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STEP3 2001 -- Pure Mathematics

Exam: STEP3  |  Year: 2001  |  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隐函数求导,数学归纳法,递推关系,Maclaurin级数展开
2微积分 CalculusChallenging反双曲函数恒等式,积分求面积,区域边界分析
3代数与方程 Algebra and EquationsStandard判别式分析,韦达定理,不等式约束,区域作图
4微积分 CalculusChallenging反三角函数恒等式,分段函数分析,函数图像描绘
5微积分 CalculusHard三次方程分析,参数方程法线,轨迹方程推导,分类讨论
6立体几何 / 3D GeometryChallenging向量法,平面方程,三角形特殊点,几何证明
7微分方程 / Differential EquationsChallenging正交轨线法,可分离变量微分方程,曲线族与包络
8复数 / Complex NumbersHard复数模和辐角,轨迹方程,分式线性变换,复平面几何

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

1 Given that y=ln⁡(x+(x2+1))y = \ln (x + \sqrt{(x^2 + 1)}), show that dydx=1(x2+1)\frac{dy}{dx} = \frac{1}{\sqrt{(x^2 + 1)}}.

Prove by induction that, for n⩾0n \geqslant 0,

(x2+1)y(n+2)+(2n+1)xy(n+1)+n2y(n)=0,(x^2 + 1) y^{(n+2)} + (2n + 1) xy^{(n+1)} + n^2y^{(n)} = 0 ,

where y(n)=dnydxny^{(n)} = \frac{d^ny}{dx^n} and y(0)=yy^{(0)} = y.

Using this result in the case x=0x = 0, or otherwise, show that the Maclaurin series for yy begins

x−x36+3x540x - \frac{x^3}{6} + \frac{3x^5}{40}

and find the next non-zero term.

Model Solution

Part (a): Show that dydx=1x2+1\frac{dy}{dx} = \frac{1}{\sqrt{x^2 + 1}}

Let y=ln⁡ ⁣(x+x2+1)y = \ln\!\left(x + \sqrt{x^2 + 1}\right).

Differentiating using the chain rule:

dydx=1x+x2+1⋅ddx ⁣(x+x2+1)\frac{dy}{dx} = \frac{1}{x + \sqrt{x^2 + 1}} \cdot \frac{d}{dx}\!\left(x + \sqrt{x^2 + 1}\right)

=1x+x2+1⋅(1+xx2+1)= \frac{1}{x + \sqrt{x^2 + 1}} \cdot \left(1 + \frac{x}{\sqrt{x^2 + 1}}\right)

=1x+x2+1⋅x2+1+xx2+1= \frac{1}{x + \sqrt{x^2 + 1}} \cdot \frac{\sqrt{x^2 + 1} + x}{\sqrt{x^2 + 1}}

=1x2+1■= \frac{1}{\sqrt{x^2 + 1}} \qquad \blacksquare

Part (b): Prove by induction that (x2+1)y(n+2)+(2n+1)x y(n+1)+n2y(n)=0(x^2 + 1) y^{(n+2)} + (2n+1) x\, y^{(n+1)} + n^2 y^{(n)} = 0

First, from part (a), we have (x2+1)1/2dydx=1(x^2 + 1)^{1/2} \frac{dy}{dx} = 1, so:

(x2+1) ⁣(dydx)2=1(*)(x^2 + 1)\!\left(\frac{dy}{dx}\right)^2 = 1 \qquad \text{(*)}

Differentiating (*) with respect to xx:

2x ⁣(dydx)2+2(x2+1)dydxd2ydx2=02x\!\left(\frac{dy}{dx}\right)^2 + 2(x^2 + 1)\frac{dy}{dx}\frac{d^2y}{dx^2} = 0

Since dydx≠0\frac{dy}{dx} \neq 0:

xdydx+(x2+1)d2ydx2=0(**)x\frac{dy}{dx} + (x^2 + 1)\frac{d^2y}{dx^2} = 0 \qquad \text{(**)}

This is the case n=0n = 0 of the recurrence (since y(0)=yy^{(0)} = y does not appear, the n=0n=0 case reduces to (x2+1)y′′+xy′=0(x^2+1)y'' + xy' = 0, which is (**)).

Base case n=0n = 0. We have just shown (x2+1)y(2)+x y(1)=0(x^2 + 1)y^{(2)} + x\,y^{(1)} = 0. (The term 02⋅y(0)=00^2 \cdot y^{(0)} = 0 vanishes.)

Inductive step. Assume the result holds for some n⩾0n \geqslant 0:

(x2+1)y(n+2)+(2n+1)x y(n+1)+n2y(n)=0(IH)(x^2 + 1) y^{(n+2)} + (2n+1) x\, y^{(n+1)} + n^2 y^{(n)} = 0 \qquad \text{(IH)}

Differentiate (IH) with respect to xx:

2x y(n+2)+(x2+1)y(n+3)+(2n+1)y(n+1)+(2n+1)x y(n+2)+n2y(n+1)=02x\, y^{(n+2)} + (x^2 + 1) y^{(n+3)} + (2n+1) y^{(n+1)} + (2n+1) x\, y^{(n+2)} + n^2 y^{(n+1)} = 0

Collecting terms:

(x2+1)y(n+3)+[2x+(2n+1)x] y(n+2)+[(2n+1)+n2] y(n+1)=0(x^2 + 1) y^{(n+3)} + [2x + (2n+1)x]\, y^{(n+2)} + [(2n+1) + n^2]\, y^{(n+1)} = 0

(x2+1)y(n+3)+(2n+3)x y(n+2)+(n+1)2y(n+1)=0(x^2 + 1) y^{(n+3)} + (2n+3) x\, y^{(n+2)} + (n+1)^2 y^{(n+1)} = 0

This is exactly the recurrence with nn replaced by n+1n + 1. By induction, the result holds for all n⩾0n \geqslant 0. ■\blacksquare

Part (c): Maclaurin series

Setting x=0x = 0 in the recurrence:

(0+1)y(n+2)(0)+0+n2y(n)(0)=0(0 + 1) y^{(n+2)}(0) + 0 + n^2 y^{(n)}(0) = 0

y(n+2)(0)=−n2 y(n)(0)(***)y^{(n+2)}(0) = -n^2\, y^{(n)}(0) \qquad \text{(***)}

We compute the derivatives at x=0x = 0:

  • y(0)=ln⁡(0+1)=0y(0) = \ln(0 + 1) = 0, so y(0)(0)=0y^{(0)}(0) = 0.
  • y′(0)=10+1=1y'(0) = \frac{1}{\sqrt{0+1}} = 1.
  • From (***): y′′(0)=−02⋅y(0)=0y''(0) = -0^2 \cdot y(0) = 0.
  • y(3)(0)=−12⋅y′(0)=−1y^{(3)}(0) = -1^2 \cdot y'(0) = -1.
  • y(4)(0)=−22⋅y′′(0)=0y^{(4)}(0) = -2^2 \cdot y''(0) = 0.
  • y(5)(0)=−32⋅y(3)(0)=−9⋅(−1)=9y^{(5)}(0) = -3^2 \cdot y^{(3)}(0) = -9 \cdot (-1) = 9.
  • y(6)(0)=−42⋅y(4)(0)=0y^{(6)}(0) = -4^2 \cdot y^{(4)}(0) = 0.
  • y(7)(0)=−52⋅y(5)(0)=−25⋅9=−225y^{(7)}(0) = -5^2 \cdot y^{(5)}(0) = -25 \cdot 9 = -225.

The Maclaurin series is:

y=∑k=0∞y(k)(0)k!xk=x−x33!+9x55!−225x77!+⋯y = \sum_{k=0}^{\infty} \frac{y^{(k)}(0)}{k!} x^k = x - \frac{x^3}{3!} + \frac{9 x^5}{5!} - \frac{225 x^7}{7!} + \cdots

=x−x36+9x5120−225x75040+⋯= x - \frac{x^3}{6} + \frac{9x^5}{120} - \frac{225 x^7}{5040} + \cdots

=x−x36+3x540−5x7112+⋯= x - \frac{x^3}{6} + \frac{3x^5}{40} - \frac{5x^7}{112} + \cdots

The first three terms are x−x36+3x540x - \frac{x^3}{6} + \frac{3x^5}{40} as required, and the next non-zero term is −5x7112-\dfrac{5x^7}{112}.


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

2 Show that cosh⁡−1x=ln⁡(x+(x2−1))\cosh^{-1} x = \ln (x + \sqrt{(x^2 - 1)}).

Show that the area of the region defined by the inequalities y2⩾x2−8y^2 \geqslant x^2 - 8 and x2⩾25y2−16x^2 \geqslant 25y^2 - 16 is (72/5)ln⁡2(72/5) \ln 2.

Model Solution

Part (a): Show that cosh⁡−1x=ln⁡ ⁣(x+x2−1)\cosh^{-1} x = \ln\!\left(x + \sqrt{x^2 - 1}\right)

Let y=cosh⁡−1xy = \cosh^{-1} x, so x=cosh⁡yx = \cosh y with y⩾0y \geqslant 0.

From cosh⁡y=ey+e−y2=x\cosh y = \frac{e^y + e^{-y}}{2} = x, multiply by 2ey2e^y:

e2y−2x ey+1=0e^{2y} - 2x\, e^y + 1 = 0

This is quadratic in eye^y:

ey=2x±4x2−42=x±x2−1e^y = \frac{2x \pm \sqrt{4x^2 - 4}}{2} = x \pm \sqrt{x^2 - 1}

Since y⩾0y \geqslant 0, we need ey⩾1e^y \geqslant 1. Both roots are positive (product = 1), so x+x2−1⩾1x + \sqrt{x^2 - 1} \geqslant 1 and x−x2−1⩽1x - \sqrt{x^2 - 1} \leqslant 1 (since their product is 1). Therefore ey=x+x2−1e^y = x + \sqrt{x^2 - 1}, giving:

cosh⁡−1x=ln⁡ ⁣(x+x2−1)■\cosh^{-1} x = \ln\!\left(x + \sqrt{x^2 - 1}\right) \qquad \blacksquare

Part (b): Area of the region

The region is defined by y2⩾x2−8y^2 \geqslant x^2 - 8 and x2⩾25y2−16x^2 \geqslant 25y^2 - 16.

Both inequalities are unchanged when xx or yy is replaced by its negative, so the total area is four times the area in the first quadrant.

In the first quadrant, the second inequality gives

0⩽y⩽15x2+16.0 \leqslant y \leqslant \frac{1}{5}\sqrt{x^2+16}.

The first inequality is automatic when 0⩽x<80 \leqslant x < \sqrt8, and gives y⩾x2−8y \geqslant \sqrt{x^2-8} when x⩾8x \geqslant \sqrt8.

The two upper boundary curves meet when

x2−8=15x2+16.\sqrt{x^2-8}=\frac15\sqrt{x^2+16}.

Squaring gives 25x2−200=x2+1625x^2-200=x^2+16, so x2=9x^2=9. Thus in the first quadrant the bounded part runs from x=0x=0 to x=3x=3, with the lower boundary changing at x=8x=\sqrt8.

The first-quadrant area is therefore

∫0815x2+16 dx+∫83[15x2+16−x2−8]dx\int_0^{\sqrt{8}} \frac{1}{5}\sqrt{x^2+16}\, dx + \int_{\sqrt{8}}^{3} \left[\frac{1}{5}\sqrt{x^2+16} - \sqrt{x^2-8}\right] dx

=15∫03x2+16 dx−∫83x2−8 dx= \frac{1}{5}\int_0^{3} \sqrt{x^2+16}\, dx - \int_{\sqrt{8}}^{3} \sqrt{x^2-8}\, dx

Integral 1: ∫x2+16 dx\int \sqrt{x^2 + 16}\, dx.

Using the standard formula ∫x2+a2 dx=x2x2+a2+a22ln⁡ ⁣(x+x2+a2)+C\int \sqrt{x^2 + a^2}\, dx = \frac{x}{2}\sqrt{x^2+a^2} + \frac{a^2}{2}\ln\!\left(x + \sqrt{x^2+a^2}\right) + C:

∫03x2+16 dx=[x2x2+16+8ln⁡ ⁣(x+x2+16)]03\int_0^3 \sqrt{x^2+16}\, dx = \left[\frac{x}{2}\sqrt{x^2+16} + 8\ln\!\left(x + \sqrt{x^2+16}\right)\right]_0^3

=3225+8ln⁡(3+5)−0−8ln⁡4= \frac{3}{2}\sqrt{25} + 8\ln(3+5) - 0 - 8\ln 4

=152+8ln⁡8−8ln⁡4=152+8ln⁡2= \frac{15}{2} + 8\ln 8 - 8\ln 4 = \frac{15}{2} + 8\ln 2

Integral 2: ∫x2−8 dx\int \sqrt{x^2 - 8}\, dx.

Using ∫x2−a2 dx=x2x2−a2−a22ln⁡ ⁣∣x+x2−a2∣+C\int \sqrt{x^2 - a^2}\, dx = \frac{x}{2}\sqrt{x^2-a^2} - \frac{a^2}{2}\ln\!\left|x + \sqrt{x^2-a^2}\right| + C:

∫83x2−8 dx=[x2x2−8−4ln⁡ ⁣(x+x2−8)]83\int_{\sqrt{8}}^{3} \sqrt{x^2-8}\, dx = \left[\frac{x}{2}\sqrt{x^2-8} - 4\ln\!\left(x + \sqrt{x^2-8}\right)\right]_{\sqrt{8}}^{3}

=321−4ln⁡(3+1)−0+4ln⁡(8)= \frac{3}{2}\sqrt{1} - 4\ln(3+1) - 0 + 4\ln(\sqrt{8})

=32−4ln⁡4+4ln⁡8=32−4ln⁡4+4⋅32ln⁡2= \frac{3}{2} - 4\ln 4 + 4\ln\sqrt{8} = \frac{3}{2} - 4\ln 4 + 4 \cdot \frac{3}{2}\ln 2

=32−8ln⁡2+6ln⁡2=32−2ln⁡2= \frac{3}{2} - 8\ln 2 + 6\ln 2 = \frac{3}{2} - 2\ln 2

Thus the first-quadrant area is

15 ⁣(152+8ln⁡2)−(32−2ln⁡2)=185ln⁡2.\frac{1}{5}\!\left(\frac{15}{2}+8\ln2\right)-\left(\frac{3}{2}-2\ln2\right)=\frac{18}{5}\ln2.

Multiplying by 44 for the four quadrants gives

A=4⋅185ln⁡2=725ln⁡2.■A=4\cdot\frac{18}{5}\ln2=\frac{72}{5}\ln2. \qquad \blacksquare


Topic: 代数与方程 Algebra and Equations  |  Difficulty: Standard  |  Marks: 20

3 Consider the equation

x2−bx+c=0,x^2 - bx + c = 0 ,

where bb and cc are real numbers.

(i) Show that the roots of the equation are real and positive if and only if b>0b > 0 and b2⩾4c>0b^2 \geqslant 4c > 0, and sketch the region of the bb-cc plane in which these conditions hold.

(ii) Sketch the region of the bb-cc plane in which the roots of the equation are real and less than 1 in magnitude.

Model Solution

Part (i)

Let the roots be α\alpha and β\beta. By Vieta’s formulas:

α+β=b(1)\alpha + \beta = b \qquad \text{(1)}

αβ=c(2)\alpha \beta = c \qquad \text{(2)}

We prove both directions of the “if and only if”.

Forward direction. Suppose both roots are real and positive.

Since α>0\alpha > 0 and β>0\beta > 0:

  • From (1): b=α+β>0b = \alpha + \beta > 0.
  • From (2): c=αβ>0c = \alpha \beta > 0.
  • Real roots require discriminant Δ=b2−4c⩾0\Delta = b^2 - 4c \geqslant 0, i.e., b2⩾4cb^2 \geqslant 4c.

Combining: b>0b > 0 and b2⩾4c>0b^2 \geqslant 4c > 0.

Reverse direction. Suppose b>0b > 0 and b2⩾4c>0b^2 \geqslant 4c > 0.

  • b2⩾4cb^2 \geqslant 4c means Δ⩾0\Delta \geqslant 0, so the roots are real.
  • 4c>04c > 0 gives c>0c > 0, so αβ=c>0\alpha \beta = c > 0: the roots have the same sign.
  • b>0b > 0 gives α+β=b>0\alpha + \beta = b > 0: the roots are not both negative.

Since the roots have the same sign and their sum is positive, both roots are positive.

This completes the proof. ■\blacksquare

Sketch of the region. In the bb-cc plane, the conditions are:

  1. b>0b > 0 (right of the cc-axis, not including it),
  2. c>0c > 0 (above the bb-axis, not including it),
  3. c⩽b24c \leqslant \frac{b^2}{4} (on or below the parabola c=b24c = \frac{b^2}{4}).

The region is bounded below by the positive bb-axis, on the left by the cc-axis (excluded), and above by the parabola c=b24c = \frac{b^2}{4} (included). The parabola passes through the origin and opens upward. The boundary c=0c = 0 (the bb-axis) is excluded since 4c>04c > 0, while the parabola c=b24c = \frac{b^2}{4} is included.

Part (ii)

We need the roots to satisfy −1<α,β<1-1 < \alpha, \beta < 1, i.e., both roots lie strictly between −1-1 and 11.

Since the coefficient of x2x^2 is positive, the parabola y=x2−bx+cy = x^2 - bx + c opens upward. Both roots lie in (−1,1)(-1, 1) if and only if:

(a) f(1)>0f(1) > 0: the value at x=1x = 1 is positive (so x=1x = 1 is to the right of both roots),

(b) f(−1)>0f(-1) > 0: the value at x=−1x = -1 is positive (so x=−1x = -1 is to the left of both roots),

(c) Δ⩾0\Delta \geqslant 0: the roots are real.

Evaluating:

f(1)=1−b+c>0  ⟹  c>b−1(a)f(1) = 1 - b + c > 0 \implies c > b - 1 \qquad \text{(a)}

f(−1)=1+b+c>0  ⟹  c>−b−1(b)f(-1) = 1 + b + c > 0 \implies c > -b - 1 \qquad \text{(b)}

b2⩾4c(c)b^2 \geqslant 4c \qquad \text{(c)}

Since α,β∈(−1,1)\alpha,\beta\in(-1,1), their sum satisfies −2<α+β<2-2<\alpha+\beta<2, so the region must also have −2<b<2-2<b<2. Conversely, the conditions

−2<b<2,c>∣b∣−1,c⩽b24-2<b<2,\qquad c>|b|-1,\qquad c\leqslant \frac{b^2}{4}

give real roots, put the endpoints x=−1x=-1 and x=1x=1 outside the interval between the roots, and keep the vertex between the endpoints. Hence both roots lie strictly in (−1,1)(-1,1).

Sketch of the region. The boundary curves are:

  • c=b−1c = b - 1: a line with gradient 1 and cc-intercept −1-1.
  • c=−b−1c = -b - 1: a line with gradient −1-1 and cc-intercept −1-1.
  • c=b24c = \frac{b^2}{4}: the parabola from part (i).

The two lines meet at (0,−1)(0, -1), forming a V-shape opening upward. The parabola intersects c=b−1c = b - 1 at b=2b = 2 (giving the point (2,1)(2, 1)) and intersects c=−b−1c = -b - 1 at b=−2b = -2 (giving the point (−2,1)(-2, 1)).

The region is:

  • Above both lines: c>b−1c > b - 1 and c>−b−1c > -b - 1, equivalently c>∣b∣−1c > |b| - 1.
  • Below or on the parabola: c⩽b24c \leqslant \frac{b^2}{4}.
  • Between the vertical lines b=−2b=-2 and b=2b=2, with both vertical boundary lines excluded.

This region lies between b=−2b = -2 and b=2b = 2, bounded below by the V-shaped pair of lines (excluded) and above by the parabola (included). The region has a roughly lens-shaped appearance, widest near b=0b = 0 where the gap between the parabola (c=0c = 0) and the lines (c=−1c = -1) is greatest.


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

4 In this question, the function sin⁡−1\sin^{-1} is defined to have domain −1⩽x⩽1-1 \leqslant x \leqslant 1 and range −π2⩽x⩽π2-\frac{\pi}{2} \leqslant x \leqslant \frac{\pi}{2} and the function tan⁡−1\tan^{-1} is defined to have the real numbers as its domain and range −π2<x<π2-\frac{\pi}{2} < x < \frac{\pi}{2}.

(i) Let

g(x)=2x1+x2 , −∞<x<∞ .g(x) = \frac{2x}{1 + x^2} \text{ , } \quad -\infty < x < \infty \text{ .}

Sketch the graph of g(x)g(x) and state the range of gg.

(ii) Let

f(x)=sin⁡−1(2x1+x2) , −∞<x<∞ .f(x) = \sin^{-1} \left( \frac{2x}{1 + x^2} \right) \text{ , } \quad -\infty < x < \infty \text{ .}

Show that f(x)=2tan⁡−1xf(x) = 2 \tan^{-1} x for −1⩽x⩽1-1 \leqslant x \leqslant 1 and f(x)=π−2tan⁡−1xf(x) = \pi - 2 \tan^{-1} x for x⩾1x \geqslant 1. Sketch the graph of f(x)f(x).

Model Solution

Part (i)

We analyse g(x)=2x1+x2g(x) = \frac{2x}{1 + x^2}.

Derivative. Using the quotient rule:

g′(x)=2(1+x2)−2x⋅2x(1+x2)2=2+2x2−4x2(1+x2)2=2(1−x2)(1+x2)2g'(x) = \frac{2(1 + x^2) - 2x \cdot 2x}{(1 + x^2)^2} = \frac{2 + 2x^2 - 4x^2}{(1 + x^2)^2} = \frac{2(1 - x^2)}{(1 + x^2)^2}

Setting g′(x)=0g'(x) = 0: 1−x2=01 - x^2 = 0, so x=±1x = \pm 1.

  • g′(x)>0g'(x) > 0 for ∣x∣<1|x| < 1: gg is increasing on (−1,1)(-1, 1).
  • g′(x)<0g'(x) < 0 for ∣x∣>1|x| > 1: gg is decreasing on (−∞,−1)(-\infty, -1) and (1,∞)(1, \infty).

Key values. g(−1)=−22=−1g(-1) = \frac{-2}{2} = -1 (local minimum), g(1)=22=1g(1) = \frac{2}{2} = 1 (local maximum), g(0)=0g(0) = 0.

Behaviour at infinity. g(x)→0+g(x) \to 0^+ as x→+∞x \to +\infty, and g(x)→0−g(x) \to 0^- as x→−∞x \to -\infty.

Symmetry. g(−x)=−2x1+x2=−g(x)g(-x) = \frac{-2x}{1 + x^2} = -g(x), so gg is an odd function (symmetric about the origin).

Graph. The curve passes through the origin, rises to a maximum of 11 at x=1x = 1, then decays toward 00 as x→∞x \to \infty. By odd symmetry, it falls to a minimum of −1-1 at x=−1x = -1 and approaches 00 from below as x→−∞x \to -\infty. The xx-axis is a horizontal asymptote.

Range. The maximum value is g(1)=1g(1) = 1 and the minimum value is g(−1)=−1g(-1) = -1. Since gg is continuous and achieves all values between −1-1 and 11:

range of g=[−1,1].\text{range of } g = [-1, 1].

Part (ii)

Let θ=tan⁡−1x\theta = \tan^{-1} x, so x=tan⁡θx = \tan\theta with θ∈(−π2,π2)\theta \in \left(-\frac{\pi}{2}, \frac{\pi}{2}\right).

Then:

2x1+x2=2tan⁡θ1+tan⁡2θ=2tan⁡θsec⁡2θ=2sin⁡θcos⁡θ=sin⁡2θ\frac{2x}{1 + x^2} = \frac{2\tan\theta}{1 + \tan^2\theta} = \frac{2\tan\theta}{\sec^2\theta} = 2\sin\theta\cos\theta = \sin 2\theta

So f(x)=sin⁡−1(sin⁡2θ)f(x) = \sin^{-1}(\sin 2\theta).

We evaluate sin⁡−1(sin⁡2θ)\sin^{-1}(\sin 2\theta) using the range of sin⁡−1\sin^{-1}, which is [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right].

Case 1: −1⩽x⩽1-1 \leqslant x \leqslant 1.

Here θ=tan⁡−1x∈[−π4,π4]\theta = \tan^{-1} x \in \left[-\frac{\pi}{4}, \frac{\pi}{4}\right], so 2θ∈[−π2,π2]2\theta \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right].

Since 2θ2\theta lies in the range of sin⁡−1\sin^{-1}:

f(x)=sin⁡−1(sin⁡2θ)=2θ=2tan⁡−1xf(x) = \sin^{-1}(\sin 2\theta) = 2\theta = 2\tan^{-1} x

Case 2: x⩾1x \geqslant 1.

Here θ=tan⁡−1x∈[π4,π2)\theta = \tan^{-1} x \in \left[\frac{\pi}{4}, \frac{\pi}{2}\right), so 2θ∈[π2,π)2\theta \in \left[\frac{\pi}{2}, \pi\right).

For 2θ∈[π2,π)2\theta \in \left[\frac{\pi}{2}, \pi\right), we use the identity sin⁡(π−2θ)=sin⁡2θ\sin(\pi - 2\theta) = \sin 2\theta and note that π−2θ∈(0,π2]⊂[−π2,π2]\pi - 2\theta \in \left(0, \frac{\pi}{2}\right] \subset \left[-\frac{\pi}{2}, \frac{\pi}{2}\right]:

f(x)=sin⁡−1(sin⁡2θ)=π−2θ=π−2tan⁡−1xf(x) = \sin^{-1}(\sin 2\theta) = \pi - 2\theta = \pi - 2\tan^{-1} x

Case 3: x⩽−1x \leqslant -1 (by symmetry).

Since gg is odd, we have f(−x)=sin⁡−1(−g(x))=−sin⁡−1(g(x))=−f(x)f(-x) = \sin^{-1}(-g(x)) = -\sin^{-1}(g(x)) = -f(x), so ff is odd.

For x⩽−1x \leqslant -1, using f(x)=−f(−x)f(x) = -f(-x) and Case 2 (since −x⩾1-x \geqslant 1):

f(x)=−[π−2tan⁡−1(−x)]=−π+2tan⁡−1(−x)=−π−2tan⁡−1xf(x) = -[\pi - 2\tan^{-1}(-x)] = -\pi + 2\tan^{-1}(-x) = -\pi - 2\tan^{-1} x

This completes the derivation. ■\blacksquare

Sketch of f(x)f(x).

The piecewise definition is:

f(x)={−π−2tan⁡−1xx⩽−12tan⁡−1x−1⩽x⩽1π−2tan⁡−1xx⩾1f(x) = \begin{cases} -\pi - 2\tan^{-1} x & x \leqslant -1 \\ 2\tan^{-1} x & -1 \leqslant x \leqslant 1 \\ \pi - 2\tan^{-1} x & x \geqslant 1 \end{cases}

Key features:

  • ff is continuous everywhere (check at x=±1x = \pm 1: f(1)=π2f(1) = \frac{\pi}{2}, f(−1)=−π2f(-1) = -\frac{\pi}{2}).
  • ff is an odd function: symmetric about the origin.
  • On [−1,1][-1, 1], ff increases from −π2-\frac{\pi}{2} to π2\frac{\pi}{2} with an inflection point at the origin (this portion is 2tan⁡−1x2\tan^{-1} x).
  • For x⩾1x \geqslant 1, ff decreases from π2\frac{\pi}{2} toward 00 as x→∞x \to \infty (horizontal asymptote y=0y = 0).
  • For x⩽−1x \leqslant -1, ff increases from −π2-\frac{\pi}{2} toward 00 as x→−∞x \to -\infty (horizontal asymptote y=0y = 0).
  • Not differentiable at x=±1x = \pm 1 (the left and right derivatives differ).

The graph looks like a stretched S-curve on [−1,1][-1, 1] that flattens out to the xx-axis on both sides.


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

5 Show that the equation x3+px+q=0x^3 + px + q = 0 has exactly one real solution if p⩾0p \geqslant 0.

A parabola CC is given parametrically by

x=at2,y=2at(a>0) .x = at^2, \quad y = 2at \quad (a > 0) \text{ .}

Find an equation which must be satisfied by tt at points on CC at which the normal passes through the point (h,k)(h, k). Hence show that, if h⩽2ah \leqslant 2a, exactly one normal to CC will pass through (h,k)(h, k).

Find, in Cartesian form, the equation of the locus of the points from which exactly two normals can be drawn to CC. Sketch the locus.

Model Solution

Part (a): Show that x3+px+q=0x^3 + px + q = 0 has exactly one real solution if p⩾0p \geqslant 0

Let f(x)=x3+px+qf(x) = x^3 + px + q.

f′(x)=3x2+pf'(x) = 3x^2 + p

Since p⩾0p \geqslant 0 and 3x2⩾03x^2 \geqslant 0 for all xx, we have f′(x)⩾0f'(x) \geqslant 0 for all xx. Moreover, f′(x)=0f'(x) = 0 only at x=0x = 0 (when p=0p = 0), so ff is strictly increasing.

A strictly increasing continuous function can cross the xx-axis at most once. Since f(x)→+∞f(x) \to +\infty as x→+∞x \to +\infty and f(x)→−∞f(x) \to -\infty as x→−∞x \to -\infty, by the intermediate value theorem, ff has exactly one real root. ■\blacksquare

Part (b): Find the equation for tt at normal points through (h,k)(h, k)

For the parabola x=at2x = at^2, y=2aty = 2at:

dydx=dy/dtdx/dt=2a2at=1t\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{2a}{2at} = \frac{1}{t}

The slope of the normal at parameter tt is −t-t. The normal at (at2,2at)(at^2, 2at) is:

y−2at=−t(x−at2)y - 2at = -t(x - at^2)

For this to pass through (h,k)(h, k):

k−2at=−t(h−at2)k - 2at = -t(h - at^2)

k−2at=−th+at3k - 2at = -th + at^3

at3+(2a−h)t−k=0(*)at^3 + (2a - h)t - k = 0 \qquad \text{(*)}

This is the required equation. ■\blacksquare

Part (c): If h⩽2ah \leqslant 2a, exactly one normal passes through (h,k)(h, k)

Equation (*) can be written as t3+2a−ha t−ka=0t^3 + \frac{2a - h}{a}\,t - \frac{k}{a} = 0.

Since h⩽2ah \leqslant 2a, we have 2a−h⩾02a - h \geqslant 0, so the coefficient 2a−ha⩾0\frac{2a - h}{a} \geqslant 0 (using a>0a > 0).

By part (a), this cubic in tt has exactly one real solution. Each real value of tt gives a distinct point on the parabola, so exactly one normal to CC passes through (h,k)(h, k). ■\blacksquare

Part (d): Locus of points from which exactly two normals can be drawn

Exactly two normals means the cubic (*) has exactly two distinct real roots, i.e., one root is repeated. Let the roots be s,s,t3s, s, t_3 with s≠t3s \neq t_3.

From Vieta’s formulas for t3+2a−ha t−ka=0t^3 + \frac{2a-h}{a}\,t - \frac{k}{a} = 0:

2s+t3=0  ⟹  t3=−2s(1)2s + t_3 = 0 \implies t_3 = -2s \qquad \text{(1)}

s2+2st3=2a−ha(2)s^2 + 2st_3 = \frac{2a - h}{a} \qquad \text{(2)}

s2t3=ka(3)s^2 t_3 = \frac{k}{a} \qquad \text{(3)}

From (1) and (3):

s2(−2s)=ka  ⟹  k=−2as3s^2(-2s) = \frac{k}{a} \implies k = -2as^3

From (1) and (2):

s2+2s(−2s)=2a−ha  ⟹  −3s2=2a−has^2 + 2s(-2s) = \frac{2a - h}{a} \implies -3s^2 = \frac{2a - h}{a}

h=2a+3as2=a(2+3s2)h = 2a + 3as^2 = a(2 + 3s^2)

To eliminate ss: from k=−2as3k = -2as^3, we get s3=−k2as^3 = -\frac{k}{2a}, so s6=k24a2s^6 = \frac{k^2}{4a^2}.

From h=a(2+3s2)h = a(2 + 3s^2): s2=h−2a3as^2 = \frac{h - 2a}{3a}, so s6=(h−2a)327a3s^6 = \frac{(h-2a)^3}{27a^3}.

Equating:

k24a2=(h−2a)327a3\frac{k^2}{4a^2} = \frac{(h - 2a)^3}{27a^3}

27ak2=4(h−2a)327ak^2 = 4(h - 2a)^3

This is a semicubical parabola (Neile’s parabola) with a cusp at (2a,0)(2a, 0). It exists only for h⩾2ah \geqslant 2a (since s2⩾0s^2 \geqslant 0 requires h⩾2ah \geqslant 2a).

The locus is the curve:

27ak2=4(h−2a)3\boxed{27ak^2 = 4(h - 2a)^3}

This is the evolute of the parabola CC. The cusp is at (2a,0)(2a, 0), which is the focus of the parabola. The curve extends to the right (for h>2ah > 2a), and the region inside this evolute is where three normals can be drawn to CC.


Topic: 立体几何 / 3D Geometry  |  Difficulty: Challenging  |  Marks: 20

6 The plane

xa+yb+zc=1\frac{x}{a} + \frac{y}{b} + \frac{z}{c} = 1

meets the co-ordinate axes at the points A,BA, B and CC. The point MM has coordinates (12a,12b,12c)(\frac{1}{2}a, \frac{1}{2}b, \frac{1}{2}c) and OO is the origin.

Show that OMOM meets the plane at the centroid (13a,13b,13c)(\frac{1}{3}a, \frac{1}{3}b, \frac{1}{3}c) of triangle ABCABC. Show also that the perpendiculars to the plane from OO and from MM meet the plane at the orthocentre and at the circumcentre of triangle ABCABC respectively.

Hence prove that the centroid of a triangle lies on the line segment joining its orthocentre and circumcentre, and that it divides this line segment in the ratio 2:12 : 1.

[The orthocentre of a triangle is the point at which the three altitudes intersect; the circumcentre of a triangle is the point equidistant from the three vertices.]

Model Solution

The plane xa+yb+zc=1\frac{x}{a} + \frac{y}{b} + \frac{z}{c} = 1 meets the coordinate axes at A=(a,0,0)A = (a, 0, 0), B=(0,b,0)B = (0, b, 0), C=(0,0,c)C = (0, 0, c).

Part (a): OMOM meets the plane at the centroid of △ABC\triangle ABC

The line from O=(0,0,0)O = (0,0,0) through M=(12a,12b,12c)M = (\frac{1}{2}a, \frac{1}{2}b, \frac{1}{2}c) is:

(x,y,z)=t ⁣(12a,12b,12c)=(ta2,tb2,tc2)(x, y, z) = t\!\left(\tfrac{1}{2}a, \tfrac{1}{2}b, \tfrac{1}{2}c\right) = \left(\tfrac{ta}{2}, \tfrac{tb}{2}, \tfrac{tc}{2}\right)

Substituting into the plane equation:

ta/2a+tb/2b+tc/2c=1  ⟹  3t2=1  ⟹  t=23\frac{ta/2}{a} + \frac{tb/2}{b} + \frac{tc/2}{c} = 1 \implies \frac{3t}{2} = 1 \implies t = \frac{2}{3}

The intersection point is (a3,b3,c3)\left(\frac{a}{3}, \frac{b}{3}, \frac{c}{3}\right).

The centroid of △ABC\triangle ABC is G=A+B+C3=(a3,b3,c3)G = \frac{A + B + C}{3} = \left(\frac{a}{3}, \frac{b}{3}, \frac{c}{3}\right).

These are the same point. ■\blacksquare

Part (b): The perpendicular from OO meets the plane at the orthocentre

The normal to the plane is n=(1a,1b,1c)\mathbf{n} = \left(\frac{1}{a}, \frac{1}{b}, \frac{1}{c}\right). The perpendicular from OO to the plane is:

(x,y,z)=t ⁣(1a,1b,1c)(x, y, z) = t\!\left(\frac{1}{a}, \frac{1}{b}, \frac{1}{c}\right)

Substituting into the plane equation:

ta2+tb2+tc2=1  ⟹  t=11a2+1b2+1c2\frac{t}{a^2} + \frac{t}{b^2} + \frac{t}{c^2} = 1 \implies t = \frac{1}{\frac{1}{a^2} + \frac{1}{b^2} + \frac{1}{c^2}}

Let S=1a2+1b2+1c2S = \frac{1}{a^2} + \frac{1}{b^2} + \frac{1}{c^2}. The foot of the perpendicular is:

H=(1aS,1bS,1cS)H = \left(\frac{1}{aS}, \frac{1}{bS}, \frac{1}{cS}\right)

We now verify this is the orthocentre of △ABC\triangle ABC. It is enough to show that HH lies on the three altitudes. For example,

AH→=(1aS−a,1bS,1cS),BC→=(0,−b,c)\overrightarrow{AH} = \left(\frac{1}{aS} - a, \frac{1}{bS}, \frac{1}{cS}\right), \quad \overrightarrow{BC} = (0, -b, c)

so

AH→⋅BC→=−bbS+ccS=−1S+1S=0.\overrightarrow{AH} \cdot \overrightarrow{BC} = -\frac{b}{bS} + \frac{c}{cS} = -\frac{1}{S} + \frac{1}{S} = 0.

By symmetry (cyclic permutation of a,b,ca, b, c):

BH→⋅CA→=0,CH→⋅AB→=0.\overrightarrow{BH} \cdot \overrightarrow{CA} = 0,\qquad \overrightarrow{CH} \cdot \overrightarrow{AB} = 0.

Thus HH lies on all three altitudes, confirming it is the orthocentre. ■\blacksquare

Part (c): The perpendicular from MM meets the plane at the circumcentre

The perpendicular from M=(a2,b2,c2)M = (\frac{a}{2}, \frac{b}{2}, \frac{c}{2}) in direction n=(1a,1b,1c)\mathbf{n} = (\frac{1}{a}, \frac{1}{b}, \frac{1}{c}):

(x,y,z)=(a2+ta,b2+tb,c2+tc)(x, y, z) = \left(\frac{a}{2} + \frac{t}{a}, \frac{b}{2} + \frac{t}{b}, \frac{c}{2} + \frac{t}{c}\right)

Substituting into the plane:

12+ta2+12+tb2+12+tc2=1\frac{1}{2} + \frac{t}{a^2} + \frac{1}{2} + \frac{t}{b^2} + \frac{1}{2} + \frac{t}{c^2} = 1

32+tS=1  ⟹  t=−12S\frac{3}{2} + tS = 1 \implies t = -\frac{1}{2S}

The foot of the perpendicular is:

Oc=(a2−12aS,b2−12bS,c2−12cS)O_c = \left(\frac{a}{2} - \frac{1}{2aS}, \frac{b}{2} - \frac{1}{2bS}, \frac{c}{2} - \frac{1}{2cS}\right)

We verify this is equidistant from AA, BB, CC. Let α=1a2S\alpha = \frac{1}{a^2 S}, β=1b2S\beta = \frac{1}{b^2 S}, γ=1c2S\gamma = \frac{1}{c^2 S}, so α+β+γ=1\alpha + \beta + \gamma = 1.

Then Oc=(a(1−α)2,b(1−β)2,c(1−γ)2)O_c = \left(\frac{a(1-\alpha)}{2}, \frac{b(1-\beta)}{2}, \frac{c(1-\gamma)}{2}\right).

Distance to A=(a,0,0)A = (a, 0, 0):

∣OcA∣2=a2(1+α)24+b2(1−β)24+c2(1−γ)24|O_c A|^2 = \frac{a^2(1+\alpha)^2}{4} + \frac{b^2(1-\beta)^2}{4} + \frac{c^2(1-\gamma)^2}{4}

Distance to B=(0,b,0)B = (0, b, 0):

∣OcB∣2=a2(1−α)24+b2(1+β)24+c2(1−γ)24|O_c B|^2 = \frac{a^2(1-\alpha)^2}{4} + \frac{b^2(1+\beta)^2}{4} + \frac{c^2(1-\gamma)^2}{4}

Distance to C=(0,0,c)C = (0, 0, c):

∣OcC∣2=a2(1−α)24+b2(1−β)24+c2(1+γ)24|O_c C|^2 = \frac{a^2(1-\alpha)^2}{4} + \frac{b^2(1-\beta)^2}{4} + \frac{c^2(1+\gamma)^2}{4}

Computing ∣OcA∣2−∣OcB∣2|O_c A|^2 - |O_c B|^2:

=a2[(1+α)2−(1−α)2]−b2[(1+β)2−(1−β)2]4= \frac{a^2[(1+\alpha)^2 - (1-\alpha)^2] - b^2[(1+\beta)^2 - (1-\beta)^2]}{4}

=4a2α−4b2β4=a2α−b2β=1S−1S=0= \frac{4a^2\alpha - 4b^2\beta}{4} = a^2\alpha - b^2\beta = \frac{1}{S} - \frac{1}{S} = 0

Similarly ∣OcB∣2−∣OcC∣2=0|O_c B|^2 - |O_c C|^2 = 0. So OcO_c is equidistant from all three vertices, confirming it is the circumcentre. ■\blacksquare

Part (d): The centroid divides the orthocentre—circumcentre segment in the ratio 2:12:1

The centroid, orthocentre, and circumcentre all lie in the plane of △ABC\triangle ABC. We show G=2Oc+H3G = \frac{2O_c + H}{3}.

2Oc+H3=13(a(1−α)+1aS,  b(1−β)+1bS,  c(1−γ)+1cS)\frac{2O_c + H}{3} = \frac{1}{3}\left(a(1-\alpha) + \frac{1}{aS}, \; b(1-\beta) + \frac{1}{bS}, \; c(1-\gamma) + \frac{1}{cS}\right)

Since 1aS=aα\frac{1}{aS} = a\alpha:

a(1−α)+aα=aa(1-\alpha) + a\alpha = a

So the first component is a3\frac{a}{3}. By symmetry, the second and third components are b3\frac{b}{3} and c3\frac{c}{3}.

Therefore 2Oc+H3=(a3,b3,c3)=G\frac{2O_c + H}{3} = \left(\frac{a}{3}, \frac{b}{3}, \frac{c}{3}\right) = G.

This means GG lies on the segment HOcHO_c and divides it in the ratio HG:GOc=2:1HG : GO_c = 2 : 1 (with GG closer to OcO_c). ■\blacksquare


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

7 Sketch the graph of the function ln⁡x−12x2\ln x - \frac{1}{2}x^2.

Show that the differential equation dydx=2xyx2−1\frac{\mathrm{d}y}{\mathrm{d}x} = \frac{2xy}{x^2 - 1} describes a family of parabolas each of which passes through the points (1,0)(1, 0) and (−1,0)(-1, 0) and has its vertex on the yy-axis.

Hence find the equation of the curve that passes through the point (1,1)(1, 1) and intersects each of the above parabolas orthogonally. Sketch this curve.

[Two curves intersect orthogonally if their tangents at the point of intersection are perpendicular.]

Model Solution

Part (a): Sketch of f(x)=ln⁡x−12x2f(x) = \ln x - \frac{1}{2}x^2

Domain: x>0x > 0.

Derivative. f′(x)=1x−x=1−x2xf'(x) = \frac{1}{x} - x = \frac{1 - x^2}{x}.

Setting f′(x)=0f'(x) = 0: x=1x = 1 (since x>0x > 0).

  • f′(x)>0f'(x) > 0 for 0<x<10 < x < 1: ff is increasing.
  • f′(x)<0f'(x) < 0 for x>1x > 1: ff is decreasing.

So x=1x = 1 is a maximum. f(1)=0−12=−12f(1) = 0 - \frac{1}{2} = -\frac{1}{2}.

Behaviour at boundaries. f(x)→−∞f(x) \to -\infty as x→0+x \to 0^+ (since ln⁡x→−∞\ln x \to -\infty) and f(x)→−∞f(x) \to -\infty as x→+∞x \to +\infty (since −12x2-\frac{1}{2}x^2 dominates).

Root. Since f(1)=−12<0f(1) = -\frac{1}{2} < 0 and f(x)<0f(x) < 0 at both endpoints, ff is negative everywhere. The graph has a single maximum at (1,−12)(1, -\frac{1}{2}) and lies entirely below the xx-axis.

The curve is an inverted bell shape, rising from −∞-\infty near x=0x = 0, reaching a peak of −12-\frac{1}{2} at x=1x = 1, then falling back to −∞-\infty.

Part (b): The differential equation describes a family of parabolas

dydx=2xyx2−1\frac{dy}{dx} = \frac{2xy}{x^2 - 1}

Separating variables:

dyy=2xx2−1 dx\frac{dy}{y} = \frac{2x}{x^2 - 1}\,dx

Integrating:

ln⁡∣y∣=ln⁡∣x2−1∣+C\ln|y| = \ln|x^2 - 1| + C

∣y∣=eC∣x2−1∣|y| = e^C |x^2 - 1|

y=A(x2−1)y = A(x^2 - 1)

where AA is an arbitrary constant. This is a family of parabolas y=A(x2−1)y = A(x^2 - 1), each with vertex at (0,−A)(0, -A) (on the yy-axis) and each passing through (1,0)(1, 0) and (−1,0)(-1, 0). ■\blacksquare

Part (c): Orthogonal trajectory through (1,1)(1, 1)

For the family y=A(x2−1)y = A(x^2 - 1), the slope is dydx=2Ax\frac{dy}{dx} = 2Ax. The orthogonal trajectory has slope −12Ax=−x2−12xy-\frac{1}{2Ax} = -\frac{x^2 - 1}{2xy} (using A=yx2−1A = \frac{y}{x^2 - 1}).

So the orthogonal trajectory satisfies:

dydx=−x2−12xy\frac{dy}{dx} = -\frac{x^2 - 1}{2xy}

Separating variables:

2y dy=−x2−1x dx=(−x+1x)dx2y\,dy = -\frac{x^2 - 1}{x}\,dx = \left(-x + \frac{1}{x}\right) dx

Integrating:

y2=−x22+ln⁡∣x∣+Cy^2 = -\frac{x^2}{2} + \ln|x| + C

Since we need the curve to pass through (1,1)(1, 1):

1=−12+ln⁡1+C  ⟹  C=321 = -\frac{1}{2} + \ln 1 + C \implies C = \frac{3}{2}

The orthogonal trajectory is:

y2+x22−ln⁡x=32(x>0)y^2 + \frac{x^2}{2} - \ln x = \frac{3}{2} \qquad (x > 0)

or equivalently:

y=±32−x22+ln⁡xy = \pm\sqrt{\frac{3}{2} - \frac{x^2}{2} + \ln x}

Substitution confirms that (1,1)(1,1) lies on the curve. The slope of the orthogonal trajectory at (1,1)(1,1) is 00, as given by dydx=−x2−12xy\frac{dy}{dx}=-\frac{x^2-1}{2xy}.

Sketch. The curve is symmetric about the xx-axis. It exists for x>0x > 0 where 32−x22+ln⁡x⩾0\frac{3}{2} - \frac{x^2}{2} + \ln x \geqslant 0. This expression tends to −∞-\infty as x→0+x\to0^+ and also as x→∞x\to\infty, and has its maximum at x=1x=1. Hence the curve is a closed loop passing through (1,±1)(1,\pm1), with two positive xx-intercepts determined by 32−x22+ln⁡x=0\frac{3}{2} - \frac{x^2}{2} + \ln x = 0.


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

8 (i) Prove that the equations ∣z−(1+i)∣2=2(*)|z - (1 + i)|^2 = 2 \qquad \text{(*)} and ∣z−(1−i)∣2=2∣z−1∣2|z - (1 - i)|^2 = 2|z - 1|^2 describe the same locus in the complex zz-plane. Sketch this locus.

(ii) Prove that the equation arg⁡(z−2z)=π4(**)\arg\left(\frac{z - 2}{z}\right) = \frac{\pi}{4} \qquad \text{(**)} describes part of this same locus, and show on your sketch which part.

(iii) The complex number ww is related to zz by w=2z.w = \frac{2}{z} . Determine the locus produced in the complex ww-plane if zz satisfies (*). Sketch this locus and indicate the part of this locus that corresponds to (**).

Model Solution

Part (i): The two equations describe the same locus

Let z=x+iyz = x + iy.

Equation (*): ∣z−(1+i)∣2=2|z - (1+i)|^2 = 2

(x−1)2+(y−1)2=2(x - 1)^2 + (y - 1)^2 = 2

x2+y2−2x−2y=0(I)x^2 + y^2 - 2x - 2y = 0 \qquad \text{(I)}

Second equation: ∣z−(1−i)∣2=2∣z−1∣2|z - (1-i)|^2 = 2|z - 1|^2

(x−1)2+(y+1)2=2(x−1)2+2y2(x - 1)^2 + (y + 1)^2 = 2(x - 1)^2 + 2y^2

x2−2x+1+y2+2y+1=2x2−4x+2+2y2x^2 - 2x + 1 + y^2 + 2y + 1 = 2x^2 - 4x + 2 + 2y^2

0=x2+y2−2x−2y0 = x^2 + y^2 - 2x - 2y

This is identical to (I). Therefore both equations describe the same locus: a circle centred at (1,1)(1, 1) with radius 2\sqrt{2}. ■\blacksquare

Sketch. The circle passes through the origin and through (2,0)(2, 0), (0,2)(0, 2), and (2,2)(2, 2).

Part (ii): The arg equation describes part of this locus

Let z=x+iyz = x + iy. We compute:

z−2z=(x−2)+iyx+iy\frac{z - 2}{z} = \frac{(x - 2) + iy}{x + iy}

Multiplying numerator and denominator by the conjugate of the denominator:

=[(x−2)+iy](x−iy)x2+y2= \frac{[(x-2) + iy](x - iy)}{x^2 + y^2}

Numerator: (x−2)x+y2+i[yx−(x−2)y]=(x2−2x+y2)+i(2y)(x-2)x + y^2 + i[yx - (x-2)y] = (x^2 - 2x + y^2) + i(2y)

z−2z=x2+y2−2xx2+y2+i2yx2+y2\frac{z - 2}{z} = \frac{x^2 + y^2 - 2x}{x^2 + y^2} + i\frac{2y}{x^2 + y^2}

The condition arg⁡(z−2z)=π4\arg\left(\frac{z-2}{z}\right) = \frac{\pi}{4} requires:

Im=Re>0\text{Im} = \text{Re} > 0

Setting Im == Re:

2yx2+y2=x2+y2−2xx2+y2\frac{2y}{x^2 + y^2} = \frac{x^2 + y^2 - 2x}{x^2 + y^2}

2y=x2+y2−2x2y = x^2 + y^2 - 2x

(x−1)2+(y−1)2=2(x - 1)^2 + (y - 1)^2 = 2

This is exactly the circle from part (i). ■\blacksquare

The additional constraint Re >0> 0 gives x2+y2−2x>0x^2+y^2-2x>0. On the circle from part (i), this is equivalent to 2y>02y>0, so y>0y>0. Thus (**) describes the upper arc of the circle from z=0z=0 to z=2z=2, with both endpoints excluded because the argument is undefined there.

Part (iii): Locus in the ww-plane

Given w=2zw = \frac{2}{z}, so z=2w=2wˉ∣w∣2z = \frac{2}{w} = \frac{2\bar{w}}{|w|^2}. With w=u+ivw = u + iv:

z=2(u−iv)u2+v2=2uu2+v2−i2vu2+v2z = \frac{2(u - iv)}{u^2 + v^2} = \frac{2u}{u^2 + v^2} - i\frac{2v}{u^2 + v^2}

Substituting into equation (*): ∣z−(1+i)∣2=2|z - (1+i)|^2 = 2, i.e., (x−1)2+(y−1)2=2(x-1)^2 + (y-1)^2 = 2 where x=2uu2+v2x = \frac{2u}{u^2+v^2}, y=−2vu2+v2y = \frac{-2v}{u^2+v^2}:

(2uu2+v2−1)2+(−2vu2+v2−1)2=2\left(\frac{2u}{u^2+v^2} - 1\right)^2 + \left(\frac{-2v}{u^2+v^2} - 1\right)^2 = 2

Let r2=u2+v2r^2 = u^2 + v^2. Expanding:

(2u−r2)2+(2v+r2)2r4=2\frac{(2u - r^2)^2 + (2v + r^2)^2}{r^4} = 2

(2u−r2)2+(2v+r2)2=2r4(2u - r^2)^2 + (2v + r^2)^2 = 2r^4

Expanding the left side:

4u2−4ur2+r4+4v2+4vr2+r4=2r44u^2 - 4ur^2 + r^4 + 4v^2 + 4vr^2 + r^4 = 2r^4

4(u2+v2)−4r2(u−v)+2r4=2r44(u^2 + v^2) - 4r^2(u - v) + 2r^4 = 2r^4

4r2−4r2(u−v)=04r^2 - 4r^2(u - v) = 0

Since r2≠0r^2 \neq 0 (as z≠0z \neq 0):

1−(u−v)=0  ⟹  u−v=11 - (u - v) = 0 \implies u - v = 1

The locus is the line u−v=1u - v = 1, i.e., Re⁡(w)−Im⁡(w)=1\operatorname{Re}(w) - \operatorname{Im}(w) = 1. ■\blacksquare

Sketch. This is a straight line in the ww-plane passing through (1,0)(1, 0) and (0,−1)(0, -1) with gradient 11.

Which part corresponds to () :**

For the arc in part (ii), z=x+iyz=x+iy lies on the circle with y>0y>0. Since w=2/zw=2/z, we have

v=Im⁡(w)=−2yx2+y2<0.v=\operatorname{Im}(w)=-\frac{2y}{x^2+y^2}<0.

Thus the corresponding part of the line is

u−v=1,v<0,u-v=1,\qquad v<0,

with endpoint (1,0)(1,0) excluded and the other endpoint approached at (0,−1)(0,-1) as z→0z\to0 along the arc.