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STEP3 2011 -- Pure Mathematics

Exam: STEP3  |  Year: 2011  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1微分方程 Differential EquationsStandard变量代换, 积分因子, 降阶法
2代数 AlgebraStandard有理根定理, 反证法, 整除性分析
3代数 AlgebraChallenging三次多项式分解, 复数单位根, 代数恒等式
4分析 AnalysisChallengingYoung不等式, 积分性质, 反三角函数
5几何与力学 Geometry and MechanicsHard参数方程, 扫掠面积公式, 三角积分
6积分 Integral CalculusChallenging变量代换, 双曲函数恒等式, artanh 与对数关系
7数论与代数 Number Theory & AlgebraChallenging数学归纳法, 二项展开, Pell 方程结构
8复数 Complex NumbersChallengingMöbius 变换, 实虚部分离, 半角代换 tan(θ/2), 轨迹分析

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

1 (i) Find the general solution of the differential equation dudx−(x+2x+1)u=0.\frac{\mathrm{d}u}{\mathrm{d}x} - \left( \frac{x + 2}{x + 1} \right) u = 0 .

(ii) Show that substituting y=ze−xy = ze^{-x} (where zz is a function of xx) into the second order differential equation (x+1)d2ydx2+xdydx−y=0(*)(x + 1) \frac{\mathrm{d}^2y}{\mathrm{d}x^2} + x \frac{\mathrm{d}y}{\mathrm{d}x} - y = 0 \qquad \text{(*)} leads to a first order differential equation for dzdx\frac{\mathrm{d}z}{\mathrm{d}x}. Find zz and hence show that the general solution of (∗)(*) is y=Ax+Be−x,y = Ax + Be^{-x} , where AA and BB are arbitrary constants.

(iii) Find the general solution of the differential equation (x+1)d2ydx2+xdydx−y=(x+1)2.(x + 1) \frac{\mathrm{d}^2y}{\mathrm{d}x^2} + x \frac{\mathrm{d}y}{\mathrm{d}x} - y = (x + 1)^2 .

Hint
  1. (i) The differential equation can be solved either by separating variables or using an integrating factor. In either case, ∫(x+2x+1)dx\int \left( \frac{x+2}{x+1} \right) dx, or the negative of it is required, and this can be found either by re-writing (x+2x+1)\left( \frac{x+2}{x+1} \right) as 1+1x+11 + \frac{1}{x+1} or using the substitution, v=x+1v = x + 1. Thus the solution is u=k(x+1)exu = k(x + 1)e^x.

(ii) The substitution y=ze−xy = ze^{-x} yields dydx=z′e−x−ze−x\frac{dy}{dx} = z'e^{-x} - ze^{-x}, and d2ydx2=z′′e−x−2z′e−x+ze−x\frac{d^2y}{dx^2} = z''e^{-x} - 2z'e^{-x} + ze^{-x}.

Substituting these expressions in the differential equation and simplifying gives

((x+1)z′′−(x+2)z′)e−x=0((x + 1)z'' - (x + 2)z')e^{-x} = 0 which is effectively the first order differential equation from part (i) with u=z′u = z'.

So z′=k(x+1)exz' = k(x + 1)e^x, which is an exact differential (or integration by parts could be used), z=kxex+cz = kxe^x + c and so y=Ax+Be−xy = Ax + Be^{-x} as required.

(iii) Part (ii)’s substitution gives z′′−(x+2)(x+1)z′=(x+1)exz'' - \frac{(x+2)}{(x+1)}z' = (x + 1)e^x which using the integrating factor from part (i) gives e−xx+1z′=∫1dx=x+c\frac{e^{-x}}{x+1}z' = \int 1 dx = x + c, and thus

y=(x2+1)+Ax+Be−xy = (x^2 + 1) + Ax + Be^{-x}. Alternatively, the solution to part (ii) is the complementary function and a quadratic particular integral should be conjectured, which in view of the cf need only be y=Cx2+Dy = Cx^2 + D, yielding the same result.

Model Solution

Part (i)

The equation is first-order linear. Separating variables:

dudx=x+2x+1 u\frac{\mathrm{d}u}{\mathrm{d}x} = \frac{x + 2}{x + 1} \, u

∫duu=∫x+2x+1 dx\int \frac{\mathrm{d}u}{u} = \int \frac{x + 2}{x + 1} \, \mathrm{d}x

We simplify the integrand: x+2x+1=1+1x+1\frac{x + 2}{x + 1} = 1 + \frac{1}{x + 1}, so

ln⁡∣u∣=x+ln⁡∣x+1∣+const\ln |u| = x + \ln|x + 1| + \text{const}

u=k(x+1)exu = k(x + 1)e^x

where kk is an arbitrary constant.

Part (ii)

Let y=ze−xy = ze^{-x}. Then:

dydx=z′e−x−ze−x=(z′−z)e−x\frac{\mathrm{d}y}{\mathrm{d}x} = z'e^{-x} - ze^{-x} = (z' - z)e^{-x}

d2ydx2=(z′′−z′)e−x−(z′−z)e−x=(z′′−2z′+z)e−x\frac{\mathrm{d}^2y}{\mathrm{d}x^2} = (z'' - z')e^{-x} - (z' - z)e^{-x} = (z'' - 2z' + z)e^{-x}

Substituting into (x+1)d2ydx2+xdydx−y=0(x + 1)\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + x\frac{\mathrm{d}y}{\mathrm{d}x} - y = 0:

(x+1)(z′′−2z′+z)e−x+x(z′−z)e−x−ze−x=0(x + 1)(z'' - 2z' + z)e^{-x} + x(z' - z)e^{-x} - ze^{-x} = 0

Dividing through by e−xe^{-x}:

(x+1)z′′−2(x+1)z′+(x+1)z+xz′−xz−z=0(x + 1)z'' - 2(x + 1)z' + (x + 1)z + xz' - xz - z = 0

Collecting terms:

(x+1)z′′+[−2(x+1)+x]z′+[(x+1)−x−1]z=0(x + 1)z'' + [-2(x + 1) + x]z' + [(x + 1) - x - 1]z = 0

(x+1)z′′−(x+2)z′=0(x + 1)z'' - (x + 2)z' = 0

This is a first-order equation in z′z', which is exactly the equation from part (i) with u=z′u = z'. So:

z′=k(x+1)exz' = k(x + 1)e^x

Integrating (by parts, with u=x+1u = x + 1, dv=exdx\mathrm{d}v = e^x \mathrm{d}x):

z=k∫(x+1)ex dx=k[xex]+c=kxex+cz = k \int (x + 1)e^x \, \mathrm{d}x = k[xe^x] + c = kxe^x + c

Therefore y=ze−x=kx+ce−xy = ze^{-x} = kx + ce^{-x}, i.e.,

y=Ax+Be−xy = Ax + Be^{-x}

where AA and BB are arbitrary constants.

Part (iii)

Using the same substitution y=ze−xy = ze^{-x}, the left-hand side of

(x+1)d2ydx2+xdydx−y=(x+1)2(x + 1)\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + x\frac{\mathrm{d}y}{\mathrm{d}x} - y = (x + 1)^2

reduces (as in part (ii)) to [(x+1)z′′−(x+2)z′]e−x[(x + 1)z'' - (x + 2)z']e^{-x}. So:

[(x+1)z′′−(x+2)z′]e−x=(x+1)2[(x + 1)z'' - (x + 2)z']e^{-x} = (x + 1)^2

(x+1)z′′−(x+2)z′=(x+1)2ex(x + 1)z'' - (x + 2)z' = (x + 1)^2 e^x

Setting u=z′u = z':

u′−x+2x+1u=(x+1)exu' - \frac{x + 2}{x + 1} u = (x + 1)e^x

The integrating factor is e−xx+1\frac{e^{-x}}{x + 1} (from part (i)). Multiplying through:

ddx(e−xx+1u)=1\frac{\mathrm{d}}{\mathrm{d}x}\left( \frac{e^{-x}}{x + 1} u \right) = 1

e−xx+1u=x+c1\frac{e^{-x}}{x + 1} u = x + c_1

u=(x+c1)(x+1)exu = (x + c_1)(x + 1)e^x

Since u=z′u = z', integrating:

z=∫(x+c1)(x+1)ex dx=∫(x2+(c1+1)x+c1)ex dxz = \int (x + c_1)(x + 1)e^x \, \mathrm{d}x = \int (x^2 + (c_1 + 1)x + c_1)e^x \, \mathrm{d}x

Using ∫xex dx=xex−ex\int xe^x \, \mathrm{d}x = xe^x - e^x and ∫x2ex dx=(x2−2x+2)ex\int x^2 e^x \, \mathrm{d}x = (x^2 - 2x + 2)e^x:

z=(x2−2x+2)ex+(c1+1)(xex−ex)+c1ex+c2z = (x^2 - 2x + 2)e^x + (c_1 + 1)(xe^x - e^x) + c_1 e^x + c_2

=[x2−2x+2+(c1+1)x−(c1+1)+c1]ex+c2= \left[ x^2 - 2x + 2 + (c_1 + 1)x - (c_1 + 1) + c_1 \right] e^x + c_2

=[x2+(c1−1)x+1]ex+c2= \left[ x^2 + (c_1 - 1)x + 1 \right] e^x + c_2

Therefore y=ze−x=x2+(c1−1)x+1+c2e−xy = ze^{-x} = x^2 + (c_1 - 1)x + 1 + c_2 e^{-x}.

Setting A=c1−1A = c_1 - 1 and B=c2B = c_2:

y=(x2+1)+Ax+Be−xy = (x^2 + 1) + Ax + Be^{-x}

where AA and BB are arbitrary constants.

Examiner Notes

As might be expected, this was a very popular question, in fact the most popular being attempted by very nearly all the candidates. Fortunately, it was also generally well-attempted, with scores well above those for other questions. Apart from frequent algebraic errors and overlooking terms, especially when using results from a previous part that required adaptation, the main difficulties were in showing that (*) in part (ii) did indeed lead to a first order differential equation in dzdx\frac{dz}{dx}, and the consequent solution of that equation. Part (iii) was generally well done. At the other end of the scale, some candidates did leave their answers to part (i) in the form ln⁡u=\ln u =.


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

2 The polynomial f(x)f(x) is defined by f(x)=xn+an−1xn−1+⋯+a2x2+a1x+a0,f(x) = x^n + a_{n-1}x^{n-1} + \dots + a_2x^2 + a_1x + a_0 , where n⩾2n \geqslant 2 and the coefficients a0,…,an−1a_0, \dots, a_{n-1} are integers, with a0≠0a_0 \neq 0. Suppose that the equation f(x)=0f(x) = 0 has a rational root p/qp/q, where pp and qq are integers with no common factor greater than 1, and q>0q > 0. By considering qn−1f(p/q)q^{n-1}f(p/q), find the value of qq and deduce that any rational root of the equation f(x)=0f(x) = 0 must be an integer.

(i) Show that the nnth root of 2 is irrational for n⩾2n \geqslant 2.

(ii) Show that the cubic equation x3−x+1=0x^3 - x + 1 = 0 has no rational roots.

(iii) Show that the polynomial equation xn−5x+7=0x^n - 5x + 7 = 0 has no rational roots for n⩾2n \geqslant 2.

Hint
  1. Parts (ii) and (iii) could be shown by applying the stem and then considering the left hand side of each equation for the cases nn even and nn odd.
Model Solution

Stem. Suppose f(x)=xn+an−1xn−1+⋯+a1x+a0f(x) = x^n + a_{n-1}x^{n-1} + \dots + a_1 x + a_0 has a rational root p/qp/q where gcd⁡(p,q)=1\gcd(p, q) = 1 and q>0q > 0. Then f(p/q)=0f(p/q) = 0:

pnqn+an−1pn−1qn−1+⋯+a1pq+a0=0\frac{p^n}{q^n} + a_{n-1}\frac{p^{n-1}}{q^{n-1}} + \dots + a_1 \frac{p}{q} + a_0 = 0

Multiplying by qn−1q^{n-1}:

pnq+an−1pn−1+an−2pn−2q+⋯+a1pqn−2+a0qn−1=0\frac{p^n}{q} + a_{n-1}p^{n-1} + a_{n-2}p^{n-2}q + \dots + a_1 pq^{n-2} + a_0 q^{n-1} = 0

All terms except the first are integers, so pnq\frac{p^n}{q} must be an integer. Since gcd⁡(p,q)=1\gcd(p, q) = 1, we have gcd⁡(pn,q)=1\gcd(p^n, q) = 1, so q=1q = 1. Therefore any rational root of f(x)=0f(x) = 0 must be an integer, and by the factor theorem it must divide a0a_0.

Part (i)

Suppose 2n\sqrt[n]{2} is rational for some n⩾2n \geqslant 2. Then x=2nx = \sqrt[n]{2} satisfies xn−2=0x^n - 2 = 0, which is a monic polynomial with integer coefficients and constant term −2≠0-2 \neq 0. By the stem, any rational root must be an integer dividing −2-2, i.e., x∈{1,−1,2,−2}x \in \{1, -1, 2, -2\}.

  • x=1x = 1: 1−2=−1≠01 - 2 = -1 \neq 0.
  • x=−1x = -1: (−1)n−2(-1)^n - 2. For nn even this is −1-1, for nn odd this is −3-3. Neither is zero.
  • x=2x = 2: 2n−2⩾22^n - 2 \geqslant 2 for n⩾2n \geqslant 2. Not zero.
  • x=−2x = -2: (−2)n−2(-2)^n - 2. For n=2n = 2 this is 22; for n⩾3n \geqslant 3, ∣(−2)n∣⩾8>2|(-2)^n| \geqslant 8 > 2. Not zero.

None of the candidates is a root, so 2n\sqrt[n]{2} is irrational for all n⩾2n \geqslant 2.

Part (ii)

The equation x3−x+1=0x^3 - x + 1 = 0 is monic with integer coefficients and constant term 11. By the stem, any rational root must be an integer dividing 11, so x=1x = 1 or x=−1x = -1.

  • x=1x = 1: 1−1+1=1≠01 - 1 + 1 = 1 \neq 0.
  • x=−1x = -1: −1+1+1=1≠0-1 + 1 + 1 = 1 \neq 0.

So x3−x+1=0x^3 - x + 1 = 0 has no rational roots.

Part (iii)

The equation xn−5x+7=0x^n - 5x + 7 = 0 is monic with integer coefficients and constant term 77. By the stem, any rational root must be an integer dividing 77, so x∈{1,−1,7,−7}x \in \{1, -1, 7, -7\}.

  • x=1x = 1: 1−5+7=3≠01 - 5 + 7 = 3 \neq 0.
  • x=−1x = -1: (−1)n+5+7(-1)^n + 5 + 7. For nn even this is 1313; for nn odd this is 1111. Neither is zero.
  • x=7x = 7: 7n−35+7=7n−287^n - 35 + 7 = 7^n - 28. For n=2n = 2: 49−28=21≠049 - 28 = 21 \neq 0. For n⩾3n \geqslant 3: 7n⩾3437^n \geqslant 343, so 7n−28>07^n - 28 > 0. Not zero.
  • x=−7x = -7: (−7)n+35+7=(−7)n+42(-7)^n + 35 + 7 = (-7)^n + 42. For nn even: 7n+42>07^n + 42 > 0. For nn odd: −7n+42-7^n + 42. For n=2n = 2: 49+42>049 + 42 > 0. For n⩾3n \geqslant 3: 7n⩾343>427^n \geqslant 343 > 42, so −7n+42<0-7^n + 42 < 0. Not zero.

None of the candidates is a root, so xn−5x+7=0x^n - 5x + 7 = 0 has no rational roots for n⩾2n \geqslant 2.

Examiner Notes
  1. Of the attempts, about a third were close to completely correct, and nearly all the others were barely doing more than grasping at crumbs, reflecting the fact that candidates either did or did not know what they were doing. There was negligible middle ground.

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

3 Show that, provided q2≠4p3q^2 \neq 4p^3, the polynomial

x3−3px+q(p≠0, q≠0)x^3 - 3px + q \qquad (p \neq 0, \ q \neq 0)

can be written in the form

a(x−α)3+b(x−β)3,a(x - \alpha)^3 + b(x - \beta)^3 ,

where α\alpha and β\beta are the roots of the quadratic equation pt2−qt+p2=0pt^2 - qt + p^2 = 0, and aa and bb are constants which you should express in terms of α\alpha and β\beta.

Hence show that one solution of the equation x3−24x+48=0x^3 - 24x + 48 = 0 is

x=2(2−213)1−213x = \frac{2(2 - 2^{\frac{1}{3}})}{1 - 2^{\frac{1}{3}}}

and obtain similar expressions for the other two solutions in terms of ω\omega, where ω=e2πi/3\omega = e^{2\pi i/3}.

Find also the roots of x3−3px+q=0x^3 - 3px + q = 0 when p=r2p = r^2 and q=2r3q = 2r^3 for some non-zero constant rr.

Hint
  1. Considering the quadratic equation pt2−qt+p2=0pt^2 - qt + p^2 = 0, the condition q2≠4p3q^2 \neq 4p^3 shows, by considering the discriminant, that the roots are unequal. Supposing that x3−3px+qx^3 - 3px + q can be written as a(x−α)3+b(x−β)3a(x - \alpha)^3 + b(x - \beta)^3, and equating coefficients generates the four equations a+b=1a + b = 1 −3aα−3bβ=0-3a\alpha - 3b\beta = 0 3α2a+3β2b=−3p3\alpha^2 a + 3\beta^2 b = -3p −α3a−β3b=q-\alpha^3 a - \beta^3 b = q

The first pair may be solved simultaneously to give a=−βα−βa = \frac{-\beta}{\alpha - \beta} and b=αα−βb = \frac{\alpha}{\alpha - \beta}. Substitution yields p=αβp = \alpha\beta and q=αβ(α+β)q = \alpha\beta(\alpha + \beta), or alternatively, αβ=p\alpha\beta = p and α+β=qp\alpha + \beta = \frac{q}{p} and so α\alpha and β\beta satisfy t2−qpt+p=0t^2 - \frac{q}{p}t + p = 0 i.e. pt2−qt+p2=0pt^2 - qt + p^2 = 0. For p=8p = 8, q=48q = 48, q2−4p3=28≠0q^2 - 4p^3 = 2^8 \neq 0. Hence α\alpha and β\beta are the roots of 8t2−48t+64=08t^2 - 48t + 64 = 0, i.e. t2−6t+8=0t^2 - 6t + 8 = 0 and wlog α=2\alpha = 2, β=4\beta = 4, a=2a = 2, b=−1b = -1. So x3−24x+48=0x^3 - 24x + 48 = 0 can be re-arranged as (x−4x−2)3=2\left(\frac{x-4}{x-2}\right)^3 = 2

As ω3=1\omega^3 = 1, x−4x−2=23\frac{x-4}{x-2} = \sqrt[3]{2}, ω23\omega\sqrt[3]{2}, ω223\omega^2\sqrt[3]{2} and so x=2(2−23)1−23,2(2−ω23)1−ω23,2(2−ω223)1−ω223x = \frac{2(2-\sqrt[3]{2})}{1-\sqrt[3]{2}}, \frac{2(2-\omega\sqrt[3]{2})}{1-\omega\sqrt[3]{2}}, \frac{2(2-\omega^2\sqrt[3]{2})}{1-\omega^2\sqrt[3]{2}}

If q=2r3q = 2r^3 and p=r2p = r^2, q2=4p3q^2 = 4p^3 so the first part cannot be used. However, x3−3r2x+2r3=0x^3 - 3r^2x + 2r^3 = 0 can be readily factorised as (x−r)2(x+2r)=0(x - r)^2(x + 2r) = 0 and so x=rx = r (repeated) or −2r-2r

Model Solution

Part 1: Expressing the cubic in the required form

Suppose x3−3px+q=a(x−α)3+b(x−β)3x^3 - 3px + q = a(x - \alpha)^3 + b(x - \beta)^3. Expanding the right-hand side:

a(x−α)3+b(x−β)3=a(x3−3αx2+3α2x−α3)+b(x3−3βx2+3β2x−β3)a(x - \alpha)^3 + b(x - \beta)^3 = a(x^3 - 3\alpha x^2 + 3\alpha^2 x - \alpha^3) + b(x^3 - 3\beta x^2 + 3\beta^2 x - \beta^3)

=(a+b)x3−3(aα+bβ)x2+3(aα2+bβ2)x−(aα3+bβ3).= (a + b)x^3 - 3(a\alpha + b\beta)x^2 + 3(a\alpha^2 + b\beta^2)x - (a\alpha^3 + b\beta^3).

Equating coefficients with x3−3px+qx^3 - 3px + q:

a+b=1⋯(1)a + b = 1 \qquad \cdots (1) aα+bβ=0⋯(2)a\alpha + b\beta = 0 \qquad \cdots (2) aα2+bβ2=−p⋯(3)a\alpha^2 + b\beta^2 = -p \qquad \cdots (3) −(aα3+bβ3)=q⋯(4)-(a\alpha^3 + b\beta^3) = q \qquad \cdots (4)

From equation (2), a=−bβ/αa = -b\beta/\alpha (assuming α≠0\alpha \neq 0, which holds since αβ=p≠0\alpha\beta = p \neq 0). Substituting into (1):

−bβα+b=1  ⟹  b(α−βα)=1  ⟹  b=αα−β.-\frac{b\beta}{\alpha} + b = 1 \implies b\left(\frac{\alpha - \beta}{\alpha}\right) = 1 \implies b = \frac{\alpha}{\alpha - \beta}.

Then a=1−b=−βα−βa = 1 - b = \frac{-\beta}{\alpha - \beta}.

We need α≠β\alpha \neq \beta for these to be well-defined. The discriminant of pt2−qt+p2=0pt^2 - qt + p^2 = 0 is q2−4p3q^2 - 4p^3, so q2≠4p3q^2 \neq 4p^3 guarantees distinct roots.

Verifying equations (3) and (4) and finding the quadratic for α,β\alpha, \beta:

From equation (2), aα+bβ=0a\alpha + b\beta = 0, so aα=−bβa\alpha = -b\beta.

For equation (3): aα2+bβ2=α(aα)+β(bβ)=α(−bβ)+β(bβ)=bβ(β−α)a\alpha^2 + b\beta^2 = \alpha(a\alpha) + \beta(b\beta) = \alpha(-b\beta) + \beta(b\beta) = b\beta(\beta - \alpha).

Substituting b=αα−βb = \frac{\alpha}{\alpha - \beta}:

bβ(β−α)=αβ(β−α)α−β=−αβ.b\beta(\beta - \alpha) = \frac{\alpha\beta(\beta - \alpha)}{\alpha - \beta} = -\alpha\beta.

So equation (3) gives −αβ=−p-\alpha\beta = -p, hence αβ=p\alpha\beta = p.

For equation (4): aα3+bβ3=α2(aα)+β2(bβ)=α2(−bβ)+β2(bβ)=bβ(β2−α2)=bβ(β−α)(β+α)a\alpha^3 + b\beta^3 = \alpha^2(a\alpha) + \beta^2(b\beta) = \alpha^2(-b\beta) + \beta^2(b\beta) = b\beta(\beta^2 - \alpha^2) = b\beta(\beta - \alpha)(\beta + \alpha).

bβ(β−α)(β+α)=αβ(β−α)(β+α)α−β=−αβ(α+β)=−p(α+β).b\beta(\beta - \alpha)(\beta + \alpha) = \frac{\alpha\beta(\beta - \alpha)(\beta + \alpha)}{\alpha - \beta} = -\alpha\beta(\alpha + \beta) = -p(\alpha + \beta).

So equation (4) gives −(−p(α+β))=q-(-p(\alpha + \beta)) = q, hence p(α+β)=qp(\alpha + \beta) = q, giving α+β=q/p\alpha + \beta = q/p.

Since αβ=p\alpha\beta = p and α+β=q/p\alpha + \beta = q/p, the numbers α\alpha and β\beta are roots of:

t2−qpt+p=0  ⟺  pt2−qt+p2=0.t^2 - \frac{q}{p}t + p = 0 \iff pt^2 - qt + p^2 = 0.

This completes the proof that x3−3px+q=a(x−α)3+b(x−β)3x^3 - 3px + q = a(x - \alpha)^3 + b(x - \beta)^3 where α,β\alpha, \beta are roots of pt2−qt+p2=0pt^2 - qt + p^2 = 0, with a=−βα−βa = \frac{-\beta}{\alpha - \beta} and b=αα−βb = \frac{\alpha}{\alpha - \beta}.

Part 2: Solving x3−24x+48=0x^3 - 24x + 48 = 0

Here p=8p = 8 and q=48q = 48. We check q2−4p3=2304−2048=256≠0q^2 - 4p^3 = 2304 - 2048 = 256 \neq 0, so the result applies.

The quadratic for α,β\alpha, \beta is 8t2−48t+64=08t^2 - 48t + 64 = 0, i.e., t2−6t+8=0t^2 - 6t + 8 = 0, giving (t−2)(t−4)=0(t-2)(t-4) = 0.

Taking α=2\alpha = 2 and β=4\beta = 4:

a=−42−4=2,b=22−4=−1.a = \frac{-4}{2 - 4} = 2, \qquad b = \frac{2}{2 - 4} = -1.

So the equation becomes:

2(x−2)3−(x−4)3=0  ⟹  (x−4)3=2(x−2)3.2(x - 2)^3 - (x - 4)^3 = 0 \implies (x - 4)^3 = 2(x - 2)^3.

Provided x≠2x \neq 2, we divide:

(x−4x−2)3=2  ⟹  x−4x−2=21/3ωk,k=0,1,2,\left(\frac{x - 4}{x - 2}\right)^3 = 2 \implies \frac{x - 4}{x - 2} = 2^{1/3}\omega^k, \quad k = 0, 1, 2,

where ω=e2πi/3\omega = e^{2\pi i/3} is a primitive cube root of unity.

Solving x−4x−2=c\frac{x - 4}{x - 2} = c for xx: x−4=c(x−2)x - 4 = c(x - 2), so x(1−c)=4−2cx(1 - c) = 4 - 2c, giving x=4−2c1−c=2(2−c)1−cx = \frac{4 - 2c}{1 - c} = \frac{2(2 - c)}{1 - c}.

For k=0k = 0: c=21/3c = 2^{1/3}, so

x=2(2−21/3)1−21/3.x = \frac{2(2 - 2^{1/3})}{1 - 2^{1/3}}.

For k=1k = 1: c=ω⋅21/3c = \omega \cdot 2^{1/3}, so

x=2(2−ω⋅21/3)1−ω⋅21/3.x = \frac{2(2 - \omega \cdot 2^{1/3})}{1 - \omega \cdot 2^{1/3}}.

For k=2k = 2: c=ω2⋅21/3c = \omega^2 \cdot 2^{1/3}, so

x=2(2−ω2⋅21/3)1−ω2⋅21/3.x = \frac{2(2 - \omega^2 \cdot 2^{1/3})}{1 - \omega^2 \cdot 2^{1/3}}.

Part 3: Finding roots when p=r2p = r^2 and q=2r3q = 2r^3

Here q2−4p3=4r6−4r6=0q^2 - 4p^3 = 4r^6 - 4r^6 = 0, so the method above does not apply (the quadratic has a repeated root). Instead, we factorise directly:

x3−3r2x+2r3=0.x^3 - 3r^2 x + 2r^3 = 0.

Testing x=rx = r: r3−3r3+2r3=0r^3 - 3r^3 + 2r^3 = 0. So (x−r)(x - r) is a factor. Performing the division:

x3−3r2x+2r3=(x−r)(x2+rx−2r2)=(x−r)(x−r)(x+2r)=(x−r)2(x+2r).x^3 - 3r^2 x + 2r^3 = (x - r)(x^2 + rx - 2r^2) = (x - r)(x - r)(x + 2r) = (x - r)^2(x + 2r).

The roots are x=rx = r (repeated) and x=−2rx = -2r.


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

4 The following result applies to any function ff which is continuous, has positive gradient and satisfies f(0)=0f(0) = 0:

ab⩽∫0af(x) dx+∫0bf−1(y) dy,(*)ab \leqslant \int_{0}^{a} f(x) \, dx + \int_{0}^{b} f^{-1}(y) \, dy , \qquad \text{(*)}

where f−1f^{-1} denotes the inverse function of ff, and a⩾0a \geqslant 0 and b⩾0b \geqslant 0.

(i) By considering the graph of y=f(x)y = f(x), explain briefly why the inequality (∗*) holds. In the case a>0a > 0 and b>0b > 0, state a condition on aa and bb under which equality holds.

(ii) By taking f(x)=xp−1f(x) = x^{p-1} in (∗*), where p>1p > 1, show that if 1p+1q=1\frac{1}{p} + \frac{1}{q} = 1 then

ab⩽app+bqq.ab \leqslant \frac{a^p}{p} + \frac{b^q}{q} .

Verify that equality holds under the condition you stated above.

(iii) Show that, for 0⩽a⩽12π0 \leqslant a \leqslant \frac{1}{2}\pi and 0⩽b⩽10 \leqslant b \leqslant 1,

ab⩽barcsin⁡b+1−b2−cos⁡a.ab \leqslant b \arcsin b + \sqrt{1 - b^2} - \cos a .

Deduce that, for t⩾1t \geqslant 1,

arcsin⁡(t−1)⩾t−t2−1.\arcsin(t^{-1}) \geqslant t - \sqrt{t^2 - 1} .

Hint
  1. (i) ∫0af(x)dx\int_0^a f(x)dx is the area between the curve y=f(x)y = f(x), the xx axis, and the line x=ax = a ∫0bf−1(y)dy\int_0^b f^{-1}(y)dy is the area between the curve y=f(x)y = f(x), the yy axis, and the line y=by = b.

The sum of these areas is greater than or equal to the area of the rectangle with corners (0,0)(0,0), (a,0)(a,0), (a,b)(a,b) and (0,b)(0,b), with equality holding if b=f(a)b = f(a).

(ii) With f(x)=xp−1f(x) = x^{p-1}, the sum of the two integrals is 1pap+p−1pbpp−1\frac{1}{p}a^p + \frac{p-1}{p}b^{\frac{p}{p-1}}

But as 1p+1q=1\frac{1}{p} + \frac{1}{q} = 1, 1q=p−1p\frac{1}{q} = \frac{p-1}{p}, and so the required result follows by applying the result of part (i). If b=ap−1b = a^{p-1}, simple algebra shows a=bq−1a = b^{q-1}, so 1pap+1qbq=1pab+1qba=ab\frac{1}{p} a^p + \frac{1}{q} b^q = \frac{1}{p} ab + \frac{1}{q} ba = ab and equality is verified.

(iii) f(x)=sin⁡xf(x) = \sin x satisfies the conditions of part (i) So ∫0af(x)dx=1−cos⁡a\int_0^a f(x) dx = 1 - \cos a, and, by parts, ∫0bf−1(y)dy=bsin⁡−1b+1−b2−1\int_0^b f^{-1}(y) dy = b \sin^{-1} b + \sqrt{1 - b^2} - 1 which together give the required result.

Choosing a=0a = 0, and b=t−1b = t^{-1}, part (i) gives 0≤t−1sin⁡−1(t−1)+1−t−2−10 \le t^{-1} \sin^{-1}(t^{-1}) + \sqrt{1 - t^{-2}} - 1 which can be re-arranged to give the required result.

Model Solution

Part (i)

The integral ∫0af(x) dx\int_0^a f(x) \, \mathrm{d}x is the area between the curve y=f(x)y = f(x), the xx-axis, and the line x=ax = a. The integral ∫0bf−1(y) dy\int_0^b f^{-1}(y) \, \mathrm{d}y is the area between the curve y=f(x)y = f(x), the yy-axis, and the line y=by = b.

Since ff is continuous with positive gradient and f(0)=0f(0) = 0, the function is strictly increasing. The sum of these two areas always covers the rectangle [0,a]×[0,b][0, a] \times [0, b], so:

ab⩽∫0af(x) dx+∫0bf−1(y) dy.ab \leqslant \int_0^a f(x) \, \mathrm{d}x + \int_0^b f^{-1}(y) \, \mathrm{d}y.

Equality holds when b=f(a)b = f(a) (equivalently a=f−1(b)a = f^{-1}(b)), since in this case the two integrals partition the rectangle exactly with no overlap or gap.

Part (ii)

Taking f(x)=xp−1f(x) = x^{p-1} for p>1p > 1. This is continuous with positive gradient for x>0x > 0 and f(0)=0f(0) = 0, so the conditions of (∗*) are satisfied.

The inverse function: y=xp−1y = x^{p-1} gives x=y1/(p−1)=yq−1x = y^{1/(p-1)} = y^{q-1} since 1p+1q=1\frac{1}{p} + \frac{1}{q} = 1 implies q−1=1p−1q - 1 = \frac{1}{p-1}.

Computing the integrals:

∫0axp−1 dx=app\int_0^a x^{p-1} \, \mathrm{d}x = \frac{a^p}{p}

∫0byq−1 dy=bqq\int_0^b y^{q-1} \, \mathrm{d}y = \frac{b^q}{q}

By (∗*):

ab⩽app+bqqab \leqslant \frac{a^p}{p} + \frac{b^q}{q}

Equality check. Equality in (∗*) holds when b=f(a)=ap−1b = f(a) = a^{p-1}, i.e., a=b1/(p−1)=bq−1a = b^{1/(p-1)} = b^{q-1}. Then ap=a⋅ap−1=aba^p = a \cdot a^{p-1} = ab and bq=b⋅bq−1=ba=abb^q = b \cdot b^{q-1} = ba = ab. So:

app+bqq=abp+abq=ab(1p+1q)=ab.\frac{a^p}{p} + \frac{b^q}{q} = \frac{ab}{p} + \frac{ab}{q} = ab\left(\frac{1}{p} + \frac{1}{q}\right) = ab.

Equality is verified.

Part (iii)

Take f(x)=sin⁡xf(x) = \sin x for 0⩽x⩽π20 \leqslant x \leqslant \frac{\pi}{2}. This is continuous with positive gradient and f(0)=0f(0) = 0, so the conditions of (∗*) are satisfied.

The inverse function is f−1(y)=arcsin⁡yf^{-1}(y) = \arcsin y for 0⩽y⩽10 \leqslant y \leqslant 1.

Computing the integrals:

∫0asin⁡x dx=[−cos⁡x]0a=1−cos⁡a\int_0^a \sin x \, \mathrm{d}x = [-\cos x]_0^a = 1 - \cos a

For ∫0barcsin⁡y dy\int_0^b \arcsin y \, \mathrm{d}y, integrate by parts with u=arcsin⁡yu = \arcsin y, dv=dy\mathrm{d}v = \mathrm{d}y:

∫0barcsin⁡y dy=[yarcsin⁡y]0b−∫0by1−y2 dy\int_0^b \arcsin y \, \mathrm{d}y = [y \arcsin y]_0^b - \int_0^b \frac{y}{\sqrt{1 - y^2}} \, \mathrm{d}y

=barcsin⁡b+[1−y2]0b=barcsin⁡b+1−b2−1= b \arcsin b + [\sqrt{1 - y^2}]_0^b = b \arcsin b + \sqrt{1 - b^2} - 1

By (∗*):

ab⩽(1−cos⁡a)+(barcsin⁡b+1−b2−1)ab \leqslant (1 - \cos a) + (b \arcsin b + \sqrt{1 - b^2} - 1)

ab⩽barcsin⁡b+1−b2−cos⁡aab \leqslant b \arcsin b + \sqrt{1 - b^2} - \cos a

Deduction. In this inequality, set a=0a = 0 (which gives 0⩽0 \leqslant something) and b=t−1b = t^{-1} for t⩾1t \geqslant 1 (so 0<b⩽10 < b \leqslant 1). Since a=0a = 0, the left side is 00:

0⩽t−1arcsin⁡(t−1)+1−t−2−10 \leqslant t^{-1} \arcsin(t^{-1}) + \sqrt{1 - t^{-2}} - 1

1⩽t−1arcsin⁡(t−1)+1−t−21 \leqslant t^{-1} \arcsin(t^{-1}) + \sqrt{1 - t^{-2}}

Multiply through by t>0t > 0:

t⩽arcsin⁡(t−1)+t1−t−2t \leqslant \arcsin(t^{-1}) + t\sqrt{1 - t^{-2}}

Since t1−t−2=t2−1t\sqrt{1 - t^{-2}} = \sqrt{t^2 - 1} for t⩾1t \geqslant 1:

t⩽arcsin⁡(t−1)+t2−1t \leqslant \arcsin(t^{-1}) + \sqrt{t^2 - 1}

arcsin⁡(t−1)⩾t−t2−1\arcsin(t^{-1}) \geqslant t - \sqrt{t^2 - 1}


Topic: 几何与力学 Geometry and Mechanics  |  Difficulty: Hard  |  Marks: 20

5 A movable point PP has cartesian coordinates (x,y)(x, y), where xx and yy are functions of tt. The polar coordinates of PP with respect to the origin OO are rr and θ\theta. Starting with the expression

12∫r2 dθ\frac{1}{2} \int r^2 \, \mathrm{d}\theta

for the area swept out by OPOP, obtain the equivalent expression

12∫(xdydt−ydxdt)dt.(*) \frac{1}{2} \int \left( x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t} \right) \mathrm{d}t . \qquad \text{(*)}

The ends of a thin straight rod ABAB lie on a closed convex curve C\mathcal{C}. The point PP on the rod is a fixed distance aa from AA and a fixed distance bb from BB. The angle between ABAB and the positive xx direction is tt. As AA and BB move anticlockwise round C\mathcal{C}, the angle tt increases from 00 to 2π2\pi and PP traces a closed convex curve D\mathcal{D} inside C\mathcal{C}, with the origin OO lying inside D\mathcal{D}, as shown in the diagram.

Let (x,y)(x, y) be the coordinates of PP. Write down the coordinates of AA and BB in terms of a,b,x,ya, b, x, y and tt.

The areas swept out by OA,OBOA, OB and OPOP are denoted by [A],[B][A], [B] and [P][P], respectively. Show, using (∗)(*), that

[A]=[P]+πa2−af[A] = [P] + \pi a^2 - af

where

f=12∫02π((x+dydt)cos⁡t+(y−dxdt)sin⁡t)dt.f = \frac{1}{2} \int_0^{2\pi} \left( \left( x + \frac{\mathrm{d}y}{\mathrm{d}t} \right) \cos t + \left( y - \frac{\mathrm{d}x}{\mathrm{d}t} \right) \sin t \right) \mathrm{d}t .

Obtain a corresponding expression for [B][B] involving bb. Hence show that the area between the curves C\mathcal{C} and D\mathcal{D} is πab\pi ab.

Hint

r2dθ=(x2+y2)ddt(tan⁡−1(yx))dt=(x2+y2)11+(yx)2(xdydt−ydxdt)x2dt=(xdydt−ydxdt)dtr^2 d\theta = (x^2 + y^2) \frac{d}{dt} \left( \tan^{-1} \left( \frac{y}{x} \right) \right) dt = (x^2 + y^2) \frac{1}{1 + \left( \frac{y}{x} \right)^2} \frac{\left( x \frac{dy}{dt} - y \frac{dx}{dt} \right)}{x^2} dt = \left( x \frac{dy}{dt} - y \frac{dx}{dt} \right) dt

and hence integrating gives the result.

A is (x−acos⁡t,y−asin⁡t)(x - a \cos t, y - a \sin t) and B is (x+bcos⁡t,y+bsin⁡t)(x + b \cos t, y + b \sin t)

[A]=12∫02π(x−acos⁡t)(dydt−acos⁡t)−(y−asin⁡t)(dxdt+asin⁡t)dt[A] = \frac{1}{2} \int_0^{2\pi} (x - a \cos t) \left( \frac{dy}{dt} - a \cos t \right) - (y - a \sin t) \left( \frac{dx}{dt} + a \sin t \right) dt using (*) which leads directly to [A]=[P]−af+πa2[A] = [P] - af + \pi a^2.

Replacing −a-a by bb gives [B]=[P]+bf+πb2[B] = [P] + bf + \pi b^2 As [A]=[B][A] = [B], these expressions can be equated to give f=π(a−b)f = \pi(a - b).

The area between curves CC and DD is [A]−[P]=−af+πa2[A] - [P] = -af + \pi a^2 which by substitution gives πab\pi ab as required.

Model Solution

Deriving the Cartesian area formula.

In polar coordinates, r2=x2+y2r^2 = x^2 + y^2 and θ=arctan⁡(y/x)\theta = \arctan(y/x). Differentiating θ\theta with respect to tt:

dθdt=11+(y/x)2⋅xdydt−ydxdtx2=xdydt−ydxdtx2+y2\frac{\mathrm{d}\theta}{\mathrm{d}t} = \frac{1}{1 + (y/x)^2} \cdot \frac{x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t}}{x^2} = \frac{x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t}}{x^2 + y^2}

So:

r2 dθ=(x2+y2)⋅xdydt−ydxdtx2+y2 dt=(xdydt−ydxdt)dtr^2 \, \mathrm{d}\theta = (x^2 + y^2) \cdot \frac{x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t}}{x^2 + y^2} \, \mathrm{d}t = \left( x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t} \right) \mathrm{d}t

Therefore:

12∫r2 dθ=12∫(xdydt−ydxdt)dt(*)\frac{1}{2}\int r^2 \, \mathrm{d}\theta = \frac{1}{2}\int \left( x \frac{\mathrm{d}y}{\mathrm{d}t} - y \frac{\mathrm{d}x}{\mathrm{d}t} \right) \mathrm{d}t \qquad \text{(*)}

Coordinates of AA and BB.

Point AA is distance aa from PP along the rod in the direction opposite to BB. Since the rod makes angle tt with the positive xx-direction:

A=(x−acos⁡t,y−asin⁡t)A = (x - a\cos t, \quad y - a\sin t) B=(x+bcos⁡t,y+bsin⁡t)B = (x + b\cos t, \quad y + b\sin t)

Computing [A][A].

Using (∗*):

[A]=12∫02π(xAdyAdt−yAdxAdt)dt[A] = \frac{1}{2}\int_0^{2\pi} \left( x_A \frac{\mathrm{d}y_A}{\mathrm{d}t} - y_A \frac{\mathrm{d}x_A}{\mathrm{d}t} \right) \mathrm{d}t

where xA=x−acos⁡tx_A = x - a\cos t and yA=y−asin⁡ty_A = y - a\sin t. Differentiating:

dxAdt=dxdt+asin⁡t,dyAdt=dydt−acos⁡t\frac{\mathrm{d}x_A}{\mathrm{d}t} = \frac{\mathrm{d}x}{\mathrm{d}t} + a\sin t, \qquad \frac{\mathrm{d}y_A}{\mathrm{d}t} = \frac{\mathrm{d}y}{\mathrm{d}t} - a\cos t

The integrand is:

(x−acos⁡t)(dydt−acos⁡t)−(y−asin⁡t)(dxdt+asin⁡t)(x - a\cos t)\left(\frac{\mathrm{d}y}{\mathrm{d}t} - a\cos t\right) - (y - a\sin t)\left(\frac{\mathrm{d}x}{\mathrm{d}t} + a\sin t\right)

Expanding and collecting terms gives:

xAy˙A=(x−acos⁡t)(y˙−acos⁡t)=xy˙−axcos⁡t−ay˙cos⁡t+a2cos⁡2t.x_A \dot{y}_A = (x - a\cos t)(\dot{y} - a\cos t) = x\dot{y} - ax\cos t - a\dot{y}\cos t + a^2\cos^2 t.

yAx˙A=(y−asin⁡t)(x˙+asin⁡t)=yx˙+aysin⁡t−ax˙sin⁡t−a2sin⁡2t.y_A \dot{x}_A = (y - a\sin t)(\dot{x} + a\sin t) = y\dot{x} + ay\sin t - a\dot{x}\sin t - a^2\sin^2 t.

xAy˙A−yAx˙A=(xy˙−yx˙)−axcos⁡t−ay˙cos⁡t−aysin⁡t+ax˙sin⁡t+a2cos⁡2t+a2sin⁡2tx_A\dot{y}_A - y_A\dot{x}_A = (x\dot{y} - y\dot{x}) - ax\cos t - a\dot{y}\cos t - ay\sin t + a\dot{x}\sin t + a^2\cos^2 t + a^2\sin^2 t

=(xy˙−yx˙)−a(xcos⁡t+ysin⁡t)−a(y˙cos⁡t−x˙sin⁡t)+a2= (x\dot{y} - y\dot{x}) - a(x\cos t + y\sin t) - a(\dot{y}\cos t - \dot{x}\sin t) + a^2

=(xy˙−yx˙)−a[(x+y˙)cos⁡t+(y−x˙)sin⁡t]+a2= (x\dot{y} - y\dot{x}) - a[(x + \dot{y})\cos t + (y - \dot{x})\sin t] + a^2

Thus the integrand for [A][A] is:

(xy˙−yx˙)−a[(x+y˙)cos⁡t+(y−x˙)sin⁡t]+a2(x\dot{y} - y\dot{x}) - a[(x + \dot{y})\cos t + (y - \dot{x})\sin t] + a^2

Now:

[A]=12∫02π[(xy˙−yx˙)−a((x+y˙)cos⁡t+(y−x˙)sin⁡t)+a2]dt[A] = \frac{1}{2}\int_0^{2\pi}\left[(x\dot{y} - y\dot{x}) - a\left(\left(x + \dot{y}\right)\cos t + (y - \dot{x})\sin t\right) + a^2\right]\mathrm{d}t

=[P]−a⋅12∫02π[(x+y˙)cos⁡t+(y−x˙)sin⁡t]dt+a22∫02πdt= [P] - a \cdot \frac{1}{2}\int_0^{2\pi}\left[\left(x + \dot{y}\right)\cos t + (y - \dot{x})\sin t\right]\mathrm{d}t + \frac{a^2}{2}\int_0^{2\pi}\mathrm{d}t

[A]=[P]−af+πa2[A] = [P] - af + \pi a^2

Computing [B][B].

Replacing aa by −b-b in the coordinates (since B=(x+bcos⁡t,y+bsin⁡t)=(x−(−b)cos⁡t,y−(−b)sin⁡t)B = (x + b\cos t, y + b\sin t) = (x - (-b)\cos t, y - (-b)\sin t)):

[B]=[P]−(−b)f+π(−b)2=[P]+bf+πb2[B] = [P] - (-b)f + \pi(-b)^2 = [P] + bf + \pi b^2

Finding the area between C\mathcal{C} and D\mathcal{D}.

Since AA and BB trace the same closed curve C\mathcal{C}, we have [A]=[B][A] = [B]. Equating:

[P]−af+πa2=[P]+bf+πb2[P] - af + \pi a^2 = [P] + bf + \pi b^2

−af−bf=πb2−πa2-af - bf = \pi b^2 - \pi a^2

−f(a+b)=−π(a2−b2)=−π(a−b)(a+b)-f(a + b) = -\pi(a^2 - b^2) = -\pi(a - b)(a + b)

Since a+b>0a + b > 0:

f=π(a−b)f = \pi(a - b)

The area enclosed by C\mathcal{C} is [A][A] and by D\mathcal{D} is [P][P]. The area between the curves is:

[A]−[P]=πa2−af=πa2−aπ(a−b)=πa2−πa2+πab=πab[A] - [P] = \pi a^2 - af = \pi a^2 - a\pi(a - b) = \pi a^2 - \pi a^2 + \pi ab = \pi ab

Examiner Notes

Less than a third of the candidates attempted this. There were quite a few perfect scores, however the vast majority scored less than a quarter of the marks, which was the

mean mark. The general result at the start of the question was the key to success. Those that stumbled with handling four variables in terms of the fifth one, and the consequent calculus, did not attempt to make further progress into the rest of the question.


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

6 The definite integrals T,U,VT, U, V and XX are defined by

T=∫1312artanh tt dt ,U=∫ln⁡2ln⁡3u2sinh⁡u du ,T = \int_{\frac{1}{3}}^{\frac{1}{2}} \frac{\text{artanh } t}{t} \, dt \, , \qquad U = \int_{\ln 2}^{\ln 3} \frac{u}{2 \sinh u} \, du \, ,

V=−∫1312ln⁡v1−v2 dv ,X=∫12ln⁡212ln⁡3ln⁡(coth⁡x) dx .V = -\int_{\frac{1}{3}}^{\frac{1}{2}} \frac{\ln v}{1 - v^2} \, dv \, , \qquad X = \int_{\frac{1}{2} \ln 2}^{\frac{1}{2} \ln 3} \ln(\coth x) \, dx \, .

Show, without evaluating any of them, that T,U,VT, U, V and XX are all equal.

Hint

Using the substitution t=tanh⁡(u2)t = \tanh \left( \frac{u}{2} \right), then it can be shown that T=UT = U, by making use of 2sinh⁡(u2)cosh⁡(u2)=sinh⁡u2 \sinh \left( \frac{u}{2} \right) \cosh \left( \frac{u}{2} \right) = \sinh u to obtain the integrand, and tanh⁡−1t=12ln⁡(1+t1−t)\tanh^{-1} t = \frac{1}{2} \ln \left( \frac{1+t}{1-t} \right) to obtain the limits.

If instead, integration by parts is used differentiating tanh⁡−1t\tanh^{-1} t and integrating 1t\frac{1}{t}, and

employing tanh⁡−1t=12ln⁡(1+t1−t)\tanh^{-1} t = \frac{1}{2} \ln \left( \frac{1+t}{1-t} \right) to demonstrate that [tanh⁡−1tln⁡t]131=0[\tanh^{-1} t \ln t]_{\frac{1}{3}}^1 = 0, T=VT = V.

The substitution t=e−2xt = e^{-2x} can be used to demonstrate that T=XT = X.

(Alternatively, starting from UU, the substitution u=2tanh⁡−1tu = 2 \tanh^{-1} t obtains U=TU = T, the substitution u=−ln⁡vu = -\ln v obtains U=VU = V, and the substitution u=2xu = 2x followed by integration by parts yields U=XU = X; starting from VV, by parts it can be shown that V=TV = T, using the substitution v=e−uv = e^{-u} that V=UV = U, and the substitution v=tanh⁡xv = \tanh x that V=XV = X; or starting from XX, the substitution x=−12ln⁡tx = -\frac{1}{2} \ln t gives X=TX = T, integration by parts gives X=UX = U, and the substitution x=tanh⁡−1vx = \tanh^{-1} v gives X=VX = V.)

Model Solution

We show T=U=V=XT = U = V = X by establishing pairwise equalities through substitutions and integration by parts.

Showing T=UT = U:

Use the substitution t=tanh⁡(u/2)t = \tanh(u/2) in TT.

Limits: t=1/3t = 1/3 gives tanh⁡(u/2)=1/3\tanh(u/2) = 1/3, so u/2=artanh(1/3)=12ln⁡1+1/31−1/3=12ln⁡2u/2 = \text{artanh}(1/3) = \frac{1}{2}\ln\frac{1+1/3}{1-1/3} = \frac{1}{2}\ln 2, hence u=ln⁡2u = \ln 2. Similarly t=1/2t = 1/2 gives u=ln⁡3u = \ln 3.

Differential: dt=12sech2(u/2) du\mathrm{d}t = \frac{1}{2}\text{sech}^2(u/2) \, \mathrm{d}u.

Integrand: artanh(t)=u/2\text{artanh}(t) = u/2 and t=tanh⁡(u/2)t = \tanh(u/2), so:

artanh(t)t dt=u/2tanh⁡(u/2)⋅12sech2(u/2) du=u sech2(u/2)4tanh⁡(u/2) du\frac{\text{artanh}(t)}{t} \, \mathrm{d}t = \frac{u/2}{\tanh(u/2)} \cdot \frac{1}{2}\text{sech}^2(u/2) \, \mathrm{d}u = \frac{u \, \text{sech}^2(u/2)}{4\tanh(u/2)} \, \mathrm{d}u

Since sech2(u/2)tanh⁡(u/2)=cosh⁡−2(u/2)sinh⁡(u/2)/cosh⁡(u/2)=1sinh⁡(u/2)cosh⁡(u/2)=2sinh⁡u\frac{\text{sech}^2(u/2)}{\tanh(u/2)} = \frac{\cosh^{-2}(u/2)}{\sinh(u/2)/\cosh(u/2)} = \frac{1}{\sinh(u/2)\cosh(u/2)} = \frac{2}{\sinh u}:

T=∫ln⁡2ln⁡3u4⋅2sinh⁡u du=∫ln⁡2ln⁡3u2sinh⁡u du=UT = \int_{\ln 2}^{\ln 3} \frac{u}{4} \cdot \frac{2}{\sinh u} \, \mathrm{d}u = \int_{\ln 2}^{\ln 3} \frac{u}{2\sinh u} \, \mathrm{d}u = U

Showing T=VT = V:

Use the substitution t=tanh⁡xt = \tanh x in TT.

Limits: t=1/3t = 1/3 gives x=artanh(1/3)=12ln⁡2x = \text{artanh}(1/3) = \frac{1}{2}\ln 2. Similarly t=1/2t = 1/2 gives x=12ln⁡3x = \frac{1}{2}\ln 3.

Differential: dt=sech2x dx\mathrm{d}t = \text{sech}^2 x \, \mathrm{d}x. Also artanh(t)=x\text{artanh}(t) = x and t=tanh⁡xt = \tanh x, so 1−t2=1−tanh⁡2x=sech2x1 - t^2 = 1 - \tanh^2 x = \text{sech}^2 x.

T=∫12ln⁡212ln⁡3xtanh⁡x⋅sech2x dxT = \int_{\frac{1}{2}\ln 2}^{\frac{1}{2}\ln 3} \frac{x}{\tanh x} \cdot \text{sech}^2 x \, \mathrm{d}x

But sech2xtanh⁡x=1−tanh⁡2xtanh⁡x=1tanh⁡x−tanh⁡x\frac{\text{sech}^2 x}{\tanh x} = \frac{1 - \tanh^2 x}{\tanh x} = \frac{1}{\tanh x} - \tanh x, and we can also write:

sech2xtanh⁡x=1sinh⁡xcosh⁡x=2sinh⁡2x\frac{\text{sech}^2 x}{\tanh x} = \frac{1}{\sinh x \cosh x} = \frac{2}{\sinh 2x}

To show T=VT=V, integrate TT by parts:

T=∫1/31/2artanh(t)⋅1t dtT = \int_{1/3}^{1/2} \text{artanh}(t) \cdot \frac{1}{t} \, \mathrm{d}t

Let u=artanh(t)u = \text{artanh}(t), dv=1tdt\mathrm{d}v = \frac{1}{t}\mathrm{d}t, so du=11−t2dt\mathrm{d}u = \frac{1}{1-t^2}\mathrm{d}t and v=ln⁡tv = \ln t.

T=[artanh(t)ln⁡t]1/31/2−∫1/31/2ln⁡t1−t2 dtT = [\text{artanh}(t) \ln t]_{1/3}^{1/2} - \int_{1/3}^{1/2} \frac{\ln t}{1 - t^2} \, \mathrm{d}t

Evaluating the boundary term: artanh(t)=12ln⁡1+t1−t\text{artanh}(t) = \frac{1}{2}\ln\frac{1+t}{1-t}.

At t=1/2t = 1/2: 12ln⁡3⋅ln⁡(1/2)=−ln⁡2ln⁡32\frac{1}{2}\ln 3 \cdot \ln(1/2) = -\frac{\ln 2 \ln 3}{2}.

At t=1/3t = 1/3: 12ln⁡2⋅ln⁡(1/3)=−ln⁡2ln⁡32\frac{1}{2}\ln 2 \cdot \ln(1/3) = -\frac{\ln 2 \ln 3}{2}.

So [artanh(t)ln⁡t]1/31/2=−ln⁡2ln⁡32−(−ln⁡2ln⁡32)=0[\text{artanh}(t) \ln t]_{1/3}^{1/2} = -\frac{\ln 2 \ln 3}{2} - \left(-\frac{\ln 2 \ln 3}{2}\right) = 0.

Therefore:

T=−∫1/31/2ln⁡t1−t2 dt=VT = -\int_{1/3}^{1/2} \frac{\ln t}{1 - t^2} \, \mathrm{d}t = V

Showing T=XT = X:

Use the substitution t=e−2xt = e^{-2x} in TT.

Limits: t=1/3t = 1/3 gives x=12ln⁡3x = \frac{1}{2}\ln 3. t=1/2t = 1/2 gives x=12ln⁡2x = \frac{1}{2}\ln 2.

Differential: dt=−2e−2xdx\mathrm{d}t = -2e^{-2x}\mathrm{d}x.

For the integrand: artanh(t)=12ln⁡1+e−2x1−e−2x=12ln⁡ex+e−xex−e−x=12ln⁡(coth⁡x)\text{artanh}(t) = \frac{1}{2}\ln\frac{1+e^{-2x}}{1-e^{-2x}} = \frac{1}{2}\ln\frac{e^x + e^{-x}}{e^x - e^{-x}} = \frac{1}{2}\ln(\coth x).

So:

T=∫12ln⁡312ln⁡212ln⁡(coth⁡x)e−2x⋅(−2e−2x) dx=∫12ln⁡212ln⁡3ln⁡(coth⁡x) dx=XT = \int_{\frac{1}{2}\ln 3}^{\frac{1}{2}\ln 2} \frac{\frac{1}{2}\ln(\coth x)}{e^{-2x}} \cdot (-2e^{-2x}) \, \mathrm{d}x = \int_{\frac{1}{2}\ln 2}^{\frac{1}{2}\ln 3} \ln(\coth x) \, \mathrm{d}x = X

Conclusion. Since T=UT = U, T=VT = V, and T=XT = X, all four integrals are equal.


Topic: 数论与代数 Number Theory & Algebra  |  Difficulty: Challenging  |  Marks: 20

7 Let

Tn=(a+1+a)n ,T_n = \left( \sqrt{a+1} + \sqrt{a} \right)^n \, ,

where nn is a positive integer and aa is any given positive integer.

(i) In the case when nn is even, show by induction that TnT_n can be written in the form

An+Bna(a+1) ,A_n + B_n \sqrt{a(a+1)} \, ,

where AnA_n and BnB_n are integers (depending on aa and nn) and An2=a(a+1)Bn2+1A_n^2 = a(a+1)B_n^2 + 1.

(ii) In the case when nn is odd, show by considering (a+1+a)Tm(\sqrt{a+1} + \sqrt{a})T_m where mm is even, or otherwise, that TnT_n can be written in the form

Cna+1+Dna ,C_n \sqrt{a+1} + D_n \sqrt{a} \, ,

where CnC_n and DnD_n are integers (depending on aa and nn) and (a+1)Cn2=aDn2+1(a+1)C_n^2 = aD_n^2 + 1.

(iii) Deduce that, for each nn, TnT_n can be written as the sum of the square roots of two consecutive integers.

Hint

(i) The induction requires Tk+2=Ak+2+Bk+2a(a+1)T_{k+2} = A_{k+2} + B_{k+2} \sqrt{a(a+1)} and Ak+22−a(a+1)Bk+22=1A_{k+2}^2 - a(a+1) B_{k+2}^2 = 1. Tk+2=(Ak+Bka(a+1))(a+1+a)2=(Ak+Bka(a+1))T2T_{k+2} = \left( A_k + B_k \sqrt{a(a+1)} \right) (\sqrt{a+1} + \sqrt{a})^2 = \left( A_k + B_k \sqrt{a(a+1)} \right) T_2

T2=(2a+1+2a(a+1))T_2 = \left( 2a + 1 + 2\sqrt{a(a + 1)} \right) and so A2=2a+1A_2 = 2a + 1 and B2=2B_2 = 2, and A22−a(a+1)B22=(2a+1)2−a(a+1)22=1A_2^2 - a(a + 1)B_2^2 = (2a + 1)^2 - a(a + 1)2^2 = 1 the result is true for n=2n = 2. Evaluating Tk+2T_{k+2} using (Ak+Bka(a+1))T2\left( A_k + B_k\sqrt{a(a + 1)} \right) T_2 then Ak+2=(2a+1)Ak+2a(a+1)BkA_{k+2} = (2a + 1)A_k + 2a(a + 1)B_k and Bk+2=2Ak+(2a+1)BkB_{k+2} = 2A_k + (2a + 1)B_k, and so substituting and simplifying, Ak+22−a(a+1)Bk+22=Ak2−a(a+1)Bk2=1A_{k+2}^2 - a(a + 1)B_{k+2}^2 = A_k^2 - a(a + 1)B_k^2 = 1 by the induction.

(ii) Tn=(a+1+a)Tm=(a+1+a)(Am+Bma(a+1))T_n = (\sqrt{a + 1} + \sqrt{a})T_m = (\sqrt{a + 1} + \sqrt{a})\left( A_m + B_m\sqrt{a(a + 1)} \right)

=(Am+aBm)a+1+(Am+(a+1)Bm)a= (A_m + aB_m)\sqrt{a + 1} + (A_m + (a + 1)B_m)\sqrt{a} which is of required form because

Cn=Am+aBmC_n = A_m + aB_m and Dn=Am+(a+1)BmD_n = A_m + (a + 1)B_m are integers and

(a+1)Cn2−aDn2=(a+1)(Am+aBm)2−a(Am+(a+1)Bm)2(a + 1)C_n^2 - aD_n^2 = (a + 1)(A_m + aB_m)^2 - a(A_m + (a + 1)B_m)^2

=Am2−a(a+1)Bm2=1= A_m^2 - a(a + 1)B_m^2 = 1 as required.

Trivially the case n=1n = 1 is true.

(iii) In the case that nn is even,

Tn=An+Bna(a+1)=An2+a(a+1)Bn2=a(a+1)Bn2+1+a(a+1)Bn2T_n = A_n + B_n\sqrt{a(a + 1)} = \sqrt{A_n^2} + \sqrt{a(a + 1)B_n^2} = \sqrt{a(a + 1)B_n^2 + 1} + \sqrt{a(a + 1)B_n^2} as required,

and in the case that nn is odd, Tn=Cna+1+Dna=(a+1)Cn2+aDn2=T_n = C_n\sqrt{a + 1} + D_n\sqrt{a} = \sqrt{(a + 1)C_n^2} + \sqrt{aD_n^2} = aDn2+1+aDn2\sqrt{aD_n^2 + 1} + \sqrt{aD_n^2} as required.

Model Solution

Part (i): nn even.

We prove by induction on even nn that Tn=An+Bna(a+1)T_n = A_n + B_n\sqrt{a(a+1)} where An,BnA_n, B_n are integers and An2=a(a+1)Bn2+1A_n^2 = a(a+1)B_n^2 + 1.

Base case n=2n = 2:

T2=(a+1+a)2=(a+1)+2a(a+1)+a=(2a+1)+2a(a+1)T_2 = (\sqrt{a+1} + \sqrt{a})^2 = (a+1) + 2\sqrt{a(a+1)} + a = (2a+1) + 2\sqrt{a(a+1)}

So A2=2a+1A_2 = 2a+1 and B2=2B_2 = 2, which are integers. Checking:

A22−a(a+1)B22=(2a+1)2−a(a+1)⋅4=4a2+4a+1−4a2−4a=1A_2^2 - a(a+1)B_2^2 = (2a+1)^2 - a(a+1) \cdot 4 = 4a^2 + 4a + 1 - 4a^2 - 4a = 1

Inductive step. Suppose Tk=Ak+Bka(a+1)T_k = A_k + B_k\sqrt{a(a+1)} with Ak2−a(a+1)Bk2=1A_k^2 - a(a+1)B_k^2 = 1 for some even kk. Then:

Tk+2=Tk⋅T2=(Ak+Bka(a+1))((2a+1)+2a(a+1))T_{k+2} = T_k \cdot T_2 = (A_k + B_k\sqrt{a(a+1)})((2a+1) + 2\sqrt{a(a+1)})

Expanding:

Ak+2=(2a+1)Ak+2a(a+1)BkA_{k+2} = (2a+1)A_k + 2a(a+1)B_k

Bk+2=2Ak+(2a+1)BkB_{k+2} = 2A_k + (2a+1)B_k

Both are integers (since Ak,Bk,aA_k, B_k, a are integers). Now verify Ak+22−a(a+1)Bk+22=1A_{k+2}^2 - a(a+1)B_{k+2}^2 = 1:

Ak+22=[(2a+1)Ak+2a(a+1)Bk]2=(2a+1)2Ak2+4a(a+1)(2a+1)AkBk+4a2(a+1)2Bk2A_{k+2}^2 = [(2a+1)A_k + 2a(a+1)B_k]^2 = (2a+1)^2 A_k^2 + 4a(a+1)(2a+1)A_k B_k + 4a^2(a+1)^2 B_k^2

a(a+1)Bk+22=a(a+1)[2Ak+(2a+1)Bk]2=4a(a+1)Ak2+4a(a+1)(2a+1)AkBk+a(a+1)(2a+1)2Bk2a(a+1)B_{k+2}^2 = a(a+1)[2A_k + (2a+1)B_k]^2 = 4a(a+1)A_k^2 + 4a(a+1)(2a+1)A_k B_k + a(a+1)(2a+1)^2 B_k^2

Subtracting (the cross terms cancel):

Ak+22−a(a+1)Bk+22=[(2a+1)2−4a(a+1)]Ak2+[4a2(a+1)2−a(a+1)(2a+1)2]Bk2A_{k+2}^2 - a(a+1)B_{k+2}^2 = [(2a+1)^2 - 4a(a+1)]A_k^2 + [4a^2(a+1)^2 - a(a+1)(2a+1)^2]B_k^2

Computing the coefficients:

(2a+1)2−4a(a+1)=4a2+4a+1−4a2−4a=1(2a+1)^2 - 4a(a+1) = 4a^2 + 4a + 1 - 4a^2 - 4a = 1

4a2(a+1)2−a(a+1)(2a+1)2=a(a+1)[4a(a+1)−(2a+1)2]=a(a+1)[4a2+4a−4a2−4a−1]=−a(a+1)4a^2(a+1)^2 - a(a+1)(2a+1)^2 = a(a+1)[4a(a+1) - (2a+1)^2] = a(a+1)[4a^2+4a - 4a^2-4a-1] = -a(a+1)

So:

Ak+22−a(a+1)Bk+22=Ak2−a(a+1)Bk2=1A_{k+2}^2 - a(a+1)B_{k+2}^2 = A_k^2 - a(a+1)B_k^2 = 1

by the induction hypothesis. This completes the induction.

Part (ii): nn odd.

For odd nn, write n=m+1n = m + 1 where mm is even. Then:

Tn=(a+1+a)⋅Tm=(a+1+a)(Am+Bma(a+1))T_n = (\sqrt{a+1} + \sqrt{a}) \cdot T_m = (\sqrt{a+1} + \sqrt{a})(A_m + B_m\sqrt{a(a+1)})

Expanding:

=Ama+1+Bm(a+1)a+Ama+Bmaa+1= A_m\sqrt{a+1} + B_m(a+1)\sqrt{a} + A_m\sqrt{a} + B_m a\sqrt{a+1}

=(Am+aBm)a+1+(Am+(a+1)Bm)a= (A_m + aB_m)\sqrt{a+1} + (A_m + (a+1)B_m)\sqrt{a}

So Cn=Am+aBmC_n = A_m + aB_m and Dn=Am+(a+1)BmD_n = A_m + (a+1)B_m, which are integers.

Checking the identity:

(a+1)Cn2−aDn2=(a+1)(Am+aBm)2−a(Am+(a+1)Bm)2(a+1)C_n^2 - aD_n^2 = (a+1)(A_m + aB_m)^2 - a(A_m + (a+1)B_m)^2

Expanding:

=(a+1)(Am2+2aAmBm+a2Bm2)−a(Am2+2(a+1)AmBm+(a+1)2Bm2)= (a+1)(A_m^2 + 2aA_m B_m + a^2 B_m^2) - a(A_m^2 + 2(a+1)A_m B_m + (a+1)^2 B_m^2)

=(a+1)Am2+2a(a+1)AmBm+a2(a+1)Bm2−aAm2−2a(a+1)AmBm−a(a+1)2Bm2= (a+1)A_m^2 + 2a(a+1)A_m B_m + a^2(a+1)B_m^2 - aA_m^2 - 2a(a+1)A_m B_m - a(a+1)^2 B_m^2

The cross terms cancel:

=[(a+1)−a]Am2+[a2(a+1)−a(a+1)2]Bm2=Am2+a(a+1)[a−(a+1)]Bm2= [(a+1) - a]A_m^2 + [a^2(a+1) - a(a+1)^2]B_m^2 = A_m^2 + a(a+1)[a - (a+1)]B_m^2

=Am2−a(a+1)Bm2=1= A_m^2 - a(a+1)B_m^2 = 1

by part (i). (For n=1n = 1: T1=a+1+aT_1 = \sqrt{a+1} + \sqrt{a}, so C1=D1=1C_1 = D_1 = 1 and (a+1)−a=1(a+1) - a = 1.)

Part (iii): TnT_n as a sum of square roots of consecutive integers.

Case 1: nn even. We have Tn=An+Bna(a+1)T_n = A_n + B_n\sqrt{a(a+1)} with An2=a(a+1)Bn2+1A_n^2 = a(a+1)B_n^2 + 1.

Tn=An2+a(a+1)Bn2=a(a+1)Bn2+1+a(a+1)Bn2T_n = \sqrt{A_n^2} + \sqrt{a(a+1)B_n^2} = \sqrt{a(a+1)B_n^2 + 1} + \sqrt{a(a+1)B_n^2}

The quantities under the square roots, a(a+1)Bn2+1a(a+1)B_n^2 + 1 and a(a+1)Bn2a(a+1)B_n^2, are consecutive integers.

Case 2: nn odd. We have Tn=Cna+1+DnaT_n = C_n\sqrt{a+1} + D_n\sqrt{a} with (a+1)Cn2=aDn2+1(a+1)C_n^2 = aD_n^2 + 1.

Tn=(a+1)Cn2+aDn2=aDn2+1+aDn2T_n = \sqrt{(a+1)C_n^2} + \sqrt{aD_n^2} = \sqrt{aD_n^2 + 1} + \sqrt{aD_n^2}

Again, aDn2+1aD_n^2 + 1 and aDn2aD_n^2 are consecutive integers.

In both cases, TnT_n is the sum of the square roots of two consecutive integers.


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

8 The complex numbers zz and ww are related by

w=1+izi+z .w = \frac{1 + iz}{i + z} \, .

Let z=x+iyz = x + iy and w=u+ivw = u + iv, where x,y,ux, y, u and vv are real. Express uu and vv in terms of xx and yy.

(i) By setting x=tan⁡(θ/2)x = \tan(\theta/2), or otherwise, show that if the locus of zz is the real axis y=0y = 0, −∞<x<∞-\infty < x < \infty, then the locus of ww is the circle u2+v2=1u^2 + v^2 = 1 with one point omitted.

(ii) Find the locus of ww when the locus of zz is the line segment y=0y = 0, −1<x<1-1 < x < 1.

(iii) Find the locus of ww when the locus of zz is the line segment x=0x = 0, −1<y<1-1 < y < 1.

(iv) Find the locus of ww when the locus of zz is the line y=1y = 1, −∞<x<∞-\infty < x < \infty.

Hint
  1. w=u+iv=1+i(x+iy)i+(x+iy)=2xx2+(1+y)2+ix2−(1−y2)x2+(1+y)2w = u + iv = \frac{1+i(x+iy)}{i+(x+iy)} = \frac{2x}{x^2+(1+y)^2} + i\frac{x^2-(1-y^2)}{x^2+(1+y)^2} using the complex conjugate, so u=2xx2+(1+y)2u = \frac{2x}{x^2+(1+y)^2} and v=x2−(1−y2)x2+(1+y)2v = \frac{x^2-(1-y^2)}{x^2+(1+y)^2}

(i) If x=tan⁡θ2x = \tan \frac{\theta}{2}, y=0y = 0, then u=sin⁡θu = \sin \theta, and v=−cos⁡θv = -\cos \theta, using the general result and so u2+v2=1u^2 + v^2 = 1 but the point θ=π\theta = \pi i.e. (0,1) is not included.

(ii) If −1<x<1-1 < x < 1, and y=0y = 0, then it is the same locus as (i) except −π2<θ<π2-\frac{\pi}{2} < \theta < \frac{\pi}{2}, and so it is the semi-circle that is the part of u2+v2=1u^2 + v^2 = 1 below the uu axis.

(iii) x=0x = 0, then u=0u = 0 and v=y−1y+1v = \frac{y-1}{y+1}, and as −1<y<1-1 < y < 1 which is that part of the vv axis below the uu axis, i.e. −∞<v<0-\infty < v < 0.

(iv) Let x=2tan⁡θ2x = 2 \tan \frac{\theta}{2} and y=1y = 1, so as −∞<x<∞-\infty < x < \infty, −π<θ<π-\pi < \theta < \pi, then u=12sin⁡θu = \frac{1}{2} \sin \theta and v=12(1−cos⁡θ)v = \frac{1}{2}(1 - \cos \theta), so the locus is the circle u2+(v−12)2=(12)2u^2 + \left( v - \frac{1}{2} \right)^2 = \left( \frac{1}{2} \right)^2 excluding the point θ=π\theta = \pi, which is (0,1).

Model Solution

Expressing uu and vv.

With z=x+iyz = x + iy:

w=1+i(x+iy)i+(x+iy)=1−y+ixx+i(1+y)w = \frac{1 + i(x + iy)}{i + (x + iy)} = \frac{1 - y + ix}{x + i(1 + y)}

Multiplying numerator and denominator by the conjugate of the denominator:

w=(1−y+ix)(x−i(1+y))x2+(1+y)2w = \frac{(1 - y + ix)(x - i(1 + y))}{x^2 + (1 + y)^2}

Numerator:

(1−y)x+(1−y)(−i)(1+y)+ix⋅x+ix(−i)(1+y)(1-y)x + (1-y)(-i)(1+y) + ix \cdot x + ix(-i)(1+y)

=x(1−y)+x2i−i(1−y2)+x(1+y)= x(1-y) + x^2 i - i(1-y^2) + x(1+y)

=[x(1−y)+x(1+y)]+i[x2−(1−y2)]= [x(1-y) + x(1+y)] + i[x^2 - (1-y^2)]

=2x+i(x2+y2−1)= 2x + i(x^2 + y^2 - 1)

So:

u=2xx2+(1+y)2,v=x2+y2−1x2+(1+y)2u = \frac{2x}{x^2 + (1+y)^2}, \qquad v = \frac{x^2 + y^2 - 1}{x^2 + (1+y)^2}

Part (i): Locus when y=0y = 0, −∞<x<∞-\infty < x < \infty.

Setting y=0y = 0:

u=2xx2+1,v=x2−1x2+1u = \frac{2x}{x^2 + 1}, \qquad v = \frac{x^2 - 1}{x^2 + 1}

Set x=tan⁡(θ/2)x = \tan(\theta/2) where −π<θ<π-\pi < \theta < \pi. Using the half-angle identities:

u=2tan⁡(θ/2)1+tan⁡2(θ/2)=sin⁡θu = \frac{2\tan(\theta/2)}{1 + \tan^2(\theta/2)} = \sin\theta

v=tan⁡2(θ/2)−1tan⁡2(θ/2)+1=−cos⁡θv = \frac{\tan^2(\theta/2) - 1}{\tan^2(\theta/2) + 1} = -\cos\theta

So u2+v2=sin⁡2θ+cos⁡2θ=1u^2 + v^2 = \sin^2\theta + \cos^2\theta = 1, i.e., the locus lies on the unit circle.

As xx ranges over (−∞,∞)(-\infty, \infty), θ\theta ranges over (−π,π)(-\pi, \pi). The point θ=π\theta = \pi (i.e., u=0u = 0, v=1v = 1) corresponds to x=tan⁡(π/2)x = \tan(\pi/2) which is undefined. So the locus is the circle u2+v2=1u^2 + v^2 = 1 with the point (0,1)(0, 1) omitted.

Part (ii): Locus when y=0y = 0, −1<x<1-1 < x < 1.

With y=0y = 0 and x=tan⁡(θ/2)x = \tan(\theta/2), the condition −1<x<1-1 < x < 1 gives −1<tan⁡(θ/2)<1-1 < \tan(\theta/2) < 1, so −π/4<θ/2<π/4-\pi/4 < \theta/2 < \pi/4, i.e., −π/2<θ<π/2-\pi/2 < \theta < \pi/2.

For θ∈(−π/2,π/2)\theta \in (-\pi/2, \pi/2): sin⁡θ\sin\theta ranges over (−1,1)(-1, 1) and cos⁡θ>0\cos\theta > 0, so v=−cos⁡θ<0v = -\cos\theta < 0.

The locus is the semicircle u2+v2=1u^2 + v^2 = 1 with v<0v < 0 (the lower half of the unit circle, excluding the endpoints (±1,0)(\pm 1, 0)).

Part (iii): Locus when x=0x = 0, −1<y<1-1 < y < 1.

Setting x=0x = 0:

u=0,v=y2−1(1+y)2=(y−1)(y+1)(y+1)2=y−1y+1u = 0, \qquad v = \frac{y^2 - 1}{(1 + y)^2} = \frac{(y-1)(y+1)}{(y+1)^2} = \frac{y - 1}{y + 1}

For −1<y<1-1 < y < 1: y−1<0y - 1 < 0 and y+1>0y + 1 > 0, so v<0v < 0. As y→−1+y \to -1^+, v→−∞v \to -\infty; as y→1−y \to 1^-, v→0−v \to 0^-.

The locus is the negative vv-axis: the set of points (0,v)(0, v) with v<0v < 0.

Part (iv): Locus when y=1y = 1, −∞<x<∞-\infty < x < \infty.

Setting y=1y = 1:

u=2xx2+4,v=x2x2+4u = \frac{2x}{x^2 + 4}, \qquad v = \frac{x^2}{x^2 + 4}

Note that v=x2x2+4v = \frac{x^2}{x^2 + 4} and u=2xx2+4u = \frac{2x}{x^2 + 4}, so v=x2⋅uv = \frac{x}{2} \cdot u (when x≠0x \neq 0), giving x=2v/ux = 2v/u.

Alternatively, observe that v=1−4x2+4v = 1 - \frac{4}{x^2 + 4}. We compute:

u2+(v−12)2=4x2(x2+4)2+(x2x2+4−12)2u^2 + \left(v - \frac{1}{2}\right)^2 = \frac{4x^2}{(x^2+4)^2} + \left(\frac{x^2}{x^2+4} - \frac{1}{2}\right)^2

=4x2(x2+4)2+(x2−42(x2+4))2=4x2(x2+4)2+(x2−4)24(x2+4)2= \frac{4x^2}{(x^2+4)^2} + \left(\frac{x^2 - 4}{2(x^2+4)}\right)^2 = \frac{4x^2}{(x^2+4)^2} + \frac{(x^2-4)^2}{4(x^2+4)^2}

=16x2+x4−8x2+164(x2+4)2=x4+8x2+164(x2+4)2=(x2+4)24(x2+4)2=14= \frac{16x^2 + x^4 - 8x^2 + 16}{4(x^2+4)^2} = \frac{x^4 + 8x^2 + 16}{4(x^2+4)^2} = \frac{(x^2+4)^2}{4(x^2+4)^2} = \frac{1}{4}

So the locus lies on the circle u2+(v−12)2=14u^2 + (v - \frac{1}{2})^2 = \frac{1}{4}, centered at (0,12)(0, \frac{1}{2}) with radius 12\frac{1}{2}.

The point (0,1)(0, 1) on this circle requires u=0u = 0 and v=1v = 1, which gives x=0x = 0 and 04=0≠1\frac{0}{4} = 0 \neq 1. Checking: u=0u = 0 requires x=0x = 0, then v=0v = 0. So (0,1)(0, 1) is not attained. As x→±∞x \to \pm\infty, u→0u \to 0 and v→1v \to 1, approaching (0,1)(0,1) but never reaching it.

The locus is the circle u2+(v−12)2=14u^2 + (v - \frac{1}{2})^2 = \frac{1}{4} with the point (0,1)(0, 1) omitted.