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STEP3 2023 -- Pure Mathematics

STEP3 2023 — Section A (Pure Mathematics)

Section titled “STEP3 2023 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2023  |  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Challenging坐标几何,切线方程,判别式,韦达定理,参数化方法
2纯数Challenging极坐标面积公式,三角函数积分,极限计算,渐近分析
3纯数Hard复数几何意义,韦达定理(三次方程),曲线草图,不等式证明
4纯数Hardde Moivre定理,二项式展开,代入法求系数,多项式因式分解
5纯数Challenging因数分解,素数性质,韦达定理,不等式推理,反证法
6纯数ChallengingMaclaurin级数展开,不等式证明,导数分析,驻点判定,函数图像
7纯数Challenging积分换元,分部积分,完全平方式构造,非负函数性质
8纯数Hard特征方程,分段求解,连续可微条件,函数对称性,递推构造

Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

1 The distinct points P(2ap,ap2)P(2ap, ap^2) and Q(2aq,aq2)Q(2aq, aq^2) lie on the curve x2=4ayx^2 = 4ay, where a>0a > 0.

(i) Given that

(p+q)2=p2q2+6pq+5,(∗)(p + q)^2 = p^2q^2 + 6pq + 5 , \qquad (\ast)

show that the line through PP and QQ is a tangent to the circle with centre (0,3a)(0, 3a) and radius 2a2a.

(ii) Show that, for any given value of pp with p2≠1p^2 \neq 1, there are two distinct real values of qq that satisfy equation (∗)(\ast).

Let these values be q1q_1 and q2q_2. Find expressions, in terms of pp, for q1+q2q_1 + q_2 and q1q2q_1q_2.

(iii) Show that, for any given value of pp with p2≠1p^2 \neq 1, there is a triangle with one vertex at PP such that all three vertices lie on the curve x2=4ayx^2 = 4ay and all three sides are tangents to the circle with centre (0,3a)(0, 3a) and radius 2a2a.

Hint

(i) The line through PP and QQ is y−ap2x−2ap=y−aq2x−2aq\frac{y - ap^2}{x - 2ap} = \frac{y - aq^2}{x - 2aq}

y−ap2x−2ap=ap2−aq22ap−2aq=p+q2\frac{y - ap^2}{x - 2ap} = \frac{ap^2 - aq^2}{2ap - 2aq} = \frac{p + q}{2}

y−aq2x−2aq=ap2−aq22ap−2aq=p+q2\frac{y - aq^2}{x - 2aq} = \frac{ap^2 - aq^2}{2ap - 2aq} = \frac{p + q}{2}

or multiplied to remove denominators.

M1

(y−ap2)(x−2aq)=(y−aq2)(x−2ap)(y - ap^2)(x - 2aq) = (y - aq^2)(x - 2ap)

(2ap−2aq)y+2a2(p2q−pq2)=(ap2−aq2)x(2ap - 2aq)y + 2a^2(p^2q - pq^2) = (ap^2 - aq^2)x

PP and QQ are distinct thus p≠qp \neq q and so p−q≠0p - q \neq 0

Therefore 2y+2apq=(p+q)x2y + 2apq = (p + q)x that is (p+q)x−2y−2apq=0(p + q)x - 2y - 2apq = 0

A1

The perpendicular distance of (0,3a)(0, 3a) from the line PQPQ is 2a2a which requires

∣−6a−2apq((p+q)2+4)∣=2a\left| \frac{-6a - 2apq}{\sqrt{((p + q)^2 + 4)}} \right| = 2a

M1 A1 A1 A1

that is (pq+3)2=(p+q)2+4(pq + 3)^2 = (p + q)^2 + 4 M1 A1

i.e. (p+q)2=p2q2+6pq+9−4=p2q2+6pq+5(p + q)^2 = p^2q^2 + 6pq + 9 - 4 = p^2q^2 + 6pq + 5 (∗)(\ast)

A1* (9)

(I) (p+q)x−2y−2apq=0(p + q)x - 2y - 2apq = 0 meets x2+(y−3a)2=4a2x^2 + (y - 3a)^2 = 4a^2 when

4(y+apq)2+(p+q)2(y2−6ay+5a2)=04(y + apq)^2 + (p + q)^2(y^2 - 6ay + 5a^2) = 0

M1 A1

(4+(p+q)2)y2−(6a(p+q)2−8apq)y+(5a2(p+q)2+4a2p2q2)=0(4 + (p + q)^2)y^2 - (6a(p + q)^2 - 8apq)y + (5a^2(p + q)^2 + 4a^2p^2q^2) = 0

A1

Thus using (p+q)2=p2q2+6pq+5(p + q)^2 = p^2q^2 + 6pq + 5 , M1

(pq+3)2y2−2a(pq+3)(3pq+5)y+a2(3pq+5)2=0(pq + 3)^2y^2 - 2a(pq + 3)(3pq + 5)y + a^2(3pq + 5)^2 = 0

which is a perfect square, A1

so (pq+3)y−a(3pq+5)=0(pq + 3)y - a(3pq + 5) = 0 which only has a single root so the line is a tangent. A1 A1*

(II) Foot of perpendicular from (0,3a)(0,3a) to (p+q)x−2y−2apq=0(p + q)x - 2y - 2apq = 0 is at intersection with (p+q)y+2x=3a(p+q)(p + q)y + 2x = 3a(p + q) M1 A1

So solving (p+q)2y+4y+4apq=3a(p+q)2(p + q)^2y + 4y + 4apq = 3a(p + q)^2 A1

y=3a(p+q)2−4apq(p+q)2+4 and x=(p+q)2(3a−3a(p+q)2−4apq(p+q)2+4)=2a(p+q)(3+pq)(p+q)2+4y = \frac{3a(p+q)^2-4apq}{(p+q)^2+4} \text{ and } x = \frac{(p+q)}{2} \left( 3a - \frac{3a(p+q)^2-4apq}{(p+q)^2+4} \right) = \frac{2a(p+q)(3+pq)}{(p+q)^2+4}

A1

and so the square of the distance is M1 A1

[2a(p+q)(3+pq)(p+q)2+4]2+[4a(3+pq)(p+q)2+4]2=[2a(3+pq)(p+q)2+4]2(4+(p+q)2)\left[ \frac{2a(p+q)(3+pq)}{(p+q)^2+4} \right]^2 + \left[ \frac{4a(3+pq)}{(p+q)^2+4} \right]^2 = \left[ \frac{2a(3+pq)}{(p+q)^2+4} \right]^2 (4 + (p+q)^2) =4a2(3+pq)24+(p+q)2=4a2= \frac{4a^2(3+pq)^2}{4+(p+q)^2} = 4a^2

using given condition. A1*

(III) Method is possible by differentiation of circle equation. Partial or incorrect solution by this method zero marks; completely correct solution full marks; completely correct solution except minor inaccuracy, withhold one accuracy mark and final accuracy mark.

(ii) (∗)(\ast) can be re-written

q2(p2−1)+4pq+(5−p2)=0q^2(p^2 - 1) + 4pq + (5 - p^2) = 0 M1

Considering this as a quadratic equation for qq, to be two distinct roots, p2−1≠0p^2 - 1 \neq 0 (it is given that p2≠1p^2 \neq 1) E1 and the discriminant needs to be positive.

16p2−4(p2−1)(5−p2)=4(p4−2p2+5)=4(p2−1)2+16>016p^2 - 4(p^2 - 1)(5 - p^2) = 4(p^4 - 2p^2 + 5) = 4(p^2 - 1)^2 + 16 > 0

as required. M1 A1

q1+q2=−4p(p2−1),q1q2=(5−p2)(p2−1)A1 A1 (6)q_1 + q_2 = \frac{-4p}{(p^2-1)}, \quad q_1q_2 = \frac{(5-p^2)}{(p^2-1)} \quad \text{A1 A1 (6)}

(iii) Given PP, with p2≠1p^2 \neq 1, by (ii) points Q1Q_1 and Q2Q_2 can be defined with parameters q1q_1 and q2q_2 where q1q_1 and q2q_2 are the roots of (∗)(\ast). So by (i), PQ1PQ_1 and PQ2PQ_2 are tangents to the circle centre (0,3a)(0,3a) radius 2a2a. E1

The perpendicular distance of (0,3a)(0,3a) from the line Q1Q2Q_1Q_2 is

∣−6a−2aq1q2((q1+q2)2+4)∣=∣−6a−2a(5−p2p2−1)((−4pp2−1)2+4)∣=2a∣3(p2−1)+(5−p2)16p2+4(p2−1)2∣\left| \frac{-6a - 2aq_1q_2}{\sqrt{((q_1 + q_2)^2 + 4)}} \right| = \left| \frac{-6a - 2a \left( \frac{5-p^2}{p^2-1} \right)}{\sqrt{\left( \left( \frac{-4p}{p^2-1} \right)^2 + 4 \right)}} \right| = 2a \left| \frac{3(p^2-1) + (5-p^2)}{\sqrt{16p^2 + 4(p^2-1)^2}} \right|

M1 A1

=2a∣2p2+24p4+16p2+4∣=2a= 2a \left| \frac{2p^2 + 2}{\sqrt{4p^4 + 16p^2 + 4}} \right| = 2a

A1

Alternative Q1Q2Q_1Q_2 is the third such line provided that (q1q2+3)2=(q1+q2)2+4(q_1q_2 + 3)^2 = (q_1 + q_2)^2 + 4

Diagrammatically, take aa as the midpoint of the base of the isosceles triangle, take bb as the vector from this midpoint to the remaining vertex, and take ss as the ratio of half the base length to the altitude length.

M1 A1 A1

Thus PQ1Q2PQ_1Q_2 is the triangle required.

Model Solution

Part (i)

The gradient of line PQPQ is

m=ap2−aq22ap−2aq=a(p−q)(p+q)2a(p−q)=p+q2m = \frac{ap^2 - aq^2}{2ap - 2aq} = \frac{a(p - q)(p + q)}{2a(p - q)} = \frac{p + q}{2}

since p≠qp \neq q (the points are distinct). The equation of line PQPQ through PP is

y−ap2=p+q2(x−2ap)y - ap^2 = \frac{p + q}{2}(x - 2ap)

Rearranging:

2y−2ap2=(p+q)x−2ap(p+q)2y - 2ap^2 = (p + q)x - 2ap(p + q)

(p+q)x−2y−2ap(p+q)+2ap2=0(p + q)x - 2y - 2ap(p + q) + 2ap^2 = 0

(p+q)x−2y−2apq=0(p + q)x - 2y - 2apq = 0

The perpendicular distance from the centre (0,3a)(0, 3a) of the circle to this line is

d=∣(p+q)(0)−2(3a)−2apq∣(p+q)2+4=∣−6a−2apq∣(p+q)2+4=2a∣pq+3∣(p+q)2+4d = \frac{|(p + q)(0) - 2(3a) - 2apq|}{\sqrt{(p + q)^2 + 4}} = \frac{|-6a - 2apq|}{\sqrt{(p + q)^2 + 4}} = \frac{2a|pq + 3|}{\sqrt{(p + q)^2 + 4}}

For the line to be tangent to the circle of radius 2a2a, we require d=2ad = 2a:

2a∣pq+3∣(p+q)2+4=2a\frac{2a|pq + 3|}{\sqrt{(p + q)^2 + 4}} = 2a

∣pq+3∣=(p+q)2+4|pq + 3| = \sqrt{(p + q)^2 + 4}

Squaring both sides:

(pq+3)2=(p+q)2+4(pq + 3)^2 = (p + q)^2 + 4

Expanding the left side:

p2q2+6pq+9=(p+q)2+4p^2q^2 + 6pq + 9 = (p + q)^2 + 4

(p+q)2=p2q2+6pq+5(p + q)^2 = p^2q^2 + 6pq + 5

This is precisely the given condition. Therefore, the line through PP and QQ is tangent to the circle with centre (0,3a)(0, 3a) and radius 2a2a. ■\qquad \blacksquare

Part (ii)

Expanding the given condition (p+q)2=p2q2+6pq+5(p + q)^2 = p^2q^2 + 6pq + 5:

p2+2pq+q2=p2q2+6pq+5p^2 + 2pq + q^2 = p^2q^2 + 6pq + 5

q2−p2q2+2pq−6pq+p2−5=0q^2 - p^2q^2 + 2pq - 6pq + p^2 - 5 = 0

q2(1−p2)−4pq+(p2−5)=0q^2(1 - p^2) - 4pq + (p^2 - 5) = 0

q2(p2−1)+4pq+(5−p2)=0q^2(p^2 - 1) + 4pq + (5 - p^2) = 0

This is a quadratic equation in qq. Since p2≠1p^2 \neq 1, the coefficient of q2q^2 is non-zero. For two distinct real roots, we need the discriminant to be strictly positive:

Δ=(4p)2−4(p2−1)(5−p2)\Delta = (4p)^2 - 4(p^2 - 1)(5 - p^2)

=16p2−4(5p2−p4−5+p2)= 16p^2 - 4(5p^2 - p^4 - 5 + p^2)

=16p2+4p4−24p2+20= 16p^2 + 4p^4 - 24p^2 + 20

=4p4−8p2+20= 4p^4 - 8p^2 + 20

=4(p4−2p2+1)+16=4(p2−1)2+16= 4(p^4 - 2p^2 + 1) + 16 = 4(p^2 - 1)^2 + 16

Since 4(p2−1)2≥04(p^2 - 1)^2 \geq 0, we have Δ≥16>0\Delta \geq 16 > 0 for all real pp. Therefore, for any given pp with p2≠1p^2 \neq 1, there are two distinct real values of qq satisfying the given equation.

By Vieta’s formulae applied to the quadratic in qq (with coefficients A=p2−1A = p^2 - 1, B=4pB = 4p, C=5−p2C = 5 - p^2):

q1+q2=−4pp2−1,q1q2=5−p2p2−1q_1 + q_2 = -\frac{4p}{p^2 - 1}, \qquad q_1 q_2 = \frac{5 - p^2}{p^2 - 1}

Part (iii)

Given P(2ap,ap2)P(2ap, ap^2) with p2≠1p^2 \neq 1, part (ii) provides two distinct real values q1,q2q_1, q_2 satisfying the given condition. Define Q1(2aq1,aq12)Q_1(2aq_1, aq_1^2) and Q2(2aq2,aq22)Q_2(2aq_2, aq_2^2) on the curve x2=4ayx^2 = 4ay.

By part (i), since each qiq_i satisfies the condition with pp, the lines PQ1PQ_1 and PQ2PQ_2 are both tangent to the circle. Moreover, PQ1PQ_1 and PQ2PQ_2 are distinct lines (since q1≠q2q_1 \neq q_2 gives different slopes (p+q1)/2≠(p+q2)/2(p + q_1)/2 \neq (p + q_2)/2).

It remains to show that Q1Q2Q_1Q_2 is also tangent to the circle. By the same criterion as part (i), the line through Q1Q_1 and Q2Q_2 is tangent if and only if

(q1q2+3)2=(q1+q2)2+4(q_1 q_2 + 3)^2 = (q_1 + q_2)^2 + 4

Using the expressions from part (ii):

q1q2+3=5−p2p2−1+3=5−p2+3(p2−1)p2−1=2(p2+1)p2−1q_1 q_2 + 3 = \frac{5 - p^2}{p^2 - 1} + 3 = \frac{5 - p^2 + 3(p^2 - 1)}{p^2 - 1} = \frac{2(p^2 + 1)}{p^2 - 1}

(q1q2+3)2=4(p2+1)2(p2−1)2(q_1 q_2 + 3)^2 = \frac{4(p^2 + 1)^2}{(p^2 - 1)^2}

(q1+q2)2+4=16p2(p2−1)2+4=16p2+4(p2−1)2(p2−1)2(q_1 + q_2)^2 + 4 = \frac{16p^2}{(p^2 - 1)^2} + 4 = \frac{16p^2 + 4(p^2 - 1)^2}{(p^2 - 1)^2}

=4p4+8p2+4(p2−1)2=4(p2+1)2(p2−1)2= \frac{4p^4 + 8p^2 + 4}{(p^2 - 1)^2} = \frac{4(p^2 + 1)^2}{(p^2 - 1)^2}

These are equal, so Q1Q2Q_1Q_2 is tangent to the circle.

The line Q1Q2Q_1Q_2 cannot pass through PP: if it did, PP would lie on a tangent to the circle through Q1Q_1 and Q2Q_2, meaning PQ1PQ_1 and Q1Q2Q_1Q_2 would be the same line, contradicting the fact that PQ1PQ_1 and PQ2PQ_2 are distinct. Therefore PP, Q1Q_1, Q2Q_2 are non-collinear and form a triangle with all three sides tangent to the circle with centre (0,3a)(0, 3a) and radius 2a2a. ■\qquad \blacksquare

Examiner Notes

最受欢迎题目之一(93%作答),平均分9.5/20。常见错误:使用距离公式时漏掉绝对值符号;第(iii)部分很多考生重复前面的计算而非利用(i)(ii)的结果,解法不够简洁。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

2 The polar curves C1C_1 and C2C_2 are defined for 0⩽θ⩽π0 \leqslant \theta \leqslant \pi by

r=k(1+sin⁡θ)r = k(1 + \sin \theta)

r=k+cos⁡θr = k + \cos \theta

respectively, where kk is a constant greater than 1.

(i) Sketch the curves on the same diagram. Show that if θ=α\theta = \alpha at the point where the curves intersect, tan⁡α=1k\tan \alpha = \frac{1}{k}.

(ii) The region A is defined by the inequalities

0⩽θ⩽αandr⩽k(1+sin⁡θ).0 \leqslant \theta \leqslant \alpha \quad \text{and} \quad r \leqslant k(1 + \sin \theta).

Show that the area of A can be written as

k24(3α−sin⁡αcos⁡α)+k2(1−cos⁡α).\frac{k^2}{4}(3\alpha - \sin \alpha \cos \alpha) + k^2(1 - \cos \alpha).

(iii) The region B is defined by the inequalities

α⩽θ⩽πandr⩽k+cos⁡θ.\alpha \leqslant \theta \leqslant \pi \quad \text{and} \quad r \leqslant k + \cos \theta.

Find an expression in terms of kk and α\alpha for the area of B.

(iv) The total area of regions A and B is denoted by RR. The area of the region enclosed by C1C_1 and the lines θ=0\theta = 0 and θ=π\theta = \pi is denoted by SS. The area of the region enclosed by C2C_2 and the lines θ=0\theta = 0 and θ=π\theta = \pi is denoted by TT.

Show that as k→∞k \to \infty, RT→1\frac{R}{T} \to 1

and find the limit of RS\frac{R}{S}

as k→∞k \to \infty.

Hint

G1 G1 G1

At intersection, when θ=α\theta = \alpha , k(1+sin⁡θ)=k+cos⁡θk(1 + \sin \theta) = k + \cos \theta

Therefore, ksin⁡α=cos⁡αk \sin \alpha = \cos \alpha , that is, tan⁡α=1k\tan \alpha = \frac{1}{k} B1* (5)

(ii) Area A is

12∫0α(k(1+sin⁡θ))2dθ=k22∫0α1+2sin⁡θ+sin⁡2θ dθ\frac{1}{2} \int_{0}^{\alpha} (k(1 + \sin \theta))^2 d\theta = \frac{k^2}{2} \int_{0}^{\alpha} 1 + 2 \sin \theta + \sin^2 \theta \ d\theta

M1

=k22∫0α1+2sin⁡θ+1−cos⁡2θ2 dθ=k22[32θ−2cos⁡θ−14sin⁡2θ]0α= \frac{k^2}{2} \int_{0}^{\alpha} 1 + 2 \sin \theta + \frac{1 - \cos 2\theta}{2} \ d\theta = \frac{k^2}{2} \left[ \frac{3}{2}\theta - 2 \cos \theta - \frac{1}{4} \sin 2\theta \right]_{0}^{\alpha}

dM1 A1

=k22{32α−2cos⁡α−14sin⁡2α+2}=k22{32α−2cos⁡α−12sin⁡αcos⁡α+2}= \frac{k^2}{2} \left\{ \frac{3}{2}\alpha - 2 \cos \alpha - \frac{1}{4} \sin 2\alpha + 2 \right\} = \frac{k^2}{2} \left\{ \frac{3}{2}\alpha - 2 \cos \alpha - \frac{1}{2} \sin \alpha \cos \alpha + 2 \right\}

=k24(3α−sin⁡αcos⁡α)+k2(1−cos⁡α)= \frac{k^2}{4} (3\alpha - \sin \alpha \cos \alpha) + k^2(1 - \cos \alpha)

A1* (4)

(iii) Area B is 12∫απ(k+cos⁡θ)2dθ=12∫απk2+2kcos⁡θ+cos⁡2θ dθ=12∫απk2+2kcos⁡θ+1+cos⁡2θ2 dθ\frac{1}{2} \int_{\alpha}^{\pi} (k + \cos \theta)^2 d\theta = \frac{1}{2} \int_{\alpha}^{\pi} k^2 + 2k \cos \theta + \cos^2 \theta \ d\theta = \frac{1}{2} \int_{\alpha}^{\pi} k^2 + 2k \cos \theta + \frac{1 + \cos 2\theta}{2} \ d\theta

M1 M1

=12[k2θ+2ksin⁡θ+12θ+14sin⁡2θ]απ=12{k2π+π2−k2α−2ksin⁡α−α2−14sin⁡2α}= \frac{1}{2} \left[ k^2\theta + 2k \sin \theta + \frac{1}{2}\theta + \frac{1}{4} \sin 2\theta \right]_{\alpha}^{\pi} = \frac{1}{2} \left\{ k^2\pi + \frac{\pi}{2} - k^2\alpha - 2k \sin \alpha - \frac{\alpha}{2} - \frac{1}{4} \sin 2\alpha \right\}

A1

=12{k2π+π2−k2α−2ksin⁡α−α2−12sin⁡αcos⁡α}= \frac{1}{2} \left\{ k^2 \pi + \frac{\pi}{2} - k^2 \alpha - 2k \sin \alpha - \frac{\alpha}{2} - \frac{1}{2} \sin \alpha \cos \alpha \right\}

=14{2k2π+π−2k2α−4ksin⁡α−α−sin⁡αcos⁡α}= \frac{1}{4} \left\{ 2k^2 \pi + \pi - 2k^2 \alpha - 4k \sin \alpha - \alpha - \sin \alpha \cos \alpha \right\}

A1 (4)

(iv) As k→∞k \to \infty, α\alpha is small as tan⁡α=1k\tan \alpha = \frac{1}{k} so α≈sin⁡α≈tan⁡α=1k\alpha \approx \sin \alpha \approx \tan \alpha = \frac{1}{k} and cos⁡α≈1−12k2\cos \alpha \approx 1 - \frac{1}{2k^2} M1

Area A is k2+\frac{k}{2} + terms of lower order in kk A1

Area B is k2π2+\frac{k^2 \pi}{2} + terms of lower order in kk A1

So, area R is k2π2+\frac{k^2 \pi}{2} + terms of lower order in kk

Area T is

12∫0π(k+cos⁡θ)2dθ=14(2k2π+π)\frac{1}{2} \int_{0}^{\pi} (k + \cos \theta)^2 d\theta = \frac{1}{4} (2k^2 \pi + \pi)

or alternatively, use of result from (iii) with α=0\alpha = 0

which is k2π2+\frac{k^2 \pi}{2} + terms of lower order in kk B1

Thus, as required,

area of Rarea of T=k2π2+terms of lower order in kk2π2+terms of lower order in k→1\frac{area\ of\ R}{area\ of\ T} = \frac{\frac{k^2 \pi}{2} + \text{terms of lower order in } k}{\frac{k^2 \pi}{2} + \text{terms of lower order in } k} \to 1

E1

Area S is

12∫0π(k(1+sin⁡θ))2dθ=k24×3π+2k2=k2(3π4+2)\frac{1}{2} \int_{0}^{\pi} (k(1 + \sin \theta))^2 d\theta = \frac{k^2}{4} \times 3\pi + 2k^2 = k^2 \left( \frac{3\pi}{4} + 2 \right)

or alternatively, use of result from (ii) with α=π\alpha = \pi

B1

Thus

area of Rarea of S→π2(3π4+2)=2π3π+8\frac{area\ of\ R}{area\ of\ S} \to \frac{\frac{\pi}{2}}{\left( \frac{3\pi}{4} + 2 \right)} = \frac{2\pi}{3\pi + 8}

A1 (7)

Model Solution

Part (i)

C1:r=k(1+sin⁡θ)C_1: r = k(1 + \sin\theta) is a cardioid-like curve. At θ=0\theta = 0, r=kr = k; at θ=π/2\theta = \pi/2, r=2kr = 2k (maximum); at θ=π\theta = \pi, r=kr = k. It is symmetric about θ=π/2\theta = \pi/2 and always positive since k>1k > 1.

C2:r=k+cos⁡θC_2: r = k + \cos\theta is roughly circular. At θ=0\theta = 0, r=k+1r = k + 1 (maximum); at θ=π/2\theta = \pi/2, r=kr = k; at θ=π\theta = \pi, r=k−1>0r = k - 1 > 0.

At θ=0\theta = 0: r1=k<k+1=r2r_1 = k < k + 1 = r_2, so C1C_1 is inside C2C_2. At θ=π/2\theta = \pi/2: r1=2k>k=r2r_1 = 2k > k = r_2, so C1C_1 is outside C2C_2. Therefore the curves cross once in (0,π/2)(0, \pi/2) at θ=α\theta = \alpha.

At the intersection, k(1+sin⁡α)=k+cos⁡αk(1 + \sin\alpha) = k + \cos\alpha:

ksin⁡α=cos⁡αk\sin\alpha = \cos\alpha

tan⁡α=1k\tan\alpha = \frac{1}{k}

Part (ii)

A=12∫0α[k(1+sin⁡θ)]2 dθ=k22∫0α(1+sin⁡θ)2 dθA = \frac{1}{2}\int_0^\alpha [k(1 + \sin\theta)]^2 \, d\theta = \frac{k^2}{2}\int_0^\alpha (1 + \sin\theta)^2 \, d\theta

Expanding the integrand:

(1+sin⁡θ)2=1+2sin⁡θ+sin⁡2θ(1 + \sin\theta)^2 = 1 + 2\sin\theta + \sin^2\theta

Using sin⁡2θ=1−cos⁡2θ2\sin^2\theta = \frac{1 - \cos 2\theta}{2}:

=32+2sin⁡θ−cos⁡2θ2= \frac{3}{2} + 2\sin\theta - \frac{\cos 2\theta}{2}

Integrating:

∫0α(32+2sin⁡θ−cos⁡2θ2)dθ=[3θ2−2cos⁡θ−sin⁡2θ4]0α\int_0^\alpha \left(\frac{3}{2} + 2\sin\theta - \frac{\cos 2\theta}{2}\right) d\theta = \left[\frac{3\theta}{2} - 2\cos\theta - \frac{\sin 2\theta}{4}\right]_0^\alpha

=3α2−2cos⁡α−sin⁡2α4+2= \frac{3\alpha}{2} - 2\cos\alpha - \frac{\sin 2\alpha}{4} + 2

Using sin⁡2α=2sin⁡αcos⁡α\sin 2\alpha = 2\sin\alpha\cos\alpha:

=3α2−2cos⁡α−sin⁡αcos⁡α2+2= \frac{3\alpha}{2} - 2\cos\alpha - \frac{\sin\alpha\cos\alpha}{2} + 2

Therefore:

A=k22(3α2−2cos⁡α−sin⁡αcos⁡α2+2)=k24(3α−sin⁡αcos⁡α)+k2(1−cos⁡α)A = \frac{k^2}{2}\left(\frac{3\alpha}{2} - 2\cos\alpha - \frac{\sin\alpha\cos\alpha}{2} + 2\right) = \frac{k^2}{4}(3\alpha - \sin\alpha\cos\alpha) + k^2(1 - \cos\alpha)

Part (iii)

B=12∫απ(k+cos⁡θ)2 dθB = \frac{1}{2}\int_\alpha^\pi (k + \cos\theta)^2 \, d\theta

Expanding:

(k+cos⁡θ)2=k2+2kcos⁡θ+cos⁡2θ(k + \cos\theta)^2 = k^2 + 2k\cos\theta + \cos^2\theta

Using cos⁡2θ=1+cos⁡2θ2\cos^2\theta = \frac{1 + \cos 2\theta}{2}:

=k2+12+2kcos⁡θ+cos⁡2θ2= k^2 + \frac{1}{2} + 2k\cos\theta + \frac{\cos 2\theta}{2}

Integrating:

∫απ(k2+12+2kcos⁡θ+cos⁡2θ2)dθ=[k2θ+θ2+2ksin⁡θ+sin⁡2θ4]απ\int_\alpha^\pi \left(k^2 + \frac{1}{2} + 2k\cos\theta + \frac{\cos 2\theta}{2}\right) d\theta = \left[k^2\theta + \frac{\theta}{2} + 2k\sin\theta + \frac{\sin 2\theta}{4}\right]_\alpha^\pi

At θ=π\theta = \pi: k2π+π2+0+0k^2\pi + \frac{\pi}{2} + 0 + 0. At θ=α\theta = \alpha: k2α+α2+2ksin⁡α+sin⁡2α4k^2\alpha + \frac{\alpha}{2} + 2k\sin\alpha + \frac{\sin 2\alpha}{4}.

B=12(k2(π−α)+π−α2−2ksin⁡α−sin⁡2α4)B = \frac{1}{2}\left(k^2(\pi - \alpha) + \frac{\pi - \alpha}{2} - 2k\sin\alpha - \frac{\sin 2\alpha}{4}\right)

Using sin⁡2α=2sin⁡αcos⁡α\sin 2\alpha = 2\sin\alpha\cos\alpha:

B=k2(π−α)2+π−α4−ksin⁡α−sin⁡αcos⁡α4B = \frac{k^2(\pi - \alpha)}{2} + \frac{\pi - \alpha}{4} - k\sin\alpha - \frac{\sin\alpha\cos\alpha}{4}

Part (iv)

Since tan⁡α=1/k\tan\alpha = 1/k and k>1k > 1, we have α∈(0,π/4)\alpha \in (0, \pi/4). As k→∞k \to \infty, α→0\alpha \to 0.

Area of TT: Using the result from (iii) with α=0\alpha = 0:

T=12∫0π(k+cos⁡θ)2 dθ=k2π2+π4T = \frac{1}{2}\int_0^\pi (k + \cos\theta)^2 \, d\theta = \frac{k^2\pi}{2} + \frac{\pi}{4}

Area of SS: Using the result from (ii) with α=π\alpha = \pi:

S=k24(3π−sin⁡πcos⁡π)+k2(1−cos⁡π)=3k2π4+2k2=k2(3π4+2)S = \frac{k^2}{4}(3\pi - \sin\pi\cos\pi) + k^2(1 - \cos\pi) = \frac{3k^2\pi}{4} + 2k^2 = k^2\left(\frac{3\pi}{4} + 2\right)

Behaviour of AA as k→∞k \to \infty: Using sin⁡α=1k2+1\sin\alpha = \frac{1}{\sqrt{k^2+1}} and cos⁡α=kk2+1\cos\alpha = \frac{k}{\sqrt{k^2+1}}:

k2(3α−sin⁡αcos⁡α)4=3k2α4−k34(k2+1)\frac{k^2(3\alpha - \sin\alpha\cos\alpha)}{4} = \frac{3k^2\alpha}{4} - \frac{k^3}{4(k^2+1)}

Since α=arctan⁡(1/k)∼1/k\alpha = \arctan(1/k) \sim 1/k as k→∞k \to \infty, the first term ∼3k/4\sim 3k/4 and the second ∼k/4\sim k/4, so this expression ∼k/2\sim k/2.

k2(1−cos⁡α)=k2(1−kk2+1)=k2k2+1(k2+1+k)→12k^2(1 - \cos\alpha) = k^2\left(1 - \frac{k}{\sqrt{k^2+1}}\right) = \frac{k^2}{\sqrt{k^2+1}\left(\sqrt{k^2+1} + k\right)} \to \frac{1}{2}

Therefore Area A∼k/2A \sim k/2 as k→∞k \to \infty.

Behaviour of BB as k→∞k \to \infty: The leading term is k2(π−α)2∼k2π2\frac{k^2(\pi - \alpha)}{2} \sim \frac{k^2\pi}{2}. The remaining terms (π−α)/4(\pi - \alpha)/4, ksin⁡αk\sin\alpha, and sin⁡αcos⁡α/4\sin\alpha\cos\alpha/4 are bounded. Therefore Area B=k2π2+O(k)B = \frac{k^2\pi}{2} + O(k).

The ratio R/TR/T:

R=A+B=k2π2+O(k)R = A + B = \frac{k^2\pi}{2} + O(k)

RT=k2π2+O(k)k2π2+π4→1 as k→∞\frac{R}{T} = \frac{\frac{k^2\pi}{2} + O(k)}{\frac{k^2\pi}{2} + \frac{\pi}{4}} \to 1 \text{ as } k \to \infty

The ratio R/SR/S:

RS=k2π2+O(k)k2(3π4+2)→π/23π/4+2=2π3π+8\frac{R}{S} = \frac{\frac{k^2\pi}{2} + O(k)}{k^2\left(\frac{3\pi}{4} + 2\right)} \to \frac{\pi/2}{3\pi/4 + 2} = \frac{2\pi}{3\pi + 8}

Examiner Notes

全卷最成功的题目,平均分12+/20。第(iv)部分最难,关键观察 α→0 需用 tanα=1/k 严格论证。常见错误:未注意 α 依赖于 k,过早代入 α=0 导致错误结论如 k·sinα→0。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

3 (i) Show that, if aa and bb are complex numbers, with b≠0b \neq 0, and ss is a positive real number, then the points in the Argand diagram representing the complex numbers a+sbia + sbi, a−sbia - sbi and a+ba + b form an isosceles triangle.

Given three points which form an isosceles triangle in the Argand diagram, explain with the aid of a diagram how to determine the values of aa, bb and ss so that the vertices of the triangle represent complex numbers a+sbia + sbi, a−sbia - sbi and a+ba + b.

(ii) Show that, if the roots of the equation z3+pz+q=0z^3 + pz + q = 0, where pp and qq are complex numbers, are represented in the Argand diagram by the vertices of an isosceles triangle, then there is a non-zero real number ss such that

p3q2=27(3s2−1)34(9s2+1)2.\frac{p^3}{q^2} = \frac{27(3s^2 - 1)^3}{4(9s^2 + 1)^2}.

(iii) Sketch the graph y=(3x−1)3(9x+1)2y = \frac{(3x - 1)^3}{(9x + 1)^2}, identifying any stationary points.

(iv) Show that if the roots of the equation z3+pz+q=0z^3 + pz + q = 0 are represented in the Argand diagram by the vertices of an isosceles triangle then p3q2\frac{p^3}{q^2} is a real number and p3q2>−274\frac{p^3}{q^2} > -\frac{27}{4}.

Hint

(i) sbisbi represents a vector perpendicular to the vector represented by bb. E1 Thus, the two points represented by a±sbia \pm sbi are equidistant from the point represented by aa E1 and they are joined to it by vectors which are perpendicular to that joining it to CC so they form a base of a triangle which has altitude from aa to a+ba + b and has two equal length sides, by Pythagoras. E1 (3)

Alternative Distance a+ba + b to a+sbia + sbi is ∣(a+sbi)−(a+b)∣=∣b∣∣si−1∣=∣b∣s2+1|(a + sbi) - (a + b)| = |b||si - 1| = |b|\sqrt{s^2 + 1} as ss is real, E1 and distance a+ba + b to a−sbia - sbi is ∣(a−sbi)−(a+b)∣=∣b∣∣−si−1∣=∣b∣s2+1|(a - sbi) - (a + b)| = |b||-si - 1| = |b|\sqrt{s^2 + 1} , E1 so two equal length sides. E1

aa is represented by the midpoint of the base. B1 bb is represented by the vector joining the midpoint of the base to the other vertex. B1 ss is the scale factor that the magnitude of the altitude is multiplied by to obtain half the base. B1

The sketch should show the vertical asymptote at x=−19x=-\frac{1}{9}, the oblique asymptote y=13x−1127y=\frac{1}{3}x-\frac{11}{27}, the intercepts (13,0)\left(\frac{1}{3},0\right) and (0,−1)(0,-1), and the stationary maximum at (−1,−1)(-1,-1). (3)

(ii) We require complex aa and bb and real ss such that

(a+sbi)+(a−sbi)+(a+b)=0⇒b=−3a(a + sbi) + (a - sbi) + (a + b) = 0 \Rightarrow b = -3a M1 A1

and

(a+sbi)(a−sbi)+(a−sbi)(a+b)+(a+b)(a+sbi)=p(a + sbi)(a - sbi) + (a - sbi)(a + b) + (a + b)(a + sbi) = p

so

a2+s2b2+2a(a+b)=p⇒3a2(3s2−1)=pa^2 + s^2b^2 + 2a(a + b) = p \Rightarrow 3a^2(3s^2 - 1) = p

A1

and

(a+sbi)(a−sbi)(a+b)=−q⇒−2a3(9s2+1)=−q(a + sbi)(a - sbi)(a + b) = -q \Rightarrow -2a^3(9s^2 + 1) = -q

Therefore

p3q2=[3a2(3s2−1)]3[2a3(9s2+1)]2=27(3s2−1)34(9s2+1)2\frac{p^3}{q^2} = \frac{[3a^2(3s^2 - 1)]^3}{[2a^3(9s^2 + 1)]^2} = \frac{27(3s^2 - 1)^3}{4(9s^2 + 1)^2}

A1* (5)

(iii)

y=(3x−1)3(9x+1)2y = \frac{(3x - 1)^3}{(9x + 1)^2}

has xx intercept at (13,0)(\frac{1}{3}, 0), yy intercept at (0,−1)(0, -1) G1 a vertical asymptote at x=−19x = -\frac{1}{9} and an asymptote y=13x−1127y = \frac{1}{3}x - \frac{11}{27} as x→±∞x \to \pm\infty. G1

dydx=(9x+1)29(3x−1)2−(3x−1)318(9x+1)(9x+1)4\frac{dy}{dx} = \frac{(9x + 1)^2 9(3x - 1)^2 - (3x - 1)^3 18(9x + 1)}{(9x + 1)^4} =9(3x−1)2(9x+1−6x+2)(9x+1)3=27(3x−1)2(x+1)(9x+1)3= \frac{9(3x - 1)^2 (9x + 1 - 6x + 2)}{(9x + 1)^3} = \frac{27(3x - 1)^2 (x + 1)}{(9x + 1)^3}

M1 A1

Thus, the stationary points are a maximum at (−1,−1)(-1, -1) and a point of inflection at (13,0)(\frac{1}{3}, 0). G1 G1

FeatureValue
xx-intercept(13,0)\left(\frac{1}{3}, 0\right)
yy-intercept(0,−1)(0, -1)
Maximum(−1,−1)(-1, -1)
Vertical asymptotex=−19x = -\frac{1}{9}
Slant asymptotey=13x−1127y = \frac{1}{3}x - \frac{11}{27}

(6)

(iv) If the roots of z3+pz+q=0z^3 + pz + q = 0 represent the vertices of an isosceles triangle, then by (ii), p3q2\frac{p^3}{q^2} must be real E1 and as s2>0s^2 > 0, from (iii) p3q2>274×−1=−274\frac{p^3}{q^2} > \frac{27}{4} \times -1 = \frac{-27}{4} E1 as y=(3x−1)3(9x+1)2y = \frac{(3x-1)^3}{(9x+1)^2} is increasing for x>0x > 0. E1 (3)

Model Solution

Part (i)

Let the three points be P=a+sbiP = a + sbi, Q=a−sbiQ = a - sbi, and R=a+bR = a + b.

We compute the distances from RR to each of PP and QQ:

∣R−P∣=∣(a+b)−(a+sbi)∣=∣b−sbi∣=∣b(1−si)∣=∣b∣ ∣1−si∣=∣b∣1+s2|R - P| = |(a + b) - (a + sbi)| = |b - sbi| = |b(1 - si)| = |b|\,|1 - si| = |b|\sqrt{1 + s^2}

∣R−Q∣=∣(a+b)−(a−sbi)∣=∣b+sbi∣=∣b(1+si)∣=∣b∣ ∣1+si∣=∣b∣1+s2|R - Q| = |(a + b) - (a - sbi)| = |b + sbi| = |b(1 + si)| = |b|\,|1 + si| = |b|\sqrt{1 + s^2}

Since ∣R−P∣=∣R−Q∣=∣b∣1+s2|R - P| = |R - Q| = |b|\sqrt{1 + s^2}, the triangle PQRPQR has two equal sides and is therefore isosceles. ■\qquad \blacksquare

For the explanation: given an isosceles triangle in the Argand diagram, we identify:

  • aa is the complex number represented by the midpoint of the base (the side that is not one of the two equal sides).
  • bb is the vector from the midpoint of the base to the apex (the vertex opposite the base).
  • ss is the ratio: (half the base length) / (altitude from apex to base). More precisely, if the base has length 2L2L and the altitude has length HH, then s=L/Hs = L/H.

Since bb is the vector from the midpoint of the base to the apex, the apex is at a+ba + b. The base is perpendicular to bb (rotated by 90∘90\circ), so the two base vertices are at a+sbia + sbi and a−sbia - sbi, where ss scales the perpendicular displacement relative to ∣b∣|b|.

Part (ii)

Let the three roots of z3+pz+q=0z^3 + pz + q = 0 be a+sbia + sbi, a−sbia - sbi, and a+ba + b, forming an isosceles triangle.

By Vieta’s formulas (noting the coefficient of z2z^2 is 0):

Sum of roots:

(a+sbi)+(a−sbi)+(a+b)=0(a + sbi) + (a - sbi) + (a + b) = 0

3a+b=0  ⟹  b=−3a...(1)3a + b = 0 \implies b = -3a \qquad \text{...(1)}

Sum of products of pairs:

(a+sbi)(a−sbi)+(a−sbi)(a+b)+(a+b)(a+sbi)=p(a + sbi)(a - sbi) + (a - sbi)(a + b) + (a + b)(a + sbi) = p

The first product is a2+s2b2a^2 + s^2 b^2. For the second and third products, using b=−3ab = -3a so a+b=−2aa + b = -2a:

(a−sbi)(−2a)+(−2a)(a+sbi)=−2a(a−sbi)−2a(a+sbi)=−2a⋅2a=−4a2(a - sbi)(-2a) + (-2a)(a + sbi) = -2a(a - sbi) - 2a(a + sbi) = -2a \cdot 2a = -4a^2

Therefore:

a2+s2b2−4a2=pa^2 + s^2 b^2 - 4a^2 = p

−3a2+9s2a2=p-3a^2 + 9s^2 a^2 = p

p=3a2(3s2−1)...(2)p = 3a^2(3s^2 - 1) \qquad \text{...(2)}

Product of roots:

(a+sbi)(a−sbi)(a+b)=−q(a + sbi)(a - sbi)(a + b) = -q

(a2+s2b2)(−2a)=−q(a^2 + s^2 b^2)(-2a) = -q

(a2+9s2a2)(−2a)=−q(a^2 + 9s^2 a^2)(-2a) = -q

q=2a3(1+9s2)...(3)q = 2a^3(1 + 9s^2) \qquad \text{...(3)}

Now we compute p3q2\frac{p^3}{q^2}:

p3q2=[3a2(3s2−1)]3[2a3(9s2+1)]2=27a6(3s2−1)34a6(9s2+1)2=27(3s2−1)34(9s2+1)2\frac{p^3}{q^2} = \frac{[3a^2(3s^2 - 1)]^3}{[2a^3(9s^2 + 1)]^2} = \frac{27a^6(3s^2 - 1)^3}{4a^6(9s^2 + 1)^2} = \frac{27(3s^2 - 1)^3}{4(9s^2 + 1)^2}

as required. ■\qquad \blacksquare

Part (iii)

Let y=(3x−1)3(9x+1)2y = \frac{(3x - 1)^3}{(9x + 1)^2}.

Intercepts:

  • xx-intercept: 3x−1=0  ⟹  x=133x - 1 = 0 \implies x = \frac{1}{3}, so the point is (13, 0)\left(\frac{1}{3},\, 0\right).
  • yy-intercept: x=0x = 0 gives y=(−1)312=−1y = \frac{(-1)^3}{1^2} = -1, so the point is (0, −1)(0,\, -1).

Asymptotes:

  • Vertical asymptote at 9x+1=09x + 1 = 0, i.e. x=−19x = -\frac{1}{9}.
  • As x→±∞x \to \pm\infty: performing polynomial long division of (3x−1)3=27x3−27x2+9x−1(3x-1)^3 = 27x^3 - 27x^2 + 9x - 1 by (9x+1)2=81x2+18x+1(9x+1)^2 = 81x^2 + 18x + 1:

27x3−27x2+9x−181x2+18x+1=13x−1127+lower order81x2+18x+1\frac{27x^3 - 27x^2 + 9x - 1}{81x^2 + 18x + 1} = \frac{1}{3}x - \frac{11}{27} + \frac{\text{lower order}}{81x^2 + 18x + 1}

So the slant asymptote is y=13x−1127y = \frac{1}{3}x - \frac{11}{27}.

Stationary points:

dydx=(9x+1)2⋅9(3x−1)2−(3x−1)3⋅18(9x+1)(9x+1)4\frac{dy}{dx} = \frac{(9x+1)^2 \cdot 9(3x-1)^2 - (3x-1)^3 \cdot 18(9x+1)}{(9x+1)^4}

=9(3x−1)2(9x+1)−18(3x−1)3(9x+1)3= \frac{9(3x-1)^2(9x+1) - 18(3x-1)^3}{(9x+1)^3}

=9(3x−1)2[(9x+1)−2(3x−1)](9x+1)3= \frac{9(3x-1)^2[(9x+1) - 2(3x-1)]}{(9x+1)^3}

=9(3x−1)2(9x+1−6x+2)(9x+1)3=9(3x−1)2(3x+3)(9x+1)3=27(3x−1)2(x+1)(9x+1)3= \frac{9(3x-1)^2(9x + 1 - 6x + 2)}{(9x+1)^3} = \frac{9(3x-1)^2(3x + 3)}{(9x+1)^3} = \frac{27(3x-1)^2(x+1)}{(9x+1)^3}

Setting dydx=0\frac{dy}{dx} = 0: the numerator vanishes when x=13x = \frac{1}{3} (double root) or x=−1x = -1.

At x=−1x = -1: y=(−4)3(−8)2=−6464=−1y = \frac{(-4)^3}{(-8)^2} = \frac{-64}{64} = -1.

Sign of dydx\frac{dy}{dx} near x=−1x = -1: The factor (3x−1)2>0(3x-1)^2 > 0 and (9x+1)3<0(9x+1)^3 < 0 near x=−1x = -1. For x<−1x < -1: (x+1)<0(x+1) < 0, so dydx=(+)(−)(−)>0\frac{dy}{dx} = \frac{(+)(-)}{(-)} > 0. For −1<x<−19-1 < x < -\frac{1}{9}: (x+1)>0(x+1) > 0, so dydx=(+)(+)(−)<0\frac{dy}{dx} = \frac{(+)(+)}{(-)} < 0. So x=−1x = -1 is a local maximum.

At x=13x = \frac{1}{3}: y=0y = 0. The factor (3x−1)2≥0(3x-1)^2 \geq 0 means dydx\frac{dy}{dx} does not change sign here; this is a point of inflection.

Sketch summary:

  • The curve passes through (0,−1)(0, -1) and (13,0)\left(\frac{1}{3}, 0\right).
  • There is a local maximum at (−1,−1)(-1, -1).
  • There is a vertical asymptote at x=−19x = -\frac{1}{9}.
  • As x→−19−x \to -\frac{1}{9}^-, y→−∞y \to -\infty; as x→−19+x \to -\frac{1}{9}^+, y→+∞y \to +\infty.
  • The curve approaches the slant asymptote y=13x−1127y = \frac{1}{3}x - \frac{11}{27} for large ∣x∣|x|.

Part (iv)

From part (ii), if the roots form an isosceles triangle, then

p3q2=27(3s2−1)34(9s2+1)2\frac{p^3}{q^2} = \frac{27(3s^2 - 1)^3}{4(9s^2 + 1)^2}

for some non-zero real ss. Since ss is real, s2s^2 is a positive real number, so the right-hand side is real. Therefore p3q2\frac{p^3}{q^2} is real. ■\qquad \blacksquare

Now let x=s2>0x = s^2 > 0, so p3q2=27(3x−1)34(9x+1)2=274⋅(3x−1)3(9x+1)2\frac{p^3}{q^2} = \frac{27(3x - 1)^3}{4(9x + 1)^2} = \frac{27}{4} \cdot \frac{(3x - 1)^3}{(9x + 1)^2}.

From part (iii), the stationary points of f(x)=(3x−1)3(9x+1)2f(x) = \frac{(3x-1)^3}{(9x+1)^2} occur at x=−1x = -1 and x=13x = \frac{1}{3}.

For x>0x > 0: the only stationary point is x=13x = \frac{1}{3} where f ⁣(13)=0f\!\left(\frac{1}{3}\right) = 0, and this is a point of inflection (not a maximum or minimum). Since f(0)=−1f(0) = -1 and f(x)→+∞f(x) \to +\infty as x→+∞x \to +\infty, the function is increasing on (0,∞)(0,\infty), with a horizontal tangent at x=13x=\frac{1}{3}.

Therefore, for all x>0x > 0:

f(x)⩾f(0)=−1f(x) \geqslant f(0) = -1

(with the infimum −1-1 approached as x→0+x \to 0^+ but x>0x > 0). Thus f(x)>−1f(x)>-1 for all x>0x>0.

Hence:

p3q2=274f(s2)>274⋅(−1)=−274\frac{p^3}{q^2} = \frac{27}{4} f(s^2) > \frac{27}{4} \cdot (-1) = -\frac{27}{4}

■\qquad \blacksquare

Examiner Notes

最不受欢迎的纯数题(45%作答),平均分6/20。常见错误:将 a 和 b 误视为实数;第(iii)部分图像差异大,少有人指定无穷远处渐近行为和拐点性质;第(iv)部分未能从图中正确推导不等式。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

4 Let nn be a positive integer. The polynomial p is defined by the identity

p(cos⁡θ)≡cos⁡((2n+1)θ)+1.p(\cos \theta) \equiv \cos ((2n + 1)\theta) + 1 .

(i) Show that

cos⁡((2n+1)θ)=∑r=0n(2n+12r)cos⁡2n+1−2rθ(cos⁡2θ−1)r.\cos ((2n + 1)\theta) = \sum_{r=0}^{n} \binom{2n + 1}{2r} \cos^{2n+1-2r} \theta(\cos^2 \theta - 1)^r .

(ii) By considering the expansion of (1+t)2n+1(1 + t)^{2n+1} for suitable values of tt, show that the coefficient of x2n+1x^{2n+1} in the polynomial p(x)p(x) is 22n2^{2n}.

(iii) Show that the coefficient of x2n−1x^{2n-1} in the polynomial p(x)p(x) is −(2n+1)22n−2-(2n + 1)2^{2n-2}.

(iv) It is given that there exists a polynomial q such that

p(x)=(x+1)[q(x)]2p(x) = (x + 1) [q(x)]^2

and the coefficient of xnx^n in q(x)q(x) is greater than 0.

Write down the coefficient of xnx^n in the polynomial q(x)q(x) and, for n⩾2n \geqslant 2, show that the coefficient of xn−2x^{n-2} in the polynomial q(x)q(x) is

2n−2(1−n).2^{n-2}(1 - n) .

Hint

(i) By de Moivre,

cos⁡((2n+1)θ)+isin⁡((2n+1)θ)=(cos⁡θ+isin⁡θ)2n+1\cos((2n + 1)\theta) + i \sin((2n + 1)\theta) = (\cos \theta + i \sin \theta)^{2n+1}

Expanding by the binomial theorem and equating real parts

cos⁡((2n+1)θ)=cos⁡2n+1θ−(2n+12)cos⁡2n−1θsin⁡2θ+⋯+(−1)n(2n+12n)cos⁡θsin⁡2nθ\cos((2n + 1)\theta) = \cos^{2n+1} \theta - \binom{2n + 1}{2} \cos^{2n-1} \theta \sin^2 \theta + \dots + (-1)^n \binom{2n + 1}{2n} \cos \theta \sin^{2n} \theta

M1 A1

=cos⁡2n+1θ+(2n+12)cos⁡2n−1θ(cos⁡2θ−1)+⋯+(2n+12n)cos⁡θ(cos⁡2θ−1)n= \cos^{2n+1} \theta + \binom{2n + 1}{2} \cos^{2n-1} \theta (\cos^2 \theta - 1) + \dots + \binom{2n + 1}{2n} \cos \theta (\cos^2 \theta - 1)^n

M1

=∑r=0n(2n+12r)cos⁡2n+1−2rθ(cos⁡2θ−1)r= \sum_{r=0}^{n} \binom{2n + 1}{2r} \cos^{2n+1-2r} \theta (\cos^2 \theta - 1)^r

A1* (4)

Notice, for (iv), that this expression only contains odd powers of cos⁡θ\cos \theta.

(ii) The coefficient of x2n+1x^{2n+1} in p(x)p(x) is

∑r=0n(2n+12r)\sum_{r=0}^{n} \binom{2n + 1}{2r}

B1

(1+x)2n+1=∑r=02n+1(2n+1r)xr=∑r=0n(2n+12r)x2r+∑r=0n(2n+12r+1)x2r+1(1 + x)^{2n+1} = \sum_{r=0}^{2n+1} \binom{2n + 1}{r} x^r = \sum_{r=0}^{n} \binom{2n + 1}{2r} x^{2r} + \sum_{r=0}^{n} \binom{2n + 1}{2r + 1} x^{2r+1}

Substituting x=1x = 1,

22n+1=∑r=0n(2n+12r)+∑r=0n(2n+12r+1)2^{2n+1} = \sum_{r=0}^{n} \binom{2n + 1}{2r} + \sum_{r=0}^{n} \binom{2n + 1}{2r + 1}

and substituting x=−1x = -1,

M1

0=∑r=0n(2n+12r)−∑r=0n(2n+12r+1)0 = \sum_{r=0}^{n} \binom{2n + 1}{2r} - \sum_{r=0}^{n} \binom{2n + 1}{2r + 1}

A1

Adding these two results,

22n+1=2∑r=0n(2n+12r)2^{2n+1} = 2 \sum_{r=0}^{n} \binom{2n + 1}{2r}

and so the required coefficient is 22n2^{2n} as required. A1 (4)*

(iii) The coefficient of x2n−1x^{2n-1} in p(x)p(x) is

∑r=0n−r(2n+12r)\sum_{r=0}^{n} -r \binom{2n+1}{2r} B1

As

(1+x)2n+1=∑r=02n+1(2n+1r)xr=∑r=0n(2n+12r)x2r+∑r=0n(2n+12r+1)x2r+1(1+x)^{2n+1} = \sum_{r=0}^{2n+1} \binom{2n+1}{r} x^r = \sum_{r=0}^{n} \binom{2n+1}{2r} x^{2r} + \sum_{r=0}^{n} \binom{2n+1}{2r+1} x^{2r+1}

differentiating with respect to xx

(2n+1)(1+x)2n=∑r=0n2r(2n+12r)x2r−1+∑r=0n(2r+1)(2n+12r+1)x2r(2n+1)(1+x)^{2n} = \sum_{r=0}^{n} 2r \binom{2n+1}{2r} x^{2r-1} + \sum_{r=0}^{n} (2r+1) \binom{2n+1}{2r+1} x^{2r}

M1

Substituting x=1x=1,

(2n+1)22n=∑r=0n2r(2n+12r)+∑r=0n(2r+1)(2n+12r+1)(2n+1)2^{2n} = \sum_{r=0}^{n} 2r \binom{2n+1}{2r} + \sum_{r=0}^{n} (2r+1) \binom{2n+1}{2r+1} M1

and substituting x=−1x=-1,

0=−∑r=0n2r(2n+12r)+∑r=0n(2r+1)(2n+12r+1)0 = -\sum_{r=0}^{n} 2r \binom{2n+1}{2r} + \sum_{r=0}^{n} (2r+1) \binom{2n+1}{2r+1} A1

Subtracting these two results

(2n+1)22n=2∑r=0n2r(2n+12r)=4∑r=0nr(2n+12r)(2n+1)2^{2n} = 2 \sum_{r=0}^{n} 2r \binom{2n+1}{2r} = 4 \sum_{r=0}^{n} r \binom{2n+1}{2r}

and so the required coefficient is

−(2n+1)22n÷4=−(2n+1)22n−2-(2n+1)2^{2n} \div 4 = -(2n+1)2^{2n-2} A1* (5)

Alternative

∑r=0n−r(2n+12r)=−∑r=0nr(2n+1)!(2n−2r+1)!(2r)!=−2n+12∑r=1n(2n)!(2n−2r+1)!(2r−1)!\sum_{r=0}^{n} -r \binom{2n+1}{2r} = -\sum_{r=0}^{n} r \frac{(2n+1)!}{(2n-2r+1)! (2r)!} = -\frac{2n+1}{2} \sum_{r=1}^{n} \frac{(2n)!}{(2n-2r+1)! (2r-1)!}

=−2n+12∑r=1n(2n2r−1)=−2n+12∑r=0n−1(2n2r+1)= -\frac{2n+1}{2} \sum_{r=1}^{n} \binom{2n}{2r-1} = -\frac{2n+1}{2} \sum_{r=0}^{n-1} \binom{2n}{2r+1} M1

As in (ii),

∑r=0n−1(2n2r+1)=1222n\sum_{r=0}^{n-1} \binom{2n}{2r+1} = \frac{1}{2} 2^{2n} A1

so

∑r=0n−r(2n+12r)=−2n+121222n=−(2n+1)22n−2\sum_{r=0}^{n} -r \binom{2n+1}{2r} = -\frac{2n+1}{2} \frac{1}{2} 2^{2n} = -(2n+1) 2^{2n-2} A1 (5)*

(iv) Suppose

q(x)=axn+bxn−1+cxn−2+…q(x) = ax^n + bx^{n-1} + cx^{n-2} + \dots

then

p(x)=(x+1)[axn+bxn−1+cxn−2+… ]2p(x) = (x+1) [ax^n + bx^{n-1} + cx^{n-2} + \dots]^2 =(x+1)(a2x2n+2abx2n−1+(b2+2ac)x2n−2+… )= (x+1) (a^2 x^{2n} + 2ab x^{2n-1} + (b^2 + 2ac) x^{2n-2} + \dots) =a2x2n+1+(a2+2ab)x2n+(b2+2ac+2ab)x2n−1+…= a^2 x^{2n+1} + (a^2 + 2ab) x^{2n} + (b^2 + 2ac + 2ab) x^{2n-1} + \dots

M1 A1

Thus a2=22na^2 = 2^{2n}, a2+2ab=0a^2 + 2ab = 0, and b2+2ac+2ab=−(2n+1)22n−2b^2 + 2ac + 2ab = -(2n+1) 2^{2n-2} dM1 A1

Therefore a=2na = 2^n (as a>0a > 0), B1

b=−a2=−2n−1b = \frac{-a}{2} = -2^{n-1} A1

and

22n−2+2n+1c−22n=−(2n+1)22n−22^{2n-2} + 2^{n+1}c - 2^{2n} = -(2n+1) 2^{2n-2}

so

2n−3+c−2n−1=−(2n+1)2n−32^{n-3} + c - 2^{n-1} = -(2n+1) 2^{n-3} c=2n−3(4−1−2n−1)=2n−2(1−n)c = 2^{n-3} (4 - 1 - 2n - 1) = 2^{n-2} (1 - n)

as required. A1(7)*

Model Solution

Part (i)

By de Moivre’s theorem:

cos⁡((2n+1)θ)+isin⁡((2n+1)θ)=(cos⁡θ+isin⁡θ)2n+1\cos((2n+1)\theta) + i\sin((2n+1)\theta) = (\cos\theta + i\sin\theta)^{2n+1}

Expanding the right-hand side by the binomial theorem:

(cos⁡θ+isin⁡θ)2n+1=∑k=02n+1(2n+1k)cos⁡2n+1−kθ⋅(isin⁡θ)k(\cos\theta + i\sin\theta)^{2n+1} = \sum_{k=0}^{2n+1} \binom{2n+1}{k} \cos^{2n+1-k}\theta \cdot (i\sin\theta)^k

The real part consists of terms where kk is even (so that iki^k is real). Setting k=2rk = 2r for r=0,1,…,nr = 0, 1, \ldots, n:

cos⁡((2n+1)θ)=∑r=0n(2n+12r)cos⁡2n+1−2rθ⋅(isin⁡θ)2r\cos((2n+1)\theta) = \sum_{r=0}^{n} \binom{2n+1}{2r} \cos^{2n+1-2r}\theta \cdot (i\sin\theta)^{2r}

Since i2r=(−1)ri^{2r} = (-1)^r and sin⁡2rθ=(1−cos⁡2θ)r\sin^{2r}\theta = (1 - \cos^2\theta)^r, we have (isin⁡θ)2r=(−1)rsin⁡2rθ=(cos⁡2θ−1)r(i\sin\theta)^{2r} = (-1)^r \sin^{2r}\theta = (\cos^2\theta - 1)^r.

Therefore:

cos⁡((2n+1)θ)=∑r=0n(2n+12r)cos⁡2n+1−2rθ (cos⁡2θ−1)r\cos((2n+1)\theta) = \sum_{r=0}^{n} \binom{2n+1}{2r} \cos^{2n+1-2r}\theta\,(\cos^2\theta - 1)^r

■\qquad \blacksquare

Part (ii)

Setting x=cos⁡θx = \cos\theta and t=cos⁡2θ−1=x2−1t = \cos^2\theta - 1 = x^2 - 1, the result of part (i) gives:

cos⁡((2n+1)θ)=∑r=0n(2n+12r)x2n+1−2r tr\cos((2n+1)\theta) = \sum_{r=0}^{n} \binom{2n+1}{2r} x^{2n+1-2r}\, t^r

Note that x2n+1−2r=x⋅x2(n−r)=x⋅(x2)n−r=x⋅(t+1)n−rx^{2n+1-2r} = x \cdot x^{2(n-r)} = x \cdot (x^2)^{n-r} = x \cdot (t+1)^{n-r}, so each term contains only odd powers of xx. Therefore p(x)=cos⁡((2n+1)θ)+1p(x) = \cos((2n+1)\theta) + 1 is indeed a polynomial in xx with the same leading terms.

The coefficient of x2n+1x^{2n+1} in p(x)p(x) is obtained by taking the leading term from each summand, which gives:

coefficient of x2n+1=∑r=0n(2n+12r)\text{coefficient of } x^{2n+1} = \sum_{r=0}^{n} \binom{2n+1}{2r}

Now consider the expansion of (1+t)2n+1(1 + t)^{2n+1}:

(1+t)2n+1=∑r=02n+1(2n+1r)tr(1+t)^{2n+1} = \sum_{r=0}^{2n+1} \binom{2n+1}{r} t^r

Substituting t=1t = 1:

22n+1=∑r=02n+1(2n+1r)=∑r=0n(2n+12r)+∑r=0n(2n+12r+1)...(1)2^{2n+1} = \sum_{r=0}^{2n+1} \binom{2n+1}{r} = \sum_{r=0}^{n} \binom{2n+1}{2r} + \sum_{r=0}^{n} \binom{2n+1}{2r+1} \qquad \text{...(1)}

Substituting t=−1t = -1:

0=∑r=02n+1(2n+1r)(−1)r=∑r=0n(2n+12r)−∑r=0n(2n+12r+1)...(2)0 = \sum_{r=0}^{2n+1} \binom{2n+1}{r}(-1)^r = \sum_{r=0}^{n} \binom{2n+1}{2r} - \sum_{r=0}^{n} \binom{2n+1}{2r+1} \qquad \text{...(2)}

Adding equations (1) and (2):

22n+1=2∑r=0n(2n+12r)2^{2n+1} = 2\sum_{r=0}^{n} \binom{2n+1}{2r}

∑r=0n(2n+12r)=22n\sum_{r=0}^{n} \binom{2n+1}{2r} = 2^{2n}

Therefore the coefficient of x2n+1x^{2n+1} in p(x)p(x) is 22n2^{2n}. ■\qquad \blacksquare

Part (iii)

From part (i), each term in the sum ∑r=0n(2n+12r)x2n+1−2r(x2−1)r\sum_{r=0}^{n} \binom{2n+1}{2r} x^{2n+1-2r}(x^2 - 1)^r contributes to the coefficient of x2n−1x^{2n-1} when the expansion of (x2−1)r(x^2 - 1)^r produces a term with x2(r−1)x^{2(r-1)}, i.e. from the constant in (x2−1)r(x^2-1)^r times x2n+1−2rx^{2n+1-2r} we get x2n+1−2rx^{2n+1-2r}, and from the x2x^2 term of (x2−1)r(x^2-1)^r (which has coefficient −r-r from choosing one factor of x2x^2 and r−1r-1 factors of −1-1) times x2n+1−2rx^{2n+1-2r} we get x2n+3−2rx^{2n+3-2r}.

More precisely, the contribution to x2n−1x^{2n-1} from the rr-th term requires:

x2n+1−2r⋅(term of degree 2r−2 in (x2−1)r)x^{2n+1-2r} \cdot (\text{term of degree } 2r - 2 \text{ in } (x^2-1)^r)

Consider the identity from part (i) with t=x2−1t = x^2 - 1:

cos⁡((2n+1)θ)+1=∑r=0n(2n+12r)x2n+1−2r(x2−1)r+1\cos((2n+1)\theta) + 1 = \sum_{r=0}^{n} \binom{2n+1}{2r} x^{2n+1-2r}(x^2 - 1)^r + 1

The term x2n+1−2r(x2−1)rx^{2n+1-2r}(x^2-1)^r can be expanded. Its contribution to the coefficient of x2n−1x^{2n-1} requires (x2−1)r(x^2-1)^r to contribute x2r−2x^{2r-2}, which means choosing exactly one factor of (−1)(-1) from rr factors (coefficient −r-r) times x2(r−1)x^{2(r-1)} from the remaining factors. So the contribution is (2n+12r)⋅(−r)\binom{2n+1}{2r} \cdot (-r).

Therefore the coefficient of x2n−1x^{2n-1} in p(x)p(x) is:

∑r=0n−r(2n+12r)\sum_{r=0}^{n} -r\binom{2n+1}{2r}

To evaluate this, consider the binomial expansion:

(1+t)2n+1=∑k=02n+1(2n+1k)tk(1+t)^{2n+1} = \sum_{k=0}^{2n+1}\binom{2n+1}{k}t^k

Differentiating with respect to tt:

(2n+1)(1+t)2n=∑k=12n+1k(2n+1k)tk−1(2n+1)(1+t)^{2n} = \sum_{k=1}^{2n+1} k\binom{2n+1}{k}t^{k-1}

Substituting t=1t = 1:

(2n+1)22n=∑k=12n+1k(2n+1k)=∑r=0n2r(2n+12r)+∑r=0n(2r+1)(2n+12r+1)...(3)(2n+1)2^{2n} = \sum_{k=1}^{2n+1} k\binom{2n+1}{k} = \sum_{r=0}^{n} 2r\binom{2n+1}{2r} + \sum_{r=0}^{n}(2r+1)\binom{2n+1}{2r+1} \qquad \text{...(3)}

Substituting t=−1t = -1:

0=∑k=12n+1k(2n+1k)(−1)k−1=∑r=0n2r(2n+12r)(−1)2r−1+∑r=0n(2r+1)(2n+12r+1)(−1)2r0 = \sum_{k=1}^{2n+1} k\binom{2n+1}{k}(-1)^{k-1} = \sum_{r=0}^{n} 2r\binom{2n+1}{2r}(-1)^{2r-1} + \sum_{r=0}^{n}(2r+1)\binom{2n+1}{2r+1}(-1)^{2r}

=−∑r=0n2r(2n+12r)+∑r=0n(2r+1)(2n+12r+1)...(4)= -\sum_{r=0}^{n} 2r\binom{2n+1}{2r} + \sum_{r=0}^{n}(2r+1)\binom{2n+1}{2r+1} \qquad \text{...(4)}

Subtracting (4) from (3):

(2n+1)22n=2∑r=0n2r(2n+12r)=4∑r=0nr(2n+12r)(2n+1)2^{2n} = 2\sum_{r=0}^{n} 2r\binom{2n+1}{2r} = 4\sum_{r=0}^{n} r\binom{2n+1}{2r}

Therefore:

∑r=0nr(2n+12r)=(2n+1)22n4=(2n+1)22n−2\sum_{r=0}^{n} r\binom{2n+1}{2r} = \frac{(2n+1)2^{2n}}{4} = (2n+1)2^{2n-2}

The coefficient of x2n−1x^{2n-1} in p(x)p(x) is:

−∑r=0nr(2n+12r)=−(2n+1)22n−2-\sum_{r=0}^{n} r\binom{2n+1}{2r} = -(2n+1)2^{2n-2}

■\qquad \blacksquare

Part (iv)

From parts (ii) and (iii), p(x)=22nx2n+1−(2n+1)22n−2x2n−1+…p(x) = 2^{2n}x^{2n+1} - (2n+1)2^{2n-2}x^{2n-1} + \ldots (only odd powers of xx appear, plus the constant term +1+1).

Write q(x)=axn+bxn−1+cxn−2+…q(x) = ax^n + bx^{n-1} + cx^{n-2} + \ldots with a>0a > 0.

Then:

[q(x)]2=a2x2n+2abx2n−1+(b2+2ac)x2n−2+…[q(x)]^2 = a^2x^{2n} + 2abx^{2n-1} + (b^2 + 2ac)x^{2n-2} + \ldots

Multiplying by (x+1)(x+1):

(x+1)[q(x)]2=a2x2n+1+(a2+2ab)x2n+(b2+2ac+2ab)x2n−1+…(x+1)[q(x)]^2 = a^2x^{2n+1} + (a^2 + 2ab)x^{2n} + (b^2 + 2ac + 2ab)x^{2n-1} + \ldots

Coefficient of x2n+1x^{2n+1}:

a2=22n  ⟹  a=2n(a>0)a^2 = 2^{2n} \implies a = 2^n \qquad (a > 0)

Coefficient of x2nx^{2n}:

Since p(x)p(x) contains only odd powers of xx (from part (i), every term has odd degree in cos⁡θ\cos\theta), the coefficient of x2nx^{2n} in p(x)p(x) is 00:

a2+2ab=0  ⟹  22n+2⋅2n⋅b=0  ⟹  b=−22n2n+1=−2n−1a^2 + 2ab = 0 \implies 2^{2n} + 2 \cdot 2^n \cdot b = 0 \implies b = -\frac{2^{2n}}{2^{n+1}} = -2^{n-1}

Coefficient of x2n−1x^{2n-1}:

b2+2ac+2ab=−(2n+1)22n−2b^2 + 2ac + 2ab = -(2n+1)2^{2n-2}

Substituting a=2na = 2^n and b=−2n−1b = -2^{n-1}:

(−2n−1)2+2⋅2n⋅c+2⋅2n⋅(−2n−1)=−(2n+1)22n−2(-2^{n-1})^2 + 2 \cdot 2^n \cdot c + 2 \cdot 2^n \cdot (-2^{n-1}) = -(2n+1)2^{2n-2}

22n−2+2n+1c−22n=−(2n+1)22n−22^{2n-2} + 2^{n+1}c - 2^{2n} = -(2n+1)2^{2n-2}

2n+1c=−(2n+1)22n−2−22n−2+22n2^{n+1}c = -(2n+1)2^{2n-2} - 2^{2n-2} + 2^{2n}

2n+1c=22n−2[−(2n+1)−1+4]=22n−2(2−2n)2^{n+1}c = 2^{2n-2}[-(2n+1) - 1 + 4] = 2^{2n-2}(2 - 2n)

c=22n−2⋅2(1−n)2n+1=22n−1−n−1(1−n)=2n−2(1−n)c = \frac{2^{2n-2} \cdot 2(1-n)}{2^{n+1}} = 2^{2n-1-n-1}(1-n) = 2^{n-2}(1-n)

Therefore the coefficient of xnx^n in q(x)q(x) is 2n\boxed{2^n}, and the coefficient of xn−2x^{n-2} in q(x)q(x) is 2n−2(1−n)2^{n-2}(1-n). ■\qquad \blacksquare

Examiner Notes

全卷最难(平均分5/20)。大多数考生仅在第(i)部分有实质性进展。第(ii)部分常见错误:写下系数后无进展或未利用代入 t=±1 的技巧。第(iv)部分几乎仅被前三部分成功的考生尝试。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

5 (i) Show that if 1x+2y=27,\frac{1}{x} + \frac{2}{y} = \frac{2}{7}, then (2x−7)(y−7)=49(2x - 7)(y - 7) = 49.

By considering the factors of 49, find all the pairs of positive integers xx and yy such that 1x+2y=27.\frac{1}{x} + \frac{2}{y} = \frac{2}{7}.

(ii) Let pp and qq be prime numbers such that p2+pq+q2=n2p^2 + pq + q^2 = n^2 where nn is a positive integer. Show that (p+q+n)(p+q−n)=pq(p + q + n)(p + q - n) = pq and hence explain why p+q=n+1p + q = n + 1.

Hence find the possible values of pp and qq.

(iii) Let pp and qq be positive and p3+q3+3pq2=n3.p^3 + q^3 + 3pq^2 = n^3. Show that p+q−n<pp + q - n < p and p+q−n<qp + q - n < q.

Show that there are no prime numbers pp and qq such that p3+q3+3pq2p^3 + q^3 + 3pq^2 is the cube of an integer.

Hint

(i)

1x+2y=27\frac{1}{x} + \frac{2}{y} = \frac{2}{7}

7y+14x=2xy7y + 14x = 2xy 2xy−7y−14x+49=492xy - 7y - 14x + 49 = 49 (2x−7)(y−7)=49(2x - 7)(y - 7) = 49 B1*

Thus 2x−7=1,y−7=492x - 7 = 1, y - 7 = 49, or 2x−7=7,y−7=72x - 7 = 7, y - 7 = 7, or 2x−7=49,y−7=12x - 7 = 49, y - 7 = 1

M1

and so (x,y)=(4,56),(7,14)(x, y) = (4, 56), (7, 14), or (28,8)(28, 8) A1 (3)

(ii)

p2+pq+q2=n2p^2 + pq + q^2 = n^2 p2+2pq+q2−n2=pqp^2 + 2pq + q^2 - n^2 = pq (p+q)2−n2=pq(p + q)^2 - n^2 = pq (p+q+n)(p+q−n)=pq(p + q + n)(p + q - n) = pq

B1*

p+q+n≠pp + q + n \neq p and p+q+n≠qp + q + n \neq q as p,qp, q, and nn are all positive. p+q+n>p+q−np + q + n > p + q - n so p+q+n≠1p + q + n \neq 1 as that would require p+q−n=pq>1p + q - n = pq > 1. M1

Thus p+q+n=pqp + q + n = pq and p+q−n=1p + q - n = 1 as required. A1*

Therefore p+q+p+q−1=pqp + q + p + q - 1 = pq M1

pq−2p−2q+4=3pq - 2p - 2q + 4 = 3

(p−2)(q−2)=3(p - 2)(q - 2) = 3

dM1

Thus p−2=1,q−2=3p - 2 = 1, q - 2 = 3, or p−2=3,q−2=1p - 2 = 3, q - 2 = 1

Alternative (I)

pq−2p−2q+4=3pq - 2p - 2q + 4 = 3

pq−2p−2q+1=0pq - 2p - 2q + 1 = 0

p(q−2)=2q−1p(q - 2) = 2q - 1

p=2q−1q−2=2+3q−2p = \frac{2q - 1}{q - 2} = 2 + \frac{3}{q - 2}

as q≠2q \neq 2 (q=2q = 2 would yield -4+4-3=0) so q−2=1q - 2 = 1 or 33 E1

and so (p,q)=(3,5)(p, q) = (3, 5), or (5,3)(5, 3) A1 (6)

Alternative (II) p+q+n=pqp + q + n = pq and p+q−n=1p + q - n = 1 yield p+q=n+1p + q = n + 1 and pq=2n+1pq = 2n + 1

Therefore, pp and qq are solutions of t2−(n+1)t+(2n+1)=0t^2 - (n + 1)t + (2n + 1) = 0

Hence t=(n+1)±(n+1)2−4(2n+1)2=(n+1)±(n−3)2+122t = \frac{(n+1) \pm \sqrt{(n+1)^2 - 4(2n+1)}}{2} = \frac{(n+1) \pm \sqrt{(n-3)^2 + 12}}{2}

For integer tt we require that (n−3)2+12(n - 3)^2 + 12 is a perfect square (in fact an even perfect square).

Thus the difference of squares between (n−3)2+12(n - 3)^2 + 12 and (n−3)2(n - 3)^2 is 12. Successive squares, z2z^2 and (z+1)2(z + 1)^2 differ by 2z+12z + 1, which for z≥6z \ge 6 is ≥13\ge 13. Thus (n−3)≤5(n - 3) \le 5. Then, either by listing potential solutions exhaustively, or justifying that (n−3)2+12(n - 3)^2 + 12 and (n−3)2(n - 3)^2 have to be squares differing by 7+57 + 5 and hence (n−3)2=22(n - 3)^2 = 2^2 giving (p,q)=(3,5)(p, q) = (3, 5), or (5,3)(5, 3). E1 A1 (6)

(iii) If p3+q3+3pq2=n3p^3 + q^3 + 3pq^2 = n^3, and as p,qp, q, and hence nn are all positive, then p3<n3p^3 < n^3 and

q3<n3q^3 < n^3 so p<np < n and q<nq < n, E1 and hence p+q−n<pp + q - n < p and p+q−n<qp + q - n < q. A1*

If p3+q3+3pq2+3p2q=n3+3p2qp^3 + q^3 + 3pq^2 + 3p^2q = n^3 + 3p^2q M1 (p+q)3−n3=3p2q(p + q)^3 - n^3 = 3p^2q dM1

(p+q−n)((p+q)2+(p+q)n+n2)=3p2q(p + q - n)((p + q)^2 + (p + q)n + n^2) = 3p^2q A1

As p+q−n<pp + q - n < p and p+q−n<qp + q - n < q, so p+q−n=1p + q - n = 1 or 33 A1

If p+q−n=1p + q - n = 1 then (n+1)3−n3=3p2q(n + 1)^3 - n^3 = 3p^2q and hence 3n2+3n+1=3p2q3n^2 + 3n + 1 = 3p^2q M1 which is not possible as LHS is not a multiple of 3 and RHS is. E1

If p+q−n=3p + q - n = 3, then (n+3)3−n3=3p2q(n + 3)^3 - n^3 = 3p^2q and hence 9n2+27n+27=3p2q9n^2 + 27n + 27 = 3p^2q, that is

3(n2+3n+3)=p2q3(n^2 + 3n + 3) = p^2q. M1 So pp or qq must divide 3 and hence must be 3 as pp and qq are prime. E1

If p=3p = 3, then q−n=0q - n = 0 but q<nq < n and vice versa if q=3q = 3 E1* (11)

Model Solution

Part (i)

Starting from 1x+2y=27\frac{1}{x} + \frac{2}{y} = \frac{2}{7}, multiply both sides by 7xy7xy:

7y+14x=2xy7y + 14x = 2xy

Rearranging:

2xy−14x−7y=02xy - 14x - 7y = 0

We use the factorisation technique: add 49 to both sides:

2xy−14x−7y+49=492xy - 14x - 7y + 49 = 49

Factor by grouping: take 2x2x from the first two terms and −7-7 from the last two:

2x(y−7)−7(y−7)=492x(y - 7) - 7(y - 7) = 49

(2x−7)(y−7)=49■(2x - 7)(y - 7) = 49 \qquad \blacksquare

Now we find all positive integer solutions. Since xx and yy are positive integers, we need 2x−72x - 7 and y−7y - 7 to be integer factors of 49. Also, since 1x+2y=27\frac{1}{x} + \frac{2}{y} = \frac{2}{7} with x,y>0x, y > 0, we need x>72x > \frac{7}{2} (i.e., x≥4x \geq 4) and y>7y > 7 (i.e., y≥8y \geq 8), so 2x−7≥12x - 7 \geq 1 and y−7≥1y - 7 \geq 1. Therefore both factors must be positive.

The positive factor pairs of 49=7249 = 7^2 are (1,49)(1, 49), (7,7)(7, 7), and (49,1)(49, 1).

Case 1: 2x−7=12x - 7 = 1, y−7=49y - 7 = 49, giving x=4x = 4, y=56y = 56.

Case 2: 2x−7=72x - 7 = 7, y−7=7y - 7 = 7, giving x=7x = 7, y=14y = 14.

Case 3: 2x−7=492x - 7 = 49, y−7=1y - 7 = 1, giving x=28x = 28, y=8y = 8.

The solutions are (x,y)=(4,56)(x, y) = (4, 56), (7,14)(7, 14), and (28,8)(28, 8).

Part (ii)

Starting from p2+pq+q2=n2p^2 + pq + q^2 = n^2, we add pqpq to both sides:

p2+2pq+q2=n2+pqp^2 + 2pq + q^2 = n^2 + pq

(p+q)2−n2=pq(p + q)^2 - n^2 = pq

(p+q+n)(p+q−n)=pq■(p + q + n)(p + q - n) = pq \qquad \blacksquare

Since pp, qq, and nn are all positive, we have p+q+n>p+q−np + q + n > p + q - n (as n>0n > 0). We also note p+q+n>pp + q + n > p and p+q+n>qp + q + n > q (since q+n>0q + n > 0 and p+n>0p + n > 0).

Now (p+q+n)(p+q−n)=pq(p + q + n)(p + q - n) = pq, and pqpq is a positive integer. Since pp and qq are prime, the only positive factorisations of pqpq are 1×pq1 \times pq, p×qp \times q, q×pq \times p, and pq×1pq \times 1.

Since p+q+np + q + n cannot equal 1 (it exceeds p≥2p \geq 2), and p+q+np + q + n cannot equal pp or qq (it exceeds both), the only possibility is:

p+q+n=pqandp+q−n=1p + q + n = pq \qquad \text{and} \qquad p + q - n = 1

From the second equation: n=p+q−1n = p + q - 1. Substituting into the first:

p+q+(p+q−1)=pqp + q + (p + q - 1) = pq

2p+2q−1=pq2p + 2q - 1 = pq

pq−2p−2q=−1pq - 2p - 2q = -1

(p−2)(q−2)=3(p - 2)(q - 2) = 3

Since pp and qq are prime, p−2p - 2 and q−2q - 2 are integers. The factor pairs of 3 are (1,3)(1, 3) and (3,1)(3, 1) (we exclude negative pairs as they give p≤0p \leq 0 or q≤0q \leq 0).

Case 1: p−2=1p - 2 = 1, q−2=3q - 2 = 3, giving p=3p = 3, q=5q = 5.

Case 2: p−2=3p - 2 = 3, q−2=1q - 2 = 1, giving p=5p = 5, q=3q = 3.

Verification: 32+3⋅5+52=9+15+25=49=723^2 + 3 \cdot 5 + 5^2 = 9 + 15 + 25 = 49 = 7^2, so n=7n = 7.

The possible values are (p,q)=(3,5)(p, q) = (3, 5) or (5,3)(5, 3).

Part (iii)

First, we show p+q−n<pp + q - n < p and p+q−n<qp + q - n < q.

Since pp and qq are positive, p3>0p^3 > 0 and q3>0q^3 > 0, so from p3+q3+3pq2=n3p^3 + q^3 + 3pq^2 = n^3:

n3=p3+q3+3pq2>p3  ⟹  n>pn^3 = p^3 + q^3 + 3pq^2 > p^3 \implies n > p

n3=p3+q3+3pq2>q3  ⟹  n>qn^3 = p^3 + q^3 + 3pq^2 > q^3 \implies n > q

Therefore p+q−n<pp + q - n < p (since q−n<0q - n < 0) and p+q−n<qp + q - n < q (since p−n<0p - n < 0). ■\qquad \blacksquare

Now we show no prime pair works. We use the identity (p+q)3=p3+3p2q+3pq2+q3(p + q)^3 = p^3 + 3p^2q + 3pq^2 + q^3:

(p+q)3=(p3+q3+3pq2)+3p2q=n3+3p2q(p + q)^3 = (p^3 + q^3 + 3pq^2) + 3p^2q = n^3 + 3p^2q

(p+q)3−n3=3p2q(p + q)^3 - n^3 = 3p^2q

Factorising the left side:

(p+q−n)[(p+q)2+(p+q)n+n2]=3p2q(p + q - n)\big[(p + q)^2 + (p + q)n + n^2\big] = 3p^2q

Since p+q−np + q - n is a positive integer dividing 3p2q3p^2q, and p+q−n<pp + q - n < p and p+q−n<qp + q - n < q, the factor p+q−np + q - n cannot be divisible by pp or qq. Therefore p+q−np + q - n divides 3, giving p+q−n=1p + q - n = 1 or p+q−n=3p + q - n = 3.

Case p+q−n=1p + q - n = 1: Then n=p+q−1n = p + q - 1, so (p+q)3−n3=(p+q)3−(p+q−1)3(p + q)^3 - n^3 = (p+q)^3 - (p+q-1)^3. Let m=p+qm = p + q:

m3−(m−1)3=3m2−3m+1=3p2qm^3 - (m - 1)^3 = 3m^2 - 3m + 1 = 3p^2q

The left side 3m2−3m+1≡1(mod3)3m^2 - 3m + 1 \equiv 1 \pmod{3}, but 3p2q≡0(mod3)3p^2q \equiv 0 \pmod{3}. Contradiction.

Case p+q−n=3p + q - n = 3: Then n=p+q−3n = p + q - 3, so with m=p+qm = p + q:

m3−(m−3)3=9m2−27m+27=3(3m2−9m+9)=3p2qm^3 - (m-3)^3 = 9m^2 - 27m + 27 = 3(3m^2 - 9m + 9) = 3p^2q

So 3(m2−3m+3)=p2q3(m^2 - 3m + 3) = p^2q. Since 3 divides p2qp^2q and pp, qq are prime, either p=3p = 3 or q=3q = 3.

If p=3p = 3: then 3(m2−3m+3)=9q3(m^2 - 3m + 3) = 9q, so q=m2−3m+33q = \frac{m^2 - 3m + 3}{3}. But also q=m−p=m−3q = m - p = m - 3, so:

m−3=m2−3m+33  ⟹  3m−9=m2−3m+3  ⟹  m2−6m+12=0m - 3 = \frac{m^2 - 3m + 3}{3} \implies 3m - 9 = m^2 - 3m + 3 \implies m^2 - 6m + 12 = 0

The discriminant is 36−48=−12<036 - 48 = -12 < 0, so no real solution exists.

If q=3q = 3: then 3(m2−3m+3)=9p3(m^2 - 3m + 3) = 9p, so p=m2−3m+33p = \frac{m^2 - 3m + 3}{3}. But also p=m−q=m−3p = m - q = m - 3, giving the same equation m2−6m+12=0m^2 - 6m + 12 = 0 with no real solution.

In both sub-cases we reach a contradiction. Therefore there are no prime numbers pp and qq such that p3+q3+3pq2p^3 + q^3 + 3pq^2 is the cube of an integer. ■\qquad \blacksquare

Examiner Notes

最受欢迎的题目,平均分9/20。常见错误:处理不等式时缺乏精确性;从结果反推而未验证逻辑可逆。第(iii)部分关键:识别 p+q-n 必须为 1 或 3,但很少有考生成功排除两种情况。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

6 (i) By considering the Maclaurin series for exe^x, show that for all real xx,

cosh⁡2x⩾1+x2.\cosh^2 x \geqslant 1 + x^2.

Hence show that the function f, defined for all real xx by f(x)=tan⁡−1x−tanh⁡xf(x) = \tan^{-1} x - \tanh x, is an increasing function.

Sketch the graph y=f(x)y = f(x).

(ii) Function g is defined for all real xx by g(x)=tan⁡−1x−12πtanh⁡xg(x) = \tan^{-1} x - \frac{1}{2} \pi \tanh x.

(a) Show that g has at least two stationary points.

(b) Show, by considering its derivative, that (1+x2)sinh⁡x−xcosh⁡x(1 + x^2) \sinh x - x \cosh x is non-negative for x⩾0x \geqslant 0.

(c) Show that cosh⁡2x1+x2\frac{\cosh^2 x}{1 + x^2} is an increasing function for x⩾0x \geqslant 0.

(d) Hence or otherwise show that g has exactly two stationary points.

(e) Sketch the graph y=g(x)y = g(x).

Hint

(i)

ex=1+x+x22!+x33!+…e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots cosh⁡x=12(ex+e−x)=12(1+x+x22!+x33!+⋯+1−x+x22!−x33!+… )=1+x22!+…\cosh x = \frac{1}{2}(e^x + e^{-x}) = \frac{1}{2}\left(1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots + 1 - x + \frac{x^2}{2!} - \frac{x^3}{3!} + \dots\right) = 1 + \frac{x^2}{2!} + \dots cosh⁡2x=(1+x22!+x44!+… )2=1+x2+x43+⋯≥1+x2\cosh^2 x = \left(1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \dots\right)^2 = 1 + x^2 + \frac{x^4}{3} + \dots \geq 1 + x^2

B1*

as all terms are of even degree with positive coefficients.

Alternative

cosh⁡x=12(ex+e−x)=1+x22!+⋯≥1+x22!\cosh x = \frac{1}{2}(e^x + e^{-x}) = 1 + \frac{x^2}{2!} + \dots \geq 1 + \frac{x^2}{2!} cosh⁡2x≥(1+x22!)2=1+x2+x44≥1+x2\cosh^2 x \geq \left(1 + \frac{x^2}{2!}\right)^2 = 1 + x^2 + \frac{x^4}{4} \geq 1 + x^2

B1*

f(x)=tan⁡−1x−tanh⁡xf(x) = \tan^{-1} x - \tanh x

f′(x)=11+x2−sech2x=cosh⁡2x−(1+x2)(1+x2)cosh⁡2xf'(x) = \frac{1}{1 + x^2} - \text{sech}^2 x = \frac{\cosh^2 x - (1 + x^2)}{(1 + x^2) \cosh^2 x}

M1

We have shown that the numerator cosh⁡2x−(1+x2)≥0\cosh^2 x - (1 + x^2) \geq 0 and the denominator is positive so f′(x)≥0f'(x) \geq 0 and hence the function ff is increasing. E1*

When x=0x = 0, f(x)=f′(x)=0f(x) = f'(x) = 0 and for all other xx, f′(x)>0f'(x) > 0

f(−x)=−f(x)f(-x) = -f(x)

G1

As x→±∞x \to \pm\infty, f(x)→±(π2−1)f(x) \to \pm\left(\frac{\pi}{2} - 1\right) respectively. G1 (5)

The sketch should show that ff is odd, passes through the origin with horizontal tangent, is increasing, and tends to ±(π2−1)\pm\left(\frac{\pi}{2}-1\right) as x→±∞x\to\pm\infty.

(ii) (a) g(x)=tan⁡−1x−12πtanh⁡xg(x) = \tan^{-1} x - \frac{1}{2} \pi \tanh x g′(x)=11+x2−12πsech⁡2x=2cosh⁡2x−π(1+x2)2(1+x2)cosh⁡2xg'(x) = \frac{1}{1 + x^2} - \frac{1}{2} \pi \operatorname{sech}^2 x = \frac{2 \cosh^2 x - \pi (1 + x^2)}{2 (1 + x^2) \cosh^2 x} M1

As in (i), the denominator is positive. When x=0x = 0, the numerator =2−π<0= 2 - \pi < 0. A1

The numerator =(2−π)(1+x2)+2(x43+… )→∞= (2 - \pi)(1 + x^2) + 2 \left( \frac{x^4}{3} + \dots \right) \to \infty as x→∞x \to \infty. M1 Thus, there is a value of x≠0x \neq 0 for which g′(x)=0g'(x) = 0 and as g′(x)g'(x) is an even function, there is also the value −x-x. E1 Hence, there are at least two stationary points for g. (4)

Alternative

g(0)=0g(0) = 0 E1 and g(x)→0g(x) \to 0 as x→∞x \to \infty E1 and g(x)g(x) is not identically zero E1 so there must be a stationary point for positive xx, and similarly for negative. E1

(b) ddx[(1+x2)sinh⁡x−xcosh⁡x]=(1+x2)cosh⁡x+2xsinh⁡x−xsinh⁡x−cosh⁡x\frac{d}{dx} [(1 + x^2) \sinh x - x \cosh x] = (1 + x^2) \cosh x + 2x \sinh x - x \sinh x - \cosh x M1

=x2cosh⁡x+xsinh⁡x≥0= x^2 \cosh x + x \sinh x \geq 0

for x≥0x \geq 0 A1

as x2≥0x^2 \geq 0 and cosh⁡x≥1\cosh x \geq 1 for all xx and sinh⁡x≥0\sinh x \geq 0 for x≥0x \geq 0 E1

When x=0x = 0, (1+x2)sinh⁡x−xcosh⁡x=0(1 + x^2) \sinh x - x \cosh x = 0 and we have shown (1+x2)sinh⁡x−xcosh⁡x(1 + x^2) \sinh x - x \cosh x is increasing for x≥0x \geq 0, thus (1+x2)sinh⁡x−xcosh⁡x(1 + x^2) \sinh x - x \cosh x is non-negative for x≥0x \geq 0. E1 (4)

(c) ddx[cosh⁡2x1+x2]=(1+x2)2cosh⁡xsinh⁡x−2xcosh⁡2x(1+x2)2=2cosh⁡x((1+x2)sinh⁡x−xcosh⁡x)(1+x2)2\frac{d}{dx} \left[ \frac{\cosh^2 x}{1 + x^2} \right] = \frac{(1 + x^2) 2 \cosh x \sinh x - 2x \cosh^2 x}{(1 + x^2)^2} = \frac{2 \cosh x ((1 + x^2) \sinh x - x \cosh x)}{(1 + x^2)^2} M1 A1

2cosh⁡x(1+x2)2>0\frac{2 \cosh x}{(1 + x^2)^2} > 0 for all xx and by (b) (1+x2)sinh⁡x−xcosh⁡x≥0(1 + x^2) \sinh x - x \cosh x \geq 0 for x≥0x \geq 0

so cosh⁡2x1+x2\frac{\cosh^2 x}{1 + x^2} is increasing for x≥0x \geq 0. E1 (3)

(d)

g′(x)=11+x2−12πsech⁡2x=1cosh⁡2x[cosh⁡2x1+x2−12π]g'(x) = \frac{1}{1 + x^2} - \frac{1}{2} \pi \operatorname{sech}^2 x = \frac{1}{\cosh^2 x} \left[ \frac{\cosh^2 x}{1 + x^2} - \frac{1}{2} \pi \right]

By (c) , g′g' is increasing for x≥0x \geq 0 , and thus there is exactly one value of xx for x>0x > 0 that g′(x)=0g'(x) = 0

Similarly, as g′g' is an even function, there is exactly one value of xx for x<0x < 0 that g′(x)=0g'(x) = 0 Thus there are exactly two stationary points. E1 (1)

(e)

xxSketch value of yy
−2-20.50.5
−1-111
0000
11−1-1
22−0.5-0.5

G3 (3)

Model Solution

Part (i)

The Maclaurin series for exe^x is:

ex=1+x+x22!+x33!+x44!+⋯e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \cdots

Therefore:

cosh⁡x=ex+e−x2=1+x22!+x44!+x66!+⋯=∑k=0∞x2k(2k)!\cosh x = \frac{e^x + e^{-x}}{2} = 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \frac{x^6}{6!} + \cdots = \sum_{k=0}^{\infty} \frac{x^{2k}}{(2k)!}

Squaring:

cosh⁡2x=(∑k=0∞x2k(2k)!)2\cosh^2 x = \left(\sum_{k=0}^{\infty} \frac{x^{2k}}{(2k)!}\right)^2

The coefficient of x0x^0 is 1⋅1=11 \cdot 1 = 1. The coefficient of x2x^2 is 1⋅12!+12!⋅1=11 \cdot \frac{1}{2!} + \frac{1}{2!} \cdot 1 = 1. The coefficient of x4x^4 is 1⋅14!+12!⋅12!+14!⋅1=112+14+112=131 \cdot \frac{1}{4!} + \frac{1}{2!} \cdot \frac{1}{2!} + \frac{1}{4!} \cdot 1 = \frac{1}{12} + \frac{1}{4} + \frac{1}{12} = \frac{1}{3}.

In general, every coefficient in the expansion is a sum of products of positive terms 1(2k)!\frac{1}{(2k)!}, so all coefficients are non-negative. Therefore:

cosh⁡2x=1+x2+x43+(terms of degree ≥6 with non-negative coefficients)\cosh^2 x = 1 + x^2 + \frac{x^4}{3} + (\text{terms of degree } \geq 6 \text{ with non-negative coefficients})

cosh⁡2x≥1+x2for all real x■\cosh^2 x \geq 1 + x^2 \qquad \text{for all real } x \qquad \blacksquare

Now consider f(x)=tan⁡−1x−tanh⁡xf(x) = \tan^{-1} x - \tanh x. Differentiating:

f′(x)=11+x2−sech⁡2x=11+x2−1cosh⁡2xf'(x) = \frac{1}{1 + x^2} - \operatorname{sech}^2 x = \frac{1}{1 + x^2} - \frac{1}{\cosh^2 x}

=cosh⁡2x−(1+x2)(1+x2)cosh⁡2x= \frac{\cosh^2 x - (1 + x^2)}{(1 + x^2)\cosh^2 x}

The denominator (1+x2)cosh⁡2x>0(1 + x^2)\cosh^2 x > 0 for all xx. By the inequality just proved, cosh⁡2x−(1+x2)≥0\cosh^2 x - (1 + x^2) \geq 0, so f′(x)≥0f'(x) \geq 0 for all xx.

Moreover, f′(x)=0f'(x) = 0 only when cosh⁡2x=1+x2\cosh^2 x = 1 + x^2, which from the series expansion requires all higher-order terms to vanish, i.e., x=0x = 0. So f′(x)>0f'(x) > 0 for all x≠0x \neq 0, and ff is (strictly) increasing. ■\qquad \blacksquare

Sketch of y=f(x)y = f(x):

Since f(−x)=tan⁡−1(−x)−tanh⁡(−x)=−tan⁡−1x+tanh⁡x=−f(x)f(-x) = \tan^{-1}(-x) - \tanh(-x) = -\tan^{-1} x + \tanh x = -f(x), the function ff is odd.

At x=0x = 0: f(0)=0f(0) = 0. Since f′(0)=0f'(0) = 0 and f′(x)>0f'(x) > 0 for x≠0x \neq 0, the graph passes through the origin with a horizontal tangent, then rises on both sides.

As x→+∞x \to +\infty: tan⁡−1x→π2\tan^{-1} x \to \frac{\pi}{2} and tanh⁡x→1\tanh x \to 1, so f(x)→π2−1≈0.571f(x) \to \frac{\pi}{2} - 1 \approx 0.571.

As x→−∞x \to -\infty: f(x)→−(π2−1)f(x) \to -\left(\frac{\pi}{2} - 1\right).

The graph is an S-shaped curve through the origin with horizontal asymptotes y=±(π2−1)y = \pm\left(\frac{\pi}{2} - 1\right), increasing everywhere with a flat point at the origin.

Part (ii)(a)

g(x)=tan⁡−1x−π2tanh⁡xg(x) = \tan^{-1} x - \frac{\pi}{2}\tanh x

g′(x)=11+x2−π2sech⁡2x=2cosh⁡2x−π(1+x2)2(1+x2)cosh⁡2xg'(x) = \frac{1}{1 + x^2} - \frac{\pi}{2}\operatorname{sech}^2 x = \frac{2\cosh^2 x - \pi(1 + x^2)}{2(1 + x^2)\cosh^2 x}

The denominator is positive for all xx. Let N(x)=2cosh⁡2x−π(1+x2)N(x) = 2\cosh^2 x - \pi(1 + x^2) be the numerator.

At x=0x = 0: N(0)=2−π<0N(0) = 2 - \pi < 0.

As x→∞x \to \infty: using cosh⁡2x=1+x2+x43+⋯\cosh^2 x = 1 + x^2 + \frac{x^4}{3} + \cdots:

N(x)=2(1+x2+x43+⋯ )−π(1+x2)=(2−π)(1+x2)+2x43+⋯N(x) = 2\left(1 + x^2 + \frac{x^4}{3} + \cdots\right) - \pi(1 + x^2) = (2 - \pi)(1 + x^2) + \frac{2x^4}{3} + \cdots

Since (2−π)(1+x2)(2 - \pi)(1 + x^2) grows like −1.14x2-1.14 x^2 while 2x43\frac{2x^4}{3} grows like 0.67x40.67 x^4, the x4x^4 term dominates for large xx, so N(x)→+∞N(x) \to +\infty as x→∞x \to \infty.

By the Intermediate Value Theorem, there exists x0>0x_0 > 0 with N(x0)=0N(x_0) = 0, i.e., g′(x0)=0g'(x_0) = 0.

Since g′(−x)=g′(x)g'(-x) = g'(x) (both 11+x2\frac{1}{1+x^2} and sech⁡2x\operatorname{sech}^2 x are even functions), g′g' is even, so g′(−x0)=0g'(-x_0) = 0 as well.

Therefore gg has at least two stationary points (at x=x0x = x_0 and x=−x0x = -x_0). ■\qquad \blacksquare

Part (ii)(b)

Let h(x)=(1+x2)sinh⁡x−xcosh⁡xh(x) = (1 + x^2)\sinh x - x\cosh x.

h′(x)=ddx[(1+x2)sinh⁡x]−ddx[xcosh⁡x]h'(x) = \frac{d}{dx}\big[(1+x^2)\sinh x\big] - \frac{d}{dx}\big[x\cosh x\big]

=2xsinh⁡x+(1+x2)cosh⁡x−(cosh⁡x+xsinh⁡x)= 2x\sinh x + (1+x^2)\cosh x - (\cosh x + x\sinh x)

=2xsinh⁡x+(1+x2)cosh⁡x−cosh⁡x−xsinh⁡x= 2x\sinh x + (1+x^2)\cosh x - \cosh x - x\sinh x

=xsinh⁡x+x2cosh⁡x= x\sinh x + x^2\cosh x

For x≥0x \geq 0: x2≥0x^2 \geq 0 and cosh⁡x≥1>0\cosh x \geq 1 > 0, so x2cosh⁡x≥0x^2\cosh x \geq 0. Also x≥0x \geq 0 and sinh⁡x≥0\sinh x \geq 0 for x≥0x \geq 0, so xsinh⁡x≥0x\sinh x \geq 0.

Therefore h′(x)≥0h'(x) \geq 0 for x≥0x \geq 0.

At x=0x = 0: h(0)=(1)(0)−0=0h(0) = (1)(0) - 0 = 0.

Since h(0)=0h(0) = 0 and hh is increasing for x≥0x \geq 0, we have h(x)≥0h(x) \geq 0 for x≥0x \geq 0.

Therefore (1+x2)sinh⁡x−xcosh⁡x≥0(1 + x^2)\sinh x - x\cosh x \geq 0 for x≥0x \geq 0. ■\qquad \blacksquare

Part (ii)(c)

ddx[cosh⁡2x1+x2]=2cosh⁡xsinh⁡x⋅(1+x2)−cosh⁡2x⋅2x(1+x2)2\frac{d}{dx}\left[\frac{\cosh^2 x}{1 + x^2}\right] = \frac{2\cosh x \sinh x \cdot (1 + x^2) - \cosh^2 x \cdot 2x}{(1 + x^2)^2}

=2cosh⁡x[(1+x2)sinh⁡x−xcosh⁡x](1+x2)2= \frac{2\cosh x\big[(1 + x^2)\sinh x - x\cosh x\big]}{(1 + x^2)^2}

For x≥0x \geq 0: cosh⁡x>0\cosh x > 0 and (1+x2)2>0(1 + x^2)^2 > 0. By part (b), (1+x2)sinh⁡x−xcosh⁡x≥0(1 + x^2)\sinh x - x\cosh x \geq 0.

Therefore ddx[cosh⁡2x1+x2]≥0\frac{d}{dx}\left[\frac{\cosh^2 x}{1 + x^2}\right] \geq 0 for x≥0x \geq 0, so cosh⁡2x1+x2\frac{\cosh^2 x}{1 + x^2} is an increasing function for x≥0x \geq 0. ■\qquad \blacksquare

Part (ii)(d)

We can write:

g′(x)=11+x2−π2⋅1cosh⁡2x=1cosh⁡2x[cosh⁡2x1+x2−π2]g'(x) = \frac{1}{1 + x^2} - \frac{\pi}{2}\cdot\frac{1}{\cosh^2 x} = \frac{1}{\cosh^2 x}\left[\frac{\cosh^2 x}{1 + x^2} - \frac{\pi}{2}\right]

Since 1cosh⁡2x>0\frac{1}{\cosh^2 x} > 0 for all xx, the sign of g′(x)g'(x) is determined by cosh⁡2x1+x2−π2\frac{\cosh^2 x}{1 + x^2} - \frac{\pi}{2}.

By part (c), cosh⁡2x1+x2\frac{\cosh^2 x}{1 + x^2} is increasing for x≥0x \geq 0. At x=0x = 0: cosh⁡201+0=1<π2\frac{\cosh^2 0}{1 + 0} = 1 < \frac{\pi}{2}, so g′(0)<0g'(0) < 0.

As x→∞x \to \infty: cosh⁡2x1+x2→∞\frac{\cosh^2 x}{1 + x^2} \to \infty (exponential growth dominates polynomial growth), so eventually cosh⁡2x1+x2>π2\frac{\cosh^2 x}{1 + x^2} > \frac{\pi}{2} and g′(x)>0g'(x) > 0.

Since cosh⁡2x1+x2\frac{\cosh^2 x}{1 + x^2} is continuous and strictly increasing for x≥0x \geq 0, there is exactly one x0>0x_0 > 0 where cosh⁡2x01+x02=π2\frac{\cosh^2 x_0}{1 + x_0^2} = \frac{\pi}{2}, giving exactly one positive stationary point.

Since g′g' is an even function, there is exactly one negative stationary point at x=−x0x = -x_0.

Therefore gg has exactly two stationary points. ■\qquad \blacksquare

Part (ii)(e)

gg is an odd function: g(−x)=−g(x)g(-x) = -g(x).

At x=0x = 0: g(0)=0g(0) = 0 and g′(0)=1−π2<0g'(0) = 1 - \frac{\pi}{2} < 0.

As x→+∞x \to +\infty: tan⁡−1x→π2\tan^{-1} x \to \frac{\pi}{2} and tanh⁡x→1\tanh x \to 1, so g(x)→π2−π2=0g(x) \to \frac{\pi}{2} - \frac{\pi}{2} = 0. The approach is from below since g′(0)<0g'(0) < 0 and gg must dip below zero.

As x→−∞x \to -\infty: g(x)→0g(x) \to 0 from above (by odd symmetry).

Key features:

  • gg passes through the origin with negative slope.
  • There is a local minimum at x=x0>0x = x_0 > 0 with g(x0)<0g(x_0) < 0.
  • By odd symmetry, there is a local maximum at x=−x0<0x = -x_0 < 0 with g(−x0)=−g(x0)>0g(-x_0) = -g(x_0) > 0.
  • For x>0x > 0: gg decreases from 0, reaches a minimum at x0x_0, then increases back toward 0.
  • For x<0x < 0: gg increases from 0, reaches a maximum at −x0-x_0, then decreases back toward 0.

The graph is an odd, wave-like curve that starts from 0−0^- at −∞-\infty, rises to a positive peak, passes through the origin with negative slope, falls to a negative trough, then returns to 0+0^+ at +∞+\infty.

Examiner Notes

第四受欢迎(75%作答),第二成功(平均分10+/20)。第(ii)(a)最难,常见错误:未论证 g(x) 或 g’(x) 在无穷远处的行为。第(d)部分常见错误:未考虑 cosh²x/(1+x²) 的对称性。第(e)部分常见错误:图像反射,x>0 时 g(x) 应为负值。


Topic: 纯数  |  Difficulty: Challenging  |  Marks: 20

7 (i) Let ff be a continuous function defined for 0⩽x⩽10 \leqslant x \leqslant 1. Show that

∫01f(x) dx=2∫01xf(x) dx .\int_{0}^{1} f(\sqrt{x}) \, dx = 2 \int_{0}^{1} xf(x) \, dx \, .

(ii) Let gg be a continuous function defined for 0⩽x⩽10 \leqslant x \leqslant 1 such that

∫01(g(x))2 dx=∫01g(x) dx−13 .\int_{0}^{1} (g(x))^2 \, dx = \int_{0}^{1} g(\sqrt{x}) \, dx - \frac{1}{3} \, .

Show that ∫01(g(x)−x)2 dx=0\int_{0}^{1} (g(x) - x)^2 \, dx = 0 and explain why g(x)=xg(x) = x for 0⩽x⩽10 \leqslant x \leqslant 1.

(iii) Let hh be a continuous function defined for 0⩽x⩽10 \leqslant x \leqslant 1 with derivative h′h' such that

∫01(h′(x))2 dx=2h(1)−2∫01h(x) dx−13 .\int_{0}^{1} (h'(x))^2 \, dx = 2h(1) - 2 \int_{0}^{1} h(x) \, dx - \frac{1}{3} \, .

Given that h(0)=0h(0) = 0, find hh.

(iv) Let kk be a continuous function defined for 0⩽x⩽10 \leqslant x \leqslant 1 and aa be a real number, such that

∫01eax(k(x))2 dx=2∫01k(x) dx+e−aa−1a2−14 .\int_{0}^{1} e^{ax} (k(x))^2 \, dx = 2 \int_{0}^{1} k(x) \, dx + \frac{e^{-a}}{a} - \frac{1}{a^2} - \frac{1}{4} \, .

Show that aa must be equal to 2 and find kk.

Hint

(i)

Let x=u2x = u^2, dxdu=2u\frac{dx}{du} = 2u, x=u\sqrt{x} = u M1 ∫01f(x) dx=∫01f(u) 2u du=2∫01xf(x) dx\int_{0}^{1} f(\sqrt{x}) \ dx = \int_{0}^{1} f(u) \ 2u \ du = 2 \int_{0}^{1} x f(x) \ dx

as required. A1* (2)

(ii) ∫01(g(x)−x)2 dx=∫01(g(x))2 dx−2∫01x g(x) dx+∫01x2 dx\int_{0}^{1} (g(x) - x)^2 \ dx = \int_{0}^{1} (g(x))^2 \ dx - 2 \int_{0}^{1} x \ g(x) \ dx + \int_{0}^{1} x^2 \ dx

=∫01g(x) dx−13−2∫01x g(x) dx+∫01x2 dx= \int_{0}^{1} g(\sqrt{x}) \ dx - \frac{1}{3} - 2 \int_{0}^{1} x \ g(x) \ dx + \int_{0}^{1} x^2 \ dx M1 =2∫01x g(x) dx−13−2∫01x g(x) dx+[x33]01= 2 \int_{0}^{1} x \ g(x) \ dx - \frac{1}{3} - 2 \int_{0}^{1} x \ g(x) \ dx + \left[ \frac{x^3}{3} \right]_{0}^{1}

M1 =0−13+13=0= 0 - \frac{1}{3} + \frac{1}{3} = 0 A1*

(g(x)−x)2≥0(g(x) - x)^2 \geq 0

So, the area under the graph of y=(g(x)−x)2≥0y = (g(x) - x)^2 \geq 0, and the area can only equal zero if (g(x)−x)2=0(g(x) - x)^2 = 0 for 0≤x≤10 \leq x \leq 1, that is g(x)=xg(x) = x. E1 (4)

(iii) ∫01(h′(x)−x)2 dx=∫01(h′(x))2−2xh′(x)+x2 dx\int_{0}^{1} (h'(x) - x)^2 \ dx = \int_{0}^{1} (h'(x))^2 - 2xh'(x) + x^2 \ dx

M1

We are given that

∫01(h′(x))2=2h(1)−2∫01h(x) dx−13\int_{0}^{1} (h'(x))^2 = 2h(1) - 2 \int_{0}^{1} h(x) \ dx - \frac{1}{3}

Integrating by parts

∫012xh′(x) dx=[2xh(x)]01−2∫01h(x) dx=2h(1)−2∫01h(x) dx\int_{0}^{1} 2xh'(x) \ dx = [2xh(x)]_{0}^{1} - 2 \int_{0}^{1} h(x) \ dx = 2h(1) - 2 \int_{0}^{1} h(x) \ dx M1 A1

and

∫01x2dx=[x33]01=13\int_{0}^{1} x^{2} dx = \left[ \frac{x^{3}}{3} \right]_{0}^{1} = \frac{1}{3}

So,

∫01(h′(x)−x)2dx=2h(1)−2∫01h(x)dx−13−(2h(1)−2∫01h(x)dx)+13=0\int_{0}^{1} (h'(x) - x)^{2} dx = 2h(1) - 2 \int_{0}^{1} h(x) dx - \frac{1}{3} - \left( 2h(1) - 2 \int_{0}^{1} h(x) dx \right) + \frac{1}{3} = 0

A1

As in (ii) with g, h′(x)=xh'(x) = x. Thus h(x)=12x2+ch(x) = \frac{1}{2}x^{2} + c but h(0)=0h(0) = 0 so c=0c = 0 and thus h(x)=12x2h(x) = \frac{1}{2}x^{2}

E1 M1 A1 A1 (8)

(iv)

∫01(e12axk(x)−e−12ax)2dx=∫01eax(k(x))2−2k(x)+e−axdx\int_{0}^{1} \left( e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} \right)^{2} dx = \int_{0}^{1} e^{ax} (k(x))^{2} - 2k(x) + e^{-ax} dx

M1 dM1

=2∫01k(x)dx+e−aa−1a2−14−2∫01k(x)dx−[e−aa]01= 2 \int_{0}^{1} k(x) dx + \frac{e^{-a}}{a} - \frac{1}{a^{2}} - \frac{1}{4} - 2 \int_{0}^{1} k(x) dx - \left[ \frac{e^{-a}}{a} \right]_{0}^{1}

=e−aa−1a2−14−e−aa+1a=−1a2+1a−14=−4−4a+a24a2=−(2−a)24a2= \frac{e^{-a}}{a} - \frac{1}{a^{2}} - \frac{1}{4} - \frac{e^{-a}}{a} + \frac{1}{a} = -\frac{1}{a^{2}} + \frac{1}{a} - \frac{1}{4} = -\frac{4 - 4a + a^{2}}{4a^{2}} = -\frac{(2 - a)^{2}}{4a^{2}}

A1 A1

As before, ∫01(e12axk(x)−e−12ax)2dx≥0\int_{0}^{1} \left( e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} \right)^{2} dx \geq 0 but −(2−a)24a2≤0-\frac{(2 - a)^{2}}{4a^{2}} \leq 0 A1

Therefore, ∫01(e12axk(x)−e−12ax)2dx=0\int_{0}^{1} \left( e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} \right)^{2} dx = 0 and (2−a)24a2=0\frac{(2 - a)^{2}}{4a^{2}} = 0 E1

Thus e12axk(x)−e−12ax=0e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} = 0 and 2−a=02 - a = 0

So a=2a = 2 and k(x)=e−ax=e−2xk(x) = e^{-ax} = e^{-2x} A1 (6)

Model Solution

Part (i)

Substitute u=xu = \sqrt{x}, so x=u2x = u^2 and dx=2u dudx = 2u \, du. When x=0x = 0, u=0u = 0; when x=1x = 1, u=1u = 1.

∫01f(x) dx=∫01f(u)⋅2u du=2∫01uf(u) du=2∫01xf(x) dx\int_0^1 f(\sqrt{x}) \, dx = \int_0^1 f(u) \cdot 2u \, du = 2 \int_0^1 u f(u) \, du = 2 \int_0^1 x f(x) \, dx

where the last step relabels the dummy variable uu as xx. ■\qquad \blacksquare

Part (ii)

Expand the integrand:

∫01(g(x)−x)2 dx=∫01(g(x))2 dx−2∫01x g(x) dx+∫01x2 dx...(1)\int_0^1 (g(x) - x)^2 \, dx = \int_0^1 (g(x))^2 \, dx - 2 \int_0^1 x \, g(x) \, dx + \int_0^1 x^2 \, dx \qquad \text{...(1)}

From the given equation:

∫01(g(x))2 dx=∫01g(x) dx−13\int_0^1 (g(x))^2 \, dx = \int_0^1 g(\sqrt{x}) \, dx - \frac{1}{3}

By part (i), ∫01g(x) dx=2∫01x g(x) dx\int_0^1 g(\sqrt{x}) \, dx = 2 \int_0^1 x \, g(x) \, dx, so:

∫01(g(x))2 dx=2∫01x g(x) dx−13\int_0^1 (g(x))^2 \, dx = 2 \int_0^1 x \, g(x) \, dx - \frac{1}{3}

Substituting into (1):

∫01(g(x)−x)2 dx=2∫01x g(x) dx−13−2∫01x g(x) dx+∫01x2 dx\int_0^1 (g(x) - x)^2 \, dx = 2 \int_0^1 x \, g(x) \, dx - \frac{1}{3} - 2 \int_0^1 x \, g(x) \, dx + \int_0^1 x^2 \, dx

=−13+[x33]01=−13+13=0■= -\frac{1}{3} + \left[ \frac{x^3}{3} \right]_0^1 = -\frac{1}{3} + \frac{1}{3} = 0 \qquad \blacksquare

Since gg is continuous, (g(x)−x)2(g(x) - x)^2 is a continuous non-negative function on [0,1][0, 1]. A non-negative continuous function whose integral is zero must be identically zero: if (g(x0)−x0)2>0(g(x_0) - x_0)^2 > 0 at some point x0x_0, then by continuity (g(x)−x)2>0(g(x) - x)^2 > 0 in a neighbourhood of x0x_0, making the integral strictly positive, a contradiction.

Therefore (g(x)−x)2=0(g(x) - x)^2 = 0 for all 0⩽x⩽10 \leqslant x \leqslant 1, which gives g(x)=xg(x) = x. ■\qquad \blacksquare

Part (iii)

Expand the integrand:

∫01(h′(x)−x)2 dx=∫01(h′(x))2 dx−2∫01x h′(x) dx+∫01x2 dx...(2)\int_0^1 (h'(x) - x)^2 \, dx = \int_0^1 (h'(x))^2 \, dx - 2 \int_0^1 x \, h'(x) \, dx + \int_0^1 x^2 \, dx \qquad \text{...(2)}

Middle term (integration by parts, using h(0)=0h(0) = 0):

∫012x h′(x) dx=[2x h(x)]01−∫012h(x) dx=2h(1)−2∫01h(x) dx\int_0^1 2x \, h'(x) \, dx = \left[ 2x \, h(x) \right]_0^1 - \int_0^1 2h(x) \, dx = 2h(1) - 2 \int_0^1 h(x) \, dx

Last term:

∫01x2 dx=13\int_0^1 x^2 \, dx = \frac{1}{3}

Substituting into (2) along with the given equation ∫01(h′(x))2 dx=2h(1)−2∫01h(x) dx−13\int_0^1 (h'(x))^2 \, dx = 2h(1) - 2\int_0^1 h(x)\,dx - \frac{1}{3}:

∫01(h′(x)−x)2 dx=(2h(1)−2∫01h(x) dx−13)−(2h(1)−2∫01h(x) dx)+13=0\int_0^1 (h'(x) - x)^2 \, dx = \left( 2h(1) - 2 \int_0^1 h(x)\,dx - \frac{1}{3} \right) - \left( 2h(1) - 2 \int_0^1 h(x)\,dx \right) + \frac{1}{3} = 0

Since (h′(x)−x)2(h'(x) - x)^2 is continuous and non-negative with zero integral, the same argument as in (ii) gives h′(x)=xh'(x) = x for all 0⩽x⩽10 \leqslant x \leqslant 1.

Integrating: h(x)=x22+Ch(x) = \frac{x^2}{2} + C. Using h(0)=0h(0) = 0 gives C=0C = 0, so:

h(x)=x22■h(x) = \frac{x^2}{2} \qquad \blacksquare

Part (iv)

Consider the integral of a perfect square:

∫01(e12axk(x)−e−12ax)2dx\int_0^1 \left( e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} \right)^2 dx

Expanding the square:

=∫01[eax(k(x))2−2e12axk(x)⋅e−12ax+e−ax]dx= \int_0^1 \left[ e^{ax}(k(x))^2 - 2 e^{\frac{1}{2}ax} k(x) \cdot e^{-\frac{1}{2}ax} + e^{-ax} \right] dx

=∫01eax(k(x))2 dx−2∫01k(x) dx+∫01e−ax dx= \int_0^1 e^{ax}(k(x))^2 \, dx - 2 \int_0^1 k(x) \, dx + \int_0^1 e^{-ax} \, dx

Substituting the given equation for ∫01eax(k(x))2 dx\int_0^1 e^{ax}(k(x))^2 \, dx:

=(2∫01k(x) dx+e−aa−1a2−14)−2∫01k(x) dx+∫01e−ax dx= \left( 2 \int_0^1 k(x) \, dx + \frac{e^{-a}}{a} - \frac{1}{a^2} - \frac{1}{4} \right) - 2 \int_0^1 k(x) \, dx + \int_0^1 e^{-ax} \, dx

=e−aa−1a2−14+∫01e−ax dx= \frac{e^{-a}}{a} - \frac{1}{a^2} - \frac{1}{4} + \int_0^1 e^{-ax} \, dx

Evaluating the remaining integral (a≠0a \neq 0):

∫01e−ax dx=[−1ae−ax]01=−e−aa+1a=1−e−aa\int_0^1 e^{-ax} \, dx = \left[ -\frac{1}{a} e^{-ax} \right]_0^1 = -\frac{e^{-a}}{a} + \frac{1}{a} = \frac{1 - e^{-a}}{a}

Therefore:

∫01(e12axk(x)−e−12ax)2dx=e−aa−1a2−14+1−e−aa\int_0^1 \left( e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} \right)^2 dx = \frac{e^{-a}}{a} - \frac{1}{a^2} - \frac{1}{4} + \frac{1 - e^{-a}}{a}

=1a−1a2−14=4a−4−a24a2=−(a−2)24a2= \frac{1}{a} - \frac{1}{a^2} - \frac{1}{4} = \frac{4a - 4 - a^2}{4a^2} = -\frac{(a - 2)^2}{4a^2}

The left-hand side is the integral of a non-negative continuous function, so it is ⩾0\geqslant 0. The right-hand side is −(a−2)24a2⩽0-\frac{(a-2)^2}{4a^2} \leqslant 0 for all a≠0a \neq 0.

Therefore both sides equal zero. From the right-hand side: (a−2)2=0(a - 2)^2 = 0, so a=2a = 2. ■\qquad \blacksquare

From the left-hand side: e12axk(x)−e−12ax=0e^{\frac{1}{2}ax} k(x) - e^{-\frac{1}{2}ax} = 0 for all x∈[0,1]x \in [0, 1], giving k(x)=e−ax=e−2xk(x) = e^{-ax} = e^{-2x}.

a=2,k(x)=e−2x\boxed{a = 2, \quad k(x) = e^{-2x}}

Examiner Notes

第三受欢迎,平均分9.4/20。第(ii)部分常见错误:未使用 (g(x)−x)²≥0 或错误声称严格大于零。第(iii)部分:对 xh’(x) 分部积分的考生普遍成功。第(iv)部分常见错误:未能分解关于 1/a 的二次式,或无理由地令二次式为零。


Topic: 纯数  |  Difficulty: Hard  |  Marks: 20

8 If y={k1(x)x⩽bk2(x)x⩾by = \begin{cases} k_1(x) & x \leqslant b \\ k_2(x) & x \geqslant b \end{cases} with k1(b)=k2(b)k_1(b) = k_2(b), then yy is said to be continuously differentiable at x=bx = b if k1′(b)=k2′(b)k'_1(b) = k'_2(b).

(i) Let f(x)=xe−xf(x) = xe^{-x}. Verify that, for all real xx, y=f(x)y = f(x) is a solution to the differential equation d2ydx2+2dydx+y=0\frac{d^2y}{dx^2} + 2\frac{dy}{dx} + y = 0 and that y=0y = 0 and dydx=1\frac{dy}{dx} = 1 when x=0x = 0. Show that f′(x)⩾0f'(x) \geqslant 0 for x⩽1x \leqslant 1.

(ii) You are given the differential equation d2ydx2+2∣dydx∣+y=0\frac{d^2y}{dx^2} + 2\left| \frac{dy}{dx} \right| + y = 0 where y=0y = 0 and dydx=1\frac{dy}{dx} = 1 when x=0x = 0. Let y={g1(x)x⩽1g2(x)x⩾1y = \begin{cases} g_1(x) & x \leqslant 1 \\ g_2(x) & x \geqslant 1 \end{cases} be a solution of the differential equation which is continuously differentiable at x=1x = 1. Write down an expression for g1(x)g_1(x) and find an expression for g2(x)g_2(x).

(iii) State the geometrical relationship between the curves y=g1(x)y = g_1(x) and y=g2(x)y = g_2(x).

(iv) Prove that if y=k(x)y = k(x) is a solution of the differential equation d2ydx2+pdydx+qy=0\frac{d^2y}{dx^2} + p\frac{dy}{dx} + qy = 0 in the interval r⩽x⩽sr \leqslant x \leqslant s, where pp and qq are constants, then, in a suitable interval which you should state, y=k(c−x)y = k(c - x) satisfies the differential equation d2ydx2−pdydx+qy=0 .\frac{d^2y}{dx^2} - p\frac{dy}{dx} + qy = 0 \, .

(v) You are given the differential equation

d2ydx2+2∣dydx∣+2y=0\frac{\mathrm{d}^2y}{\mathrm{d}x^2} + 2 \left| \frac{\mathrm{d}y}{\mathrm{d}x} \right| + 2y = 0

where y=0y = 0 and dydx=1\frac{\mathrm{d}y}{\mathrm{d}x} = 1 when x=0x = 0.

Let h(x)=e−xsin⁡xh(x) = e^{-x} \sin x. Show that h′(14π)=0h'(\frac{1}{4}\pi) = 0.

It is given that y=h(x)y = h(x) satisfies the differential equation in the interval −34π⩽x⩽14π-\frac{3}{4}\pi \leqslant x \leqslant \frac{1}{4}\pi and that h′(x)⩾0h'(x) \geqslant 0 in this interval.

In a solution to the differential equation which is continuously differentiable at (n+14)π(n + \frac{1}{4})\pi for all n∈Zn \in \mathbb{Z}, find yy in terms of xx in the intervals

(a) 14π⩽x⩽54π\frac{1}{4}\pi \leqslant x \leqslant \frac{5}{4}\pi,

(b) 54π⩽x⩽94π\frac{5}{4}\pi \leqslant x \leqslant \frac{9}{4}\pi.

Hint

(i) y=xe−xy = xe^{-x} dydx=e−x−xe−x=(1−x)e−x\frac{dy}{dx} = e^{-x} - xe^{-x} = (1 - x)e^{-x} d2ydx2=−e−x−(1−x)e−x=(x−2)e−x\frac{d^2y}{dx^2} = -e^{-x} - (1 - x)e^{-x} = (x - 2)e^{-x} d2ydx2+2dydx+y=(x−2)e−x+2(1−x)e−x+xe−x=0\frac{d^2y}{dx^2} + 2\frac{dy}{dx} + y = (x - 2)e^{-x} + 2(1 - x)e^{-x} + xe^{-x} = 0

M1 A1

x=0,y=xe−x=0,dydx=(1−x)e−x=1x = 0, \quad y = xe^{-x} = 0, \quad \frac{dy}{dx} = (1 - x)e^{-x} = 1

B1*

For x≤1x \le 1, (1−x)≥0(1 - x) \ge 0, e−x>0e^{-x} > 0, so dydx=(1−x)e−x≥0\frac{dy}{dx} = (1 - x)e^{-x} \ge 0 E1 (4)

(ii) From (i), g1(x)=xe−xg_1(x) = xe^{-x}

B1

Consider y=g2(x)=(a+bx)exy = g_2(x) = (a + bx)e^x for x≥1x \ge 1 B1

Then g2g_2 must be a solution of d2ydx2−2dydx+y=0\frac{d^2y}{dx^2} - 2\frac{dy}{dx} + y = 0, g1(1)=g2(1)g_1(1) = g_2(1), and g1′(1)=g2′(1)g'_1(1) = g'_2(1) dydx=bex+(a+bx)ex=((a+b)+bx)ex\frac{dy}{dx} = be^x + (a + bx)e^x = ((a + b) + bx)e^x d2ydx2=bex+((a+b)+bx)ex=((a+2b)+bx)ex\frac{d^2y}{dx^2} = be^x + ((a + b) + bx)e^x = ((a + 2b) + bx)e^x d2ydx2−2dydx+y=((a+2b)+bx)ex−2((a+b)+bx)ex+(a+bx)ex=0\frac{d^2y}{dx^2} - 2\frac{dy}{dx} + y = ((a + 2b) + bx)e^x - 2((a + b) + bx)e^x + (a + bx)e^x = 0

as required.

g1(1)=g2(1)⇒e−1=(a+b)eg_1(1) = g_2(1) \Rightarrow e^{-1} = (a + b)e g1′(1)=g2′(1)⇒0=(a+2b)eg'_1(1) = g'_2(1) \Rightarrow 0 = (a + 2b)e

M1 A1

So a=−2ba = -2b and thus b=−e−2b = -e^{-2}

Hence, g2(x)=(2e−2−e−2x)ex=(2−x)ex−2g_2(x) = (2e^{-2} - e^{-2}x)e^x = (2 - x)e^{x-2} A1ft (5)

(iii) y=g2(x)y = g_2(x) is a reflection of y=g1(x)y = g_1(x) in x=1x = 1, B1 which can be justified by substituting for xx using x′=2−xx' = 2 - x in y=g1(x)y = g_1(x), xe−x=(2−x′)ex′−2xe^{-x} = (2 - x')e^{x'-2} as expected. E1 (2)

(iv) If y=k(c−x)y = k(c - x), then dydx=−k′(c−x)\frac{dy}{dx} = -k'(c - x), and d2ydx2=k′′(c−x)\frac{d^2y}{dx^2} = k''(c - x) M1

So d2ydx2−pdydx+qy=k′′(c−x)+pk′(c−x)+qk(c−x)=0\frac{d^2y}{dx^2} - p\frac{dy}{dx} + qy = k''(c - x) + pk'(c - x) + qk(c - x) = 0 A1 provided that r≤c−x≤sr \leq c - x \leq s

i.e. c−s≤x≤c−rc - s \leq x \leq c - r B1 (3)

(v) If h(x)=e−xsin⁡xh(x) = e^{-x} \sin x, then h′(x)=−e−xsin⁡x+e−xcos⁡xh'(x) = -e^{-x} \sin x + e^{-x} \cos x,

so h′(π4)=−e−π4sin⁡π4+e−π4cos⁡π4=−12e−π4+12e−π4=0h'\left(\frac{\pi}{4}\right) = -e^{-\frac{\pi}{4}} \sin \frac{\pi}{4} + e^{-\frac{\pi}{4}} \cos \frac{\pi}{4} = -\frac{1}{\sqrt{2}}e^{-\frac{\pi}{4}} + \frac{1}{\sqrt{2}}e^{-\frac{\pi}{4}} = 0 as required. B1*

(a) Using (iv), the solution for 14π≤x≤54π\frac{1}{4}\pi \leq x \leq \frac{5}{4}\pi must be y=e−(c−x)sin⁡(c−x)y = e^{-(c-x)} \sin(c - x) M1 where

−34π≤(c−x)≤14π-\frac{3}{4}\pi \leq (c - x) \leq \frac{1}{4}\pi. M1 That is c=12πc = \frac{1}{2}\pi. So y=ex−12πcos⁡xy = e^{x-\frac{1}{2}\pi} \cos x A1

(b) Similarly, the solution for 54π≤x≤94π\frac{5}{4}\pi \leq x \leq \frac{9}{4}\pi must be y=ec−x−12πcos⁡(c−x)y = e^{c-x-\frac{1}{2}\pi} \cos(c - x) where

14π≤(c−x)≤54π\frac{1}{4}\pi \leq (c - x) \leq \frac{5}{4}\pi. That is c=52πc = \frac{5}{2}\pi. B1 So y=e2π−xsin⁡xy = e^{2\pi-x} \sin x B1 (6)

Model Solution

Part (i)

Let f(x)=xe−xf(x) = xe^{-x}. We compute the derivatives:

f′(x)=e−x−xe−x=(1−x)e−xf'(x) = e^{-x} - xe^{-x} = (1 - x)e^{-x}

f′′(x)=−e−x−(1−x)e−x=(x−2)e−xf''(x) = -e^{-x} - (1 - x)e^{-x} = (x - 2)e^{-x}

Substituting into the left-hand side of the differential equation:

f′′(x)+2f′(x)+f(x)=(x−2)e−x+2(1−x)e−x+xe−xf''(x) + 2f'(x) + f(x) = (x - 2)e^{-x} + 2(1 - x)e^{-x} + xe^{-x}

=e−x[(x−2)+2(1−x)+x]=e−x[x−2+2−2x+x]=0= e^{-x}\big[(x - 2) + 2(1 - x) + x\big] = e^{-x}[x - 2 + 2 - 2x + x] = 0

So y=xe−xy = xe^{-x} satisfies the differential equation for all real xx. ■\qquad \blacksquare

At x=0x = 0:

y=0⋅e0=0,dydx=(1−0)e0=1y = 0 \cdot e^{0} = 0, \qquad \frac{dy}{dx} = (1 - 0)e^{0} = 1

as required. ■\qquad \blacksquare

For x⩽1x \leqslant 1: we have (1−x)⩾0(1 - x) \geqslant 0 and e−x>0e^{-x} > 0 for all real xx. Therefore:

f′(x)=(1−x)e−x⩾0for x⩽1■f'(x) = (1 - x)e^{-x} \geqslant 0 \qquad \text{for } x \leqslant 1 \qquad \blacksquare

Part (ii)

Since y′(0)=1>0y'(0) = 1 > 0, the solution initially has y′>0y' > 0, so ∣y′∣=y′|y'| = y' and the differential equation becomes:

d2ydx2+2dydx+y=0\frac{d^2y}{dx^2} + 2\frac{dy}{dx} + y = 0

This is the same equation as in part (i), with the same initial conditions y(0)=0y(0) = 0 and y′(0)=1y'(0) = 1. By part (i), g1(x)=xe−xg_1(x) = xe^{-x} is the solution while y′⩾0y' \geqslant 0.

Since g1′(x)=(1−x)e−xg_1'(x) = (1 - x)e^{-x}, we have g1′(x)⩾0g_1'(x) \geqslant 0 for x⩽1x \leqslant 1 and g1′(1)=0g_1'(1) = 0. For x>1x > 1, g1′(x)<0g_1'(x) < 0, so the sign of y′y' changes at x=1x = 1.

Therefore g1(x)=xe−xg_1(x) = xe^{-x} for x⩽1x \leqslant 1.

For x⩾1x \geqslant 1, we have y′⩽0y' \leqslant 0 (by the continuously differentiable condition, y′(1)=0y'(1) = 0 and y′y' becomes negative), so ∣y′∣=−y′|y'| = -y' and the differential equation becomes:

d2ydx2−2dydx+y=0\frac{d^2y}{dx^2} - 2\frac{dy}{dx} + y = 0

The auxiliary equation is r2−2r+1=0r^2 - 2r + 1 = 0, giving (r−1)2=0(r - 1)^2 = 0, so r=1r = 1 is a repeated root. The general solution is:

g2(x)=(A+Bx)exg_2(x) = (A + Bx)e^x

We determine AA and BB from the continuous differentiability conditions at x=1x = 1.

Matching function values g1(1)=g2(1)g_1(1) = g_2(1):

1⋅e−1=(A+B)e  ⟹  A+B=e−2...(1)1 \cdot e^{-1} = (A + B)e \implies A + B = e^{-2} \qquad \text{...(1)}

Matching derivatives g1′(1)=g2′(1)g_1'(1) = g_2'(1). First:

g2′(x)=Bex+(A+Bx)ex=(A+B+Bx)exg_2'(x) = Be^x + (A + Bx)e^x = (A + B + Bx)e^x

g2′(1)=(A+2B)eg_2'(1) = (A + 2B)e

Since g1′(1)=0g_1'(1) = 0:

(A+2B)e=0  ⟹  A+2B=0  ⟹  A=−2B...(2)(A + 2B)e = 0 \implies A + 2B = 0 \implies A = -2B \qquad \text{...(2)}

Substituting (2) into (1):

−2B+B=e−2  ⟹  −B=e−2  ⟹  B=−e−2-2B + B = e^{-2} \implies -B = e^{-2} \implies B = -e^{-2}

A=−2(−e−2)=2e−2A = -2(-e^{-2}) = 2e^{-2}

Therefore:

g2(x)=(2e−2−e−2x)ex=(2−x)ex−2g_2(x) = (2e^{-2} - e^{-2}x)e^x = (2 - x)e^{x - 2}

We verify that g2′(x)<0g_2'(x) < 0 for x>1x > 1 to confirm the equation remains y′′−2y′+y=0y'' - 2y' + y = 0:

g2′(x)=(1−x)ex−2g_2'(x) = (1 - x)e^{x - 2}

For x>1x > 1: (1−x)<0(1 - x) < 0 and ex−2>0e^{x-2} > 0, so g2′(x)<0g_2'(x) < 0. This confirms ∣y′∣=−y′|y'| = -y' for x>1x > 1.

g1(x)=xe−x,g2(x)=(2−x)ex−2\boxed{g_1(x) = xe^{-x}, \qquad g_2(x) = (2 - x)e^{x - 2}}

Part (iii)

The curve y=g2(x)y = g_2(x) is the reflection of y=g1(x)y = g_1(x) in the vertical line x=1x = 1.

To see this, substitute x′=2−xx' = 2 - x (which reflects in x=1x = 1) into g1g_1:

g1(2−x)=(2−x)e−(2−x)=(2−x)ex−2=g2(x)g_1(2 - x) = (2 - x)e^{-(2 - x)} = (2 - x)e^{x - 2} = g_2(x)

So replacing xx by 2−x2 - x in g1g_1 gives g2g_2, confirming the reflection. ■\qquad \blacksquare

Part (iv)

Let y=k(x)y = k(x) be a solution of y′′+py′+qy=0y'' + py' + qy = 0 on [r,s][r, s], and let m(x)=k(c−x)m(x) = k(c - x).

Differentiating using the chain rule:

m′(x)=−k′(c−x)m'(x) = -k'(c - x)

m′′(x)=k′′(c−x)m''(x) = k''(c - x)

Substituting into y′′−py′+qyy'' - py' + qy:

m′′(x)−pm′(x)+qm(x)=k′′(c−x)+pk′(c−x)+qk(c−x)m''(x) - pm'(x) + qm(x) = k''(c - x) + pk'(c - x) + qk(c - x)

Since kk satisfies k′′+pk′+qk=0k'' + pk' + qk = 0 for all values of its argument in [r,s][r, s], and c−xc - x is the argument, we need c−x∈[r,s]c - x \in [r, s].

This requires r⩽c−x⩽sr \leqslant c - x \leqslant s, i.e., c−s⩽x⩽c−rc - s \leqslant x \leqslant c - r.

Therefore y=k(c−x)y = k(c - x) satisfies y′′−py′+qy=0y'' - py' + qy = 0 in the interval c−s⩽x⩽c−rc - s \leqslant x \leqslant c - r. ■\qquad \blacksquare

Part (v)

Showing h′(14π)=0h'(\frac{1}{4}\pi) = 0:

h(x)=e−xsin⁡xh(x) = e^{-x}\sin x

h′(x)=−e−xsin⁡x+e−xcos⁡x=e−x(cos⁡x−sin⁡x)h'(x) = -e^{-x}\sin x + e^{-x}\cos x = e^{-x}(\cos x - \sin x)

h′(π4)=e−π/4(cos⁡π4−sin⁡π4)=e−π/4(12−12)=0■h'\left(\frac{\pi}{4}\right) = e^{-\pi/4}\left(\cos\frac{\pi}{4} - \sin\frac{\pi}{4}\right) = e^{-\pi/4}\left(\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}\right) = 0 \qquad \blacksquare

(a) Finding yy for 14π⩽x⩽54π\frac{1}{4}\pi \leqslant x \leqslant \frac{5}{4}\pi:

On the interval [−34π,14π][-\frac{3}{4}\pi, \frac{1}{4}\pi], y=h(x)=e−xsin⁡xy = h(x) = e^{-x}\sin x satisfies y′′+2y′+2y=0y'' + 2y' + 2y = 0 (since h′(x)⩾0h'(x) \geqslant 0, so ∣y′∣=y′|y'| = y').

At x=14πx = \frac{1}{4}\pi, h′(14π)=0h'(\frac{1}{4}\pi) = 0. For xx just beyond 14π\frac{1}{4}\pi, cos⁡x−sin⁡x<0\cos x - \sin x < 0, so y′y' becomes negative. Therefore on [14π,54π][\frac{1}{4}\pi, \frac{5}{4}\pi], ∣y′∣=−y′|y'| = -y' and the equation becomes:

y′′−2y′+2y=0y'' - 2y' + 2y = 0

By part (iv) with p=2p = 2: if y=k(x)y = k(x) solves y′′+2y′+2y=0y'' + 2y' + 2y = 0, then y=k(c−x)y = k(c - x) solves y′′−2y′+2y=0y'' - 2y' + 2y = 0 on the interval c−s⩽x⩽c−rc - s \leqslant x \leqslant c - r.

We need k(c−x)k(c - x) to use the known solution hh on [−34π,14π][-\frac{3}{4}\pi, \frac{1}{4}\pi], so we require c−x∈[−34π,14π]c - x \in [-\frac{3}{4}\pi, \frac{1}{4}\pi] for x∈[14π,54π]x \in [\frac{1}{4}\pi, \frac{5}{4}\pi].

At x=14πx = \frac{1}{4}\pi: c−14π⩽14πc - \frac{1}{4}\pi \leqslant \frac{1}{4}\pi, so c⩽12πc \leqslant \frac{1}{2}\pi.

At x=54πx = \frac{5}{4}\pi: c−54π⩾−34πc - \frac{5}{4}\pi \geqslant -\frac{3}{4}\pi, so c⩾12πc \geqslant \frac{1}{2}\pi.

Therefore c=12πc = \frac{1}{2}\pi and the solution is:

y=h(π2−x)=e−(π/2−x)sin⁡(π2−x)=ex−π/2cos⁡xy = h\left(\frac{\pi}{2} - x\right) = e^{-(\pi/2 - x)}\sin\left(\frac{\pi}{2} - x\right) = e^{x - \pi/2}\cos x

Verification of continuous differentiability at x=14πx = \frac{1}{4}\pi:

From the left: h(π4)=e−π/4sin⁡π4=e−π/42h(\frac{\pi}{4}) = e^{-\pi/4}\sin\frac{\pi}{4} = \frac{e^{-\pi/4}}{\sqrt{2}}.

From the right: eπ/4−π/2cos⁡π4=e−π/4⋅12=e−π/42e^{\pi/4 - \pi/2}\cos\frac{\pi}{4} = e^{-\pi/4} \cdot \frac{1}{\sqrt{2}} = \frac{e^{-\pi/4}}{\sqrt{2}}. Values match. ✓\checkmark

From the left: h′(π4)=0h'(\frac{\pi}{4}) = 0.

From the right: ddx[ex−π/2cos⁡x]=ex−π/2(cos⁡x−sin⁡x)\frac{d}{dx}[e^{x - \pi/2}\cos x] = e^{x - \pi/2}(\cos x - \sin x), at x=π4x = \frac{\pi}{4}: e−π/4⋅0=0e^{-\pi/4} \cdot 0 = 0. Derivatives match. ✓\checkmark

(b) Finding yy for 54π⩽x⩽94π\frac{5}{4}\pi \leqslant x \leqslant \frac{9}{4}\pi:

On [14π,54π][\frac{1}{4}\pi, \frac{5}{4}\pi], the solution is m(x)=ex−π/2cos⁡xm(x) = e^{x - \pi/2}\cos x, satisfying y′′−2y′+2y=0y'' - 2y' + 2y = 0 (since m′(x)=ex−π/2(cos⁡x−sin⁡x)⩽0m'(x) = e^{x-\pi/2}(\cos x - \sin x) \leqslant 0 there).

At x=54πx = \frac{5}{4}\pi: m′(54π)=e3π/4(cos⁡5π4−sin⁡54π)=e3π/4(−12+12)=0m'(\frac{5}{4}\pi) = e^{3\pi/4}(\cos\frac{5\pi}{4} - \sin\frac{5}{4}\pi) = e^{3\pi/4}(-\frac{1}{\sqrt{2}} + \frac{1}{\sqrt{2}}) = 0.

For xx just beyond 54π\frac{5}{4}\pi: cos⁡x−sin⁡x>0\cos x - \sin x > 0 (e.g., at x=32πx = \frac{3}{2}\pi: cos⁡3π2−sin⁡3π2=0+1=1\cos\frac{3\pi}{2} - \sin\frac{3\pi}{2} = 0 + 1 = 1), so y′y' becomes positive. Therefore ∣y′∣=y′|y'| = y' and the equation returns to y′′+2y′+2y=0y'' + 2y' + 2y = 0.

By part (iv) with p=−2p = -2: if y=m(x)y = m(x) solves y′′−2y′+2y=0y'' - 2y' + 2y = 0, then y=m(c−x)y = m(c - x) solves y′′+2y′+2y=0y'' + 2y' + 2y = 0 on [c−54π,c−14π][c - \frac{5}{4}\pi, c - \frac{1}{4}\pi].

We need [c−54π,c−14π]=[54π,94π][c - \frac{5}{4}\pi, c - \frac{1}{4}\pi] = [\frac{5}{4}\pi, \frac{9}{4}\pi]:

c−54π=54π  ⟹  c=52πc - \frac{5}{4}\pi = \frac{5}{4}\pi \implies c = \frac{5}{2}\pi

Check: c−14π=52π−14π=94πc - \frac{1}{4}\pi = \frac{5}{2}\pi - \frac{1}{4}\pi = \frac{9}{4}\pi. ✓\checkmark

The solution is:

y=m(5π2−x)=e(5π/2−x)−π/2cos⁡(5π2−x)=e2π−xcos⁡(5π2−x)y = m\left(\frac{5\pi}{2} - x\right) = e^{(5\pi/2 - x) - \pi/2}\cos\left(\frac{5\pi}{2} - x\right) = e^{2\pi - x}\cos\left(\frac{5\pi}{2} - x\right)

Since 5π2=2π+π2\frac{5\pi}{2} = 2\pi + \frac{\pi}{2}:

cos⁡(5π2−x)=cos⁡(2π+π2−x)=cos⁡(π2−x)=sin⁡x\cos\left(\frac{5\pi}{2} - x\right) = \cos\left(2\pi + \frac{\pi}{2} - x\right) = \cos\left(\frac{\pi}{2} - x\right) = \sin x

Therefore:

y=e2π−xsin⁡x\boxed{y = e^{2\pi - x}\sin x}

Verification of continuous differentiability at x=54πx = \frac{5}{4}\pi:

From the left: e5π/4−π/2cos⁡5π4=e3π/4⋅(−12)e^{5\pi/4 - \pi/2}\cos\frac{5\pi}{4} = e^{3\pi/4} \cdot \left(-\frac{1}{\sqrt{2}}\right).

From the right: e2π−5π/4sin⁡5π4=e3π/4⋅(−12)e^{2\pi - 5\pi/4}\sin\frac{5\pi}{4} = e^{3\pi/4} \cdot \left(-\frac{1}{\sqrt{2}}\right). Values match. ✓\checkmark

From the left: m′(5π4)=0m'(\frac{5\pi}{4}) = 0 (computed above).

From the right: ddx[e2π−xsin⁡x]=e2π−x(cos⁡x−sin⁡x)\frac{d}{dx}[e^{2\pi - x}\sin x] = e^{2\pi - x}(\cos x - \sin x), at x=5π4x = \frac{5\pi}{4}: e3π/4(−12+12)=0e^{3\pi/4}(-\frac{1}{\sqrt{2}} + \frac{1}{\sqrt{2}}) = 0. Derivatives match. ✓\checkmark

Examiner Notes

中等受欢迎(略低于Q2),平均分7.3/20。第(ii)部分常见错误:直接翻转 g₁ 的符号而非重新求解。第(iii)部分极差。第(v)(b)部分常见错误:在 −π/4 而非 5π/4 处匹配函数值。