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STEP3 2004 -- Pure Mathematics

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STEP3 2004 — Section A (Pure Mathematics)

Section titled “STEP3 2004 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2004  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1积分/Integration(双曲函数与代数积分)Challenging换元法,部分分式分解,双曲函数恒等式,反正切积分,指数换元
2曲线分析/Curve analysis(渐近线与曲线描绘)Standard渐近线分析,因式分解,差平方公式,曲线描绘
3不等式与级数/Inequalities and series(凸函数与级数估计)Challenging凸函数性质,积分不等式,伸缩求和法,级数估计
4几何序列/Geometric sequences(相切圆问题)Challenging几何级数求和,三角恒等式,微分求极值,相切条件
5三角方程/Trigonometric equations(辅助角公式)Standard辅助角公式,正切加法公式,双角公式,解的验证
6递推序列与不变量 (Recurrence Sequences and Invariants)Challenging差分法, 不变量证明, 二次方程求根, 构造周期序列
7积分序列与级数估计 (Integral Sequences and Series Estimation)Challenging分部积分, 裂项求和, 不等式放缩, 积分递推
8微分方程与解曲线 (Differential Equations and Solution Curves)Challenging变量代换, 积分因子法, 曲线分类

Topic: 积分/Integration(双曲函数与代数积分)  |  Difficulty: Challenging  |  Marks: 20

1 Show that 0asinhx2cosh2x1dx=122ln(2cosha12cosha+1)+122ln(2+121)\int_{0}^{a} \frac{\sinh x}{2 \cosh^{2} x - 1} \, dx = \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} \cosh a - 1}{\sqrt{2} \cosh a + 1} \right) + \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right) and find 0acoshx1+2sinh2xdx.\int_{0}^{a} \frac{\cosh x}{1 + 2 \sinh^{2} x} \, dx \, . Hence show that 0coshxsinhx1+2sinh2xdx=π22122ln(2+121).\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2 \sinh^{2} x} \, dx = \frac{\pi}{2\sqrt{2}} - \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right) \, . By substituting u=exu = e^{x} in this result, or otherwise, find 111+u4du.\int_{1}^{\infty} \frac{1}{1 + u^{4}} \, du \, .

Hint

The substitution u=coshxu = \cosh x should suggest itself (because of the factor of dudx=sinhx\frac{du}{dx} = \sinh x in the numerator), and the resulting integral can be tackled by splitting the integrand into partial fractions:

0asinhx2cosh2x1dx=1coshadu2u21=121cosha12u112u+1du\int_{0}^{a} \frac{\sinh x}{2 \cosh^{2} x - 1} dx = \int_{1}^{\cosh a} \frac{du}{2u^{2} - 1} = \frac{1}{2} \int_{1}^{\cosh a} \frac{1}{\sqrt{2}u - 1} - \frac{1}{\sqrt{2}u + 1} du

=122[ln(2u1)ln(2u+1)]1cosha=122(ln(2cosha12cosha+1)+ln(2+121))= \frac{1}{2\sqrt{2}} \left[ \ln \left( \sqrt{2}u - 1 \right) - \ln \left( \sqrt{2}u + 1 \right) \right]_{1}^{\cosh a} = \frac{1}{2\sqrt{2}} \left( \ln \left( \frac{\sqrt{2} \cosh a - 1}{\sqrt{2} \cosh a + 1} \right) + \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right) \right)

Similarly, substituting u=sinhxu = \sinh x, and then recognising an arctan integral:

0acoshx1+2sinh2xdx=0sinhadu1+2u2=12[arctan(2u)]0sinha=12arctan(2sinha)\int_{0}^{a} \frac{\cosh x}{1 + 2 \sinh^{2} x} dx = \int_{0}^{\sinh a} \frac{du}{1 + 2u^{2}} = \frac{1}{\sqrt{2}} \left[ \arctan \left( \sqrt{2}u \right) \right]_{0}^{\sinh a} = \frac{1}{\sqrt{2}} \arctan \left( \sqrt{2} \sinh a \right)

To show that

0coshxsinhx1+2sinh2xdx=π22122ln(2+121)\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2 \sinh^{2} x} dx = \frac{\pi}{2\sqrt{2}} - \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right)

note that

a cosh2x=sinh2x+1\cosh^{2} x = \sinh^{2} x + 1, so 2cosh2x1=1+2sinh2x2 \cosh^{2} x - 1 = 1 + 2 \sinh^{2} x, and the integral required is the second minus the first of those calculated earlier, as aa \to \infty.

b as aa \to \infty, sinha\sinh a \to \infty, so arctan(2sinha)π2\arctan \left( \sqrt{2} \sinh a \right) \to \frac{\pi}{2}

c as aa \to \infty, cosha\cosh a \to \infty, so 2cosha12cosha+11\frac{\sqrt{2} \cosh a - 1}{\sqrt{2} \cosh a + 1} \to 1 and ln(2cosha12cosha+1)0\ln \left( \frac{\sqrt{2} \cosh a - 1}{\sqrt{2} \cosh a + 1} \right) \to 0.

Substituting u=exu = e^{x}, so that coshx=12(u+1u)\cosh x = \frac{1}{2} \left( u + \frac{1}{u} \right) and sinhx=12(u1u)\sinh x = \frac{1}{2} \left( u - \frac{1}{u} \right):

0coshxsinhx1+2sinh2xdx=1(u+1u)(u1u)1+12(u22+1u2)1udu=121+u4du\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2 \sinh^{2} x} dx = \int_{1}^{\infty} \frac{\left( u + \frac{1}{u} \right) - \left( u - \frac{1}{u} \right)}{1 + \frac{1}{2} \left( u^{2} - 2 + \frac{1}{u^{2}} \right)} \frac{1}{u} du = \int_{1}^{\infty} \frac{2}{1 + u^{4}} du

so 111+u4du=π42142ln(2+121)\int_{1}^{\infty} \frac{1}{1 + u^{4}} du = \frac{\pi}{4\sqrt{2}} - \frac{1}{4\sqrt{2}} \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right).

Model Solution

Part 1: Show that

0asinhx2cosh2x1dx=122ln(2cosha12cosha+1)+122ln(2+121)\int_{0}^{a} \frac{\sinh x}{2 \cosh^{2} x - 1} \, dx = \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} \cosh a - 1}{\sqrt{2} \cosh a + 1} \right) + \frac{1}{2\sqrt{2}} \ln \left( \frac{\sqrt{2} + 1}{\sqrt{2} - 1} \right)

Substitute u=coshxu = \cosh x, so du=sinhxdxdu = \sinh x \, dx. When x=0x = 0, u=1u = 1; when x=ax = a, u=coshau = \cosh a.

0asinhx2cosh2x1dx=1coshadu2u21\int_{0}^{a} \frac{\sinh x}{2 \cosh^{2} x - 1} \, dx = \int_{1}^{\cosh a} \frac{du}{2u^{2} - 1}

Factor the denominator: 2u21=(2u1)(2u+1)2u^{2} - 1 = (\sqrt{2}u - 1)(\sqrt{2}u + 1). Using partial fractions:

12u21=1(2u1)(2u+1)=A2u1+B2u+1\frac{1}{2u^{2} - 1} = \frac{1}{(\sqrt{2}u - 1)(\sqrt{2}u + 1)} = \frac{A}{\sqrt{2}u - 1} + \frac{B}{\sqrt{2}u + 1}

Multiplying through: 1=A(2u+1)+B(2u1)1 = A(\sqrt{2}u + 1) + B(\sqrt{2}u - 1).

Setting u=12u = \frac{1}{\sqrt{2}}: 1=2A1 = 2A, so A=12A = \frac{1}{2}. Setting u=12u = -\frac{1}{\sqrt{2}}: 1=2B1 = -2B, so B=12B = -\frac{1}{2}.

12u21=12(12u112u+1)\frac{1}{2u^{2} - 1} = \frac{1}{2}\left(\frac{1}{\sqrt{2}u - 1} - \frac{1}{\sqrt{2}u + 1}\right)

Therefore:

1coshadu2u21=121cosha(12u112u+1)du\int_{1}^{\cosh a} \frac{du}{2u^{2} - 1} = \frac{1}{2} \int_{1}^{\cosh a} \left(\frac{1}{\sqrt{2}u - 1} - \frac{1}{\sqrt{2}u + 1}\right) du

=12[12ln(2u1)12ln(2u+1)]1cosha= \frac{1}{2} \left[ \frac{1}{\sqrt{2}} \ln(\sqrt{2}u - 1) - \frac{1}{\sqrt{2}} \ln(\sqrt{2}u + 1) \right]_{1}^{\cosh a}

=122[ln(2u12u+1)]1cosha= \frac{1}{2\sqrt{2}} \left[ \ln\left(\frac{\sqrt{2}u - 1}{\sqrt{2}u + 1}\right) \right]_{1}^{\cosh a}

=122(ln(2cosha12cosha+1)ln(212+1))= \frac{1}{2\sqrt{2}} \left( \ln\left(\frac{\sqrt{2}\cosh a - 1}{\sqrt{2}\cosh a + 1}\right) - \ln\left(\frac{\sqrt{2} - 1}{\sqrt{2} + 1}\right) \right)

Since ln(212+1)=ln(2+121)-\ln\left(\frac{\sqrt{2} - 1}{\sqrt{2} + 1}\right) = \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right):

0asinhx2cosh2x1dx=122ln(2cosha12cosha+1)+122ln(2+121)as required.\int_{0}^{a} \frac{\sinh x}{2 \cosh^{2} x - 1} \, dx = \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2}\cosh a - 1}{\sqrt{2}\cosh a + 1}\right) + \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right) \qquad \text{as required.}

Part 2: Find 0acoshx1+2sinh2xdx\int_{0}^{a} \frac{\cosh x}{1 + 2 \sinh^{2} x} \, dx

Substitute u=sinhxu = \sinh x, so du=coshxdxdu = \cosh x \, dx. When x=0x = 0, u=0u = 0; when x=ax = a, u=sinhau = \sinh a.

0acoshx1+2sinh2xdx=0sinhadu1+2u2\int_{0}^{a} \frac{\cosh x}{1 + 2\sinh^{2} x} \, dx = \int_{0}^{\sinh a} \frac{du}{1 + 2u^{2}}

=0sinhadu1+(2u)2=12[arctan(2u)]0sinha=12arctan(2sinha)= \int_{0}^{\sinh a} \frac{du}{1 + (\sqrt{2}u)^{2}} = \frac{1}{\sqrt{2}} \left[ \arctan(\sqrt{2}u) \right]_{0}^{\sinh a} = \frac{1}{\sqrt{2}} \arctan(\sqrt{2}\sinh a)

Part 3: Hence show that

0coshxsinhx1+2sinh2xdx=π22122ln(2+121)\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2\sinh^{2} x} \, dx = \frac{\pi}{2\sqrt{2}} - \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right)

Using the identity cosh2xsinh2x=1\cosh^{2} x - \sinh^{2} x = 1, we have:

2cosh2x1=2(sinh2x+1)1=1+2sinh2x2\cosh^{2} x - 1 = 2(\sinh^{2} x + 1) - 1 = 1 + 2\sinh^{2} x

So the two denominators are identical. We split the integral:

0coshxsinhx1+2sinh2xdx=0coshx1+2sinh2xdx0sinhx1+2sinh2xdx\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2\sinh^{2} x} \, dx = \int_{0}^{\infty} \frac{\cosh x}{1 + 2\sinh^{2} x} \, dx - \int_{0}^{\infty} \frac{\sinh x}{1 + 2\sinh^{2} x} \, dx

Note the second integral has the same denominator as the first (since 2cosh2x1=1+2sinh2x2\cosh^{2}x - 1 = 1 + 2\sinh^{2}x), so we can use the results from Parts 1 and 2 with aa \to \infty.

First integral: Taking aa \to \infty, sinha\sinh a \to \infty, so arctan(2sinha)π2\arctan(\sqrt{2}\sinh a) \to \frac{\pi}{2}.

0coshx1+2sinh2xdx=12π2=π22\int_{0}^{\infty} \frac{\cosh x}{1 + 2\sinh^{2} x} \, dx = \frac{1}{\sqrt{2}} \cdot \frac{\pi}{2} = \frac{\pi}{2\sqrt{2}}

Second integral: Taking aa \to \infty, cosha\cosh a \to \infty, so:

2cosha12cosha+1=21cosha2+1cosha1\frac{\sqrt{2}\cosh a - 1}{\sqrt{2}\cosh a + 1} = \frac{\sqrt{2} - \frac{1}{\cosh a}}{\sqrt{2} + \frac{1}{\cosh a}} \to 1

and ln(2cosha12cosha+1)ln1=0\ln\left(\frac{\sqrt{2}\cosh a - 1}{\sqrt{2}\cosh a + 1}\right) \to \ln 1 = 0. Thus:

0sinhx2cosh2x1dx=0+122ln(2+121)=122ln(2+121)\int_{0}^{\infty} \frac{\sinh x}{2\cosh^{2} x - 1} \, dx = 0 + \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right) = \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right)

Therefore:

0coshxsinhx1+2sinh2xdx=π22122ln(2+121)as required.\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2\sinh^{2} x} \, dx = \frac{\pi}{2\sqrt{2}} - \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right) \qquad \text{as required.}

Part 4: Find 111+u4du\int_{1}^{\infty} \frac{1}{1 + u^{4}} \, du

Substitute u=exu = e^{x}, so x=lnux = \ln u and dx=duudx = \frac{du}{u}. When x=0x = 0, u=1u = 1; when xx \to \infty, uu \to \infty.

Using the exponential definitions of hyperbolic functions:

coshx=ex+ex2=u+u12,sinhx=exex2=uu12\cosh x = \frac{e^{x} + e^{-x}}{2} = \frac{u + u^{-1}}{2}, \qquad \sinh x = \frac{e^{x} - e^{-x}}{2} = \frac{u - u^{-1}}{2}

The numerator:

coshxsinhx=u+u12uu12=u1=1u\cosh x - \sinh x = \frac{u + u^{-1}}{2} - \frac{u - u^{-1}}{2} = u^{-1} = \frac{1}{u}

The denominator:

1+2sinh2x=1+2(uu12)2=1+(uu1)22=1+u22+u221 + 2\sinh^{2} x = 1 + 2\left(\frac{u - u^{-1}}{2}\right)^{2} = 1 + \frac{(u - u^{-1})^{2}}{2} = 1 + \frac{u^{2} - 2 + u^{-2}}{2}

=2+u22+u22=u2+u22=u4+12u2= \frac{2 + u^{2} - 2 + u^{-2}}{2} = \frac{u^{2} + u^{-2}}{2} = \frac{u^{4} + 1}{2u^{2}}

So the integral becomes:

0coshxsinhx1+2sinh2xdx=11/uu4+12u2duu=12u2u(u4+1)1udu=12u4+1du\int_{0}^{\infty} \frac{\cosh x - \sinh x}{1 + 2\sinh^{2} x} \, dx = \int_{1}^{\infty} \frac{1/u}{\frac{u^{4}+1}{2u^{2}}} \cdot \frac{du}{u} = \int_{1}^{\infty} \frac{2u^{2}}{u(u^{4}+1)} \cdot \frac{1}{u} \, du = \int_{1}^{\infty} \frac{2}{u^{4}+1} \, du

Combining with the result from Part 3:

21du1+u4=π22122ln(2+121)2 \int_{1}^{\infty} \frac{du}{1 + u^{4}} = \frac{\pi}{2\sqrt{2}} - \frac{1}{2\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right)

1du1+u4=π42142ln(2+121)\int_{1}^{\infty} \frac{du}{1 + u^{4}} = \frac{\pi}{4\sqrt{2}} - \frac{1}{4\sqrt{2}} \ln\left(\frac{\sqrt{2} + 1}{\sqrt{2} - 1}\right)


Topic: 曲线分析/Curve analysis(渐近线与曲线描绘)  |  Difficulty: Standard  |  Marks: 20

2 The equation of a curve is y=f(x)y = f(x) where f(x)=x416(2x+1)2x2(x4).f(x) = x - 4 - \frac{16(2x + 1)^{2}}{x^{2}(x - 4)} \, . (i) Write down the equations of the vertical and oblique asymptotes to the curve and show that the oblique asymptote is a tangent to the curve.

(ii) Show that the equation f(x)=0f(x) = 0 has a double root.

(iii) Sketch the curve.

Hint

(i) Inspection of the denominator shows that the vertical asymptotes are at x=0x = 0, x=4x = 4, and the third term in f(x)f(x) tends to zero as x|x| \rightarrow \infty, so the oblique asymptote is just y=x4y = x - 4.

The oblique asymptote meets the curve when 16(2x+1)2x2(x4)=0\frac{16(2x + 1)^2}{x^2(x - 4)} = 0 or (2x+1)2=0(2x + 1)^2 = 0, hence there is a double root at x=12x = -\frac{1}{2} and hence the asymptote touches rather than crosses the curve at (12,92)(-\frac{1}{2}, -\frac{9}{2}), so is a tangent there.

(ii) f(x)=0f(x) = 0 when x2(x4)216(2x+1)2=0x^2(x - 4)^2 - 16(2x + 1)^2 = 0.

The left hand side of this equation is a difference of two squares, so factorises to give (x(x4)4(2x+1))(x(x4)+4(2x+1))=0(x(x - 4) - 4(2x + 1))(x(x - 4) + 4(2x + 1)) = 0; that is, (x212x4)(x+2)2=0(x^2 - 12x - 4)(x + 2)^2 = 0, which has a double root at x=2x = -2.

(iii) On your sketch you should show:

  • the double root at (2,0)(-2, 0) — the curve has a local maximum here and touches the xx-axis;
  • the remaining roots (solutions of x212x4=0x^2 - 12x - 4 = 0) at x=6±210x = 6 \pm 2\sqrt{10};
  • the curve approaching the oblique asymptote y=x4y = x - 4 from below as xx \rightarrow \infty, approaching it from above as xx \rightarrow -\infty and touching it at (12,92)(-\frac{1}{2}, -\frac{9}{2});
  • f(x)f(x) \rightarrow \infty as x0x \rightarrow 0 from above or below, f(x)+f(x) \rightarrow +\infty as x4x \rightarrow 4 from below and f(x)f(x) \rightarrow -\infty as x4x \rightarrow 4 from above;
  • local minima at some xx value with 0<x<40 < x < 4 and with y>0y > 0 and at some xx value with 2<x<12-2 < x < -\frac{1}{2} and with 92>y>x4-\frac{9}{2} > y > x - 4 — note that this second minimum is not at the point of tangency with the oblique asymptote.
Model Solution

Part (i): Asymptotes and tangency

f(x)=x416(2x+1)2x2(x4)f(x) = x - 4 - \frac{16(2x+1)^{2}}{x^{2}(x-4)}

Vertical asymptotes: The denominator x2(x4)=0x^{2}(x-4) = 0 when x=0x = 0 or x=4x = 4. Since the numerators are non-zero at these points, the vertical asymptotes are x=0x = 0 and x=4x = 4.

Oblique asymptote: As x|x| \to \infty, the fraction 16(2x+1)2x2(x4)0\frac{16(2x+1)^{2}}{x^{2}(x-4)} \to 0 (degree 2 numerator over degree 3 denominator), so f(x)x4f(x) \to x - 4. The oblique asymptote is y=x4y = x - 4.

Show the oblique asymptote is a tangent: Setting f(x)=x4f(x) = x - 4:

x416(2x+1)2x2(x4)=x4x - 4 - \frac{16(2x+1)^{2}}{x^{2}(x-4)} = x - 4

16(2x+1)2x2(x4)=0\frac{16(2x+1)^{2}}{x^{2}(x-4)} = 0

This requires (2x+1)2=0(2x+1)^{2} = 0, i.e., x=12x = -\frac{1}{2}. Since (2x+1)2(2x+1)^{2} has a double root, the curve touches the asymptote at x=12x = -\frac{1}{2} rather than crossing it.

At x=12x = -\frac{1}{2}: f(12)=1240=92f(-\frac{1}{2}) = -\frac{1}{2} - 4 - 0 = -\frac{9}{2}, and the asymptote gives y=124=92y = -\frac{1}{2} - 4 = -\frac{9}{2}. So the point of tangency is (12,92)\left(-\frac{1}{2}, -\frac{9}{2}\right).

To confirm tangency, we verify the slopes match. Since f(x)=(x4)g(x)f(x) = (x-4) - g(x) where g(x)=16(2x+1)2x2(x4)g(x) = \frac{16(2x+1)^{2}}{x^{2}(x-4)}:

f(x)=1g(x)f'(x) = 1 - g'(x)

Near x=12x = -\frac{1}{2}, g(x)=16(2x+1)2x2(x4)g(x) = \frac{16(2x+1)^{2}}{x^{2}(x-4)} has a double zero in the numerator at x=12x = -\frac{1}{2} while the denominator is 14(92)=980\frac{1}{4} \cdot (-\frac{9}{2}) = -\frac{9}{8} \neq 0. By the product rule, g(12)=0g'(-\frac{1}{2}) = 0 (the factor (2x+1)2(2x+1)^{2} contributes zero along with its derivative (2x+1)4(2x+1) \cdot 4 evaluated at x=12x = -\frac{1}{2}). Therefore f(12)=10=1f'(-\frac{1}{2}) = 1 - 0 = 1, which equals the slope of y=x4y = x - 4. The asymptote is indeed tangent at (12,92)\left(-\frac{1}{2}, -\frac{9}{2}\right).

Part (ii): Show f(x)=0f(x) = 0 has a double root

Setting f(x)=0f(x) = 0:

x4=16(2x+1)2x2(x4)x - 4 = \frac{16(2x+1)^{2}}{x^{2}(x-4)}

Multiplying both sides by x2(x4)x^{2}(x-4) (valid for x0,4x \neq 0, 4):

x2(x4)2=16(2x+1)2x^{2}(x-4)^{2} = 16(2x+1)^{2}

The left side is [x(x4)]2[x(x-4)]^{2} and the right side is [4(2x+1)]2[4(2x+1)]^{2}, so this is a difference of two squares:

[x(x4)]2[4(2x+1)]2=0[x(x-4)]^{2} - [4(2x+1)]^{2} = 0

[x(x4)4(2x+1)][x(x4)+4(2x+1)]=0[x(x-4) - 4(2x+1)][x(x-4) + 4(2x+1)] = 0

Expanding the first factor:

x24x8x4=x212x4x^{2} - 4x - 8x - 4 = x^{2} - 12x - 4

Expanding the second factor:

x24x+8x+4=x2+4x+4=(x+2)2x^{2} - 4x + 8x + 4 = x^{2} + 4x + 4 = (x+2)^{2}

So the equation becomes:

(x212x4)(x+2)2=0(x^{2} - 12x - 4)(x+2)^{2} = 0

The factor (x+2)2=0(x+2)^{2} = 0 gives x=2x = -2 as a double root. (The quadratic x212x4=0x^{2} - 12x - 4 = 0 gives two simple roots at x=6±210x = 6 \pm 2\sqrt{10}.)

Therefore f(x)=0f(x) = 0 has a double root at x=2x = -2.

Part (iii): Sketch of the curve

The key features are:

Asymptotes:

  • Vertical: x=0x = 0 and x=4x = 4
  • Oblique: y=x4y = x - 4 (tangent to the curve at (12,92)(-\frac{1}{2}, -\frac{9}{2}))

Roots:

  • Double root at x=2x = -2 (curve touches xx-axis): f(2)=61694(6)=6+6=0f(-2) = -6 - \frac{16 \cdot 9}{4 \cdot (-6)} = -6 + 6 = 0
  • Simple roots at x=62100.32x = 6 - 2\sqrt{10} \approx 0.32 and x=6+21012.32x = 6 + 2\sqrt{10} \approx 12.32

Behaviour near asymptotes:

Near x=0x = 0: 16(2x+1)2x2(x4)164x2=4x2\frac{16(2x+1)^{2}}{x^{2}(x-4)} \approx \frac{16}{-4x^{2}} = \frac{-4}{x^{2}}, so f(x)x4+4x2+f(x) \approx x - 4 + \frac{4}{x^{2}} \to +\infty from both sides.

Near x=4x = 4: write x=4+ϵx = 4 + \epsilon. Then x4=ϵx - 4 = \epsilon and 16(2x+1)2x2(x4)168116ϵ=81ϵ\frac{16(2x+1)^{2}}{x^{2}(x-4)} \approx \frac{16 \cdot 81}{16\epsilon} = \frac{81}{\epsilon}. So f(x)ϵ81ϵf(x) \approx \epsilon - \frac{81}{\epsilon}:

  • As x4x \to 4^{-} (ϵ0\epsilon \to 0^{-}): f(x)81ϵ+f(x) \approx -\frac{81}{\epsilon} \to +\infty
  • As x4+x \to 4^{+} (ϵ0+\epsilon \to 0^{+}): f(x)81ϵf(x) \approx -\frac{81}{\epsilon} \to -\infty

Approach to oblique asymptote:

The curve minus the asymptote is f(x)(x4)=16(2x+1)2x2(x4)f(x) - (x-4) = -\frac{16(2x+1)^{2}}{x^{2}(x-4)}. The sign depends on x2(x4)x^{2}(x-4) (since 16(2x+1)20-16(2x+1)^{2} \leqslant 0):

  • For x>4x > 4: x2(x4)>0x^{2}(x-4) > 0, so f(x)<x4f(x) < x - 4 (approaches from below)
  • For 0<x<40 < x < 4: x2(x4)<0x^{2}(x-4) < 0, so f(x)>x4f(x) > x - 4 (approaches from above)
  • For x<0x < 0: x2(x4)<0x^{2}(x-4) < 0, so f(x)>x4f(x) > x - 4 (approaches from above)

Behaviour at the double root x=2x = -2:

Since f(2)=0f(-2) = 0 and f(x)>x4f(x) > x - 4 for x<0x < 0 (with x4=6x - 4 = -6 at x=2x = -2), the curve touches the xx-axis at (2,0)(-2, 0) and stays above it nearby, forming a local maximum.

Summary of the sketch:

The curve has two branches separated by the vertical asymptotes:

  • Left branch (x<0x < 0): Comes down from the oblique asymptote as xx \to -\infty, touches the asymptote at (12,92)(-\frac{1}{2}, -\frac{9}{2}), rises to touch the xx-axis at (2,0)(-2, 0) (local maximum), then plunges to ++\infty as x0x \to 0^{-}.
  • Middle branch (0<x<40 < x < 4): Starts at ++\infty as x0+x \to 0^{+}, dips below the xx-axis crossing at x=62100.32x = 6 - 2\sqrt{10} \approx 0.32, has a local minimum with y>0y > 0 somewhere in (0,4)(0, 4), then rises to ++\infty as x4x \to 4^{-}.
  • Right branch (x>4x > 4): Comes from -\infty as x4+x \to 4^{+}, crosses the xx-axis at x=6+21012.32x = 6 + 2\sqrt{10} \approx 12.32, then approaches y=x4y = x - 4 from below as x+x \to +\infty.

Topic: 不等式与级数/Inequalities and series(凸函数与级数估计)  |  Difficulty: Challenging  |  Marks: 20

3 Given that f(x)>0f''(x) > 0 when axba \leqslant x \leqslant b, explain with the aid of a sketch why (ba)f(a+b2)<abf(x)dx<(ba)f(a)+f(b)2.(b-a) f\left(\frac{a+b}{2}\right) < \int_{a}^{b} f(x) \, dx < (b-a) \frac{f(a)+f(b)}{2} \, .

By choosing suitable aa, bb and f(x)f(x), show that 4(2n1)2<1n11n<12(1n2+1(n1)2),\frac{4}{(2n-1)^2} < \frac{1}{n-1} - \frac{1}{n} < \frac{1}{2} \left( \frac{1}{n^2} + \frac{1}{(n-1)^2} \right) \, , where nn is an integer greater than 1.

Deduce that 4(132+152+172+)<1<12+(122+132+142+).4 \left( \frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots \right) < 1 < \frac{1}{2} + \left( \frac{1}{2^2} + \frac{1}{3^2} + \frac{1}{4^2} + \cdots \right) \, .

Show that 12(132+142+152+162+)<132+152+172+\frac{1}{2} \left( \frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \frac{1}{6^2} + \cdots \right) < \frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots and hence show that 32<n=11n2<74.\frac{3}{2} < \sum_{n=1}^{\infty} \frac{1}{n^2} < \frac{7}{4} \, .

Hint

The sketch should show a curve with increasing gradient: because the gradient is increasing, the curve lies below the chord joining (a,f(a))(a, f(a)) and (b,f(b))(b, f(b)) and above the tangent to the curve at (a+b2,f(a+b2))\left(\frac{a+b}{2}, f\left(\frac{a+b}{2}\right)\right). The illustration is clearer if f(x)>0f(x) > 0 for axba \leqslant x \leqslant b: then the area of the trapezium cut off by the chord and the lines x=ax = a, x=bx = b and y=0y = 0, which is (ba)f(a)+f(b)2(b - a) \frac{f(a) + f(b)}{2}, is larger than the area represented by the integral and the area of the trapezium cut off by the tangent and the lines x=ax = a, x=bx = b and y=0y = 0, which is (ba)f(a+b2)(b - a) f\left(\frac{a+b}{2}\right), is smaller than the area represented by the integral.

Choose f(x)=1x2f(x) = \frac{1}{x^2}, checking that this has f(x)>0f''(x) > 0, a=n1a = n - 1 and b=nb = n to get the quoted result.

Take the sum from n=2n = 2 to \infty of each term in the inequality: the left hand sum is directly as quoted; in the middle sum, you need to notice that it telescopes, so that all the terms except the first cancel in pairs; in the right hand sum, each reciprocal square occurs twice, cancelling the factor of 12\frac{1}{2}, except the first.

For the next part, observe that 1(n+1)2<1n2\frac{1}{(n+1)^2} < \frac{1}{n^2}, so 12(1n2+1(n+1)2)<12(1n2+1n2)=1n2\frac{1}{2} \left( \frac{1}{n^2} + \frac{1}{(n+1)^2} \right) < \frac{1}{2} \left( \frac{1}{n^2} + \frac{1}{n^2} \right) = \frac{1}{n^2}.

Finally, combine the two previous results to get

2(132+142+152+)<1<12+122+132+142+,2 \left( \frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \cdots \right) < 1 < \frac{1}{2} + \frac{1}{2^2} + \frac{1}{3^2} + \frac{1}{4^2} + \cdots,

so that if S=n=11n2S = \sum_{n=1}^{\infty} \frac{1}{n^2}, then 2(S1122)<1<S122 \left( S - 1 - \frac{1}{2^2} \right) < 1 < S - \frac{1}{2}; rearranging these inequalities gives the required bounds on SS.

Model Solution

Part (i): The integral inequality

Since f(x)>0f''(x) > 0 on [a,b][a, b], the function ff is strictly convex (its gradient is strictly increasing). This has two geometric consequences:

  1. The curve y=f(x)y = f(x) lies below the chord joining (a,f(a))(a, f(a)) and (b,f(b))(b, f(b)), so the trapezium area (ba)f(a)+f(b)2(b-a)\frac{f(a)+f(b)}{2} exceeds the area under the curve.

  2. The curve y=f(x)y = f(x) lies above the tangent line at the midpoint x=a+b2x = \frac{a+b}{2}. The tangent at (a+b2,f ⁣(a+b2))\left(\frac{a+b}{2}, f\!\left(\frac{a+b}{2}\right)\right) has equation y=f ⁣(a+b2)+f ⁣(a+b2) ⁣(xa+b2)y = f\!\left(\frac{a+b}{2}\right) + f'\!\left(\frac{a+b}{2}\right)\!\left(x - \frac{a+b}{2}\right). Integrating this tangent from aa to bb:

ab[f ⁣(a+b2)+f ⁣(a+b2) ⁣(xa+b2)]dx=(ba)f ⁣(a+b2)+f ⁣(a+b2)0=(ba)f ⁣(a+b2)\int_{a}^{b} \left[ f\!\left(\frac{a+b}{2}\right) + f'\!\left(\frac{a+b}{2}\right)\!\left(x - \frac{a+b}{2}\right) \right] dx = (b-a)\,f\!\left(\frac{a+b}{2}\right) + f'\!\left(\frac{a+b}{2}\right) \cdot 0 = (b-a)\,f\!\left(\frac{a+b}{2}\right)

since ab(xa+b2)dx=0\int_a^b \left(x - \frac{a+b}{2}\right) dx = 0 by symmetry.

Therefore:

(ba)f ⁣(a+b2)<abf(x)dx<(ba)f(a)+f(b)2(...)(b-a)\,f\!\left(\frac{a+b}{2}\right) < \int_a^b f(x)\,dx < (b-a)\,\frac{f(a)+f(b)}{2} \qquad \text{(...)}

Part (ii): Choosing aa, bb, f(x)f(x)

Take f(x)=1x2f(x) = \frac{1}{x^2}, a=n1a = n-1, b=nb = n (with n>1n > 1 an integer). Then f(x)=6x4>0f''(x) = \frac{6}{x^4} > 0, so the inequality applies.

  • Midpoint value: f ⁣(a+b2)=f ⁣(n12)=1(n12)2=4(2n1)2f\!\left(\frac{a+b}{2}\right) = f\!\left(n - \frac{1}{2}\right) = \frac{1}{\left(n - \frac{1}{2}\right)^2} = \frac{4}{(2n-1)^2}

  • Integral: n1n1x2dx=[1x]n1n=1n+1n1=1n11n\int_{n-1}^{n} \frac{1}{x^2}\,dx = \left[-\frac{1}{x}\right]_{n-1}^{n} = -\frac{1}{n} + \frac{1}{n-1} = \frac{1}{n-1} - \frac{1}{n}

  • Trapezium estimate: (ba)f(a)+f(b)2=112 ⁣(1(n1)2+1n2)(b-a)\frac{f(a)+f(b)}{2} = 1 \cdot \frac{1}{2}\!\left(\frac{1}{(n-1)^2} + \frac{1}{n^2}\right)

Substituting into (…):

4(2n1)2<1n11n<12 ⁣(1(n1)2+1n2)(...)\frac{4}{(2n-1)^2} < \frac{1}{n-1} - \frac{1}{n} < \frac{1}{2}\!\left(\frac{1}{(n-1)^2} + \frac{1}{n^2}\right) \qquad \text{(...)}

Part (iii): Deduce the series inequality

Sum the left inequality of (**) from n=2n = 2 to NN:

n=2N4(2n1)2<n=2N(1n11n)\sum_{n=2}^{N} \frac{4}{(2n-1)^2} < \sum_{n=2}^{N} \left(\frac{1}{n-1} - \frac{1}{n}\right)

The right side telescopes:

n=2N(1n11n)=(1112)+(1213)++(1N11N)=11N\sum_{n=2}^{N} \left(\frac{1}{n-1} - \frac{1}{n}\right) = \left(\frac{1}{1} - \frac{1}{2}\right) + \left(\frac{1}{2} - \frac{1}{3}\right) + \cdots + \left(\frac{1}{N-1} - \frac{1}{N}\right) = 1 - \frac{1}{N}

As NN \to \infty, the right side tends to 11, so:

4 ⁣(132+152+172+)14\!\left(\frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots\right) \leqslant 1

In fact the inequality is strict (each term of the left inequality of (**) is strict), giving:

4 ⁣(132+152+172+)<1(...)4\!\left(\frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots\right) < 1 \qquad \text{(...)}

Now sum the right inequality of (**) from n=2n = 2 to NN:

n=2N(1n11n)<n=2N12 ⁣(1(n1)2+1n2)\sum_{n=2}^{N} \left(\frac{1}{n-1} - \frac{1}{n}\right) < \sum_{n=2}^{N} \frac{1}{2}\!\left(\frac{1}{(n-1)^2} + \frac{1}{n^2}\right)

The right side: each reciprocal square 1k2\frac{1}{k^2} for 2kN12 \leqslant k \leqslant N-1 appears twice (once from n=kn = k giving 1(n1)2\frac{1}{(n-1)^2}, once from n=k+1n = k+1 giving 1n2\frac{1}{n^2}), while 112\frac{1}{1^2} appears once (from n=2n=2) and 1N2\frac{1}{N^2} appears once (from n=Nn=N). So:

12 ⁣(1+1N2+2k=2N11k2)=12+12N2+k=2N11k2\frac{1}{2}\!\left(1 + \frac{1}{N^2} + 2\sum_{k=2}^{N-1}\frac{1}{k^2}\right) = \frac{1}{2} + \frac{1}{2N^2} + \sum_{k=2}^{N-1}\frac{1}{k^2}

Taking NN \to \infty and using the left side 1\to 1:

112+k=21k2=12+(122+132+142+)1 \leqslant \frac{1}{2} + \sum_{k=2}^{\infty}\frac{1}{k^2} = \frac{1}{2} + \left(\frac{1}{2^2} + \frac{1}{3^2} + \frac{1}{4^2} + \cdots\right)

Again the inequality is strict:

1<12+(122+132+142+)(...)1 < \frac{1}{2} + \left(\frac{1}{2^2} + \frac{1}{3^2} + \frac{1}{4^2} + \cdots\right) \qquad \text{(...)}

Part (iv): Prove the final bounds on 1n2\sum \frac{1}{n^2}

We show 12 ⁣(132+142+152+)<132+152+172+\frac{1}{2}\!\left(\frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \cdots\right) < \frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots

It suffices to show 12 ⁣(1k2+1(k+1)2)<1k2\frac{1}{2}\!\left(\frac{1}{k^2} + \frac{1}{(k+1)^2}\right) < \frac{1}{k^2} for each odd k3k \geqslant 3, since the left side pairs consecutive terms while the right picks out the odd ones.

This holds because 1(k+1)2<1k2\frac{1}{(k+1)^2} < \frac{1}{k^2}, so 12 ⁣(1k2+1(k+1)2)<12 ⁣(1k2+1k2)=1k2\frac{1}{2}\!\left(\frac{1}{k^2} + \frac{1}{(k+1)^2}\right) < \frac{1}{2}\!\left(\frac{1}{k^2} + \frac{1}{k^2}\right) = \frac{1}{k^2}.

Writing this more explicitly: group the left side as

12 ⁣(132+142)+12 ⁣(152+162)+12 ⁣(172+182)+\frac{1}{2}\!\left(\frac{1}{3^2} + \frac{1}{4^2}\right) + \frac{1}{2}\!\left(\frac{1}{5^2} + \frac{1}{6^2}\right) + \frac{1}{2}\!\left(\frac{1}{7^2} + \frac{1}{8^2}\right) + \cdots

Each pair satisfies 12 ⁣(1(2m+1)2+1(2m+2)2)<1(2m+1)2\frac{1}{2}\!\left(\frac{1}{(2m+1)^2} + \frac{1}{(2m+2)^2}\right) < \frac{1}{(2m+1)^2}, so the sum of the pairs is less than 132+152+172+\frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots, as required.

Now let S=n=11n2=1+14+19+S = \sum_{n=1}^{\infty} \frac{1}{n^2} = 1 + \frac{1}{4} + \frac{1}{9} + \cdots

From (***):

4 ⁣(132+152+172+)<14\!\left(\frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots\right) < 1

Using the inequality just proved, 412 ⁣(132+142+152+)<4 ⁣(132+152+172+)<14 \cdot \frac{1}{2}\!\left(\frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \cdots\right) < 4\!\left(\frac{1}{3^2} + \frac{1}{5^2} + \frac{1}{7^2} + \cdots\right) < 1, so:

2 ⁣(132+142+152+)<12\!\left(\frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \cdots\right) < 1

Since 132+142+152+=S114\frac{1}{3^2} + \frac{1}{4^2} + \frac{1}{5^2} + \cdots = S - 1 - \frac{1}{4}, we get 2 ⁣(S54)<12\!\left(S - \frac{5}{4}\right) < 1, giving S<54+12=74S < \frac{5}{4} + \frac{1}{2} = \frac{7}{4}.

From (****):

1<12+(122+132+142+)=12+S11 < \frac{1}{2} + \left(\frac{1}{2^2} + \frac{1}{3^2} + \frac{1}{4^2} + \cdots\right) = \frac{1}{2} + S - 1

so S>1+12=32S > 1 + \frac{1}{2} = \frac{3}{2}.

Therefore:

32<n=11n2<74\frac{3}{2} < \sum_{n=1}^{\infty} \frac{1}{n^2} < \frac{7}{4}


Topic: 几何序列/Geometric sequences(相切圆问题)  |  Difficulty: Challenging  |  Marks: 20

4 The triangle OABOAB is isosceles, with OA=OBOA = OB and angle AOB=2αAOB = 2\alpha where 0<α<π20 < \alpha < \frac{\pi}{2}. The semi-circle C0C_0 has its centre at the midpoint of the base ABAB of the triangle, and the sides OAOA and OBOB of the triangle are both tangent to the semi-circle. C1,C2,C3,C_1, C_2, C_3, \dots are circles such that CnC_n is tangent to Cn1C_{n-1} and to sides OAOA and OBOB of the triangle.

Let rnr_n be the radius of CnC_n. Show that rn+1rn=1sinα1+sinα.\frac{r_{n+1}}{r_n} = \frac{1 - \sin \alpha}{1 + \sin \alpha} \, .

Let SS be the total area of the semi-circle C0C_0 and the circles C1,C2,C3,C_1, C_2, C_3, \dots. Show that S=1+sin2α4sinαπr02.S = \frac{1 + \sin^2 \alpha}{4 \sin \alpha} \pi r_0^2 \, .

Show that there are values of α\alpha for which SS is more than four fifths of the area of triangle OABOAB.

Hint

If circle nn has centre OnO_n then OOn=rnsinαOO_n = \frac{r_n}{\sin \alpha}, OOn+1=rn+1sinαOO_{n+1} = \frac{r_{n+1}}{\sin \alpha} and OOnOOn+1=rn+rn+1OO_n - OO_{n+1} = r_n + r_{n+1}.

Substituting and multiplying by sinα\sin \alpha gives rnrn+1=sinα(rn+rn+1)r_n - r_{n+1} = \sin \alpha(r_n + r_{n+1}) which simplifies to rn+1rn=1sinα1+sinα\frac{r_{n+1}}{r_n} = \frac{1 - \sin \alpha}{1 + \sin \alpha}.

This result then implies that rn=(1sinα1+sinα)nr0r_n = \left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right)^n r_0, so the total area is

S=12πr02+π((1sinα1+sinα)r0)2+π((1sinα1+sinα)2r0)2+π((1sinα1+sinα)3r0)2+S = \frac{1}{2} \pi r_0^2 + \pi \left( \left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right) r_0 \right)^2 + \pi \left( \left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right)^2 r_0 \right)^2 + \pi \left( \left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right)^3 r_0 \right)^2 + \dots

which is almost a geometric series with common ratio (1sinα1+sinα)2\left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right)^2, so

S=πr021(1sinα1+sinα)212πr02=((1+sinα)24sinα12)πr02=1+sin2α4sinαπr02.S = \frac{\pi r_0^2}{1 - \left( \frac{1 - \sin \alpha}{1 + \sin \alpha} \right)^2} - \frac{1}{2} \pi r_0^2 = \left( \frac{(1 + \sin \alpha)^2}{4 \sin \alpha} - \frac{1}{2} \right) \pi r_0^2 = \frac{1 + \sin^2 \alpha}{4 \sin \alpha} \pi r_0^2.

Area TT of triangle OAB=12AB×OO0=r0cosαr0sinαOAB = \frac{1}{2} AB \times OO_0 = \frac{r_0}{\cos \alpha} \frac{r_0}{\sin \alpha},

so ST=π4cosα(1+sin2α)=π4cosα(2cos2α)\frac{S}{T} = \frac{\pi}{4} \cos \alpha (1 + \sin^2 \alpha) = \frac{\pi}{4} \cos \alpha (2 - \cos^2 \alpha).

By differentiation, the maximum ST\frac{S}{T} occurs where 23cos2α=02 - 3 \cos^2 \alpha = 0 (not sinα=0\sin \alpha = 0) and equals

π423(223)=π323>23=1624>1625=45.\frac{\pi}{4} \sqrt{\frac{2}{3}} \left( 2 - \frac{2}{3} \right) = \frac{\pi}{3} \sqrt{\frac{2}{3}} > \sqrt{\frac{2}{3}} = \sqrt{\frac{16}{24}} > \sqrt{\frac{16}{25}} = \frac{4}{5}.

Model Solution

Part (i): Show that rn+1rn=1sinα1+sinα\frac{r_{n+1}}{r_n} = \frac{1 - \sin \alpha}{1 + \sin \alpha}

Let OO be the apex of the isosceles triangle, and let OnO_n be the centre of circle CnC_n. Since CnC_n is tangent to both sides OAOA and OBOB, and the angle between these sides is 2α2\alpha, the centre OnO_n lies on the angle bisector from OO.

The distance from OO to OnO_n can be found by considering the right triangle formed by OO, the point of tangency on OAOA, and OnO_n. The angle at OO is α\alpha and the opposite side is rnr_n, so:

OOn=rnsinαOO_n = \frac{r_n}{\sin \alpha}

Similarly, OOn+1=rn+1sinαOO_{n+1} = \frac{r_{n+1}}{\sin \alpha}.

Since CnC_n and Cn+1C_{n+1} are externally tangent to each other, the distance between their centres equals the sum of their radii. Also, On+1O_{n+1} lies between OO and OnO_n (since Cn+1C_{n+1} is the smaller circle closer to OO), so:

OOnOOn+1=rn+rn+1OO_n - OO_{n+1} = r_n + r_{n+1}

Substituting:

rnsinαrn+1sinα=rn+rn+1\frac{r_n}{\sin \alpha} - \frac{r_{n+1}}{\sin \alpha} = r_n + r_{n+1}

Multiplying both sides by sinα\sin \alpha:

rnrn+1=sinα(rn+rn+1)r_n - r_{n+1} = \sin \alpha \, (r_n + r_{n+1})

rnrn+1=rnsinα+rn+1sinαr_n - r_{n+1} = r_n \sin \alpha + r_{n+1} \sin \alpha

rn(1sinα)=rn+1(1+sinα)r_n(1 - \sin \alpha) = r_{n+1}(1 + \sin \alpha)

rn+1rn=1sinα1+sinαas required.\frac{r_{n+1}}{r_n} = \frac{1 - \sin \alpha}{1 + \sin \alpha} \qquad \text{as required.}

Part (ii): Show that S=1+sin2α4sinαπr02S = \frac{1 + \sin^2 \alpha}{4 \sin \alpha} \pi r_0^2

From Part (i), the ratio k=1sinα1+sinαk = \frac{1 - \sin \alpha}{1 + \sin \alpha} is constant, so rn=knr0r_n = k^n r_0 for n1n \geqslant 1.

The total area is:

S=12πr02+n=1πrn2=12πr02+πr02n=1k2nS = \frac{1}{2}\pi r_0^2 + \sum_{n=1}^{\infty} \pi r_n^2 = \frac{1}{2}\pi r_0^2 + \pi r_0^2 \sum_{n=1}^{\infty} k^{2n}

The geometric series sums to n=1k2n=k21k2\sum_{n=1}^{\infty} k^{2n} = \frac{k^2}{1 - k^2}, so:

S=πr02(12+k21k2)=πr02(1k2+2k22(1k2))=πr021+k22(1k2)S = \pi r_0^2 \left( \frac{1}{2} + \frac{k^2}{1 - k^2} \right) = \pi r_0^2 \left( \frac{1 - k^2 + 2k^2}{2(1 - k^2)} \right) = \pi r_0^2 \cdot \frac{1 + k^2}{2(1 - k^2)}

Now compute k2k^2 and 1k21 - k^2:

k2=(1sinα)2(1+sinα)2k^2 = \frac{(1 - \sin \alpha)^2}{(1 + \sin \alpha)^2}

1k2=(1+sinα)2(1sinα)2(1+sinα)2=4sinα(1+sinα)21 - k^2 = \frac{(1 + \sin \alpha)^2 - (1 - \sin \alpha)^2}{(1 + \sin \alpha)^2} = \frac{4 \sin \alpha}{(1 + \sin \alpha)^2}

1+k2=(1+sinα)2+(1sinα)2(1+sinα)2=2(1+sin2α)(1+sinα)21 + k^2 = \frac{(1 + \sin \alpha)^2 + (1 - \sin \alpha)^2}{(1 + \sin \alpha)^2} = \frac{2(1 + \sin^2 \alpha)}{(1 + \sin \alpha)^2}

Therefore:

1+k22(1k2)=2(1+sin2α)(1+sinα)2(1+sinα)224sinα=1+sin2α4sinα\frac{1 + k^2}{2(1 - k^2)} = \frac{2(1 + \sin^2 \alpha)}{(1 + \sin \alpha)^2} \cdot \frac{(1 + \sin \alpha)^2}{2 \cdot 4 \sin \alpha} = \frac{1 + \sin^2 \alpha}{4 \sin \alpha}

S=1+sin2α4sinαπr02as required.S = \frac{1 + \sin^2 \alpha}{4 \sin \alpha} \, \pi r_0^2 \qquad \text{as required.}

Part (iii): Show that S>45TS > \frac{4}{5} T for some values of α\alpha

The area of triangle OABOAB is T=12ABhT = \frac{1}{2} \cdot AB \cdot h where hh is the height from OO to ABAB.

The base AB=2r0cosαAB = 2 \cdot \frac{r_0}{\cos \alpha} (from the right triangle at the base, where the tangent from AA to the semicircle gives half-base =r0cosα= \frac{r_0}{\cos \alpha}).

The height from OO to the base ABAB is r0sinα\frac{r_0}{\sin \alpha} (the distance from OO to the centre of C0C_0 along the angle bisector, which equals r0sinα\frac{r_0}{\sin \alpha}).

T=122r0cosαr0sinα=r02sinαcosαT = \frac{1}{2} \cdot \frac{2r_0}{\cos \alpha} \cdot \frac{r_0}{\sin \alpha} = \frac{r_0^2}{\sin \alpha \cos \alpha}

The ratio:

ST=1+sin2α4sinαπr02sinαcosαr02=πcosα(1+sin2α)4\frac{S}{T} = \frac{1 + \sin^2 \alpha}{4 \sin \alpha} \cdot \pi r_0^2 \cdot \frac{\sin \alpha \cos \alpha}{r_0^2} = \frac{\pi \cos \alpha (1 + \sin^2 \alpha)}{4}

Since sin2α=1cos2α\sin^2 \alpha = 1 - \cos^2 \alpha:

ST=πcosα(2cos2α)4\frac{S}{T} = \frac{\pi \cos \alpha (2 - \cos^2 \alpha)}{4}

Let c=cosαc = \cos \alpha and define g(c)=c(2c2)=2cc3g(c) = c(2 - c^2) = 2c - c^3 for 0<c<10 < c < 1. Then:

g(c)=23c2=0    c=23g'(c) = 2 - 3c^2 = 0 \implies c = \sqrt{\frac{2}{3}}

At this critical point:

g ⁣(23)=23(223)=2343=4323=469g\!\left(\sqrt{\frac{2}{3}}\right) = \sqrt{\frac{2}{3}}\left(2 - \frac{2}{3}\right) = \sqrt{\frac{2}{3}} \cdot \frac{4}{3} = \frac{4}{3}\sqrt{\frac{2}{3}} = \frac{4\sqrt{6}}{9}

So the maximum ratio is:

ST=π4469=π69\frac{S}{T} = \frac{\pi}{4} \cdot \frac{4\sqrt{6}}{9} = \frac{\pi\sqrt{6}}{9}

Now π69>45\frac{\pi\sqrt{6}}{9} > \frac{4}{5} is equivalent to 5π6>365\pi\sqrt{6} > 36, i.e., 150π2>1296150\pi^2 > 1296, i.e., π2>8.64\pi^2 > 8.64. Since π29.87>8.64\pi^2 \approx 9.87 > 8.64, this holds.

Therefore there exist values of α\alpha (specifically, α=arccos23\alpha = \arccos\sqrt{\frac{2}{3}}) for which SS exceeds 45\frac{4}{5} of the area of triangle OABOAB.


Topic: 三角方程/Trigonometric equations(辅助角公式)  |  Difficulty: Standard  |  Marks: 20

5 Show that if cos(xα)=cosβ\cos(x - \alpha) = \cos \beta then either tanx=tan(α+β)\tan x = \tan(\alpha + \beta) or tanx=tan(αβ)\tan x = \tan(\alpha - \beta). By choosing suitable values of xx, α\alpha and β\beta, give an example to show that if tanx=tan(α+β)\tan x = \tan(\alpha + \beta), then cos(xα)\cos(x - \alpha) need not equal cosβ\cos \beta.

Let ω\omega be the acute angle such that tanω=43\tan \omega = \frac{4}{3}.

(i) For 0x2π0 \leqslant x \leqslant 2\pi, solve the equation

cosx7sinx=5\cos x - 7 \sin x = 5

giving both solutions in terms of ω\omega.

(i) For 0x2π0 \leqslant x \leqslant 2\pi, solve the equation

2cosx+11sinx=102 \cos x + 11 \sin x = 10

showing that one solution is twice the other and giving both in terms of ω\omega.

Hint

If cos(xα)=cosβ\cos(x - \alpha) = \cos \beta then xα=2nπ±βx - \alpha = 2n\pi \pm \beta so x=α±β+2nπx = \alpha \pm \beta + 2n\pi so tanx=tan(α±β)\tan x = \tan(\alpha \pm \beta) however, for example, x=πx = \pi, α=β=0\alpha = \beta = 0 has tanx=tanπ=tan0=tan(α+β)\tan x = \tan \pi = \tan 0 = \tan(\alpha + \beta) but cos(xα)=cosπ=11=cosβ\cos(x - \alpha) = \cos \pi = -1 \neq 1 = \cos \beta.

a Writing cosx7sinx=Rcos(xα)\cos x - 7 \sin x = R \cos(x - \alpha) requires R=50=52R = \sqrt{50} = 5\sqrt{2} and tanα=7\tan \alpha = -7, so cos(xα)=cosβ\cos(x - \alpha) = \cos \beta, where cosβ=12\cos \beta = \frac{1}{\sqrt{2}}, so we can take tanβ=1\tan \beta = 1.

Hence tanx=tan(α+β)=tanα+tanβ1tanαtanβ=7±11±7=34 or 43.\text{Hence } \tan x = \tan(\alpha + \beta) = \frac{\tan \alpha + \tan \beta}{1 - \tan \alpha \tan \beta} = \frac{-7 \pm 1}{1 \pm 7} = -\frac{3}{4} \text{ or } \frac{4}{3}.

The first of these gives x=12π+ωx = \frac{1}{2}\pi + \omega or x=32π+ωx = \frac{3}{2}\pi + \omega (since arctan34=π2arctan43\arctan \frac{3}{4} = \frac{\pi}{2} - \arctan \frac{4}{3}) and the second x=ωx = \omega or x=π+ωx = \pi + \omega. However, the first solution in each case does not satisfy the original equation (both have sinx>0\sin x > 0, so cosx7sinx<1\cos x - 7 \sin x < 1), so x=32π+ωx = \frac{3}{2}\pi + \omega or π+ω\pi + \omega.

b proceeding as in (i), cos(xα)=cosβ\cos(x - \alpha) = \cos \beta, where tanα=112\tan \alpha = \frac{11}{2} and R=55R = 5\sqrt{5}, so cosβ=25\cos \beta = \frac{2}{\sqrt{5}} and so tanβ=12\tan \beta = \frac{1}{2}. Hence tanx=22±2411=247\tan x = \frac{22 \pm 2}{4 \mp 11} = -\frac{24}{7} or 43\frac{4}{3}.

Notice that tan2ω=2tanω1tan2ω=247\tan 2\omega = \frac{2 \tan \omega}{1 - \tan^2 \omega} = -\frac{24}{7} so the solutions are x=ωx = \omega and x=2ωx = 2\omega, again eliminating the other two possibilities, ω+π\omega + \pi and 2ω+π2\omega + \pi, by checking in the original equation.

Model Solution

Part (i): Show the trigonometric implication and provide a counterexample

If cos(xα)=cosβ\cos(x - \alpha) = \cos \beta, then xα=2nπ±βx - \alpha = 2n\pi \pm \beta for some integer nn.

Case 1: xα=2nπ+βx - \alpha = 2n\pi + \beta, so x=α+β+2nπx = \alpha + \beta + 2n\pi, giving tanx=tan(α+β)\tan x = \tan(\alpha + \beta).

Case 2: xα=2nπβx - \alpha = 2n\pi - \beta, so x=αβ+2nπx = \alpha - \beta + 2n\pi, giving tanx=tan(αβ)\tan x = \tan(\alpha - \beta).

Therefore either tanx=tan(α+β)\tan x = \tan(\alpha + \beta) or tanx=tan(αβ)\tan x = \tan(\alpha - \beta).

Counterexample: Take x=πx = \pi, α=0\alpha = 0, β=0\beta = 0. Then tanx=tanπ=0=tan(0+0)=tan(α+β)\tan x = \tan \pi = 0 = \tan(0 + 0) = \tan(\alpha + \beta), but cos(xα)=cosπ=11=cosβ\cos(x - \alpha) = \cos \pi = -1 \neq 1 = \cos \beta. So tanx=tan(α+β)\tan x = \tan(\alpha + \beta) does not imply cos(xα)=cosβ\cos(x - \alpha) = \cos \beta.

Part (ii): Solve cosx7sinx=5\cos x - 7 \sin x = 5 for 0x2π0 \leqslant x \leqslant 2\pi

Write cosx7sinx=Rcos(xα)\cos x - 7 \sin x = R \cos(x - \alpha) where R=1+49=50=52R = \sqrt{1 + 49} = \sqrt{50} = 5\sqrt{2} and tanα=7\tan \alpha = 7 (since cosx7sinx=Rcosαcosx+Rsinαsinx\cos x - 7\sin x = R\cos\alpha\cos x + R\sin\alpha\sin x requires Rcosα=1R\cos\alpha = 1 and Rsinα=7R\sin\alpha = 7).

Wait, let me be more careful. We want Rcos(xα)=Rcosαcosx+Rsinαsinx=cosx7sinxR\cos(x - \alpha) = R\cos\alpha\cos x + R\sin\alpha\sin x = \cos x - 7\sin x, so Rcosα=1R\cos\alpha = 1 and Rsinα=7R\sin\alpha = -7. Thus tanα=7\tan\alpha = -7.

The equation becomes 52cos(xα)=55\sqrt{2}\cos(x - \alpha) = 5, so cos(xα)=12\cos(x - \alpha) = \frac{1}{\sqrt{2}}.

By the result from Part (i) with β\beta such that cosβ=12\cos\beta = \frac{1}{\sqrt{2}} (so tanβ=1\tan\beta = 1):

tanx=tan(α+β)ortanx=tan(αβ)\tan x = \tan(\alpha + \beta) \quad \text{or} \quad \tan x = \tan(\alpha - \beta)

Using the tangent addition formula with tanα=7\tan\alpha = -7 and tanβ=1\tan\beta = 1:

tan(α+β)=7+11+7=68=34\tan(\alpha + \beta) = \frac{-7 + 1}{1 + 7} = \frac{-6}{8} = -\frac{3}{4}

tan(αβ)=7117=86=43\tan(\alpha - \beta) = \frac{-7 - 1}{1 - 7} = \frac{-8}{-6} = \frac{4}{3}

Since tanω=43\tan\omega = \frac{4}{3} with ω\omega acute, and tan(π+ω)=tanω=43\tan(\pi + \omega) = \tan\omega = \frac{4}{3}.

For tanx=43\tan x = \frac{4}{3}: x=ωx = \omega or x=π+ωx = \pi + \omega.

For tanx=34\tan x = -\frac{3}{4}: since arctan34=π2ω\arctan\frac{3}{4} = \frac{\pi}{2} - \omega (complementary angles), tan(π2ω)=34\tan\left(\frac{\pi}{2} - \omega\right) = \frac{3}{4}, so tanx=34\tan x = -\frac{3}{4} gives x=π(π2ω)=π2+ωx = \pi - \left(\frac{\pi}{2} - \omega\right) = \frac{\pi}{2} + \omega or x=2π(π2ω)=3π2+ωx = 2\pi - \left(\frac{\pi}{2} - \omega\right) = \frac{3\pi}{2} + \omega.

We have four candidates: ω\omega, π+ω\pi + \omega, π2+ω\frac{\pi}{2} + \omega, 3π2+ω\frac{3\pi}{2} + \omega. We must check which satisfy the original equation (the tangent result only gives necessary conditions).

Note cosα=152\cos\alpha = \frac{1}{5\sqrt{2}} and sinα=752\sin\alpha = \frac{-7}{5\sqrt{2}}, so α\alpha is in the fourth quadrant. For cos(xα)=12\cos(x - \alpha) = \frac{1}{\sqrt{2}}, we need xα=±π4+2nπx - \alpha = \pm\frac{\pi}{4} + 2n\pi.

Let me check directly. We need cosx7sinx=5\cos x - 7\sin x = 5.

  • x=ωx = \omega: cosω=35\cos\omega = \frac{3}{5}, sinω=45\sin\omega = \frac{4}{5}, so 35285=55\frac{3}{5} - \frac{28}{5} = -5 \neq 5. Not a solution.
  • x=π+ωx = \pi + \omega: cos(π+ω)=35\cos(\pi + \omega) = -\frac{3}{5}, sin(π+ω)=45\sin(\pi + \omega) = -\frac{4}{5}, so 35+285=5-\frac{3}{5} + \frac{28}{5} = 5. Solution.
  • x=π2+ωx = \frac{\pi}{2} + \omega: cos(π2+ω)=sinω=45\cos(\frac{\pi}{2} + \omega) = -\sin\omega = -\frac{4}{5}, sin(π2+ω)=cosω=35\sin(\frac{\pi}{2} + \omega) = \cos\omega = \frac{3}{5}, so 45215=55-\frac{4}{5} - \frac{21}{5} = -5 \neq 5. Not a solution.
  • x=3π2+ωx = \frac{3\pi}{2} + \omega: cos(3π2+ω)=sinω=45\cos(\frac{3\pi}{2} + \omega) = \sin\omega = \frac{4}{5}, sin(3π2+ω)=cosω=35\sin(\frac{3\pi}{2} + \omega) = -\cos\omega = -\frac{3}{5}, so 45+215=5\frac{4}{5} + \frac{21}{5} = 5. Solution.

The solutions are x=π+ωx = \pi + \omega and x=3π2+ωx = \frac{3\pi}{2} + \omega.

Part (iii): Solve 2cosx+11sinx=102 \cos x + 11 \sin x = 10 for 0x2π0 \leqslant x \leqslant 2\pi

Write 2cosx+11sinx=Rcos(xα)2\cos x + 11\sin x = R\cos(x - \alpha) where R=4+121=125=55R = \sqrt{4 + 121} = \sqrt{125} = 5\sqrt{5} and Rcosα=2R\cos\alpha = 2, Rsinα=11R\sin\alpha = 11, so tanα=112\tan\alpha = \frac{11}{2}.

The equation becomes 55cos(xα)=105\sqrt{5}\cos(x - \alpha) = 10, so cos(xα)=25\cos(x - \alpha) = \frac{2}{\sqrt{5}}.

By Part (i), with cosβ=25\cos\beta = \frac{2}{\sqrt{5}} (so tanβ=12\tan\beta = \frac{1}{2}):

tanx=tan(α+β)ortanx=tan(αβ)\tan x = \tan(\alpha + \beta) \quad \text{or} \quad \tan x = \tan(\alpha - \beta)

tan(α+β)=112+12111212=61114=674=247\tan(\alpha + \beta) = \frac{\frac{11}{2} + \frac{1}{2}}{1 - \frac{11}{2} \cdot \frac{1}{2}} = \frac{6}{1 - \frac{11}{4}} = \frac{6}{-\frac{7}{4}} = -\frac{24}{7}

tan(αβ)=112121+11212=51+114=5154=43\tan(\alpha - \beta) = \frac{\frac{11}{2} - \frac{1}{2}}{1 + \frac{11}{2} \cdot \frac{1}{2}} = \frac{5}{1 + \frac{11}{4}} = \frac{5}{\frac{15}{4}} = \frac{4}{3}

Now tanω=43\tan\omega = \frac{4}{3}, so tan(αβ)=tanω\tan(\alpha - \beta) = \tan\omega, giving x=ωx = \omega or x=π+ωx = \pi + \omega.

For tan(α+β)=247\tan(\alpha + \beta) = -\frac{24}{7}: note that tan2ω=2tanω1tan2ω=8/3116/9=8/37/9=247\tan 2\omega = \frac{2\tan\omega}{1 - \tan^2\omega} = \frac{8/3}{1 - 16/9} = \frac{8/3}{-7/9} = -\frac{24}{7}.

So tanx=tan2ω\tan x = \tan 2\omega, giving x=2ωx = 2\omega or x=π+2ωx = \pi + 2\omega.

We have four candidates: ω\omega, π+ω\pi + \omega, 2ω2\omega, π+2ω\pi + 2\omega. Checking each:

  • x=ωx = \omega: 2cosω+11sinω=235+1145=6+445=102\cos\omega + 11\sin\omega = 2 \cdot \frac{3}{5} + 11 \cdot \frac{4}{5} = \frac{6 + 44}{5} = 10. Solution.
  • x=2ωx = 2\omega: cos2ω=1tan2ω1+tan2ω=116/91+16/9=7/925/9=725\cos 2\omega = \frac{1 - \tan^2\omega}{1 + \tan^2\omega} = \frac{1 - 16/9}{1 + 16/9} = \frac{-7/9}{25/9} = -\frac{7}{25}, sin2ω=2tanω1+tan2ω=8/325/9=2425\sin 2\omega = \frac{2\tan\omega}{1 + \tan^2\omega} = \frac{8/3}{25/9} = \frac{24}{25}. Then 2(725)+112425=14+26425=25025=102(-\frac{7}{25}) + 11 \cdot \frac{24}{25} = \frac{-14 + 264}{25} = \frac{250}{25} = 10. Solution.
  • x=π+ωx = \pi + \omega: 2cos(π+ω)+11sin(π+ω)=2cosω11sinω=10102\cos(\pi + \omega) + 11\sin(\pi + \omega) = -2\cos\omega - 11\sin\omega = -10 \neq 10. Not a solution.
  • x=π+2ωx = \pi + 2\omega: similarly gives 1010-10 \neq 10. Not a solution.

The solutions are x=ωx = \omega and x=2ωx = 2\omega, where one solution is twice the other.


Topic: 递推序列与不变量 (Recurrence Sequences and Invariants)  |  Difficulty: Challenging  |  Marks: 20

6 Given a sequence w0,w1,w2,w_0, w_1, w_2, \dots, the sequence F1,F2,F_1, F_2, \dots is defined by

Fn=wn2+wn124wnwn1.F_n = w_n^2 + w_{n-1}^2 - 4w_n w_{n-1} .

Show that FnFn1=(wnwn2)(wn+wn24wn1)F_n - F_{n-1} = (w_n - w_{n-2})(w_n + w_{n-2} - 4w_{n-1}) for n2n \geqslant 2.

(i) The sequence u0,u1,u2,u_0, u_1, u_2, \dots has u0=1u_0 = 1, and u1=2u_1 = 2 and satisfies

un=4un1un2(n2).u_n = 4u_{n-1} - u_{n-2} \quad (n \geqslant 2) .

Prove that un2+un12=4unun13u_n^2 + u_{n-1}^2 = 4u_n u_{n-1} - 3 for n1n \geqslant 1.

(ii) A sequence v0,v1,v2,v_0, v_1, v_2, \dots has v0=1v_0 = 1 and satisfies

vn2+vn12=4vnvn13(n1).(*)v_n^2 + v_{n-1}^2 = 4v_n v_{n-1} - 3 \quad (n \geqslant 1) . \qquad \text{(*)}

(a) Find v1v_1 and prove that, for each n2n \geqslant 2, either vn=4vn1vn2v_n = 4v_{n-1} - v_{n-2} or vn=vn2v_n = v_{n-2}.

(b) Show that the sequence, with period 2, defined by

vn={1for n even2for n oddv_n = \begin{cases} 1 & \text{for } n \text{ even} \\ 2 & \text{for } n \text{ odd} \end{cases}

satisfies (*).

(c) Find a sequence vnv_n with period 4 which has v0=1v_0 = 1, and satisfies (*).

Hint

6 FnFn1=wn2+wn124wnwn1wn12wn22+4wn1wn2=wn2wn224wn1(wnwn2)F_n - F_{n-1} = w_n^2 + w_{n-1}^2 - 4w_n w_{n-1} - w_{n-1}^2 - w_{n-2}^2 + 4w_{n-1} w_{n-2} = w_n^2 - w_{n-2}^2 - 4w_{n-1}(w_n - w_{n-2}) =(wnwn2)(wn+wn24wn1.)= (w_n - w_{n-2})(w_n + w_{n-2} - 4w_{n-1}.) (+)

(i) Let wnw_n be unu_n; then un+un24un1=0u_n + u_{n-2} - 4u_{n-1} = 0, so FnFn1=0F_n - F_{n-1} = 0 for n2n \geq 2, by (+), but F1=u12+u024u1u0=3F_1 = u_1^2 + u_0^2 - 4u_1 u_0 = -3 so Fn=3F_n = -3 for n1n \geq 1

(ii) In this part, let wnw_n be vnv_n.

(a) v12+1=4v13(v12)2=0v1=2v_1^2 + 1 = 4v_1 - 3 \Rightarrow (v_1 - 2)^2 = 0 \Rightarrow v_1 = 2 Fn=vn2+vn124vnvn1=3F_n = v_n^2 + v_{n-1}^2 - 4v_n v_{n-1} = -3 for n1n \geq 1

vnvn2=0\Rightarrow v_n - v_{n-2} = 0 or vn+vn24vn1=0v_n + v_{n-2} - 4v_{n-1} = 0, for n2n \geq 2, by (+).

(b) Since 1,2,1,2,1, 2, 1, 2, \dots satisfies vnvn2=0v_n - v_{n-2} = 0 for n2n \geq 2, FnF_n is constant, by (+) and since v0=1,v1=2v_0 = 1, v_1 = 2 that constant is 3-3, so the sequence satisfies (*).

(c) The sequence 1,2,7,2,1, 2, 7, 2, \dots, with period 4, satisfies vnvn2=0v_n - v_{n-2} = 0 for odd n2n \geq 2 and vn+vn24vn1=0v_n + v_{n-2} - 4v_{n-1} = 0 for even n2n \geq 2, so FnF_n is constant, by (+), and since v0=1,v1=2v_0 = 1, v_1 = 2 that constant is 3-3, so the sequence satisfies (*).

Model Solution

Preliminary: Show that FnFn1=(wnwn2)(wn+wn24wn1)F_n - F_{n-1} = (w_n - w_{n-2})(w_n + w_{n-2} - 4w_{n-1})

FnFn1=(wn2+wn124wnwn1)(wn12+wn224wn1wn2)F_n - F_{n-1} = (w_n^2 + w_{n-1}^2 - 4w_n w_{n-1}) - (w_{n-1}^2 + w_{n-2}^2 - 4w_{n-1} w_{n-2})

=wn2wn224wn1(wnwn2)= w_n^2 - w_{n-2}^2 - 4w_{n-1}(w_n - w_{n-2})

=(wnwn2)(wn+wn2)4wn1(wnwn2)= (w_n - w_{n-2})(w_n + w_{n-2}) - 4w_{n-1}(w_n - w_{n-2})

=(wnwn2)(wn+wn24wn1)(...)= (w_n - w_{n-2})(w_n + w_{n-2} - 4w_{n-1}) \qquad \text{(...)}

Part (i): Prove that un2+un12=4unun13u_n^2 + u_{n-1}^2 = 4u_n u_{n-1} - 3 for n1n \geqslant 1

Define Fn=un2+un124unun1F_n = u_n^2 + u_{n-1}^2 - 4u_n u_{n-1}. Since un=4un1un2u_n = 4u_{n-1} - u_{n-2}, we have un+un24un1=0u_n + u_{n-2} - 4u_{n-1} = 0.

By the result (…), FnFn1=(unun2)(un+un24un1)=0F_n - F_{n-1} = (u_n - u_{n-2})(u_n + u_{n-2} - 4u_{n-1}) = 0 for all n2n \geqslant 2.

So FnF_n is constant for n1n \geqslant 1. Computing F1F_1:

F1=u12+u024u1u0=4+18=3F_1 = u_1^2 + u_0^2 - 4u_1 u_0 = 4 + 1 - 8 = -3

Therefore Fn=3F_n = -3 for all n1n \geqslant 1, i.e.:

un2+un124unun1=3u_n^2 + u_{n-1}^2 - 4u_n u_{n-1} = -3

un2+un12=4unun13for n1.(...)u_n^2 + u_{n-1}^2 = 4u_n u_{n-1} - 3 \qquad \text{for } n \geqslant 1. \qquad \text{(...)}

Part (ii)(a): Find v1v_1 and prove the disjunction

Setting n=1n = 1 in (*): v12+v02=4v1v03v_1^2 + v_0^2 = 4v_1 v_0 - 3.

v12+1=4v13v_1^2 + 1 = 4v_1 - 3

v124v1+4=0v_1^2 - 4v_1 + 4 = 0

(v12)2=0(v_1 - 2)^2 = 0

v1=2v_1 = 2

Now let Fn=vn2+vn124vnvn1F_n = v_n^2 + v_{n-1}^2 - 4v_n v_{n-1}. From (*), Fn=3F_n = -3 for all n1n \geqslant 1.

For n2n \geqslant 2, using (…):

FnFn1=(vnvn2)(vn+vn24vn1)=0F_n - F_{n-1} = (v_n - v_{n-2})(v_n + v_{n-2} - 4v_{n-1}) = 0

since both Fn=3F_n = -3 and Fn1=3F_{n-1} = -3. Therefore:

(vnvn2)(vn+vn24vn1)=0(v_n - v_{n-2})(v_n + v_{n-2} - 4v_{n-1}) = 0

So either vn=vn2v_n = v_{n-2} or vn=4vn1vn2v_n = 4v_{n-1} - v_{n-2} for each n2n \geqslant 2.

Part (ii)(b): Show the period-2 sequence satisfies (*)

The sequence is 1,2,1,2,1,2,1, 2, 1, 2, 1, 2, \ldots with v0=1v_0 = 1, v1=2v_1 = 2.

For all n2n \geqslant 2, vn=vn2v_n = v_{n-2} (this is the definition of period 2). By the result (…), FnFn1=0F_n - F_{n-1} = 0, so FnF_n is constant. Since:

F1=v12+v024v1v0=4+18=3F_1 = v_1^2 + v_0^2 - 4v_1 v_0 = 4 + 1 - 8 = -3

we have Fn=3F_n = -3 for all n1n \geqslant 1, which is exactly (*).

Part (ii)(c): Find a period-4 sequence with v0=1v_0 = 1 satisfying (*)

We need a sequence where the pattern of choices (either vn=vn2v_n = v_{n-2} or vn=4vn1vn2v_n = 4v_{n-1} - v_{n-2}) repeats with period 4. We already know v0=1v_0 = 1 and v1=2v_1 = 2.

To get period 4, we need v2v0v_2 \neq v_0 (otherwise it would be period 2). So at n=2n = 2, choose v2=4v1v0=81=7v_2 = 4v_1 - v_0 = 8 - 1 = 7.

For period 4, we need v3=v1=2v_3 = v_1 = 2 (using vn=vn2v_n = v_{n-2} at n=3n = 3). Then v4=v0=1v_4 = v_0 = 1 and v5=v1=2v_5 = v_1 = 2, confirming period 4.

Let’s verify: the sequence is 1,2,7,2,1,2,7,2,1, 2, 7, 2, 1, 2, 7, 2, \ldots

Check (*): vn2+vn12=4vnvn13v_n^2 + v_{n-1}^2 = 4v_n v_{n-1} - 3 for each n1n \geqslant 1.

  • n=1n = 1: 4+1=83=54 + 1 = 8 - 3 = 5. ✓
  • n=2n = 2: 49+4=563=5349 + 4 = 56 - 3 = 53. ✓
  • n=3n = 3: 4+49=563=534 + 49 = 56 - 3 = 53. ✓
  • n=4n = 4: 1+4=83=51 + 4 = 8 - 3 = 5. ✓

At n=2n = 2: v2=4v1v0=7v_2 = 4v_1 - v_0 = 7 (recurrence). At n=3n = 3: v3=v1=2v_3 = v_1 = 2 (period 2 step). At n=4n = 4: v4=v2=7v_4 = v_2 = 7? No, we need v4=1v_4 = 1. Check: v4=4v3v2=87=1v_4 = 4v_3 - v_2 = 8 - 7 = 1. ✓ (recurrence). At n=5n = 5: v5=v3=2v_5 = v_3 = 2? Check: v5=4v4v3=42=2v_5 = 4v_4 - v_3 = 4 - 2 = 2. ✓ (both options give the same).

The sequence vn=1,2,7,2,1,2,7,2,v_n = 1, 2, 7, 2, 1, 2, 7, 2, \ldots has period 4, satisfies v0=1v_0 = 1, and satisfies (*).


Topic: 积分序列与级数估计 (Integral Sequences and Series Estimation)  |  Difficulty: Challenging  |  Marks: 20

7 For n=1,2,3,n = 1, 2, 3, \dots, let

In=01tn1(t+1)ndt.I_n = \int_0^1 \frac{t^{n-1}}{(t+1)^n} \, dt \, .

By considering the greatest value taken by tt+1\frac{t}{t+1} for 0t10 \leqslant t \leqslant 1 show that In+1<12InI_{n+1} < \frac{1}{2} I_n.

Show also that In+1=1n2n+InI_{n+1} = -\frac{1}{n \, 2^n} + I_n.

Deduce that In<1n2n1I_n < \frac{1}{n \, 2^{n-1}}.

Prove that

ln2=r=1n1r2r+In+1\ln 2 = \sum_{r=1}^n \frac{1}{r \, 2^r} + I_{n+1}

and hence show that 23<ln2<1724\frac{2}{3} < \ln 2 < \frac{17}{24}.

Hint

7 On 0t10 \leqslant t \leqslant 1, the integrand is non-negative and 0tt+1=11t+1120 \leqslant \frac{t}{t+1} = 1 - \frac{1}{t+1} \leqslant \frac{1}{2}, so

In+1=01tn(t+1)n+1dt=01tt+1tn1(t+1)ndt<1201tn1(t+1)ndt=12In.I_{n+1} = \int_{0}^{1} \frac{t^n}{(t+1)^{n+1}} dt = \int_{0}^{1} \frac{t}{t+1} \frac{t^{n-1}}{(t+1)^n} dt < \frac{1}{2} \int_{0}^{1} \frac{t^{n-1}}{(t+1)^n} dt = \frac{1}{2} I_n.

Integration by parts gives

In+1=[tnn(t+1)n]01+01ntn1n(t+1)ndt=1n2n+In,I_{n+1} = \left[ -\frac{t^n}{n(t+1)^n} \right]_{0}^{1} + \int_{0}^{1} \frac{nt^{n-1}}{n(t+1)^n} dt = -\frac{1}{n2^n} + I_n,

so In>2In+1=1n2n1+2In    In<1n2n1().I_n > 2I_{n+1} = -\frac{1}{n2^{n-1}} + 2I_n \implies I_n < \frac{1}{n2^{n-1}} \quad (*).

Since 12r=IrIr+1\frac{1}{2^r} = I_r - I_{r+1}, r=1n1r2r=(I1I2)+(I2I3)++(InIn+1)=I1In+1\sum_{r=1}^{n} \frac{1}{r2^r} = (I_1 - I_2) + (I_2 - I_3) + \dots + (I_n - I_{n+1}) = I_1 - I_{n+1}, and

I1=011t+1dt=ln2, so ln2=r=1n1r2r+In+1.I_1 = \int_{0}^{1} \frac{1}{t+1} dt = \ln 2, \text{ so } \ln 2 = \sum_{r=1}^{n} \frac{1}{r2^r} + I_{n+1}.

Hence ln2>r=131r2r=23\ln 2 > \sum_{r=1}^{3} \frac{1}{r2^r} = \frac{2}{3} and, by inequality ()(*), ln2=r=121r2r+I3<r=121r2r+1322=1724.\ln 2 = \sum_{r=1}^{2} \frac{1}{r2^r} + I_3 < \sum_{r=1}^{2} \frac{1}{r2^r} + \frac{1}{3 \cdot 2^2} = \frac{17}{24}.

Model Solution

Part (i): Show that In+1<12InI_{n+1} < \frac{1}{2} I_n

On the interval 0t10 \leqslant t \leqslant 1, the function tt+1=11t+1\frac{t}{t+1} = 1 - \frac{1}{t+1} is increasing, so its greatest value is attained at t=1t = 1:

tt+112\frac{t}{t+1} \leqslant \frac{1}{2}

Since the integrand of In+1I_{n+1} is non-negative for t[0,1]t \in [0,1], we write:

In+1=01tn(t+1)n+1dt=01tt+1tn1(t+1)ndtI_{n+1} = \int_0^1 \frac{t^n}{(t+1)^{n+1}} \, dt = \int_0^1 \frac{t}{t+1} \cdot \frac{t^{n-1}}{(t+1)^n} \, dt

Because tt+112\frac{t}{t+1} \leqslant \frac{1}{2} on [0,1][0,1] with strict inequality on [0,1)[0,1):

In+1<1201tn1(t+1)ndt=12InI_{n+1} < \frac{1}{2} \int_0^1 \frac{t^{n-1}}{(t+1)^n} \, dt = \frac{1}{2} I_n

Part (ii): Show that In+1=1n2n+InI_{n+1} = -\frac{1}{n \, 2^n} + I_n

We apply integration by parts to In+1=01tn(t+1)n+1dtI_{n+1} = \int_0^1 \frac{t^n}{(t+1)^{n+1}} \, dt.

Let u=tnu = t^n and dv=(t+1)(n+1)dtdv = (t+1)^{-(n+1)} \, dt. Then du=ntn1dtdu = n t^{n-1} \, dt and v=1n(t+1)nv = -\frac{1}{n(t+1)^n}.

In+1=[tnn(t+1)n]01+01ntn1n(t+1)ndtI_{n+1} = \left[ -\frac{t^n}{n(t+1)^n} \right]_0^1 + \int_0^1 \frac{n t^{n-1}}{n(t+1)^n} \, dt

Evaluating the boundary term:

[tnn(t+1)n]01=1n2n0=1n2n\left[ -\frac{t^n}{n(t+1)^n} \right]_0^1 = -\frac{1}{n \cdot 2^n} - 0 = -\frac{1}{n \, 2^n}

The remaining integral is:

01tn1(t+1)ndt=In\int_0^1 \frac{t^{n-1}}{(t+1)^n} \, dt = I_n

Therefore:

In+1=1n2n+In(...)I_{n+1} = -\frac{1}{n \, 2^n} + I_n \qquad \text{(...)}

Part (iii): Deduce that In<1n2n1I_n < \frac{1}{n \, 2^{n-1}}

From the recurrence (…), In=In+1+1n2nI_n = I_{n+1} + \frac{1}{n \, 2^n}. From Part (i), In+1<12InI_{n+1} < \frac{1}{2} I_n, so:

In=In+1+1n2n<12In+1n2nI_n = I_{n+1} + \frac{1}{n \, 2^n} < \frac{1}{2} I_n + \frac{1}{n \, 2^n}

Subtracting 12In\frac{1}{2} I_n from both sides:

12In<1n2n\frac{1}{2} I_n < \frac{1}{n \, 2^n}

In<1n2n1(**)I_n < \frac{1}{n \, 2^{n-1}} \qquad \text{(**)}

Part (iv): Prove that ln2=r=1n1r2r+In+1\ln 2 = \sum_{r=1}^n \frac{1}{r \, 2^r} + I_{n+1}

From the recurrence (…):

IrIr+1=1r2rI_r - I_{r+1} = \frac{1}{r \, 2^r}

Summing from r=1r = 1 to nn:

r=1n1r2r=r=1n(IrIr+1)=(I1I2)+(I2I3)++(InIn+1)=I1In+1\sum_{r=1}^n \frac{1}{r \, 2^r} = \sum_{r=1}^n (I_r - I_{r+1}) = (I_1 - I_2) + (I_2 - I_3) + \cdots + (I_n - I_{n+1}) = I_1 - I_{n+1}

This telescopes, leaving only I1In+1I_1 - I_{n+1}. Now:

I1=011t+1dt=[ln(t+1)]01=ln2I_1 = \int_0^1 \frac{1}{t+1} \, dt = \left[ \ln(t+1) \right]_0^1 = \ln 2

Therefore:

ln2=r=1n1r2r+In+1\ln 2 = \sum_{r=1}^n \frac{1}{r \, 2^r} + I_{n+1}

Part (v): Show that 23<ln2<1724\frac{2}{3} < \ln 2 < \frac{17}{24}

Since In+1>0I_{n+1} > 0 (the integrand is positive on [0,1][0,1]), we have:

ln2=r=1n1r2r+In+1>r=1n1r2r\ln 2 = \sum_{r=1}^n \frac{1}{r \, 2^r} + I_{n+1} > \sum_{r=1}^n \frac{1}{r \, 2^r}

Taking n=3n = 3:

ln2>112+124+138=12+18+124=12+3+124=1624=23\ln 2 > \frac{1}{1 \cdot 2} + \frac{1}{2 \cdot 4} + \frac{1}{3 \cdot 8} = \frac{1}{2} + \frac{1}{8} + \frac{1}{24} = \frac{12 + 3 + 1}{24} = \frac{16}{24} = \frac{2}{3}

For the upper bound, take n=2n = 2:

ln2=112+124+I3=12+18+I3=58+I3\ln 2 = \frac{1}{1 \cdot 2} + \frac{1}{2 \cdot 4} + I_3 = \frac{1}{2} + \frac{1}{8} + I_3 = \frac{5}{8} + I_3

By inequality (**), I3<1322=112I_3 < \frac{1}{3 \cdot 2^2} = \frac{1}{12}, so:

ln2<58+112=1524+224=1724\ln 2 < \frac{5}{8} + \frac{1}{12} = \frac{15}{24} + \frac{2}{24} = \frac{17}{24}

Therefore 23<ln2<1724\frac{2}{3} < \ln 2 < \frac{17}{24}.


Topic: 微分方程与解曲线 (Differential Equations and Solution Curves)  |  Difficulty: Challenging  |  Marks: 20

8 Show that if

dydx=f(x)y+g(x)y\frac{dy}{dx} = f(x)y + \frac{g(x)}{y}

then the substitution u=y2u = y^2 gives a linear differential equation for u(x)u(x).

Hence or otherwise solve the differential equation

dydx=yx1y.\frac{dy}{dx} = \frac{y}{x} - \frac{1}{y} \, .

Determine the solution curves of this equation which pass through (1,1)(1, 1), (2,2)(2, 2) and (4,4)(4, 4) and sketch graphs of all three curves on the same axes.

Hint

8 If u=y2u = y^2 then dudx=2ydydx=2f(x)y2+2g(x)=2f(x)u+2g(x)\frac{du}{dx} = 2y \frac{dy}{dx} = 2f(x)y^2 + 2g(x) = 2f(x)u + 2g(x),

which is a linear differential equation for u(x)u(x).

In this case, f(x)=1xf(x) = \frac{1}{x}, g(x)=1g(x) = -1 so the differential equation is dudx=2ux2\frac{du}{dx} = \frac{2u}{x} - 2.

The integrating factor is e2xdx=e2lnx=1x2e^{\int \frac{2}{x} dx} = e^{2 \ln x} = \frac{1}{x^2}, giving 1x2dudx2ux3=ddx(ux2)=2x2\frac{1}{x^2} \frac{du}{dx} - \frac{2u}{x^3} = \frac{d}{dx} \left( \frac{u}{x^2} \right) = \frac{-2}{x^2}

so that ux2=2x2dx=2x+c\frac{u}{x^2} = \int \frac{-2}{x^2} dx = \frac{2}{x} + c or u=y2=cx2+2xu = y^2 = cx^2 + 2x.

The solution curves which pass through (1,1)(1, 1), (2,2)(2, 2) and (4,4)(4, 4) are y2+(x1)2=1y^2 + (x - 1)^2 = 1, y2=2xy^2 = 2x and (x+2)22y2=4(x + 2)^2 - 2y^2 = 4 respectively. In drawing these curves it should be made clear that all of them pass through the origin, and that this is their only point of intersection; that the first is a circle with centre (1,0)(1, 0), the second a parabola and the third an hyperbola with centre (2,0)(-2, 0) and asymptotes y=±x+22y = \pm \frac{x+2}{\sqrt{2}}.

Model Solution

Part (i): Show that u=y2u = y^2 gives a linear differential equation

Given:

dydx=f(x)y+g(x)y\frac{dy}{dx} = f(x)y + \frac{g(x)}{y}

Set u=y2u = y^2. Then dudx=2ydydx\frac{du}{dx} = 2y \frac{dy}{dx}, so:

dudx=2y(f(x)y+g(x)y)=2f(x)y2+2g(x)=2f(x)u+2g(x)\frac{du}{dx} = 2y \left( f(x)y + \frac{g(x)}{y} \right) = 2f(x)y^2 + 2g(x) = 2f(x)u + 2g(x)

This is a linear first-order ODE for u(x)u(x):

dudx2f(x)u=2g(x)\frac{du}{dx} - 2f(x)u = 2g(x)

Part (ii): Solve dydx=yx1y\frac{dy}{dx} = \frac{y}{x} - \frac{1}{y}

Here f(x)=1xf(x) = \frac{1}{x} and g(x)=1g(x) = -1. With u=y2u = y^2:

dudx=2ux2\frac{du}{dx} = \frac{2u}{x} - 2

Rearranging:

dudx2ux=2\frac{du}{dx} - \frac{2u}{x} = -2

The integrating factor is:

e2xdx=e2lnx=1x2e^{\int -\frac{2}{x} \, dx} = e^{-2 \ln x} = \frac{1}{x^2}

Multiplying both sides by 1x2\frac{1}{x^2}:

1x2dudx2ux3=2x2\frac{1}{x^2} \frac{du}{dx} - \frac{2u}{x^3} = -\frac{2}{x^2}

The left side is ddx ⁣(ux2)\frac{d}{dx}\!\left(\frac{u}{x^2}\right), so:

ddx ⁣(ux2)=2x2\frac{d}{dx}\!\left(\frac{u}{x^2}\right) = -\frac{2}{x^2}

Integrating:

ux2=2x2dx=2x+c\frac{u}{x^2} = \int -\frac{2}{x^2} \, dx = \frac{2}{x} + c

Therefore:

u=cx2+2xu = cx^2 + 2x

Substituting back u=y2u = y^2:

y2=cx2+2xy^2 = cx^2 + 2x

Part (iii): Solution curves through (1,1)(1, 1), (2,2)(2, 2) and (4,4)(4, 4)

Curve through (1,1)(1, 1): Substituting x=1x = 1, y=1y = 1:

1=c+2    c=11 = c + 2 \implies c = -1

So y2=x2+2xy^2 = -x^2 + 2x, i.e., x2+y22x=0x^2 + y^2 - 2x = 0. Completing the square:

(x1)2+y2=1(x - 1)^2 + y^2 = 1

This is a circle centred at (1,0)(1, 0) with radius 11. Since y2=2xx2=x(2x)0y^2 = 2x - x^2 = x(2-x) \geqslant 0, we need 0x20 \leqslant x \leqslant 2.

Curve through (2,2)(2, 2): Substituting x=2x = 2, y=2y = 2:

4=4c+4    c=04 = 4c + 4 \implies c = 0

So y2=2xy^2 = 2x. This is a parabola opening to the right, valid for x0x \geqslant 0.

Curve through (4,4)(4, 4): Substituting x=4x = 4, y=4y = 4:

16=16c+8    c=1216 = 16c + 8 \implies c = \frac{1}{2}

So y2=12x2+2xy^2 = \frac{1}{2}x^2 + 2x, i.e., 2y2=x2+4x2y^2 = x^2 + 4x. Completing the square:

2y2=(x+2)24    (x+2)24y22=12y^2 = (x + 2)^2 - 4 \implies \frac{(x+2)^2}{4} - \frac{y^2}{2} = 1

This is a hyperbola centred at (2,0)(-2, 0) with asymptotes y=±x+22y = \pm \frac{x+2}{\sqrt{2}}. The right branch passes through the origin and (4,4)(4, 4).

Sketch description: All three curves pass through the origin (setting y=0y = 0 in y2=cx2+2xy^2 = cx^2 + 2x gives x=0x = 0 for any cc). The origin is their only common point. The sketch should show:

  • The circle (x1)2+y2=1(x-1)^2 + y^2 = 1 (a complete circle, symmetric about the xx-axis, passing through (0,0)(0,0) and (2,0)(2,0)).
  • The parabola y2=2xy^2 = 2x opening rightward, passing through the origin and (2,2)(2,2).
  • The right branch of the hyperbola (x+2)24y22=1\frac{(x+2)^2}{4} - \frac{y^2}{2} = 1, passing through the origin and (4,4)(4,4), with asymptotes y=±x+22y = \pm \frac{x+2}{\sqrt{2}}.