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STEP3 2024 -- Pure Mathematics

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STEP3 2024 — Section A (Pure Mathematics)

Section titled “STEP3 2024 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2024  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1纯数Routine部分分式分解,伸缩求和(telescoping series),极限运算,级数拆分
2纯数Standard两边平方去根号,渐近分析,图像法,构造法
3纯数Standard求导分析单调性,极限分析,分类讨论(c≥1/2, 0<c<1/2, c=0)
4纯数Standard切线方程推导,两直线夹角公式(m₁-m₂)/(1+m₁m₂)=±1,轨迹方程消参
5纯数Challenging矩阵迹的循环性质,行列式求导(Jacobi公式),矩阵微分方程求解,构造反例
6纯数Hard微分方程组求解,变量消元(d(x-y)/dt等),必要条件分析,控制理论思想
7纯数Challenging几何级数估计,交错级数配对,阶乘与e的级数展开关系,反证法,适当选取n值
8纯数Challenging直线对的代数判据(p²-q²=4r),曲线交点分析,因式分解,蕴含方向论证

Topic: 纯数  |  Difficulty: Routine  |  Marks: 20

1 Throughout this question, NN is an integer with N1N \geqslant 1 and SN=r=1N1r2S_N = \sum_{r=1}^{N} \frac{1}{r^2}.

You may assume that limNSN\lim_{N \to \infty} S_N exists and is equal to 16π2\frac{1}{6}\pi^2.

(i) Show that 1r+11r+1r2=1r2(r+1).\frac{1}{r+1} - \frac{1}{r} + \frac{1}{r^2} = \frac{1}{r^2(r+1)}.

Hence show that r=1N1r2(r+1)=r=1N1r21+1N+1.\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = \sum_{r=1}^{N} \frac{1}{r^2} - 1 + \frac{1}{N+1}.

Show further that r=11r2(r+1)=16π21\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)} = \frac{1}{6}\pi^2 - 1.

(ii) Find r=1N1r2(r+1)(r+2)\sum_{r=1}^{N} \frac{1}{r^2(r+1)(r+2)} in terms of SNS_N, and hence evaluate r=11r2(r+1)(r+2)\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)(r+2)}.

(iii) Show that r=11r2(r+1)2=r=12r2(r+1)1.\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)^2} = \sum_{r=1}^{\infty} \frac{2}{r^2(r+1)} - 1.

Hint

(i)

1r+11r+1r2=1r2(r+1)[r2r(r+1)+(r+1)]\frac{1}{r+1} - \frac{1}{r} + \frac{1}{r^2} = \frac{1}{r^2(r+1)} [r^2 - r(r+1) + (r+1)] =1r2(r+1)[r2r2r+r+1]=1r2(r+1)= \frac{1}{r^2(r+1)} [r^2 - r^2 - r + r + 1] = \frac{1}{r^2(r+1)}

*B1

Thus

r=1N1r2(r+1)=r=1N1r+1r=1N1r+r=1N1r2\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = \sum_{r=1}^{N} \frac{1}{r+1} - \sum_{r=1}^{N} \frac{1}{r} + \sum_{r=1}^{N} \frac{1}{r^2} =r=2N+11rr=1N1r+r=1N1r2= \sum_{r=2}^{N+1} \frac{1}{r} - \sum_{r=1}^{N} \frac{1}{r} + \sum_{r=1}^{N} \frac{1}{r^2}

M1

=1N+11+r=1N1r2= \frac{1}{N+1} - 1 + \sum_{r=1}^{N} \frac{1}{r^2}

as required. *A1

So, as NN \rightarrow \infty,

LHSr=11r2(r+1),1N+10,and r=1N1r216π2LHS \rightarrow \sum_{r=1}^{\infty} \frac{1}{r^2(r+1)}, \frac{1}{N+1} \rightarrow 0, \text{and } \sum_{r=1}^{N} \frac{1}{r^2} \rightarrow \frac{1}{6}\pi^2

and hence

r=11r2(r+1)=16π21\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)} = \frac{1}{6}\pi^2 - 1

*B1 (4)

(ii)

1r2(r+1)(r+2)=Ar+Br2+Cr+1+Dr+2\frac{1}{r^2(r+1)(r+2)} = \frac{A}{r} + \frac{B}{r^2} + \frac{C}{r+1} + \frac{D}{r+2}

M1

1=Ar(r+1)(r+2)+B(r+1)(r+2)+Cr2(r+2)+Dr2(r+1)1 = Ar(r+1)(r+2) + B(r+1)(r+2) + Cr^2(r+2) + Dr^2(r+1)

r=01=2BB=12r = 0 \quad 1 = 2B \quad B = \frac{1}{2}

r=11=Cr = -1 \quad 1 = C

r=21=4DD=14r = -2 \quad 1 = -4D \quad D = -\frac{1}{4}

r3 terms0=A+C+DA=34r^3 \text{ terms} \quad 0 = A + C + D \quad A = -\frac{3}{4}

M1 A1 (3)


Thus

r=1N1r2(r+1)(r+2)=34r=1N1r+12r=1N1r2+r=1N1r+114r=1N1r+2\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)(r+2)} = -\frac{3}{4} \sum_{r=1}^{N} \frac{1}{r} + \frac{1}{2} \sum_{r=1}^{N} \frac{1}{r^{2}} + \sum_{r=1}^{N} \frac{1}{r+1} - \frac{1}{4} \sum_{r=1}^{N} \frac{1}{r+2}

M1

=3438+12SN+12+1N+1141N+1141N+2= -\frac{3}{4} - \frac{3}{8} + \frac{1}{2} S_{N} + \frac{1}{2} + \frac{1}{N+1} - \frac{1}{4} \frac{1}{N+1} - \frac{1}{4} \frac{1}{N+2}

dM1 A1ft

So

r=1N1r2(r+1)(r+2)=12SN+341N+1141N+258\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)(r+2)} = \frac{1}{2} S_{N} + \frac{3}{4} \frac{1}{N+1} - \frac{1}{4} \frac{1}{N+2} - \frac{5}{8}

and taking limits as NN \rightarrow \infty

M1

r=11r2(r+1)(r+2)=12×16π258=112π258\sum_{r=1}^{\infty} \frac{1}{r^{2}(r+1)(r+2)} = \frac{1}{2} \times \frac{1}{6} \pi^{2} - \frac{5}{8} = \frac{1}{12} \pi^{2} - \frac{5}{8}

A1 (5)

(iii)

1r2(r+1)2=Ar+Br2+Cr+1+D(r+1)2\frac{1}{r^{2}(r+1)^{2}} = \frac{A}{r} + \frac{B}{r^{2}} + \frac{C}{r+1} + \frac{D}{(r+1)^{2}}

M1

1=Ar(r+1)2+B(r+1)2+Cr2(r+1)+Dr21 = Ar(r+1)^{2} + B(r+1)^{2} + Cr^{2}(r+1) + Dr^{2} r=01=Br = 0 \quad 1 = B r=11=Dr = -1 \quad 1 = D r3 terms0=A+Cr^{3} \text{ terms} \quad 0 = A + C r2 terms0=2A+B+C+Dr^{2} \text{ terms} \quad 0 = 2A + B + C + D

M1

2=2A+C-2 = 2A + C A=2C=2A = -2 \quad C = 2

Thus

1r2(r+1)2=2r+1r2+2r+1+1(r+1)2\frac{1}{r^{2}(r+1)^{2}} = \frac{-2}{r} + \frac{1}{r^{2}} + \frac{2}{r+1} + \frac{1}{(r+1)^{2}}

A1 (3)


r=1N1r2(r+1)2=r=1N2r+r=1N1r2+r=1N2(r+1)+r=1N1(r+1)2\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)^{2}} = \sum_{r=1}^{N} \frac{-2}{r} + \sum_{r=1}^{N} \frac{1}{r^{2}} + \sum_{r=1}^{N} \frac{2}{(r+1)} + \sum_{r=1}^{N} \frac{1}{(r+1)^{2}} =r=1N2r+r=1N1r2+r=2N+12r+r=2N+11r2= \sum_{r=1}^{N} \frac{-2}{r} + \sum_{r=1}^{N} \frac{1}{r^{2}} + \sum_{r=2}^{N+1} \frac{2}{r} + \sum_{r=2}^{N+1} \frac{1}{r^{2}}

M1

=2+2N+1+2r=1N1r21+1(N+1)2= -2 + \frac{2}{N+1} + 2 \sum_{r=1}^{N} \frac{1}{r^{2}} - 1 + \frac{1}{(N+1)^{2}}

That is

r=1N1r2(r+1)2=2SN3+2N+1+1(N+1)2\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)^{2}} = 2S_{N} - 3 + \frac{2}{N+1} + \frac{1}{(N+1)^{2}}

A1

From part (i),

r=1N1r2(r+1)=1N+11+r=1N1r2=SN1+1N+1\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)} = \frac{1}{N+1} - 1 + \sum_{r=1}^{N} \frac{1}{r^{2}} = S_{N} - 1 + \frac{1}{N+1}

Thus

r=1N1r2(r+1)2=2(r=1N1r2(r+1)+11N+1)3+2N+1+1(N+1)2\sum_{r=1}^{N} \frac{1}{r^{2}(r+1)^{2}} = 2 \left( \sum_{r=1}^{N} \frac{1}{r^{2}(r+1)} + 1 - \frac{1}{N+1} \right) - 3 + \frac{2}{N+1} + \frac{1}{(N+1)^{2}} M1 =2r=1N1r2(r+1)1+1(N+1)2= 2 \sum_{r=1}^{N} \frac{1}{r^{2}(r+1)} - 1 + \frac{1}{(N+1)^{2}} A1

Letting NN \rightarrow \infty ,

r=11r2(r+1)2=r=12r2(r+1)1\sum_{r=1}^{\infty} \frac{1}{r^{2}(r+1)^{2}} = \sum_{r=1}^{\infty} \frac{2}{r^{2}(r+1)} - 1 B1* (5)


Model Solution

Part (i)

We show the identity by combining the left-hand side over a common denominator r2(r+1)r^2(r+1):

1r+11r+1r2=r2r(r+1)+(r+1)r2(r+1)=r2r2r+r+1r2(r+1)=1r2(r+1)\frac{1}{r+1} - \frac{1}{r} + \frac{1}{r^2} = \frac{r^2 - r(r+1) + (r+1)}{r^2(r+1)} = \frac{r^2 - r^2 - r + r + 1}{r^2(r+1)} = \frac{1}{r^2(r+1)}

as required.

Now summing from r=1r = 1 to NN:

r=1N1r2(r+1)=r=1N1r+1r=1N1r+r=1N1r2\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = \sum_{r=1}^{N} \frac{1}{r+1} - \sum_{r=1}^{N} \frac{1}{r} + \sum_{r=1}^{N} \frac{1}{r^2}

Re-indexing the first sum by setting s=r+1s = r + 1:

r=1N1r+1=s=2N+11s\sum_{r=1}^{N} \frac{1}{r+1} = \sum_{s=2}^{N+1} \frac{1}{s}

Therefore:

r=1N1r2(r+1)=r=2N+11rr=1N1r+r=1N1r2\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = \sum_{r=2}^{N+1} \frac{1}{r} - \sum_{r=1}^{N} \frac{1}{r} + \sum_{r=1}^{N} \frac{1}{r^2}

The first two sums telescope:

r=2N+11rr=1N1r=1N+11\sum_{r=2}^{N+1} \frac{1}{r} - \sum_{r=1}^{N} \frac{1}{r} = \frac{1}{N+1} - 1

Hence:

r=1N1r2(r+1)=r=1N1r21+1N+1\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = \sum_{r=1}^{N} \frac{1}{r^2} - 1 + \frac{1}{N+1}

as required.

Taking the limit as NN \to \infty: since 1N+10\frac{1}{N+1} \to 0 and r=1N1r216π2\sum_{r=1}^{N} \frac{1}{r^2} \to \frac{1}{6}\pi^2:

r=11r2(r+1)=16π21\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)} = \frac{1}{6}\pi^2 - 1


Part (ii)

We perform a partial fraction decomposition:

1r2(r+1)(r+2)=Ar+Br2+Cr+1+Dr+2\frac{1}{r^2(r+1)(r+2)} = \frac{A}{r} + \frac{B}{r^2} + \frac{C}{r+1} + \frac{D}{r+2}

Multiplying both sides by r2(r+1)(r+2)r^2(r+1)(r+2):

1=Ar(r+1)(r+2)+B(r+1)(r+2)+Cr2(r+2)+Dr2(r+1)1 = Ar(r+1)(r+2) + B(r+1)(r+2) + Cr^2(r+2) + Dr^2(r+1)

Setting r=0r = 0: 1=2B1 = 2B, so B=12B = \frac{1}{2}.

Setting r=1r = -1: 1=C1 = C, so C=1C = 1.

Setting r=2r = -2: 1=D(2)2(1)=4D1 = D(-2)^2(-1) = -4D, so D=14D = -\frac{1}{4}.

Comparing r3r^3 coefficients: 0=A+C+D=A+1140 = A + C + D = A + 1 - \frac{1}{4}, so A=34A = -\frac{3}{4}.

Therefore:

1r2(r+1)(r+2)=34r+12r2+1r+114(r+2)\frac{1}{r^2(r+1)(r+2)} = -\frac{3}{4r} + \frac{1}{2r^2} + \frac{1}{r+1} - \frac{1}{4(r+2)}

Summing from r=1r = 1 to NN:

r=1N1r2(r+1)(r+2)=34r=1N1r+12r=1N1r2+r=1N1r+114r=1N1r+2\sum_{r=1}^{N} \frac{1}{r^2(r+1)(r+2)} = -\frac{3}{4}\sum_{r=1}^{N}\frac{1}{r} + \frac{1}{2}\sum_{r=1}^{N}\frac{1}{r^2} + \sum_{r=1}^{N}\frac{1}{r+1} - \frac{1}{4}\sum_{r=1}^{N}\frac{1}{r+2}

Re-indexing the third and fourth sums:

r=1N1r+1=r=2N+11r=r=1N1r1+1N+1\sum_{r=1}^{N} \frac{1}{r+1} = \sum_{r=2}^{N+1} \frac{1}{r} = \sum_{r=1}^{N} \frac{1}{r} - 1 + \frac{1}{N+1}

r=1N1r+2=r=3N+21r=r=1N1r112+1N+1+1N+2\sum_{r=1}^{N} \frac{1}{r+2} = \sum_{r=3}^{N+2} \frac{1}{r} = \sum_{r=1}^{N} \frac{1}{r} - 1 - \frac{1}{2} + \frac{1}{N+1} + \frac{1}{N+2}

Substituting and collecting the coefficients of r=1N1r\sum_{r=1}^{N} \frac{1}{r}:

34+114=0-\frac{3}{4} + 1 - \frac{1}{4} = 0

so the harmonic sum terms cancel entirely. We are left with:

12SN+(1+1N+1)14(32+1N+1+1N+2)\frac{1}{2}S_N + \left(-1 + \frac{1}{N+1}\right) - \frac{1}{4}\left(-\frac{3}{2} + \frac{1}{N+1} + \frac{1}{N+2}\right)

Collecting constant terms and NN-dependent terms:

=12SN1+1N+1+3814(N+1)14(N+2)= \frac{1}{2}S_N - 1 + \frac{1}{N+1} + \frac{3}{8} - \frac{1}{4(N+1)} - \frac{1}{4(N+2)}

=12SN+34(N+1)14(N+2)58= \frac{1}{2}S_N + \frac{3}{4(N+1)} - \frac{1}{4(N+2)} - \frac{5}{8}

Taking the limit as NN \to \infty, the terms 34(N+1)\frac{3}{4(N+1)} and 14(N+2)\frac{1}{4(N+2)} vanish:

r=11r2(r+1)(r+2)=12π2658=π21258\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)(r+2)} = \frac{1}{2} \cdot \frac{\pi^2}{6} - \frac{5}{8} = \frac{\pi^2}{12} - \frac{5}{8}


Part (iii)

We perform a partial fraction decomposition:

1r2(r+1)2=Ar+Br2+Cr+1+D(r+1)2\frac{1}{r^2(r+1)^2} = \frac{A}{r} + \frac{B}{r^2} + \frac{C}{r+1} + \frac{D}{(r+1)^2}

Multiplying both sides by r2(r+1)2r^2(r+1)^2:

1=Ar(r+1)2+B(r+1)2+Cr2(r+1)+Dr21 = Ar(r+1)^2 + B(r+1)^2 + Cr^2(r+1) + Dr^2

Setting r=0r = 0: 1=B1 = B, so B=1B = 1.

Setting r=1r = -1: 1=D1 = D, so D=1D = 1.

Comparing r3r^3 coefficients: 0=A+C0 = A + C.

Comparing r2r^2 coefficients: 0=2A+B+C+D=2A+C+20 = 2A + B + C + D = 2A + C + 2.

Substituting C=AC = -A into the second equation: 0=2AA+2=A+20 = 2A - A + 2 = A + 2, so A=2A = -2 and C=2C = 2.

Therefore:

1r2(r+1)2=2r+1r2+2r+1+1(r+1)2\frac{1}{r^2(r+1)^2} = -\frac{2}{r} + \frac{1}{r^2} + \frac{2}{r+1} + \frac{1}{(r+1)^2}

Summing from r=1r = 1 to NN:

r=1N1r2(r+1)2=2r=1N1r+r=1N1r2+2r=1N1r+1+r=1N1(r+1)2\sum_{r=1}^{N} \frac{1}{r^2(r+1)^2} = -2\sum_{r=1}^{N}\frac{1}{r} + \sum_{r=1}^{N}\frac{1}{r^2} + 2\sum_{r=1}^{N}\frac{1}{r+1} + \sum_{r=1}^{N}\frac{1}{(r+1)^2}

The first and third sums telescope:

2r=1N1r+2r=2N+11r=21+2N+1=2+2N+1-2\sum_{r=1}^{N}\frac{1}{r} + 2\sum_{r=2}^{N+1}\frac{1}{r} = -2 \cdot 1 + \frac{2}{N+1} = -2 + \frac{2}{N+1}

The second and fourth sums combine:

r=1N1r2+r=2N+11r2=2SN1+1(N+1)2\sum_{r=1}^{N}\frac{1}{r^2} + \sum_{r=2}^{N+1}\frac{1}{r^2} = 2S_N - 1 + \frac{1}{(N+1)^2}

Combining all parts:

r=1N1r2(r+1)2=2SN3+2N+1+1(N+1)2(...)\sum_{r=1}^{N} \frac{1}{r^2(r+1)^2} = 2S_N - 3 + \frac{2}{N+1} + \frac{1}{(N+1)^2} \qquad \text{(...)}

From part (i), we know r=1N1r2(r+1)=SN1+1N+1\sum_{r=1}^{N} \frac{1}{r^2(r+1)} = S_N - 1 + \frac{1}{N+1}, so SN=r=1N1r2(r+1)+11N+1S_N = \sum_{r=1}^{N} \frac{1}{r^2(r+1)} + 1 - \frac{1}{N+1}. Substituting into (…):

r=1N1r2(r+1)2=2(r=1N1r2(r+1)+11N+1)3+2N+1+1(N+1)2\sum_{r=1}^{N} \frac{1}{r^2(r+1)^2} = 2\left(\sum_{r=1}^{N} \frac{1}{r^2(r+1)} + 1 - \frac{1}{N+1}\right) - 3 + \frac{2}{N+1} + \frac{1}{(N+1)^2}

=2r=1N1r2(r+1)+22N+13+2N+1+1(N+1)2= 2\sum_{r=1}^{N} \frac{1}{r^2(r+1)} + 2 - \frac{2}{N+1} - 3 + \frac{2}{N+1} + \frac{1}{(N+1)^2}

=2r=1N1r2(r+1)1+1(N+1)2= 2\sum_{r=1}^{N} \frac{1}{r^2(r+1)} - 1 + \frac{1}{(N+1)^2}

Taking the limit as NN \to \infty:

r=11r2(r+1)2=2r=11r2(r+1)1\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)^2} = 2\sum_{r=1}^{\infty} \frac{1}{r^2(r+1)} - 1

Examiner Notes

全卷最受欢迎且得分最高的题目(均分约15/20,98%+考生尝试)。考官报告指出:关键易错点包括将调和级数误当作收敛级数处理、将∞当作数字代入表达式。部分分式分解有多种正确方法,但解释需要清晰完整。


Topic: 纯数  |  Difficulty: Standard  |  Marks: 20

2 (i) Solve the inequalities

**(a)** $\sqrt{4x^2 - 8x + 64} \leqslant |x + 8|$,
**(b)** $\sqrt{4x^2 - 8x + 64} \leqslant |3x - 8|$.
**(ii)** **(a)** Let $f(x) = \sqrt{4x^2 - 8x + 64} - 2(x - 1)$.
Show, by considering $(\sqrt{4x^2 - 8x + 64} + 2(x - 1))f(x)$ or otherwise, that $f(x) \to 0$ as $x \to \infty$.
**(b)** Sketch $y = \sqrt{4x^2 - 8x + 64}$ and $y = 2(x - 1)$ on the same axes.
**(iii)** Find a value of $m$ and the corresponding value of $c$ such that the solution set of the inequality

4x25x+4mx+c\sqrt{4x^2 - 5x + 4} \leqslant |mx + c|

is $\{x : x \geqslant 3\}$.
**(iv)** Find values of $p, q, m$ and $c$ such that the solution set of the inequality

x2+px+qmx+c|x^2 + px + q| \leqslant mx + c

is $\{x : -5 \leqslant x \leqslant 1\} \cup \{x : 5 \leqslant x \leqslant 7\}$.
Hint

(i) (a)**

4x28x+64x+8\sqrt{4x^2 - 8x + 64} \leq |x + 8|

4x28x+64(x+8)2=x2+16x+644x^2 - 8x + 64 \leq (x + 8)^2 = x^2 + 16x + 64

Thus

3x224x=3x(x8)03x^2 - 24x = 3x(x - 8) \leq 0

M1

G1 or consideration of intervals M1

Alternative method Solve for critical values M1

Sketch graph

![Graph showing a parabola and an absolute value function intersecting on a grid

G1 ]

So 0x80 \leq x \leq 8 A1 (3)

(b)

4x28x+643x8\sqrt{4x^2 - 8x + 64} \leq |3x - 8|

4x28x+64(3x8)2=9x248x+644x^2 - 8x + 64 \leq (3x - 8)^2 = 9x^2 - 48x + 64

Thus

5x240x=5x(x8)05x^2 - 40x = 5x(x - 8) \geq 0

M1


GRAPH G1 or consideration of intervals M1

Alternative method Solve for critical values M1

Sketch graph

![A blue curve and a red V-shaped curve intersecting on a coordinate grid G1 ]

So x0x \le 0 or x8x \ge 8 A1 (3)

(ii) (a)

(4x28x+64+2(x1))f(x)(\sqrt{4x^2 - 8x + 64} + 2(x - 1)) f(x) =(4x28x+64+2(x1))(4x28x+642(x1))= (\sqrt{4x^2 - 8x + 64} + 2(x - 1))(\sqrt{4x^2 - 8x + 64} - 2(x - 1)) =4x28x+644x2+8x4=60= 4x^2 - 8x + 64 - 4x^2 + 8x - 4 = 60

Thus f(x)=60(4x28x+64+2(x1))f(x) = \frac{60}{(\sqrt{4x^2 - 8x + 64} + 2(x - 1))}

and so f(x)0f(x) \to 0 as xx \to \infty

E1 (1)


(b)

G2 (2)

(iii) Require one critical value 3, so 3m+c=±53m + c = \pm 5

M1

and as only one critical value choose m=2m = 2 and c=1c = -1, or m=2m = -2 and c=1c = 1

dM1 A1

4x25x+42x1\sqrt{4x^2 - 5x + 4} \le |2x - 1|

4x25x+4(2x1)2=4x24x+14x^2 - 5x + 4 \le (2x - 1)^2 = 4x^2 - 4x + 1

Giving x3x \ge 3

M1

G1 (5)


(iv) To obtain 4 critical values require quadratic to cross x axis and so

E1

x2+px+q=mx+cx^2 + px + q = mx + c has roots -5 and 7 giving pm=2p - m = -2 and qc=35q - c = -35

M1 A1

and

(x2+px+q)=mx+c-(x^2 + px + q) = mx + c

has roots 1 and 5 giving p+m=6p + m = -6 and q+c=5q + c = 5

B1

Thus, p=4p = -4, q=15,m=2q = -15, m = -2, c=20c = 20

A1

x y (quadratic) y (linear)
-5 0 30
-2 11 24
0 15 20
1 12 18
3 6 14
5 0 10
7 0 6

G1 (6)


Model Solution

Part (i)(a)

We need to solve 4x28x+64x+8\sqrt{4x^2 - 8x + 64} \leqslant |x + 8|.

The left-hand side is a square root, so it is non-negative for all real xx. The right-hand side is an absolute value, also non-negative. Since both sides are non-negative, we may square both sides without changing the direction of the inequality:

4x28x+64(x+8)2=x2+16x+644x^2 - 8x + 64 \leqslant (x + 8)^2 = x^2 + 16x + 64

Rearranging:

3x224x03x^2 - 24x \leqslant 0

3x(x8)03x(x - 8) \leqslant 0

The product 3x(x8)3x(x-8) is zero at x=0x = 0 and x=8x = 8, and is negative when 0<x<80 < x < 8 (one factor positive, one negative). Therefore the solution set is 0x80 \leqslant x \leqslant 8.


Part (i)(b)

We need to solve 4x28x+643x8\sqrt{4x^2 - 8x + 64} \leqslant |3x - 8|.

Again, both sides are non-negative, so squaring preserves the inequality:

4x28x+64(3x8)2=9x248x+644x^2 - 8x + 64 \leqslant (3x - 8)^2 = 9x^2 - 48x + 64

Rearranging:

05x240x0 \leqslant 5x^2 - 40x

5x(x8)05x(x - 8) \geqslant 0

The product 5x(x8)5x(x-8) is zero at x=0x = 0 and x=8x = 8, and is non-negative when x0x \leqslant 0 or x8x \geqslant 8 (both factors same sign). Therefore the solution set is x0x \leqslant 0 or x8x \geqslant 8.


Part (ii)(a)

Let f(x)=4x28x+642(x1)f(x) = \sqrt{4x^2 - 8x + 64} - 2(x - 1). Consider the product:

(4x28x+64+2(x1))f(x)\left(\sqrt{4x^2 - 8x + 64} + 2(x - 1)\right) f(x)

=(4x28x+64)2(2(x1))2= \left(\sqrt{4x^2 - 8x + 64}\right)^2 - \left(2(x - 1)\right)^2

=(4x28x+64)4(x22x+1)= (4x^2 - 8x + 64) - 4(x^2 - 2x + 1)

=4x28x+644x2+8x4=60= 4x^2 - 8x + 64 - 4x^2 + 8x - 4 = 60

Therefore:

f(x)=604x28x+64+2(x1)f(x) = \frac{60}{\sqrt{4x^2 - 8x + 64} + 2(x - 1)}

As xx \to \infty, the denominator 4x28x+64+2(x1)\sqrt{4x^2 - 8x + 64} + 2(x - 1) \to \infty (both terms grow without bound), so f(x)0f(x) \to 0.


Part (ii)(b)

Complete the square: 4x28x+64=4(x1)2+604x^2 - 8x + 64 = 4(x - 1)^2 + 60, so y=4(x1)2+60y = \sqrt{4(x-1)^2 + 60}.

Key features:

  • Symmetric about x=1x = 1.
  • At x=1x = 1: y=60=2157.75y = \sqrt{60} = 2\sqrt{15} \approx 7.75.
  • As x±x \to \pm\infty: yy \to \infty.

The line y=2(x1)y = 2(x - 1) passes through (1,0)(1, 0) with gradient 2. From part (ii)(a), this is an asymptote of the curve for large xx. Since f(x)>0f(x) > 0 for all xx, the curve lies strictly above this asymptote.

The sketch shows the curve starting at (0,215)(0, 2\sqrt{15}), decreasing to its minimum 2152\sqrt{15} at x=1x = 1, then increasing and approaching the dashed line y=2(x1)y = 2(x-1) from above as xx \to \infty. The left branch rises steeply as xx \to -\infty.


Part (iii)

We need mm and cc such that 4x25x+4mx+c\sqrt{4x^2 - 5x + 4} \leqslant |mx + c| has solution set {x:x3}\{x : x \geqslant 3\}.

Squaring both sides (valid since both are non-negative):

4x25x+4m2x2+2mcx+c24x^2 - 5x + 4 \leqslant m^2 x^2 + 2mcx + c^2

(m24)x2+(2mc+5)x+(c24)0(m^2 - 4)x^2 + (2mc + 5)x + (c^2 - 4) \geqslant 0

For the solution set to be x3x \geqslant 3 (a single boundary point), the quadratic must reduce to a linear expression with positive coefficient and root at x=3x = 3. This requires m2=4m^2 = 4, i.e. m=±2m = \pm 2.

The inequality becomes linear: (2mc+5)x+(c24)0(2mc + 5)x + (c^2 - 4) \geqslant 0, giving x4c22mc+5x \geqslant \frac{4 - c^2}{2mc + 5} (when 2mc+5>02mc + 5 > 0).

Setting 4c22mc+5=3\frac{4 - c^2}{2mc + 5} = 3: 4c2=6mc+154 - c^2 = 6mc + 15, i.e. c2+6mc+11=0c^2 + 6mc + 11 = 0.

With m=2m = 2: c2+12c+11=(c+1)(c+11)=0c^2 + 12c + 11 = (c+1)(c+11) = 0, so c=1c = -1 or c=11c = -11.

  • c=1c = -1: 2(2)(1)+5=1>02(2)(-1) + 5 = 1 > 0. Solution: x3x \geqslant 3. Check at x=3x = 3: 3615+4=5\sqrt{36 - 15 + 4} = 5 and 61=5|6 - 1| = 5. Equality holds. Valid.
  • c=11c = -11: 2(2)(11)+5=39<02(2)(-11) + 5 = -39 < 0. Direction flips. Not valid.

With m=2m = -2: c212c+11=(c1)(c11)=0c^2 - 12c + 11 = (c-1)(c-11) = 0, giving c=1c = 1 or c=11c = 11.

  • c=1c = 1: 2(2)(1)+5=1>02(-2)(1) + 5 = 1 > 0. But mx+c=2x+1=2x1|mx + c| = |-2x + 1| = |2x - 1|, same as m=2,c=1m = 2, c = -1.

So m=2m = 2, c=1c = -1.

Verification: 4x25x+42x1\sqrt{4x^2 - 5x + 4} \leqslant |2x - 1|. Squaring: 4x25x+44x24x+14x^2 - 5x + 4 \leqslant 4x^2 - 4x + 1, giving x3x \geqslant 3.


Part (iv)

We need p,q,m,cp, q, m, c such that x2+px+qmx+c|x^2 + px + q| \leqslant mx + c has solution set {5x1}{5x7}\{-5 \leqslant x \leqslant 1\} \cup \{5 \leqslant x \leqslant 7\}.

Since mx+c0mx + c \geqslant 0 on the solution set, and the solution has two separate intervals, the quadratic x2+px+qx^2 + px + q must be negative in the gap (1,5)(1, 5). At the boundary points, equality holds.

At x=5x = -5 and x=7x = 7 (where the quadratic is non-negative): x2+px+q=mx+cx^2 + px + q = mx + c.

Substituting: 255p+q=5m+c25 - 5p + q = -5m + c and 49+7p+q=7m+c49 + 7p + q = 7m + c.

Subtracting: 24+12p=12m24 + 12p = 12m, so pm=2p - m = -2.

At x=1x = 1 and x=5x = 5 (where the quadratic is negative): (x2+px+q)=mx+c-(x^2 + px + q) = mx + c.

Substituting: (1+p+q)=m+c-(1 + p + q) = m + c and (25+5p+q)=5m+c-(25 + 5p + q) = 5m + c.

Subtracting: 244p=4m-24 - 4p = 4m, so p+m=6p + m = -6.

From pm=2p - m = -2 and p+m=6p + m = -6: p=4p = -4, m=2m = -2.

From (1+p+q)=m+c-(1 + p + q) = m + c: 3q=2+c3 - q = -2 + c, so q+c=5q + c = 5.

From 255p+q=5m+c25 - 5p + q = -5m + c: 45+q=10+c45 + q = 10 + c, so qc=35q - c = -35.

Adding: 2q=302q = -30, so q=15q = -15 and c=20c = 20.

Therefore p=4p = -4, q=15q = -15, m=2m = -2, c=20c = 20.

Verification: The quadratic is x24x15=(x+5)(x7)x^2 - 4x - 15 = (x + 5)(x - 7), with roots at x=5x = -5 and x=7x = 7, negative on (5,7)(-5, 7). The linear function is 2x+20-2x + 20.

  • At x=5x = -5: 0=030|0| = 0 \leqslant 30. OK.
  • At x=1x = 1: 1415=1818|1 - 4 - 15| = 18 \leqslant 18. OK (boundary).
  • At x=5x = 5: 252015=1010|25 - 20 - 15| = 10 \leqslant 10. OK (boundary).
  • At x=7x = 7: 0=06|0| = 0 \leqslant 6. OK.
  • At x=3x = 3 (in gap): 91215=18|9 - 12 - 15| = 18 and 6+20=14-6 + 20 = 14. So 181418 \leqslant 14 is false. Correctly excluded.
  • At x=8x = 8 (outside): 643215=17|64 - 32 - 15| = 17 and 16+20=4-16 + 20 = 4. So 17417 \leqslant 4 is false. Correctly excluded.
Examiner Notes

约75%考生尝试,均分约10/20。常见问题:平方前未说明LHS为实数且两边为正;(ii)(a)中仅凭首项抵消就断言f(x)→0不得满分;作图需体现渐近线和关于x=1的对称性;(iv)部分使用图像法的考生表现明显更好,常见错误是四个根未能正确对应二次函数的正负号。


Topic: 纯数  |  Difficulty: Standard  |  Marks: 20

3 Throughout this question, consider only x>0x > 0.

(i) Let g(x)=ln(1+1x)x+cx(x+1)g(x) = \ln \left( 1 + \frac{1}{x} \right) - \frac{x + c}{x(x + 1)} where c0c \geqslant 0.

(a) Show that y=g(x)y = g(x) has positive gradient for all x>0x > 0 when c12c \geqslant \frac{1}{2}.

(b) Find the values of xx for which y=g(x)y = g(x) has negative gradient when 0c<120 \leqslant c < \frac{1}{2}.

(ii) It is given that, for all c>0c > 0, g(x)g(x) \to -\infty as x0x \to 0.

Sketch, for x>0x > 0, the graphs of y=g(x)y = g(x) in the cases

(a) c=34c = \frac{3}{4},

(b) c=14c = \frac{1}{4}.

(iii) The function f is defined as f(x)=(1+1x)x+c.f(x) = \left( 1 + \frac{1}{x} \right)^{x+c}. Show that, for x>0x > 0,

(a) f is a decreasing function when c12c \geqslant \frac{1}{2};

(b) f has a turning point when 0<c<120 < c < \frac{1}{2};

(c) f is an increasing function when c=0c = 0.

Hint

(i) (a)

y=g(x)=ln(1+1x)x+cx(x+1)=ln(x+1)lnxx+cx(x+1)y = g(x) = \ln \left( 1 + \frac{1}{x} \right) - \frac{x + c}{x(x + 1)} = \ln(x + 1) - \ln x - \frac{x + c}{x(x + 1)}

dydx=1x+11xx(x+1)(x+c)(2x+1)x2(x+1)2\frac{dy}{dx} = \frac{1}{x + 1} - \frac{1}{x} - \frac{x(x + 1) - (x + c)(2x + 1)}{x^2(x + 1)^2}

M1

=x2(x+1)x(x+1)2x(x+1)+(x+c)(2x+1)x2(x+1)2= \frac{x^2(x + 1) - x(x + 1)^2 - x(x + 1) + (x + c)(2x + 1)}{x^2(x + 1)^2}

=(2c1)x+cx2(x+1)2= \frac{(2c - 1)x + c}{x^2(x + 1)^2}

A1

When c12c \geq \frac{1}{2}, as x>0x > 0, (2c1)x0(2c - 1)x \geq 0, and c>0c > 0, so the numerator is positive and the denominator is a non-zero square so also positive, so y=g(x)y = g(x) has positive gradient.

E1 (3)

(b) y=g(x)y = g(x) has negative gradient for 0c<120 \leq c < \frac{1}{2}, if

(2c1)x+c<0(2c - 1)x + c < 0

That is

(2c1)x<c(2c - 1)x < -c

So

x>c2c1=c12cx > \frac{-c}{2c - 1} = \frac{c}{1 - 2c}

B1 (1)

(ii) (a)

If c=34c = \frac{3}{4}, then from (i) (a) the gradient is positive

E1

and we are given that g(x)g(x) \rightarrow -\infty as x0x \rightarrow 0.

The gradient tends to zero as xx \rightarrow \infty, and to \infty as x0x \rightarrow 0. E1

Also, g(x)0g(x) \rightarrow 0 as xx \rightarrow \infty. E1


G1 (4)

(b)

If c=14c = \frac{1}{4}, then from (i)(b) the gradient is negative for x>12x > \frac{1}{2}.

B1

The gradient is zero when x=12x = \frac{1}{2}, and positive when x<12x < \frac{1}{2}, and tending to zero as xx \rightarrow \infty, and to \infty as x0x \rightarrow 0. B1

Again, we are given that g(x)g(x) \rightarrow -\infty as x0x \rightarrow 0, and g(x)0g(x) \rightarrow 0 as xx \rightarrow \infty.

There is a turning point (maximum) at (12,ln31)=(12,ln3e)(\frac{1}{2}, \ln 3 - 1) = (\frac{1}{2}, \ln \frac{3}{e}) which is above the x-axis.

M1 A1

G1 (5)


(iii)

f(x)=(1+1x)x+cf(x) = \left( 1 + \frac{1}{x} \right)^{x+c}

ln(f(x))=(x+c)ln(1+1x)\ln(f(x)) = (x + c) \ln \left( 1 + \frac{1}{x} \right)

Thus

f(x)f(x)=ln(1+1x)+(x+c)(1x+11x)=g(x)\frac{f'(x)}{f(x)} = \ln \left( 1 + \frac{1}{x} \right) + (x + c) \left( \frac{1}{x + 1} - \frac{1}{x} \right) = g(x)

f(x)=f(x)g(x)f'(x) = f(x)g(x)

M1 A1 (2)

Also, f(x)f(x) is positive for x>0x > 0.

(a) As has been demonstrated in (i) (a) and (ii) (a), g(x)<0g(x) < 0 for x>0x > 0 when c12c \geq \frac{1}{2}, so

f(x)<0f'(x) < 0 and f is a decreasing function. [E1]

(b) As has been demonstrated in (i) (b) and (ii) (b), g(x)=0g(x) = 0 for some x>0x > 0 when 0<c<120 < c < \frac{1}{2}, so f(x)=0f'(x) = 0 for some x and f has a turning point. [E1]

(c) When c=0c = 0,

g(x)=1x(x+1)2g'(x) = \frac{-1}{x(x + 1)^2}

Is always negative and \rightarrow -\infty as x0x \rightarrow 0, and 0\rightarrow 0 as xx \rightarrow \infty

[E1]

whilst g(x)g(x) \rightarrow \infty as x0x \rightarrow 0, and g(x)0g(x) \rightarrow 0 as xx \rightarrow \infty

so g(x)g(x) is positive for all x>0x > 0, [E1]

thus f(x)f'(x) is too and thus f is an increasing function

for all x>0x > 0 [E1 (5)]


Model Solution

Part (i)(a)

We write g(x)=ln(x+1)lnxx+cx(x+1)g(x) = \ln(x+1) - \ln x - \frac{x+c}{x(x+1)} and compute g(x)g'(x).

The first two terms give: ddx[ln(x+1)lnx]=1x+11x=1x(x+1)\frac{d}{dx}[\ln(x+1) - \ln x] = \frac{1}{x+1} - \frac{1}{x} = \frac{-1}{x(x+1)}

For the third term, using the quotient rule with numerator x+cx + c and denominator x2+xx^2 + x: ddx[x+cx2+x]=1(x2+x)(x+c)(2x+1)(x2+x)2\frac{d}{dx}\left[\frac{x+c}{x^2+x}\right] = \frac{1 \cdot (x^2+x) - (x+c)(2x+1)}{(x^2+x)^2}

Expanding the numerator: x2+x(2x2+x+2cx+c)=x22cxcx^2 + x - (2x^2 + x + 2cx + c) = -x^2 - 2cx - c

So the third term contributes x22cxcx2(x+1)2\frac{-x^2 - 2cx - c}{x^2(x+1)^2} to g(x)g'(x) (with a minus sign from the definition of gg).

Combining over the common denominator x2(x+1)2x^2(x+1)^2: g(x)=x(x+1)x2(x+1)2x22cxcx2(x+1)2=x2x+x2+2cx+cx2(x+1)2=(2c1)x+cx2(x+1)2g'(x) = \frac{-x(x+1)}{x^2(x+1)^2} - \frac{-x^2 - 2cx - c}{x^2(x+1)^2} = \frac{-x^2 - x + x^2 + 2cx + c}{x^2(x+1)^2} = \frac{(2c-1)x + c}{x^2(x+1)^2}

When c12c \geqslant \frac{1}{2} and x>0x > 0:

  • 2c102c - 1 \geqslant 0, so (2c1)x0(2c-1)x \geqslant 0
  • c12>0c \geqslant \frac{1}{2} > 0

Hence the numerator (2c1)x+c>0(2c-1)x + c > 0. The denominator x2(x+1)2>0x^2(x+1)^2 > 0, so g(x)>0g'(x) > 0 for all x>0x > 0. \qquad \blacksquare


Part (i)(b)

When 0c<120 \leqslant c < \frac{1}{2}, the gradient is negative when: (2c1)x+c<0(2c-1)x + c < 0

Since 2c1<02c - 1 < 0, dividing by this negative quantity reverses the inequality: x>c2c1=c12cx > \frac{-c}{2c-1} = \frac{c}{1-2c}

When c=0c = 0: this gives x>0x > 0, so g(x)<0g'(x) < 0 for all x>0x > 0.

When 0<c<120 < c < \frac{1}{2}: g(x)g(x) has negative gradient for x>c12cx > \frac{c}{1-2c}.


Part (ii)(a): c=34c = \frac{3}{4}

Since c=3412c = \frac{3}{4} \geqslant \frac{1}{2}, part (i)(a) tells us gg has positive gradient for all x>0x > 0, so gg is strictly increasing.

We are given g(x)g(x) \to -\infty as x0x \to 0. As xx \to \infty: ln(1+1/x)0\ln(1+1/x) \to 0 and x+cx(x+1)0\frac{x+c}{x(x+1)} \to 0, so g(x)0g(x) \to 0.

Since gg is increasing and approaches 00 from below, we have g(x)<0g(x) < 0 for all x>0x > 0.

The graph rises monotonically from -\infty, asymptotic to y=0y = 0 from below.

Part (ii)(b): c=14c = \frac{1}{4}

Since c=14<12c = \frac{1}{4} < \frac{1}{2}, part (i)(b) gives c12c=1/41/2=12\frac{c}{1-2c} = \frac{1/4}{1/2} = \frac{1}{2}.

  • g(x)>0g'(x) > 0 for 0<x<120 < x < \frac{1}{2} (increasing)
  • g(x)=0g'(x) = 0 at x=12x = \frac{1}{2} (turning point)
  • g(x)<0g'(x) < 0 for x>12x > \frac{1}{2} (decreasing)

At the turning point: g ⁣(12)=ln ⁣(1+2)12+141232=ln33/43/4=ln31g\!\left(\tfrac{1}{2}\right) = \ln\!\left(1 + 2\right) - \frac{\frac{1}{2} + \frac{1}{4}}{\frac{1}{2} \cdot \frac{3}{2}} = \ln 3 - \frac{3/4}{3/4} = \ln 3 - 1

Since ln31.099>1\ln 3 \approx 1.099 > 1, this maximum is positive. The graph rises from -\infty to a maximum at (12,ln31)\left(\frac{1}{2},\, \ln 3 - 1\right) above the xx-axis, then decreases towards y=0y = 0 from above.


Part (iii)

Taking logarithms: lnf(x)=(x+c)ln ⁣(1+1x)\ln f(x) = (x+c)\ln\!\left(1 + \frac{1}{x}\right)

Differentiating using the product rule: f(x)f(x)=ln ⁣(1+1x)+(x+c)ddxln ⁣(1+1x)\frac{f'(x)}{f(x)} = \ln\!\left(1 + \frac{1}{x}\right) + (x+c) \cdot \frac{d}{dx}\ln\!\left(1 + \frac{1}{x}\right)

Now ddxln ⁣(1+1x)=11+1/x(1x2)=xx+1(1x2)=1x(x+1)\frac{d}{dx}\ln\!\left(1 + \frac{1}{x}\right) = \frac{1}{1+1/x} \cdot \left(-\frac{1}{x^2}\right) = \frac{x}{x+1} \cdot \left(-\frac{1}{x^2}\right) = \frac{-1}{x(x+1)}.

Therefore: f(x)f(x)=ln ⁣(1+1x)x+cx(x+1)=g(x)\frac{f'(x)}{f(x)} = \ln\!\left(1 + \frac{1}{x}\right) - \frac{x+c}{x(x+1)} = g(x)

So f(x)=f(x)g(x)f'(x) = f(x)\,g(x).

Since x>0x > 0, we have 1+1x>1>01 + \frac{1}{x} > 1 > 0, so f(x)>0f(x) > 0. The sign of f(x)f'(x) is determined entirely by the sign of g(x)g(x).

(a) When c12c \geqslant \frac{1}{2}: By part (i)(a), gg is increasing. By part (ii)(a), g(x)<0g(x) < 0 for all x>0x > 0 (since gg increases towards 00 from below). Hence f(x)<0f'(x) < 0 for all x>0x > 0, and ff is a decreasing function.

(b) When 0<c<120 < c < \frac{1}{2}: From the analysis in part (ii)(b), gg increases from -\infty (as x0x \to 0) to a positive maximum, then decreases towards 00 (as xx \to \infty). By the intermediate value theorem, gg equals 00 at exactly one value of xx. At this point f(x)=0f'(x) = 0, so ff has a turning point.

(c) When c=0c = 0:

g(x)=(201)x+0x2(x+1)2=xx2(x+1)2=1x(x+1)2<0for all x>0g'(x) = \frac{(2 \cdot 0 - 1)x + 0}{x^2(x+1)^2} = \frac{-x}{x^2(x+1)^2} = \frac{-1}{x(x+1)^2} < 0 \quad \text{for all } x > 0

So gg is strictly decreasing. As xx \to \infty: g(x)0g(x) \to 0. As x0+x \to 0^+: ln(1+1/x)+\ln(1+1/x) \to +\infty while 1x+11\frac{1}{x+1} \to 1, so g(x)+g(x) \to +\infty.

Since gg decreases from ++\infty to 00, we have g(x)>0g(x) > 0 for all x>0x > 0. Hence f(x)>0f'(x) > 0 for all x>0x > 0, and ff is an increasing function.

Examiner Notes

第二受欢迎题目,均分约9/20。常见问题:(i)(a)中c≥1/2时正梯度的充分论证常缺失;(i)(b)中忘记不等式在除以负数时需要反向;(ii)作图中多数能正确画出,但(a)中需论证正梯度和渐近线,(b)中需论证拐点前的正梯度;(iii)中忘记提及f>0是丢分常见原因。


Topic: 纯数  |  Difficulty: Standard  |  Marks: 20

4 (i) Show that if the acute angle between straight lines with gradients m1m_1 and m2m_2 is 4545^\circ, then

m1m21+m1m2=±1.\frac{m_1 - m_2}{1 + m_1 m_2} = \pm 1.

The curve CC has equation 4ay=x24ay = x^2 (where a0a \neq 0).

(ii) If pqp \neq q, show that the tangents to the curve CC at the points with xx-coordinates pp and qq meet at a point with xx-coordinate 12(p+q)\frac{1}{2}(p + q). Find the yy-coordinate of this point in terms of pp and qq.

Show further that any two tangents to the curve CC which are at 4545^\circ to each other meet on the curve (y+3a)2=8a2+x2(y + 3a)^2 = 8a^2 + x^2.

(iii) Show that the acute angle between any two tangents to the curve CC which meet on the curve (y+7a)2=48a2+3x2(y + 7a)^2 = 48a^2 + 3x^2 is constant. Find this acute angle.

Hint

(i)**

Suppose m1=tanθ1m_1 = \tan \theta_1 and m2=tanθ2m_2 = \tan \theta_2, where 12π<θ1,θ212π-\frac{1}{2}\pi < \theta_1, \theta_2 \le \frac{1}{2}\pi, then as the angle between the lines is 4545^\circ, θ1θ2=±14π\theta_1 - \theta_2 = \pm \frac{1}{4}\pi, or ±34π\pm \frac{3}{4}\pi. [M1]

Therefore

tan(θ1θ2)=±1\tan(\theta_1 - \theta_2) = \pm 1

and so

tan(θ1θ2)=tanθ1tanθ21+tanθ1tanθ2=±1\tan(\theta_1 - \theta_2) = \frac{\tan \theta_1 - \tan \theta_2}{1 + \tan \theta_1 \tan \theta_2} = \pm 1 [M1]

i.e.

m1m21+m1m2=±1\frac{m_1 - m_2}{1 + m_1 m_2} = \pm 1 [*A1 (3)]

(ii)

4ay=x24ay = x^2

4adydx=2x4a \frac{dy}{dx} = 2x

So the tangent at the point with x-coordinate pp is

yp24a=p2a(xp)y - \frac{p^2}{4a} = \frac{p}{2a}(x - p)

4ay+p2=2px4ay + p^2 = 2px [M1]

The tangents 4ay+p2=2px4ay + p^2 = 2px, 4ay+q2=2qx4ay + q^2 = 2qx meet when

2(pq)x=p2q2=(pq)(p+q)2(p - q)x = p^2 - q^2 = (p - q)(p + q) and as (pq)0(p - q) \neq 0,

[M1]

x=12(p+q)x = \frac{1}{2}(p + q) [*A1]

So

y=2p×12(p+q)p24a=pq4ay = \frac{2p \times \frac{1}{2}(p + q) - p^2}{4a} = \frac{pq}{4a} [A1 (4)]


and if the tangents meet at 4545^\circ, then

p2aq2a1+p2aq2a=±1\frac{\frac{p}{2a} - \frac{q}{2a}}{1 + \frac{p}{2a} \frac{q}{2a}} = \pm 1

M1 M1

2a(pq)=±(4a2+pq)2a(p - q) = \pm(4a^2 + pq) (4a2+pq)2=4a2(pq)2=4a2((p+q)24pq)(4a^2 + pq)^2 = 4a^2(p - q)^2 = 4a^2((p + q)^2 - 4pq)

M1

Thus the point of intersection satisfies

(4a2+4ay)2=4a2((2x)216ay)(4a^2 + 4ay)^2 = 4a^2((2x)^2 - 16ay)

M1

That simplifies to

(a+y)2=x24ay(a + y)^2 = x^2 - 4ay y2+6ay+a2=x2y^2 + 6ay + a^2 = x^2 y2+6ay+9a2=x2+8a2y^2 + 6ay + 9a^2 = x^2 + 8a^2 (y+3a)2=x2+8a2(y + 3a)^2 = x^2 + 8a^2

*M1 A1 (6)

(iii)

If

(y+7a)2=48a2+3x2(y + 7a)^2 = 48a^2 + 3x^2 (pq4a+7a)2=48a2+3(12(p+q))2\left(\frac{pq}{4a} + 7a\right)^2 = 48a^2 + 3\left(\frac{1}{2}(p + q)\right)^2

M1

(pq+28a2)2=768a4+12a2(p+q)2(pq + 28a^2)^2 = 768a^4 + 12a^2(p + q)^2 p2q2+56a2pq+784a4=768a4+12a2(pq)2+48a2pqp^2q^2 + 56a^2pq + 784a^4 = 768a^4 + 12a^2(p - q)^2 + 48a^2pq

M1

p2q2+8a2pq+16a4=12a2(pq)2p^2q^2 + 8a^2pq + 16a^4 = 12a^2(p - q)^2

M1 A1

(pq+4a2)2=3(2a(pq))2(pq + 4a^2)^2 = 3(2a(p - q))^2

p2aq2a1+p2aq2a=±13\frac{\frac{p}{2a} - \frac{q}{2a}}{1 + \frac{p}{2a} \frac{q}{2a}} = \pm \frac{1}{\sqrt{3}}

M1 A1

Thus the tangents are at a constant angle to each other which is 3030^\circ. A1 (7)


Model Solution

Part (i)

Let the two lines make angles θ1\theta_1 and θ2\theta_2 with the positive xx-axis, where m1=tanθ1m_1 = \tan\theta_1 and m2=tanθ2m_2 = \tan\theta_2. The angle between the two lines is θ1θ2|\theta_1 - \theta_2|.

If the acute angle between the lines is 45°45°, then: θ1θ2=±45°orθ1θ2=±135°\theta_1 - \theta_2 = \pm 45° \quad \text{or} \quad \theta_1 - \theta_2 = \pm 135°

(since θ1θ2\theta_1 - \theta_2 and θ1θ2+180°\theta_1 - \theta_2 + 180° give the same pair of lines).

In all cases, tan(θ1θ2)=±1\tan(\theta_1 - \theta_2) = \pm 1 (as tan45°=1\tan 45° = 1 and tan135°=1\tan 135° = -1).

Using the tangent subtraction formula: tan(θ1θ2)=tanθ1tanθ21+tanθ1tanθ2=m1m21+m1m2\tan(\theta_1 - \theta_2) = \frac{\tan\theta_1 - \tan\theta_2}{1 + \tan\theta_1\tan\theta_2} = \frac{m_1 - m_2}{1 + m_1 m_2}

Therefore: m1m21+m1m2=±1\frac{m_1 - m_2}{1 + m_1 m_2} = \pm 1 \qquad \blacksquare


Part (ii)

The curve CC has equation 4ay=x24ay = x^2, so y=x24ay = \frac{x^2}{4a} and dydx=x2a\frac{dy}{dx} = \frac{x}{2a}.

The tangent at x=px = p passes through (p,p24a)\left(p, \frac{p^2}{4a}\right) with gradient p2a\frac{p}{2a}: yp24a=p2a(xp)y - \frac{p^2}{4a} = \frac{p}{2a}(x - p)

Multiply through by 4a4a: 4ayp2=2p(xp)=2px2p24ay - p^2 = 2p(x - p) = 2px - 2p^2 4ay=2pxp2()4ay = 2px - p^2 \qquad (\star)

Similarly, the tangent at x=qx = q: 4ay=2qxq2()4ay = 2qx - q^2 \qquad (\star\star)

Setting ()=()(\star) = (\star\star): 2pxp2=2qxq22px - p^2 = 2qx - q^2 2(pq)x=p2q2=(pq)(p+q)2(p - q)x = p^2 - q^2 = (p - q)(p + q)

Since pqp \neq q, divide by pqp - q: x=p+q2x = \frac{p + q}{2}

Substituting back into ()(\star): 4ay=2pp+q2p2=p2+pqp2=pq4ay = 2p \cdot \frac{p+q}{2} - p^2 = p^2 + pq - p^2 = pq y=pq4ay = \frac{pq}{4a}

So the tangents meet at (p+q2,pq4a)\left(\frac{p+q}{2},\, \frac{pq}{4a}\right).


Now suppose the two tangents are at 45°45° to each other. Their gradients are p2a\frac{p}{2a} and q2a\frac{q}{2a}, so by part (i): p2aq2a1+p2aq2a=±1\frac{\frac{p}{2a} - \frac{q}{2a}}{1 + \frac{p}{2a} \cdot \frac{q}{2a}} = \pm 1

pq2a4a2+pq4a2=±1\frac{\frac{p-q}{2a}}{\frac{4a^2 + pq}{4a^2}} = \pm 1

2a(pq)4a2+pq=±1\frac{2a(p-q)}{4a^2 + pq} = \pm 1

Squaring both sides: 4a2(pq)2=(4a2+pq)2()4a^2(p-q)^2 = (4a^2 + pq)^2 \qquad (\dagger)

Now express ()(\dagger) in terms of the meeting point. Let X=p+q2X = \frac{p+q}{2} and Y=pq4aY = \frac{pq}{4a}, so p+q=2Xp + q = 2X and pq=4aYpq = 4aY.

Then: (pq)2=(p+q)24pq=4X216aY(p-q)^2 = (p+q)^2 - 4pq = 4X^2 - 16aY

Substituting into ()(\dagger): 4a2(4X216aY)=(4a2+4aY)24a^2(4X^2 - 16aY) = (4a^2 + 4aY)^2

Divide by 16a216a^2: X24aY=(a+Y)2X^2 - 4aY = (a + Y)^2

X24aY=a2+2aY+Y2X^2 - 4aY = a^2 + 2aY + Y^2

X2=Y2+6aY+a2X^2 = Y^2 + 6aY + a^2

Adding 8a28a^2 to both sides: X2+8a2=Y2+6aY+9a2=(Y+3a)2X^2 + 8a^2 = Y^2 + 6aY + 9a^2 = (Y + 3a)^2

Therefore the meeting point (X,Y)(X, Y) satisfies (Y+3a)2=X2+8a2(Y + 3a)^2 = X^2 + 8a^2, i.e.:

(y+3a)2=x2+8a2(y + 3a)^2 = x^2 + 8a^2 \qquad \blacksquare


Part (iii)

The meeting point of tangents at x=px = p and x=qx = q is (p+q2,pq4a)\left(\frac{p+q}{2},\, \frac{pq}{4a}\right).

If this point lies on (y+7a)2=48a2+3x2(y + 7a)^2 = 48a^2 + 3x^2, then: (pq4a+7a)2=48a2+3(p+q2)2\left(\frac{pq}{4a} + 7a\right)^2 = 48a^2 + 3\left(\frac{p+q}{2}\right)^2

Multiply through by 16a216a^2: (pq+28a2)2=768a4+12a2(p+q)2(pq + 28a^2)^2 = 768a^4 + 12a^2(p+q)^2

Expand the left side: p2q2+56a2pq+784a4=768a4+12a2(p+q)2p^2q^2 + 56a^2 pq + 784a^4 = 768a^4 + 12a^2(p+q)^2

Use (p+q)2=(pq)2+4pq(p+q)^2 = (p-q)^2 + 4pq: p2q2+56a2pq+784a4=768a4+12a2(pq)2+48a2pqp^2q^2 + 56a^2 pq + 784a^4 = 768a^4 + 12a^2(p-q)^2 + 48a^2 pq

p2q2+8a2pq+16a4=12a2(pq)2p^2q^2 + 8a^2 pq + 16a^4 = 12a^2(p-q)^2

The left side factors: (pq+4a2)2=12a2(pq)2=3[2a(pq)]2(pq + 4a^2)^2 = 12a^2(p-q)^2 = 3 \cdot [2a(p-q)]^2

Taking square roots: pq+4a2=±2a(pq)3pq + 4a^2 = \pm 2a(p-q)\sqrt{3}

Now recall the tangent angle formula from part (i): m1m21+m1m2=p2aq2a1+pq4a2=2a(pq)4a2+pq\frac{m_1 - m_2}{1 + m_1 m_2} = \frac{\frac{p}{2a} - \frac{q}{2a}}{1 + \frac{pq}{4a^2}} = \frac{2a(p-q)}{4a^2 + pq}

From (pq+4a2)2=3[2a(pq)]2(pq + 4a^2)^2 = 3 \cdot [2a(p-q)]^2: (2a(pq)4a2+pq)2=4a2(pq)2(4a2+pq)2=4a2(pq)212a2(pq)2=13\left(\frac{2a(p-q)}{4a^2 + pq}\right)^2 = \frac{4a^2(p-q)^2}{(4a^2 + pq)^2} = \frac{4a^2(p-q)^2}{12a^2(p-q)^2} = \frac{1}{3}

Therefore: m1m21+m1m2=13=tan30°\left|\frac{m_1 - m_2}{1 + m_1 m_2}\right| = \frac{1}{\sqrt{3}} = \tan 30°

Since tanθ=13\tan\theta = \frac{1}{\sqrt{3}} gives θ=30°\theta = 30°, the acute angle between any two such tangents is 30°30°. \qquad \blacksquare

Examiner Notes

第四受欢迎题目,均分约10/20,第三成功。Part(i)需要完整论证:定义角度、考虑正切函数的周期性、讨论哪种情况对应锐角。Part(ii)中y坐标错误(代入抛物线方程而非切线方程)是常见失误。Part(iii)对多数考生有挑战性,不少人靠猜测30°/45°/60°作答。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

5 In this question, M and N are non-singular 2×22 \times 2 matrices.

The trace of the matrix M=(abcd)\mathbf{M} = \begin{pmatrix} a & b \\ c & d \end{pmatrix} is defined as tr(M)=a+d\text{tr}(\mathbf{M}) = a + d.

(i) Prove that, for any two matrices M and N, tr(MN)=tr(NM)\text{tr}(\mathbf{MN}) = \text{tr}(\mathbf{NM}) and derive an expression for tr(M+N)\text{tr}(\mathbf{M} + \mathbf{N}) in terms of tr(M)\text{tr}(\mathbf{M}) and tr(N)\text{tr}(\mathbf{N}).

The entries in matrix M are functions of tt and dMdt\frac{d\mathbf{M}}{dt} denotes the matrix whose entries are the derivatives of the corresponding entries in M.

(ii) Show that

1detMddt(detM)=tr(M1dMdt).\frac{1}{\det \mathbf{M}} \frac{d}{dt} (\det \mathbf{M}) = \text{tr} \left( \mathbf{M}^{-1} \frac{d\mathbf{M}}{dt} \right).

(iii) In this part, matrix M satisfies the differential equation

dMdt=MNNM,\frac{d\mathbf{M}}{dt} = \mathbf{MN} - \mathbf{NM},

where the entries in matrix N are also functions of tt.

Show that detM\det \mathbf{M}, tr(M)\text{tr}(\mathbf{M}) and tr(M2)\text{tr}(\mathbf{M}^2) are independent of tt.

In the case N=(tt0t)\mathbf{N} = \begin{pmatrix} t & t \\ 0 & t \end{pmatrix}, and given that M=(ABCD)\mathbf{M} = \begin{pmatrix} A & B \\ C & D \end{pmatrix} when t=0t = 0, find M as a function of tt.

(iv) In this part, matrix M satisfies the differential equation

dMdt=MN,\frac{d\mathbf{M}}{dt} = \mathbf{MN},

where the entries in matrix N are again functions of tt.

The trace of M is non-zero and independent of tt. Is it necessarily true that tr(N)=0\text{tr}(\mathbf{N}) = 0?

Hint

(i)

Let

N=(efgh)N = \begin{pmatrix} e & f \\ g & h \end{pmatrix} MN=(abcd)(efgh)=(ae+bgaf+bhce+dgcf+dh)MN = \begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} e & f \\ g & h \end{pmatrix} = \begin{pmatrix} ae + bg & af + bh \\ ce + dg & cf + dh \end{pmatrix} NM=(efgh)(abcd)=(ea+fceb+fdga+hcgb+hd)NM = \begin{pmatrix} e & f \\ g & h \end{pmatrix} \begin{pmatrix} a & b \\ c & d \end{pmatrix} = \begin{pmatrix} ea + fc & eb + fd \\ ga + hc & gb + hd \end{pmatrix} tr(MN)=ae+bg+cf+dh=ea+gb+fc+hdtr(MN) = ae + bg + cf + dh = ea + gb + fc + hd =ea+fc+gb+hd=tr(NM)= ea + fc + gb + hd = tr(NM)

M1A1

tr(M+N)=tr((abcd)+(efgh))=tr(a+eb+fc+gd+h)=a+e+d+htr(M + N) = tr \left( \begin{pmatrix} a & b \\ c & d \end{pmatrix} + \begin{pmatrix} e & f \\ g & h \end{pmatrix} \right) = tr \begin{pmatrix} a + e & b + f \\ c + g & d + h \end{pmatrix} = a + e + d + h =a+d+e+h=tr(M)+tr(N)= a + d + e + h = tr(M) + tr(N) B1 (3)

(ii) 1detMddt(detM)=1adbc×ddt(adbc)=1adbc×(a˙d+ad˙b˙cbc˙)\frac{1}{\det M} \frac{d}{dt} (\det M) = \frac{1}{ad - bc} \times \frac{d}{dt} (ad - bc) = \frac{1}{ad - bc} \times (\dot{a}d + a\dot{d} - \dot{b}c - b\dot{c})

M1

tr(M1dMdt)=tr(1adbc(dbca)(a˙b˙c˙d˙))=tr(1adbc(da˙bc˙db˙bd˙ca˙+ac˙cb˙+ad˙))tr \left( M^{-1} \frac{dM}{dt} \right) = tr \left( \frac{1}{ad - bc} \begin{pmatrix} d & -b \\ -c & a \end{pmatrix} \begin{pmatrix} \dot{a} & \dot{b} \\ \dot{c} & \dot{d} \end{pmatrix} \right) = tr \left( \frac{1}{ad - bc} \begin{pmatrix} d\dot{a} - b\dot{c} & d\dot{b} - b\dot{d} \\ -c\dot{a} + a\dot{c} & -c\dot{b} + a\dot{d} \end{pmatrix} \right) =1adbc×(da˙bc˙cb˙+ad˙)=1detMddt(detM)= \frac{1}{ad - bc} \times (d\dot{a} - b\dot{c} - c\dot{b} + a\dot{d}) = \frac{1}{\det M} \frac{d}{dt} (\det M) M1 *A1 (3)

(iii)

tr(M1dMdt)=tr(M1(MNNM))=tr(M1MNM1NM)=tr(N)tr(NMM1)=0tr \left( M^{-1} \frac{dM}{dt} \right) = tr(M^{-1}(MN - NM)) = tr(M^{-1}MN - M^{-1}NM) = tr(N) - tr(NMM^{-1}) = 0

Thus

1detMddt(detM)=0\frac{1}{\det M} \frac{d}{dt} (\det M) = 0

and so detM\det M is independent of tt

E1

ddt(tr(M))=tr(dMdt)=tr(MNNM)=tr(MN)tr(NM)=0\frac{d}{dt} (tr(M)) = tr \left( \frac{dM}{dt} \right) = tr(MN - NM) = tr(MN) - tr(NM) = 0

so tr(M)tr(M) is independent of tt

E1


tr(M2)=tr((abcd)(abcd))=tr(a2+bcab+bdac+cdbc+d2)=a2+bc+bc+d2tr(M^2) = tr \left( \begin{pmatrix} a & b \\ c & d \end{pmatrix} \begin{pmatrix} a & b \\ c & d \end{pmatrix} \right) = tr \begin{pmatrix} a^2 + bc & ab + bd \\ ac + cd & bc + d^2 \end{pmatrix} = a^2 + bc + bc + d^2 =a2+2ad+d2+2(bcad)=(a+d)22detM=(trM)22detM= a^2 + 2ad + d^2 + 2(bc - ad) = (a + d)^2 - 2 \det M = (tr M)^2 - 2 \det M M1 A1

Therefore

ddt(tr(M2))=ddt((trM)2)ddt(2detM)=0\frac{d}{dt}(tr(M^2)) = \frac{d}{dt}((tr M)^2) - \frac{d}{dt}(2 \det M) = 0

and so tr(M2)tr(M^2) is independent of t

E1 (5) dMdt=MNNM\frac{dM}{dt} = MN - NM

So

(A˙B˙C˙D˙)=(ABCD)(tt0t)(tt0t)(ABCD)=(CtAtDt0Ct)\begin{pmatrix} \dot{A} & \dot{B} \\ \dot{C} & \dot{D} \end{pmatrix} = \begin{pmatrix} A & B \\ C & D \end{pmatrix} \begin{pmatrix} t & t \\ 0 & t \end{pmatrix} - \begin{pmatrix} t & t \\ 0 & t \end{pmatrix} \begin{pmatrix} A & B \\ C & D \end{pmatrix} = \begin{pmatrix} -Ct & At - Dt \\ 0 & Ct \end{pmatrix}

M1 A1

Thus CC is a constant,

A1

A=a12Ct2,D=d+12Ct2A = a - \frac{1}{2}Ct^2, D = d + \frac{1}{2}Ct^2

A1

and as

B˙=AtDt=(ad)tCt3\dot{B} = At - Dt = (a - d)t - Ct^3

M1 B=b+12(ad)t214Ct4B = b + \frac{1}{2}(a - d)t^2 - \frac{1}{4}Ct^4 A1 (6)

(iv) If

dMdt=MN\frac{dM}{dt} = MN

Then for example,

M=(et1+etet1et),N=(1et01)M = \begin{pmatrix} e^t & 1 + e^t \\ e^t & 1 - e^t \end{pmatrix}, N = \begin{pmatrix} 1 & -e^{-t} \\ 0 & 1 \end{pmatrix}

dMdt=(etetetet)\frac{dM}{dt} = \begin{pmatrix} e^t & e^t \\ e^t & -e^t \end{pmatrix}

And

N=(et1+etet1et)(1et01)=(etetetet)N = \begin{pmatrix} e^t & 1 + e^t \\ e^t & 1 - e^t \end{pmatrix} \begin{pmatrix} 1 & -e^{-t} \\ 0 & 1 \end{pmatrix} = \begin{pmatrix} e^t & e^t \\ e^t & -e^t \end{pmatrix}

M1 A1

and

tr(N)=2tr(N) = 2

so no.

A1 (3)


Model Solution

Part (i)

Let M=(abcd)\mathbf{M} = \begin{pmatrix} a & b \\ c & d \end{pmatrix} and N=(efgh)\mathbf{N} = \begin{pmatrix} e & f \\ g & h \end{pmatrix}.

Computing the products:

MN=(ae+bgaf+bhce+dgcf+dh),NM=(ea+fceb+fdga+hcgb+hd)\mathbf{MN} = \begin{pmatrix} ae + bg & af + bh \\ ce + dg & cf + dh \end{pmatrix}, \qquad \mathbf{NM} = \begin{pmatrix} ea + fc & eb + fd \\ ga + hc & gb + hd \end{pmatrix}

Taking traces:

tr(MN)=ae+bg+cf+dh,tr(NM)=ea+fc+gb+hd\text{tr}(\mathbf{MN}) = ae + bg + cf + dh, \qquad \text{tr}(\mathbf{NM}) = ea + fc + gb + hd

Since scalar multiplication is commutative (ae=eaae = ea, bg=gbbg = gb, cf=fccf = fc, dh=hddh = hd), the two expressions are term-by-term equal, so

tr(MN)=tr(NM).\text{tr}(\mathbf{MN}) = \text{tr}(\mathbf{NM}).

For the trace of the sum:

M+N=(a+eb+fc+gd+h)\mathbf{M} + \mathbf{N} = \begin{pmatrix} a + e & b + f \\ c + g & d + h \end{pmatrix}

tr(M+N)=(a+e)+(d+h)=(a+d)+(e+h)=tr(M)+tr(N).\text{tr}(\mathbf{M} + \mathbf{N}) = (a + e) + (d + h) = (a + d) + (e + h) = \text{tr}(\mathbf{M}) + \text{tr}(\mathbf{N}).

Part (ii)

Let M=(abcd)\mathbf{M} = \begin{pmatrix} a & b \\ c & d \end{pmatrix} where a,b,c,da, b, c, d are functions of tt. Then detM=adbc\det \mathbf{M} = ad - bc, and by the product rule:

ddt(detM)=ddt(adbc)=a˙d+ad˙b˙cbc˙.(...)\frac{d}{dt}(\det \mathbf{M}) = \frac{d}{dt}(ad - bc) = \dot{a}d + a\dot{d} - \dot{b}c - b\dot{c}. \qquad \text{(...)}

We have M1=1adbc(dbca)\mathbf{M}^{-1} = \frac{1}{ad - bc}\begin{pmatrix} d & -b \\ -c & a \end{pmatrix} and dMdt=(a˙b˙c˙d˙)\frac{d\mathbf{M}}{dt} = \begin{pmatrix} \dot{a} & \dot{b} \\ \dot{c} & \dot{d} \end{pmatrix}, so

M1dMdt=1adbc(dbca)(a˙b˙c˙d˙)=1adbc(da˙bc˙db˙bd˙ca˙+ac˙cb˙+ad˙)\mathbf{M}^{-1}\frac{d\mathbf{M}}{dt} = \frac{1}{ad - bc}\begin{pmatrix} d & -b \\ -c & a \end{pmatrix}\begin{pmatrix} \dot{a} & \dot{b} \\ \dot{c} & \dot{d} \end{pmatrix} = \frac{1}{ad - bc}\begin{pmatrix} d\dot{a} - b\dot{c} & d\dot{b} - b\dot{d} \\ -c\dot{a} + a\dot{c} & -c\dot{b} + a\dot{d} \end{pmatrix}

Taking the trace (sum of diagonal entries):

tr(M1dMdt)=da˙bc˙cb˙+ad˙adbc=a˙d+ad˙b˙cbc˙adbc\text{tr}\left(\mathbf{M}^{-1}\frac{d\mathbf{M}}{dt}\right) = \frac{d\dot{a} - b\dot{c} - c\dot{b} + a\dot{d}}{ad - bc} = \frac{\dot{a}d + a\dot{d} - \dot{b}c - b\dot{c}}{ad - bc}

The numerator is identical to (…), so

1detMddt(detM)=tr(M1dMdt).\frac{1}{\det \mathbf{M}}\frac{d}{dt}(\det \mathbf{M}) = \text{tr}\left(\mathbf{M}^{-1}\frac{d\mathbf{M}}{dt}\right).

Part (iii)

Given dMdt=MNNM\frac{d\mathbf{M}}{dt} = \mathbf{MN} - \mathbf{NM}.

det M: Using part (ii),

1detMddt(detM)=tr(M1(MNNM))=tr(N)tr(M1NM).\frac{1}{\det \mathbf{M}}\frac{d}{dt}(\det \mathbf{M}) = \text{tr}\left(\mathbf{M}^{-1}(\mathbf{MN} - \mathbf{NM})\right) = \text{tr}(\mathbf{N}) - \text{tr}(\mathbf{M}^{-1}\mathbf{NM}).

Setting X=M\mathbf{X} = \mathbf{M} and Y=M1N\mathbf{Y} = \mathbf{M}^{-1}\mathbf{N} in tr(XY)=tr(YX)\text{tr}(\mathbf{XY}) = \text{tr}(\mathbf{YX}):

tr(MM1N)=tr(M1NM)\text{tr}(\mathbf{M} \cdot \mathbf{M}^{-1}\mathbf{N}) = \text{tr}(\mathbf{M}^{-1}\mathbf{N} \cdot \mathbf{M})

tr(N)=tr(M1NM).\text{tr}(\mathbf{N}) = \text{tr}(\mathbf{M}^{-1}\mathbf{NM}).

So 1detMddt(detM)=tr(N)tr(N)=0\frac{1}{\det \mathbf{M}}\frac{d}{dt}(\det \mathbf{M}) = \text{tr}(\mathbf{N}) - \text{tr}(\mathbf{N}) = 0, hence detM\det \mathbf{M} is independent of tt.

tr(M): The derivative of the trace is the trace of the derivative (since differentiation acts entry-wise):

ddttr(M)=tr(dMdt)=tr(MNNM)=tr(MN)tr(NM)=0\frac{d}{dt}\text{tr}(\mathbf{M}) = \text{tr}\left(\frac{d\mathbf{M}}{dt}\right) = \text{tr}(\mathbf{MN} - \mathbf{NM}) = \text{tr}(\mathbf{MN}) - \text{tr}(\mathbf{NM}) = 0

by part (i). Hence tr(M)\text{tr}(\mathbf{M}) is independent of tt.

tr(M²): For M=(abcd)\mathbf{M} = \begin{pmatrix} a & b \\ c & d \end{pmatrix}:

M2=(a2+bcab+bdac+cdbc+d2),tr(M2)=a2+2bc+d2\mathbf{M}^2 = \begin{pmatrix} a^2 + bc & ab + bd \\ ac + cd & bc + d^2 \end{pmatrix}, \qquad \text{tr}(\mathbf{M}^2) = a^2 + 2bc + d^2

We also compute:

(trM)22detM=(a+d)22(adbc)=a2+2ad+d22ad+2bc=a2+2bc+d2=tr(M2)(\text{tr}\,\mathbf{M})^2 - 2\det \mathbf{M} = (a + d)^2 - 2(ad - bc) = a^2 + 2ad + d^2 - 2ad + 2bc = a^2 + 2bc + d^2 = \text{tr}(\mathbf{M}^2)

So tr(M2)=(trM)22detM\text{tr}(\mathbf{M}^2) = (\text{tr}\,\mathbf{M})^2 - 2\det \mathbf{M}. Since both tr(M)\text{tr}(\mathbf{M}) and detM\det \mathbf{M} are independent of tt, so is tr(M2)\text{tr}(\mathbf{M}^2).

Finding M(t): With N=(tt0t)\mathbf{N} = \begin{pmatrix} t & t \\ 0 & t \end{pmatrix} and M=(abcd)\mathbf{M} = \begin{pmatrix} a & b \\ c & d \end{pmatrix}:

MN=(at(a+b)tct(c+d)t),NM=((a+c)t(b+d)tctdt)\mathbf{MN} = \begin{pmatrix} at & (a + b)t \\ ct & (c + d)t \end{pmatrix}, \qquad \mathbf{NM} = \begin{pmatrix} (a + c)t & (b + d)t \\ ct & dt \end{pmatrix}

dMdt=MNNM=(ct(ad)t0ct)\frac{d\mathbf{M}}{dt} = \mathbf{MN} - \mathbf{NM} = \begin{pmatrix} -ct & (a - d)t \\ 0 & ct \end{pmatrix}

Reading off each entry of dMdt\frac{d\mathbf{M}}{dt}:

c˙=0\dot{c} = 0: so c=Cc = C (constant, equal to its initial value at t=0t = 0).

a˙=Ct\dot{a} = -Ct: integrating, a=A12Ct2a = A - \frac{1}{2}Ct^2.

d˙=Ct\dot{d} = Ct: integrating, d=D+12Ct2d = D + \frac{1}{2}Ct^2.

b˙=(ad)t\dot{b} = (a - d)t: substituting the expressions for aa and dd:

b˙=((A12Ct2)(D+12Ct2))t=(AD)tCt3\dot{b} = \left(\left(A - \tfrac{1}{2}Ct^2\right) - \left(D + \tfrac{1}{2}Ct^2\right)\right)t = (A - D)t - Ct^3

Integrating: b=B+12(AD)t214Ct4b = B + \frac{1}{2}(A - D)t^2 - \frac{1}{4}Ct^4.

Therefore

M(t)=(A12Ct2B+12(AD)t214Ct4CD+12Ct2).\mathbf{M}(t) = \begin{pmatrix} A - \frac{1}{2}Ct^2 & B + \frac{1}{2}(A - D)t^2 - \frac{1}{4}Ct^4 \\[6pt] C & D + \frac{1}{2}Ct^2 \end{pmatrix}.

Part (iv)

No. We construct a counterexample.

Let N=(1et01)\mathbf{N} = \begin{pmatrix} 1 & -e^{-t} \\ 0 & 1 \end{pmatrix} and M=(et1+etet1et)\mathbf{M} = \begin{pmatrix} e^t & 1 + e^t \\ e^t & 1 - e^t \end{pmatrix}.

First, both matrices are non-singular: detM=et(1et)(1+et)et=2e2t0\det \mathbf{M} = e^t(1 - e^t) - (1 + e^t)e^t = -2e^{2t} \neq 0 and detN=10\det \mathbf{N} = 1 \neq 0.

We have tr(M)=et+1et=1\text{tr}(\mathbf{M}) = e^t + 1 - e^t = 1, which is non-zero and independent of tt.

We verify dMdt=MN\frac{d\mathbf{M}}{dt} = \mathbf{MN}:

dMdt=(etetetet)\frac{d\mathbf{M}}{dt} = \begin{pmatrix} e^t & e^t \\ e^t & -e^t \end{pmatrix}

MN=(et1+etet1et)(1et01)=(et1+1+etet1+1et)=(etetetet)\mathbf{MN} = \begin{pmatrix} e^t & 1 + e^t \\ e^t & 1 - e^t \end{pmatrix}\begin{pmatrix} 1 & -e^{-t} \\ 0 & 1 \end{pmatrix} = \begin{pmatrix} e^t & -1 + 1 + e^t \\ e^t & -1 + 1 - e^t \end{pmatrix} = \begin{pmatrix} e^t & e^t \\ e^t & -e^t \end{pmatrix}

Since dMdt=MN\frac{d\mathbf{M}}{dt} = \mathbf{MN}, all conditions of the problem are satisfied. But tr(N)=1+1=20\text{tr}(\mathbf{N}) = 1 + 1 = 2 \neq 0, so it is not necessarily true that tr(N)=0\text{tr}(\mathbf{N}) = 0.

Examiner Notes

均分约8/20。Part(i)很直接但部分考生遗漏tr(M+N)的结果。Part(iii)常见错误:忽略矩阵乘法的非交换性、将A/B/C/D视为常数、对标量链规则直接应用于M²。Part(iv)需要构造反例,仅6人满分——多数考生要么未能给出满足所有条件的反例,要么错误地试图证明命题成立。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

6 (i) A particle moves in two-dimensional space. Its position is given by coordinates (x,y)(x, y) which satisfy

dxdt=x+3y+udydt=x+y+u\begin{aligned} \frac{dx}{dt} &= -x + 3y + u \\ \frac{dy}{dt} &= x + y + u \end{aligned}

where tt is the time and uu is a function of time. At time t=0t = 0, the particle has position (x0,y0)(x_0, y_0).

(a) By considering dxdtdydt\frac{dx}{dt} - \frac{dy}{dt}, show that if the particle is at the origin (0,0)(0, 0) at some time t>0t > 0, then it is necessary that x0=y0x_0 = y_0.

(b) Given that x0=y0x_0 = y_0, find a constant value of uu that ensures that the particle is at the origin at a time t=Tt = T, where T>0T > 0.

(ii) A particle whose position in three-dimensional space is given by co-ordinates (x,y,z)(x, y, z) moves with time tt such that

dxdt=4y5z+udydt=x2z+udzdt=x2y+u\begin{aligned} \frac{dx}{dt} &= 4y - 5z + u \\ \frac{dy}{dt} &= x - 2z + u \\ \frac{dz}{dt} &= x - 2y + u \end{aligned}

where uu is a function of time. At time t=0t = 0, the particle has position (x0,y0,z0)(x_0, y_0, z_0).

(a) Show that, if the particle is at the origin (0,0,0)(0, 0, 0) at some time t>0t > 0, it is necessary that y0y_0 is the mean of x0x_0 and z0z_0.

(b) Show further that, if the particle is at the origin (0,0,0)(0, 0, 0) at some time t>0t > 0, it is necessary that x0=y0=z0x_0 = y_0 = z_0.

(c) Given that x0=y0=z0x_0 = y_0 = z_0, find a constant value of uu that ensures that the particle is at the origin at a time t=Tt = T, where T>0T > 0.

Hint

(i) (a)**

dxdt=x+3y+u\frac{dx}{dt} = -x + 3y + u

dydt=x+y+u\frac{dy}{dt} = x + y + u dxdtdydt=d(xy)dt=2(xy)\frac{dx}{dt} - \frac{dy}{dt} = \frac{d(x - y)}{dt} = -2(x - y)

M1

xy=Ae2tx - y = Ae^{-2t}

A1

If x=y=0x = y = 0 at some time t>0t > 0, then A=0A = 0, [A1]

so considering t=0t = 0, x0y0=0x_0 - y_0 = 0 which gives the required result. [E1 (4)]

(b) If x0=y0x_0 = y_0, then at t=0t = 0, xy=0x - y = 0 so A=0A = 0 and hence x=yx = y for all tt

E1

Thus

dxdt=2x+u\frac{dx}{dt} = 2x + u

dxdt2x=u\frac{dx}{dt} - 2x = u

e2tdxdt2e2tx=e2tue^{-2t} \frac{dx}{dt} - 2e^{-2t}x = e^{-2t}u

M1 A1

t=0t = 0, x=x0x = x_0 so x0=12u+cx_0 = -\frac{1}{2}u + c and we want x=0x = 0 when t=Tt = T

so

0=12u+ce2T0 = -\frac{1}{2}u + ce^{2T}

Thus c=12ue2Tc = \frac{1}{2}ue^{-2T}, x0=12u+12ue2Tx_0 = -\frac{1}{2}u + \frac{1}{2}ue^{-2T}

and hence,

u=2x0e2T1e2Tu = \frac{2x_0 e^{2T}}{1 - e^{2T}}

dM1 A1 (5)


(ii) (a)

dxdt2dydt+dzdt=d(x2y+z)dt=(x2y+z)\frac{dx}{dt} - 2\frac{dy}{dt} + \frac{dz}{dt} = \frac{d(x - 2y + z)}{dt} = -(x - 2y + z)

Thus

x2y+z=Aetx - 2y + z = Ae^{-t}

M1 A1

If x=y=z=0x = y = z = 0 at some time t>0t > 0, then A=0A = 0, so considering t=0t = 0, x02y0+z0=0x_0 - 2y_0 + z_0 = 0 which gives the required result. E1 (3)

(b) we know from (a) that if x=y=z=0x = y = z = 0 at some time t>0t > 0, then A=0A = 0, and so

x2y+z=0x - 2y + z = 0 or 2y=x+z2y = x + z E1

Thus

dxdt=2x3z+u\frac{dx}{dt} = 2x - 3z + u

and

dzdt=z+u\frac{dz}{dt} = -z + u

So

dxdtdzdt=ddt(xz)=2(xz)\frac{dx}{dt} - \frac{dz}{dt} = \frac{d}{dt}(x - z) = 2(x - z)

and so

xz=Be2tx - z = Be^{2t}

M1 A1

But as x=z=0x = z = 0 at some time t>0t > 0, B=0B = 0 and so x=zx = z for all tt

and thus x=y=zx = y = z for all tt

Hence

x0=y0=z0x_0 = y_0 = z_0

E1 (4)


(c)

Given x0=y0=z0x_0 = y_0 = z_0 we know that (a) and (b) apply (as similarly in (i)), so dzdt=z+u\frac{dz}{dt} = -z + u

M1

Thus z=u+cetz = u + ce^{-t}

A1

t=0t = 0 , z=z0z = z_0 so z0=u+cz_0 = u + c and 0=u+ceT0 = u + ce^{-T}

dM1

c=ueTc = -ue^T

u=z01eTu = \frac{z_0}{1 - e^T}

A1 (4)


Model Solution

Part (i)(a)

Subtracting the two equations:

dxdtdydt=(x+3y+u)(x+y+u)=2x+2y=2(xy)\frac{dx}{dt} - \frac{dy}{dt} = (-x + 3y + u) - (x + y + u) = -2x + 2y = -2(x - y)

So ddt(xy)=2(xy)\frac{d}{dt}(x - y) = -2(x - y), which is a separable ODE with solution

xy=Ae2tx - y = Ae^{-2t}

where AA is a constant. At t=0t = 0: A=x0y0A = x_0 - y_0.

If the particle is at the origin at some time t>0t > 0, then x=y=0x = y = 0 at that time, so xy=0x - y = 0, giving Ae2t=0Ae^{-2t} = 0. Since e2t0e^{-2t} \neq 0 for all tt, we must have A=0A = 0, hence x0=y0x_0 = y_0.

Part (i)(b)

Given x0=y0x_0 = y_0, we have A=0A = 0, so x=yx = y for all t0t \geq 0.

Substituting y=xy = x into dxdt=x+3y+u\frac{dx}{dt} = -x + 3y + u:

dxdt=x+3x+u=2x+u\frac{dx}{dt} = -x + 3x + u = 2x + u

Rearranging: dxdt2x=u\frac{dx}{dt} - 2x = u. Multiplying both sides by the integrating factor e2te^{-2t}:

ddt(xe2t)=ue2t\frac{d}{dt}\left(xe^{-2t}\right) = ue^{-2t}

Integrating:

xe2t=u2e2t+Kxe^{-2t} = -\frac{u}{2}e^{-2t} + K

where KK is a constant of integration. At t=0t = 0: x0=u2+Kx_0 = -\frac{u}{2} + K, so K=x0+u2K = x_0 + \frac{u}{2}.

Thus

x=u2+(x0+u2)e2tx = -\frac{u}{2} + \left(x_0 + \frac{u}{2}\right)e^{2t}

Setting x=0x = 0 at t=Tt = T:

0=u2+(x0+u2)e2T0 = -\frac{u}{2} + \left(x_0 + \frac{u}{2}\right)e^{2T}

u2=(x0+u2)e2T\frac{u}{2} = \left(x_0 + \frac{u}{2}\right)e^{2T}

u2(1e2T)=x0e2T\frac{u}{2}\left(1 - e^{2T}\right) = x_0 e^{2T}

u=2x0e2T1e2Tu = \frac{2x_0 e^{2T}}{1 - e^{2T}}

Part (ii)(a)

Consider dxdt2dydt+dzdt\frac{dx}{dt} - 2\frac{dy}{dt} + \frac{dz}{dt}:

=(4y5z+u)2(x2z+u)+(x2y+u)= (4y - 5z + u) - 2(x - 2z + u) + (x - 2y + u)

=4y5z+u2x+4z2u+x2y+u= 4y - 5z + u - 2x + 4z - 2u + x - 2y + u

=x+2yz=(x2y+z)= -x + 2y - z = -(x - 2y + z)

So ddt(x2y+z)=(x2y+z)\frac{d}{dt}(x - 2y + z) = -(x - 2y + z), giving x2y+z=Aetx - 2y + z = Ae^{-t}.

At t=0t = 0: A=x02y0+z0A = x_0 - 2y_0 + z_0.

If the particle is at the origin at some t>0t > 0, then x=y=z=0x = y = z = 0, so Aet=0Ae^{-t} = 0, hence A=0A = 0, giving x02y0+z0=0x_0 - 2y_0 + z_0 = 0, i.e., y0=x0+z02y_0 = \frac{x_0 + z_0}{2}.

Part (ii)(b)

From part (a), x2y+z=0x - 2y + z = 0 for all tt, so 2y=x+z2y = x + z.

Substituting y=x+z2y = \frac{x + z}{2} into the first and third equations:

dxdt=4x+z25z+u=2x+2z5z+u=2x3z+u\frac{dx}{dt} = 4 \cdot \frac{x + z}{2} - 5z + u = 2x + 2z - 5z + u = 2x - 3z + u

dzdt=x2x+z2+u=xxz+u=z+u\frac{dz}{dt} = x - 2 \cdot \frac{x + z}{2} + u = x - x - z + u = -z + u

Subtracting:

dxdtdzdt=(2x3z+u)(z+u)=2x2z=2(xz)\frac{dx}{dt} - \frac{dz}{dt} = (2x - 3z + u) - (-z + u) = 2x - 2z = 2(x - z)

So ddt(xz)=2(xz)\frac{d}{dt}(x - z) = 2(x - z), giving xz=Be2tx - z = Be^{2t}.

At t=0t = 0: B=x0z0B = x_0 - z_0.

If x=z=0x = z = 0 at some t>0t > 0, then Be2t=0Be^{2t} = 0. Since e2t0e^{2t} \neq 0, we need B=0B = 0, hence x0=z0x_0 = z_0.

Combined with y0=x0+z02=x0+x02=x0y_0 = \frac{x_0 + z_0}{2} = \frac{x_0 + x_0}{2} = x_0, we conclude x0=y0=z0x_0 = y_0 = z_0.

Part (ii)(c)

Given x0=y0=z0x_0 = y_0 = z_0, from parts (a) and (b) we have x2y+z=0x - 2y + z = 0 and xz=0x - z = 0 for all tt. So x=zx = z and 2y=x+z=2x2y = x + z = 2x, giving y=x=zy = x = z for all tt.

From dzdt=z+u\frac{dz}{dt} = -z + u:

dzdt+z=u\frac{dz}{dt} + z = u

Multiplying by the integrating factor ete^t:

ddt(zet)=uet\frac{d}{dt}\left(ze^t\right) = ue^t

Integrating: zet=uet+Kze^t = ue^t + K.

At t=0t = 0: z0=u+Kz_0 = u + K, so K=z0uK = z_0 - u.

Thus z=u+(z0u)etz = u + (z_0 - u)e^{-t}.

Setting z=0z = 0 at t=Tt = T:

0=u+(z0u)eT0 = u + (z_0 - u)e^{-T}

uueT=z0eTu - ue^{-T} = -z_0 e^{-T}

u(1eT)=z0eTu(1 - e^{-T}) = -z_0 e^{-T}

u=z0eT1eTu = \frac{-z_0 e^{-T}}{1 - e^{-T}}

Multiplying numerator and denominator by eTe^T:

u=z01eTu = \frac{z_0}{1 - e^T}

Examiner Notes

纯数部分最不受欢迎且得分最低。考官报告:成功考生通常将方程改写为d(x-y)/dt=-2(x-y);也有考生用积分因子法。常见错误:将x=y=0代入微分方程后积分(混淆了条件);正确得出x=y但未说明这蕴含x₀=y₀。Part(ii)中巧妙组合后两个方程得出y=z再推x=z的方法值得学习。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

7 In this question, you need not consider issues of convergence.

For positive integer nn let

f(n)=1n+1+1(n+1)(n+2)+1(n+1)(n+2)(n+3)+f(n) = \frac{1}{n + 1} + \frac{1}{(n + 1)(n + 2)} + \frac{1}{(n + 1)(n + 2)(n + 3)} + \dots

and

g(n)=1n+11(n+1)(n+2)+1(n+1)(n+2)(n+3)g(n) = \frac{1}{n + 1} - \frac{1}{(n + 1)(n + 2)} + \frac{1}{(n + 1)(n + 2)(n + 3)} - \dots

(i) Show, by considering a geometric series, that 0<f(n)<1n0 < f(n) < \frac{1}{n}.

(ii) Show, by comparing consecutive terms, that 0<g(n)<1n+10 < g(n) < \frac{1}{n + 1}.

(iii) Show, for positive integer nn, that (2n)!ef(2n)(2n)! e - f(2n) and (2n)!e+g(2n)\frac{(2n)!}{e} + g(2n) are both integers.

(iv) Show that if qe=peqe = \frac{p}{e} for some positive integers pp and qq, then qf(2n)+pg(2n)qf(2n) + pg(2n) is an integer for all positive integers nn.

(v) Hence show that the number e2e^2 is irrational.

Hint

(i)** Each term of f(n)>0f(n) > 0 so their sum is too.

[E1]

1(n+1)(n+2)...(n+r)<1(n+1)r\frac{1}{(n+1)(n+2)...(n+r)} < \frac{1}{(n+1)^r} so f(n)=1n+1+1(n+1)(n+2)+<1n+1+1(n+1)2+=1/n+111/n+1=1nf(n) = \frac{1}{n+1} + \frac{1}{(n+1)(n+2)} + \dots < \frac{1}{n+1} + \frac{1}{(n+1)^2} + \dots = \frac{1/n+1}{1-1/n+1} = \frac{1}{n}

[M1 A1(3)]

Thus 0<f(n)<1n0 < f(n) < \frac{1}{n}

(ii) 1n+11(n+1)(n+2)>0\frac{1}{n+1} - \frac{1}{(n+1)(n+2)} > 0, 1(n+1)(n+2)(n+3)1(n+1)(n+2)(n+3)(n+4)>0\frac{1}{(n+1)(n+2)(n+3)} - \frac{1}{(n+1)(n+2)(n+3)(n+4)} > 0, etc so g(n)>0g(n) > 0

[M1 A1]

Also, 1(n+1)(n+2)1(n+1)(n+2)(n+3)>0\frac{1}{(n+1)(n+2)} - \frac{1}{(n+1)(n+2)(n+3)} > 0, 1(n+1)(n+2)(n+3)(n+4)1(n+1)(n+2)(n+3)(n+4)(n+5)>0\frac{1}{(n+1)(n+2)(n+3)(n+4)} - \frac{1}{(n+1)(n+2)(n+3)(n+4)(n+5)} > 0, etc

so g(n)=1n+1a sum of positive terms<1n+1g(n) = \frac{1}{n+1} - \text{a sum of positive terms} < \frac{1}{n+1}

[M1 A1 (4)]

Thus 0<g(n)<1n+10 < g(n) < \frac{1}{n+1}

(iii)

(2n)!ef(2n)(2n)! e - f(2n) =(2n)!(1+1+12!+13!+)12n+11(2n+1)(2n+2)1(2n+1)(2n+2)(2n+3)= (2n)! \left( 1 + 1 + \frac{1}{2!} + \frac{1}{3!} + \dots \right) - \frac{1}{2n+1} - \frac{1}{(2n+1)(2n+2)} - \frac{1}{(2n+1)(2n+2)(2n+3)} - \dots

[M1 A1]

=(2n)!(1+1+12!++1(2n)!)= (2n)! \left( 1 + 1 + \frac{1}{2!} + \dots + \frac{1}{(2n)!} \right) +(2n)!(2n+1)!+(2n)!(2n+2)!+12n+11(2n+1)(2n+2)1(2n+1)(2n+2)(2n+3)+ \frac{(2n)!}{(2n+1)!} + \frac{(2n)!}{(2n+2)!} + \dots - \frac{1}{2n+1} - \frac{1}{(2n+1)(2n+2)} - \frac{1}{(2n+1)(2n+2)(2n+3)} - \dots =(2n)!(1+1+12!++1(2n)!)= (2n)! \left( 1 + 1 + \frac{1}{2!} + \dots + \frac{1}{(2n)!} \right)

which is an integer. [M1 A1(4)]


(2n)!e+g(2n)=(2n)!e1+g(2n)\frac{(2n)!}{e} + g(2n) = (2n)! e^{-1} + g(2n) =(2n)!(11+12!13!+)+12n+11(2n+1)(2n+2)+1(2n+1)(2n+2)(2n+3)= (2n)! \left( 1 - 1 + \frac{1}{2!} - \frac{1}{3!} + \cdots \right) + \frac{1}{2n+1} - \frac{1}{(2n+1)(2n+2)} + \frac{1}{(2n+1)(2n+2)(2n+3)} - \cdots

M1 A1

=(2n)!(11+12!++1(2n)!)= (2n)! \left( 1 - 1 + \frac{1}{2!} + \cdots + \frac{1}{(2n)!} \right) (2n)!(2n+1)!+(2n)!(2n+2)!+12n+11(2n+1)(2n+2)+1(2n+1)(2n+2)(2n+3)- \frac{(2n)!}{(2n+1)!} + \frac{(2n)!}{(2n+2)!} - \cdots + \frac{1}{2n+1} - \frac{1}{(2n+1)(2n+2)} + \frac{1}{(2n+1)(2n+2)(2n+3)} - \cdots =(2n)!(11+12!++1(2n)!)= (2n)! \left( 1 - 1 + \frac{1}{2!} + \cdots + \frac{1}{(2n)!} \right)

M1 A1 (4)

which is an integer.

(iv) q((2n)!ef(2n))q((2n)! e - f(2n)) is an integer as is p((2n)!e+g(2n))p \left( \frac{(2n)!}{e} + g(2n) \right)

Thus (p((2n)!e+g(2n)))(q((2n)!ef(2n)))\left( p \left( \frac{(2n)!}{e} + g(2n) \right) \right) - (q((2n)! e - f(2n))) is an integer.

(p((2n)!e+g(2n)))(q((2n)!ef(2n)))=(2n)!(peqe)+pg(2n)+qf(2n)\left( p \left( \frac{(2n)!}{e} + g(2n) \right) \right) - (q((2n)! e - f(2n))) = (2n)! \left( \frac{p}{e} - qe \right) + pg(2n) + qf(2n)

M1

=pg(2n)+qf(2n)= pg(2n) + qf(2n)

so pg(2n)+qf(2n)pg(2n) + qf(2n) is an integer as required. A1(2)

(v) As (iv) is true for all positive integers nn, it must be true for n=max(p,q)n = \max(p, q)

By (ii) pg(2n)<p2n+1n2n+1<12pg(2n) < \frac{p}{2n+1} \leq \frac{n}{2n+1} < \frac{1}{2}

By (i) qf(2n)<q2nn2n=12qf(2n) < \frac{q}{2n} \leq \frac{n}{2n} = \frac{1}{2}

M1

Therefore, pg(2n)+qf(2n)<12+12=1pg(2n) + qf(2n) < \frac{1}{2} + \frac{1}{2} = 1

and trivially by (i) and (ii)

pg(2n)+qf(2n)>0pg(2n) + qf(2n) > 0

A1

This means that pg(2n)+qf(2n)pg(2n) + qf(2n) cannot be an integer which contradicts the result of (iv)

and hence there are no integers such that pe=qe\frac{p}{e} = qe, that is such that pq=e2\frac{p}{q} = e^2 and so e2e^2 is irrational. E1 (3)


Model Solution

Part (i)

Each term of f(n)f(n) is positive (since nn is a positive integer), so f(n)>0f(n) > 0.

For the upper bound, observe that for r1r \geq 1:

(n+1)(n+2)(n+r)(n+1)r(n + 1)(n + 2) \cdots (n + r) \geq (n + 1)^r

since each factor n+kn+1n + k \geq n + 1 for k=1,2,,rk = 1, 2, \ldots, r, with strict inequality for r2r \geq 2. Therefore:

1(n+1)(n+2)(n+r)1(n+1)r\frac{1}{(n + 1)(n + 2) \cdots (n + r)} \leq \frac{1}{(n + 1)^r}

with strict inequality for r2r \geq 2. Summing over all terms:

f(n)=r=11(n+1)(n+2)(n+r)<r=11(n+1)rf(n) = \sum_{r=1}^{\infty} \frac{1}{(n+1)(n+2)\cdots(n+r)} < \sum_{r=1}^{\infty} \frac{1}{(n+1)^r}

The right-hand side is a geometric series with first term 1n+1\frac{1}{n+1} and common ratio 1n+1\frac{1}{n+1}:

r=11(n+1)r=1n+111n+1=1n+1nn+1=1n\sum_{r=1}^{\infty} \frac{1}{(n+1)^r} = \frac{\frac{1}{n+1}}{1 - \frac{1}{n+1}} = \frac{\frac{1}{n+1}}{\frac{n}{n+1}} = \frac{1}{n}

Therefore 0<f(n)<1n0 < f(n) < \frac{1}{n}. \qquad \blacksquare


Part (ii)

Write g(n)=T1T2+T3T4+g(n) = T_1 - T_2 + T_3 - T_4 + \cdots where

Tr=1(n+1)(n+2)(n+r)T_r = \frac{1}{(n+1)(n+2)\cdots(n+r)}

Showing g(n)>0g(n) > 0: Group consecutive pairs from the start:

g(n)=(T1T2)+(T3T4)+(T5T6)+g(n) = (T_1 - T_2) + (T_3 - T_4) + (T_5 - T_6) + \cdots

Each pair is positive since Tr>Tr+1T_r > T_{r+1} (each Tr+1T_{r+1} is TrT_r multiplied by 1n+r+1<1\frac{1}{n+r+1} < 1). A sum of positive terms is positive, so g(n)>0g(n) > 0.

Showing g(n)<1n+1g(n) < \frac{1}{n+1}: Group differently by taking the first term and pairing the rest:

g(n)=T1(T2T3)(T4T5)g(n) = T_1 - (T_2 - T_3) - (T_4 - T_5) - \cdots

Each bracketed pair is positive (again since Tr>Tr+1T_r > T_{r+1}). Therefore g(n)=T1(positive terms)<T1=1n+1g(n) = T_1 - (\text{positive terms}) < T_1 = \frac{1}{n+1}.

Therefore 0<g(n)<1n+10 < g(n) < \frac{1}{n+1}. \qquad \blacksquare


Part (iii)

Using e=k=01k!e = \sum_{k=0}^{\infty} \frac{1}{k!}:

(2n)!e=(2n)!(1+1+12!+13!+)(2n)!\, e = (2n)! \left(1 + 1 + \frac{1}{2!} + \frac{1}{3!} + \cdots \right)

Split this into two parts: terms up to k=2nk = 2n and terms for k>2nk > 2n:

(2n)!e=k=02n(2n)!k!integer+k=2n+1(2n)!k!(2n)!\, e = \underbrace{\sum_{k=0}^{2n} \frac{(2n)!}{k!}}_{\text{integer}} + \sum_{k=2n+1}^{\infty} \frac{(2n)!}{k!}

The first sum is an integer since (2n)!k!\frac{(2n)!}{k!} is an integer for 0k2n0 \leq k \leq 2n. For the second sum, substitute k=2n+rk = 2n + r with r1r \geq 1:

k=2n+1(2n)!k!=r=1(2n)!(2n+r)!=r=11(2n+1)(2n+2)(2n+r)=f(2n)\sum_{k=2n+1}^{\infty} \frac{(2n)!}{k!} = \sum_{r=1}^{\infty} \frac{(2n)!}{(2n+r)!} = \sum_{r=1}^{\infty} \frac{1}{(2n+1)(2n+2)\cdots(2n+r)} = f(2n)

Therefore (2n)!e=integer+f(2n)(2n)!\, e = \text{integer} + f(2n), which gives:

(2n)!ef(2n)=integer(2n)!\, e - f(2n) = \text{integer} \qquad \blacksquare

For the second expression, use e1=k=0(1)kk!e^{-1} = \sum_{k=0}^{\infty} \frac{(-1)^k}{k!}:

(2n)!e=(2n)!(11+12!13!+)\frac{(2n)!}{e} = (2n)! \left(1 - 1 + \frac{1}{2!} - \frac{1}{3!} + \cdots \right)

Split into terms up to k=2nk = 2n and terms for k>2nk > 2n:

(2n)!e=k=02n(1)k(2n)!k!integer+k=2n+1(1)k(2n)!k!\frac{(2n)!}{e} = \underbrace{\sum_{k=0}^{2n} \frac{(-1)^k (2n)!}{k!}}_{\text{integer}} + \sum_{k=2n+1}^{\infty} \frac{(-1)^k (2n)!}{k!}

The first sum is again an integer. For the second sum, with k=2n+rk = 2n + r, r1r \geq 1:

k=2n+1(1)k(2n)!k!=r=1(1)2n+r(2n+1)(2n+2)(2n+r)=r=1(1)r(2n+1)(2n+2)(2n+r)=g(2n)\sum_{k=2n+1}^{\infty} \frac{(-1)^k (2n)!}{k!} = \sum_{r=1}^{\infty} \frac{(-1)^{2n+r}}{(2n+1)(2n+2)\cdots(2n+r)} = \sum_{r=1}^{\infty} \frac{(-1)^r}{(2n+1)(2n+2)\cdots(2n+r)} = -g(2n)

since (1)2n=1(-1)^{2n} = 1. Therefore:

(2n)!e=integerg(2n)\frac{(2n)!}{e} = \text{integer} - g(2n)

which gives:

(2n)!e+g(2n)=integer\frac{(2n)!}{e} + g(2n) = \text{integer} \qquad \blacksquare

Part (iv)

From part (iii), both (2n)!ef(2n)(2n)!\, e - f(2n) and (2n)!e+g(2n)\frac{(2n)!}{e} + g(2n) are integers. Therefore:

q((2n)!ef(2n))andp((2n)!e+g(2n))q\left((2n)!\, e - f(2n)\right) \quad \text{and} \quad p\left(\frac{(2n)!}{e} + g(2n)\right)

are both integers (products of integers). Their difference is also an integer:

p((2n)!e+g(2n))q((2n)!ef(2n))=(2n)!(peqe)+pg(2n)+qf(2n)p\left(\frac{(2n)!}{e} + g(2n)\right) - q\left((2n)!\, e - f(2n)\right) = (2n)! \left(\frac{p}{e} - qe\right) + pg(2n) + qf(2n)

Since pe=qe\frac{p}{e} = qe, i.e. peqe=0\frac{p}{e} - qe = 0, the first term vanishes. Therefore:

pg(2n)+qf(2n) is an integerpg(2n) + qf(2n) \text{ is an integer} \qquad \blacksquare

Part (v)

Suppose for contradiction that e2e^2 is rational, so e2=pqe^2 = \frac{p}{q} for some positive integers p,qp, q. Then qe=peqe = \frac{p}{e}, and by part (iv), qf(2n)+pg(2n)qf(2n) + pg(2n) is an integer for all positive integers nn.

Choose n=max(p,q)n = \max(p, q), which ensures npn \geq p and nqn \geq q. Then:

  • From part (i): qf(2n)<q2nn2n=12qf(2n) < \frac{q}{2n} \leq \frac{n}{2n} = \frac{1}{2}
  • From part (ii): pg(2n)<p2n+1<p2nn2n=12pg(2n) < \frac{p}{2n+1} < \frac{p}{2n} \leq \frac{n}{2n} = \frac{1}{2}

Also, since both f(2n)f(2n) and g(2n)g(2n) are positive and p,qp, q are positive:

0<qf(2n)+pg(2n)<12+12=10 < qf(2n) + pg(2n) < \frac{1}{2} + \frac{1}{2} = 1

But qf(2n)+pg(2n)qf(2n) + pg(2n) is supposed to be an integer, and no integer lies strictly between 0 and 1. This is a contradiction.

Therefore e2e^2 is irrational. \qquad \blacksquare

Examiner Notes

第三受欢迎题目,均分约9/20。Part(i)(ii)容易猜出几何级数形式但缺乏严格论证无法得满分。Part(ii)中配对连续项的论证常缺乏必要细节。Part(iii)中将1/e展开为倒数而非e⁻¹是常见错误,容易迷失方向。Part(v)反证法中选取合适的n值是难点。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

8 (i) Explain why the equation (yx+3)(y+x5)=0(y - x + 3)(y + x - 5) = 0 represents a pair of straight lines with gradients 1 and 1-1. Show further that the equation

y2x2+py+qx+r=0y^2 - x^2 + py + qx + r = 0

represents a pair of straight lines with gradients 1 and 1-1 if and only if p2q2=4rp^2 - q^2 = 4r.

In the remainder of this question, C1C_1 is the curve with equation x=y2+2sy+s(s+1)x = y^2 + 2sy + s(s + 1) and C2C_2 is the curve with equation y=x2y = x^2.

(ii) Explain why the coordinates of any point which lies on both of the curves C1C_1 and C2C_2 also satisfy the equation

y2+2sy+s(s+1)x+k(yx2)=0y^2 + 2sy + s(s + 1) - x + k(y - x^2) = 0

for any real number kk.

Given that ss is such that C1C_1 and C2C_2 intersect at four distinct points, show that choosing k=1k = 1 gives an equation representing a pair of straight lines, with gradients 1 and 1-1, on which all four points of intersection lie.

(iii) Show that if C1C_1 and C2C_2 intersect at four distinct points, then s<34s < -\frac{3}{4}.

(iv) Show that if s<34s < -\frac{3}{4}, then C1C_1 and C2C_2 intersect at four distinct points.

Hint

(i)** (yx+3)(y+x5)=0(y - x + 3)(y + x - 5) = 0 if and only if either yx+3=0y - x + 3 = 0 or y+x5=0y + x - 5 = 0. These are the equations of two straight lines with gradients 1 and -1.

E1

A pair of straight lines with gradients 1 and -1 can be expressed as yx+a=0y - x + a = 0 and

y+x+b=0y + x + b = 0. Thus (yx+a)(y+x+b)=0(y - x + a)(y + x + b) = 0 can be expressed

y2x2+py+qx+r=0y^2 - x^2 + py + qx + r = 0 if and only if a+b=pa + b = p, ab=qa - b = q, and ab=rab = r. M1 A1

Hence, a=12(p+q)a = \frac{1}{2}(p + q), b=12(pq)b = \frac{1}{2}(p - q) and so 12(p+q)12(pq)=r\frac{1}{2}(p + q)\frac{1}{2}(p - q) = r which can be written

p2q2=4rp^2 - q^2 = 4r. *M1 A1 (5)

(ii) If a point (x,y)(x, y) lies on C1C_1, then x=y2+2sy+s(s+1)=0x = y^2 + 2sy + s(s + 1) = 0 which can be rearranged as y2+2sy+s(s+1)x=0y^2 + 2sy + s(s + 1) - x = 0. If a point (x,y)(x, y) lies on C2C_2, then y=x2y = x^2 which can be expressed as k(yx2)=0k(y - x^2) = 0 for any real number kk. Thus, if it lies on both

y2+2sy+s(s+1)x+k(yx2)=0y^2 + 2sy + s(s + 1) - x + k(y - x^2) = 0 for any real number kk

E1 E1

If k=1k = 1,

y2x2+(2s+1)yx+s(s+1)=0y^2 - x^2 + (2s + 1)y - x + s(s + 1) = 0

and

(2s+1)2(1)2=4s2+4s=4s(s+1)(2s + 1)^2 - (-1)^2 = 4s^2 + 4s = 4s(s + 1)

satisfying the condition as derived in (i). M1 A1 (4)

(iii) If C1C_1 and C2C_2 intersect at four distinct points, then they do so on the pair of straight lines,

y2x2+(2s+1)yx+s(s+1)=0y^2 - x^2 + (2s + 1)y - x + s(s + 1) = 0.

E1

y2x2+(2s+1)yx+s(s+1)=(y+x+s+1)(yx+s)y^2 - x^2 + (2s + 1)y - x + s(s + 1) = (y + x + s + 1)(y - x + s) B1

Therefore, y+x+s+1=0y + x + s + 1 = 0 must meet C2C_2 at two distinct points and yx+s=0y - x + s = 0 must meet C2C_2 at two different distinct points. E1

Thus, solving x2+x+s+1=0x^2 + x + s + 1 = 0 having two distinct roots, the discriminant 14(s+1)>01 - 4(s + 1) > 0

That is s<34s < -\frac{3}{4} M1 A1

and solving x2x+s=0x^2 - x + s = 0 having two distinct roots, the discriminant 14s>01 - 4s > 0 i.e. s<14s < \frac{1}{4}

So it is necessary that s<34s < -\frac{3}{4}. *A1 (6)


(iv) If s<34s < -\frac{3}{4} for C1C_1 and C2C_2 to intersect at four points, they do so on the pair of straight lines, two distinct on each of the lines in (iii) as shown by the non-zero discriminants in (iii) and that will be four distinct points provided that the point of intersection of the two lines is not one of them. E1 E1

The intersection of

y+x+s+1=0y + x + s + 1 = 0 and yx+s=0y - x + s = 0 is at (12,2s+12)(-\frac{1}{2}, -\frac{2s+1}{2}) which will only lie on C2C_2 if 2s+12=(12)2-\frac{2s+1}{2} = (-\frac{1}{2})^2 that is if s=34s = -\frac{3}{4} which is prohibited. M1 A1 E1 (5)


Model Solution

Part (i)

The equation (yx+3)(y+x5)=0(y - x + 3)(y + x - 5) = 0 holds if and only if either yx+3=0y - x + 3 = 0 or y+x5=0y + x - 5 = 0. These are equations of straight lines. The line y=x3y = x - 3 has gradient 1, and the line y=x+5y = -x + 5 has gradient 1-1.


For the general case, suppose we have a pair of straight lines with gradients 1 and 1-1. These can be written as:

yx+a=0andy+x+b=0y - x + a = 0 \quad \text{and} \quad y + x + b = 0

for some constants a,ba, b. Their combined equation is:

(yx+a)(y+x+b)=0(y - x + a)(y + x + b) = 0

Expanding:

y2+xy+byxyx2bx+ay+ax+ab=0y^2 + xy + by - xy - x^2 - bx + ay + ax + ab = 0 y2x2+(a+b)y+(ab)x+ab=0y^2 - x^2 + (a + b)y + (a - b)x + ab = 0

Comparing with y2x2+py+qx+r=0y^2 - x^2 + py + qx + r = 0, we need:

p=a+b,q=ab,r=abp = a + b, \quad q = a - b, \quad r = ab

From the first two equations: a=p+q2a = \frac{p + q}{2} and b=pq2b = \frac{p - q}{2}.

Therefore:

r=ab=p+q2pq2=p2q24r = ab = \frac{p + q}{2} \cdot \frac{p - q}{2} = \frac{p^2 - q^2}{4}

which gives p2q2=4rp^2 - q^2 = 4r.

Conversely, if p2q2=4rp^2 - q^2 = 4r, set a=p+q2a = \frac{p+q}{2} and b=pq2b = \frac{p-q}{2}. Then ab=p2q24=rab = \frac{p^2 - q^2}{4} = r, and the equation factors as (yx+a)(y+x+b)=0(y - x + a)(y + x + b) = 0, representing a pair of lines with gradients 1 and 1-1.

Therefore y2x2+py+qx+r=0y^2 - x^2 + py + qx + r = 0 represents a pair of straight lines with gradients 1 and 1-1 if and only if p2q2=4rp^2 - q^2 = 4r. \qquad \blacksquare


Part (ii)

If a point (x,y)(x, y) lies on C1C_1, then x=y2+2sy+s(s+1)x = y^2 + 2sy + s(s+1), which rearranges to:

y2+2sy+s(s+1)x=0y^2 + 2sy + s(s+1) - x = 0

If a point (x,y)(x, y) lies on C2C_2, then y=x2y = x^2, i.e. yx2=0y - x^2 = 0, so k(yx2)=0k(y - x^2) = 0 for any real number kk.

Therefore, if a point lies on both curves, both equations hold simultaneously, and adding them gives:

y2+2sy+s(s+1)x+k(yx2)=0for any kRy^2 + 2sy + s(s+1) - x + k(y - x^2) = 0 \qquad \text{for any } k \in \mathbb{R} \qquad \blacksquare

Setting k=1k = 1:

y2x2+(2s+1)yx+s(s+1)=0y^2 - x^2 + (2s + 1)y - x + s(s + 1) = 0

This is of the form y2x2+py+qx+r=0y^2 - x^2 + py + qx + r = 0 with p=2s+1p = 2s + 1, q=1q = -1, r=s(s+1)r = s(s+1).

Checking the condition from part (i):

p2q2=(2s+1)21=4s2+4s+11=4s2+4s=4s(s+1)=4rp^2 - q^2 = (2s+1)^2 - 1 = 4s^2 + 4s + 1 - 1 = 4s^2 + 4s = 4s(s+1) = 4r

So the condition p2q2=4rp^2 - q^2 = 4r is satisfied, and the equation represents a pair of straight lines with gradients 1 and 1-1. All four intersection points of C1C_1 and C2C_2 lie on these lines. \qquad \blacksquare


Part (iii)

We show: if C1C_1 and C2C_2 intersect at four distinct points, then s<34s < -\frac{3}{4}.

From part (ii), with k=1k = 1, the equation becomes:

y2x2+(2s+1)yx+s(s+1)=0y^2 - x^2 + (2s+1)y - x + s(s+1) = 0

The pair of lines with gradients 1 and 1-1 takes the form yx+a=0y - x + a = 0 and y+x+b=0y + x + b = 0. Expanding their product:

(yx+a)(y+x+b)=y2x2+(a+b)y+(ab)x+ab(y - x + a)(y + x + b) = y^2 - x^2 + (a + b)y + (a - b)x + ab

Comparing with y2x2+(2s+1)yx+s(s+1)=0y^2 - x^2 + (2s+1)y - x + s(s+1) = 0:

a+b=2s+1,ab=1,ab=s(s+1)a + b = 2s + 1, \quad a - b = -1, \quad ab = s(s+1)

From the first two: a=sa = s, b=s+1b = s + 1. Checking: ab=s(s+1)ab = s(s+1). Correct.

The equation factors as:

(yx+s)(y+x+s+1)=0(y - x + s)(y + x + s + 1) = 0

giving the two lines yx+s=0y - x + s = 0 (i.e. y=xsy = x - s) and y+x+s+1=0y + x + s + 1 = 0 (i.e. y=xs1y = -x - s - 1).

For four distinct intersection points, each line must meet C2C_2 (y=x2y = x^2) at two distinct points, and no intersection point is shared between the two lines.

Line 1: y=xsy = x - s. Substituting into y=x2y = x^2:

x2=xs    x2x+s=0x^2 = x - s \implies x^2 - x + s = 0

Discriminant: Δ1=14s\Delta_1 = 1 - 4s.

For two distinct real roots: 14s>01 - 4s > 0, i.e. s<14s < \frac{1}{4}.

Line 2: y=xs1y = -x - s - 1. Substituting into y=x2y = x^2:

x2=xs1    x2+x+s+1=0x^2 = -x - s - 1 \implies x^2 + x + s + 1 = 0

Discriminant: Δ2=14(s+1)=34s\Delta_2 = 1 - 4(s + 1) = -3 - 4s.

For two distinct real roots: 34s>0-3 - 4s > 0, i.e. s<34s < -\frac{3}{4}.

Since s<34s < -\frac{3}{4} is the more restrictive condition, and both are necessary for four intersection points, we conclude that if C1C_1 and C2C_2 intersect at four distinct points, then s<34s < -\frac{3}{4}. \qquad \blacksquare


Part (iv)

We show: if s<34s < -\frac{3}{4}, then C1C_1 and C2C_2 intersect at four distinct points.

From part (ii), when k=1k = 1, the equation factors as:

(yx+s)(y+x+s+1)=0(y - x + s)(y + x + s + 1) = 0

and any intersection point of C1C_1 and C2C_2 lies on these two lines.

Step 1: Each line meets C2C_2 at two distinct points.

For yx+s=0y - x + s = 0 with y=x2y = x^2: the equation x2x+s=0x^2 - x + s = 0 has discriminant 14s1 - 4s.

Since s<34s < -\frac{3}{4}, we have 14s>1+3=4>01 - 4s > 1 + 3 = 4 > 0. Two distinct real roots.

For y+x+s+1=0y + x + s + 1 = 0 with y=x2y = x^2: the equation x2+x+s+1=0x^2 + x + s + 1 = 0 has discriminant 34s-3 - 4s.

Since s<34s < -\frac{3}{4}, we have 34s>3+3=0-3 - 4s > -3 + 3 = 0. Two distinct real roots.

So each line meets C2C_2 at two points, giving at most four intersection points.

Step 2: No intersection point is shared (the four points are distinct).

The two lines yx+s=0y - x + s = 0 and y+x+s+1=0y + x + s + 1 = 0 intersect at the point obtained by solving simultaneously:

Adding: 2y+2s+1=02y + 2s + 1 = 0, so y=2s+12y = -\frac{2s+1}{2}. Subtracting: 2x+1=02x + 1 = 0, so x=12x = -\frac{1}{2}.

This intersection point lies on C2C_2 (y=x2y = x^2) if and only if:

2s+12=(12)2=14-\frac{2s + 1}{2} = \left(-\frac{1}{2}\right)^2 = \frac{1}{4} (2s+1)=12    2s+1=12    s=34-(2s + 1) = \frac{1}{2} \implies 2s + 1 = -\frac{1}{2} \implies s = -\frac{3}{4}

Since s<34s < -\frac{3}{4}, the intersection point of the two lines does not lie on C2C_2. Therefore none of the four points is shared, and C1C_1 and C2C_2 intersect at exactly four distinct points. \qquad \blacksquare

Examiner Notes

纯数中较不受欢迎的题目。Part(iii)(iv)中考官特别指出蕴含方向(implication direction)让很多考生困惑:Part(iii)需要’四交点→s<-3/4’,Part(iv)需要’s<-3/4→四交点’。因式分解时的符号错误是常见问题(建议展开验证)。少数考生通过考虑直线与y=x²相切的情况同时解决(iii)(iv)两部分。