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STEP2 2014 -- Pure Mathematics

Exam: STEP2  |  Year: 2014  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1几何与三角 (Geometry & Trigonometry)Standard三角恒等式cos²θ+sin²θ=1,二次方程判别式,坐标几何距离分析,延长线上的几何推理
2微积分 (Calculus)Challenging三角函数积分计算,反例构造方法,二次函数代入不等式,三角函数代入不等式,π的近似值比较
3微积分 (Calculus)Challenging点到直线距离公式,隐函数微分,微分方程求解,y”=0的特殊情形分析,圆的方程推导
4微积分 (Calculus)Standardu=1/x代换,对称区间上的积分性质,arctan恒等式,参数选择技巧,无穷积分计算
5微分方程 (Differential Equations)Standard齐次微分方程的y=xu代换,分离变量法,坐标平移消常数项,初值条件代入
6三角函数与级数 (Trigonometric Series)Challenging三角恒等式求和, 导数求驻点, 数学归纳法, 不等式证明
7绝对值函数与方程 (Absolute Value Functions & Equations)Standard分段函数分析, 图像绘制, 绝对值方程求解, 分类讨论
8二项式展开与组合数学 (Binomial Expansion & Combinatorics)Hard二项式系数公式, 比值法判断单调性, 不等式放缩, 分类讨论

Topic: 几何与三角 (Geometry & Trigonometry)  |  Difficulty: Standard  |  Marks: 20

1 In the triangle ABCABC, the base ABAB is of length 1 unit and the angles at AA and BB are α\alpha and β\beta respectively, where 0<α⩽β0 < \alpha \leqslant \beta. The points PP and QQ lie on the sides ACAC and BCBC respectively, with AP=PQ=QB=xAP = PQ = QB = x. The line PQPQ makes an angle of θ\theta with the line through PP parallel to ABAB.

(i) Show that xcos⁡θ=1−xcos⁡α−xcos⁡βx \cos \theta = 1 - x \cos \alpha - x \cos \beta, and obtain an expression for xsin⁡θx \sin \theta in terms of xx, α\alpha and β\beta. Hence show that

(1+2cos⁡(α+β))x2−2(cos⁡α+cos⁡β)x+1=0.(*)(1 + 2 \cos(\alpha + \beta))x^2 - 2(\cos \alpha + \cos \beta)x + 1 = 0 . \qquad \text{(*)}

Show that (∗)(*) is also satisfied if PP and QQ lie on ACAC produced and BCBC produced, respectively. [By definition, PP lies on ACAC produced if PP lies on the line through AA and CC and the points are in the order A,C,PA, C, P.]

(ii) State the condition on α\alpha and β\beta for (∗)(*) to be linear in xx. If this condition does not hold (but the condition 0<α⩽β0 < \alpha \leqslant \beta still holds), show that (∗)(*) has distinct real roots.

(iii) Find the possible values of xx in the two cases (a) α=β=45∘\alpha = \beta = 45^\circ and (b) α=30∘\alpha = 30^\circ, β=90∘\beta = 90^\circ, and illustrate each case with a sketch.

Hint

Drawing a diagram and considering the horizontal and vertical distances will establish the relationships for xcos⁡θx \cos \theta and xsin⁡θx \sin \theta easily. The quadratic equation will then follow from use of the identity cos⁡2θ+sin⁡2θ≡1\cos^2 \theta + \sin^2 \theta \equiv 1. The same reasoning applied to a diagram showing the case where P and Q lie on AC produced and BC produced will show that the same equation is satisfied.

() will be linear if the coefficient of x2x^2 is 0, so therefore cos⁡(α+β)\cos(\alpha + \beta) will need to equal −12-\frac{1}{2}, which gives a relationship between α\alpha and β\beta. For () to have distinct roots the discriminant must be positive. Using some trigonometric identities it can be shown that the discriminant is equal to 4(1−(sin⁡α−sin⁡β)2)4(1 - (\sin \alpha - \sin \beta)^2) and it should be easy to explain why this must be greater than 0.

The first case in part (iii) leads to x=2±1x = \sqrt{2} \pm 1 and so there are two diagrams to be drawn. In each case the line joining P to Q will be horizontal.

The second case in part (iii) is an example where (*) is linear. This leads to x=33x = \frac{\sqrt{3}}{3}. Therefore Q is at the same point as C and so the point P is the midpoint of AC.

Model Solution

Part (i)

Set up coordinates with AA at the origin and BB at (1,0)(1, 0). Then ACAC makes angle α\alpha with ABAB, and BCBC makes angle π−β\pi - \beta with the positive xx-axis (since β\beta is the interior angle at BB).

Since AP=xAP = x, the coordinates of PP are:

P=(xcos⁡α,  xsin⁡α)P = (x\cos\alpha,\; x\sin\alpha)

Since QB=xQB = x and QQ lies on BCBC with BB at (1,0)(1,0), moving from BB toward CC by distance xx:

Q=(1−xcos⁡β,  xsin⁡β)Q = (1 - x\cos\beta,\; x\sin\beta)

The line PQPQ has length xx and makes angle θ\theta with the horizontal. The horizontal component of PQ⃗\vec{PQ} is:

xcos⁡θ=(1−xcos⁡β)−xcos⁡α=1−xcos⁡α−xcos⁡β(...)x\cos\theta = (1 - x\cos\beta) - x\cos\alpha = 1 - x\cos\alpha - x\cos\beta \qquad \text{(...)}

The vertical component of PQ⃗\vec{PQ} is:

xsin⁡θ=xsin⁡β−xsin⁡α(...)x\sin\theta = x\sin\beta - x\sin\alpha \qquad \text{(...)}

Using cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1, we square and add:

(1−xcos⁡α−xcos⁡β)2+(xsin⁡β−xsin⁡α)2=x2(1 - x\cos\alpha - x\cos\beta)^2 + (x\sin\beta - x\sin\alpha)^2 = x^2

Expanding the left side:

1−2xcos⁡α−2xcos⁡β+x2cos⁡2α+2x2cos⁡αcos⁡β+x2cos⁡2β+x2sin⁡2β−2x2sin⁡αsin⁡β+x2sin⁡2α1 - 2x\cos\alpha - 2x\cos\beta + x^2\cos^2\alpha + 2x^2\cos\alpha\cos\beta + x^2\cos^2\beta + x^2\sin^2\beta - 2x^2\sin\alpha\sin\beta + x^2\sin^2\alpha

Collecting the x2x^2 terms using cos⁡2α+sin⁡2α=1\cos^2\alpha + \sin^2\alpha = 1 and cos⁡2β+sin⁡2β=1\cos^2\beta + \sin^2\beta = 1:

x2(2+2cos⁡αcos⁡β−2sin⁡αsin⁡β)=x2(2+2cos⁡(α+β))x^2(2 + 2\cos\alpha\cos\beta - 2\sin\alpha\sin\beta) = x^2(2 + 2\cos(\alpha + \beta))

So the equation becomes:

1−2x(cos⁡α+cos⁡β)+x2(2+2cos⁡(α+β))=x21 - 2x(\cos\alpha + \cos\beta) + x^2(2 + 2\cos(\alpha + \beta)) = x^2

1−2x(cos⁡α+cos⁡β)+x2(1+2cos⁡(α+β))=01 - 2x(\cos\alpha + \cos\beta) + x^2(1 + 2\cos(\alpha + \beta)) = 0

(1+2cos⁡(α+β))x2−2(cos⁡α+cos⁡β)x+1=0(∗)(1 + 2\cos(\alpha + \beta))x^2 - 2(\cos\alpha + \cos\beta)x + 1 = 0 \qquad (*)

Extension to ACAC produced and BCBC produced: If PP lies on ACAC produced (order A,C,PA, C, P) and QQ lies on BCBC produced (order B,C,QB, C, Q), then PP and QQ are on the opposite sides of CC from AA and BB. The horizontal and vertical displacements become:

xcos⁡θ=1+xcos⁡α+xcos⁡βorxcos⁡θ=−(1+xcos⁡α+xcos⁡β)x\cos\theta = 1 + x\cos\alpha + x\cos\beta \quad \text{or} \quad x\cos\theta = -(1 + x\cos\alpha + x\cos\beta)

depending on the direction of PQ⃗\vec{PQ}. In either case, squaring gives (1+xcos⁡α+xcos⁡β)2(1 + x\cos\alpha + x\cos\beta)^2, and the vertical displacement squared is (xsin⁡β−xsin⁡α)2(x\sin\beta - x\sin\alpha)^2 (or its negative, which squares to the same). Adding and using cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1:

(1+xcos⁡α+xcos⁡β)2+(xsin⁡β−xsin⁡α)2=x2(1 + x\cos\alpha + x\cos\beta)^2 + (x\sin\beta - x\sin\alpha)^2 = x^2

Expanding:

1+2xcos⁡α+2xcos⁡β+x2cos⁡2α+2x2cos⁡αcos⁡β+x2cos⁡2β+x2sin⁡2β−2x2sin⁡αsin⁡β+x2sin⁡2α=x21 + 2x\cos\alpha + 2x\cos\beta + x^2\cos^2\alpha + 2x^2\cos\alpha\cos\beta + x^2\cos^2\beta + x^2\sin^2\beta - 2x^2\sin\alpha\sin\beta + x^2\sin^2\alpha = x^2

This simplifies to:

(1+2cos⁡(α+β))x2+2(cos⁡α+cos⁡β)x+1=0(1 + 2\cos(\alpha + \beta))x^2 + 2(\cos\alpha + \cos\beta)x + 1 = 0

Since xx can be negative in this configuration (measuring the “signed distance” along the produced line), replacing xx by −x-x recovers (∗)(*). Alternatively, since the quadratic in xx from the original case already accounts for both signs of xx, the same equation (∗)(*) is satisfied.

Part (ii)

(∗)(*) is linear in xx when the coefficient of x2x^2 is zero:

1+2cos⁡(α+β)=0  ⟹  cos⁡(α+β)=−121 + 2\cos(\alpha + \beta) = 0 \implies \cos(\alpha + \beta) = -\frac{1}{2}

Since 0<α⩽β0 < \alpha \leqslant \beta and α+β<π\alpha + \beta < \pi (angles of a triangle), we need α+β=2π3\alpha + \beta = \frac{2\pi}{3}, i.e., α+β=120°\alpha + \beta = 120°.

Distinct real roots: If 1+2cos⁡(α+β)≠01 + 2\cos(\alpha + \beta) \neq 0, the discriminant is:

Δ=4(cos⁡α+cos⁡β)2−4(1+2cos⁡(α+β))\Delta = 4(\cos\alpha + \cos\beta)^2 - 4(1 + 2\cos(\alpha + \beta))

Using cos⁡α+cos⁡β=2cos⁡ ⁣α+β2cos⁡ ⁣α−β2\cos\alpha + \cos\beta = 2\cos\!\tfrac{\alpha+\beta}{2}\cos\!\tfrac{\alpha-\beta}{2}:

Δ=16cos⁡2 ⁣α+β2cos⁡2 ⁣α−β2−4−8cos⁡(α+β)\Delta = 16\cos^2\!\tfrac{\alpha+\beta}{2}\cos^2\!\tfrac{\alpha-\beta}{2} - 4 - 8\cos(\alpha+\beta)

Setting ϕ=α+β2\phi = \frac{\alpha+\beta}{2} and using cos⁡(α+β)=2cos⁡2ϕ−1\cos(\alpha+\beta) = 2\cos^2\phi - 1:

Δ=16cos⁡2ϕcos⁡2 ⁣α−β2−8(2cos⁡2ϕ−1)−4=16cos⁡2ϕcos⁡2 ⁣α−β2−16cos⁡2ϕ+4\Delta = 16\cos^2\phi\cos^2\!\tfrac{\alpha-\beta}{2} - 8(2\cos^2\phi - 1) - 4 = 16\cos^2\phi\cos^2\!\tfrac{\alpha-\beta}{2} - 16\cos^2\phi + 4

=4−16cos⁡2ϕsin⁡2 ⁣α−β2=4(1−4cos⁡2ϕsin⁡2 ⁣α−β2)= 4 - 16\cos^2\phi\sin^2\!\tfrac{\alpha-\beta}{2} = 4\left(1 - 4\cos^2\phi\sin^2\!\tfrac{\alpha-\beta}{2}\right)

Since 0<α⩽β0 < \alpha \leqslant \beta and α+β<π\alpha + \beta < \pi, we have 0<ϕ<π20 < \phi < \frac{\pi}{2} so cos⁡ϕ<1\cos\phi < 1 (strict, since α+β<π\alpha + \beta < \pi), and 0⩽α−β2<π20 \leqslant \frac{\alpha-\beta}{2} < \frac{\pi}{2} so sin⁡ ⁣α−β2<1\sin\!\tfrac{\alpha-\beta}{2} < 1. Therefore:

4cos⁡2ϕsin⁡2 ⁣α−β2<14\cos^2\phi\sin^2\!\tfrac{\alpha-\beta}{2} < 1

which gives Δ>0\Delta > 0, so (∗)(*) has distinct real roots. □\square

Part (iii)

(a) α=β=45°\alpha = \beta = 45°: cos⁡(α+β)=cos⁡90°=0\cos(\alpha+\beta) = \cos 90° = 0, cos⁡α+cos⁡β=2\cos\alpha + \cos\beta = \sqrt{2}.

x2−22 x+1=0x^2 - 2\sqrt{2}\,x + 1 = 0

x=22±8−42=2±1x = \frac{2\sqrt{2} \pm \sqrt{8 - 4}}{2} = \sqrt{2} \pm 1

So x=2+1x = \sqrt{2} + 1 (extended case, PP and QQ beyond CC) or x=2−1x = \sqrt{2} - 1 (internal case, PP and QQ on ACAC and BCBC).

In both cases PQPQ is horizontal (θ=0\theta = 0) since α=β\alpha = \beta gives xsin⁡θ=x(sin⁡β−sin⁡α)=0x\sin\theta = x(\sin\beta - \sin\alpha) = 0.

(b) α=30°\alpha = 30°, β=90°\beta = 90°: α+β=120°\alpha + \beta = 120°, so (∗)(*) is linear:

−2(cos⁡30°+cos⁡90°)x+1=0  ⟹  −3 x+1=0  ⟹  x=13=33-2(\cos 30° + \cos 90°)x + 1 = 0 \implies -\sqrt{3}\,x + 1 = 0 \implies x = \frac{1}{\sqrt{3}} = \frac{\sqrt{3}}{3}

Since BCBC is vertical (angle 90°90° at BB) and QB=33QB = \frac{\sqrt{3}}{3}, while BCBC has length 33\frac{\sqrt{3}}{3} (by the sine rule), QQ coincides with CC. Then PP is the midpoint of ACAC.

Examiner Notes

While the first part of the question was successfully completed by many of the candidates, there were quite a few diagrams drawn showing the point P further from the line AB than Q. Those who established the expression for xcos⁡θx \cos \theta were usually able to find an expression for xsin⁡θx \sin \theta and good justifications of the quadratic equation were given. The case where P and Q lie on the lines AC produced and BC produced caused a lot of difficulty for many of the candidates, many of whom tried unsuccessfully to create an argument based on similar triangles.

The condition for (*) to be linear in xx did not cause much difficulty, although a number of candidates did not give the value of cos⁡−1(−12)\cos^{-1} \left( -\frac{1}{2} \right). Many candidates realised that the justification that the roots were distinct would involve the discriminant, although some solutions included the case where the discriminant could be equal to 0 were produced. However, very few solutions were able to give a clear justification that the discriminant must be greater than 0.

In the final part some candidates sketched the graph of the quadratic rather than sketching the triangle in the two cases given. In the second case many candidates did not realise that Q was at the same point as C.


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

2 This question concerns the inequality

∫0π(f(x))2 dx⩽∫0π(f′(x))2 dx.(*)\int_{0}^{\pi} (f(x))^2 \, \mathrm{d}x \leqslant \int_{0}^{\pi} (f'(x))^2 \, \mathrm{d}x . \qquad \text{(*)}

(i) Show that (∗)(*) is satisfied in the case f(x)=sin⁡nxf(x) = \sin nx, where nn is a positive integer.

Show by means of counterexamples that (∗)(*) is not necessarily satisfied if either f(0)≠0f(0) \neq 0 or f(π)≠0f(\pi) \neq 0.

(ii) You may now assume that (∗)(*) is satisfied for any (differentiable) function ff for which f(0)=f(π)=0f(0) = f(\pi) = 0.

By setting f(x)=ax2+bx+cf(x) = ax^2 + bx + c, where a,ba, b and cc are suitably chosen, show that π2⩽10\pi^2 \leqslant 10.

By setting f(x)=psin⁡12x+qcos⁡12x+rf(x) = p \sin \frac{1}{2}x + q \cos \frac{1}{2}x + r, where p,qp, q and rr are suitably chosen, obtain another inequality for π\pi.

Which of these inequalities leads to a better estimate for π2\pi^2?

Hint

By rewriting in terms of cos⁡2nx\cos 2nx it can be shown that ∫0πsin⁡2nx dx=π2\int_{0}^{\pi} \sin^2 nx \, dx = \frac{\pi}{2} and ∫0πn2cos⁡2nx dx=n2π2\int_{0}^{\pi} n^2 \cos^2 nx \, dx = \frac{n^2 \pi}{2}. Therefore () must be satisfied as nn is a positive integer. The function f(x)=xf(x) = x does not satisfy () and f(0)=0f(0) = 0 but f(π)≠0f(\pi) \neq 0. The function g(x)=f(π−x)g(x) = f(\pi - x) will therefore provide a counterexample where g(π)=0g(\pi) = 0, but g(0)≠0g(0) \neq 0.

In part (ii), f(x)=x2−πxf(x) = x^2 - \pi x will need to be selected to be able to use the assumption that () is satisfied. The two sides of () can then be evaluated:

∫0πx4−2πx3+π2x2 dx=π530\int_{0}^{\pi} x^4 - 2\pi x^3 + \pi^2 x^2 \, dx = \frac{\pi^5}{30}

∫0π4x2−4πx+π2 dx=π33\int_{0}^{\pi} 4x^2 - 4\pi x + \pi^2 \, dx = \frac{\pi^3}{3}

Substitution into (*) then leads to the inequality π2≤10\pi^2 \leq 10.

To satisfy the conditions on f(x)f(x) for the second type of function, the values of pp, qq and rr must satisfy q+r=0q + r = 0 and p+r=0p + r = 0. Evaluating the integrals then leads to π≤227\pi \leq \frac{22}{7}.

Since (227)2<10(\frac{22}{7})^2 < 10, π≤227\pi \leq \frac{22}{7} leads to a better estimate for π2\pi^2.

Model Solution

Part (i)

Let f(x)=sin⁡nxf(x) = \sin nx where nn is a positive integer. Then f′(x)=ncos⁡nxf'(x) = n\cos nx.

Left side:

∫0πsin⁡2nx dx=∫0π1−cos⁡2nx2 dx=π2−12[sin⁡2nx2n]0π=π2\int_0^\pi \sin^2 nx \, dx = \int_0^\pi \frac{1 - \cos 2nx}{2} \, dx = \frac{\pi}{2} - \frac{1}{2}\left[\frac{\sin 2nx}{2n}\right]_0^\pi = \frac{\pi}{2}

since sin⁡2nπ=0\sin 2n\pi = 0.

Right side:

∫0πn2cos⁡2nx dx=n2∫0π1+cos⁡2nx2 dx=n2π2\int_0^\pi n^2\cos^2 nx \, dx = n^2 \int_0^\pi \frac{1 + \cos 2nx}{2} \, dx = \frac{n^2\pi}{2}

Since n⩾1n \geqslant 1, we have n2π2⩾π2\frac{n^2\pi}{2} \geqslant \frac{\pi}{2}, so (∗)(*) is satisfied. □\square

Counterexamples:

Case f(π)≠0f(\pi) \neq 0: Let f(x)=xf(x) = x. Then f(0)=0f(0) = 0 but f(π)=π≠0f(\pi) = \pi \neq 0. We have f′(x)=1f'(x) = 1, so:

∫0πx2 dx=π33,∫0π1 dx=π\int_0^\pi x^2 \, dx = \frac{\pi^3}{3}, \qquad \int_0^\pi 1 \, dx = \pi

Since π33>π\frac{\pi^3}{3} > \pi (as π2>3\pi^2 > 3), (∗)(*) is violated.

Case f(0)≠0f(0) \neq 0: Let g(x)=f(π−x)=π−xg(x) = f(\pi - x) = \pi - x. Then g(π)=0g(\pi) = 0 but g(0)=π≠0g(0) = \pi \neq 0. We have g′(x)=−1g'(x) = -1, so:

∫0π(π−x)2 dx=π33,∫0π1 dx=π\int_0^\pi (\pi - x)^2 \, dx = \frac{\pi^3}{3}, \qquad \int_0^\pi 1 \, dx = \pi

Again π33>π\frac{\pi^3}{3} > \pi, so (∗)(*) is violated. □\square

Part (ii)

Quadratic function: Choose f(x)=x2−πxf(x) = x^2 - \pi x so that f(0)=0f(0) = 0 and f(π)=π2−π2=0f(\pi) = \pi^2 - \pi^2 = 0.

Left side:

∫0π(x2−πx)2 dx=∫0π(x4−2πx3+π2x2) dx\int_0^\pi (x^2 - \pi x)^2 \, dx = \int_0^\pi (x^4 - 2\pi x^3 + \pi^2 x^2) \, dx

=[x55−2πx44+π2x33]0π=π55−π52+π53=π5(6−15+1030)=π530= \left[\frac{x^5}{5} - \frac{2\pi x^4}{4} + \frac{\pi^2 x^3}{3}\right]_0^\pi = \frac{\pi^5}{5} - \frac{\pi^5}{2} + \frac{\pi^5}{3} = \pi^5\left(\frac{6 - 15 + 10}{30}\right) = \frac{\pi^5}{30}

Right side: f′(x)=2x−πf'(x) = 2x - \pi, so:

∫0π(2x−π)2 dx=∫0π(4x2−4πx+π2) dx=[4x33−2πx2+π2x]0π\int_0^\pi (2x - \pi)^2 \, dx = \int_0^\pi (4x^2 - 4\pi x + \pi^2) \, dx = \left[\frac{4x^3}{3} - 2\pi x^2 + \pi^2 x\right]_0^\pi

=4π33−2π3+π3=π3(43−1)=π33= \frac{4\pi^3}{3} - 2\pi^3 + \pi^3 = \pi^3\left(\frac{4}{3} - 1\right) = \frac{\pi^3}{3}

By (∗)(*): π530⩽π33\frac{\pi^5}{30} \leqslant \frac{\pi^3}{3}, giving π2⩽10\pi^2 \leqslant 10. □\square

Trigonometric function: Choose f(x)=psin⁡x2+qcos⁡x2+rf(x) = p\sin\frac{x}{2} + q\cos\frac{x}{2} + r with f(0)=f(π)=0f(0) = f(\pi) = 0:

f(0)=q+r=0  ⟹  q=−rf(0) = q + r = 0 \implies q = -r f(π)=p+r=0  ⟹  p=−rf(\pi) = p + r = 0 \implies p = -r

So f(x)=r(−sin⁡x2−cos⁡x2+1)f(x) = r(-\sin\frac{x}{2} - \cos\frac{x}{2} + 1), and we may take r=1r = 1 (the inequality is homogeneous in rr), giving f(x)=1−sin⁡x2−cos⁡x2f(x) = 1 - \sin\frac{x}{2} - \cos\frac{x}{2}.

Left side: f(x)2=1+sin⁡2x2+cos⁡2x2−2sin⁡x2−2cos⁡x2+2sin⁡x2cos⁡x2f(x)^2 = 1 + \sin^2\frac{x}{2} + \cos^2\frac{x}{2} - 2\sin\frac{x}{2} - 2\cos\frac{x}{2} + 2\sin\frac{x}{2}\cos\frac{x}{2}

=2−2sin⁡x2−2cos⁡x2+sin⁡x= 2 - 2\sin\frac{x}{2} - 2\cos\frac{x}{2} + \sin x

∫0πf(x)2 dx=2π−2 ⁣∫0π ⁣sin⁡x2 dx−2 ⁣∫0π ⁣cos⁡x2 dx+∫0π ⁣sin⁡x dx\int_0^\pi f(x)^2 \, dx = 2\pi - 2\!\int_0^\pi\!\sin\frac{x}{2}\,dx - 2\!\int_0^\pi\!\cos\frac{x}{2}\,dx + \int_0^\pi\!\sin x\,dx

=2π−2[−2cos⁡x2]0π−2[2sin⁡x2]0π+[−cos⁡x]0π= 2\pi - 2\left[-2\cos\frac{x}{2}\right]_0^\pi - 2\left[2\sin\frac{x}{2}\right]_0^\pi + [-\cos x]_0^\pi

=2π−2(−2⋅0+2)−2(2−0)+(1+1)=2π−4−4+2=2π−6= 2\pi - 2(-2\cdot 0 + 2) - 2(2 - 0) + (1 + 1) = 2\pi - 4 - 4 + 2 = 2\pi - 6

Right side: f′(x)=−12cos⁡x2+12sin⁡x2f'(x) = -\frac{1}{2}\cos\frac{x}{2} + \frac{1}{2}\sin\frac{x}{2}, so f′(x)2=14cos⁡2x2+14sin⁡2x2−12sin⁡x2cos⁡x2f'(x)^2 = \frac{1}{4}\cos^2\frac{x}{2} + \frac{1}{4}\sin^2\frac{x}{2} - \frac{1}{2}\sin\frac{x}{2}\cos\frac{x}{2}

=14−12sin⁡x2cos⁡x2=14−14sin⁡x= \frac{1}{4} - \frac{1}{2}\sin\frac{x}{2}\cos\frac{x}{2} = \frac{1}{4} - \frac{1}{4}\sin x

∫0πf′(x)2 dx=π4−14∫0πsin⁡x dx=π4−14⋅2=π4−12=π−24\int_0^\pi f'(x)^2 \, dx = \frac{\pi}{4} - \frac{1}{4}\int_0^\pi \sin x \, dx = \frac{\pi}{4} - \frac{1}{4}\cdot 2 = \frac{\pi}{4} - \frac{1}{2} = \frac{\pi - 2}{4}

By (∗)(*): 2π−6⩽π−242\pi - 6 \leqslant \frac{\pi - 2}{4}, so 8π−24⩽π−28\pi - 24 \leqslant \pi - 2, giving 7π⩽227\pi \leqslant 22, i.e., π⩽227\pi \leqslant \frac{22}{7}.

Comparison: Since (227)2=48449≈9.878<10\left(\frac{22}{7}\right)^2 = \frac{484}{49} \approx 9.878 < 10, the inequality π⩽227\pi \leqslant \frac{22}{7} gives a better estimate for π2\pi^2. □\square

Examiner Notes

This was one of the more popular questions of the paper. Most candidates successfully showed that the first inequality was satisfied, but when producing counterexamples, some failed to show that either f(x)≠0f(x) \neq 0 or f(π)≠0f(\pi) \neq 0 for their chosen functions. In the second part many candidates did not attempt to choose values of aa, bb and cc, but substituted the general form of the quadratic function into the inequality instead. In the case where the function involved trigonometric functions, many of those who attempted it were able to deduce that p=q=−rp = q = -r, but several candidates made mistakes in the required integration. Those who established two inequalities were able to decide which gives the better estimate for π\pi.


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

3 (i) Show, geometrically or otherwise, that the shortest distance between the origin and the line y=mx+cy = mx + c, where c⩾0c \geqslant 0, is c(m2+1)−12c(m^2 + 1)^{-\frac{1}{2}}.

(ii) The curve CC lies in the xx-yy plane. Let the line LL be tangent to CC at a point PP on CC, and let aa be the shortest distance between the origin and LL. The curve CC has the property that the distance aa is the same for all points PP on CC.

Let PP be the point on CC with coordinates (x,y(x))(x, y(x)). Given that the tangent to CC at PP is not vertical, show that

(y−xy′)2=a2(1+(y′)2).(*)(y - xy')^2 = a^2(1 + (y')^2) . \qquad \text{(*)}

By first differentiating (∗)(*) with respect to xx, show that either y=mx±a(1+m2)12y = mx \pm a(1 + m^2)^{\frac{1}{2}} for some mm or x2+y2=a2x^2 + y^2 = a^2.

(iii) Now suppose that CC (as defined above) is a continuous curve for −∞<x<∞-\infty < x < \infty, consisting of the arc of a circle and two straight lines. Sketch an example of such a curve which has a non-vertical tangent at each point.

Hint

By drawing a diagram and marking the shortest distance a pair of similar triangles can be used to show that c/mcm2+1/m=dc\frac{c/m}{c\sqrt{m^2+1}/m} = \frac{d}{c}, which simplifies to d=c/m2+1d = c/\sqrt{m^2 + 1}.

For the second part, the tangent to the curve at the general point (x,y)(x, y) will have a gradient of y′y' and so the yy-intercept will be at the point (0,y−xy′)(0, y - xy'). Therefore the result from part (i) can be applied using m=y′m = y' and c=y−xy′c = y - xy' to give a=(y−xy′)/(y′)2+1a = (y - xy')/\sqrt{(y')^2 + 1}, which rearranges to give the required result.

Differentiating the equation then gives y′′(a2y′+x(y−xy′))=0y''(a^2y' + x(y - xy')) = 0 and so either y′′=0y'' = 0 or

a2y′+x(y−xy′)=0.a^2y' + x(y - xy') = 0.

If y′′=0y'' = 0 then the equation will be of a straight line and the yy-intercept can be deduced in terms of mm.

If a2y′+x(y−xy′)=0a^2y' + x(y - xy') = 0, then the differential equation can be solved to give the equation of a circle.

Part (iii) then requires combining the two possible cases from part (ii) to construct a curve which satisfies the conditions given. This must be an arc of a circle with no vertical tangents, with straight lines at either end of the arc in the direction of the tangents to the circle at that point.

Model Solution

Part (i)

The line y=mx+cy = mx + c can be written as mx−y+c=0mx - y + c = 0. The perpendicular from the origin to this line has gradient −1m-\frac{1}{m}, so its equation is y=−xmy = -\frac{x}{m}.

Substituting into y=mx+cy = mx + c:

−xm=mx+c  ⟹  −x=m2x+mc  ⟹  x=−mcm2+1-\frac{x}{m} = mx + c \implies -x = m^2 x + mc \implies x = -\frac{mc}{m^2 + 1}

y=−xm=cm2+1y = -\frac{x}{m} = \frac{c}{m^2 + 1}

The distance from the origin to this point is:

d=x2+y2=m2c2(m2+1)2+c2(m2+1)2=cm2+1m2+1=cm2+1=c(m2+1)−1/2d = \sqrt{x^2 + y^2} = \sqrt{\frac{m^2 c^2}{(m^2+1)^2} + \frac{c^2}{(m^2+1)^2}} = \frac{c\sqrt{m^2 + 1}}{m^2 + 1} = \frac{c}{\sqrt{m^2 + 1}} = c(m^2+1)^{-1/2}

since c⩾0c \geqslant 0. □\square

Part (ii)

The tangent to CC at P=(x,y)P = (x, y) has gradient y′y', so its equation is:

Y−y=y′(X−x)  ⟹  Y=y′X+(y−xy′)Y - y = y'(X - x) \implies Y = y'X + (y - xy')

This has gradient m=y′m = y' and yy-intercept c=y−xy′c = y - xy'. By part (i), the distance from the origin to this tangent is:

a=y−xy′1+(y′)2a = \frac{y - xy'}{\sqrt{1 + (y')^2}}

Squaring: a2(1+(y′)2)=(y−xy′)2a^2(1 + (y')^2) = (y - xy')^2. □\square

Differentiating (∗)(*): Differentiate both sides with respect to xx:

LHS: 2a2y′y′′\text{LHS: } 2a^2 y' y''

RHS: 2(y−xy′)⋅ddx(y−xy′)=2(y−xy′)(y′−y′−xy′′)=−2xy′′(y−xy′)\text{RHS: } 2(y - xy') \cdot \frac{d}{dx}(y - xy') = 2(y - xy')(y' - y' - xy'') = -2xy''(y - xy')

So: 2a2y′y′′=−2xy′′(y−xy′)2a^2 y' y'' = -2xy''(y - xy')

y′′(a2y′+x(y−xy′))=0y''\left(a^2 y' + x(y - xy')\right) = 0

Case 1: y′′=0y'' = 0. Then y=mx+ky = mx + k for constants mm and kk. Substituting into (∗)(*):

a2(1+m2)=(y−xy′)2=(mx+k−mx)2=k2a^2(1 + m^2) = (y - xy')^2 = (mx + k - mx)^2 = k^2

k=±a1+m2k = \pm a\sqrt{1 + m^2}

So y=mx±a(1+m2)1/2y = mx \pm a(1 + m^2)^{1/2}. □\square

Case 2: a2y′+x(y−xy′)=0a^2 y' + x(y - xy') = 0. Rearranging:

a2y′+xy−x2y′=0  ⟹  y′(a2−x2)=−xy  ⟹  dydx=−xya2−x2a^2 y' + xy - x^2 y' = 0 \implies y'(a^2 - x^2) = -xy \implies \frac{dy}{dx} = \frac{-xy}{a^2 - x^2}

Separating variables: dyy=−xa2−x2 dx=xx2−a2 dx\frac{dy}{y} = \frac{-x}{a^2 - x^2}\,dx = \frac{x}{x^2 - a^2}\,dx

Integrating: ln⁡∣y∣=12ln⁡∣x2−a2∣+const\ln|y| = \frac{1}{2}\ln|x^2 - a^2| + \text{const}

y2=K(x2−a2)y^2 = K(x^2 - a^2)

Substituting into (∗)(*): (y−xy′)2=a2(1+(y′)2)(y - xy')^2 = a^2(1 + (y')^2).

From the DE: y′=−xya2−x2y' = \frac{-xy}{a^2 - x^2}, so y−xy′=y+x2ya2−x2=a2ya2−x2y - xy' = y + \frac{x^2 y}{a^2 - x^2} = \frac{a^2 y}{a^2 - x^2}.

(∗)(*) gives: a4y2(a2−x2)2=a2(1+x2y2(a2−x2)2)=a2⋅(a2−x2)2+x2y2(a2−x2)2\frac{a^4 y^2}{(a^2 - x^2)^2} = a^2\left(1 + \frac{x^2 y^2}{(a^2 - x^2)^2}\right) = a^2 \cdot \frac{(a^2 - x^2)^2 + x^2 y^2}{(a^2 - x^2)^2}

a2y2=(a2−x2)2+x2y2a^2 y^2 = (a^2 - x^2)^2 + x^2 y^2

y2(a2−x2)=(a2−x2)2y^2(a^2 - x^2) = (a^2 - x^2)^2

If a2≠x2a^2 \neq x^2: y2=a2−x2y^2 = a^2 - x^2, i.e., x2+y2=a2x^2 + y^2 = a^2. □\square

Part (iii)

From part (ii), the curve CC consists of straight lines y=mx±a1+m2y = mx \pm a\sqrt{1+m^2} and/or circular arcs x2+y2=a2x^2 + y^2 = a^2.

To construct a continuous curve for −∞<x<∞-\infty < x < \infty with no vertical tangent, take the lower semicircle x2+y2=a2x^2 + y^2 = a^2 (i.e., y=−a2−x2y = -\sqrt{a^2 - x^2}) for −acos⁡ϕ⩽x⩽acos⁡ϕ-a\cos\phi \leqslant x \leqslant a\cos\phi (where 0<ϕ<π20 < \phi < \frac{\pi}{2}), and attach tangent lines at the endpoints.

At the point (acos⁡ϕ,−asin⁡ϕ)(a\cos\phi, -a\sin\phi) on the circle, the tangent has gradient −cot⁡ϕ-\cot\phi (from implicit differentiation 2x+2yy′=02x + 2yy' = 0 gives y′=−x/y=−cot⁡ϕy' = -x/y = -\cot\phi). The tangent line is:

y+asin⁡ϕ=−cot⁡ϕ(x−acos⁡ϕ)y + a\sin\phi = -\cot\phi(x - a\cos\phi)

This line extends to x→+∞x \to +\infty. Similarly, at (−acos⁡ϕ,−asin⁡ϕ)(-a\cos\phi, -a\sin\phi), the tangent has gradient cot⁡ϕ\cot\phi and extends to x→−∞x \to -\infty.

The resulting curve is continuous, has non-vertical tangent at every point (choose ϕ\phi so that cot⁡ϕ\cot\phi is finite, i.e., ϕ≠π2\phi \neq \frac{\pi}{2}), and consists of one circular arc and two straight lines. □\square

Examiner Notes

Many candidates produced a correct solution to the first part of the question. There were a number of popular methods, such as the use of similar triangles, but an algebraic approach finding the intersection between the line and a perpendicular line through the origin was the most popular. Some candidates however, simply stated a formula for the shortest distance from a point to a line. Establishing the differential equation in the second part of the question was generally done well, but many candidates struggled with the solution of the differential equation. A common error was to ignore the case y′′=0y'' = 0 and simply find the circle solution.

The final part of the question was attempted by only a few of the candidates, many of whom did not produce an example that satisfied all of the conditions stated in the question, in particular the condition that the tangents should not be vertical at any point was often missed.


Topic: 微积分 (Calculus)  |  Difficulty: Standard  |  Marks: 20

4 (i) By using the substitution u=1/xu = 1/x, show that for b>0b > 0

∫1/bbxln⁡x(a2+x2)(a2x2+1) dx=0.\int_{1/b}^{b} \frac{x \ln x}{(a^2 + x^2)(a^2x^2 + 1)} \, dx = 0 .

(ii) By using the substitution u=1/xu = 1/x, show that for b>0b > 0,

∫1/bbarctan⁡xx dx=πln⁡b2.\int_{1/b}^{b} \frac{\arctan x}{x} \, dx = \frac{\pi \ln b}{2} .

(iii) By using the result ∫0∞1a2+x2 dx=π2a\int_{0}^{\infty} \frac{1}{a^2 + x^2} \, dx = \frac{\pi}{2a} (where a>0a > 0), and a substitution of the

form u=k/xu = k/x, for suitable kk, show that

∫0∞1(a2+x2)2 dx=π4a3(a>0).\int_{0}^{\infty} \frac{1}{(a^2 + x^2)^2} \, dx = \frac{\pi}{4a^3} \quad (a > 0) .

Hint

In part (i), if the required integral is called II then the given substitution leads to an integral which can be shown to be equal to −I-I. This means that 2I=02I = 0 and so I=0I = 0.

In part (ii), once the substitution has been completed, the integral will simplify to ∫1/bbarctan⁡1uudu\int_{1/b}^{b} \frac{\arctan \frac{1}{u}}{u} du. Since arctan⁡x+arctan⁡(1x)=π2\arctan x + \arctan \left(\frac{1}{x}\right) = \frac{\pi}{2} the integral can be shown to be equal to 12∫1/bbπ2xdx\frac{1}{2} \int_{1/b}^{b} \frac{\pi}{2x} dx, which then simplifies to the required result.

In part (iii), making with the substitution in terms of kk and simplifying will show that the integral is equivalent to

∫0∞ku2(a2u2+k2)2du\int_{0}^{\infty} \frac{ku^2}{(a^2u^2 + k^2)^2} du

Therefore choosing k=a2k = a^2, the integral can be simplified further to

1a2∫0∞u2(a2+u2)2du=1a2∫0∞1a2+u2du−1a2∫0∞a2(a2+u2)2du\frac{1}{a^2} \int_{0}^{\infty} \frac{u^2}{(a^2 + u^2)^2} du = \frac{1}{a^2} \int_{0}^{\infty} \frac{1}{a^2 + u^2} du - \frac{1}{a^2} \int_{0}^{\infty} \frac{a^2}{(a^2 + u^2)^2} du

The result then follows by using the given value for ∫0∞1a2+x2dx\int_{0}^{\infty} \frac{1}{a^2+x^2} dx.

Model Solution

Part (i)

Let I=∫1/bbxln⁡x(a2+x2)(a2x2+1) dxI = \int_{1/b}^{b} \frac{x\ln x}{(a^2 + x^2)(a^2 x^2 + 1)}\,dx.

Substitute u=1/xu = 1/x, so x=1/ux = 1/u, dx=−1/u2 dudx = -1/u^2\,du. When x=1/bx = 1/b, u=bu = b; when x=bx = b, u=1/bu = 1/b.

I=∫b1/b1uln⁡1u(a2+1u2)(a2u2+1)⋅−1u2 duI = \int_{b}^{1/b} \frac{\frac{1}{u}\ln\frac{1}{u}}{\left(a^2 + \frac{1}{u^2}\right)\left(\frac{a^2}{u^2} + 1\right)} \cdot \frac{-1}{u^2}\,du

Simplify the denominator:

a2+1u2=a2u2+1u2,a2u2+1=a2+u2u2a^2 + \frac{1}{u^2} = \frac{a^2 u^2 + 1}{u^2}, \qquad \frac{a^2}{u^2} + 1 = \frac{a^2 + u^2}{u^2}

So the denominator is (a2u2+1)(a2+u2)u4\frac{(a^2 u^2 + 1)(a^2 + u^2)}{u^4}.

The integrand becomes:

−ln⁡u/u(a2u2+1)(a2+u2)/u4⋅−1u2=ln⁡u⋅u(a2u2+1)(a2+u2)\frac{-\ln u / u}{(a^2 u^2 + 1)(a^2 + u^2)/u^4} \cdot \frac{-1}{u^2} = \frac{\ln u \cdot u}{(a^2 u^2 + 1)(a^2 + u^2)}

Reversing the limits (which removes the negative sign):

I=∫1/bbuln⁡u(a2+u2)(a2u2+1) du=II = \int_{1/b}^{b} \frac{u\ln u}{(a^2 + u^2)(a^2 u^2 + 1)}\,du = I

But we also had a sign change from ln⁡(1/u)=−ln⁡u\ln(1/u) = -\ln u, so actually I=−II = -I, giving 2I=02I = 0, hence I=0I = 0. □\square

Part (ii)

Let I=∫1/bbarctan⁡xx dxI = \int_{1/b}^{b} \frac{\arctan x}{x}\,dx.

Substitute u=1/xu = 1/x, dx=−1/u2 dudx = -1/u^2\,du. When x=1/bx = 1/b, u=bu = b; when x=bx = b, u=1/bu = 1/b.

I=∫b1/barctan⁡(1/u)1/u⋅−1u2 du=∫1/bbarctan⁡(1/u)u duI = \int_{b}^{1/b} \frac{\arctan(1/u)}{1/u} \cdot \frac{-1}{u^2}\,du = \int_{1/b}^{b} \frac{\arctan(1/u)}{u}\,du

Using the identity arctan⁡(1/u)=π2−arctan⁡u\arctan(1/u) = \frac{\pi}{2} - \arctan u (for u>0u > 0):

I=∫1/bbπ2−arctan⁡uu du=π2∫1/bbduu−∫1/bbarctan⁡uu duI = \int_{1/b}^{b} \frac{\frac{\pi}{2} - \arctan u}{u}\,du = \frac{\pi}{2}\int_{1/b}^{b} \frac{du}{u} - \int_{1/b}^{b} \frac{\arctan u}{u}\,du

Since ∫1/bbduu=[ln⁡u]1/bb=ln⁡b−ln⁡(1/b)=2ln⁡b\int_{1/b}^{b} \frac{du}{u} = [\ln u]_{1/b}^{b} = \ln b - \ln(1/b) = 2\ln b, and the second integral equals II:

I=π2⋅2ln⁡b−I=πln⁡b−II = \frac{\pi}{2} \cdot 2\ln b - I = \pi\ln b - I

2I=πln⁡b  ⟹  I=πln⁡b2□2I = \pi\ln b \implies I = \frac{\pi\ln b}{2} \qquad \square

Part (iii)

Let J=∫0∞dx(a2+x2)2J = \int_0^\infty \frac{dx}{(a^2 + x^2)^2}.

Substitute u=a2/xu = a^2/x (so k=a2k = a^2), x=a2/ux = a^2/u, dx=−a2/u2 dudx = -a^2/u^2\,du. When x=0x = 0, u=∞u = \infty; when x=∞x = \infty, u=0u = 0.

J=∫∞01(a2+a4u2)2⋅−a2u2 du=∫0∞a2/u2(a2u2+a4u2)2 duJ = \int_{\infty}^{0} \frac{1}{\left(a^2 + \frac{a^4}{u^2}\right)^2} \cdot \frac{-a^2}{u^2}\,du = \int_0^\infty \frac{a^2/u^2}{\left(\frac{a^2 u^2 + a^4}{u^2}\right)^2}\,du

=∫0∞a2u2a4(u2+a2)2 du=1a2∫0∞u2(u2+a2)2 du= \int_0^\infty \frac{a^2 u^2}{a^4(u^2 + a^2)^2}\,du = \frac{1}{a^2}\int_0^\infty \frac{u^2}{(u^2 + a^2)^2}\,du

Write u2(u2+a2)2=(u2+a2)−a2(u2+a2)2=1u2+a2−a2(u2+a2)2\frac{u^2}{(u^2 + a^2)^2} = \frac{(u^2 + a^2) - a^2}{(u^2 + a^2)^2} = \frac{1}{u^2 + a^2} - \frac{a^2}{(u^2 + a^2)^2}

So: J=1a2∫0∞duu2+a2−1a2∫0∞a2 du(u2+a2)2=1a2⋅π2a−JJ = \frac{1}{a^2}\int_0^\infty \frac{du}{u^2 + a^2} - \frac{1}{a^2}\int_0^\infty \frac{a^2\,du}{(u^2 + a^2)^2} = \frac{1}{a^2} \cdot \frac{\pi}{2a} - J

2J=π2a3  ⟹  J=π4a3□2J = \frac{\pi}{2a^3} \implies J = \frac{\pi}{4a^3} \qquad \square

Examiner Notes

Many candidates were able to perform the given substitution correctly and then correctly explain how this demonstrates that the integral is equal to 1. The second part caused more difficulty, particularly with candidates not able to state the relationship between arctan⁡x\arctan x and arctan⁡(1x)\arctan (\frac{1}{x}). Attempts to integrate with the substitution v=arctan⁡(1u)v = \arctan (\frac{1}{u}) often resulted in an incorrect application of the chain rule when finding dvdu\frac{dv}{du}.

In the final part of the question many candidates attempted to use integration by parts to reach the given answer.


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

5 Given that y=xuy = xu, where uu is a function of xx, write down an expression for dydx\frac{dy}{dx}.

(i) Use the substitution y=xuy = xu to solve

dydx=2y+xy−2x\frac{dy}{dx} = \frac{2y + x}{y - 2x}

given that the solution curve passes through the point (1,1)(1, 1).

Give your answer in the form of a quadratic in xx and yy.

(ii) Using the substitutions x=X+ax = X + a and y=Y+by = Y + b for appropriate values of aa and bb, or otherwise, solve

dydx=x−2y−42x+y−3,\frac{dy}{dx} = \frac{x - 2y - 4}{2x + y - 3},

given that the solution curve passes through the point (1,1)(1, 1).

Hint

Using the substitution y=xuy = xu, the differential equation can be simplified to

xdudx=1+4u−u2u−2x \frac{du}{dx} = \frac{1 + 4u - u^2}{u - 2}

This can be solved by separating the variables after which making the substitution u=yxu = \frac{y}{x} and substituting the point on the curve gives the required quadratic in xx and yy.

In part (ii), dYdX\frac{dY}{dX} can be shown to be equal to dydx\frac{dy}{dx}. The values of aa and bb need to be chosen so that the right hand side of the differential equation has no constant terms in the numerator or denominator. This leads to the simultaneous equations:

a−2b−4=0a - 2b - 4 = 0

2a+b−3=02a + b - 3 = 0

Solving these and substituting the values into the differential equation gives dYdX=X−2Y2X+Y\frac{dY}{dX} = \frac{X - 2Y}{2X + Y}, and so

dXdY=2X+YX−2Y\frac{dX}{dY} = \frac{2X + Y}{X - 2Y}

This is the same differential equation as in part (i), with x=Yx = Y and y=Xy = X. Most of the solution in part (i) can therefore be applied, but the point on the curve is different, so the constant in the final solution will need to be calculated for this case.

Model Solution

If y=xuy = xu, then dydx=u+xdudx\frac{dy}{dx} = u + x\frac{du}{dx}.

Part (i)

Substituting into dydx=2y+xy−2x\frac{dy}{dx} = \frac{2y + x}{y - 2x}:

u+xdudx=2xu+xxu−2x=2u+1u−2u + x\frac{du}{dx} = \frac{2xu + x}{xu - 2x} = \frac{2u + 1}{u - 2}

xdudx=2u+1u−2−u=2u+1−u(u−2)u−2=−u2+4u+1u−2x\frac{du}{dx} = \frac{2u + 1}{u - 2} - u = \frac{2u + 1 - u(u - 2)}{u - 2} = \frac{-u^2 + 4u + 1}{u - 2}

Separating variables:

u−2−u2+4u+1 du=dxx\frac{u - 2}{-u^2 + 4u + 1}\,du = \frac{dx}{x}

Factor the denominator: −u2+4u+1=−(u2−4u−1)=−(u−2−3)(u−2+3)-u^2 + 4u + 1 = -(u^2 - 4u - 1) = -(u - 2 - \sqrt{3})(u - 2 + \sqrt{3}).

Let v=u−2v = u - 2. Then the integrand becomes −v(v−3)(v+3)\frac{-v}{(v - \sqrt{3})(v + \sqrt{3})}. Partial fractions:

−v(v−3)(v+3)=Av−3+Bv+3\frac{-v}{(v - \sqrt{3})(v + \sqrt{3})} = \frac{A}{v - \sqrt{3}} + \frac{B}{v + \sqrt{3}}

A=−323=−12A = \frac{-\sqrt{3}}{2\sqrt{3}} = -\frac{1}{2}, B=3−23=−12\quad B = \frac{\sqrt{3}}{-2\sqrt{3}} = -\frac{1}{2}

So: ∫(−1/2v−3+−1/2v+3)dv=ln⁡∣x∣+C\int \left(\frac{-1/2}{v - \sqrt{3}} + \frac{-1/2}{v + \sqrt{3}}\right)dv = \ln|x| + C

−12ln⁡∣v−3∣−12ln⁡∣v+3∣=ln⁡∣x∣+C-\frac{1}{2}\ln|v - \sqrt{3}| - \frac{1}{2}\ln|v + \sqrt{3}| = \ln|x| + C

−12ln⁡∣v2−3∣=ln⁡∣x∣+C-\frac{1}{2}\ln|v^2 - 3| = \ln|x| + C

ln⁡∣v2−3∣=−2ln⁡∣x∣−2C=ln⁡(x−2)+C′\ln|v^2 - 3| = -2\ln|x| - 2C = \ln(x^{-2}) + C'

∣v2−3∣=Kx2|v^2 - 3| = \frac{K}{x^2}

Substituting v=u−2=yx−2=y−2xxv = u - 2 = \frac{y}{x} - 2 = \frac{y - 2x}{x}:

(y−2xx)2−3=Kx2\left(\frac{y - 2x}{x}\right)^2 - 3 = \frac{K}{x^2}

(y−2x)2−3x2=K(y - 2x)^2 - 3x^2 = K

y2−4xy+4x2−3x2=Ky^2 - 4xy + 4x^2 - 3x^2 = K

x2−4xy+y2=Kx^2 - 4xy + y^2 = K

Applying the initial condition (1,1)(1, 1): 1−4+1=K1 - 4 + 1 = K, so K=−2K = -2.

x2−4xy+y2=−2x^2 - 4xy + y^2 = -2

or equivalently: y2−4xy+x2+2=0y^2 - 4xy + x^2 + 2 = 0. □\square

Part (ii)

With x=X+ax = X + a, y=Y+by = Y + b: dydx=dYdX\frac{dy}{dx} = \frac{dY}{dX}. The DE becomes:

dYdX=(X+a)−2(Y+b)−42(X+a)+(Y+b)−3=X−2Y+(a−2b−4)2X+Y+(2a+b−3)\frac{dY}{dX} = \frac{(X + a) - 2(Y + b) - 4}{2(X + a) + (Y + b) - 3} = \frac{X - 2Y + (a - 2b - 4)}{2X + Y + (2a + b - 3)}

Set constant terms to zero:

a−2b=42a+b=3a - 2b = 4 \qquad 2a + b = 3

From the first: a=4+2ba = 4 + 2b. Substituting: 8+4b+b=3  ⟹  b=−18 + 4b + b = 3 \implies b = -1, a=2a = 2.

The DE becomes dYdX=X−2Y2X+Y\frac{dY}{dX} = \frac{X - 2Y}{2X + Y}, which is the same form as part (i) (with XX and YY in place of xx and yy).

From part (i), the solution is Y2−4XY+X2=KY^2 - 4XY + X^2 = K.

The point (x,y)=(1,1)(x, y) = (1, 1) corresponds to (X,Y)=(1−2,1−(−1))=(−1,2)(X, Y) = (1 - 2, 1 - (-1)) = (-1, 2).

4−4(−1)(2)+1=K  ⟹  K=134 - 4(-1)(2) + 1 = K \implies K = 13

Substituting back X=x−2X = x - 2, Y=y+1Y = y + 1:

(y+1)2−4(x−2)(y+1)+(x−2)2=13(y + 1)^2 - 4(x - 2)(y + 1) + (x - 2)^2 = 13

Expanding:

y2+2y+1−4(xy+x−2y−2)+x2−4x+4=13y^2 + 2y + 1 - 4(xy + x - 2y - 2) + x^2 - 4x + 4 = 13

y2+2y+1−4xy−4x+8y+8+x2−4x+4=13y^2 + 2y + 1 - 4xy - 4x + 8y + 8 + x^2 - 4x + 4 = 13

x2−4xy+y2−8x+10y=0x^2 - 4xy + y^2 - 8x + 10y = 0

y2−4xy+x2−8x+10y=0□y^2 - 4xy + x^2 - 8x + 10y = 0 \qquad \square

Examiner Notes

This was the most popular question on the paper and the question which had the highest average score. Most candidates correctly solved the differential equation in the first part of the question, but many then calculated the constant term incorrectly. In the second part of the question most candidates were able to find the appropriate values of a and b, but then did not see how to apply the result from part (i) and so did the integration again or just copied the answer from the first part. Some candidates again struggled to obtain the correct constant for the integration and others did not substitute the correct values for the point on the curve (taking (X,Y)(X, Y) as (1,1)(1, 1) rather than (x,y)(x, y)).


Topic: 三角函数与级数 (Trigonometric Series)  |  Difficulty: Challenging  |  Marks: 20

6 By simplifying sin⁡(r+12)x−sin⁡(r−12)x\sin(r + \frac{1}{2})x - \sin(r - \frac{1}{2})x or otherwise show that, for sin⁡12x≠0\sin \frac{1}{2}x \neq 0,

cos⁡x+cos⁡2x+⋯+cos⁡nx=sin⁡(n+12)x−sin⁡12x2sin⁡12x.\cos x + \cos 2x + \dots + \cos nx = \frac{\sin(n + \frac{1}{2})x - \sin \frac{1}{2}x}{2 \sin \frac{1}{2}x}.

The functions SnS_n, for n=1,2,…n = 1, 2, \dots, are defined by

Sn(x)=∑r=1n1rsin⁡rx(0⩽x⩽π).S_n(x) = \sum_{r=1}^{n} \frac{1}{r} \sin rx \quad (0 \leqslant x \leqslant \pi).

(i) Find the stationary points of S2(x)S_2(x) for 0⩽x⩽π0 \leqslant x \leqslant \pi, and sketch this function.

(ii) Show that if Sn(x)S_n(x) has a stationary point at x=x0x = x_0, where 0<x0<π0 < x_0 < \pi, then

sin⁡nx0=(1−cos⁡nx0)tan⁡12x0\sin nx_0 = (1 - \cos nx_0) \tan \frac{1}{2}x_0

and hence that Sn(x0)⩾Sn−1(x0)S_n(x_0) \geqslant S_{n-1}(x_0). Deduce that if Sn−1(x)>0S_{n-1}(x) > 0 for all xx in the interval 0<x<π0 < x < \pi, then Sn(x)>0S_n(x) > 0 for all xx in this interval.

(iii) Prove that Sn(x)⩾0S_n(x) \geqslant 0 for n⩾1n \geqslant 1 and 0⩽x⩽π0 \leqslant x \leqslant \pi.

Hint

One of the standard trigonometric formulas can be used to show that

sin⁡(r+12)x−sin⁡(r−12)x=2cos⁡rxsin⁡12x.\sin \left( r + \frac{1}{2} \right) x - \sin \left( r - \frac{1}{2} \right) x = 2 \cos rx \sin \frac{1}{2} x.

Summing these from r=1r = 1 to r=nr = n will then give the required result.

In part (i), the definition can be rewritten as S2(x)=sin⁡x+12sin⁡2xS_2(x) = \sin x + \frac{1}{2} \sin 2x. The stationary points can then be evaluated by differentiating the function. The sketch is then easy to complete.

For part (ii), differentiating the function gives Sn′(x)=cos⁡x+cos⁡2x+⋯+cos⁡nxS'_n(x) = \cos x + \cos 2x + \dots + \cos nx. Applying the result from the start of the question, this can be written as

Sn′(x)=sin⁡(n+12x)−sin⁡12x2sin⁡12xS'_n(x) = \frac{\sin(n + \frac{1}{2}x) - \sin \frac{1}{2}x}{2 \sin \frac{1}{2}x}

Since sin⁡12x≠0\sin \frac{1}{2}x \neq 0 in the given range, the stationary points are where sin⁡(n+12)x−sin⁡12x=0\sin (n + \frac{1}{2})x - \sin \frac{1}{2}x = 0. This can then be simplified to the required form by splitting (n+12)x(n + \frac{1}{2})x into functions of nxnx and 12x\frac{1}{2}x and noting that sin⁡12x≠0\sin \frac{1}{2}x \neq 0 and cos⁡12x≠0\cos \frac{1}{2}x \neq 0 in the given range, so both can be divided by. By noting that the difference between Sn−1(x)S_{n-1}(x) and Sn(x)S_n(x) is 1nsin⁡nx\frac{1}{n} \sin nx the result just shown can be used to show the final result of part (ii). Part (iii) then follows by induction.

Model Solution

Preliminary result: Using the identity sin⁡A−sin⁡B=2cos⁡A+B2sin⁡A−B2\sin A - \sin B = 2\cos\frac{A+B}{2}\sin\frac{A-B}{2}:

sin⁡ ⁣(r+12)x−sin⁡ ⁣(r−12)x=2cos⁡(rx)sin⁡ ⁣x2\sin\!\left(r + \tfrac{1}{2}\right)x - \sin\!\left(r - \tfrac{1}{2}\right)x = 2\cos(rx)\sin\!\tfrac{x}{2}

Summing from r=1r = 1 to r=nr = n:

∑r=1n2cos⁡(rx)sin⁡ ⁣x2=∑r=1n[sin⁡ ⁣(r+12)x−sin⁡ ⁣(r−12)x]\sum_{r=1}^{n} 2\cos(rx)\sin\!\tfrac{x}{2} = \sum_{r=1}^{n}\left[\sin\!\left(r + \tfrac{1}{2}\right)x - \sin\!\left(r - \tfrac{1}{2}\right)x\right]

The right side telescopes:

=sin⁡ ⁣(n+12)x−sin⁡ ⁣x2= \sin\!\left(n + \tfrac{1}{2}\right)x - \sin\!\tfrac{x}{2}

Dividing by 2sin⁡x22\sin\frac{x}{2} (which is nonzero for sin⁡x2≠0\sin\frac{x}{2} \neq 0):

cos⁡x+cos⁡2x+⋯+cos⁡nx=sin⁡(n+12)x−sin⁡x22sin⁡x2□\cos x + \cos 2x + \cdots + \cos nx = \frac{\sin(n + \frac{1}{2})x - \sin\frac{x}{2}}{2\sin\frac{x}{2}} \qquad \square

Part (i)

S2(x)=sin⁡x+12sin⁡2xS_2(x) = \sin x + \frac{1}{2}\sin 2x.

S2′(x)=cos⁡x+cos⁡2xS_2'(x) = \cos x + \cos 2x

Using cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1:

S2′(x)=2cos⁡2x+cos⁡x−1=(2cos⁡x−1)(cos⁡x+1)S_2'(x) = 2\cos^2 x + \cos x - 1 = (2\cos x - 1)(\cos x + 1)

Setting S2′(x)=0S_2'(x) = 0: cos⁡x=12\cos x = \frac{1}{2} (giving x=π3x = \frac{\pi}{3}) or cos⁡x=−1\cos x = -1 (giving x=πx = \pi).

At x=0x = 0: S2(0)=0S_2(0) = 0. At x=π3x = \frac{\pi}{3}: S2=32+34=334S_2 = \frac{\sqrt{3}}{2} + \frac{\sqrt{3}}{4} = \frac{3\sqrt{3}}{4}. At x=πx = \pi: S2(π)=0S_2(\pi) = 0.

The stationary points are x=π3x = \frac{\pi}{3} (maximum) and x=πx = \pi (endpoint minimum).

Sketch: S2S_2 starts at 00, rises to 334≈1.30\frac{3\sqrt{3}}{4} \approx 1.30 at x=π3x = \frac{\pi}{3}, then falls back to 00 at x=πx = \pi. The curve is smooth and positive on (0,π)(0, \pi).

Part (ii)

Sn′(x)=cos⁡x+cos⁡2x+⋯+cos⁡nx=sin⁡(n+12)x−sin⁡x22sin⁡x2S_n'(x) = \cos x + \cos 2x + \cdots + \cos nx = \frac{\sin(n + \frac{1}{2})x - \sin\frac{x}{2}}{2\sin\frac{x}{2}}

At a stationary point x0∈(0,π)x_0 \in (0, \pi), we have Sn′(x0)=0S_n'(x_0) = 0, so:

sin⁡ ⁣(n+12)x0=sin⁡ ⁣x02\sin\!\left(n + \tfrac{1}{2}\right)x_0 = \sin\!\tfrac{x_0}{2}

Since sin⁡x02≠0\sin\frac{x_0}{2} \neq 0 and cos⁡x02≠0\cos\frac{x_0}{2} \neq 0 for x0∈(0,π)x_0 \in (0, \pi), we expand sin⁡(n+12)x0=sin⁡(nx0)cos⁡x02+cos⁡(nx0)sin⁡x02\sin(n + \frac{1}{2})x_0 = \sin(nx_0)\cos\frac{x_0}{2} + \cos(nx_0)\sin\frac{x_0}{2}:

sin⁡(nx0)cos⁡ ⁣x02+cos⁡(nx0)sin⁡ ⁣x02=sin⁡ ⁣x02\sin(nx_0)\cos\!\tfrac{x_0}{2} + \cos(nx_0)\sin\!\tfrac{x_0}{2} = \sin\!\tfrac{x_0}{2}

sin⁡(nx0)cos⁡ ⁣x02=sin⁡ ⁣x02(1−cos⁡(nx0))\sin(nx_0)\cos\!\tfrac{x_0}{2} = \sin\!\tfrac{x_0}{2}(1 - \cos(nx_0))

Dividing by cos⁡x02\cos\frac{x_0}{2}:

sin⁡(nx0)=(1−cos⁡(nx0))tan⁡ ⁣x02□\sin(nx_0) = (1 - \cos(nx_0))\tan\!\tfrac{x_0}{2} \qquad \square

Since tan⁡x02>0\tan\frac{x_0}{2} > 0 for x0∈(0,π)x_0 \in (0, \pi) and 1−cos⁡(nx0)⩾01 - \cos(nx_0) \geqslant 0, we conclude sin⁡(nx0)⩾0\sin(nx_0) \geqslant 0.

Now Sn(x0)=Sn−1(x0)+1nsin⁡(nx0)S_n(x_0) = S_{n-1}(x_0) + \frac{1}{n}\sin(nx_0), so:

Sn(x0)⩾Sn−1(x0)□S_n(x_0) \geqslant S_{n-1}(x_0) \qquad \square

Deduction: If Sn−1(x)>0S_{n-1}(x) > 0 for all x∈(0,π)x \in (0, \pi), then at every interior stationary point of SnS_n we have Sn(x0)⩾Sn−1(x0)>0S_n(x_0) \geqslant S_{n-1}(x_0) > 0. Since Sn(0)=Sn(π)=0S_n(0) = S_n(\pi) = 0, the minimum of SnS_n on [0,π][0, \pi] is either 00 (at the endpoints) or occurs at an interior stationary point where Sn>0S_n > 0. In either case, Sn(x)⩾0S_n(x) \geqslant 0 for 0⩽x⩽π0 \leqslant x \leqslant \pi, and since SnS_n is not identically zero, Sn(x)>0S_n(x) > 0 for 0<x<π0 < x < \pi. □\square

Part (iii)

We prove Sn(x)⩾0S_n(x) \geqslant 0 for all n⩾1n \geqslant 1 and 0⩽x⩽π0 \leqslant x \leqslant \pi by induction.

Base case: S1(x)=sin⁡x⩾0S_1(x) = \sin x \geqslant 0 for x∈[0,π]x \in [0, \pi]. ✓\checkmark

Inductive step: Assume Sn−1(x)⩾0S_{n-1}(x) \geqslant 0 for x∈[0,π]x \in [0, \pi].

SnS_n is continuous on [0,π][0, \pi] with Sn(0)=0S_n(0) = 0 and Sn(π)=0S_n(\pi) = 0. If SnS_n achieves a negative value, its minimum on [0,π][0, \pi] must be negative and occur at an interior point x0∈(0,π)x_0 \in (0, \pi) (since SnS_n is non-negative at the endpoints). At such a minimum, Sn′(x0)=0S_n'(x_0) = 0.

By part (ii), Sn(x0)⩾Sn−1(x0)⩾0S_n(x_0) \geqslant S_{n-1}(x_0) \geqslant 0 (by the inductive hypothesis). This contradicts Sn(x0)<0S_n(x_0) < 0.

Therefore Sn(x)⩾0S_n(x) \geqslant 0 for all x∈[0,π]x \in [0, \pi]. By induction, the result holds for all n⩾1n \geqslant 1. □\square

Examiner Notes

This was one of the less popular of the pure maths questions, but the average mark achieved on this paper was one of the highest for the paper. The first section did not present too much difficulty for the majority of candidates, with a variety of methods being used to show the first result such as proof by induction or use of ex=cos⁡x+isin⁡xe^x = \cos x + i \sin x. In the second part of the question many of the candidates struggled to explain the reasoning clearly to show the required result. Most candidates who reached the final part of the question realised that the previous part provides the basis for a proof by induction.


Topic: 绝对值函数与方程 (Absolute Value Functions & Equations)  |  Difficulty: Standard  |  Marks: 20

7 (i) The function ff is defined by f(x)=∣x−a∣+∣x−b∣f(x) = |x - a| + |x - b|, where a<ba < b. Sketch the graph of f(x)f(x), giving the gradient in each of the regions x<ax < a, a<x<ba < x < b and x>bx > b. Sketch on the same diagram the graph of g(x)g(x), where g(x)=∣2x−a−b∣g(x) = |2x - a - b|.

What shape is the quadrilateral with vertices (a,0)(a, 0), (b,0)(b, 0), (b,f(b))(b, f(b)) and (a,f(a))(a, f(a))?

(ii) Show graphically that the equation

∣x−a∣+∣x−b∣=∣x−c∣,|x - a| + |x - b| = |x - c|,

where a<ba < b, has 0, 1 or 2 solutions, stating the relationship of cc to aa and bb in each case.

(iii) For the equation

∣x−a∣+∣x−b∣=∣x−c∣+∣x−d∣,|x - a| + |x - b| = |x - c| + |x - d|,

where a<ba < b, c<dc < d and d−c<b−ad - c < b - a, determine the number of solutions in the various cases that arise, stating the relationship between a,b,ca, b, c and dd in each case.

Hint

By considering the regions x≤ax \le a, a<x<ba < x < b and x≥bx \ge b, f(x)f(x) can be written as

f(x)=a+b−2xx≤ab−aa<x<b2x−a−bx≥bf(x) = \begin{matrix} a + b - 2x & x \le a \\ b - a & a < x < b \\ 2x - a - b & x \ge b \end{matrix}

Therefore the graph of y=f(x)y = f(x) will be made up of two sloping sections (with gradients 2 and -2 and a horizontal section). The graph of y=g(x)y = g(x) will have the same definition in the regions x≤ax \le a and x≥bx \ge b, with the sloping edges extending to a point of intersection on the xx-axis. The quadrilateral with therefore have sides of equal length and right angles at each vertex, so it is a square.

In part (ii), sketches of the cases where c=ac = a and c=bc = b show that these cases give just one solution. If a<c<ba < c < b there will be no solutions and in the other regions there will be two solutions.

In part (iii) the graphs for the two sides of the equation can be related to graphs of the form of g(x)g(x) (apart from the section which is replaced by a horizontal line) in the first part of the question. Since d−c<b−ad - c < b - a, the horizontal sections of the two graphs must be at different heights so the number of solutions can be seen to be the same as the number of intersections of the graphs of the form of g(x)g(x).

Model Solution

Part (i)

For f(x)=∣x−a∣+∣x−b∣f(x) = |x - a| + |x - b| with a<ba < b, consider three regions:

  • x⩽ax \leqslant a: f(x)=(a−x)+(b−x)=a+b−2xf(x) = (a - x) + (b - x) = a + b - 2x (gradient −2-2)
  • a<x<ba < x < b: f(x)=(x−a)+(b−x)=b−af(x) = (x - a) + (b - x) = b - a (gradient 00)
  • x⩾bx \geqslant b: f(x)=(x−a)+(x−b)=2x−a−bf(x) = (x - a) + (x - b) = 2x - a - b (gradient +2+2)

The graph is a “tent” shape: two sloped lines meeting a flat section at height b−ab - a over [a,b][a, b].

For g(x)=∣2x−a−b∣=2∣x−a+b2∣g(x) = |2x - a - b| = 2|x - \frac{a+b}{2}|:

  • x⩽a+b2x \leqslant \frac{a+b}{2}: g(x)=a+b−2xg(x) = a + b - 2x (gradient −2-2)
  • x⩾a+b2x \geqslant \frac{a+b}{2}: g(x)=2x−a−bg(x) = 2x - a - b (gradient +2+2)

The graph of gg is a V-shape with vertex at (a+b2,0)(\frac{a+b}{2}, 0). Note that gg and ff share the same sloped edges for x⩽ax \leqslant a and x⩾bx \geqslant b.

The quadrilateral: The vertices are (a,0)(a, 0), (b,0)(b, 0), (b,b−a)(b, b-a), (a,b−a)(a, b-a). This has:

  • Bottom edge from (a,0)(a,0) to (b,0)(b,0): length b−ab - a
  • Right edge from (b,0)(b,0) to (b,b−a)(b,b-a): length b−ab - a
  • Top edge from (b,b−a)(b,b-a) to (a,b−a)(a,b-a): length b−ab - a
  • Left edge from (a,b−a)(a,b-a) to (a,0)(a,0): length b−ab - a

All sides equal and all angles 90°90°, so the quadrilateral is a square. □\square

Part (ii)

The equation ∣x−a∣+∣x−b∣=∣x−c∣|x - a| + |x - b| = |x - c| asks for intersections of y=f(x)y = f(x) (the tent) with y=∣x−c∣y = |x - c| (a V-shape with vertex at (c,0)(c, 0)).

Since the vertex of ∣x−c∣|x - c| lies on the xx-axis (the bottom edge of the square), the V starts at the base of the tent.

  • a<c<ba < c < b: The V-vertex is at (c,0)(c, 0), below the flat section of ff (which is at height b−a>0b - a > 0). The V’s slopes (±1\pm 1) are shallower than ff‘s slopes (±2\pm 2), so the V stays below ff everywhere. 0 solutions.

  • c<ac < a or c>bc > b: The V-vertex is outside [a,b][a, b]. On the side nearest to [a,b][a, b], the V rises with slope 11 while ff rises with slope 22, so ff starts above the V and the V cannot catch up. On the opposite side, the V rises with slope 11 and ff rises with slope 22, but ff starts above the V. However, on the far side of [a,b][a, b], ff and the V have the same slope directions but ff starts at height b−a>0b - a > 0 while the V starts from 00. The V intersects each sloped edge of ff exactly once. 2 solutions.

  • c=ac = a or c=bc = b: The V-vertex coincides with a corner of the square. One entire sloped edge of ff overlaps with one ray of the V. Infinitely many solutions (all xx on the overlapping edge).

In summary: 0 solutions if a<c<ba < c < b; 2 solutions if c<ac < a or c>bc > b; infinitely many if c=ac = a or c=bc = b.

Part (iii)

Let f(x)=∣x−a∣+∣x−b∣f(x) = |x - a| + |x - b| and h(x)=∣x−c∣+∣x−d∣h(x) = |x - c| + |x - d|. Both are tent-shaped with flat sections of heights b−ab - a and d−cd - c respectively. Since d−c<b−ad - c < b - a, ff‘s flat section is higher.

For xx outside both intervals, ff and hh have the same gradient (±2\pm 2), so f−hf - h is constant in those regions. The key is to compare the flat sections and the transitions between regions.

Case 1: [c,d]∩[a,b]=∅[c, d] \cap [a, b] = \emptyset (i.e., d⩽ad \leqslant a or b⩽cb \leqslant c): In the region between the two intervals, one function is flat and the other is sloped, and they cross. In the outer regions, both have gradient ±2\pm 2 with ff above hh. 2 solutions.

Case 2: a⩽c<d⩽ba \leqslant c < d \leqslant b ([c,d]⊆[a,b][c,d] \subseteq [a,b]): The flat section of hh (height d−cd - c) sits below the flat section of ff (height b−ab - a). At x=cx = c, ff is still decreasing (gradient −2-2) while hh becomes flat; they cross once on the left. By symmetry, they cross once on the right. 2 solutions.

Case 3: c<a<b<dc < a < b < d ([a,b]⊆[c,d][a,b] \subseteq [c,d]): The flat section of hh (height d−cd - c) is lower than ff‘s flat section (height b−ab - a). In [a,b][a, b], f=b−a>d−c=hf = b - a > d - c = h. For x⩽cx \leqslant c, both decrease with gradient −2-2 and hh is below ff. For x⩾dx \geqslant d, both increase with gradient 22 and hh is below ff. 0 solutions.

Case 4: c<a<d<bc < a < d < b (partial overlap, [c,d][c,d] extends left of [a,b][a,b]): The flat sections are at different heights (d−c<b−ad - c < b - a). Depending on the relative positions:

  • If c+d<a+bc + d < a + b: one crossing on the left transition and one below ff‘s flat section that does not occur (the flat section of hh is too low). 1 solution.
  • If c+d=a+bc + d = a + b: the right-hand outer edges coincide for x⩾dx \geqslant d. Infinitely many solutions.
  • If c+d>a+bc + d > a + b: the right-hand outer edges are separated with ff below hh, giving an additional crossing. 2 solutions.

Case 5: a<c<b<da < c < b < d (partial overlap, [c,d][c,d] extends right of [a,b][a,b]): By symmetry with Case 4:

  • If c+d<a+bc + d < a + b: 2 solutions.
  • If c+d=a+bc + d = a + b: Infinitely many solutions.
  • If c+d>a+bc + d > a + b: 1 solution.
Examiner Notes

This was another of the less popular pure maths questions. The nature of this question meant that many solutions involved a series of sketches of graphs with very little written explanation. Most candidates were able to identify that the sloping edges of y=f(x)y = f(x) would have the same gradient as the sloping edges of y=g(x)y = g(x), but many did not have both sloping edges overlapping for the two graphs. In some cases only one sloping edge of y=g(x)y = g(x) was drawn. A large number of candidates who correctly sketched the graphs identified the quadrilateral as a rectangle, rather than a square. In the second part of the question, sketches of the case with one solution often did not have the graph of y=∣x−c∣y = |x - c| meeting the xx-axis at one corner of the square identified in part (i), although many candidates were able to identify the different cases that could occur. Unfortunately in the final part of the question very few candidates used the result from the first part of the question and so considered a number of possibilities that do not exist for any values of a, b, c and d.


Topic: 二项式展开与组合数学 (Binomial Expansion & Combinatorics)  |  Difficulty: Hard  |  Marks: 20

8 For positive integers n,an, a and bb, the integer crc_r (0⩽r⩽n0 \leqslant r \leqslant n) is defined to be the coefficient of xrx^r in the expansion in powers of xx of (a+bx)n(a + bx)^n. Write down an expression for crc_r in terms of r,n,ar, n, a and bb.

For given n,an, a and bb, let mm denote a value of rr for which crc_r is greatest (that is, cm⩾crc_m \geqslant c_r for 0⩽r⩽n0 \leqslant r \leqslant n).

Show that

b(n+1)a+b−1⩽m⩽b(n+1)a+b.\frac{b(n + 1)}{a + b} - 1 \leqslant m \leqslant \frac{b(n + 1)}{a + b}.

Deduce that mm is either a unique integer or one of two consecutive integers.

Let G(n,a,b)G(n, a, b) denote the unique value of mm (if there is one) or the larger of the two possible values of mm.

(i) Evaluate G(9,1,3)G(9, 1, 3) and G(9,2,3)G(9, 2, 3).

(ii) For any positive integer kk, find G(2k,a,a)G(2k, a, a) and G(2k−1,a,a)G(2k - 1, a, a) in terms of kk.

(iii) For fixed nn and bb, determine a value of aa for which G(n,a,b)G(n, a, b) is greatest.

(iv) For fixed nn, find the greatest possible value of G(n,1,b)G(n, 1, b). For which values of bb is this greatest value achieved?

Hint

The coefficients from the binomial expansion should be easily written down. It can then be shown that

cr+1cr=b(n−r)a(r+1)\frac{c_{r+1}}{c_r} = \frac{b(n - r)}{a(r + 1)}

This will be greater than 1 (indicating that the value of crc_r is increasing) while b(n−r)>a(r+1)b(n - r) > a(r + 1), which simplifies to r<nb−aa+br < \frac{nb - a}{a + b}. Similarly, cr+1cr=1\frac{c_{r+1}}{c_r} = 1 if r=nb−aa+br = \frac{nb - a}{a + b} and cr+1cr<1\frac{c_{r+1}}{c_r} < 1 if r>nb−aa+br > \frac{nb - a}{a + b}. Therefore the maximum value of crc_r will be the first integer after nb−aa+b\frac{nb - a}{a + b} (and there will be two maximum values for crc_r if nb−aa+b\frac{nb - a}{a + b} is an integer. The required inequality summarises this information.

In parts (i) and (ii) the values need to be substituted into the inequality. Where there are two possible values, it needs to be checked that they are equal before taking the higher if this has not been justified in the first case.

In part (iii) the greatest value will be achieved when the denominator takes the smallest possible value, therefore a=1a = 1, and then in part (iv) the greatest value will be achieved by maximising the numerator. Since the maximum possible value of G(n,a,b)G(n, a, b) is nn, b≥nb \ge n will achieve this maximum.

Model Solution

General setup: By the binomial theorem, (a+bx)n=∑r=0n(nr)an−rbrxr(a + bx)^n = \sum_{r=0}^{n} \binom{n}{r} a^{n-r} b^r x^r, so:

cr=(nr)an−rbrc_r = \binom{n}{r} a^{n-r} b^r

Bounding mm: Consider the ratio:

cr+1cr=(nr+1)an−r−1br+1(nr)an−rbr=n−rr+1⋅ba\frac{c_{r+1}}{c_r} = \frac{\binom{n}{r+1} a^{n-r-1} b^{r+1}}{\binom{n}{r} a^{n-r} b^r} = \frac{n - r}{r + 1} \cdot \frac{b}{a}

cr+1>crc_{r+1} > c_r when b(n−r)a(r+1)>1\frac{b(n - r)}{a(r + 1)} > 1, i.e., bn−br>ar+abn - br > ar + a, i.e., r(a+b)<nb−ar(a + b) < nb - a:

r<nb−aa+br < \frac{nb - a}{a + b}

Similarly, cr+1=crc_{r+1} = c_r when r=nb−aa+br = \frac{nb - a}{a + b} and cr+1<crc_{r+1} < c_r when r>nb−aa+br > \frac{nb - a}{a + b}.

So crc_r increases while r<nb−aa+br < \frac{nb - a}{a + b} and decreases after. The maximum cmc_m occurs at:

m=⌈nb−aa+b⌉m = \left\lceil \frac{nb - a}{a + b} \right\rceil

If nb−aa+b\frac{nb - a}{a + b} is an integer, then cm=cm−1c_m = c_{m-1} and both mm and m−1m - 1 are maximizers.

Writing nb−aa+b=nba+b−aa+b\frac{nb - a}{a + b} = \frac{nb}{a + b} - \frac{a}{a + b}, and noting 0<aa+b<10 < \frac{a}{a+b} < 1:

nba+b−1<m⩽nba+b□\frac{nb}{a + b} - 1 < m \leqslant \frac{nb}{a + b} \qquad \square

mm is unique or two consecutive integers: The interval (nba+b−1,nba+b]\left(\frac{nb}{a+b} - 1, \frac{nb}{a+b}\right] has length 11. If nba+b\frac{nb}{a+b} is not an integer, it contains exactly one integer (namely ⌈nba+b⌉\lceil \frac{nb}{a+b} \rceil). If nba+b\frac{nb}{a+b} is an integer, it contains exactly two integers: nba+b\frac{nb}{a+b} and nba+b−1\frac{nb}{a+b} - 1. □\square

Part (i)

G(9,1,3)G(9, 1, 3): nba+b=9×31+3=274=6.75\frac{nb}{a+b} = \frac{9 \times 3}{1 + 3} = \frac{27}{4} = 6.75.

The interval is (5.75,6.75](5.75, 6.75], so m=6m = 6. Since 6.756.75 is not an integer, mm is unique.

G(9,2,3)G(9, 2, 3): nba+b=9×32+3=275=5.4\frac{nb}{a+b} = \frac{9 \times 3}{2 + 3} = \frac{27}{5} = 5.4.

The interval is (4.4,5.4](4.4, 5.4], so m=5m = 5. Since 5.45.4 is not an integer, mm is unique. □\square

Part (ii)

G(2k,a,a)G(2k, a, a): nb−aa+b=2ka−a2a=k−12\frac{nb - a}{a+b} = \frac{2ka - a}{2a} = k - \frac{1}{2}.

This is not an integer, so m=⌈k−12⌉=km = \lceil k - \frac{1}{2} \rceil = k is unique. G(2k,a,a)=kG(2k, a, a) = k. □\square

G(2k−1,a,a)G(2k - 1, a, a): We use the condition on nb−aa+b\frac{nb - a}{a+b}:

nb−aa+b=(2k−1)a−a2a=k−1\frac{nb - a}{a+b} = \frac{(2k-1)a - a}{2a} = k - 1

This is an integer, so ck−1=ckc_{k-1} = c_k (both are maximizers). GG takes the larger: G(2k−1,a,a)=kG(2k - 1, a, a) = k. □\square

Part (iii)

G(n,a,b)=⌈nba+b⌉G(n, a, b) = \left\lceil \frac{nb}{a + b} \right\rceil (taking the larger value when there are two maximizers).

For fixed nn and bb, to maximize GG we need to maximize nba+b\frac{nb}{a + b}. Since nbnb is fixed, we minimize a+ba + b, which means minimizing aa. Since aa is a positive integer, a=1a = 1.

G(n,1,b)=⌈nb1+b⌉□G(n, 1, b) = \left\lceil \frac{nb}{1 + b} \right\rceil \qquad \square

Part (iv)

G(n,1,b)=⌈nbb+1⌉G(n, 1, b) = \left\lceil \frac{nb}{b + 1} \right\rceil. Note that nbb+1=n−nb+1\frac{nb}{b+1} = n - \frac{n}{b+1}.

This is maximized when nb+1\frac{n}{b+1} is minimized, i.e., when b+1b + 1 divides nn and b+1b + 1 is as large as possible. But even without divisibility, nbb+1→n\frac{nb}{b+1} \to n as b→∞b \to \infty.

For G(n,1,b)=nG(n, 1, b) = n, we need nbb+1>n−1\frac{nb}{b+1} > n - 1, i.e., nb>(n−1)(b+1)=nb+n−b−1nb > (n-1)(b+1) = nb + n - b - 1, i.e., b>n−1b > n - 1, i.e., b⩾nb \geqslant n.

When b⩾nb \geqslant n: nbb+1⩾n2n+1=n−nn+1>n−1\frac{nb}{b+1} \geqslant \frac{n^2}{n+1} = n - \frac{n}{n+1} > n - 1, so G(n,1,b)=nG(n, 1, b) = n.

When b<nb < n: nbb+1<n(n−1)n=n−1\frac{nb}{b+1} < \frac{n(n-1)}{n} = n - 1, so G(n,1,b)⩽n−1G(n, 1, b) \leqslant n - 1.

Therefore the greatest possible value of G(n,1,b)G(n, 1, b) is nn, achieved for all b⩾nb \geqslant n. □\square

Examiner Notes

This was the least popular of the pure maths questions and also the one with the lowest average score. Many of the candidates were able to show the required result at the start of the question, although very few candidates explained that mm could be either of the two integers when the range included two integers. Parts (i) and (ii) were then quite straightforward for most candidates, although many calculated the range of values but did not justify their choice in the case where there were two possibilities. In the final two parts of the question some candidates mistakenly chose the value 0 when asked for a positive integer.