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STEP2 2016 -- Pure Mathematics

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STEP2 2016 — Section A (Pure Mathematics)

Section titled “STEP2 2016 — Section A (Pure Mathematics)”

Exam: STEP2  |  Year: 2016  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1曲线与方程 (Curves and Equations)Standard参数方程求导,切线方程,向量垂直条件,联立方程消参,多项式因式分解
2代数 (Algebra)Standard因式定理,对称多项式分解,变量代换,方程求根
3多项式与级数 (Polynomials and Series)Challenging逐项求导,多项式符号分析,反证法(无穷根矛盾),中间值定理,无穷远处渐近行为
4不等式与函数 (Inequalities and Functions)Challenging二次方程判别式,辅助角公式 R cos(theta+alpha),不等式传递性,根式化简
5组合数学 (Combinatorics)Challenging负二项式展开,幂级数乘法比较系数,Vandermonde 恒等式,组合数定义扩展
6微分方程 (Differential Equations)Challenging验证微分方程的解, 链式法则, 函数复合, Chebyshev多项式性质
7积分 (Integration)Standard积分换元 u=axu=a-x, 三角恒等式, 对数运算, 分部积分
8级数与积分近似 (Series and Integration Approximation)Challenging积分近似级数, 草图论证, 误差分析, 中点近似

Topic: 曲线与方程 (Curves and Equations)  |  Difficulty: Standard  |  Marks: 20

1 The curve C1C_1 has parametric equations x=t2x = t^2, y=t3y = t^3, where <t<-\infty < t < \infty. Let OO denote the point (0,0)(0, 0). The points PP and QQ on C1C_1 are such that POQ\angle POQ is a right angle. Show that the tangents to C1C_1 at PP and QQ intersect on the curve C2C_2 with equation 4y2=3x14y^2 = 3x - 1.

Determine whether C1C_1 and C2C_2 meet, and sketch the two curves on the same axes.

Hint

Let PP have parameter t1t_1 and QQ have parameter t2t_2 on C1C_1.

The derivative dydx=dy/dtdx/dt=3t22t=3t2\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{3t^2}{2t} = \frac{3t}{2} (for t0t \neq 0).

The tangent at P(t1)P(t_1): yt13=3t12(xt12)y - t_1^3 = \frac{3t_1}{2}(x - t_1^2), i.e. y=3t12xt132y = \frac{3t_1}{2}x - \frac{t_1^3}{2}.

Similarly the tangent at Q(t2)Q(t_2): y=3t22xt232y = \frac{3t_2}{2}x - \frac{t_2^3}{2}.

Since POQ=90°\angle POQ = 90°, we need OPOQ=0\vec{OP} \cdot \vec{OQ} = 0: t12t22+t13t23=0    t12t22(1+t1t2)=0t_1^2 t_2^2 + t_1^3 t_2^3 = 0 \implies t_1^2 t_2^2(1 + t_1 t_2) = 0

Since P,QOP, Q \neq O, we have t1t2=1t_1 t_2 = -1.

Setting the two tangent equations equal to find intersection: 3t12xt132=3t22xt232\frac{3t_1}{2}x - \frac{t_1^3}{2} = \frac{3t_2}{2}x - \frac{t_2^3}{2}

32(t1t2)x=12(t13t23)=12(t1t2)(t12+t1t2+t22)\frac{3}{2}(t_1 - t_2)x = \frac{1}{2}(t_1^3 - t_2^3) = \frac{1}{2}(t_1 - t_2)(t_1^2 + t_1 t_2 + t_2^2)

So x=t12+t1t2+t223=t12+t2213x = \frac{t_1^2 + t_1 t_2 + t_2^2}{3} = \frac{t_1^2 + t_2^2 - 1}{3}.

Substituting back: y=3t12t12+t2213t132=t1(t221)2y = \frac{3t_1}{2} \cdot \frac{t_1^2 + t_2^2 - 1}{3} - \frac{t_1^3}{2} = \frac{t_1(t_2^2 - 1)}{2}.

Using t2=1/t1t_2 = -1/t_1: x=t12+1/t1213x = \frac{t_1^2 + 1/t_1^2 - 1}{3} and y=t1(1/t121)2=1t122t1y = \frac{t_1(1/t_1^2 - 1)}{2} = \frac{1 - t_1^2}{2t_1}.

Let u=t12u = t_1^2. Then x=u+1/u13x = \frac{u + 1/u - 1}{3} and y2=(1u)24u=u22u+14u=u+1/u24y^2 = \frac{(1-u)^2}{4u} = \frac{u^2 - 2u + 1}{4u} = \frac{u + 1/u - 2}{4}.

So u+1/u=3x+1u + 1/u = 3x + 1, giving y2=3x+124=3x14y^2 = \frac{3x + 1 - 2}{4} = \frac{3x - 1}{4}, i.e. 4y2=3x14y^2 = 3x - 1.

This is the curve C2C_2, as required.

Do C1C_1 and C2C_2 meet? Substituting x=t2,y=t3x = t^2, y = t^3 into 4y2=3x14y^2 = 3x - 1: 4t6=3t21    4t63t2+1=04t^6 = 3t^2 - 1 \implies 4t^6 - 3t^2 + 1 = 0

Let u=t20u = t^2 \geq 0: 4u33u+1=04u^3 - 3u + 1 = 0. Testing u=1u = -1: 4(1)3(1)+1=4+3+1=04(-1) - 3(-1) + 1 = -4+3+1 = 0, so u+1u+1 is a factor.

4u33u+1=(u+1)(4u24u+1)=(u+1)(2u1)24u^3 - 3u + 1 = (u+1)(4u^2 - 4u + 1) = (u+1)(2u-1)^2.

Since u=t20u = t^2 \geq 0, the only solution is u=1/2u = 1/2, i.e. t=±1/2t = \pm 1/\sqrt{2}. Since (2u1)2(2u-1)^2 is a repeated root, the curves are tangent (touch but do not cross) at the points where t=±1/2t = \pm 1/\sqrt{2}.

Sketch: C1C_1 is a semicubical parabola (cuspidal curve) y2=x3y^2 = x^3 symmetric about the xx-axis with a cusp at the origin. C2C_2 is a rightward-opening parabola x=4y2+13x = \frac{4y^2+1}{3} with vertex at (1/3,0)(1/3, 0). They touch at two points where x=1/2,y=±1/(22)x = 1/2, y = \pm 1/(2\sqrt{2}).

Model Solution

Finding the tangent lines.

The curve C1C_1 has parametric equations x=t2x = t^2, y=t3y = t^3. We compute:

dydx=dy/dtdx/dt=3t22t=3t2(t0)\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{3t^2}{2t} = \frac{3t}{2} \quad (t \neq 0)

The tangent to C1C_1 at a general point with parameter tt is:

yt3=3t2(xt2)y - t^3 = \frac{3t}{2}(x - t^2)

Rearranging:

y=3t2x3t32+t3=3t2xt32y = \frac{3t}{2}x - \frac{3t^3}{2} + t^3 = \frac{3t}{2}x - \frac{t^3}{2}

So the tangent at PP (parameter t1t_1) is y=3t12xt132y = \frac{3t_1}{2}x - \frac{t_1^3}{2} and the tangent at QQ (parameter t2t_2) is y=3t22xt232y = \frac{3t_2}{2}x - \frac{t_2^3}{2}.

Using the right angle condition.

Since POQ=90\angle POQ = 90^\circ, we need OPOQ=0\vec{OP} \cdot \vec{OQ} = 0:

t12t22+t13t23=0t_1^2 \cdot t_2^2 + t_1^3 \cdot t_2^3 = 0

t12t22(1+t1t2)=0t_1^2 t_2^2(1 + t_1 t_2) = 0

Since PP and QQ are not the origin, t10t_1 \neq 0 and t20t_2 \neq 0, so t1t2=1t_1 t_2 = -1.

Finding the intersection point.

Setting the two tangent equations equal:

3t12xt132=3t22xt232\frac{3t_1}{2}x - \frac{t_1^3}{2} = \frac{3t_2}{2}x - \frac{t_2^3}{2}

32(t1t2)x=12(t13t23)=12(t1t2)(t12+t1t2+t22)\frac{3}{2}(t_1 - t_2)x = \frac{1}{2}(t_1^3 - t_2^3) = \frac{1}{2}(t_1 - t_2)(t_1^2 + t_1 t_2 + t_2^2)

Since t1t2t_1 \neq t_2 (otherwise P=QP = Q), we can divide by (t1t2)(t_1 - t_2):

x=t12+t1t2+t223x = \frac{t_1^2 + t_1 t_2 + t_2^2}{3}

Substituting t1t2=1t_1 t_2 = -1:

x=t12+t2213x = \frac{t_1^2 + t_2^2 - 1}{3}

Substituting back into the tangent at PP:

y=3t12t12+t2213t132=t1(t12+t221)t132=t1t22t12=t1(t221)2y = \frac{3t_1}{2} \cdot \frac{t_1^2 + t_2^2 - 1}{3} - \frac{t_1^3}{2} = \frac{t_1(t_1^2 + t_2^2 - 1) - t_1^3}{2} = \frac{t_1 t_2^2 - t_1}{2} = \frac{t_1(t_2^2 - 1)}{2}

Eliminating the parameters.

Using t2=1/t1t_2 = -1/t_1:

x=t12+1t1213,y=t1 ⁣(1t121)2=1t122t1x = \frac{t_1^2 + \frac{1}{t_1^2} - 1}{3}, \qquad y = \frac{t_1\!\left(\frac{1}{t_1^2} - 1\right)}{2} = \frac{1 - t_1^2}{2t_1}

Let u=t12u = t_1^2. Then x=u+u113x = \frac{u + u^{-1} - 1}{3} and y2=(1u)24u=u22u+14u=u+u124y^2 = \frac{(1 - u)^2}{4u} = \frac{u^2 - 2u + 1}{4u} = \frac{u + u^{-1} - 2}{4}.

From the expression for xx: u+u1=3x+1u + u^{-1} = 3x + 1, so:

y2=3x+124=3x14y^2 = \frac{3x + 1 - 2}{4} = \frac{3x - 1}{4}

4y2=3x14y^2 = 3x - 1

This is the equation of C2C_2, as required.

Do C1C_1 and C2C_2 meet?

Substituting x=t2x = t^2, y=t3y = t^3 into 4y2=3x14y^2 = 3x - 1:

4t6=3t21    4t63t2+1=04t^6 = 3t^2 - 1 \implies 4t^6 - 3t^2 + 1 = 0

Setting u=t20u = t^2 \geq 0: 4u33u+1=04u^3 - 3u + 1 = 0. Testing u=1u = -1: 4(1)3(1)+1=4+3+1=04(-1) - 3(-1) + 1 = -4 + 3 + 1 = 0, so (u+1)(u + 1) is a factor.

4u33u+1=(u+1)(4u24u+1)=(u+1)(2u1)24u^3 - 3u + 1 = (u + 1)(4u^2 - 4u + 1) = (u + 1)(2u - 1)^2

Since u=t20u = t^2 \geq 0, the factor (u+1)(u + 1) gives no solutions. The repeated factor (2u1)2=0(2u - 1)^2 = 0 gives u=1/2u = 1/2, i.e. t=±1/2t = \pm 1/\sqrt{2}.

The curves meet at two points: (1/2,±1/(22))(1/2, \pm 1/(2\sqrt{2})). Since the root u=1/2u = 1/2 is repeated, the curves are tangent at these points (they touch but do not cross).

Sketch. C1C_1: y2=x3y^2 = x^3 is a semicubical parabola with a cusp at the origin, symmetric about the xx-axis. C2C_2: x=(4y2+1)/3x = (4y^2 + 1)/3 is a rightward-opening parabola with vertex at (1/3,0)(1/3, 0). The two curves touch at (1/2,±1/(22))(1/2, \pm 1/(2\sqrt{2})).

Examiner Notes

This was a popular question and many very good solutions were seen. The first part of the question was a relatively straightforward application of differentiation and parametric equations and was successfully completed by many of the candidates. The sketches produced were generally the correct shape for the parabola, although in some cases it was not in the correct position. The other curve caused more problems with some candidates drawing another parabola or similar shape.


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

2 Use the factor theorem to show that a+bca + b - c is a factor of

(a+b+c)36(a+b+c)(a2+b2+c2)+8(a3+b3+c3).(a + b + c)^3 - 6(a + b + c)(a^2 + b^2 + c^2) + 8(a^3 + b^3 + c^3). (*)

Hence factorise (*) completely.

(i) Use the result above to solve the equation

(x+1)33(x+1)(2x2+5)+2(4x3+13)=0.(x + 1)^3 - 3(x + 1)(2x^2 + 5) + 2(4x^3 + 13) = 0.

(ii) By setting d+e=cd + e = c, or otherwise, show that (a+bde)(a + b - d - e) is a factor of

(a+b+d+e)36(a+b+d+e)(a2+b2+d2+e2)+8(a3+b3+d3+e3)(a + b + d + e)^3 - 6(a + b + d + e)(a^2 + b^2 + d^2 + e^2) + 8(a^3 + b^3 + d^3 + e^3)

and factorise this expression completely.

Hence solve the equation

(x+6)36(x+6)(x2+14)+8(x3+36)=0.(x + 6)^3 - 6(x + 6)(x^2 + 14) + 8(x^3 + 36) = 0.

Hint

Showing a+bca+b-c is a factor:

Substitute c=a+bc = a+b into the expression: (a+b+(a+b))36(a+b+(a+b))(a2+b2+(a+b)2)+8(a3+b3+(a+b)3)(a+b+(a+b))^3 - 6(a+b+(a+b))(a^2+b^2+(a+b)^2) + 8(a^3+b^3+(a+b)^3)

=(2a+2b)36(2a+2b)(a2+b2+a2+2ab+b2)+8(a3+b3+a3+3a2b+3ab2+b3)= (2a+2b)^3 - 6(2a+2b)(a^2+b^2+a^2+2ab+b^2) + 8(a^3+b^3+a^3+3a^2b+3ab^2+b^3)

=8(a+b)312(a+b)(2a2+2ab+2b2)+8(2a3+2b3+3a2b+3ab2)= 8(a+b)^3 - 12(a+b)(2a^2+2ab+2b^2) + 8(2a^3+2b^3+3a^2b+3ab^2)

=8(a+b)324(a+b)(a2+ab+b2)+8(2(a+b)(a2ab+b2)+3ab(a+b))= 8(a+b)^3 - 24(a+b)(a^2+ab+b^2) + 8(2(a+b)(a^2-ab+b^2)+3ab(a+b))

=8(a+b)[(a+b)23(a2+ab+b2)+2a22ab+2b2+3ab]= 8(a+b)[(a+b)^2 - 3(a^2+ab+b^2) + 2a^2-2ab+2b^2+3ab]

=8(a+b)[a2+2ab+b23a23ab3b2+2a2+ab+2b2]= 8(a+b)[a^2+2ab+b^2 - 3a^2-3ab-3b^2 + 2a^2+ab+2b^2]

=8(a+b)0=0= 8(a+b) \cdot 0 = 0

So by the factor theorem, a+bca+b-c is a factor.

Complete factorisation: By symmetry in a,b,ca, b, c, the factors b+cab+c-a and c+abc+a-b must also be factors. Since the expression has degree 3 and each factor has degree 1, we need a constant multiplier kk:

(a+b+c)36(a+b+c)(a2+b2+c2)+8(a3+b3+c3)=k(a+bc)(b+ca)(c+ab)(a+b+c)^3 - 6(a+b+c)(a^2+b^2+c^2) + 8(a^3+b^3+c^3) = k(a+b-c)(b+c-a)(c+a-b)

Setting a=1,b=0,c=0a=1, b=0, c=0: LHS =16+8=3= 1 - 6 + 8 = 3. RHS =k(1)(1)(1)=k= k(1)(-1)(1) = -k. So k=3k = -3.

The complete factorisation is 3(a+bc)(b+ca)(c+ab)-3(a+b-c)(b+c-a)(c+a-b).

(i) (x+1)33(x+1)(2x2+5)+2(4x3+13)=0(x+1)^3 - 3(x+1)(2x^2+5) + 2(4x^3+13) = 0.

Expanding: (x+1)3=x3+3x2+3x+1(x+1)^3 = x^3+3x^2+3x+1 3(x+1)(2x2+5)=6x3+6x2+15x+153(x+1)(2x^2+5) = 6x^3+6x^2+15x+15 2(4x3+13)=8x3+262(4x^3+13) = 8x^3+26

LHS =x3+3x2+3x+16x36x215x15+8x3+26=3x33x212x+12= x^3+3x^2+3x+1 - 6x^3-6x^2-15x-15 + 8x^3+26 = 3x^3-3x^2-12x+12

=3(x3x24x+4)=3(x2(x1)4(x1))=3(x1)(x24)=3(x1)(x2)(x+2)= 3(x^3-x^2-4x+4) = 3(x^2(x-1)-4(x-1)) = 3(x-1)(x^2-4) = 3(x-1)(x-2)(x+2)

Solutions: x=1,2,2x = 1, 2, -2.

(ii) Setting d+e=cd+e = c in the 4-variable version. By the same factor theorem argument (substituting e=d+a+be = d + a + b shows a+bdea+b-d-e is a factor), and by symmetry, the factors a+dbea+d-b-e and a+ebda+e-b-d are also factors.

The complete factorisation is 3(a+bde)(a+dbe)(a+ebd)-3(a+b-d-e)(a+d-b-e)(a+e-b-d).

For (x+6)36(x+6)(x2+14)+8(x3+36)=0(x+6)^3 - 6(x+6)(x^2+14) + 8(x^3+36) = 0:

(x+6)3=x3+18x2+108x+216(x+6)^3 = x^3+18x^2+108x+216 6(x+6)(x2+14)=6x3+36x2+84x+5046(x+6)(x^2+14) = 6x^3+36x^2+84x+504 8(x3+36)=8x3+2888(x^3+36) = 8x^3+288

LHS =x3+18x2+108x+2166x336x284x504+8x3+288= x^3+18x^2+108x+216 - 6x^3-36x^2-84x-504 + 8x^3+288 =3x318x2+24x=3x(x26x+8)=3x(x2)(x4)= 3x^3 - 18x^2 + 24x = 3x(x^2-6x+8) = 3x(x-2)(x-4)

Solutions: x=0,2,4x = 0, 2, 4.

Model Solution

Showing a+bca + b - c is a factor.

By the factor theorem, we substitute c=a+bc = a + b into the expression (a+b+c)36(a+b+c)(a2+b2+c2)+8(a3+b3+c3)(a + b + c)^3 - 6(a + b + c)(a^2 + b^2 + c^2) + 8(a^3 + b^3 + c^3).

With c=a+bc = a + b:

a+b+c=2(a+b),c2=(a+b)2=a2+2ab+b2a + b + c = 2(a + b), \qquad c^2 = (a + b)^2 = a^2 + 2ab + b^2

a2+b2+c2=2a2+2ab+2b2=2(a2+ab+b2)a^2 + b^2 + c^2 = 2a^2 + 2ab + 2b^2 = 2(a^2 + ab + b^2)

c3=(a+b)3=a3+3a2b+3ab2+b3c^3 = (a + b)^3 = a^3 + 3a^2b + 3ab^2 + b^3

a3+b3+c3=2a3+3a2b+3ab2+2b3=2(a3+b3)+3ab(a+b)a^3 + b^3 + c^3 = 2a^3 + 3a^2b + 3ab^2 + 2b^3 = 2(a^3 + b^3) + 3ab(a + b)

So the expression becomes:

[2(a+b)]362(a+b)2(a2+ab+b2)+8[2(a3+b3)+3ab(a+b)][2(a+b)]^3 - 6 \cdot 2(a+b) \cdot 2(a^2+ab+b^2) + 8[2(a^3+b^3) + 3ab(a+b)]

=8(a+b)324(a+b)(a2+ab+b2)+16(a3+b3)+24ab(a+b)= 8(a+b)^3 - 24(a+b)(a^2+ab+b^2) + 16(a^3+b^3) + 24ab(a+b)

Factor out (a+b)(a + b) from the first and third terms using a3+b3=(a+b)(a2ab+b2)a^3 + b^3 = (a + b)(a^2 - ab + b^2):

=8(a+b)324(a+b)(a2+ab+b2)+16(a+b)(a2ab+b2)+24ab(a+b)= 8(a+b)^3 - 24(a+b)(a^2+ab+b^2) + 16(a+b)(a^2 - ab + b^2) + 24ab(a+b)

=(a+b)[8(a+b)224(a2+ab+b2)+16(a2ab+b2)+24ab]= (a+b)\left[8(a+b)^2 - 24(a^2+ab+b^2) + 16(a^2 - ab + b^2) + 24ab\right]

Expanding the bracket:

8(a2+2ab+b2)24(a2+ab+b2)+16(a2ab+b2)+24ab8(a^2 + 2ab + b^2) - 24(a^2 + ab + b^2) + 16(a^2 - ab + b^2) + 24ab

=(824+16)a2+(162416+24)ab+(824+16)b2= (8 - 24 + 16)a^2 + (16 - 24 - 16 + 24)ab + (8 - 24 + 16)b^2

=0a2+0ab+0b2=0= 0 \cdot a^2 + 0 \cdot ab + 0 \cdot b^2 = 0

Since substituting c=a+bc = a + b gives zero, (a+bc)(a + b - c) is a factor by the factor theorem.

Complete factorisation.

The expression is symmetric in a,b,ca, b, c. By the same argument, (b+ca)(b + c - a) and (c+ab)(c + a - b) are also factors. Since the expression has degree 3 and each factor has degree 1, we have:

(a+b+c)36(a+b+c)(a2+b2+c2)+8(a3+b3+c3)=k(a+bc)(b+ca)(c+ab)(a+b+c)^3 - 6(a+b+c)(a^2+b^2+c^2) + 8(a^3+b^3+c^3) = k(a+b-c)(b+c-a)(c+a-b)

for some constant kk. Setting a=1,b=0,c=0a = 1, b = 0, c = 0:

LHS=16+8=3,RHS=k(1)(1)(1)=k\text{LHS} = 1 - 6 + 8 = 3, \qquad \text{RHS} = k(1)(-1)(1) = -k

So k=3k = -3, giving the complete factorisation:

3(a+bc)(b+ca)(c+ab)-3(a+b-c)(b+c-a)(c+a-b)

Part (i). We need to solve (x+1)33(x+1)(2x2+5)+2(4x3+13)=0(x+1)^3 - 3(x+1)(2x^2+5) + 2(4x^3+13) = 0.

Expanding each term:

(x+1)3=x3+3x2+3x+1(x+1)^3 = x^3 + 3x^2 + 3x + 1

3(x+1)(2x2+5)=3(2x3+5x+2x2+5)=6x3+6x2+15x+153(x+1)(2x^2+5) = 3(2x^3 + 5x + 2x^2 + 5) = 6x^3 + 6x^2 + 15x + 15

2(4x3+13)=8x3+262(4x^3+13) = 8x^3 + 26

Combining:

x3+3x2+3x+16x36x215x15+8x3+26=3x33x212x+12x^3 + 3x^2 + 3x + 1 - 6x^3 - 6x^2 - 15x - 15 + 8x^3 + 26 = 3x^3 - 3x^2 - 12x + 12

=3(x3x24x+4)=3[x2(x1)4(x1)]=3(x1)(x24)=3(x1)(x2)(x+2)= 3(x^3 - x^2 - 4x + 4) = 3[x^2(x - 1) - 4(x - 1)] = 3(x - 1)(x^2 - 4) = 3(x - 1)(x - 2)(x + 2)

Solutions: x=1,2,2x = 1, 2, -2.

Part (ii). We show (a+bde)(a + b - d - e) is a factor of the four-variable expression. Setting e=cde = c - d (i.e. d+e=cd + e = c) reduces the four-variable expression to the three-variable expression. When a+b=d+e=ca + b = d + e = c, we have c=a+bc = a + b and e=a+bde = a + b - d, so the expression equals zero. By the factor theorem, (a+bde)(a + b - d - e) is a factor.

By symmetry in a,b,d,ea, b, d, e, the factors (a+dbe)(a + d - b - e) and (a+ebd)(a + e - b - d) are also factors. The complete factorisation is:

3(a+bde)(a+dbe)(a+ebd)-3(a + b - d - e)(a + d - b - e)(a + e - b - d)

Solving the equation (x+6)36(x+6)(x2+14)+8(x3+36)=0(x+6)^3 - 6(x+6)(x^2+14) + 8(x^3+36) = 0.

Expanding:

(x+6)3=x3+18x2+108x+216(x+6)^3 = x^3 + 18x^2 + 108x + 216

6(x+6)(x2+14)=6(x3+14x+6x2+84)=6x3+36x2+84x+5046(x+6)(x^2+14) = 6(x^3 + 14x + 6x^2 + 84) = 6x^3 + 36x^2 + 84x + 504

8(x3+36)=8x3+2888(x^3+36) = 8x^3 + 288

Combining:

x3+18x2+108x+2166x336x284x504+8x3+288=3x318x2+24xx^3 + 18x^2 + 108x + 216 - 6x^3 - 36x^2 - 84x - 504 + 8x^3 + 288 = 3x^3 - 18x^2 + 24x

=3x(x26x+8)=3x(x2)(x4)= 3x(x^2 - 6x + 8) = 3x(x - 2)(x - 4)

Solutions: x=0,2,4x = 0, 2, 4.

Examiner Notes

This question received poor responses in terms of the average mark per attempt. Application of the factor theorem to the first part often produced a neat solution. However, a number of candidates in the first part did not use the factor theorem as requested and so produced very complicated algebraic expressions that were more of a challenge to simplify. Where the result had been successfully shown and the expression factorised, many candidates were able to see the relevance to solving the equation in part (i). Those candidates who were able to follow through the method to successfully factorise the second expression were often able to complete the question.


Topic: 多项式与级数 (Polynomials and Series)  |  Difficulty: Challenging  |  Marks: 20

3 For each non-negative integer nn, the polynomial fnf_n is defined by

fn(x)=1+x+x22!+x33!++xnn!.f_n(x) = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots + \frac{x^n}{n!} .

(i) Show that fn(x)=fn1(x)f'_n(x) = f_{n-1}(x) (for n1n \geqslant 1).

(ii) Show that, if aa is a real root of the equation

fn(x)=0,(*)f_n(x) = 0 , \qquad \text{(*)}

then a<0a < 0.

(iii) Let aa and bb be distinct real roots of (*), for n2n \geqslant 2. Show that fn(a)fn(b)>0f'_n(a) f'_n(b) > 0 and use a sketch to deduce that fn(c)=0f_n(c) = 0 for some number cc between aa and bb.

Deduce that (*) has at most one real root. How many real roots does (*) have if nn is odd? How many real roots does (*) have if nn is even?

Hint

(i) fn(x)=k=0nxkk!f_n(x) = \sum_{k=0}^{n} \frac{x^k}{k!}, so

fn(x)=k=1nkxk1k!=k=1nxk1(k1)!=j=0n1xjj!=fn1(x)f_n'(x) = \sum_{k=1}^{n} \frac{kx^{k-1}}{k!} = \sum_{k=1}^{n} \frac{x^{k-1}}{(k-1)!} = \sum_{j=0}^{n-1} \frac{x^j}{j!} = f_{n-1}(x)

(ii) If a>0a > 0, then every term akk!>0\frac{a^k}{k!} > 0 for k0k \geq 0, so fn(a)>0f_n(a) > 0. If a=0a = 0, then fn(0)=10f_n(0) = 1 \neq 0. Therefore any real root must satisfy a<0a < 0.

(iii) Suppose aa and bb are distinct real roots with a<ba < b. Then fn(a)=fn(b)=0f_n(a) = f_n(b) = 0.

From part (i), fn(x)=fn1(x)f_n'(x) = f_{n-1}(x) and fn(x)=fn1(x)+xnn!f_n(x) = f_{n-1}(x) + \frac{x^n}{n!}, so fn(x)=fn(x)xnn!f_n'(x) = f_n(x) - \frac{x^n}{n!}.

At a root: fn(a)=fn(a)ann!=ann!f_n'(a) = f_n(a) - \frac{a^n}{n!} = -\frac{a^n}{n!} and fn(b)=bnn!f_n'(b) = -\frac{b^n}{n!}.

Since a,b<0a, b < 0 (from part (ii)), ana^n and bnb^n have the same sign (both positive if nn is even, both negative if nn is odd).

So fn(a)fn(b)=anbn(n!)2=(ab)n(n!)2>0f_n'(a) \cdot f_n'(b) = \frac{a^n b^n}{(n!)^2} = \frac{(ab)^n}{(n!)^2} > 0 (since ab>0ab > 0).

This means fn(a)f_n'(a) and fn(b)f_n'(b) have the same sign, so the tangent lines at aa and bb slope in the same direction. Since fnf_n is a polynomial (hence continuous and differentiable), and fn(a)=fn(b)=0f_n(a) = f_n(b) = 0 with same-sign derivatives, by the graph fnf_n must cross zero again between aa and bb — say at some cc with a<c<ba < c < b.

But then cc is also a root, and we can repeat the argument between aa and cc, and between cc and bb, finding infinitely many roots. Since fnf_n is a polynomial of degree nn (finite), this is a contradiction. Therefore fn(x)=0f_n(x) = 0 has at most one real root.

Number of roots:

  • If nn is odd: fn(x)+f_n(x) \to +\infty as x+x \to +\infty and fn(x)f_n(x) \to -\infty as xx \to -\infty (leading term xn/n!x^n/n! dominates). By the Intermediate Value Theorem, there is at least one real root. Combined with “at most one”, there is exactly one real root.
  • If nn is even: fn(x)+f_n(x) \to +\infty as x±x \to \pm\infty. Since fn(0)=1>0f_n(0) = 1 > 0 and fnf_n has at most one real root, and any root must be negative: if there were a root a<0a < 0, then fn(a)=an/n!<0f_n'(a) = -a^n/n! < 0 (since an>0a^n > 0 for even nn), so fnf_n is decreasing at aa. But fn+f_n \to +\infty as xx \to -\infty, so fnf_n must increase then decrease, meaning fnf_n' has a zero, contradicting the fact that fn1f_{n-1} (odd degree) has exactly one real root which is negative and fn1(0)=1>0f_{n-1}(0) = 1 > 0… Actually, for even nn, fnf_n has no real roots. For n=2n=2: f2(x)=1+x+x2/2f_2(x) = 1+x+x^2/2, discriminant =12=1<0= 1-2 = -1 < 0, confirming no real roots.
Model Solution

Part (i). We have fn(x)=k=0nxkk!f_n(x) = \sum_{k=0}^{n} \frac{x^k}{k!}. Differentiating term by term:

fn(x)=k=1nkxk1k!=k=1nxk1(k1)!f_n'(x) = \sum_{k=1}^{n} \frac{kx^{k-1}}{k!} = \sum_{k=1}^{n} \frac{x^{k-1}}{(k-1)!}

Setting j=k1j = k - 1:

fn(x)=j=0n1xjj!=fn1(x)f_n'(x) = \sum_{j=0}^{n-1} \frac{x^j}{j!} = f_{n-1}(x)

Part (ii). Suppose aa is a real root of fn(x)=0f_n(x) = 0.

If a>0a > 0: every term akk!>0\frac{a^k}{k!} > 0 for k0k \geq 0, and the first term is 1>01 > 0, so fn(a)>0f_n(a) > 0. Contradiction.

If a=0a = 0: fn(0)=10f_n(0) = 1 \neq 0. Contradiction.

Therefore a<0a < 0.

Part (iii). Suppose aa and bb are distinct real roots of fn(x)=0f_n(x) = 0 with n2n \geq 2. From part (ii), a<0a < 0 and b<0b < 0.

Since fn(x)=fn1(x)+xnn!f_n(x) = f_{n-1}(x) + \frac{x^n}{n!}, we have fn(x)=fn1(x)=fn(x)xnn!f_n'(x) = f_{n-1}(x) = f_n(x) - \frac{x^n}{n!}.

At a root, fn(a)=0f_n(a) = 0, so:

fn(a)=ann!f_n'(a) = -\frac{a^n}{n!}

Similarly fn(b)=bnn!f_n'(b) = -\frac{b^n}{n!}.

Therefore:

fn(a)fn(b)=anbn(n!)2=(ab)n(n!)2f_n'(a) \cdot f_n'(b) = \frac{a^n \cdot b^n}{(n!)^2} = \frac{(ab)^n}{(n!)^2}

Since a<0a < 0 and b<0b < 0, we have ab>0ab > 0, so (ab)n>0(ab)^n > 0. Hence fn(a)fn(b)>0f_n'(a) \cdot f_n'(b) > 0.

Deducing at most one real root.

Since fn(a)f_n'(a) and fn(b)f_n'(b) have the same sign, the tangent lines at aa and bb slope in the same direction. Since fn(a)=fn(b)=0f_n(a) = f_n(b) = 0 and fnf_n is continuous:

  • If fn(a)>0f_n'(a) > 0 and fn(b)>0f_n'(b) > 0: the function is increasing at both roots. Since fn(a)=0f_n(a) = 0 and fnf_n is increasing at aa, fnf_n must be negative just to the left of aa and positive just to the right. Since fnf_n is increasing at bb too, fnf_n must be negative just to the left of bb and positive just to the right. But between aa and bb, fnf_n must go from positive (right of aa) to negative (left of bb), so by the Intermediate Value Theorem, fn(c)=0f_n(c) = 0 for some cc between aa and bb.

  • If fn(a)<0f_n'(a) < 0 and fn(b)<0f_n'(b) < 0: a symmetric argument (decreasing at both roots) also gives a root cc between aa and bb.

In either case, cc is another distinct real root. We can now repeat the argument between aa and cc, finding yet another root, and so on. This would give infinitely many roots, contradicting the fact that fnf_n is a polynomial of degree nn (which has at most nn roots). Therefore fn(x)=0f_n(x) = 0 has at most one real root.

Number of roots when nn is odd.

The leading term of fnf_n is xnn!\frac{x^n}{n!}. When nn is odd:

  • fn(x)+f_n(x) \to +\infty as x+x \to +\infty
  • fn(x)f_n(x) \to -\infty as xx \to -\infty

Since fnf_n is continuous, by the Intermediate Value Theorem, fnf_n has at least one real root. Combined with “at most one”, fn(x)=0f_n(x) = 0 has exactly one real root when nn is odd.

Number of roots when nn is even.

When nn is even, fn(x)+f_n(x) \to +\infty as x±x \to \pm \infty. We know fn(0)=1>0f_n(0) = 1 > 0 and any real root must be negative. Suppose a<0a < 0 is a root. Then:

fn(a)=ann!f_n'(a) = -\frac{a^n}{n!}

Since nn is even and a<0a < 0, an>0a^n > 0, so fn(a)<0f_n'(a) < 0: the function is decreasing at aa.

Since fn(a)=0f_n(a) = 0, fnf_n is positive just to the left of aa and negative just to the right. But fn(x)+f_n(x) \to +\infty as xx \to -\infty, so fnf_n must have decreased from ++\infty to 00 at aa, meaning fnf_n was positive for all sufficiently negative xx. As xx increases past aa, fnf_n becomes negative. But fn(0)=1>0f_n(0) = 1 > 0, so fnf_n must cross zero again at some point between aa and 00. This gives a second real root, contradicting “at most one”.

Therefore fn(x)=0f_n(x) = 0 has no real roots when nn is even.

Examiner Notes

This was the most popular question on the paper, and candidates generally scored well here. The first two parts were relatively straightforward and were answered well. The final part required careful explanation from candidates and many were not able to take the initial step of rewriting the relationship between the function and its derivative in a useful way. Those who did successfully complete this part were often able to identify the number of roots in each of the two cases.


Topic: 不等式与函数 (Inequalities and Functions)  |  Difficulty: Challenging  |  Marks: 20

4 Let

y=x2+xsinθ+1x2+xcosθ+1.y = \frac{x^2 + x \sin \theta + 1}{x^2 + x \cos \theta + 1} .

(i) Given that xx is real, show that

(ycosθsinθ)24(y1)2.(y \cos \theta - \sin \theta)^2 \geqslant 4(y - 1)^2 .

Deduce that

y2+14(y1)2,y^2 + 1 \geqslant 4(y - 1)^2 ,

and hence that

473y4+73.\frac{4 - \sqrt{7}}{3} \leqslant y \leqslant \frac{4 + \sqrt{7}}{3} .

(ii) In the case y=4+73y = \frac{4 + \sqrt{7}}{3}, show that

y2+1=2(y1)\sqrt{y^2 + 1} = 2(y - 1)

and find the corresponding values of xx and tanθ\tan \theta.

Hint

(i) From y=x2+xsinθ+1x2+xcosθ+1y = \frac{x^2 + x\sin\theta + 1}{x^2 + x\cos\theta + 1}, rearrange:

y(x2+xcosθ+1)=x2+xsinθ+1y(x^2 + x\cos\theta + 1) = x^2 + x\sin\theta + 1

(y1)x2+(ycosθsinθ)x+(y1)=0(y-1)x^2 + (y\cos\theta - \sin\theta)x + (y-1) = 0

For real xx, the discriminant must be 0\geq 0:

(ycosθsinθ)24(y1)20(y\cos\theta - \sin\theta)^2 - 4(y-1)^2 \geq 0

So (ycosθsinθ)24(y1)2(y\cos\theta - \sin\theta)^2 \geq 4(y-1)^2.

Deduction of y2+1(ycosθsinθ)2y^2 + 1 \geq (y\cos\theta - \sin\theta)^2:

Write ycosθsinθ=Rcos(θ+α)y\cos\theta - \sin\theta = R\cos(\theta + \alpha) where R=y2+1R = \sqrt{y^2+1} and tanα=1y\tan\alpha = \frac{1}{y}. Then (ycosθsinθ)2=(y2+1)cos2(θ+α)y2+1(y\cos\theta - \sin\theta)^2 = (y^2+1)\cos^2(\theta+\alpha) \leq y^2+1.

Deduction of the range: Combining: 4(y1)2(ycosθsinθ)2y2+14(y-1)^2 \leq (y\cos\theta-\sin\theta)^2 \leq y^2+1.

So 4(y1)2y2+14(y-1)^2 \leq y^2+1, i.e. 4y28y+4y2+14y^2 - 8y + 4 \leq y^2+1, i.e. 3y28y+303y^2 - 8y + 3 \leq 0.

The roots of 3y28y+3=03y^2 - 8y + 3 = 0 are y=8±64366=8±286=4±73y = \frac{8 \pm \sqrt{64-36}}{6} = \frac{8 \pm \sqrt{28}}{6} = \frac{4 \pm \sqrt{7}}{3}.

Therefore 473y4+73\frac{4-\sqrt{7}}{3} \leq y \leq \frac{4+\sqrt{7}}{3}.

(ii) When y=4+73y = \frac{4+\sqrt{7}}{3}:

y1=1+73y - 1 = \frac{1+\sqrt{7}}{3}, so 4(y1)2=4(1+7)29=4(8+27)9=8(4+7)94(y-1)^2 = \frac{4(1+\sqrt{7})^2}{9} = \frac{4(8+2\sqrt{7})}{9} = \frac{8(4+\sqrt{7})}{9}.

y2+1=(4+7)29+1=23+87+99=32+879=8(4+7)9y^2 + 1 = \frac{(4+\sqrt{7})^2}{9} + 1 = \frac{23+8\sqrt{7}+9}{9} = \frac{32+8\sqrt{7}}{9} = \frac{8(4+\sqrt{7})}{9}.

So y2+1=4(y1)2y^2+1 = 4(y-1)^2, hence y2+1=2(y1)\sqrt{y^2+1} = 2(y-1) (positive since y>1y > 1).

Finding tanθ\tan\theta: For the maximum to be achieved, both inequalities become equalities. From (y2+1)cos2(θ+α)=y2+1(y^2+1)\cos^2(\theta+\alpha) = y^2+1, we get cos2(θ+α)=1\cos^2(\theta+\alpha) = 1, so θ+α=kπ\theta + \alpha = k\pi.

With tanα=1y=34+7=3(47)167=473\tan\alpha = \frac{1}{y} = \frac{3}{4+\sqrt{7}} = \frac{3(4-\sqrt{7})}{16-7} = \frac{4-\sqrt{7}}{3}.

Taking θ+α=0\theta + \alpha = 0: tanθ=tanα=473=743\tan\theta = -\tan\alpha = -\frac{4-\sqrt{7}}{3} = \frac{\sqrt{7}-4}{3}.

Finding xx: From (y1)x2+(ycosθsinθ)x+(y1)=0(y-1)x^2 + (y\cos\theta - \sin\theta)x + (y-1) = 0 with discriminant =0= 0: x=ycosθsinθ2(y1)x = -\frac{y\cos\theta - \sin\theta}{2(y-1)}

Since ycosθsinθ=y2+1cos(θ+α)=y2+1=2(y1)y\cos\theta - \sin\theta = \sqrt{y^2+1}\cos(\theta+\alpha) = \sqrt{y^2+1} = 2(y-1):

x=2(y1)2(y1)=1x = -\frac{2(y-1)}{2(y-1)} = -1.

So x=1x = -1 and tanθ=743\tan\theta = \frac{\sqrt{7}-4}{3}.

Model Solution

Part (i): Showing the discriminant inequality.

From y=x2+xsinθ+1x2+xcosθ+1y = \dfrac{x^2 + x\sin\theta + 1}{x^2 + x\cos\theta + 1}, rearrange:

y(x2+xcosθ+1)=x2+xsinθ+1y(x^2 + x\cos\theta + 1) = x^2 + x\sin\theta + 1

(y1)x2+(ycosθsinθ)x+(y1)=0()(y - 1)x^2 + (y\cos\theta - \sin\theta)x + (y - 1) = 0 \qquad (\dagger)

For this quadratic in xx to have real solutions, the discriminant must be non-negative:

(ycosθsinθ)24(y1)20(y\cos\theta - \sin\theta)^2 - 4(y - 1)^2 \geq 0

(ycosθsinθ)24(y1)2(y\cos\theta - \sin\theta)^2 \geq 4(y - 1)^2 \qquad \checkmark

Deducing y2+14(y1)2y^2 + 1 \geq 4(y-1)^2.

Write ycosθsinθy\cos\theta - \sin\theta in the form Rcos(θ+α)R\cos(\theta + \alpha) where R=y2+1R = \sqrt{y^2 + 1} and tanα=1/y\tan\alpha = 1/y. This is valid since:

Rcos(θ+α)=R(cosθcosαsinθsinα)R\cos(\theta + \alpha) = R(\cos\theta\cos\alpha - \sin\theta\sin\alpha)

Setting Rcosα=yR\cos\alpha = y and Rsinα=1R\sin\alpha = 1 gives R=y2+1R = \sqrt{y^2 + 1}.

Since cos2(θ+α)1\cos^2(\theta + \alpha) \leq 1:

(ycosθsinθ)2=(y2+1)cos2(θ+α)y2+1(y\cos\theta - \sin\theta)^2 = (y^2 + 1)\cos^2(\theta + \alpha) \leq y^2 + 1

Combining with the discriminant inequality:

4(y1)2(ycosθsinθ)2y2+14(y - 1)^2 \leq (y\cos\theta - \sin\theta)^2 \leq y^2 + 1

4(y1)2y2+14(y - 1)^2 \leq y^2 + 1

Deducing the range of yy.

Expanding: 4y28y+4y2+14y^2 - 8y + 4 \leq y^2 + 1, so 3y28y+303y^2 - 8y + 3 \leq 0.

The roots of 3y28y+3=03y^2 - 8y + 3 = 0 are:

y=8±64366=8±286=8±276=4±73y = \frac{8 \pm \sqrt{64 - 36}}{6} = \frac{8 \pm \sqrt{28}}{6} = \frac{8 \pm 2\sqrt{7}}{6} = \frac{4 \pm \sqrt{7}}{3}

Since the coefficient of y2y^2 is positive, the quadratic is non-positive between its roots:

473y4+73\frac{4 - \sqrt{7}}{3} \leq y \leq \frac{4 + \sqrt{7}}{3}

Part (ii): The case y=4+73y = \frac{4 + \sqrt{7}}{3}.

Showing y2+1=2(y1)\sqrt{y^2 + 1} = 2(y - 1).

Compute y1=4+731=1+73y - 1 = \frac{4 + \sqrt{7}}{3} - 1 = \frac{1 + \sqrt{7}}{3}.

4(y1)2=4(1+7)29=4(1+27+7)9=4(8+27)9=8(4+7)94(y - 1)^2 = 4 \cdot \frac{(1 + \sqrt{7})^2}{9} = \frac{4(1 + 2\sqrt{7} + 7)}{9} = \frac{4(8 + 2\sqrt{7})}{9} = \frac{8(4 + \sqrt{7})}{9}

y2+1=(4+7)29+1=16+87+79+1=23+87+99=32+879=8(4+7)9y^2 + 1 = \frac{(4 + \sqrt{7})^2}{9} + 1 = \frac{16 + 8\sqrt{7} + 7}{9} + 1 = \frac{23 + 8\sqrt{7} + 9}{9} = \frac{32 + 8\sqrt{7}}{9} = \frac{8(4 + \sqrt{7})}{9}

So y2+1=4(y1)2y^2 + 1 = 4(y - 1)^2. Taking square roots (both sides positive since y>1y > 1):

y2+1=2(y1)\sqrt{y^2 + 1} = 2(y - 1)

Finding tanθ\tan\theta.

For the maximum to be achieved, both inequalities in the chain must be equalities.

From (y2+1)cos2(θ+α)=y2+1(y^2 + 1)\cos^2(\theta + \alpha) = y^2 + 1, we need cos2(θ+α)=1\cos^2(\theta + \alpha) = 1, so θ+α=kπ\theta + \alpha = k\pi for integer kk.

With tanα=1y=34+7=3(47)167=3(47)9=473\tan\alpha = \frac{1}{y} = \frac{3}{4 + \sqrt{7}} = \frac{3(4 - \sqrt{7})}{16 - 7} = \frac{3(4 - \sqrt{7})}{9} = \frac{4 - \sqrt{7}}{3}.

Taking θ+α=0\theta + \alpha = 0 (so θ=α\theta = -\alpha):

tanθ=tanα=473=743\tan\theta = -\tan\alpha = -\frac{4 - \sqrt{7}}{3} = \frac{\sqrt{7} - 4}{3}

Finding xx.

From ()(\dagger), the discriminant is zero, so there is exactly one value of xx:

x=ycosθsinθ2(y1)x = -\frac{y\cos\theta - \sin\theta}{2(y - 1)}

Since ycosθsinθ=y2+1cos(θ+α)=y2+1(±1)y\cos\theta - \sin\theta = \sqrt{y^2 + 1}\cos(\theta + \alpha) = \sqrt{y^2 + 1} \cdot (\pm 1). With θ+α=0\theta + \alpha = 0, cos(θ+α)=1\cos(\theta + \alpha) = 1, so:

ycosθsinθ=y2+1=2(y1)y\cos\theta - \sin\theta = \sqrt{y^2 + 1} = 2(y - 1)

x=2(y1)2(y1)=1x = -\frac{2(y - 1)}{2(y - 1)} = -1

Therefore x=1x = -1 and tanθ=743\tan\theta = \dfrac{\sqrt{7} - 4}{3}.

Examiner Notes

This question attracted many good responses which often successfully accomplished the first and third results of part (i) of the question, although in many cases marks were lost through incomplete explanations of some of the steps taken. Part (ii) of the question was generally answered poorly with some candidates simply stating that the square root of one expression in terms of surds was equal to the other one that they had achieved. Only a small number of candidates successfully completed the last section of this question.


Topic: 组合数学 (Combinatorics)  |  Difficulty: Challenging  |  Marks: 20

5 In this question, the definition of (pq)\begin{pmatrix} p \\ q \end{pmatrix} is taken to be

(pq)={p!q!(pq)!if pq0,0otherwise .\begin{pmatrix} p \\ q \end{pmatrix} = \begin{cases} \frac{p!}{q!(p - q)!} & \text{if } p \geqslant q \geqslant 0 \, , \\ 0 & \text{otherwise .} \end{cases}

(i) Write down the coefficient of xnx^n in the binomial expansion for (1x)N(1 - x)^{-N}, where NN is a positive integer, and write down the expansion using the Σ\Sigma summation notation.

By considering (1x)1(1x)N(1 - x)^{-1}(1 - x)^{-N}, where NN is a positive integer, show that

j=0n(N+j1j)=(N+nn).\sum_{j=0}^{n} \begin{pmatrix} N + j - 1 \\ j \end{pmatrix} = \begin{pmatrix} N + n \\ n \end{pmatrix} .

(ii) Show that, for any positive integers m,nm, n and rr with rm+nr \leqslant m + n,

(m+nr)=j=0r(mj)(nrj).\begin{pmatrix} m + n \\ r \end{pmatrix} = \sum_{j=0}^{r} \begin{pmatrix} m \\ j \end{pmatrix} \begin{pmatrix} n \\ r - j \end{pmatrix} .

(iii) Show that, for any positive integers mm and NN,

j=0n(1)j(N+mnj)(m+j1j)=(Nn).\sum_{j=0}^{n} (-1)^j \begin{pmatrix} N + m \\ n - j \end{pmatrix} \begin{pmatrix} m + j - 1 \\ j \end{pmatrix} = \begin{pmatrix} N \\ n \end{pmatrix} .

Hint

(i) The binomial expansion of (1x)N(1-x)^{-N} where NN is a positive integer:

(1x)N=n=0(N+n1n)xn(1-x)^{-N} = \sum_{n=0}^{\infty} \binom{N+n-1}{n} x^n

The coefficient of xnx^n is (N+n1n)=(N+n1)!n!(N1)!\binom{N+n-1}{n} = \frac{(N+n-1)!}{n!(N-1)!}.

Proving the identity: (1x)1(1x)N=(1x)(N+1)(1-x)^{-1}(1-x)^{-N} = (1-x)^{-(N+1)}.

(1x)1=k=0xk(1-x)^{-1} = \sum_{k=0}^{\infty} x^k, so the coefficient of xnx^n in (1x)1(1x)N(1-x)^{-1}(1-x)^{-N} is: j=0n1(N+j1j)=j=0n(N+j1j)\sum_{j=0}^{n} 1 \cdot \binom{N+j-1}{j} = \sum_{j=0}^{n} \binom{N+j-1}{j}

But (1x)(N+1)=n=0(N+nn)xn(1-x)^{-(N+1)} = \sum_{n=0}^{\infty} \binom{N+n}{n} x^n, so the coefficient of xnx^n is (N+nn)\binom{N+n}{n}.

Equating: j=0n(N+j1j)=(N+nn)\sum_{j=0}^{n} \binom{N+j-1}{j} = \binom{N+n}{n}.

(ii) Consider (1+x)m(1+x)n=(1+x)m+n(1+x)^m(1+x)^n = (1+x)^{m+n}.

The coefficient of xrx^r on the left is j=0r(mj)(nrj)\sum_{j=0}^{r} \binom{m}{j}\binom{n}{r-j} (by the Cauchy product / Vandermonde convolution).

The coefficient of xrx^r on the right is (m+nr)\binom{m+n}{r}.

Equating: (m+nr)=j=0r(mj)(nrj)\binom{m+n}{r} = \sum_{j=0}^{r} \binom{m}{j}\binom{n}{r-j}.

(iii) Consider (1+x)N+m(1+x)m=(1+x)N(1+x)^{N+m} \cdot (1+x)^{-m} = (1+x)^{N}.

(1+x)m=(1(x))m=j=0(m+j1j)(x)j=j=0(1)j(m+j1j)xj(1+x)^{-m} = (1-(-x))^{-m} = \sum_{j=0}^{\infty} \binom{m+j-1}{j}(-x)^j = \sum_{j=0}^{\infty} (-1)^j \binom{m+j-1}{j} x^j

(1+x)N+m=k=0N+m(N+mk)xk(1+x)^{N+m} = \sum_{k=0}^{N+m} \binom{N+m}{k} x^k

The coefficient of xnx^n in the product: j=0n(1)j(m+j1j)(N+mnj)\sum_{j=0}^{n} (-1)^j \binom{m+j-1}{j} \binom{N+m}{n-j}

And the coefficient of xnx^n in (1+x)N(1+x)^N is (Nn)\binom{N}{n}.

Equating: j=0n(1)j(N+mnj)(m+j1j)=(Nn)\sum_{j=0}^{n} (-1)^j \binom{N+m}{n-j} \binom{m+j-1}{j} = \binom{N}{n}.

Model Solution

Part (i): Binomial expansion of (1x)N(1 - x)^{-N}.

For a positive integer NN, the negative binomial expansion gives:

(1x)N=n=0(N+n1n)xn(1 - x)^{-N} = \sum_{n=0}^{\infty} \binom{N + n - 1}{n} x^n

The coefficient of xnx^n is (N+n1n)\dbinom{N + n - 1}{n}.

Proving the identity. Consider (1x)1(1x)N=(1x)(N+1)(1 - x)^{-1}(1 - x)^{-N} = (1 - x)^{-(N+1)}.

(1x)1=k=0xk(1 - x)^{-1} = \sum_{k=0}^{\infty} x^k, so by the Cauchy product, the coefficient of xnx^n in (1x)1(1x)N(1 - x)^{-1}(1 - x)^{-N} is:

j=0n1(N+j1j)=j=0n(N+j1j)\sum_{j=0}^{n} 1 \cdot \binom{N + j - 1}{j} = \sum_{j=0}^{n} \binom{N + j - 1}{j}

The coefficient of xnx^n in (1x)(N+1)(1 - x)^{-(N+1)} is ((N+1)+n1n)=(N+nn)\dbinom{(N+1) + n - 1}{n} = \dbinom{N + n}{n}.

Equating:

j=0n(N+j1j)=(N+nn)\sum_{j=0}^{n} \binom{N + j - 1}{j} = \binom{N + n}{n}

Part (ii): Vandermonde’s identity.

Consider (1+x)m(1+x)n=(1+x)m+n(1 + x)^m (1 + x)^n = (1 + x)^{m+n}.

The coefficient of xrx^r on the left-hand side, by the Cauchy product:

j=0r(mj)(nrj)\sum_{j=0}^{r} \binom{m}{j} \binom{n}{r - j}

The coefficient of xrx^r on the right-hand side is (m+nr)\dbinom{m + n}{r}.

Equating:

(m+nr)=j=0r(mj)(nrj)\binom{m + n}{r} = \sum_{j=0}^{r} \binom{m}{j} \binom{n}{r - j}

Part (iii): The alternating sum identity.

Consider (1+x)N+m(1+x)m=(1+x)N(1 + x)^{N+m} \cdot (1 + x)^{-m} = (1 + x)^N.

The second factor can be expanded as:

(1+x)m=(1(x))m=j=0(m+j1j)(x)j=j=0(1)j(m+j1j)xj(1 + x)^{-m} = (1 - (-x))^{-m} = \sum_{j=0}^{\infty} \binom{m + j - 1}{j} (-x)^j = \sum_{j=0}^{\infty} (-1)^j \binom{m + j - 1}{j} x^j

The first factor is:

(1+x)N+m=k=0N+m(N+mk)xk(1 + x)^{N+m} = \sum_{k=0}^{N+m} \binom{N + m}{k} x^k

By the Cauchy product, the coefficient of xnx^n in the product is:

j=0n(1)j(m+j1j)(N+mnj)\sum_{j=0}^{n} (-1)^j \binom{m + j - 1}{j} \cdot \binom{N + m}{n - j}

The coefficient of xnx^n in (1+x)N(1 + x)^N is (Nn)\dbinom{N}{n}.

Equating:

j=0n(1)j(N+mnj)(m+j1j)=(Nn)\sum_{j=0}^{n} (-1)^j \binom{N + m}{n - j} \binom{m + j - 1}{j} = \binom{N}{n}

Examiner Notes

This was the least attempted of all of the Pure questions and one that generally produced low marks for candidates, who generally appeared to have difficulty in expressing the coefficients of the binomial expansion in the required form. In each case the desired answer was given in the question, and so successful solutions also needed to be very clear about the reasoning used to reach the answer.


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

6 This question concerns solutions of the differential equation

(1x2)(dydx)2+k2y2=k2(*)(1 - x^2) \left( \frac{dy}{dx} \right)^2 + k^2y^2 = k^2 \qquad \text{(*)}

where kk is a positive integer.

For each value of kk, let yk(x)y_k(x) be the solution of ()(*) that satisfies yk(1)=1y_k(1) = 1; you may assume that there is only one such solution for each value of kk.

(i) Write down the differential equation satisfied by y1(x)y_1(x) and verify that y1(x)=xy_1(x) = x.

(ii) Write down the differential equation satisfied by y2(x)y_2(x) and verify that y2(x)=2x21y_2(x) = 2x^2 - 1.

(iii) Let z(x)=2(yn(x))21z(x) = 2(y_n(x))^2 - 1. Show that

(1x2)(dzdx)2+4n2z2=4n2(1 - x^2) \left( \frac{dz}{dx} \right)^2 + 4n^2z^2 = 4n^2

and hence obtain an expression for y2n(x)y_{2n}(x) in terms of yn(x)y_n(x).

(iv) Let v(x)=yn(ym(x))v(x) = y_n(y_m(x)). Show that v(x)=ymn(x)v(x) = y_{mn}(x).

Hint

Parts (i) and (ii) only require verification in each of the cases, so simply differentiate the functions given and substitute into the differential equation to confirm that they are solutions. Remember to check as well that the boundary conditions are satisfied.

For part (iii), differentiate the given formula for zz and substitute into the differential equation. By observing that the new differential equation is of the same form as (*), but for 2n2n instead of nn, the expression for y2n(x)y_{2n}(x) can be established.

For part (iv), again differentiate the given formula, being careful about the application of the chain rule and substitute. Again, by comparing with (*) the final result should be clear.

Model Solution

Part (i): k=1k = 1.

The differential equation with k=1k = 1 is:

(1x2)(dydx)2+y2=1(1 - x^2)\left(\frac{dy}{dx}\right)^2 + y^2 = 1

We verify y1(x)=xy_1(x) = x: dy1dx=1\frac{dy_1}{dx} = 1, and y1(1)=1y_1(1) = 1. \checkmark

Substituting: (1x2)(1)2+x2=1x2+x2=1(1 - x^2)(1)^2 + x^2 = 1 - x^2 + x^2 = 1. \checkmark

Part (ii): k=2k = 2.

The differential equation with k=2k = 2 is:

(1x2)(dydx)2+4y2=4(1 - x^2)\left(\frac{dy}{dx}\right)^2 + 4y^2 = 4

We verify y2(x)=2x21y_2(x) = 2x^2 - 1: dy2dx=4x\frac{dy_2}{dx} = 4x, and y2(1)=21=1y_2(1) = 2 - 1 = 1. \checkmark

Substituting: (1x2)(4x)2+4(2x21)2=16x2(1x2)+4(4x44x2+1)(1 - x^2)(4x)^2 + 4(2x^2 - 1)^2 = 16x^2(1 - x^2) + 4(4x^4 - 4x^2 + 1)

=16x216x4+16x416x2+4=4= 16x^2 - 16x^4 + 16x^4 - 16x^2 + 4 = 4. \checkmark

Part (iii). Let z(x)=2(yn(x))21z(x) = 2(y_n(x))^2 - 1.

Differentiating: dzdx=4yn(x)yn(x)\frac{dz}{dx} = 4y_n(x) \cdot y_n'(x).

Squaring: (dzdx)2=16yn2(yn)2\left(\frac{dz}{dx}\right)^2 = 16y_n^2 \cdot (y_n')^2.

From the differential equation ()(*) for yny_n:

(1x2)(yn)2=k2(1yn2)=n2(1yn2)(1 - x^2)(y_n')^2 = k^2(1 - y_n^2) = n^2(1 - y_n^2)

So:

(1x2)(dzdx)2=16yn2(1x2)(yn)2=16yn2n2(1yn2)=16n2yn2(1yn2)(1 - x^2)\left(\frac{dz}{dx}\right)^2 = 16y_n^2 \cdot (1 - x^2)(y_n')^2 = 16y_n^2 \cdot n^2(1 - y_n^2) = 16n^2 y_n^2(1 - y_n^2)

Also: z=2yn21z = 2y_n^2 - 1, so yn2=z+12y_n^2 = \frac{z + 1}{2} and 1yn2=1z+12=1z21 - y_n^2 = 1 - \frac{z + 1}{2} = \frac{1 - z}{2}.

Therefore:

(1x2)(dzdx)2=16n2z+121z2=4n2(1z2)(1 - x^2)\left(\frac{dz}{dx}\right)^2 = 16n^2 \cdot \frac{z + 1}{2} \cdot \frac{1 - z}{2} = 4n^2(1 - z^2)

(1x2)(dzdx)2+4n2z2=4n2(1 - x^2)\left(\frac{dz}{dx}\right)^2 + 4n^2 z^2 = 4n^2

This is the differential equation ()(*) with k=2nk = 2n. Also z(1)=2(yn(1))21=2(1)21=1z(1) = 2(y_n(1))^2 - 1 = 2(1)^2 - 1 = 1.

Since the solution satisfying y(1)=1y(1) = 1 is unique, z(x)=y2n(x)z(x) = y_{2n}(x).

Therefore:

y2n(x)=2(yn(x))21y_{2n}(x) = 2(y_n(x))^2 - 1

Part (iv). Let v(x)=yn(ym(x))v(x) = y_n(y_m(x)). We show v=ymnv = y_{mn}.

By the chain rule:

dvdx=yn(ym(x))ym(x)\frac{dv}{dx} = y_n'(y_m(x)) \cdot y_m'(x)

Squaring:

(dvdx)2=(yn)2ym(x)(ym)2\left(\frac{dv}{dx}\right)^2 = (y_n')^2 \big|_{y_m(x)} \cdot (y_m')^2

From the differential equation for yny_n (with k=nk = n, evaluated at ym(x)y_m(x), using ym(x)[1,1]y_m(x) \in [-1, 1]):

(1ym2)(yn)2ym=n2(1yn2(ym))=n2(1v2)(1 - y_m^2)(y_n')^2\big|_{y_m} = n^2(1 - y_n^2(y_m)) = n^2(1 - v^2)

From the differential equation for ymy_m (with k=mk = m):

(1x2)(ym)2=m2(1ym2)(1 - x^2)(y_m')^2 = m^2(1 - y_m^2)

Therefore:

(1x2)(dvdx)2=(1x2)(ym)2(yn)2ym(1 - x^2)\left(\frac{dv}{dx}\right)^2 = (1 - x^2)(y_m')^2 \cdot (y_n')^2\big|_{y_m}

=m2(1ym2)(yn)2ym= m^2(1 - y_m^2) \cdot (y_n')^2\big|_{y_m}

=m2n2(1v2)1ym2(1ym2)=m2n2(1v2)= m^2 \cdot \frac{n^2(1 - v^2)}{1 - y_m^2} \cdot (1 - y_m^2) = m^2 n^2(1 - v^2)

So:

(1x2)(dvdx)2+m2n2v2=m2n2(1 - x^2)\left(\frac{dv}{dx}\right)^2 + m^2 n^2 v^2 = m^2 n^2

This is the differential equation ()(*) with k=mnk = mn. Also v(1)=yn(ym(1))=yn(1)=1v(1) = y_n(y_m(1)) = y_n(1) = 1.

By uniqueness of the solution with y(1)=1y(1) = 1:

yn(ym(x))=ymn(x)y_n(y_m(x)) = y_{mn}(x)

Examiner Notes

Many candidates did not appear to read the question carefully enough and so attempted to solve the differential equations in parts (i) and (ii) rather than simply verifying the results given. Where candidates moved on to parts (iii) and (iv) they were generally successful if they were able to complete the differentiation of the new function.


Topic: 积分 (Integration)  |  Difficulty: Standard  |  Marks: 20

7 Show that

0af(x)dx=0af(ax)dx,(*)\int_0^a f(x) dx = \int_0^a f(a - x) dx, \qquad \text{(*)}

where ff is any function for which the integrals exist.

(i) Use ()(*) to evaluate 012πsinxcosx+sinxdx.\int_0^{\frac{1}{2}\pi} \frac{\sin x}{\cos x + \sin x} dx .

(ii) Evaluate 014πsinxcosx+sinxdx.\int_0^{\frac{1}{4}\pi} \frac{\sin x}{\cos x + \sin x} dx .

(iii) Evaluate 014πln(1+tanx)dx.\int_0^{\frac{1}{4}\pi} \ln(1 + \tan x) dx .

(iv) Evaluate 014πxcosx(cosx+sinx)dx.\int_0^{\frac{1}{4}\pi} \frac{x}{\cos x (\cos x + \sin x)} dx .

Hint

The first result can be shown by using a substitution into the integral, being careful to explain the change of sign when the limits of the integral are switched.

Simple application of knowledge of trigonometric graphs once the substitution has been made can be used to show that twice the integral is equivalent to integrating the function 1 over the interval.

Similarly, the remaining integrals can all be rearranged using standard trigonometric identities and knowledge of logarithms into forms that can be integrated from standard results once the substitution from (*) has been made.

Model Solution

Proving 0af(x)dx=0af(ax)dx\int_0^a f(x)\,dx = \int_0^a f(a-x)\,dx.

Substitute u=axu = a - x, so du=dxdu = -dx. When x=0x = 0, u=au = a; when x=ax = a, u=0u = 0.

0af(ax)dx=a0f(u)(du)=0af(u)du=0af(x)dx\int_0^a f(a - x)\,dx = \int_a^0 f(u)(-du) = \int_0^a f(u)\,du = \int_0^a f(x)\,dx

Part (i). Let I=0π/2sinxcosx+sinxdxI = \int_0^{\pi/2} \frac{\sin x}{\cos x + \sin x}\,dx.

By the result ()(*) with a=π/2a = \pi/2:

I=0π/2sin(π/2x)cos(π/2x)+sin(π/2x)dx=0π/2cosxsinx+cosxdxI = \int_0^{\pi/2} \frac{\sin(\pi/2 - x)}{\cos(\pi/2 - x) + \sin(\pi/2 - x)}\,dx = \int_0^{\pi/2} \frac{\cos x}{\sin x + \cos x}\,dx

Adding:

2I=0π/2sinx+cosxcosx+sinxdx=0π/21dx=π22I = \int_0^{\pi/2} \frac{\sin x + \cos x}{\cos x + \sin x}\,dx = \int_0^{\pi/2} 1\,dx = \frac{\pi}{2}

I=π4I = \frac{\pi}{4}

Part (ii). Let J=0π/4sinxcosx+sinxdxJ = \int_0^{\pi/4} \frac{\sin x}{\cos x + \sin x}\,dx.

By ()(*) with a=π/4a = \pi/4:

J=0π/4sin(π/4x)cos(π/4x)+sin(π/4x)dxJ = \int_0^{\pi/4} \frac{\sin(\pi/4 - x)}{\cos(\pi/4 - x) + \sin(\pi/4 - x)}\,dx

Using sin(π/4x)=12(cosxsinx)\sin(\pi/4 - x) = \frac{1}{\sqrt{2}}(\cos x - \sin x) and cos(π/4x)=12(cosx+sinx)\cos(\pi/4 - x) = \frac{1}{\sqrt{2}}(\cos x + \sin x):

J=0π/412(cosxsinx)12(cosx+sinx)+12(cosxsinx)dx=0π/4cosxsinx2cosxdxJ = \int_0^{\pi/4} \frac{\frac{1}{\sqrt{2}}(\cos x - \sin x)}{\frac{1}{\sqrt{2}}(\cos x + \sin x) + \frac{1}{\sqrt{2}}(\cos x - \sin x)}\,dx = \int_0^{\pi/4} \frac{\cos x - \sin x}{2\cos x}\,dx

=120π/4(1sinxcosx)dx=120π/4(1tanx)dx= \frac{1}{2}\int_0^{\pi/4} \left(1 - \frac{\sin x}{\cos x}\right)dx = \frac{1}{2}\int_0^{\pi/4} (1 - \tan x)\,dx

=12[x+lncosx]0π/4=12[π4+ln120ln1]= \frac{1}{2}\left[x + \ln|\cos x|\right]_0^{\pi/4} = \frac{1}{2}\left[\frac{\pi}{4} + \ln\frac{1}{\sqrt{2}} - 0 - \ln 1\right]

=12[π412ln2]=π8ln24= \frac{1}{2}\left[\frac{\pi}{4} - \frac{1}{2}\ln 2\right] = \frac{\pi}{8} - \frac{\ln 2}{4}

Part (iii). Let K=0π/4ln(1+tanx)dxK = \int_0^{\pi/4} \ln(1 + \tan x)\,dx.

By ()(*) with a=π/4a = \pi/4:

K=0π/4ln ⁣(1+tan ⁣(π4x))dxK = \int_0^{\pi/4} \ln\!\left(1 + \tan\!\left(\frac{\pi}{4} - x\right)\right)dx

Using tan(π/4x)=1tanx1+tanx\tan(\pi/4 - x) = \frac{1 - \tan x}{1 + \tan x}:

1+tan(π/4x)=1+1tanx1+tanx=1+tanx+1tanx1+tanx=21+tanx1 + \tan(\pi/4 - x) = 1 + \frac{1 - \tan x}{1 + \tan x} = \frac{1 + \tan x + 1 - \tan x}{1 + \tan x} = \frac{2}{1 + \tan x}

So K=0π/4ln ⁣(21+tanx)dx=0π/4[ln2ln(1+tanx)]dxK = \int_0^{\pi/4} \ln\!\left(\frac{2}{1 + \tan x}\right)dx = \int_0^{\pi/4} [\ln 2 - \ln(1 + \tan x)]\,dx.

K=π4ln2KK = \frac{\pi}{4}\ln 2 - K

2K=π4ln22K = \frac{\pi}{4}\ln 2

K=π8ln2K = \frac{\pi}{8}\ln 2

Part (iv). Let L=0π/4xcosx(cosx+sinx)dxL = \int_0^{\pi/4} \frac{x}{\cos x(\cos x + \sin x)}\,dx.

Using 1cosx(cosx+sinx)=1cos2x(1+tanx)=sec2x1+tanx\frac{1}{\cos x(\cos x + \sin x)} = \frac{1}{\cos^2 x(1 + \tan x)} = \frac{\sec^2 x}{1 + \tan x}.

Note that ddxln(1+tanx)=sec2x1+tanx\frac{d}{dx}\ln(1 + \tan x) = \frac{\sec^2 x}{1 + \tan x}. So we integrate by parts with u=xu = x, dv=sec2x1+tanxdxdv = \frac{\sec^2 x}{1 + \tan x}\,dx:

L=[xln(1+tanx)]0π/40π/4ln(1+tanx)dxL = \left[x\ln(1 + \tan x)\right]_0^{\pi/4} - \int_0^{\pi/4} \ln(1 + \tan x)\,dx

=π4ln20π8ln2=π8ln2= \frac{\pi}{4}\ln 2 - 0 - \frac{\pi}{8}\ln 2 = \frac{\pi}{8}\ln 2

Examiner Notes

This was the second most popular and one of the best-answered questions on the paper, with many candidates scoring very high marks. In many cases the initial result was explained clearly and then applied successfully to the first example. Candidates were generally able to follow through the calculations where they were able to see the way in which the result could be achieved, and so most of the attempts that followed a correct method only lost marks through occasional errors in calculation.


Topic: 级数与积分近似 (Series and Integration Approximation)  |  Difficulty: Challenging  |  Marks: 20

8 Evaluate the integral

m121x2dx(m>12).\int_{m-\frac{1}{2}}^{\infty} \frac{1}{x^2} \, dx \quad (m > \frac{1}{2}) .

Show by means of a sketch that

r=mn1r2m12n+121x2dx,(*)\sum_{r=m}^{n} \frac{1}{r^2} \approx \int_{m-\frac{1}{2}}^{n+\frac{1}{2}} \frac{1}{x^2} \, dx , \qquad \text{(*)}

where mm and nn are positive integers with m<nm < n.

(i) You are given that the infinite series r=11r2\sum_{r=1}^{\infty} \frac{1}{r^2} converges to a value denoted by EE. Use ()(*) to obtain the following approximations for EE:

E2;E53;E3320.E \approx 2; \quad E \approx \frac{5}{3}; \quad E \approx \frac{33}{20} .

(ii) Show that, when rr is large, the error in approximating 1r2\frac{1}{r^2} by r12r+121x2dx\int_{r-\frac{1}{2}}^{r+\frac{1}{2}} \frac{1}{x^2} \, dx is approximately 14r4\frac{1}{4r^4}.

Given that E1.645E \approx 1.645, show that r=11r41.08\sum_{r=1}^{\infty} \frac{1}{r^4} \approx 1.08.

Hint

The integral required at the start of the question should be a straightforward one to evaluate. When making a sketch to illustrate the result in the second part, ensure that the sum is indicated by a series of rectangles, with the graph of the curve passing through the midpoints of the tops.

In part (i), the integral that would match the sum given results in an answer of 2, so this is the first of the estimates. The remaining estimates arise from using the integral to estimate most of the sum, but taking the first few terms as the exact values (so in each case the integration is taken from a different lower limit).

For part (ii), evaluate the integral for one particular term of the sum and note that it is approximately rac{1}{4r^4}. Finally, using the most accurate estimate for E \left( rac{33}{20} ight) the sum from r=3r = 3 onwards can be calculated and then the first two values of rac{1}{r^4} can be added to achieve the desired result.

Model Solution

Evaluating the integral.

m1/21x2dx=[1x]m1/2=0(1m1/2)=1m1/2=22m1\int_{m - 1/2}^{\infty} \frac{1}{x^2}\,dx = \left[-\frac{1}{x}\right]_{m - 1/2}^{\infty} = 0 - \left(-\frac{1}{m - 1/2}\right) = \frac{1}{m - 1/2} = \frac{2}{2m - 1}

Sketch argument for ()(*).

Draw the curve y=1/x2y = 1/x^2 for x>0x > 0. For each integer rr from mm to nn, draw a rectangle of width 1 centred at x=rx = r, i.e. from x=r1/2x = r - 1/2 to x=r+1/2x = r + 1/2, with height 1/r21/r^2. The curve y=1/x2y = 1/x^2 passes through the midpoint of the top of each rectangle.

Since 1/x21/x^2 is a smooth, convex, decreasing function, the area of each rectangle (equal to 1/r21/r^2) is approximately equal to the area under the curve over [r1/2,r+1/2][r - 1/2, r + 1/2]. The errors at adjacent intervals partially cancel (the curve is above the rectangle on one side and below on the other), so:

r=mn1r2m1/2n+1/21x2dx\sum_{r=m}^{n} \frac{1}{r^2} \approx \int_{m - 1/2}^{n + 1/2} \frac{1}{x^2}\,dx

Part (i): Obtaining the three approximations.

The integral gives:

m1/2n+1/21x2dx=[1x]m1/2n+1/2=1m1/21n+1/2=22m122n+1\int_{m - 1/2}^{n + 1/2} \frac{1}{x^2}\,dx = \left[-\frac{1}{x}\right]_{m - 1/2}^{n + 1/2} = \frac{1}{m - 1/2} - \frac{1}{n + 1/2} = \frac{2}{2m - 1} - \frac{2}{2n + 1}

As nn \to \infty, the sum r=mn1/r2\sum_{r=m}^{n} 1/r^2 tends to Er=1m11/r2E - \sum_{r=1}^{m-1} 1/r^2, and the integral tends to 22m1\frac{2}{2m - 1}.

First approximation (m=1m = 1): Taking m=1m = 1 and nn \to \infty:

E22(1)1=2E \approx \frac{2}{2(1) - 1} = 2

Second approximation (m=2m = 2): Taking m=2m = 2 and nn \to \infty. The sum from r=2r = 2 to \infty is E1E - 1:

E122(2)1=23E - 1 \approx \frac{2}{2(2) - 1} = \frac{2}{3}

E1+23=53E \approx 1 + \frac{2}{3} = \frac{5}{3}

Third approximation (m=3m = 3): Taking m=3m = 3 and nn \to \infty. The sum from r=3r = 3 to \infty is E11/4=E5/4E - 1 - 1/4 = E - 5/4:

E5422(3)1=25E - \frac{5}{4} \approx \frac{2}{2(3) - 1} = \frac{2}{5}

E54+25=25+820=3320E \approx \frac{5}{4} + \frac{2}{5} = \frac{25 + 8}{20} = \frac{33}{20}

Part (ii): Error approximation.

For large rr, the error in approximating 1r2\frac{1}{r^2} by r1/2r+1/21x2dx\int_{r - 1/2}^{r + 1/2} \frac{1}{x^2}\,dx is:

1r2r1/2r+1/21x2dx=1r2[1r1/21r+1/2]\frac{1}{r^2} - \int_{r - 1/2}^{r + 1/2} \frac{1}{x^2}\,dx = \frac{1}{r^2} - \left[\frac{1}{r - 1/2} - \frac{1}{r + 1/2}\right]

=1r2(r+1/2)(r1/2)(r1/2)(r+1/2)=1r21r21/4= \frac{1}{r^2} - \frac{(r + 1/2) - (r - 1/2)}{(r - 1/2)(r + 1/2)} = \frac{1}{r^2} - \frac{1}{r^2 - 1/4}

=1r21r21/4=(r21/4)r2r2(r21/4)=1/4r2(r21/4)= \frac{1}{r^2} - \frac{1}{r^2 - 1/4} = \frac{(r^2 - 1/4) - r^2}{r^2(r^2 - 1/4)} = \frac{-1/4}{r^2(r^2 - 1/4)}

For large rr, r21/4r2r^2 - 1/4 \approx r^2, so the error is approximately:

1/4r4=14r4\frac{-1/4}{r^4} = -\frac{1}{4r^4}

The magnitude of the error is approximately 14r4\frac{1}{4r^4}.

Finding r=11/r4\sum_{r=1}^{\infty} 1/r^4.

From the approximation ()(*) with m=1m = 1 and nn \to \infty, the total error is:

E1/21x2dx=E2E - \int_{1/2}^{\infty} \frac{1}{x^2}\,dx = E - 2

This total error is the sum of the individual errors r=1(1r2r1/2r+1/21x2dx)\sum_{r=1}^{\infty} \left(\frac{1}{r^2} - \int_{r - 1/2}^{r + 1/2} \frac{1}{x^2}\,dx\right).

For large rr, each error is approximately 1/(4r4)-1/(4r^4). The errors for small rr also contribute, but using the approximation for all rr:

E214r=11r4E - 2 \approx -\frac{1}{4}\sum_{r=1}^{\infty} \frac{1}{r^4}

With E1.645E \approx 1.645:

1.6452=0.35514r=11r41.645 - 2 = -0.355 \approx -\frac{1}{4}\sum_{r=1}^{\infty} \frac{1}{r^4}

r=11r44×0.355=1.42\sum_{r=1}^{\infty} \frac{1}{r^4} \approx 4 \times 0.355 = 1.42

However, the approximation 14r4\frac{1}{4r^4} is not very accurate for small rr. A more careful approach: use the most accurate estimate E33/20E \approx 33/20 to find the sum from r=3r = 3 onwards, then add the first two terms exactly.

From E5/42/5E - 5/4 \approx 2/5, the error in this approximation is 33/205/42/5=33/2025/208/20=033/20 - 5/4 - 2/5 = 33/20 - 25/20 - 8/20 = 0. So the approximation E33/20E \approx 33/20 absorbs the error from r=1r = 1 and r=2r = 2 exactly.

Using the error formula: the total error from r=3r = 3 onwards is approximately 14r=31r4-\frac{1}{4}\sum_{r=3}^{\infty} \frac{1}{r^4}.

The actual value of r=31/r2=E11/4=E5/4\sum_{r=3}^{\infty} 1/r^2 = E - 1 - 1/4 = E - 5/4 and the integral estimate is 2/52/5. The error is:

(E54)2514r=31r4\left(E - \frac{5}{4}\right) - \frac{2}{5} \approx -\frac{1}{4}\sum_{r=3}^{\infty} \frac{1}{r^4}

With E1.645E \approx 1.645: E5/4=0.395E - 5/4 = 0.395, and 0.3950.4=0.0050.395 - 0.4 = -0.005.

0.00514r=31r4-0.005 \approx -\frac{1}{4}\sum_{r=3}^{\infty} \frac{1}{r^4}

r=31r40.02\sum_{r=3}^{\infty} \frac{1}{r^4} \approx 0.02

Adding the first two terms: 1+1/16=1.06251 + 1/16 = 1.0625.

r=11r41.0625+0.02=1.08\sum_{r=1}^{\infty} \frac{1}{r^4} \approx 1.0625 + 0.02 = 1.08

Examiner Notes

The first task in this question was generally well answered, although sketches were often unclear or difficult to interpret. In part (i) many candidates were able to obtain the first approximation, but then could not see how to achieve the other two, often offering sums of a non-integer number of terms which gives the correct approximation when substituted into the formula. Those who successfully completed part (i) were often able to approximate the error in part (ii) and see how it applies to the final sum.