 + 3x + 1\right)^2 - \left(x^4 + 6x^3 + 9x^2 - 2x - 7\right) = 2x^2 + 8x + 8 = 2(x+2)^2.

Therefore

x4+6x3+9x2−2x−7=(x2+3x+1)2−(2(x+2))2.x^4 + 6x^3 + 9x^2 - 2x - 7 = \left(x^2 + 3x + 1\right)^2 - \left(\sqrt{2}(x+2)\right)^2.

Using the difference of two squares:

x4+6x3+9x2−2x−7=(x2+(3−2)x+1−22)(x2+(3+2)x+1+22).x^4 + 6x^3 + 9x^2 - 2x - 7 = \left(x^2 + (3-\sqrt{2})x + 1 - 2\sqrt{2}\right)\left(x^2 + (3+\sqrt{2})x + 1 + 2\sqrt{2}\right).

Verification: The xx coefficient is (3−2)(1+22)+(3+2)(1−22)(3-\sqrt{2})(1+2\sqrt{2}) + (3+\sqrt{2})(1-2\sqrt{2}).

(3−2)(1+22)=3+62−2−4=−1+52(3-\sqrt{2})(1+2\sqrt{2}) = 3 + 6\sqrt{2} - \sqrt{2} - 4 = -1 + 5\sqrt{2}.

(3+2)(1−22)=3−62+2−4=−1−52(3+\sqrt{2})(1-2\sqrt{2}) = 3 - 6\sqrt{2} + \sqrt{2} - 4 = -1 - 5\sqrt{2}.

Sum =−2= -2, as required.

The constant term is (1−22)(1+22)=1−8=−7(1-2\sqrt{2})(1+2\sqrt{2}) = 1 - 8 = -7.


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

6 Find all the solution curves of the differential equation y4(dydx)4=(y2−1)2y^4 \left(\frac{dy}{dx}\right)^4 = \left(y^2 - 1\right)^2 that pass through either of the points (i) (0,32)\left(0, \frac{\sqrt{3}}{2}\right), (ii) (0,52)\left(0, \frac{\sqrt{5}}{2}\right).

Show also that y=1y = 1 and y=−1y = -1 are solutions of the differential equation. Sketch all these solution curves on a single set of axes.

Model Solution

Part (i): Solving the differential equation

The equation y4(dydx)4=(y2−1)2y^4\left(\frac{dy}{dx}\right)^4 = (y^2-1)^2 can be written as (ydydx)4=(y2−1)2\left(y\frac{dy}{dx}\right)^4 = (y^2-1)^2.

Taking square roots (both sides are non-negative): (ydydx)2=∣y2−1∣\left(y\frac{dy}{dx}\right)^2 = |y^2 - 1|.

So ydydx=±∣y2−1∣y\frac{dy}{dx} = \pm\sqrt{|y^2-1|}, which gives four ODEs depending on the signs.

Case A: ∣y∣>1|y| > 1 (so y2−1>0y^2 - 1 > 0)

ydydx=±y2−1y\frac{dy}{dx} = \pm\sqrt{y^2-1}, i.e. yy2−1 dy=± dx\frac{y}{\sqrt{y^2-1}}\, dy = \pm\, dx.

Integrating: y2−1=±x+C\sqrt{y^2-1} = \pm x + C, so

y2=(x−C)2+1(choosing appropriate sign).(⋆)y^2 = (x - C)^2 + 1 \qquad \text{(choosing appropriate sign)}. \qquad (\star)

Case B: ∣y∣<1|y| < 1 (so 1−y2>01 - y^2 > 0)

ydydx=±1−y2y\frac{dy}{dx} = \pm\sqrt{1-y^2}, i.e. y1−y2 dy=± dx\frac{y}{\sqrt{1-y^2}}\, dy = \pm\, dx.

Integrating: −1−y2=±x+C-\sqrt{1-y^2} = \pm x + C, so 1−y2=∓x+C′\sqrt{1-y^2} = \mp x + C', giving

y2=1−(x−C)2.(⋆⋆)y^2 = 1 - (x - C)^2. \qquad (\star\star)

Solution curves through (0,3/2)(0, \sqrt{3}/2)

Since y=3/2<1y = \sqrt{3}/2 < 1, we use Case B. From (⋆⋆)(\star\star): 34=1−C2\frac{3}{4} = 1 - C^2, so C=±12C = \pm\frac{1}{2}.

This gives two circles:

(x−12)2+y2=1and(x+12)2+y2=1.\left(x - \tfrac{1}{2}\right)^2 + y^2 = 1 \qquad \text{and} \qquad \left(x + \tfrac{1}{2}\right)^2 + y^2 = 1.

Both are valid solution curves (the upper semicircles satisfy the ODE with y>0y > 0).

Solution curves through (0,5/2)(0, \sqrt{5}/2)

Since y=5/2>1y = \sqrt{5}/2 > 1, we use Case A. From (⋆)(\star): 54=C2+1\frac{5}{4} = C^2 + 1, so C=±12C = \pm\frac{1}{2}.

This gives two hyperbolas:

y2−(x−12)2=1andy2−(x+12)2=1.y^2 - \left(x - \tfrac{1}{2}\right)^2 = 1 \qquad \text{and} \qquad y^2 - \left(x + \tfrac{1}{2}\right)^2 = 1.

Part (ii): Constant solutions

If y=1y = 1, then the left side is 1⋅0=01 \cdot 0 = 0 and the right side is 00.

If y=−1y = -1, then the left side is 1⋅0=01 \cdot 0 = 0 and the right side is 00.

Part (iii): Sketch

The solution curves are:

  • Two circles: (x±12)2+y2=1\left(x \pm \frac{1}{2}\right)^2 + y^2 = 1 (valid for ∣y∣<1|y| < 1)
  • Two hyperbolas: y2−(x±12)2=1y^2 - \left(x \pm \frac{1}{2}\right)^2 = 1 (valid for ∣y∣>1|y| > 1)
  • Two horizontal lines: y=1y = 1 and y=−1y = -1

The circles are centred at (±1/2,0)(\pm 1/2, 0) with radius 1, fitting within the strip ∣y∣<1|y| < 1. The hyperbolas have vertices at (±1/2,±1)(\pm 1/2, \pm 1) and open vertically, with slant asymptotes y=±(x−12)y = \pm(x-\frac12) and y=±(x+12)y = \pm(x+\frac12) as appropriate. The horizontal lines y=±1y = \pm1 are constant solution curves and boundary levels touched at the vertices, not asymptotes.

The curve through (0,3/2)(0, \sqrt{3}/2) consists of the upper arcs of both circles. The curve through (0,5/2)(0, \sqrt{5}/2) consists of the upper branches of both hyperbolas.


Topic: 三角学与坐标几何 Trigonometry and Coordinate Geometry  |  Difficulty: Challenging  |  Marks: 20

7 Given that α\alpha and β\beta are acute angles, show that α+β=π/2\alpha + \beta = \pi/2 if and only if cos⁡2α+cos⁡2β=1\cos^2 \alpha + \cos^2 \beta = 1.

In the xx–yy plane, the point AA has coordinates (0,s)(0, s) and the point CC has coordinates (s,0)(s, 0), where s>0s > 0. The point BB lies in the first quadrant (x>0,y>0x > 0, y > 0). The lengths of ABAB, OBOB and CBCB are respectively a,ba, b and cc.

Show that

(s2+b2−a2)2+(s2+b2−c2)2=4s2b2(s^2 + b^2 - a^2)^2 + (s^2 + b^2 - c^2)^2 = 4s^2b^2

and hence that

(2s2−a2−c2)2+(2b2−a2−c2)2=4a2c2.(2s^2 - a^2 - c^2)^2 + (2b^2 - a^2 - c^2)^2 = 4a^2c^2 .

Deduce that

(a−c)2⩽2b2⩽(a+c)2.(a - c)^2 \leqslant 2b^2 \leqslant (a + c)^2 .

Model Solution

Part (i): α+β=π/2\alpha + \beta = \pi/2 if and only if cos⁡2α+cos⁡2β=1\cos^2\alpha + \cos^2\beta = 1

Forward direction. Suppose α+β=π/2\alpha + \beta = \pi/2. Then β=π/2−α\beta = \pi/2 - \alpha, so

cos⁡β=cos⁡ ⁣(π2−α)=sin⁡α.\cos\beta = \cos\!\left(\frac{\pi}{2} - \alpha\right) = \sin\alpha.

Since α\alpha is acute, both sin⁡α\sin\alpha and cos⁡α\cos\alpha are non-negative, so cos⁡2β=sin⁡2α\cos^2\beta = \sin^2\alpha. Therefore

cos⁡2α+cos⁡2β=cos⁡2α+sin⁡2α=1.\cos^2\alpha + \cos^2\beta = \cos^2\alpha + \sin^2\alpha = 1.

Reverse direction. Suppose cos⁡2α+cos⁡2β=1\cos^2\alpha + \cos^2\beta = 1. Using cos⁡2α=1−sin⁡2α\cos^2\alpha = 1 - \sin^2\alpha, we get sin⁡2α+cos⁡2β=1\sin^2\alpha + \cos^2\beta = 1, so cos⁡2β=sin⁡2α\cos^2\beta = \sin^2\alpha.

Since α\alpha and β\beta are acute, cos⁡β>0\cos\beta > 0 and sin⁡α>0\sin\alpha > 0, so cos⁡β=sin⁡α=cos⁡(π/2−α)\cos\beta = \sin\alpha = \cos(\pi/2 - \alpha). Since cos⁡\cos is strictly decreasing on [0,π][0, \pi] and both β\beta and π/2−α\pi/2 - \alpha lie in (0,π/2)(0, \pi/2), we conclude β=π/2−α\beta = \pi/2 - \alpha, i.e. α+β=π/2\alpha + \beta = \pi/2. ■\qquad \blacksquare

Part (ii): The first identity

Let B=(x,y)B = (x, y) with x>0,y>0x > 0, y > 0. Let θ=∠BOx\theta = \angle BOx, so x=bcos⁡θx = b\cos\theta and y=bsin⁡θy = b\sin\theta.

Using A=(0,s)A = (0, s), C=(s,0)C = (s, 0), O=(0,0)O = (0, 0):

a2=∣AB∣2=x2+(y−s)2=x2+y2−2sy+s2=b2+s2−2sbsin⁡θa^2 = |AB|^2 = x^2 + (y - s)^2 = x^2 + y^2 - 2sy + s^2 = b^2 + s^2 - 2sb\sin\theta

c2=∣CB∣2=(x−s)2+y2=x2−2sx+s2+y2=b2+s2−2sbcos⁡θc^2 = |CB|^2 = (x - s)^2 + y^2 = x^2 - 2sx + s^2 + y^2 = b^2 + s^2 - 2sb\cos\theta

Therefore

s2+b2−a2=2sbsin⁡θ,s2+b2−c2=2sbcos⁡θ.s^2 + b^2 - a^2 = 2sb\sin\theta, \qquad s^2 + b^2 - c^2 = 2sb\cos\theta.

Squaring and adding:

(s2+b2−a2)2+(s2+b2−c2)2=4s2b2sin⁡2θ+4s2b2cos⁡2θ=4s2b2.■(s^2 + b^2 - a^2)^2 + (s^2 + b^2 - c^2)^2 = 4s^2b^2\sin^2\theta + 4s^2b^2\cos^2\theta = 4s^2b^2. \qquad \blacksquare

Part (iii): The second identity

From Part (ii), a2=s2+b2−2sbsin⁡θa^2 = s^2 + b^2 - 2sb\sin\theta and c2=s2+b2−2sbcos⁡θc^2 = s^2 + b^2 - 2sb\cos\theta, so

a2+c2=2(s2+b2)−2sb(sin⁡θ+cos⁡θ).a^2 + c^2 = 2(s^2 + b^2) - 2sb(\sin\theta + \cos\theta).

Hence

2s2−a2−c2=2s2−2(s2+b2)+2sb(sin⁡θ+cos⁡θ)=2sb(sin⁡θ+cos⁡θ)−2b22s^2 - a^2 - c^2 = 2s^2 - 2(s^2 + b^2) + 2sb(\sin\theta + \cos\theta) = 2sb(\sin\theta + \cos\theta) - 2b^2

2b2−a2−c2=2b2−2(s2+b2)+2sb(sin⁡θ+cos⁡θ)=2sb(sin⁡θ+cos⁡θ)−2s2.2b^2 - a^2 - c^2 = 2b^2 - 2(s^2 + b^2) + 2sb(\sin\theta + \cos\theta) = 2sb(\sin\theta + \cos\theta) - 2s^2.

Let u=a2+c2u = a^2 + c^2, m=s2+b2m = s^2 + b^2 and w=sin⁡θ+cos⁡θw = \sin\theta + \cos\theta. Then

(2s2−u)2+(2b2−u)2=(2s2−a2−c2)2+(2b2−a2−c2)2(2s^2 - u)^2 + (2b^2 - u)^2 = (2s^2 - a^2 - c^2)^2 + (2b^2 - a^2 - c^2)^2

=[2s2−2m+2sbw]2+[2b2−2m+2sbw]2= [2s^2 - 2m + 2sbw]^2 + [2b^2 - 2m + 2sbw]^2

=[−2b2+2sbw]2+[−2s2+2sbw]2= [-2b^2 + 2sbw]^2 + [-2s^2 + 2sbw]^2

=4b2(sw−b)2+4s2(bw−s)2= 4b^2(sw - b)^2 + 4s^2(bw - s)^2

=4[b2(s2w2−2bsw+b2)+s2(b2w2−2bsw+s2)]= 4[b^2(s^2w^2 - 2bsw + b^2) + s^2(b^2w^2 - 2bsw + s^2)]

=4[s2b2w2−2b3sw+b4+s2b2w2−2s3bw+s4]= 4[s^2b^2w^2 - 2b^3sw + b^4 + s^2b^2w^2 - 2s^3bw + s^4]

=4[2s2b2w2−2sbw(b2+s2)+s4+b4]= 4[2s^2b^2w^2 - 2sbw(b^2 + s^2) + s^4 + b^4]

=4[2s2b2w2−2sbwm+m2−2s2b2]= 4[2s^2b^2w^2 - 2sbwm + m^2 - 2s^2b^2]

Now 4a2c2=4[m2−2sbmw+4s2b2sin⁡θcos⁡θ]4a^2c^2 = 4[m^2 - 2sbmw + 4s^2b^2\sin\theta\cos\theta].

But w2−1=(sin⁡θ+cos⁡θ)2−1=2sin⁡θcos⁡θw^2 - 1 = (\sin\theta + \cos\theta)^2 - 1 = 2\sin\theta\cos\theta, so

2s2b2w2−2s2b2=4s2b2sin⁡θcos⁡θ.2s^2b^2w^2 - 2s^2b^2 = 4s^2b^2\sin\theta\cos\theta.

Thus

(2s2−a2−c2)2+(2b2−a2−c2)2=4a2c2.■(2s^2 - a^2 - c^2)^2 + (2b^2 - a^2 - c^2)^2 = 4a^2c^2. \qquad \blacksquare

Part (iv): The deduction

From Part (iii), rearranging: (2b2−a2−c2)2=4a2c2−(2s2−a2−c2)2(2b^2 - a^2 - c^2)^2 = 4a^2c^2 - (2s^2 - a^2 - c^2)^2.

Since (2s2−a2−c2)2⩾0(2s^2 - a^2 - c^2)^2 \geqslant 0, we have

(2b2−a2−c2)2⩽4a2c2,(2b^2 - a^2 - c^2)^2 \leqslant 4a^2c^2,

so ∣2b2−a2−c2∣⩽2ac|2b^2 - a^2 - c^2| \leqslant 2ac. This gives

−2ac⩽2b2−a2−c2⩽2ac.-2ac \leqslant 2b^2 - a^2 - c^2 \leqslant 2ac.

Adding a2+c2a^2 + c^2 throughout: a2+c2−2ac⩽2b2⩽a2+c2+2aca^2 + c^2 - 2ac \leqslant 2b^2 \leqslant a^2 + c^2 + 2ac, i.e.

(a−c)2⩽2b2⩽(a+c)2.■(a - c)^2 \leqslant 2b^2 \leqslant (a + c)^2. \qquad \blacksquare


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

8 Four complex numbers u1,u2,u3u_1, u_2, u_3 and u4u_4 have unit modulus, and arguments θ1,θ2,θ3\theta_1, \theta_2, \theta_3 and θ4\theta_4, respectively, with −π<θ1<θ2<θ3<θ4<π-\pi < \theta_1 < \theta_2 < \theta_3 < \theta_4 < \pi.

Show that

arg⁡(u1−u2)=12(θ1+θ2−π)+2nπ\arg (u_1 - u_2) = \frac{1}{2} (\theta_1 + \theta_2 - \pi) + 2n\pi

where n=0n = 0 or 11. Deduce that

arg⁡((u1−u2)(u4−u3))=arg⁡((u1−u4)(u3−u2))+2nπ\arg ((u_1 - u_2) (u_4 - u_3)) = \arg ((u_1 - u_4) (u_3 - u_2)) + 2n\pi

for some integer nn.

Prove that

∣(u1−u2)(u4−u3)∣+∣(u1−u4)(u3−u2)∣=∣(u1−u3)(u4−u2)∣.| (u_1 - u_2) (u_4 - u_3) | + | (u_1 - u_4) (u_3 - u_2) | = | (u_1 - u_3) (u_4 - u_2) | .

Model Solution

Part (i): Argument of u1−u2u_1 - u_2

Write uk=eiθku_k = e^{i\theta_k}. Then

u1−u2=eiθ1−eiθ2=ei(θ1+θ2)/2(ei(θ1−θ2)/2−e−i(θ1−θ2)/2)=2isin⁡ ⁣(θ1−θ22)ei(θ1+θ2)/2.u_1 - u_2 = e^{i\theta_1} - e^{i\theta_2} = e^{i(\theta_1+\theta_2)/2}\left(e^{i(\theta_1-\theta_2)/2} - e^{-i(\theta_1-\theta_2)/2}\right) = 2i\sin\!\left(\frac{\theta_1-\theta_2}{2}\right)e^{i(\theta_1+\theta_2)/2}.

Let α=θ1−θ22\alpha = \frac{\theta_1-\theta_2}{2}. Since θ1<θ2\theta_1 < \theta_2, we have α<0\alpha < 0 and therefore sin⁡α<0\sin\alpha < 0. Hence 2isin⁡α2i\sin\alpha has argument −π/2-\pi/2 modulo 2π2\pi. Thus

arg⁡(u1−u2)=θ1+θ22+3π2=θ1+θ22−π2(mod2π).\arg(u_1 - u_2) = \frac{\theta_1+\theta_2}{2} + \frac{3\pi}{2} = \frac{\theta_1+\theta_2}{2} - \frac{\pi}{2} \pmod{2\pi}.

Since θ1+θ2−π2\frac{\theta_1+\theta_2-\pi}{2} is equivalent to θ1+θ22−π2\frac{\theta_1+\theta_2}{2} - \frac{\pi}{2}, we have

arg⁡(u1−u2)=12(θ1+θ2−π)+2nπ,n=0 or 1.■\arg(u_1 - u_2) = \frac{1}{2}(\theta_1 + \theta_2 - \pi) + 2n\pi, \qquad n = 0 \text{ or } 1. \qquad \blacksquare

Part (ii): Argument of products

Using the result from Part (i):

arg⁡(u1−u2)=θ1+θ2−π2,arg⁡(u4−u3)=θ3+θ4−π2,\arg(u_1 - u_2) = \frac{\theta_1+\theta_2-\pi}{2}, \qquad \arg(u_4 - u_3) = \frac{\theta_3+\theta_4-\pi}{2},

arg⁡(u1−u4)=θ1+θ4−π2,arg⁡(u3−u2)=θ2+θ3−π2.\arg(u_1 - u_4) = \frac{\theta_1+\theta_4-\pi}{2}, \qquad \arg(u_3 - u_2) = \frac{\theta_2+\theta_3-\pi}{2}.

Therefore

arg⁡((u1−u2)(u4−u3))=θ1+θ2+θ3+θ4−2π2(mod2π),\arg((u_1-u_2)(u_4-u_3)) = \frac{\theta_1+\theta_2+\theta_3+\theta_4 - 2\pi}{2} \pmod{2\pi},

arg⁡((u1−u4)(u3−u2))=θ1+θ2+θ3+θ4−2π2(mod2π).\arg((u_1-u_4)(u_3-u_2)) = \frac{\theta_1+\theta_2+\theta_3+\theta_4 - 2\pi}{2} \pmod{2\pi}.

These are equal modulo 2π2\pi, so

arg⁡((u1−u2)(u4−u3))=arg⁡((u1−u4)(u3−u2))+2nπ.■\arg((u_1-u_2)(u_4-u_3)) = \arg((u_1-u_4)(u_3-u_2)) + 2n\pi. \qquad \blacksquare

Part (iii): The magnitude identity

Since all uku_k lie on the unit circle, ∣ui−uj∣=2∣sin⁡θi−θj2∣|u_i - u_j| = 2\left|\sin\frac{\theta_i-\theta_j}{2}\right|. With the ordering −π<θ1<θ2<θ3<θ4<π-\pi < \theta_1 < \theta_2 < \theta_3 < \theta_4 < \pi, all differences θj−θi\theta_j - \theta_i for i<ji < j are positive and less than 2π2\pi, so ∣ui−uj∣=2sin⁡θj−θi2|u_i - u_j| = 2\sin\frac{\theta_j-\theta_i}{2}.

Let α=θ2−θ1>0\alpha = \theta_2 - \theta_1 > 0, β=θ3−θ2>0\beta = \theta_3 - \theta_2 > 0, γ=θ4−θ3>0\gamma = \theta_4 - \theta_3 > 0. Then

∣(u1−u2)(u4−u3)∣=4sin⁡α2sin⁡γ2,|(u_1-u_2)(u_4-u_3)| = 4\sin\frac{\alpha}{2}\sin\frac{\gamma}{2},

∣(u1−u4)(u3−u2)∣=4sin⁡α+β+γ2sin⁡β2,|(u_1-u_4)(u_3-u_2)| = 4\sin\frac{\alpha+\beta+\gamma}{2}\sin\frac{\beta}{2},

∣(u1−u3)(u4−u2)∣=4sin⁡α+β2sin⁡β+γ2.|(u_1-u_3)(u_4-u_2)| = 4\sin\frac{\alpha+\beta}{2}\sin\frac{\beta+\gamma}{2}.

We need to show:

sin⁡α2sin⁡γ2+sin⁡α+β+γ2sin⁡β2=sin⁡α+β2sin⁡β+γ2.(†)\sin\frac{\alpha}{2}\sin\frac{\gamma}{2} + \sin\frac{\alpha+\beta+\gamma}{2}\sin\frac{\beta}{2} = \sin\frac{\alpha+\beta}{2}\sin\frac{\beta+\gamma}{2}. \qquad (\dagger)

Let A=α/2A = \alpha/2, B=β/2B = \beta/2, C=γ/2C = \gamma/2. Then (†)(\dagger) becomes

sin⁡Asin⁡C+sin⁡(A+B+C)sin⁡B=sin⁡(A+B)sin⁡(B+C).\sin A\sin C + \sin(A+B+C)\sin B = \sin(A+B)\sin(B+C).

Using the product-to-sum formula sin⁡Xsin⁡Y=12[cos⁡(X−Y)−cos⁡(X+Y)]\sin X \sin Y = \frac{1}{2}[\cos(X-Y) - \cos(X+Y)]:

RHS: sin⁡(A+B)sin⁡(B+C)=12[cos⁡(A−C)−cos⁡(A+2B+C)]\sin(A+B)\sin(B+C) = \frac{1}{2}[\cos(A-C) - \cos(A+2B+C)].

LHS: sin⁡Asin⁡C=12[cos⁡(A−C)−cos⁡(A+C)]\sin A\sin C = \frac{1}{2}[\cos(A-C) - \cos(A+C)] and

sin⁡(A+B+C)sin⁡B=12[cos⁡(A+C)−cos⁡(A+2B+C)]\sin(A+B+C)\sin B = \frac{1}{2}[\cos(A+C) - \cos(A+2B+C)].

Adding: LHS=12[cos⁡(A−C)−cos⁡(A+2B+C)]=RHS\text{LHS} = \frac{1}{2}[\cos(A-C) - \cos(A+2B+C)] = \text{RHS}. ■\qquad \blacksquare

Geometric interpretation: The four points u1,u2,u3,u4u_1, u_2, u_3, u_4 lie in order on the unit circle, forming a cyclic quadrilateral. The identity ∣(u1−u2)(u4−u3)∣+∣(u1−u4)(u3−u2)∣=∣(u1−u3)(u4−u2)∣|(u_1-u_2)(u_4-u_3)| + |(u_1-u_4)(u_3-u_2)| = |(u_1-u_3)(u_4-u_2)| is precisely Ptolemy’s theorem: for a cyclic quadrilateral, the sum of the products of opposite sides equals the product of the diagonals.