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STEP3 2014 -- Pure Mathematics

STEP3 2014 — Section A (Pure Mathematics)

Section titled “STEP3 2014 — Section A (Pure Mathematics)”

Exam: STEP3  |  Year: 2014  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1代数与级数 (Algebra and Series)Challenging对称多项式, 对数级数展开, 系数比较, 反例构造
2积分 (Integration)Standard双曲函数恒等式, 代换积分法, 分式分解, 定积分计算
3解析几何与优化 (Coordinate Geometry and Optimisation)Challenging抛物线参数方程, 法线方程, 距离优化, 分类讨论
4积分不等式 (Integral Inequalities)Hard完全微分, 积分恒等式, sec2x=1+tan2x\sec^2 x = 1 + \tan^2 x, 边值条件, 积分因子
5复数与几何 (Complex Numbers and Geometry)Challenging复数表示向量, 平行四边形判定, 正方形判定, 旋转乘 ii, 充分必要条件
6分析 (Analysis)Hard正函数积分保号性,二次积分法,凸函数判定,三角双曲函数构造
7几何 (Geometry)Hard圆的弦性质,向量表示,反证法,相似三角形
8级数与数论 (Series and Number Theory)Hard分块求和估计,几何级数界,数字组合计数,调和级数发散性

Topic: 代数与级数 (Algebra and Series)  |  Difficulty: Challenging  |  Marks: 20

1 Let aa, bb and cc be real numbers such that a+b+c=0a + b + c = 0 and let

(1+ax)(1+bx)(1+cx)=1+qx2+rx3(1 + ax)(1 + bx)(1 + cx) = 1 + qx^2 + rx^3

for all real xx. Show that q=bc+ca+abq = bc + ca + ab and r=abcr = abc.

(i) Show that the coefficient of xnx^n in the series expansion (in ascending powers of xx) of ln(1+qx2+rx3)\ln(1 + qx^2 + rx^3) is (1)n+1Sn(-1)^{n+1}S_n where

Sn=an+bn+cnn,(n1).S_n = \frac{a^n + b^n + c^n}{n}, \quad (n \geqslant 1).

(ii) Find, in terms of qq and rr, the coefficients of x2x^2, x3x^3 and x5x^5 in the series expansion (in ascending powers of xx) of ln(1+qx2+rx3)\ln(1 + qx^2 + rx^3) and hence show that S2S3=S5S_2S_3 = S_5.

(iii) Show that S2S5=S7S_2S_5 = S_7.

(iv) Give a proof of, or find a counterexample to, the claim that S2S7=S9S_2S_7 = S_9.

Hint

The stem results are obtained through algebraic expansion and equating coefficients. Using the expression (1+ax)(1+bx)(1+cx)(1 + ax)(1 + bx)(1 + cx) for 1+qx2+rx31 + qx^2 + rx^3, manipulating the logarithm of the product, and the series expansions for expressions like ln(1+ax)\ln(1 + ax) yields the displayed result. In parts (ii), (iii), and (iv), it is simplest to find S2=qS_2 = -q, S3=rS_3 = r, S5=qrS_5 = -qr, S7=q2rS_7 = q^2r, and S9=r33q3rS_9 = \frac{r^3}{3} - q^3r by expanding the series for ln(1+(qx2+rx3))\ln(1 + (qx^2 + rx^3)), and choosing a counter-example, selecting a, b and c so that r0r \neq 0.

Model Solution

Stem result. Expanding the left-hand side:

(1+ax)(1+bx)(1+cx)=(1+ax)(1+(b+c)x+bcx2)(1+ax)(1+bx)(1+cx) = (1+ax)\bigl(1 + (b+c)x + bcx^2\bigr) =1+(b+c)x+bcx2+ax+a(b+c)x2+abcx3= 1 + (b+c)x + bcx^2 + ax + a(b+c)x^2 + abcx^3 =1+(a+b+c)x+(ab+bc+ca)x2+abcx3.= 1 + (a+b+c)x + (ab+bc+ca)x^2 + abc\,x^3.

Since a+b+c=0a+b+c = 0, the coefficient of xx vanishes, giving q=ab+bc+caq = ab+bc+ca and r=abcr = abc. \square


Part (i) Since 1+qx2+rx3=(1+ax)(1+bx)(1+cx)1 + qx^2 + rx^3 = (1+ax)(1+bx)(1+cx), we have

ln(1+qx2+rx3)=ln(1+ax)+ln(1+bx)+ln(1+cx).\ln(1+qx^2+rx^3) = \ln(1+ax) + \ln(1+bx) + \ln(1+cx).

Using the standard expansion ln(1+t)=k=1(1)k+1ktk\ln(1+t) = \displaystyle\sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}\,t^k for t<1|t| < 1:

ln(1+ax)=k=1(1)k+1kakxk,\ln(1+ax) = \sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}\,a^k x^k,

and similarly for bb and cc. Summing all three:

ln(1+qx2+rx3)=k=1(1)k+1k(ak+bk+ck)xk.\ln(1+qx^2+rx^3) = \sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}\,(a^k+b^k+c^k)\,x^k.

The coefficient of xnx^n is therefore

(1)n+1n(an+bn+cn)=(1)n+1Sn.\frac{(-1)^{n+1}}{n}\,(a^n+b^n+c^n) = (-1)^{n+1}\,S_n.

\square


Part (ii) We expand ln(1+qx2+rx3)\ln(1 + qx^2 + rx^3) using ln(1+u)=uu22+u33\ln(1+u) = u - \frac{u^2}{2} + \frac{u^3}{3} - \cdots with u=qx2+rx3u = qx^2 + rx^3.

Coefficient of x2x^2: only the term u=qx2+rx3u = qx^2 + rx^3 contributes, giving qq.

Coefficient of x3x^3: only uu contributes (via rx3rx^3), giving rr.

Coefficient of x5x^5: from uu we get nothing (max power is x3x^3); from u22-\frac{u^2}{2}:

u2=(qx2+rx3)2=q2x4+2qrx5+r2x6,u^2 = (qx^2+rx^3)^2 = q^2x^4 + 2qrx^5 + r^2x^6,

so the x5x^5 contribution is 122qr=qr-\frac{1}{2}\cdot 2qr = -qr. From u33\frac{u^3}{3}:

u3=(qx2+rx3)3=q3x6+3q2rx7+,u^3 = (qx^2+rx^3)^3 = q^3x^6 + 3q^2rx^7 + \cdots,

so the x5x^5 contribution is 00. Higher terms also give no x5x^5. Therefore the coefficient of x5x^5 is qr-qr.

From Part (i), the coefficient of xnx^n is (1)n+1Sn(-1)^{n+1}S_n. Matching:

coeff of x2=q=(1)3S2=S2    S2=q,\text{coeff of } x^2 = q = (-1)^3 S_2 = -S_2 \implies S_2 = -q, coeff of x3=r=(1)4S3=S3    S3=r,\text{coeff of } x^3 = r = (-1)^4 S_3 = S_3 \implies S_3 = r, coeff of x5=qr=(1)6S5=S5    S5=qr.\text{coeff of } x^5 = -qr = (-1)^6 S_5 = S_5 \implies S_5 = -qr.

Therefore S2S3=(q)(r)=qr=S5S_2 S_3 = (-q)(r) = -qr = S_5. \square


Part (iii) We need S7S_7, so we find the coefficient of x7x^7 in ln(1+qx2+rx3)\ln(1+qx^2+rx^3).

From uu: no x7x^7 term (max power x3x^3).

From u22-\frac{u^2}{2}: u2=q2x4+2qrx5+r2x6u^2 = q^2x^4 + 2qrx^5 + r^2x^6, so no x7x^7.

From u33\frac{u^3}{3}:

u3=(qx2+rx3)3=q3x6+3q2rx7+3qr2x8+r3x9,u^3 = (qx^2+rx^3)^3 = q^3x^6 + 3q^2rx^7 + 3qr^2x^8 + r^3x^9,

so the x7x^7 contribution is 133q2r=q2r\frac{1}{3}\cdot 3q^2r = q^2r.

From u44-\frac{u^4}{4}: u4u^4 starts at x8x^8, so no x7x^7.

Higher terms also give no x7x^7. Therefore the coefficient of x7x^7 is q2rq^2r, giving

(1)8S7=q2r    S7=q2r.(-1)^8 S_7 = q^2r \implies S_7 = q^2r.

Hence S2S5=(q)(qr)=q2r=S7S_2 S_5 = (-q)(-qr) = q^2r = S_7. \square


Part (iv) We need S9S_9, so we find the coefficient of x9x^9 in ln(1+qx2+rx3)\ln(1+qx^2+rx^3).

From uu: no x9x^9.

From u22-\frac{u^2}{2}: u2=q2x4+2qrx5+r2x6u^2 = q^2x^4 + 2qrx^5 + r^2x^6, so no x9x^9.

From u33\frac{u^3}{3}: u3=q3x6+3q2rx7+3qr2x8+r3x9u^3 = q^3x^6 + 3q^2rx^7 + 3qr^2x^8 + r^3x^9, giving 13r3\frac{1}{3}r^3.

From u44-\frac{u^4}{4}: u4=(qx2+rx3)4=q4x8+4q3rx9+u^4 = (qx^2+rx^3)^4 = q^4x^8 + 4q^3rx^9 + \cdots, giving 144q3r=q3r-\frac{1}{4}\cdot 4q^3r = -q^3r.

From u55\frac{u^5}{5}: u5u^5 starts at x10x^{10}, so no x9x^9.

Higher terms also contribute nothing. Therefore the coefficient of x9x^9 is r33q3r\frac{r^3}{3} - q^3r, giving

(1)10S9=r33q3r    S9=r33q3r.(-1)^{10} S_9 = \frac{r^3}{3} - q^3r \implies S_9 = \frac{r^3}{3} - q^3r.

Now S2S7=(q)(q2r)=q3rS_2 S_7 = (-q)(q^2r) = -q^3r. The claim S2S7=S9S_2 S_7 = S_9 requires

q3r=r33q3r    r33=0    r=0.-q^3r = \frac{r^3}{3} - q^3r \implies \frac{r^3}{3} = 0 \implies r = 0.

Since the claim must hold for all valid a,b,ca, b, c, it fails whenever r0r \neq 0. A concrete counterexample: take a=1,b=1,c=2a = 1, b = 1, c = -2 (so a+b+c=0a+b+c=0). Then q=11+1(2)+(2)1=3q = 1\cdot 1 + 1\cdot(-2) + (-2)\cdot 1 = -3 and r=11(2)=2r = 1\cdot 1\cdot(-2) = -2.

S2=q=3,S7=q2r=9(2)=18,S9=(2)33(3)3(2)=8354=1703.S_2 = -q = 3, \quad S_7 = q^2r = 9\cdot(-2) = -18, \quad S_9 = \frac{(-2)^3}{3} - (-3)^3(-2) = -\frac{8}{3} - 54 = -\frac{170}{3}. S2S7=3(18)=541703=S9.S_2 S_7 = 3\cdot(-18) = -54 \neq -\frac{170}{3} = S_9.

The claim is false. \square

Examiner Notes

This was the most popular question on the paper, being attempted by approximately 14 out of every 15 candidates. It was the second most successfully attempted with a mean score of half marks. The stem of the question caused no problems, but a common mistake in part (i) was to attempt derivatives to obtain the desired result. Most candidates came unstuck in part (ii), making it much more difficult for themselves by attempting to work with expressions in a, b, and c rather than using the log series working with q and r, and as a result making sign errors, putting part (iii) beyond reach, and although they could find counterexamples for the claim in part (iv), they did so without the clear direction that working with the expressions in q and r would have made obvious.


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

2 (i) Show, by means of the substitution u=coshxu = \cosh x, that

sinhxcosh2xdx=122ln2coshx12coshx+1+C.\int \frac{\sinh x}{\cosh 2x} \, dx = \frac{1}{2\sqrt{2}} \ln \left| \frac{\sqrt{2} \cosh x - 1}{\sqrt{2} \cosh x + 1} \right| + C.

(ii) Use a similar substitution to find an expression for

coshxcosh2xdx.\int \frac{\cosh x}{\cosh 2x} \, dx.

(iii) Using parts (i) and (ii) above, show that

0111+u4du=π+2ln(2+1)42.\int_0^1 \frac{1}{1 + u^4} \, du = \frac{\pi + 2 \ln(\sqrt{2} + 1)}{4\sqrt{2}}.

Hint

The first part is solved using the given method, the formula cosh2x=2cosh2x1\cosh 2x = 2 \cosh^2 x - 1, and then employing partial fractions or the standard form quoted in the formula book. The second part requires the substitution, u=sinhxu = \sinh x, the formula cosh2x=1+2sinh2x\cosh 2x = 1 + 2 \sinh^2 x, and a standard form to give 22tan12u+c\frac{\sqrt{2}}{2} \tan^{-1} \sqrt{2} u + c. The third part can be approached by making the substitution u=exu = e^x and division of the resulting fraction in the numerator and denominator by e2xe^{2x} to give half the difference of the integrals in the first two parts. Alternatively, a similar style of working with the substitution u=exu = e^{-x} results in a sum instead of a difference.

Model Solution

Part (i) Let u=coshxu = \cosh x, so du=sinhxdxdu = \sinh x \, dx. Using the double-angle identity cosh2x=2cosh2x1=2u21\cosh 2x = 2\cosh^2 x - 1 = 2u^2 - 1:

sinhxcosh2xdx=du2u21.\int \frac{\sinh x}{\cosh 2x} \, dx = \int \frac{du}{2u^2 - 1}.

We use partial fractions. Factor 2u21=(2u1)(2u+1)2u^2 - 1 = (\sqrt{2}\,u - 1)(\sqrt{2}\,u + 1), so

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

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

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

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

Therefore

du2u21=12du2u112du2u+1\int \frac{du}{2u^2 - 1} = \frac{1}{2}\int \frac{du}{\sqrt{2}\,u - 1} - \frac{1}{2}\int \frac{du}{\sqrt{2}\,u + 1} =122ln2u1122ln2u+1+C= \frac{1}{2\sqrt{2}}\ln|\sqrt{2}\,u - 1| - \frac{1}{2\sqrt{2}}\ln|\sqrt{2}\,u + 1| + C =122ln2u12u+1+C.= \frac{1}{2\sqrt{2}}\ln\left|\frac{\sqrt{2}\,u - 1}{\sqrt{2}\,u + 1}\right| + C.

Substituting back u=coshxu = \cosh x:

sinhxcosh2xdx=122ln2coshx12coshx+1+C.\int \frac{\sinh x}{\cosh 2x} \, dx = \frac{1}{2\sqrt{2}}\ln\left|\frac{\sqrt{2}\cosh x - 1}{\sqrt{2}\cosh x + 1}\right| + C.

\square


Part (ii) Let u=sinhxu = \sinh x, so du=coshxdxdu = \cosh x \, dx. Using cosh2x=1+2sinh2x=1+2u2\cosh 2x = 1 + 2\sinh^2 x = 1 + 2u^2:

coshxcosh2xdx=du1+2u2.\int \frac{\cosh x}{\cosh 2x} \, dx = \int \frac{du}{1 + 2u^2}.

This is a standard arctangent integral. Setting v=2uv = \sqrt{2}\,u, dv=2dudv = \sqrt{2}\,du:

du1+2u2=dv/21+v2=12arctanv+C=12arctan(2sinhx)+C.\int \frac{du}{1 + 2u^2} = \int \frac{dv/\sqrt{2}}{1 + v^2} = \frac{1}{\sqrt{2}}\arctan v + C = \frac{1}{\sqrt{2}}\arctan(\sqrt{2}\,\sinh x) + C.

\square


Part (iii) We evaluate I=01du1+u4I = \displaystyle\int_0^1 \frac{du}{1 + u^4}.

Factor 1+u4=(u2+2u+1)(u22u+1)1 + u^4 = (u^2 + \sqrt{2}\,u + 1)(u^2 - \sqrt{2}\,u + 1). We use partial fractions:

11+u4=Au+Bu2+2u+1+Cu+Du22u+1.\frac{1}{1+u^4} = \frac{Au + B}{u^2 + \sqrt{2}\,u + 1} + \frac{Cu + D}{u^2 - \sqrt{2}\,u + 1}.

Multiplying through:

1=(Au+B)(u22u+1)+(Cu+D)(u2+2u+1).1 = (Au+B)(u^2 - \sqrt{2}\,u + 1) + (Cu+D)(u^2 + \sqrt{2}\,u + 1).

Expanding and collecting powers of uu:

u3:A+C=0    C=A,u^3: \quad A + C = 0 \implies C = -A, u2:2A+B+2C+D=0    22A+B+D=0,u^2: \quad -\sqrt{2}\,A + B + \sqrt{2}\,C + D = 0 \implies -2\sqrt{2}\,A + B + D = 0, u1:A2B+C+2D=0    2(DB)=0    D=B,u^1: \quad A - \sqrt{2}\,B + C + \sqrt{2}\,D = 0 \implies \sqrt{2}(D - B) = 0 \implies D = B, u0:B+D=1    2B=1    B=D=12.u^0: \quad B + D = 1 \implies 2B = 1 \implies B = D = \tfrac{1}{2}.

From u2u^2: 22A+1=0-2\sqrt{2}\,A + 1 = 0, so A=122A = \frac{1}{2\sqrt{2}}, and C=122C = -\frac{1}{2\sqrt{2}}.

Therefore

I=12201uu2+2u+1du12201uu22u+1du+1201duu2+2u+1+1201duu22u+1.I = \frac{1}{2\sqrt{2}}\int_0^1 \frac{u}{u^2+\sqrt{2}\,u+1}\,du - \frac{1}{2\sqrt{2}}\int_0^1 \frac{u}{u^2-\sqrt{2}\,u+1}\,du + \frac{1}{2}\int_0^1 \frac{du}{u^2+\sqrt{2}\,u+1} + \frac{1}{2}\int_0^1 \frac{du}{u^2-\sqrt{2}\,u+1}.

We evaluate each integral separately.

Logarithmic integrals. Write u=12(2u+2)22u = \frac{1}{2}(2u + \sqrt{2}) - \frac{\sqrt{2}}{2} in the first, and u=12(2u2)+22u = \frac{1}{2}(2u - \sqrt{2}) + \frac{\sqrt{2}}{2} in the second:

uu2+2u+1du=12ln(u2+2u+1)22duu2+2u+1,\int \frac{u}{u^2+\sqrt{2}\,u+1}\,du = \frac{1}{2}\ln(u^2+\sqrt{2}\,u+1) - \frac{\sqrt{2}}{2}\int \frac{du}{u^2+\sqrt{2}\,u+1}, uu22u+1du=12ln(u22u+1)+22duu22u+1.\int \frac{u}{u^2-\sqrt{2}\,u+1}\,du = \frac{1}{2}\ln(u^2-\sqrt{2}\,u+1) + \frac{\sqrt{2}}{2}\int \frac{du}{u^2-\sqrt{2}\,u+1}.

Substituting back, the 22\frac{\sqrt{2}}{2}-type terms cancel with parts of the 12duu2±2u+1\frac{1}{2}\int \frac{du}{u^2 \pm \sqrt{2}u + 1} contributions, and we are left with:

I=142[ln(u2+2u+1)ln(u22u+1)]01+1201duu2+2u+1+1201duu22u+1.I = \frac{1}{4\sqrt{2}}\left[\ln(u^2+\sqrt{2}\,u+1) - \ln(u^2-\sqrt{2}\,u+1)\right]_0^1 + \frac{1}{2}\int_0^1 \frac{du}{u^2+\sqrt{2}\,u+1} + \frac{1}{2}\int_0^1 \frac{du}{u^2-\sqrt{2}\,u+1}.

Arctangent integrals. Complete the square:

u2+2u+1=(u+22)2+12,u22u+1=(u22)2+12.u^2 + \sqrt{2}\,u + 1 = \left(u + \frac{\sqrt{2}}{2}\right)^2 + \frac{1}{2}, \qquad u^2 - \sqrt{2}\,u + 1 = \left(u - \frac{\sqrt{2}}{2}\right)^2 + \frac{1}{2}.

Using dww2+a2=1aarctanwa\displaystyle\int \frac{dw}{w^2 + a^2} = \frac{1}{a}\arctan\frac{w}{a} with a=12a = \frac{1}{\sqrt{2}}:

01duu2+2u+1=[2arctan ⁣(2u+1)]01=2(arctan(2+1)arctan1),\int_0^1 \frac{du}{u^2+\sqrt{2}\,u+1} = \left[\sqrt{2}\,\arctan\!\left(\sqrt{2}\,u + 1\right)\right]_0^1 = \sqrt{2}\left(\arctan(\sqrt{2}+1) - \arctan 1\right), 01duu22u+1=[2arctan ⁣(2u1)]01=2(arctan(21)+arctan1).\int_0^1 \frac{du}{u^2-\sqrt{2}\,u+1} = \left[\sqrt{2}\,\arctan\!\left(\sqrt{2}\,u - 1\right)\right]_0^1 = \sqrt{2}\left(\arctan(\sqrt{2}-1) + \arctan 1\right).

Adding these two:

arctan(2+1)+arctan(21)=π2,\arctan(\sqrt{2}+1) + \arctan(\sqrt{2}-1) = \frac{\pi}{2},

since (2+1)(21)=1(\sqrt{2}+1)(\sqrt{2}-1) = 1, and the identity arctanp+arctanq=π2\arctan p + \arctan q = \frac{\pi}{2} holds when pq=1pq = 1 and p>0p > 0. Therefore the sum of the arctangent integrals is 2π2=π22\sqrt{2} \cdot \frac{\pi}{2} = \frac{\pi\sqrt{2}}{2}.

Logarithmic part. At u=1u = 1: u2+2u+1=2+2u^2 + \sqrt{2}\,u + 1 = 2 + \sqrt{2} and u22u+1=22u^2 - \sqrt{2}\,u + 1 = 2 - \sqrt{2}. At u=0u = 0: both equal 11. So

142ln2+222.\frac{1}{4\sqrt{2}}\ln\frac{2+\sqrt{2}}{2-\sqrt{2}}.

Rationalise:

2+2222+22+2=(2+2)242=6+422=3+22=(1+2)2.\frac{2+\sqrt{2}}{2-\sqrt{2}} \cdot \frac{2+\sqrt{2}}{2+\sqrt{2}} = \frac{(2+\sqrt{2})^2}{4-2} = \frac{6+4\sqrt{2}}{2} = 3+2\sqrt{2} = (1+\sqrt{2})^2.

So the logarithmic part is 1422ln(1+2)=ln(1+2)22\frac{1}{4\sqrt{2}} \cdot 2\ln(1+\sqrt{2}) = \frac{\ln(1+\sqrt{2})}{2\sqrt{2}}.

Combining:

I=ln(1+2)22+12π22=ln(1+2)22+π22=π+2ln(2+1)42.I = \frac{\ln(1+\sqrt{2})}{2\sqrt{2}} + \frac{1}{2} \cdot \frac{\pi\sqrt{2}}{2} = \frac{\ln(1+\sqrt{2})}{2\sqrt{2}} + \frac{\pi}{2\sqrt{2}} = \frac{\pi + 2\ln(\sqrt{2}+1)}{4\sqrt{2}}.

\square

Examiner Notes

This was only marginally less popular than question 1, but was the most successfully attempted with a mean of two thirds marks. Most that attempted the question were able to do the first two parts easily, but could not find a suitable substitution to do the last part. In about a tenth of the attempts, a helpful substitution was made in part (iii) which then usually resulted in successful completion of the question. Modulus signs were often ignored, or could not be distinguished from usual parentheses, and the arbitrary constant, even though it appeared in the result for part (i), was frequently overlooked. A few did not use the correct formulae for cosh2x\cosh 2x, instead resorting to the trigon versions. A handful of candidates attempted partial fractions in the last part having correctly factorised the quartic, but this did not use the previous parts as instructed.


Topic: 解析几何与优化 (Coordinate Geometry and Optimisation)  |  Difficulty: Challenging  |  Marks: 20

3 (i) The line LL has equation y=mx+cy = mx + c, where m>0m > 0 and c>0c > 0. Show that, in the case mc>a>0mc > a > 0, the shortest distance between LL and the parabola y2=4axy^2 = 4ax is

mcamm2+1.\frac{mc - a}{m\sqrt{m^2 + 1}}.

What is the shortest distance in the case that $mc \leqslant a$?
**(ii)** Find the shortest distance between the point $(p, 0)$, where $p > 0$, and the parabola $y^2 = 4ax$, where $a > 0$, in the different cases that arise according to the value of $p/a$. [*You may wish to use the parametric coordinates $(at^2, 2at)$ of points on the parabola.*]
Hence find the shortest distance between the circle $(x - p)^2 + y^2 = b^2$, where $p > 0$ and $b > 0$, and the parabola $y^2 = 4ax$, where $a > 0$, in the different cases that arise according to the values of $p, a$ and $b$.
Hint

(i) Given that the shortest distance between the line and the parabola will be zero if they meet, investigating the solution of the equations simultaneously, and the discriminant of the resulting quadratic equation, the first result of the question is the case that they do not meet. The closest approach is the perpendicular distance of the point on the parabola where the tangent is parallel to the line, so using the standard parametric form, it is the perpendicular distance of (am2,2am)(\frac{a}{m^2}, \frac{2a}{m}) from y=mx+cy = mx + c, giving the required result with care being taken over the sign of the numerator bearing in mind the inequalities.

(ii) The shortest distance of a point on the axis from the parabola, is either the distance from the vertex to the point, or the distance along one of the normals (which are symmetrically situated) which is not the axis. If the normal at (at2,2at)(at^2, 2at) passes through (p,0)(p, 0), then p=2a+at2p = 2a + at^2. From this it can be simply shown that shortest distance is pp if pa<2\frac{p}{a} < 2, and is 2a(pa)2\sqrt{a(p - a)} if pa2\frac{p}{a} \geq 2.

Then for the circle, the results follow simply, that the shortest distance will be pbp - b if p>bp > b, and 0 otherwise if pa<2\frac{p}{a} < 2, and 2a(pa)b2\sqrt{a(p - a)} - b if 4a(pa)>b24a(p - a) > b^2 or 0 otherwise if pa2\frac{p}{a} \geq 2.

Model Solution

Part (i)

Substituting y=mx+cy = mx + c into y2=4axy^2 = 4ax:

(mx+c)2=4ax(mx + c)^2 = 4ax

m2x2+2mcx+c2=4axm^2 x^2 + 2mcx + c^2 = 4ax

m2x2+(2mc4a)x+c2=0.m^2 x^2 + (2mc - 4a)x + c^2 = 0.

This is a quadratic in xx. The discriminant is

Δ=(2mc4a)24m2c2=4(mc2a)24m2c2\Delta = (2mc - 4a)^2 - 4m^2 c^2 = 4(mc - 2a)^2 - 4m^2 c^2

=4(m2c24amc+4a2m2c2)=4(4a24amc)=16a(amc).= 4(m^2 c^2 - 4amc + 4a^2 - m^2 c^2) = 4(4a^2 - 4amc) = 16a(a - mc).

When mc>a>0mc > a > 0, we have Δ<0\Delta < 0, so the line and parabola do not meet. The shortest distance between them is therefore strictly positive.

The shortest distance from LL to the parabola occurs at a point on the parabola where the tangent is parallel to LL (i.e., has slope mm). Using the parametric form (at2,2at)(at^2, 2at) on the parabola:

dydx=dy/dtdx/dt=2a2at=1t.\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{2a}{2at} = \frac{1}{t}.

Setting 1t=m\frac{1}{t} = m gives t=1mt = \frac{1}{m}, so the point is (am2,2am)\left(\frac{a}{m^2},\, \frac{2a}{m}\right).

The perpendicular distance from a point (x0,y0)(x_0, y_0) to the line y=mx+cy = mx + c, i.e.\ mxy+c=0mx - y + c = 0, is mx0y0+cm2+1\frac{|mx_0 - y_0 + c|}{\sqrt{m^2 + 1}}.

At the point (am2,2am)\left(\frac{a}{m^2},\, \frac{2a}{m}\right):

d=mam22am+cm2+1=am2am+cm2+1=camm2+1=mcamm2+1.d = \frac{\left|m \cdot \frac{a}{m^2} - \frac{2a}{m} + c\right|}{\sqrt{m^2 + 1}} = \frac{\left|\frac{a}{m} - \frac{2a}{m} + c\right|}{\sqrt{m^2 + 1}} = \frac{\left|c - \frac{a}{m}\right|}{\sqrt{m^2 + 1}} = \frac{|mc - a|}{m\sqrt{m^2 + 1}}.

Since mc>a>0mc > a > 0, we have mca>0mc - a > 0, so mca=mca|mc - a| = mc - a, giving

d=mcamm2+1.d = \frac{mc - a}{m\sqrt{m^2 + 1}}.

When mcamc \leqslant a, the discriminant Δ0\Delta \geqslant 0, so the line and parabola intersect (or are tangent). The shortest distance in this case is 0.

Part (ii)

We seek the shortest distance from the point (p,0)(p, 0) to the parabola y2=4axy^2 = 4ax.

Using parametric coordinates (at2,2at)(at^2, 2at) on the parabola, the distance squared is

d2(t)=(at2p)2+(2at)2=(at2p)2+4a2t2.d^2(t) = (at^2 - p)^2 + (2at)^2 = (at^2 - p)^2 + 4a^2 t^2.

The normal to the parabola at parameter tt has slope t-t, and its equation is

y2at=t(xat2).y - 2at = -t(x - at^2).

If the normal passes through (p,0)(p, 0):

02at=t(pat2)=tp+at30 - 2at = -t(p - at^2) = -tp + at^3

2at+tpat3=0-2at + tp - at^3 = 0

t(p2aat2)=0.t(p - 2a - at^2) = 0.

So either t=0t = 0 (the normal at the vertex, which is the xx-axis itself), or

at2=p2a    t2=p2aa.at^2 = p - 2a \quad \implies \quad t^2 = \frac{p - 2a}{a}.

This has real solutions for tt if and only if p2ap \geqslant 2a.

Case 1: p<2ap < 2a. No normal from (p,0)(p, 0) meets the parabola at a point other than the vertex. Since p>0p > 0 and the vertex is at the origin, the closest point is the vertex itself, and the shortest distance is pp.

Case 2: p2ap \geqslant 2a. The normal through (p,0)(p, 0) meets the parabola at t2=p2aat^2 = \frac{p - 2a}{a}. The distance squared at this point is

d2=(ap2aap)2+4a2p2aad^2 = \left(a \cdot \frac{p - 2a}{a} - p\right)^2 + 4a^2 \cdot \frac{p - 2a}{a}

=(p2ap)2+4a(p2a)=4a2+4a(p2a)=4a(pa).= (p - 2a - p)^2 + 4a(p - 2a) = 4a^2 + 4a(p - 2a) = 4a(p - a).

So d=2a(pa)d = 2\sqrt{a(p - a)}. We verify this is less than pp when p>2ap > 2a: indeed 4a(pa)<p2    4ap4a2<p2    (p2a)2>04a(p-a) < p^2 \iff 4ap - 4a^2 < p^2 \iff (p - 2a)^2 > 0, which holds for p2ap \neq 2a.

Therefore:

Shortest distance={pif p<2a,2a(pa)if p2a.\text{Shortest distance} = \begin{cases} p & \text{if } p < 2a, \\[4pt] 2\sqrt{a(p - a)} & \text{if } p \geqslant 2a. \end{cases}

Distance from the circle to the parabola.

The circle (xp)2+y2=b2(x - p)^2 + y^2 = b^2 has centre (p,0)(p, 0) and radius bb. The shortest distance from the circle to the parabola equals the shortest distance from the centre (p,0)(p, 0) to the parabola, minus bb (provided this is positive; otherwise the circle and parabola meet, and the distance is 00).

Case 1: p<2ap < 2a. The shortest distance from (p,0)(p, 0) to the parabola is pp.

  • If p>bp > b: the shortest distance from the circle to the parabola is pbp - b.
  • If pbp \leqslant b: the shortest distance is 00.

Case 2: p2ap \geqslant 2a. The shortest distance from (p,0)(p, 0) to the parabola is 2a(pa)2\sqrt{a(p - a)}.

  • If 4a(pa)>b24a(p - a) > b^2, i.e.\ 2a(pa)>b2\sqrt{a(p - a)} > b: the shortest distance from the circle to the parabola is 2a(pa)b2\sqrt{a(p - a)} - b.
  • If 4a(pa)b24a(p - a) \leqslant b^2: the shortest distance is 00.
Examiner Notes

About half of the candidates attempted this, but it was the second least successfully attempted with a mean score just below a quarter marks. Most managed the first result, with those not doing so falling foul of various basic algebraic errors. The second result of part (i) was often answered with no justification. The second part was poorly done with a variety of approaches attempted such as obtaining a distance function, and then using completing the square or differentiation, or investigating the intersections of the circle and parabola. Few considered the geometry of the parabola and its normal which would have yielded the results fairly simply.


Topic: 积分不等式 (Integral Inequalities)  |  Difficulty: Hard  |  Marks: 20

4 (i) Let

I=01((y)2y2)dxandI1=01(y+ytanx)2dx,I = \int_0^1 ((y')^2 - y^2) \, dx \quad \text{and} \quad I_1 = \int_0^1 (y' + y \tan x)^2 \, dx,

where $y$ is a given function of $x$ satisfying $y = 0$ at $x = 1$. Show that $I - I_1 = 0$ and deduce that $I \geqslant 0$. Show further that $I = 0$ only if $y = 0$ for all $x$ ($0 \leqslant x \leqslant 1$).
**(ii)** Let

J=01((y)2a2y2)dx,J = \int_0^1 ((y')^2 - a^2y^2) \, dx,

where $a$ is a given positive constant and $y$ is a given function of $x$, not identically zero, satisfying $y = 0$ at $x = 1$. By considering an integral of the form

01(y+aytanbx)2dx,\int_0^1 (y' + ay \tan bx)^2 \, dx,

where $b$ is suitably chosen, show that $J \geqslant 0$. You should state the range of values of $a$, in the form $a < k$, for which your proof is valid.
In the case $a = k$, find a function $y$ (not everywhere zero) such that $J = 0$.
Hint

Expanding the bracket in the integral I1I_1, and employing sec2x=1+tan2x\sec^2 x = 1 + \tan^2 x yields II plus the integral of a perfect differential which can be evaluated simply. For I=0I = 0, y+ytanx=0y' + y \tan x = 0 over the interval which can be solved using an integrating factor and then the condition y=0,x=1y = 0, x = 1 enables the arbitrary constant to be evaluated giving the required result. In part (ii), similar working can be undertaken with the integral which is to be considered, given b=ab = a. The argument requires no discontinuity in the interval so a<π2a < \frac{\pi}{2}. The function y=cosaxy = \cos ax can be shown to meet the requirement.

Model Solution

Part (i)

We expand I1I_1:

I1=01(y+ytanx)2dx=01[(y)2+2yytanx+y2tan2x]dx.I_1 = \int_0^1 (y' + y\tan x)^2 \, dx = \int_0^1 \left[(y')^2 + 2yy'\tan x + y^2 \tan^2 x\right] dx.

We evaluate the middle integral 012yytanxdx\int_0^1 2yy'\tan x \, dx by parts. Let u=tanxu = \tan x and dv=2yydx=d(y2)dv = 2yy' \, dx = d(y^2), so du=sec2xdxdu = \sec^2 x \, dx and v=y2v = y^2. Then

012yytanxdx=[y2tanx]0101y2sec2xdx.\int_0^1 2yy'\tan x \, dx = \left[y^2 \tan x\right]_0^1 - \int_0^1 y^2 \sec^2 x \, dx.

At x=1x = 1: y2tan1y^2 \tan 1. At x=0x = 0: y2tan0=0y^2 \tan 0 = 0. But y=0y = 0 at x=1x = 1, so y2tan1=0y^2 \tan 1 = 0. Therefore

012yytanxdx=01y2sec2xdx.\int_0^1 2yy'\tan x \, dx = -\int_0^1 y^2 \sec^2 x \, dx.

Substituting back:

I1=01(y)2dx01y2sec2xdx+01y2tan2xdxI_1 = \int_0^1 (y')^2 \, dx - \int_0^1 y^2 \sec^2 x \, dx + \int_0^1 y^2 \tan^2 x \, dx

=01(y)2dx+01y2(tan2xsec2x)dx.= \int_0^1 (y')^2 \, dx + \int_0^1 y^2 (\tan^2 x - \sec^2 x) \, dx.

Using sec2x=1+tan2x\sec^2 x = 1 + \tan^2 x, we get tan2xsec2x=1\tan^2 x - \sec^2 x = -1. Therefore

I1=01(y)2dx01y2dx=I.I_1 = \int_0^1 (y')^2 \, dx - \int_0^1 y^2 \, dx = I.

Hence II1=0I - I_1 = 0.

Since I=I1I = I_1 and I1=01(y+ytanx)2dxI_1 = \int_0^1 (y' + y\tan x)^2 \, dx, and the integrand is a perfect square, we have I10I_1 \geqslant 0, so I0I \geqslant 0.

If I=0I = 0, then I1=0I_1 = 0, which requires (y+ytanx)2=0(y' + y\tan x)^2 = 0 for all x[0,1]x \in [0, 1], i.e.

y+ytanx=0.y' + y\tan x = 0.

This is a separable ODE. Dividing by yy (assuming y0y \neq 0):

yy=tanx    lny=lncosx+C    y=Acosx\frac{y'}{y} = -\tan x \quad \implies \quad \ln|y| = \ln|\cos x| + C \quad \implies \quad y = A\cos x

for some constant AA. The boundary condition y(1)=0y(1) = 0 requires Acos1=0A\cos 1 = 0. Since cos10\cos 1 \neq 0 (as 11 radian <π2< \frac{\pi}{2}), we need A=0A = 0, so y=0y = 0 for all x[0,1]x \in [0, 1].

Part (ii)

We consider

I2=01(y+aytanbx)2dxI_2 = \int_0^1 (y' + ay\tan bx)^2 \, dx

where bb is to be chosen. Expanding:

I2=01(y)2dx+2a01yytanbxdx+a201y2tan2bxdx.I_2 = \int_0^1 (y')^2 \, dx + 2a\int_0^1 yy'\tan bx \, dx + a^2\int_0^1 y^2 \tan^2 bx \, dx.

We evaluate the middle term by parts with u=tanbxu = \tan bx and dv=2yydx=d(y2)dv = 2yy' \, dx = d(y^2):

2a01yytanbxdx=a[y2tanbx]01ab01y2sec2bxdx.2a\int_0^1 yy'\tan bx \, dx = a\left[y^2 \tan bx\right]_0^1 - ab\int_0^1 y^2 \sec^2 bx \, dx.

At x=0x = 0: y2tan0=0y^2 \tan 0 = 0. At x=1x = 1: y=0y = 0, so y2tanb=0y^2 \tan b = 0 provided tanb\tan b is finite, i.e.\ bπ2+nπb \neq \frac{\pi}{2} + n\pi. Therefore

2a01yytanbxdx=ab01y2sec2bxdx.2a\int_0^1 yy'\tan bx \, dx = -ab\int_0^1 y^2 \sec^2 bx \, dx.

Substituting:

I2=01(y)2dx+01y2(a2tan2bxabsec2bx)dx.I_2 = \int_0^1 (y')^2 \, dx + \int_0^1 y^2 (a^2\tan^2 bx - ab\sec^2 bx) \, dx.

Using sec2bx=1+tan2bx\sec^2 bx = 1 + \tan^2 bx:

a2tan2bxabsec2bx=a2tan2bxab(1+tan2bx)=(a2ab)tan2bxab.a^2\tan^2 bx - ab\sec^2 bx = a^2\tan^2 bx - ab(1 + \tan^2 bx) = (a^2 - ab)\tan^2 bx - ab.

We want I2=J+(non-negative terms)I_2 = J + (\text{non-negative terms}), where J=01((y)2a2y2)dxJ = \int_0^1 ((y')^2 - a^2 y^2) \, dx. Comparing:

I2=01(y)2dx+01y2[(a2ab)tan2bxab]dx.I_2 = \int_0^1 (y')^2 \, dx + \int_0^1 y^2\left[(a^2 - ab)\tan^2 bx - ab\right] dx.

For this to equal J+01(something)2dxJ + \int_0^1 (\text{something})^2 \, dx, we need ab=a2-ab = -a^2, giving b=ab = a.

With b=ab = a: a2ab=0a^2 - ab = 0, so

I2=01(y)2dxa201y2dx=J.I_2 = \int_0^1 (y')^2 \, dx - a^2\int_0^1 y^2 \, dx = J.

Therefore J=I2=01(y+aytanax)2dx0J = I_2 = \int_0^1 (y' + ay\tan ax)^2 \, dx \geqslant 0.

Validity: This proof requires tanax\tan ax to be continuous on [0,1][0, 1], so axπ2ax \neq \frac{\pi}{2} for any x[0,1]x \in [0, 1], i.e.\ a<π2a < \frac{\pi}{2}. So the proof is valid for a<π2a < \frac{\pi}{2}, giving k=π2k = \frac{\pi}{2}.

The case a=k=π2a = k = \frac{\pi}{2}. We need a function yy, not everywhere zero, with y(1)=0y(1) = 0 and J=0J = 0. Since J=01((y)2π24y2)dxJ = \int_0^1 ((y')^2 - \frac{\pi^2}{4} y^2) \, dx, consider y=cosπx2y = \cos\frac{\pi x}{2}. Then y(1)=cosπ2=0y(1) = \cos\frac{\pi}{2} = 0 and

y=π2sinπx2,(y)2=π24sin2πx2,π24y2=π24cos2πx2.y' = -\frac{\pi}{2}\sin\frac{\pi x}{2}, \qquad (y')^2 = \frac{\pi^2}{4}\sin^2\frac{\pi x}{2}, \qquad \frac{\pi^2}{4}y^2 = \frac{\pi^2}{4}\cos^2\frac{\pi x}{2}.

Therefore

J=π2401(sin2πx2cos2πx2)dx=π2401cos(πx)dx=π24[sinπxπ]01=0.J = \frac{\pi^2}{4}\int_0^1 \left(\sin^2\frac{\pi x}{2} - \cos^2\frac{\pi x}{2}\right) dx = -\frac{\pi^2}{4}\int_0^1 \cos(\pi x) \, dx = -\frac{\pi^2}{4}\left[\frac{\sin \pi x}{\pi}\right]_0^1 = 0.

So y=cosπx2y = \cos\frac{\pi x}{2} gives J=0J = 0.

Examiner Notes

Two thirds of the candidature attempted this but with only moderate success earning just a third of the marks. The very first result was frequently obtained although some fell at the first hurdle through not appreciating that they needed to use sec2x=1+tan2x\sec^2 x = 1 + \tan^2 x, or else that there was then an exact differential. The second result in part (i) was “only if” whereas many read it, or answered it, as “if”. In part (ii), most spotted b=ab = a. There were many inappropriate functions suggested for the last part of the question, many which ignored the requirement that y=0,x=1y = 0, x = 1.


Topic: 复数与几何 (Complex Numbers and Geometry)  |  Difficulty: Challenging  |  Marks: 20

5 A quadrilateral drawn in the complex plane has vertices A,B,CA, B, C and DD, labelled anticlockwise. These vertices are represented, respectively, by the complex numbers a,b,ca, b, c and dd. Show that ABCDABCD is a parallelogram (defined as a quadrilateral in which opposite sides are parallel and equal in length) if and only if a+c=b+da + c = b + d. Show further that, in this case, ABCDABCD is a square if and only if i(ac)=bdi(a - c) = b - d.

Let PQRSPQRS be a quadrilateral in the complex plane, with vertices labelled anticlockwise, the internal angles of which are all less than 180180^\circ. Squares with centres X,Y,ZX, Y, Z and TT are constructed externally to the quadrilateral on the sides PQ,QR,RSPQ, QR, RS and SPSP, respectively.

(i) If PP and QQ are represented by the complex numbers pp and qq, respectively, show that XX can be represented by 12(p(1+i)+q(1i)).\frac{1}{2}(p(1 + i) + q(1 - i)) .

(ii) Show that XYZTXYZT is a square if and only if PQRSPQRS is a parallelogram.

Hint

ABCD is a parallelogram if and only if AB=DC\vec{AB} = \vec{DC} which yields the required result. To be a square as well, angle ABC=90ABC = 90^\circ, and AB=BC|AB| = |BC|, so cb=i(ba)c - b = i(b - a). Treating the two results as simultaneous equations to be solved for aa and cc in terms of bb and dd, the second result of the stem can be shown with reversible logic. For part (i) the same logic can be used for PXQPXQ as just used for ABCABC. From the stem, XYZT is a square if and only if i(xz)=yti(x - z) = y - t, and x+z=y+tx + z = y + t and given the working for X in part (i), these can be shown to be true treating Y, Z, and T similarly.

Model Solution

Stem: Parallelogram condition

ABCDABCD is a parallelogram if and only if AB=DC\vec{AB} = \vec{DC}, i.e.

ba=cd.b - a = c - d.

Rearranging: a+c=b+da + c = b + d. (shown)\qquad \text{(shown)}


Stem: Square condition (given parallelogram)

Suppose ABCDABCD is a parallelogram, so a+c=b+da + c = b + d. Then ABCDABCD is a square if and only if adjacent sides are perpendicular and equal in length, i.e. BC=iAB\vec{BC} = i\,\vec{AB} (rotation by 90°90°):

cb=i(ba).()c - b = i(b - a). \qquad (\star)

We show that ()(\star) together with a+c=b+da + c = b + d is equivalent to i(ac)=bdi(a - c) = b - d.

(\Rightarrow) From a+c=b+da + c = b + d: d=a+cbd = a + c - b, so

bd=2bac.b - d = 2b - a - c.

From ()(\star): c=b+i(ba)=b(1+i)iac = b + i(b - a) = b(1 + i) - ia, giving

ac=a(1+i)b(1+i)=(1+i)(ab).a - c = a(1 + i) - b(1 + i) = (1 + i)(a - b).

Therefore i(ac)=i(1+i)(ab)=(i1)(ab)i(a - c) = i(1 + i)(a - b) = (i - 1)(a - b). Meanwhile

bd=2ba[b(1+i)ia]=b(1i)a(1i)=(1i)(ab)=(i1)(ab).b - d = 2b - a - [b(1+i) - ia] = b(1 - i) - a(1 - i) = -(1 - i)(a - b) = (i - 1)(a - b).

So i(ac)=bdi(a - c) = b - d.

(\Leftarrow) Suppose a+c=b+da + c = b + d and i(ac)=bdi(a - c) = b - d. Let m=a+c2=b+d2m = \frac{a+c}{2} = \frac{b+d}{2} and set u=amu = a - m, v=bmv = b - m. Then c=muc = m - u, d=mvd = m - v, and ac=2ua - c = 2u, bd=2vb - d = 2v. The condition i(ac)=bdi(a-c) = b-d gives v=iuv = iu. Now

AB=ba=vu=u(i1),BC=cb=u(1+i).\vec{AB} = b - a = v - u = u(i - 1), \qquad \vec{BC} = c - b = -u(1 + i).

BCAB=u(1+i)u(i1)=(1+i)i1.\frac{\vec{BC}}{\vec{AB}} = \frac{-u(1+i)}{u(i-1)} = \frac{-(1+i)}{i-1}.

Multiplying numerator and denominator by (i1)=(1+i)\overline{(i-1)} = -(1+i):

(1+i)i1(1+i)(1+i)=(1+i)2i12=2i2=i.\frac{-(1+i)}{i-1} \cdot \frac{-(1+i)}{-(1+i)} = \frac{(1+i)^2}{|i-1|^2} = \frac{2i}{2} = i.

Since BC=iAB\vec{BC} = i\,\vec{AB}, the sides ABAB and BCBC are perpendicular and equal in length. Combined with the parallelogram condition, ABCDABCD is a square. \qquad \square


Part (i)

The square on side PQPQ is constructed externally. Its four vertices, in order, are

P,Q,Q+R,P+R,P, \quad Q, \quad Q + R, \quad P + R,

where R=i(qp)R = -i(q - p) is the vector PQ\vec{PQ} rotated 90°90° clockwise (toward the exterior of the anticlockwise quadrilateral).

The centre XX is the average of the four vertices:

X=14[p+q+(q+R)+(p+R)]=2p+2q+2R4=p+q+R2.X = \frac{1}{4}\bigl[p + q + (q + R) + (p + R)\bigr] = \frac{2p + 2q + 2R}{4} = \frac{p + q + R}{2}.

Substituting R=i(qp)R = -i(q - p):

X=p+qi(qp)2=p(1+i)+q(1i)2.(shown)X = \frac{p + q - i(q - p)}{2} = \frac{p(1 + i) + q(1 - i)}{2}. \qquad \text{(shown)} \quad \square


Part (ii)

By the same construction, the centres of the external squares on the four sides are:

x=12(p(1+i)+q(1i)),y=12(q(1+i)+r(1i)),x = \tfrac{1}{2}\bigl(p(1+i) + q(1-i)\bigr), \quad y = \tfrac{1}{2}\bigl(q(1+i) + r(1-i)\bigr),

z=12(r(1+i)+s(1i)),t=12(s(1+i)+p(1i)).z = \tfrac{1}{2}\bigl(r(1+i) + s(1-i)\bigr), \quad t = \tfrac{1}{2}\bigl(s(1+i) + p(1-i)\bigr).

From the stem results, XYZTXYZT is a square if and only if both:

  • (a) x+z=y+tx + z = y + t (parallelogram condition), and
  • (b) i(xz)=yti(x - z) = y - t (right angle + equal sides condition).

Condition (b) — perpendicularity:

xz=12[p(1+i)+q(1i)r(1+i)s(1i)].x - z = \tfrac{1}{2}\bigl[p(1+i) + q(1-i) - r(1+i) - s(1-i)\bigr].

Multiplying by ii and using (1+i)i=i1(1+i)i = i - 1, (1i)i=1+i(1-i)i = 1 + i:

i(xz)=12[p(i1)+q(1+i)r(i1)s(1+i)].i(x - z) = \tfrac{1}{2}\bigl[p(i-1) + q(1+i) - r(i-1) - s(1+i)\bigr].

Since r(i1)=r(1i)-r(i-1) = r(1-i):

i(xz)=12[p(i1)+q(1+i)+r(1i)s(1+i)].i(x - z) = \tfrac{1}{2}\bigl[p(i-1) + q(1+i) + r(1-i) - s(1+i)\bigr].

Now compute directly:

yt=12[q(1+i)+r(1i)s(1+i)p(1i)].y - t = \tfrac{1}{2}\bigl[q(1+i) + r(1-i) - s(1+i) - p(1-i)\bigr].

Since p(1i)=p(i1)-p(1-i) = p(i - 1), the two expressions are identical. Therefore i(xz)=yti(x - z) = y - t holds identically for all p,q,r,sp, q, r, s.

Condition (a) — parallelogram condition:

x+z=12[(p+r)(1+i)+(q+s)(1i)],x + z = \tfrac{1}{2}\bigl[(p+r)(1+i) + (q+s)(1-i)\bigr],

y+t=12[(q+s)(1+i)+(p+r)(1i)].y + t = \tfrac{1}{2}\bigl[(q+s)(1+i) + (p+r)(1-i)\bigr].

Setting u=p+ru = p + r, v=q+sv = q + s:

u(1+i)+v(1i)=v(1+i)+u(1i)u(1+i) + v(1-i) = v(1+i) + u(1-i)

(uv)(1+i)(uv)(1i)=0(u - v)(1+i) - (u - v)(1-i) = 0

(uv)[(1+i)(1i)]=0(u - v)\bigl[(1+i) - (1-i)\bigr] = 0

2i(uv)=0    u=v.2i(u - v) = 0 \implies u = v.

So x+z=y+tx + z = y + t if and only if p+r=q+sp + r = q + s, which is the condition for PQRSPQRS to be a parallelogram.

Conclusion: Condition (b) is always satisfied. Therefore XYZTXYZT is a square if and only if condition (a) holds, i.e. if and only if PQRSPQRS is a parallelogram. \qquad \square

Examiner Notes

This was a moderately popular question attempted by half the candidates, with some success, scoring a little below half marks. There were some basic problems exposed in this question such as the differences between a vector and its length, the negative of a vector and the vector, and the meaning of “if and only if” resulting in things being shown in one direction only throughout the question. Part (i) was generally well done, but in part (ii), it was commonly forgotten that there were two conditions for XYZT to be a square. Approaches using real and imaginary parts (breaking into components) were not very successful.


Topic: 分析 (Analysis)  |  Difficulty: Hard  |  Marks: 20

6 Starting from the result that h(t)>0 for 0<t<x    0xh(t)dt>0,h(t) > 0 \text{ for } 0 < t < x \implies \int_{0}^{x} h(t) \, dt > 0 , show that, if f(t)>0f''(t) > 0 for 0<t<x00 < t < x_0 and f(0)=f(0)=0f(0) = f'(0) = 0, then f(t)>0f(t) > 0 for 0<t<x00 < t < x_0.

(i) Show that, for 0<x<12π0 < x < \frac{1}{2}\pi, cosxcoshx<1.\cos x \cosh x < 1 .

(ii) Show that, for 0<x<12π0 < x < \frac{1}{2}\pi, 1coshx<sinxx<xsinhx.\frac{1}{\cosh x} < \frac{\sin x}{x} < \frac{x}{\sinh x} .

Hint

Starting from f(t)>0f''(t) > 0 for 0<t<x00 < t < x_0, integrate from 00 to t0t_0 (where 0<t0<x00 < t_0 < x_0): 0t0f(t)dt>0    f(t0)f(0)>0    f(t0)>0\int_0^{t_0} f''(t) \, dt > 0 \implies f'(t_0) - f'(0) > 0 \implies f'(t_0) > 0 since f(0)=0f'(0) = 0. Repeat the argument with f(t)f'(t): integrate from 00 to t0t_0: 0t0f(t)dt>0    f(t0)f(0)>0    f(t0)>0\int_0^{t_0} f'(t) \, dt > 0 \implies f(t_0) - f(0) > 0 \implies f(t_0) > 0 since f(0)=0f(0) = 0.

(i) Choose f(x)=1cosxcoshxf(x) = 1 - \cos x \cosh x. Then f(0)=0f(0) = 0 and f(x)=sinxcoshxcosxsinhxf'(x) = \sin x \cosh x - \cos x \sinh x, so f(0)=0f'(0) = 0. Now f(x)=2sinxsinhx>0for 0<x<π.f''(x) = 2\sin x \sinh x > 0 \quad \text{for } 0 < x < \pi. By the stem result, f(x)>0f(x) > 0 for 0<x<π0 < x < \pi, so 1cosxcoshx>01 - \cos x \cosh x > 0, i.e. cosxcoshx<1\cos x \cosh x < 1 for 0<x<π0 < x < \pi, and in particular for 0<x<12π0 < x < \frac{1}{2}\pi.

(ii) Choose g(x)=x2sinxsinhxg(x) = x^2 - \sin x \sinh x. Then g(0)=0g(0) = 0 and g(x)=2xcosxsinhxsinxcoshxg'(x) = 2x - \cos x \sinh x - \sin x \cosh x, so g(0)=0g'(0) = 0. Now g(x)=22cosxcoshx=2f(x)>0for 0<x<π.g''(x) = 2 - 2\cos x \cosh x = 2f(x) > 0 \quad \text{for } 0 < x < \pi. By the stem result, g(x)>0g(x) > 0 for 0<x<π0 < x < \pi, so x2>sinxsinhxx^2 > \sin x \sinh x, giving xsinhx>sinxx\frac{x}{\sinh x} > \frac{\sin x}{x} for 0<x<12π0 < x < \frac{1}{2}\pi.

Choose h(x)=sinxcoshxxh(x) = \sin x \cosh x - x. Then h(0)=0h(0) = 0 and h(x)=cosxcoshx+sinxsinhx1h'(x) = \cos x \cosh x + \sin x \sinh x - 1, so h(0)=0h'(0) = 0. Now h(x)=2sinxcoshx>0for 0<x<π.h''(x) = 2\sin x \cosh x > 0 \quad \text{for } 0 < x < \pi. By the stem result, h(x)>0h(x) > 0 for 0<x<π0 < x < \pi, so sinxcoshx>x\sin x \cosh x > x, giving sinxx>1coshx\frac{\sin x}{x} > \frac{1}{\cosh x} for 0<x<12π0 < x < \frac{1}{2}\pi. Combining: 1coshx<sinxx<xsinhx\frac{1}{\cosh x} < \frac{\sin x}{x} < \frac{x}{\sinh x}.

Model Solution

Stem result

Suppose f(t)>0f''(t) > 0 for 0<t<x00 < t < x_0 and f(0)=f(0)=0f(0) = f'(0) = 0. We apply the given result twice.

First application. Take h(t)=f(t)h(t) = f''(t). Since f(t)>0f''(t) > 0 for 0<t<x00 < t < x_0, for any t0t_0 with 0<t0<x00 < t_0 < x_0:

0t0f(t)dt>0    f(t0)f(0)>0    f(t0)>0,\int_0^{t_0} f''(t) \, dt > 0 \implies f'(t_0) - f'(0) > 0 \implies f'(t_0) > 0,

using f(0)=0f'(0) = 0.

Second application. Take h(t)=f(t)h(t) = f'(t). Since f(t)>0f'(t) > 0 for 0<t<x00 < t < x_0 (just shown), for any t0t_0 with 0<t0<x00 < t_0 < x_0:

0t0f(t)dt>0    f(t0)f(0)>0    f(t0)>0,\int_0^{t_0} f'(t) \, dt > 0 \implies f(t_0) - f(0) > 0 \implies f(t_0) > 0,

using f(0)=0f(0) = 0. Therefore f(t)>0f(t) > 0 for 0<t<x00 < t < x_0. \qquad \square


Part (i)

Define f(x)=1cosxcoshxf(x) = 1 - \cos x \cosh x. We verify the hypotheses of the stem result.

Check boundary conditions:

f(0)=1cos0cosh0=11=0.f(0) = 1 - \cos 0 \cdot \cosh 0 = 1 - 1 = 0.

f(x)=sinxcoshxcosxsinhx    f(0)=00=0.f'(x) = \sin x \cosh x - \cos x \sinh x \implies f'(0) = 0 - 0 = 0.

Compute ff'':

f(x)=ddx[sinxcoshxcosxsinhx]f''(x) = \frac{d}{dx}[\sin x \cosh x - \cos x \sinh x]

=(cosxcoshx+sinxsinhx)(sinxsinhx+cosxcoshx)= (\cos x \cosh x + \sin x \sinh x) - (-\sin x \sinh x + \cos x \cosh x)

=2sinxsinhx.= 2\sin x \sinh x.

For 0<x<π0 < x < \pi: sinx>0\sin x > 0 and sinhx>0\sinh x > 0, so f(x)=2sinxsinhx>0f''(x) = 2\sin x \sinh x > 0.

Apply the stem result with x0=πx_0 = \pi: f(x)>0f(x) > 0 for 0<x<π0 < x < \pi, i.e.

1cosxcoshx>0    cosxcoshx<1.1 - \cos x \cosh x > 0 \implies \cos x \cosh x < 1.

In particular, this holds for 0<x<12π0 < x < \frac{1}{2}\pi. \qquad \square


Part (ii)

We prove two inequalities separately.

Right inequality: sinxx<xsinhx\dfrac{\sin x}{x} < \dfrac{x}{\sinh x} for 0<x<12π0 < x < \frac{1}{2}\pi.

This is equivalent to sinxsinhx<x2\sin x \cdot \sinh x < x^2 (valid since sinx>0\sin x > 0, sinhx>0\sinh x > 0, x>0x > 0 in this range).

Define g(x)=x2sinxsinhxg(x) = x^2 - \sin x \sinh x. Check boundary conditions:

g(0)=00=0.g(0) = 0 - 0 = 0.

g(x)=2xcosxsinhxsinxcoshx    g(0)=000=0.g'(x) = 2x - \cos x \sinh x - \sin x \cosh x \implies g'(0) = 0 - 0 - 0 = 0.

Compute gg'':

g(x)=2(sinxsinhx+cosxcoshx)(cosxcoshx+sinxsinhx)g''(x) = 2 - (-\sin x \sinh x + \cos x \cosh x) - (\cos x \cosh x + \sin x \sinh x)

=22cosxcoshx.= 2 - 2\cos x \cosh x.

By part (i), cosxcoshx<1\cos x \cosh x < 1 for 0<x<π0 < x < \pi, so g(x)=2(1cosxcoshx)>0g''(x) = 2(1 - \cos x \cosh x) > 0 for 0<x<π0 < x < \pi.

Apply the stem result with x0=πx_0 = \pi: g(x)>0g(x) > 0 for 0<x<π0 < x < \pi, i.e. x2>sinxsinhxx^2 > \sin x \sinh x.

Dividing by xsinhx>0x \sinh x > 0:

xsinhx>sinxx.()\frac{x}{\sinh x} > \frac{\sin x}{x}. \qquad (\dagger)


Left inequality: 1coshx<sinxx\dfrac{1}{\cosh x} < \dfrac{\sin x}{x} for 0<x<12π0 < x < \frac{1}{2}\pi.

This is equivalent to x<sinxcoshxx < \sin x \cosh x (valid since coshx>0\cosh x > 0, x>0x > 0 in this range).

Define h(x)=sinxcoshxxh(x) = \sin x \cosh x - x. Check boundary conditions:

h(0)=00=0.h(0) = 0 - 0 = 0.

h(x)=cosxcoshx+sinxsinhx1    h(0)=1+01=0.h'(x) = \cos x \cosh x + \sin x \sinh x - 1 \implies h'(0) = 1 + 0 - 1 = 0.

Compute hh'':

h(x)=(sinxcoshx+cosxsinhx)+(cosxsinhx+sinxcoshx)h''(x) = (-\sin x \cosh x + \cos x \sinh x) + (\cos x \sinh x + \sin x \cosh x)

=2cosxsinhx.= 2\cos x \sinh x.

For 0<x<12π0 < x < \frac{1}{2}\pi: cosx>0\cos x > 0 and sinhx>0\sinh x > 0, so h(x)>0h''(x) > 0.

Apply the stem result with x0=12πx_0 = \frac{1}{2}\pi: h(x)>0h(x) > 0 for 0<x<12π0 < x < \frac{1}{2}\pi, i.e. sinxcoshx>x\sin x \cosh x > x.

Dividing by xcoshx>0x \cosh x > 0:

sinxx>1coshx.()\frac{\sin x}{x} > \frac{1}{\cosh x}. \qquad (\ddagger)


Combining ()(\dagger) and ()(\ddagger):

1coshx<sinxx<xsinhxfor 0<x<12π.\frac{1}{\cosh x} < \frac{\sin x}{x} < \frac{x}{\sinh x} \quad \text{for } 0 < x < \tfrac{1}{2}\pi. \qquad \square

Examiner Notes

Many did not use the required starting point, instead resorting to monotonicity or drawing pictures (graphs) which were not proofs. In parts (i) especially and (ii) as well, candidates failed to use the result that f(t)>0f(t) > 0, cavalierly using f(t)<0f(t) < 0, or even f(t)<1f(t) < 1 without justification. Many made complicated choices of functions for (i) and (ii), and then got lost in their differentiations, and finally there was frequent lack of care to ensure that quantities dividing inequalities were positive.


Topic: 几何 (Geometry)  |  Difficulty: Hard  |  Marks: 20

7 The four distinct points PiP_i (i=1,2,3,4i = 1, 2, 3, 4) are the vertices, labelled anticlockwise, of a cyclic quadrilateral. The lines P1P3P_1P_3 and P2P4P_2P_4 intersect at QQ.

(i) By considering the triangles P1QP4P_1QP_4 and P2QP3P_2QP_3 show that (P1Q)(QP3)=(P2Q)(QP4)(P_1Q)(QP_3) = (P_2Q)(QP_4).

(ii) Let pi\mathbf{p}_i be the position vector of the point PiP_i (i=1,2,3,4i = 1, 2, 3, 4). Show that there exist numbers aia_i, not all zero, such that

i=14ai=0andi=14aipi=0.(*)\sum_{i=1}^{4} a_i = 0 \quad \text{and} \quad \sum_{i=1}^{4} a_i\mathbf{p}_i = \mathbf{0} . \qquad \text{(*)}

(iii) Let aia_i (i=1,2,3,4i = 1, 2, 3, 4) be any numbers, not all zero, that satisfy (*). Show that a1+a30a_1 + a_3 \neq 0 and that the lines P1P3P_1P_3 and P2P4P_2P_4 intersect at the point with position vector

a1p1+a3p3a1+a3.\frac{a_1\mathbf{p}_1 + a_3\mathbf{p}_3}{a_1 + a_3} .

Deduce that a1a3(P1P3)2=a2a4(P2P4)2a_1a_3(P_1P_3)^2 = a_2a_4(P_2P_4)^2.

Hint

(i) Since P1P2P3P4P_1P_2P_3P_4 is cyclic, P1P4Q=P1P2Q\angle P_1P_4Q = \angle P_1P_2Q (angles in the same segment) and P4P1Q=P3P2Q\angle P_4P_1Q = \angle P_3P_2Q (angles in the same segment). Thus P1QP4P2QP3\triangle P_1QP_4 \sim \triangle P_2QP_3 (AA similarity). Therefore P1QP2Q=QP4QP3\frac{P_1Q}{P_2Q} = \frac{QP_4}{QP_3}, giving (P1Q)(QP3)=(P2Q)(QP4)(P_1Q)(QP_3) = (P_2Q)(QP_4).

(ii) Since QQ lies on P1P3P_1P_3, we can write q=p1+λ(p3p1)=(1λ)p1+λp3\mathbf{q} = \mathbf{p}_1 + \lambda(\mathbf{p}_3 - \mathbf{p}_1) = (1-\lambda)\mathbf{p}_1 + \lambda\mathbf{p}_3 for some λ\lambda. Since QQ also lies on P2P4P_2P_4, we can write q=(1μ)p2+μp4\mathbf{q} = (1-\mu)\mathbf{p}_2 + \mu\mathbf{p}_4 for some μ\mu. Equating: (1λ)p1+λp3=(1μ)p2+μp4(1-\lambda)\mathbf{p}_1 + \lambda\mathbf{p}_3 = (1-\mu)\mathbf{p}_2 + \mu\mathbf{p}_4. Setting a1=1λa_1 = 1-\lambda, a3=λa_3 = \lambda, a2=(1μ)a_2 = -(1-\mu), a4=μa_4 = -\mu: then a1+a2+a3+a4=(1λ)(1μ)+λμ=0a_1 + a_2 + a_3 + a_4 = (1-\lambda) - (1-\mu) + \lambda - \mu = 0 and a1p1+a2p2+a3p3+a4p4=0a_1\mathbf{p}_1 + a_2\mathbf{p}_2 + a_3\mathbf{p}_3 + a_4\mathbf{p}_4 = \mathbf{0}.

(iii) Suppose a1+a3=0a_1 + a_3 = 0. Then a1=a3a_1 = -a_3 and from (*): a1(p1p3)=(a2p2+a4p4)a_1(\mathbf{p}_1 - \mathbf{p}_3) = -(a_2\mathbf{p}_2 + a_4\mathbf{p}_4). Also a2+a4=0a_2 + a_4 = 0 so a4=a2a_4 = -a_2, giving a1(p1p3)=a2(p2p4)=a2(p4p2)a_1(\mathbf{p}_1 - \mathbf{p}_3) = -a_2(\mathbf{p}_2 - \mathbf{p}_4) = a_2(\mathbf{p}_4 - \mathbf{p}_2). Since P1P3P_1P_3 and P2P4P_2P_4 intersect at QQ, the vectors p3p1\mathbf{p}_3 - \mathbf{p}_1 and p4p2\mathbf{p}_4 - \mathbf{p}_2 are not parallel, so a1=a2=0a_1 = a_2 = 0, contradicting not all aia_i being zero. Thus a1+a30a_1 + a_3 \neq 0.

From (*): a1p1+a3p3=(a2p2+a4p4)a_1\mathbf{p}_1 + a_3\mathbf{p}_3 = -(a_2\mathbf{p}_2 + a_4\mathbf{p}_4) and a1+a3=(a2+a4)a_1 + a_3 = -(a_2 + a_4). The point a1p1+a3p3a1+a3=p1+a3(p3p1)a1+a3\frac{a_1\mathbf{p}_1 + a_3\mathbf{p}_3}{a_1 + a_3} = \mathbf{p}_1 + \frac{a_3(\mathbf{p}_3 - \mathbf{p}_1)}{a_1 + a_3} lies on P1P3P_1P_3. Similarly a2p2+a4p4a2+a4=p2+a4(p4p2)a2+a4\frac{a_2\mathbf{p}_2 + a_4\mathbf{p}_4}{a_2 + a_4} = \mathbf{p}_2 + \frac{a_4(\mathbf{p}_4 - \mathbf{p}_2)}{a_2 + a_4} lies on P2P4P_2P_4. These are equal, so they represent QQ.

For the final deduction: let QQ divide P1P3P_1P_3 in ratio λ:(1λ)\lambda:(1-\lambda) and P2P4P_2P_4 in ratio μ:(1μ)\mu:(1-\mu). From (i), (P1Q)(QP3)=(P2Q)(QP4)(P_1Q)(QP_3) = (P_2Q)(QP_4), so λ(1λ)(P1P3)2=μ(1μ)(P2P4)2\lambda(1-\lambda)(P_1P_3)^2 = \mu(1-\mu)(P_2P_4)^2. From the representation, a3a1+a3=λ\frac{a_3}{a_1+a_3} = \lambda and a1a1+a3=1λ\frac{a_1}{a_1+a_3} = 1-\lambda, so a1a3=(a1+a3)2λ(1λ)a_1a_3 = (a_1+a_3)^2 \lambda(1-\lambda). Similarly a2a4=(a2+a4)2μ(1μ)a_2a_4 = (a_2+a_4)^2 \mu(1-\mu). Since a1+a3=(a2+a4)a_1+a_3 = -(a_2+a_4), we get (a1+a3)2=(a2+a4)2(a_1+a_3)^2 = (a_2+a_4)^2, so a1a3(P1P3)2=a2a4(P2P4)2a_1a_3(P_1P_3)^2 = a_2a_4(P_2P_4)^2.

Model Solution

Part (i)

Since P1P2P3P4P_1P_2P_3P_4 is a cyclic quadrilateral, we apply the inscribed angle theorem (angles in the same segment):

  • P1P4Q=P1P2Q\angle P_1P_4Q = \angle P_1P_2Q: both subtend arc P1P4P_1P_4 on the same side.
  • P4P1Q=P3P2Q\angle P_4P_1Q = \angle P_3P_2Q: both subtend arc P3P4P_3P_4 on the same side.

(Note that QQ lies on segment P1P3P_1P_3 between P1P_1 and P3P_3, and on segment P2P4P_2P_4 between P2P_2 and P4P_4, so these equalities hold as stated.)

Therefore P1QP4P2QP3\triangle P_1QP_4 \sim \triangle P_2QP_3 by AA similarity (two pairs of equal angles).

From the similarity, corresponding sides are proportional:

P1QP2Q=QP4QP3\frac{P_1Q}{P_2Q} = \frac{QP_4}{QP_3}

Cross-multiplying:

(P1Q)(QP3)=(P2Q)(QP4)(P_1Q)(QP_3) = (P_2Q)(QP_4) \qquad \blacksquare

Part (ii)

Since QQ lies on line P1P3P_1P_3, we can write

q=(1λ)p1+λp3\mathbf{q} = (1-\lambda)\mathbf{p}_1 + \lambda\mathbf{p}_3

for some real number λ\lambda. Since QQ also lies on line P2P4P_2P_4, we can write

q=(1μ)p2+μp4\mathbf{q} = (1-\mu)\mathbf{p}_2 + \mu\mathbf{p}_4

for some real number μ\mu. Equating these two expressions:

(1λ)p1+λp3=(1μ)p2+μp4(1-\lambda)\mathbf{p}_1 + \lambda\mathbf{p}_3 = (1-\mu)\mathbf{p}_2 + \mu\mathbf{p}_4

Rearranging:

(1λ)p1(1μ)p2+λp3μp4=0(1-\lambda)\mathbf{p}_1 - (1-\mu)\mathbf{p}_2 + \lambda\mathbf{p}_3 - \mu\mathbf{p}_4 = \mathbf{0}

Set a1=1λa_1 = 1-\lambda, a2=(1μ)a_2 = -(1-\mu), a3=λa_3 = \lambda, a4=μa_4 = -\mu. Then:

a1+a2+a3+a4=(1λ)(1μ)+λμ=0a_1 + a_2 + a_3 + a_4 = (1-\lambda) - (1-\mu) + \lambda - \mu = 0

a1p1+a2p2+a3p3+a4p4=0a_1\mathbf{p}_1 + a_2\mathbf{p}_2 + a_3\mathbf{p}_3 + a_4\mathbf{p}_4 = \mathbf{0}

Since P1P3P_1 \neq P_3 (distinct vertices), at least one of a1,a3a_1, a_3 is non-zero, so the aia_i are not all zero. \qquad \blacksquare

Part (iii)

Showing a1+a30a_1 + a_3 \neq 0.

Suppose for contradiction that a1+a3=0a_1 + a_3 = 0, so a3=a1a_3 = -a_1.

From ai=0\sum a_i = 0: a2+a4=(a1+a3)=0a_2 + a_4 = -(a_1 + a_3) = 0, so a4=a2a_4 = -a_2.

From aipi=0\sum a_i\mathbf{p}_i = \mathbf{0}:

a1p1+a2p2a1p3a2p4=0a_1\mathbf{p}_1 + a_2\mathbf{p}_2 - a_1\mathbf{p}_3 - a_2\mathbf{p}_4 = \mathbf{0}

a1(p1p3)+a2(p2p4)=0a_1(\mathbf{p}_1 - \mathbf{p}_3) + a_2(\mathbf{p}_2 - \mathbf{p}_4) = \mathbf{0}

a1(p3p1)=a2(p4p2)a_1(\mathbf{p}_3 - \mathbf{p}_1) = a_2(\mathbf{p}_4 - \mathbf{p}_2)

Since P1P2P3P4P_1P_2P_3P_4 is a convex quadrilateral, the diagonals P1P3P_1P_3 and P2P4P_2P_4 intersect and are therefore not parallel. Hence p3p1\mathbf{p}_3 - \mathbf{p}_1 and p4p2\mathbf{p}_4 - \mathbf{p}_2 are not scalar multiples of each other. The equation above forces a1=0a_1 = 0 and a2=0a_2 = 0, giving a3=0a_3 = 0 and a4=0a_4 = 0, which contradicts the requirement that not all aia_i are zero. Therefore a1+a30a_1 + a_3 \neq 0. \qquad \blacksquare

Showing the intersection point.

Since a1+a30a_1 + a_3 \neq 0 and a2+a4=(a1+a3)0a_2 + a_4 = -(a_1 + a_3) \neq 0, we rearrange aipi=0\sum a_i\mathbf{p}_i = \mathbf{0}:

a1p1+a3p3=(a2p2+a4p4)anda1+a3=(a2+a4)a_1\mathbf{p}_1 + a_3\mathbf{p}_3 = -(a_2\mathbf{p}_2 + a_4\mathbf{p}_4) \qquad \text{and} \qquad a_1 + a_3 = -(a_2 + a_4)

Define q=a1p1+a3p3a1+a3\mathbf{q} = \dfrac{a_1\mathbf{p}_1 + a_3\mathbf{p}_3}{a_1 + a_3}. Rewriting:

q=p1+a3a1+a3(p3p1)\mathbf{q} = \mathbf{p}_1 + \frac{a_3}{a_1 + a_3}(\mathbf{p}_3 - \mathbf{p}_1)

This is a point on line P1P3P_1P_3 (with parameter λ=a3a1+a3\lambda = \frac{a_3}{a_1 + a_3}).

Similarly, using a1+a3=(a2+a4)a_1 + a_3 = -(a_2 + a_4):

q=(a2p2+a4p4)(a2+a4)=a2p2+a4p4a2+a4=p2+a4a2+a4(p4p2)\mathbf{q} = \frac{-(a_2\mathbf{p}_2 + a_4\mathbf{p}_4)}{-(a_2 + a_4)} = \frac{a_2\mathbf{p}_2 + a_4\mathbf{p}_4}{a_2 + a_4} = \mathbf{p}_2 + \frac{a_4}{a_2 + a_4}(\mathbf{p}_4 - \mathbf{p}_2)

This is a point on line P2P4P_2P_4 (with parameter μ=a4a2+a4\mu = \frac{a_4}{a_2 + a_4}).

Since q\mathbf{q} lies on both lines P1P3P_1P_3 and P2P4P_2P_4, and these lines intersect at the unique point QQ, we conclude q=OQ\mathbf{q} = \vec{OQ}. \qquad \blacksquare

Deducing a1a3(P1P3)2=a2a4(P2P4)2a_1a_3(P_1P_3)^2 = a_2a_4(P_2P_4)^2.

From the above, QQ divides P1P3P_1P_3 in ratio λ:(1λ)\lambda:(1-\lambda) where λ=a3a1+a3\lambda = \frac{a_3}{a_1+a_3}, and divides P2P4P_2P_4 in ratio μ:(1μ)\mu:(1-\mu) where μ=a4a2+a4\mu = \frac{a_4}{a_2+a_4}.

This gives:

P1Q=(1λ)P1P3,QP3=λP1P3P_1Q = (1-\lambda)\,|P_1P_3|, \quad QP_3 = \lambda\,|P_1P_3|

P2Q=(1μ)P2P4,QP4=μP2P4P_2Q = (1-\mu)\,|P_2P_4|, \quad QP_4 = \mu\,|P_2P_4|

Substituting into the result from part (i):

λ(1λ)(P1P3)2=μ(1μ)(P2P4)2()\lambda(1-\lambda)(P_1P_3)^2 = \mu(1-\mu)(P_2P_4)^2 \qquad (\dagger)

Now compute λ(1λ)\lambda(1-\lambda):

λ(1λ)=a3a1+a3a1a1+a3=a1a3(a1+a3)2\lambda(1-\lambda) = \frac{a_3}{a_1+a_3} \cdot \frac{a_1}{a_1+a_3} = \frac{a_1a_3}{(a_1+a_3)^2}

Similarly:

μ(1μ)=a4a2+a4a2a2+a4=a2a4(a2+a4)2\mu(1-\mu) = \frac{a_4}{a_2+a_4} \cdot \frac{a_2}{a_2+a_4} = \frac{a_2a_4}{(a_2+a_4)^2}

Substituting into ()(\dagger):

a1a3(a1+a3)2(P1P3)2=a2a4(a2+a4)2(P2P4)2\frac{a_1a_3}{(a_1+a_3)^2}(P_1P_3)^2 = \frac{a_2a_4}{(a_2+a_4)^2}(P_2P_4)^2

Since a1+a3=(a2+a4)a_1 + a_3 = -(a_2 + a_4), we have (a1+a3)2=(a2+a4)2(a_1+a_3)^2 = (a_2+a_4)^2. Multiplying both sides by this common value:

a1a3(P1P3)2=a2a4(P2P4)2a_1a_3(P_1P_3)^2 = a_2a_4(P_2P_4)^2 \qquad \blacksquare

Examiner Notes

Roughly two fifths of the candidates attempted this with a mean score of just over three marks making it the least well attempted question on the paper. Most could do part (i), which is GCSE material, but frustratingly quite a few stated that the triangles were similar with no justification. Part (ii) was by far the most poorly attempted part with a lot of hand-waving arguments. Part (iii) was done well by virtue of only the best candidates making it past part (i) with 75% of solutions containing good proofs by contradiction for the first result and the last two parts were pretty well done.


Topic: 级数与数论 (Series and Number Theory)  |  Difficulty: Hard  |  Marks: 20

8 The numbers f(r)f(r) satisfy f(r)>f(r+1)f(r) > f(r + 1) for r=1,2,r = 1, 2, \dots. Show that, for any non-negative integer nn,

kn(k1)f(kn+1)r=knkn+11f(r)kn(k1)f(kn)k^n(k - 1) f(k^{n+1}) \leqslant \sum_{r=k^n}^{k^{n+1}-1} f(r) \leqslant k^n(k - 1) f(k^n)

where kk is an integer greater than 1.

(i) By taking f(r)=1/rf(r) = 1/r, show that

N+12r=12N+111rN+1.\frac{N + 1}{2} \leqslant \sum_{r=1}^{2^{N+1}-1} \frac{1}{r} \leqslant N + 1 .

Deduce that the sum r=11r\sum_{r=1}^{\infty} \frac{1}{r} does not converge.

(ii) By taking f(r)=1/r3f(r) = 1/r^3, show that

r=11r3113.\sum_{r=1}^{\infty} \frac{1}{r^3} \leqslant 1\frac{1}{3} .

(iii) Let S(n)S(n) be the set of positive integers less than nn which do not have a 2 in their decimal representation and let σ(n)\sigma(n) be the sum of the reciprocals of the numbers in S(n)S(n), so for example σ(5)=1+13+14\sigma(5) = 1 + \frac{1}{3} + \frac{1}{4}. Show that S(1000)S(1000) contains 9319^3 - 1 distinct numbers.

Show that σ(n)<80\sigma(n) < 80 for all nn.

Hint

Since f(r)>f(r+1)f(r) > f(r+1), for knrkn+11k^n \leqslant r \leqslant k^{n+1}-1 we have f(kn+1)f(r)f(kn)f(k^{n+1}) \leqslant f(r) \leqslant f(k^n). The sum has kn+1kn=kn(k1)k^{n+1} - k^n = k^n(k-1) terms, so kn(k1)f(kn+1)r=knkn+11f(r)kn(k1)f(kn).k^n(k-1)f(k^{n+1}) \leqslant \sum_{r=k^n}^{k^{n+1}-1} f(r) \leqslant k^n(k-1)f(k^n).

(i) With f(r)=1/rf(r) = 1/r and k=2k = 2: 2n112n+1r=2n2n+111r2n112n2^n \cdot 1 \cdot \frac{1}{2^{n+1}} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r} \leqslant 2^n \cdot 1 \cdot \frac{1}{2^n}, i.e. 12r=2n2n+111r1\frac{1}{2} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r} \leqslant 1. Summing from n=0n = 0 to NN: N+12r=12N+111rN+1\frac{N+1}{2} \leqslant \sum_{r=1}^{2^{N+1}-1} \frac{1}{r} \leqslant N+1. Since limNN+12=\lim_{N \to \infty} \frac{N+1}{2} = \infty, the partial sums r=1M1r\sum_{r=1}^{M} \frac{1}{r} are unbounded, so r=11r\sum_{r=1}^{\infty} \frac{1}{r} does not converge.

(ii) With f(r)=1/r3f(r) = 1/r^3 and k=2k = 2: 2n123(n+1)r=2n2n+111r32n123n2^n \cdot \frac{1}{2^{3(n+1)}} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r^3} \leqslant 2^n \cdot \frac{1}{2^{3n}}, i.e. 122n+3r=2n2n+111r314n\frac{1}{2^{2n+3}} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r^3} \leqslant \frac{1}{4^n}. Summing from n=0n = 0 to \infty: r=11r3n=014n=111/4=43=113\sum_{r=1}^{\infty} \frac{1}{r^3} \leqslant \sum_{n=0}^{\infty} \frac{1}{4^n} = \frac{1}{1 - 1/4} = \frac{4}{3} = 1\frac{1}{3}.

(iii) The numbers in S(1000)S(1000) have at most 3 digits, none of which is 2. For 1-digit numbers: digits from {1,3,4,5,6,7,8,9}\{1,3,4,5,6,7,8,9\} gives 8 numbers. For 2-digit: first digit from {1,,9}{2}=8\{1,\dots,9\}\setminus\{2\} = 8 choices, second from {0,,9}{2}=9\{0,\dots,9\}\setminus\{2\} = 9 choices, giving 8×9=728 \times 9 = 72. For 3-digit: 8×9×9=6488 \times 9 \times 9 = 648. Total: 8+72+648=728=9318 + 72 + 648 = 728 = 9^3 - 1.

For σ(n)<80\sigma(n) < 80: use the stem with k=10k = 10 and f(r)=0f(r) = 0 if rr contains a 2 in its decimal representation, f(r)=1/rf(r) = 1/r otherwise. For each block [10n,10n+11][10^n, 10^{n+1}-1], the numbers without digit 2 contribute at most 10n9110n=910^n \cdot 9 \cdot \frac{1}{10^n} = 9 (by the stem upper bound, since there are at most 9×10n1×10n/(10n)9 \times 10^{n-1} \times 10^n/(10^n) valid terms). More precisely, the number of (n+1)(n+1)-digit integers with no digit 2 is 8×9n8 \times 9^n, and by the upper bound each block contributes at most 8×9n/10n8 \times 9^n / 10^n. Summing: σ(n)m=08(9/10)m=8119/10=80\sigma(n) \leqslant \sum_{m=0}^{\infty} 8 \cdot (9/10)^m = 8 \cdot \frac{1}{1-9/10} = 80. Since the bound is strict (the first block contributes strictly less than 8), σ(n)<80\sigma(n) < 80.

Model Solution

Stem result. Since ff is strictly decreasing, for every rr with knrkn+11k^n \leqslant r \leqslant k^{n+1}-1:

f(kn+1)<f(r)f(kn)f(k^{n+1}) < f(r) \leqslant f(k^n)

(The strict lower bound uses f(r)>f(r+1)f(r) > f(r+1); the upper bound uses f(kn)f(r)f(k^n) \geqslant f(r) since rknr \geqslant k^n.)

The number of terms in the sum is (kn+11)kn+1=kn+1kn=kn(k1)(k^{n+1}-1) - k^n + 1 = k^{n+1} - k^n = k^n(k-1).

Multiplying the inequalities by this count:

kn(k1)f(kn+1)<r=knkn+11f(r)kn(k1)f(kn)k^n(k-1)\,f(k^{n+1}) < \sum_{r=k^n}^{k^{n+1}-1} f(r) \leqslant k^n(k-1)\,f(k^n)

In particular:

kn(k1)f(kn+1)r=knkn+11f(r)kn(k1)f(kn)k^n(k-1)\,f(k^{n+1}) \leqslant \sum_{r=k^n}^{k^{n+1}-1} f(r) \leqslant k^n(k-1)\,f(k^n) \qquad \blacksquare

Part (i)

Take f(r)=1/rf(r) = 1/r (which is strictly decreasing) and k=2k = 2. The stem gives:

2n112n+1r=2n2n+111r2n112n2^n \cdot 1 \cdot \frac{1}{2^{n+1}} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r} \leqslant 2^n \cdot 1 \cdot \frac{1}{2^n}

12r=2n2n+111r1\frac{1}{2} \leqslant \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r} \leqslant 1

The intervals [2n,2n+11][2^n, 2^{n+1}-1] for n=0,1,,Nn = 0, 1, \ldots, N partition the integers from 11 to 2N+112^{N+1}-1. Summing:

n=0N12n=0Nr=2n2n+111rn=0N1\sum_{n=0}^{N} \frac{1}{2} \leqslant \sum_{n=0}^{N} \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r} \leqslant \sum_{n=0}^{N} 1

N+12r=12N+111rN+1\frac{N+1}{2} \leqslant \sum_{r=1}^{2^{N+1}-1} \frac{1}{r} \leqslant N+1 \qquad \blacksquare

Divergence of the harmonic series. Since r=12N+111rN+12\sum_{r=1}^{2^{N+1}-1} \frac{1}{r} \geqslant \frac{N+1}{2} and N+12\frac{N+1}{2} \to \infty as NN \to \infty, the partial sums r=1M1r\sum_{r=1}^{M} \frac{1}{r} are unbounded. Therefore r=11r\sum_{r=1}^{\infty} \frac{1}{r} does not converge. \qquad \blacksquare

Part (ii)

Take f(r)=1/r3f(r) = 1/r^3 (strictly decreasing) and k=2k = 2. The stem upper bound gives:

r=2n2n+111r32n(21)1(2n)3=2n23n=14n\sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r^3} \leqslant 2^n(2-1) \cdot \frac{1}{(2^n)^3} = \frac{2^n}{2^{3n}} = \frac{1}{4^n}

Since the intervals [2n,2n+11][2^n, 2^{n+1}-1] for n=0,1,2,n = 0, 1, 2, \ldots partition all positive integers:

r=11r3=n=0r=2n2n+111r3n=014n=1114=43=113\sum_{r=1}^{\infty} \frac{1}{r^3} = \sum_{n=0}^{\infty} \sum_{r=2^n}^{2^{n+1}-1} \frac{1}{r^3} \leqslant \sum_{n=0}^{\infty} \frac{1}{4^n} = \frac{1}{1 - \frac{1}{4}} = \frac{4}{3} = 1\tfrac{1}{3} \qquad \blacksquare

Part (iii)

Counting S(1000)S(1000). The elements of S(1000)S(1000) are positive integers less than 10001000 whose decimal representation contains no digit 22.

  • 1-digit numbers: Digits from {1,3,4,5,6,7,8,9}\{1, 3, 4, 5, 6, 7, 8, 9\} (8 choices, excluding 00 and 22). Count: 88.
  • 2-digit numbers: First digit from {1,3,4,5,6,7,8,9}\{1, 3, 4, 5, 6, 7, 8, 9\} (8 choices); second digit from {0,1,3,4,5,6,7,8,9}\{0, 1, 3, 4, 5, 6, 7, 8, 9\} (9 choices). Count: 8×9=728 \times 9 = 72.
  • 3-digit numbers: First digit: 8 choices; second and third digits: 9 choices each. Count: 8×9×9=6488 \times 9 \times 9 = 648.

Total: 8+72+648=7288 + 72 + 648 = 728.

We check: 931=7291=7289^3 - 1 = 729 - 1 = 728. \qquad \blacksquare

Showing σ(n)<80\sigma(n) < 80 for all nn.

We bound σ(n)\sigma(n) by summing over all positive integers without digit 22 (which includes S(n)S(n) as a subset, so σ(n)σ()\sigma(n) \leqslant \sigma(\infty)).

Group the positive integers without digit 22 by their number of digits dd:

  • For d=1d = 1: there are 88 such numbers, each at least 11. So the contribution is at most 88.
  • For d2d \geqslant 2: there are 8×9d18 \times 9^{d-1} such numbers, and each has dd digits so is at least 10d110^{d-1}. The contribution is at most

8×9d110d1=8(910)d1\frac{8 \times 9^{d-1}}{10^{d-1}} = 8\left(\frac{9}{10}\right)^{d-1}

Summing over all d1d \geqslant 1:

σ()d=18(910)d1=811910=8×10=80\sigma(\infty) \leqslant \sum_{d=1}^{\infty} 8\left(\frac{9}{10}\right)^{d-1} = 8 \cdot \frac{1}{1 - \frac{9}{10}} = 8 \times 10 = 80

This bound is not tight: for d=1d = 1, the actual sum 1+13+14++192.831 + \frac{1}{3} + \frac{1}{4} + \cdots + \frac{1}{9} \approx 2.83 is strictly less than 88. Therefore σ()<80\sigma(\infty) < 80.

Since σ(n)σ()<80\sigma(n) \leqslant \sigma(\infty) < 80 for every nn:

σ(n)<80\sigma(n) < 80 \qquad \blacksquare

Examiner Notes

Just fewer than half the candidates attempted this scoring just over a third of the marks. Many managed all but part (iii) easily but few managed that last part, and most did not try it. In part (i), having correctly used the result from the stem, there was frequently not enough care taken in extending this to the full sum. A not infrequent error of logic was that r=12N+111/r<N+1\sum_{r=1}^{2^{N+1}-1} 1/r < N + 1 and limNN+1=\lim_{N \to \infty} N + 1 = \infty somehow implies that r=11/r\sum_{r=1}^{\infty} 1/r does not converge.