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STEP2 1998 -- Pure Mathematics

Exam: STEP2  |  Year: 1998  |  Questions: Q1—Q8  |  Total marks per question: 20

All questions are pure mathematics. Model solutions are included below.

QTopicDifficultyKey Techniques
1代数与方程 (Algebra & Equations)Standard展开立方,奇偶性分析,整除性论证
2级数展开 (Series Expansion)Standard二项式定理,分数指数展开,数值计算
3级数求和 (Series & Summation)Challenging部分分式,裂项消去,递推数列
4积分 (Integration)Challenging递推积分,三角恒等式,积差消去
5复数 (Complex Numbers)Challenging复数模,三角不等式,数学归纳法,反证法
6解析几何与微积分 (Coordinate Geometry & Calculus)Challenging参数方程求导,切线法线方程,三角恒等式
7不等式与微积分 (Inequalities & Calculus)Challenging导数判号,不等式证明,对数求导法,三角函数性质
8向量几何 (Vector Geometry)Challenging向量参数方程,中点公式,共点证明,重心坐标

Topic: 代数与方程 (Algebra & Equations)  |  Difficulty: Standard  |  Marks: 20

1 Show that, if nn is an integer such that

(n−3)3+n3=(n+3)3,(*)(n - 3)^3 + n^3 = (n + 3)^3, \qquad \text{(*)}

then nn is even and n2n^2 is a factor of 54. Deduce that there is no integer nn which satisfies the equation (∗)(*).

Show that, if nn is an integer such that

(n−6)3+n3=(n+6)3,(**)(n - 6)^3 + n^3 = (n + 6)^3, \qquad \text{(**)}

then nn is even. Deduce that there is no integer nn which satisfies the equation (∗∗)(**).

Model Solution

Part (i): Show that if (n−3)3+n3=(n+3)3(n-3)^3 + n^3 = (n+3)^3 then nn is even and n2∣54n^2 \mid 54, and deduce no integer solution exists.

Expand each cube using (a+b)3=a3+3a2b+3ab2+b3(a+b)^3 = a^3 + 3a^2b + 3ab^2 + b^3:

(n−3)3=n3−9n2+27n−27(n-3)^3 = n^3 - 9n^2 + 27n - 27

(n+3)3=n3+9n2+27n+27(n+3)^3 = n^3 + 9n^2 + 27n + 27

Substituting into the equation:

(n3−9n2+27n−27)+n3=n3+9n2+27n+27(n^3 - 9n^2 + 27n - 27) + n^3 = n^3 + 9n^2 + 27n + 27

2n3−9n2+27n−27=n3+9n2+27n+272n^3 - 9n^2 + 27n - 27 = n^3 + 9n^2 + 27n + 27

Subtracting the right-hand side:

n3−18n2−54=0n^3 - 18n^2 - 54 = 0

Rearranging:

n2(n−18)=54(⋆)n^2(n - 18) = 54 \qquad \text{($\star$)}

nn is even. Suppose for contradiction that nn is odd. Then n2n^2 is odd and n−18n - 18 is odd (odd minus even), so the product n2(n−18)n^2(n-18) is odd. But the right-hand side 5454 is even, a contradiction. Hence nn is even.

n2n^2 is a factor of 54. From (⋆\star), since n−18n-18 is an integer, n2n^2 divides 5454.

No integer solution exists. We have 54=2×3354 = 2 \times 3^3. The positive divisors of 5454 that are perfect squares are 11 and 99 only.

  • n2=1  ⟹  n=±1n^2 = 1 \implies n = \pm 1: both are odd, contradicting nn even.
  • n2=9  ⟹  n=±3n^2 = 9 \implies n = \pm 3: both are odd, contradicting nn even.

Since no even integer has a square dividing 5454, there is no integer nn satisfying (⋆\star). ■\quad\blacksquare


Part (ii): Show that if (n−6)3+n3=(n+6)3(n-6)^3 + n^3 = (n+6)^3 then nn is even, and deduce no integer solution exists.

Expand:

(n−6)3=n3−18n2+108n−216(n-6)^3 = n^3 - 18n^2 + 108n - 216

(n+6)3=n3+18n2+108n+216(n+6)^3 = n^3 + 18n^2 + 108n + 216

Substituting:

(n3−18n2+108n−216)+n3=n3+18n2+108n+216(n^3 - 18n^2 + 108n - 216) + n^3 = n^3 + 18n^2 + 108n + 216

2n3−18n2+108n−216=n3+18n2+108n+2162n^3 - 18n^2 + 108n - 216 = n^3 + 18n^2 + 108n + 216

n3−36n2−432=0n^3 - 36n^2 - 432 = 0

n2(n−36)=432(⋆⋆)n^2(n - 36) = 432 \qquad \text{($\star\star$)}

nn is even. Suppose nn is odd. Then n2n^2 is odd and n−36n - 36 is odd, so n2(n−36)n^2(n-36) is odd. But 432432 is even, a contradiction. Hence nn is even.

No integer solution exists. Since nn is even, write n=2mn = 2m. Substituting into (⋆⋆\star\star):

4m2(2m−36)=4324m^2(2m - 36) = 432

m2(m−18)=54m^2(m - 18) = 54

Now 54=2×3354 = 2 \times 3^3, and the only perfect squares dividing 5454 are 11 and 99.

  • m2=1m^2 = 1: m=±1m = \pm 1, giving m2(m−18)=1×(−17)=−17m^2(m-18) = 1 \times (-17) = -17 or 1×(−19)=−191 \times (-19) = -19. Neither equals 5454.
  • m2=9m^2 = 9: m=±3m = \pm 3, giving m2(m−18)=9×(−15)=−135m^2(m-18) = 9 \times (-15) = -135 or 9×(−21)=−1899 \times (-21) = -189. Neither equals 5454.

No integer mm satisfies m2(m−18)=54m^2(m-18) = 54, so no integer nn satisfies (⋆⋆\star\star). ■\quad\blacksquare


Topic: 级数展开 (Series Expansion)  |  Difficulty: Standard  |  Marks: 20

2 Use the first four terms of the binomial expansion of (1−1/50)1/2(1 - 1/50)^{1/2}, writing 1/50=2/1001/50 = 2/100 to simplify the calculation, to derive the approximation 2≈1.414214\sqrt{2} \approx 1.414214.

Calculate similarly an approximation to the cube root of 2 to six decimal places by considering (1+N/125)a(1 + N/125)^a, where aa and NN are suitable numbers.

[You need not justify the accuracy of your approximations.]

Model Solution

Part (i): Approximating 2\sqrt{2}

Write 1/50=2/1001/50 = 2/100 and expand (1−2/100)1/2(1 - 2/100)^{1/2} using the binomial theorem with α=1/2\alpha = 1/2, x=−2/100x = -2/100:

(1+x)1/2=1+12x+12⋅(−12)2!x2+12⋅(−12)⋅(−32)3!x3+⋯(1+x)^{1/2} = 1 + \frac{1}{2}x + \frac{\tfrac{1}{2} \cdot (-\tfrac{1}{2})}{2!}x^2 + \frac{\tfrac{1}{2} \cdot (-\tfrac{1}{2}) \cdot (-\tfrac{3}{2})}{3!}x^3 + \cdots

Computing each coefficient:

12⋅(−12)2!=−18,12⋅(−12)⋅(−32)3!=116.\frac{\tfrac{1}{2} \cdot (-\tfrac{1}{2})}{2!} = -\frac{1}{8}, \qquad \frac{\tfrac{1}{2} \cdot (-\tfrac{1}{2}) \cdot (-\tfrac{3}{2})}{3!} = \frac{1}{16}.

With x=−2/100x = -2/100:

Term 1: 11

Term 2: 12×(−2100)=−1100=−0.01\dfrac{1}{2} \times \left(-\dfrac{2}{100}\right) = -\dfrac{1}{100} = -0.01

Term 3: −18×(−2100)2=−18×410000=−120000=−0.00005-\dfrac{1}{8} \times \left(-\dfrac{2}{100}\right)^2 = -\dfrac{1}{8} \times \dfrac{4}{10000} = -\dfrac{1}{20000} = -0.00005

Term 4: 116×(−2100)3=116×(−8106)=−12000000=−0.0000005\dfrac{1}{16} \times \left(-\dfrac{2}{100}\right)^3 = \dfrac{1}{16} \times \left(-\dfrac{8}{10^6}\right) = -\dfrac{1}{2000000} = -0.0000005

Sum:

1−1100−120000−12000000=2000000−20000−100−12000000=19798992000000=0.98994951 - \frac{1}{100} - \frac{1}{20000} - \frac{1}{2000000} = \frac{2000000 - 20000 - 100 - 1}{2000000} = \frac{1979899}{2000000} = 0.9899495

Now (1−1/50)1/2=(49/50)1/2=7/50=72/10(1 - 1/50)^{1/2} = (49/50)^{1/2} = 7/\sqrt{50} = 7\sqrt{2}/10, so:

7210≈0.9899495  ⟹  2≈107×0.9899495=19798991400000≈1.414213571...\frac{7\sqrt{2}}{10} \approx 0.9899495 \implies \sqrt{2} \approx \frac{10}{7} \times 0.9899495 = \frac{1979899}{1400000} \approx 1.414213571...

Rounding to six decimal places: 2≈1.414214\sqrt{2} \approx 1.414214. ■\quad\blacksquare


Part (ii): Approximating 21/32^{1/3}

We seek aa and NN such that (1+N/125)a(1 + N/125)^{a} relates to 21/32^{1/3}. Since 53=1255^3 = 125 and 43=644^3 = 64, observe that

(54)3×128125=12564×128125=2.\left(\frac{5}{4}\right)^3 \times \frac{128}{125} = \frac{125}{64} \times \frac{128}{125} = 2.

Taking cube roots:

21/3=54(128125)1/3=54(1+3125)1/3.2^{1/3} = \frac{5}{4}\left(\frac{128}{125}\right)^{1/3} = \frac{5}{4}\left(1 + \frac{3}{125}\right)^{1/3}.

So we take a=1/3a = 1/3 and N=3N = 3. Expanding (1+x)1/3(1 + x)^{1/3} with x=3/125x = 3/125:

(1+x)1/3=1+13x+13⋅(−23)2!x2+13⋅(−23)⋅(−53)3!x3+⋯(1+x)^{1/3} = 1 + \frac{1}{3}x + \frac{\tfrac{1}{3}\cdot(-\tfrac{2}{3})}{2!}x^2 + \frac{\tfrac{1}{3}\cdot(-\tfrac{2}{3})\cdot(-\tfrac{5}{3})}{3!}x^3 + \cdots

Computing the binomial coefficients:

13⋅(−23)2=−19,13⋅(−23)⋅(−53)6=581.\frac{\tfrac{1}{3} \cdot (-\tfrac{2}{3})}{2} = -\frac{1}{9}, \qquad \frac{\tfrac{1}{3} \cdot (-\tfrac{2}{3}) \cdot (-\tfrac{5}{3})}{6} = \frac{5}{81}.

With x=3/125x = 3/125:

Term 1: 11

Term 2: 13×3125=1125\dfrac{1}{3} \times \dfrac{3}{125} = \dfrac{1}{125}

Term 3: −19×(3125)2=−19×915625=−115625-\dfrac{1}{9} \times \left(\dfrac{3}{125}\right)^2 = -\dfrac{1}{9} \times \dfrac{9}{15625} = -\dfrac{1}{15625}

Term 4: 581×(3125)3=581×271953125=135158203125=11171875\dfrac{5}{81} \times \left(\dfrac{3}{125}\right)^3 = \dfrac{5}{81} \times \dfrac{27}{1953125} = \dfrac{135}{158203125} = \dfrac{1}{1171875}

Sum with a common denominator of 11718751171875:

1+1125−115625+11171875=1171875+9375−75+11171875=118117611718751 + \frac{1}{125} - \frac{1}{15625} + \frac{1}{1171875} = \frac{1171875 + 9375 - 75 + 1}{1171875} = \frac{1181176}{1171875}

Therefore:

21/3≈54×11811761171875=59058804687500=295294234375≈1.259921067...2^{1/3} \approx \frac{5}{4} \times \frac{1181176}{1171875} = \frac{5905880}{4687500} = \frac{295294}{234375} \approx 1.259921067...

To six decimal places: 21/3≈1.2599212^{1/3} \approx 1.259921. ■\quad\blacksquare


Topic: 级数求和 (Series & Summation)  |  Difficulty: Challenging  |  Marks: 20

3 Show that the sum SNS_N of the first NN terms of the series

11.2.3+32.3.4+53.4.5+⋯+2n−1n(n+1)(n+2)+…\frac{1}{1.2.3} + \frac{3}{2.3.4} + \frac{5}{3.4.5} + \dots + \frac{2n - 1}{n(n + 1)(n + 2)} + \dots

is

12(32+1N+1−5N+2).\frac{1}{2} \left( \frac{3}{2} + \frac{1}{N + 1} - \frac{5}{N + 2} \right).

What is the limit of SNS_N as N→∞N \to \infty?

The numbers ana_n are such that

anan−1=(n−1)(2n−1)(n+2)(2n−3).\frac{a_n}{a_{n-1}} = \frac{(n - 1)(2n - 1)}{(n + 2)(2n - 3)}.

Find an expression for an/a1a_n/a_1 and hence, or otherwise, evaluate ∑n=1∞an\sum_{n=1}^{\infty} a_n when a1=29a_1 = \frac{2}{9}.

Model Solution

Part 1: Evaluating SNS_N

The nn-th term is

un=2n−1n(n+1)(n+2).u_n = \frac{2n - 1}{n(n + 1)(n + 2)}.

Partial fractions. Write

2n−1n(n+1)(n+2)=An+Bn+1+Cn+2.\frac{2n - 1}{n(n + 1)(n + 2)} = \frac{A}{n} + \frac{B}{n + 1} + \frac{C}{n + 2}.

Multiplying through by n(n+1)(n+2)n(n+1)(n+2):

2n−1=A(n+1)(n+2)+Bn(n+2)+Cn(n+1).2n - 1 = A(n + 1)(n + 2) + Bn(n + 2) + Cn(n + 1).

  • n=0n = 0: −1=2A  ⟹  A=−12-1 = 2A \implies A = -\tfrac{1}{2}
  • n=−1n = -1: −3=−B  ⟹  B=3-3 = -B \implies B = 3
  • n=−2n = -2: −5=2C  ⟹  C=−52-5 = 2C \implies C = -\tfrac{5}{2}

Therefore

un=−12n+3n+1−52(n+2).u_n = -\frac{1}{2n} + \frac{3}{n + 1} - \frac{5}{2(n + 2)}.

Verification. n=1n = 1: −12+32−56=16=11⋅2⋅3-\frac{1}{2} + \frac{3}{2} - \frac{5}{6} = \frac{1}{6} = \frac{1}{1 \cdot 2 \cdot 3}. ✓\checkmark

n=2n = 2: −14+1−58=18=324-\frac{1}{4} + 1 - \frac{5}{8} = \frac{1}{8} = \frac{3}{24}. ✓\checkmark

Summing. Let HN=∑n=1N1nH_N = \sum_{n=1}^{N} \frac{1}{n}. Then

SN=−12HN+3∑n=1N1n+1−52∑n=1N1n+2.S_N = -\frac{1}{2}H_N + 3\sum_{n=1}^{N}\frac{1}{n+1} - \frac{5}{2}\sum_{n=1}^{N}\frac{1}{n+2}.

Re-indexing the second sum (m=n+1m = n + 1):

∑n=1N1n+1=∑m=2N+11m=HN+1N+1−1.\sum_{n=1}^{N}\frac{1}{n+1} = \sum_{m=2}^{N+1}\frac{1}{m} = H_N + \frac{1}{N+1} - 1.

Re-indexing the third sum (m=n+2m = n + 2):

∑n=1N1n+2=∑m=3N+21m=HN+1N+1+1N+2−32.\sum_{n=1}^{N}\frac{1}{n+2} = \sum_{m=3}^{N+2}\frac{1}{m} = H_N + \frac{1}{N+1} + \frac{1}{N+2} - \frac{3}{2}.

Substituting:

SN=−12HN+3 ⁣(HN+1N+1−1)−52 ⁣(HN+1N+1+1N+2−32).S_N = -\frac{1}{2}H_N + 3\!\left(H_N + \frac{1}{N+1} - 1\right) - \frac{5}{2}\!\left(H_N + \frac{1}{N+1} + \frac{1}{N+2} - \frac{3}{2}\right).

The coefficient of HNH_N is −12+3−52=0-\frac{1}{2} + 3 - \frac{5}{2} = 0, so all harmonic terms cancel. Collecting the rest:

SN=3N+1−3−52(N+1)−52(N+2)+154S_N = \frac{3}{N+1} - 3 - \frac{5}{2(N+1)} - \frac{5}{2(N+2)} + \frac{15}{4}

=12(N+1)−52(N+2)+34.= \frac{1}{2(N+1)} - \frac{5}{2(N+2)} + \frac{3}{4}.

Rewriting with a common factor of 12\frac{1}{2}:

SN=12 ⁣(32+1N+1−5N+2).(as required)S_N = \frac{1}{2}\!\left(\frac{3}{2} + \frac{1}{N+1} - \frac{5}{N+2}\right). \qquad \text{(as required)}

Check. N=1N = 1: 12(32+12−53)=12⋅13=16=11⋅2⋅3\frac{1}{2}(\frac{3}{2} + \frac{1}{2} - \frac{5}{3}) = \frac{1}{2} \cdot \frac{1}{3} = \frac{1}{6} = \frac{1}{1 \cdot 2 \cdot 3}. ✓\checkmark

N=2N = 2: 12(32+13−54)=12⋅18+4−1512=12⋅712=724\frac{1}{2}(\frac{3}{2} + \frac{1}{3} - \frac{5}{4}) = \frac{1}{2} \cdot \frac{18 + 4 - 15}{12} = \frac{1}{2} \cdot \frac{7}{12} = \frac{7}{24}. And S2=16+324=724S_2 = \frac{1}{6} + \frac{3}{24} = \frac{7}{24}. ✓\checkmark

Limit. As N→∞N \to \infty:

lim⁡N→∞SN=12 ⁣(32+0−0)=34.\lim_{N\to\infty} S_N = \frac{1}{2}\!\left(\frac{3}{2} + 0 - 0\right) = \boxed{\frac{3}{4}}.


Part 2: Using the recurrence for ana_n

For n≥2n \geq 2,

ana1=∏k=2n(k−1)(2k−1)(k+2)(2k−3).\frac{a_n}{a_1} = \prod_{k=2}^{n} \frac{(k - 1)(2k - 1)}{(k + 2)(2k - 3)}.

Separate the product into two telescoping parts:

∏k=2nk−1k+2=1⋅2⋅3⋯(n−1)4⋅5⋅6⋯(n+2)=6n(n+1)(n+2),\prod_{k=2}^{n} \frac{k - 1}{k + 2} = \frac{1 \cdot 2 \cdot 3 \cdots (n - 1)}{4 \cdot 5 \cdot 6 \cdots (n + 2)} = \frac{6}{n(n + 1)(n + 2)},

and

∏k=2n2k−12k−3=31⋅53⋅75⋯2n−12n−3=2n−1.\prod_{k=2}^{n} \frac{2k - 1}{2k - 3} = \frac{3}{1}\cdot\frac{5}{3}\cdot\frac{7}{5}\cdots\frac{2n - 1}{2n - 3} = 2n - 1.

Hence

ana1=6(2n−1)n(n+1)(n+2).\frac{a_n}{a_1} = \frac{6(2n - 1)}{n(n + 1)(n + 2)}.

This also gives a1a1=1\frac{a_1}{a_1}=1 when n=1n=1, so the formula is valid for all n≥1n \geq 1.

If a1=29a_1 = \frac{2}{9}, then

an=29⋅6(2n−1)n(n+1)(n+2)=4(2n−1)3n(n+1)(n+2).a_n = \frac{2}{9}\cdot\frac{6(2n - 1)}{n(n + 1)(n + 2)} = \frac{4(2n - 1)}{3n(n + 1)(n + 2)}.

Using the first part of the question,

∑n=1∞2n−1n(n+1)(n+2)=lim⁡N→∞SN=34.\sum_{n=1}^{\infty} \frac{2n - 1}{n(n + 1)(n + 2)} = \lim_{N\to\infty} S_N = \frac{3}{4}.

Therefore

∑n=1∞an=43⋅34=1.\sum_{n=1}^{\infty} a_n = \frac{4}{3}\cdot\frac{3}{4} = \boxed{1}.


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

4 The integral InI_n is defined by

In=∫0π(π/2−x)sin⁡(nx+x/2)cosec⁡(x/2) dx,I_n = \int_{0}^{\pi} (\pi/2 - x) \sin(nx + x/2) \operatorname{cosec}(x/2) \, dx,

where nn is a positive integer. Evaluate In−In−1I_n - I_{n-1}, and hence evaluate InI_n leaving your answer in the form of a sum.

Model Solution

Step 1: Evaluate In−In−1I_n - I_{n-1}

Write the difference as a single integral:

In−In−1=∫0π(π/2−x)[sin⁡ ⁣((n+12)x)−sin⁡ ⁣((n−12)x)]csc⁡(x/2) dx.I_n - I_{n-1} = \int_0^\pi (\pi/2 - x)\bigl[\sin\!\bigl((n + \tfrac{1}{2})x\bigr) - \sin\!\bigl((n - \tfrac{1}{2})x\bigr)\bigr]\csc(x/2)\,dx.

Using sin⁡A−sin⁡B=2cos⁡ ⁣(A+B2)sin⁡ ⁣(A−B2)\sin A - \sin B = 2\cos\!\bigl(\frac{A+B}{2}\bigr)\sin\!\bigl(\frac{A-B}{2}\bigr) with A=(n+12)xA = (n + \frac{1}{2})x and B=(n−12)xB = (n - \frac{1}{2})x:

A+B2=nx,A−B2=x/2,\frac{A+B}{2} = nx, \qquad \frac{A-B}{2} = x/2,

sin⁡ ⁣((n+12)x)−sin⁡ ⁣((n−12)x)=2cos⁡(nx)sin⁡(x/2).\sin\!\bigl((n + \tfrac{1}{2})x\bigr) - \sin\!\bigl((n - \tfrac{1}{2})x\bigr) = 2\cos(nx)\sin(x/2).

Since sin⁡(x/2)csc⁡(x/2)=1\sin(x/2)\csc(x/2) = 1:

In−In−1=∫0π2(π/2−x)cos⁡(nx) dx.(⋆)I_n - I_{n-1} = \int_0^\pi 2(\pi/2 - x)\cos(nx)\,dx. \qquad \text{($\star$)}

Evaluate by parts with u=π/2−xu = \pi/2 - x and dv=cos⁡(nx) dxdv = \cos(nx)\,dx:

In−In−1=[2(π/2−x)sin⁡(nx)n]0π+2n∫0πsin⁡(nx) dx.I_n - I_{n-1} = \left[\frac{2(\pi/2 - x)\sin(nx)}{n}\right]_0^\pi + \frac{2}{n}\int_0^\pi \sin(nx)\,dx.

The boundary term vanishes at both limits: at x=0x = 0, sin⁡0=0\sin 0 = 0; at x=πx = \pi, sin⁡(nπ)=0\sin(n\pi) = 0 for integer nn.

In−In−1=2n[−cos⁡(nx)n]0π=2n2(1−cos⁡(nπ))=2(1−(−1)n)n2.(⋆⋆)I_n - I_{n-1} = \frac{2}{n}\left[-\frac{\cos(nx)}{n}\right]_0^\pi = \frac{2}{n^2}\bigl(1 - \cos(n\pi)\bigr) = \frac{2\bigl(1 - (-1)^n\bigr)}{n^2}. \qquad \text{($\star\star$)}

This equals 4n2\frac{4}{n^2} when nn is odd, and 00 when nn is even.

Check. For n=1n = 1: 2(1−(−1))1=4\frac{2(1-(-1))}{1} = 4. For n=2n = 2: 2(1−1)4=0\frac{2(1-1)}{4} = 0. For n=3n = 3: 49\frac{4}{9}. ✓\checkmark


Step 2: Evaluate I1I_1

We use the identity

csc⁡(x/2)sin⁡ ⁣((n+12)x)=1+2∑k=1ncos⁡(kx),(⋆⋆⋆)\csc(x/2)\sin\!\bigl((n + \tfrac{1}{2})x\bigr) = 1 + 2\sum_{k=1}^{n}\cos(kx), \qquad \text{($\star\star\star$)}

which follows by induction: the base case n=0n = 0 gives 11 on both sides, and the inductive step uses 2cos⁡(nx)sin⁡(x/2)=sin⁡((n+12)x)−sin⁡((n−12)x)2\cos(nx)\sin(x/2) = \sin((n+\frac{1}{2})x) - \sin((n-\frac{1}{2})x).

For n=1n = 1: csc⁡(x/2)sin⁡(3x/2)=1+2cos⁡x\csc(x/2)\sin(3x/2) = 1 + 2\cos x, so

I1=∫0π(π/2−x)(1+2cos⁡x) dx=∫0π(π/2−x) dx⏟= 0+2∫0π(π/2−x)cos⁡x dx.I_1 = \int_0^\pi (\pi/2 - x)(1 + 2\cos x)\,dx = \underbrace{\int_0^\pi (\pi/2 - x)\,dx}_{= \, 0} + 2\int_0^\pi (\pi/2 - x)\cos x\,dx.

The first integral vanishes since π/2−x\pi/2 - x is antisymmetric about x=π/2x = \pi/2. For the second, integrate by parts:

2[(π/2−x)sin⁡x]0π+2∫0πsin⁡x dx=0+2[−cos⁡x]0π=2(1+1)=4.2\Bigl[(\pi/2 - x)\sin x\Bigr]_0^\pi + 2\int_0^\pi \sin x\,dx = 0 + 2[-\cos x]_0^\pi = 2(1 + 1) = 4.

Therefore I1=4I_1 = 4.

Check. Also, from (⋆⋆\star\star) with n=1n = 1: I1−I0=4I_1 - I_0 = 4, where I0=∫0π(π/2−x)csc⁡(x/2)sin⁡(x/2) dx=∫0π(π/2−x) dx=0I_0 = \int_0^\pi (\pi/2 - x)\csc(x/2)\sin(x/2)\,dx = \int_0^\pi (\pi/2 - x)\,dx = 0. So I1=4I_1 = 4. ✓\checkmark


Step 3: Express InI_n as a sum

By telescoping from I0=0I_0 = 0:

In=∑k=1n(Ik−Ik−1)=∑k=1n2(1−(−1)k)k2.I_n = \sum_{k=1}^{n}(I_k - I_{k-1}) = \sum_{k=1}^{n}\frac{2(1 - (-1)^k)}{k^2}.

Since 1−(−1)k=01 - (-1)^k = 0 for even kk and 22 for odd kk:

In=4∑k=1k oddn1k2=4∑m=1⌈n/2⌉1(2m−1)2.(†)I_n = 4\sum_{\substack{k = 1 \\ k \text{ odd}}}^{n}\frac{1}{k^2} = 4\sum_{m=1}^{\lceil n/2 \rceil}\frac{1}{(2m-1)^2}. \qquad \text{($\dagger$)}

Equivalently:

In=4(1+132+152+⋯+1(2⌈n/2⌉−1)2).I_n = 4\left(1 + \frac{1}{3^2} + \frac{1}{5^2} + \cdots + \frac{1}{(2\lceil n/2\rceil - 1)^2}\right).

Verification. n=1n = 1: I1=4/12=4I_1 = 4/1^2 = 4. ✓\checkmark

n=2n = 2: I2=4/12=4I_2 = 4/1^2 = 4 (only odd k≤2k \leq 2 is k=1k = 1). ✓\checkmark

n=3n = 3: I3=4(1+1/9)=40/9I_3 = 4(1 + 1/9) = 40/9. ✓\checkmark

n=4n = 4: I4=4(1+1/9)=40/9I_4 = 4(1 + 1/9) = 40/9. ✓\checkmark


Topic: 复数 (Complex Numbers)  |  Difficulty: Challenging  |  Marks: 20

5 Define the modulus of a complex number zz and give the geometric interpretation of ∣z1−z2∣|z_1 - z_2| for two complex numbers z1z_1 and z2z_2. On the basis of this interpretation establish the inequality

∣z1+z2∣⩽∣z1∣+∣z2∣.|z_1 + z_2| \leqslant |z_1| + |z_2|.

Use this result to prove, by induction, the corresponding inequality for ∣z1+⋯+zn∣|z_1 + \dots + z_n|.

The complex numbers a1,a2,…,ana_1, a_2, \dots, a_n satisfy ∣ai∣⩽3|a_i| \leqslant 3 (i=1,2,…,ni = 1, 2, \dots, n). Prove that the equation

a1z+a2z2+⋯+anzn=1a_1 z + a_2 z^2 + \dots + a_n z^n = 1

has no solution zz with ∣z∣⩽1/4|z| \leqslant 1/4.

Model Solution

Definition and geometric interpretation

Let z=x+iyz = x + iy where x,y∈Rx, y \in \mathbb{R}. The modulus of zz is defined as

∣z∣=x2+y2.|z| = \sqrt{x^2 + y^2}.

Geometrically, ∣z∣|z| is the distance from the origin to the point (x,y)(x, y) in the Argand diagram. For two complex numbers z1z_1 and z2z_2, the quantity ∣z1−z2∣|z_1 - z_2| is the distance between the points representing z1z_1 and z2z_2 in the complex plane.

Establishing the triangle inequality

Consider the triangle with vertices at 00, z1z_1, and z1+z2z_1 + z_2 in the Argand diagram. The three sides of this triangle have lengths:

  • ∣z1−0∣=∣z1∣|z_1 - 0| = |z_1| (distance from origin to z1z_1),
  • ∣(z1+z2)−z1∣=∣z2∣|(z_1 + z_2) - z_1| = |z_2| (distance from z1z_1 to z1+z2z_1 + z_2),
  • ∣(z1+z2)−0∣=∣z1+z2∣|(z_1 + z_2) - 0| = |z_1 + z_2| (distance from origin to z1+z2z_1 + z_2).

By the triangle inequality for Euclidean distance (the length of one side of a triangle cannot exceed the sum of the lengths of the other two sides):

∣z1+z2∣⩽∣z1∣+∣z2∣.(△ inequality)|z_1 + z_2| \leqslant |z_1| + |z_2|. \qquad \text{($\triangle$ inequality)}

Equality holds if and only if z1z_1 and z2z_2 lie on the same ray from the origin, i.e., z2=λz1z_2 = \lambda z_1 for some λ⩾0\lambda \geqslant 0.

Proof by induction for the general case

We prove that for any n⩾2n \geqslant 2 and complex numbers z1,z2,…,znz_1, z_2, \dots, z_n:

∣z1+z2+⋯+zn∣⩽∣z1∣+∣z2∣+⋯+∣zn∣.|z_1 + z_2 + \dots + z_n| \leqslant |z_1| + |z_2| + \dots + |z_n|.

Base case (n=2n = 2): This is the inequality established above.

Inductive step: Suppose the result holds for n=kn = k, i.e.,

∣z1+z2+⋯+zk∣⩽∣z1∣+∣z2∣+⋯+∣zk∣.|z_1 + z_2 + \dots + z_k| \leqslant |z_1| + |z_2| + \dots + |z_k|.

For n=k+1n = k + 1, let w=z1+z2+⋯+zkw = z_1 + z_2 + \dots + z_k. Then:

∣z1+z2+⋯+zk+zk+1∣=∣w+zk+1∣⩽∣w∣+∣zk+1∣|z_1 + z_2 + \dots + z_k + z_{k+1}| = |w + z_{k+1}| \leqslant |w| + |z_{k+1}|

by the base case. Applying the inductive hypothesis to ∣w∣|w|:

∣w∣+∣zk+1∣=∣z1+z2+⋯+zk∣+∣zk+1∣⩽∣z1∣+∣z2∣+⋯+∣zk∣+∣zk+1∣.|w| + |z_{k+1}| = |z_1 + z_2 + \dots + z_k| + |z_{k+1}| \leqslant |z_1| + |z_2| + \dots + |z_k| + |z_{k+1}|.

Combining: ∣z1+z2+⋯+zk+1∣⩽∣z1∣+∣z2∣+⋯+∣zk+1∣|z_1 + z_2 + \dots + z_{k+1}| \leqslant |z_1| + |z_2| + \dots + |z_{k+1}|.

By induction, the inequality holds for all n⩾2n \geqslant 2.

Proving the equation has no solution with ∣z∣⩽1/4|z| \leqslant 1/4

Suppose for contradiction that there exists zz with ∣z∣⩽1/4|z| \leqslant 1/4 satisfying

a1z+a2z2+⋯+anzn=1.a_1 z + a_2 z^2 + \dots + a_n z^n = 1.

Taking the modulus of both sides and applying the generalised triangle inequality:

1=∣a1z+a2z2+⋯+anzn∣⩽∣a1z∣+∣a2z2∣+⋯+∣anzn∣.1 = |a_1 z + a_2 z^2 + \dots + a_n z^n| \leqslant |a_1 z| + |a_2 z^2| + \dots + |a_n z^n|.

Since ∣ai∣⩽3|a_i| \leqslant 3 and ∣zk∣=∣z∣k|z^k| = |z|^k:

1⩽3∣z∣+3∣z∣2+⋯+3∣z∣n=3∣z∣(1+∣z∣+∣z∣2+⋯+∣z∣n−1).1 \leqslant 3|z| + 3|z|^2 + \dots + 3|z|^n = 3|z|\bigl(1 + |z| + |z|^2 + \dots + |z|^{n-1}\bigr).

Since ∣z∣⩽1/4<1|z| \leqslant 1/4 < 1, the geometric series satisfies:

1+∣z∣+∣z∣2+⋯+∣z∣n−1=1−∣z∣n1−∣z∣⩽11−1/4=43.1 + |z| + |z|^2 + \dots + |z|^{n-1} = \frac{1 - |z|^n}{1 - |z|} \leqslant \frac{1}{1 - 1/4} = \frac{4}{3}.

Therefore:

1⩽3∣z∣⋅43=4∣z∣⩽4⋅14=1.1 \leqslant 3|z| \cdot \frac{4}{3} = 4|z| \leqslant 4 \cdot \frac{1}{4} = 1.

This forces every inequality to be an equality, which requires both ∣z∣=1/4|z| = 1/4 and ∣z∣n=0|z|^n = 0. But ∣z∣=1/4|z| = 1/4 gives ∣z∣n=(1/4)n>0|z|^n = (1/4)^n > 0, so 1−(1/4)n1−1/4<43\frac{1 - (1/4)^n}{1 - 1/4} < \frac{4}{3}. Hence:

1⩽4⋅14⋅(1−14n)=1−14n<1,1 \leqslant 4 \cdot \frac{1}{4} \cdot \left(1 - \frac{1}{4^n}\right) = 1 - \frac{1}{4^n} < 1,

which is a contradiction. Therefore the equation has no solution with ∣z∣⩽1/4|z| \leqslant 1/4. ■\quad\blacksquare


Topic: 解析几何与微积分 (Coordinate Geometry & Calculus)  |  Difficulty: Challenging  |  Marks: 20

6 Two curves are given parametrically by

(1) x1=(θ+sin⁡θ)x_1 = (\theta + \sin \theta), y1=(1+cos⁡θ)y_1 = (1 + \cos \theta),

and

(2) x2=(θ−sin⁡θ)x_2 = (\theta - \sin \theta), y2=−(1+cos⁡θ)y_2 = -(1 + \cos \theta).

Find the gradients of the tangents to the curves at the points where θ=π/2\theta = \pi/2 and θ=3π/2\theta = 3\pi/2. Sketch, using the same axes, the curves for 0⩽θ⩽2π0 \leqslant \theta \leqslant 2\pi.

Find the equation of the normal to the curve (1) at the point with parameter θ\theta. Show that this normal is a tangent to the curve (2).

Model Solution

Gradients of the tangents

Curve (1): x1=θ+sin⁡θx_1 = \theta + \sin\theta,   y1=1+cos⁡θ\;y_1 = 1 + \cos\theta.

dx1dθ=1+cos⁡θ,dy1dθ=−sin⁡θ.\frac{dx_1}{d\theta} = 1 + \cos\theta, \qquad \frac{dy_1}{d\theta} = -\sin\theta.

dy1dx1=−sin⁡θ1+cos⁡θ.\frac{dy_1}{dx_1} = \frac{-\sin\theta}{1 + \cos\theta}.

At θ=π/2\theta = \pi/2: dx1/dθ=1+0=1\quad dx_1/d\theta = 1 + 0 = 1, dy1/dθ=−1\quad dy_1/d\theta = -1, so dy1dx1=−1\dfrac{dy_1}{dx_1} = -1.

At θ=3π/2\theta = 3\pi/2: dx1/dθ=1+0=1\quad dx_1/d\theta = 1 + 0 = 1, dy1/dθ=−(−1)=1\quad dy_1/d\theta = -(-1) = 1, so dy1dx1=1\dfrac{dy_1}{dx_1} = 1.

Curve (2): x2=θ−sin⁡θx_2 = \theta - \sin\theta,   y2=−(1+cos⁡θ)\;y_2 = -(1 + \cos\theta).

dx2dθ=1−cos⁡θ,dy2dθ=sin⁡θ.\frac{dx_2}{d\theta} = 1 - \cos\theta, \qquad \frac{dy_2}{d\theta} = \sin\theta.

dy2dx2=sin⁡θ1−cos⁡θ.\frac{dy_2}{dx_2} = \frac{\sin\theta}{1 - \cos\theta}.

At θ=π/2\theta = \pi/2: dx2/dθ=1−0=1\quad dx_2/d\theta = 1 - 0 = 1, dy2/dθ=1\quad dy_2/d\theta = 1, so dy2dx2=1\dfrac{dy_2}{dx_2} = 1.

At θ=3π/2\theta = 3\pi/2: dx2/dθ=1−0=1\quad dx_2/d\theta = 1 - 0 = 1, dy2/dθ=−1\quad dy_2/d\theta = -1, so dy2dx2=−1\dfrac{dy_2}{dx_2} = -1.

Summary of gradients:

Curve (1)Curve (2)
θ=π/2\theta = \pi/2−1-111
θ=3π/2\theta = 3\pi/211−1-1

Sketch

Both curves are cycloids (the path traced by a point on the rim of a circle of radius 1 rolling along a line).

Curve (1) is an upward-opening cycloid arch. Key points at θ=0,π/2,π,3π/2,2π\theta = 0, \pi/2, \pi, 3\pi/2, 2\pi:

(0, 2),(π/2, 1),(π, 0),(3π/2, 1),(2π, 2).(0,\, 2),\quad (\pi/2,\, 1),\quad (\pi,\, 0),\quad (3\pi/2,\, 1),\quad (2\pi,\, 2).

It starts at (0,2)(0, 2), descends to a cusp at (π,0)(\pi, 0) where it touches the xx-axis, then returns to (2π,2)(2\pi, 2). The curve is symmetric about x=πx = \pi.

Curve (2) is an inverted cycloid. Key points:

(0, −2),(π/2, −1),(π, 0),(3π/2, −1),(2π, −2).(0,\, -2),\quad (\pi/2,\, -1),\quad (\pi,\, 0),\quad (3\pi/2,\, -1),\quad (2\pi,\, -2).

It starts at (0,−2)(0, -2), rises to a cusp at (π,0)(\pi, 0) where it touches the xx-axis, then returns to (2π,−2)(2\pi, -2). The two curves are reflections of each other in the line y=0y = 0.

Normal to curve (1) at parameter θ\theta

The tangent to curve (1) at parameter θ\theta has slope

dy1dx1=−sin⁡θ1+cos⁡θ.\frac{dy_1}{dx_1} = \frac{-\sin\theta}{1 + \cos\theta}.

The normal at this point has slope equal to the negative reciprocal:

mnormal=1+cos⁡θsin⁡θ.m_{\text{normal}} = \frac{1 + \cos\theta}{\sin\theta}.

(When sin⁡θ=0\sin\theta = 0, the tangent is horizontal and the normal is vertical.)

The point on curve (1) is (θ+sin⁡θ,  1+cos⁡θ)(\theta + \sin\theta,\; 1 + \cos\theta), so the normal equation is:

y−(1+cos⁡θ)=1+cos⁡θsin⁡θ (x−(θ+sin⁡θ)).y - (1 + \cos\theta) = \frac{1 + \cos\theta}{\sin\theta}\,\bigl(x - (\theta + \sin\theta)\bigr).

Multiplying both sides by sin⁡θ\sin\theta:

(y−1−cos⁡θ)sin⁡θ=(1+cos⁡θ)(x−θ−sin⁡θ).\bigl(y - 1 - \cos\theta\bigr)\sin\theta = (1 + \cos\theta)\bigl(x - \theta - \sin\theta\bigr).

Expanding both sides:

ysin⁡θ−sin⁡θ−sin⁡θcos⁡θ=x(1+cos⁡θ)−θ(1+cos⁡θ)−sin⁡θ(1+cos⁡θ).y\sin\theta - \sin\theta - \sin\theta\cos\theta = x(1 + \cos\theta) - \theta(1 + \cos\theta) - \sin\theta(1 + \cos\theta).

Expanding the last term on the right: sin⁡θ(1+cos⁡θ)=sin⁡θ+sin⁡θcos⁡θ\sin\theta(1 + \cos\theta) = \sin\theta + \sin\theta\cos\theta, so:

ysin⁡θ−sin⁡θ−sin⁡θcos⁡θ=x(1+cos⁡θ)−θ(1+cos⁡θ)−sin⁡θ−sin⁡θcos⁡θ.y\sin\theta - \sin\theta - \sin\theta\cos\theta = x(1 + \cos\theta) - \theta(1 + \cos\theta) - \sin\theta - \sin\theta\cos\theta.

The terms −sin⁡θ−sin⁡θcos⁡θ-\sin\theta - \sin\theta\cos\theta cancel from both sides, leaving:

ysin⁡θ=x(1+cos⁡θ)−θ(1+cos⁡θ).y\sin\theta = x(1 + \cos\theta) - \theta(1 + \cos\theta).

Rearranging, the normal equation is:

x(1+cos⁡θ)−ysin⁡θ=θ(1+cos⁡θ).(⋆)x(1 + \cos\theta) - y\sin\theta = \theta(1 + \cos\theta). \qquad \text{($\star$)}

Showing the normal is tangent to curve (2)

Take the point P2P_2 on curve (2) at the same parameter value θ\theta:

P2=(θ−sin⁡θ,  −(1+cos⁡θ)).P_2 = \bigl(\theta - \sin\theta,\; -(1 + \cos\theta)\bigr).

Step 1: P2P_2 lies on the normal (⋆\star). Substitute into the left-hand side:

(θ−sin⁡θ)(1+cos⁡θ)−(−(1+cos⁡θ))sin⁡θ.(\theta - \sin\theta)(1 + \cos\theta) - \bigl(-(1 + \cos\theta)\bigr)\sin\theta.

Expanding:

=θ(1+cos⁡θ)−sin⁡θ(1+cos⁡θ)+sin⁡θ(1+cos⁡θ)=θ(1+cos⁡θ).= \theta(1 + \cos\theta) - \sin\theta(1 + \cos\theta) + \sin\theta(1 + \cos\theta) = \theta(1 + \cos\theta).

This equals the right-hand side of (⋆\star), so P2P_2 lies on the normal to curve (1) at parameter θ\theta.

Step 2: The normal has the same slope as the tangent to curve (2) at P2P_2.

The tangent to curve (2) at parameter θ\theta has slope

dy2dx2=sin⁡θ1−cos⁡θ.\frac{dy_2}{dx_2} = \frac{\sin\theta}{1 - \cos\theta}.

We verify this equals the normal slope 1+cos⁡θsin⁡θ\frac{1 + \cos\theta}{\sin\theta}:

1+cos⁡θsin⁡θ=(1+cos⁡θ)(1−cos⁡θ)sin⁡θ(1−cos⁡θ)=1−cos⁡2θsin⁡θ(1−cos⁡θ)=sin⁡2θsin⁡θ(1−cos⁡θ)=sin⁡θ1−cos⁡θ.\frac{1 + \cos\theta}{\sin\theta} = \frac{(1 + \cos\theta)(1 - \cos\theta)}{\sin\theta(1 - \cos\theta)} = \frac{1 - \cos^2\theta}{\sin\theta(1 - \cos\theta)} = \frac{\sin^2\theta}{\sin\theta(1 - \cos\theta)} = \frac{\sin\theta}{1 - \cos\theta}.

So the slopes are equal. (When sin⁡θ=0\sin\theta = 0, both the normal and the tangent to curve (2) are vertical, corresponding to the cusps at θ=0\theta = 0 and θ=π\theta = \pi.)

Conclusion: The normal to curve (1) at parameter θ\theta passes through P2P_2 on curve (2) and has the same slope as the tangent to curve (2) at P2P_2. Therefore the normal to curve (1) is a tangent to curve (2). ■\quad\blacksquare


Topic: 不等式与微积分 (Inequalities & Calculus)  |  Difficulty: Challenging  |  Marks: 20

7 Let f(x)=tan⁡x−x,g(x)=2−2cos⁡x−xsin⁡x,h(x)=2x+xcos⁡2x−32sin⁡2x,F(x)=x(cos⁡x)1/3sin⁡x.\begin{aligned} f(x) &= \tan x - x, \\ g(x) &= 2 - 2 \cos x - x \sin x, \\ h(x) &= 2x + x \cos 2x - \frac{3}{2} \sin 2x, \\ F(x) &= \frac{x(\cos x)^{1/3}}{\sin x}. \end{aligned}

(i) By considering f(0)f(0) and f′(x)f'(x), show that f(x)>0f(x) > 0 for 0<x<π/20 < x < \pi/2.

(ii) Show similarly that g(x)>0g(x) > 0 for 0<x<π/20 < x < \pi/2.

(iii) Show that h(x)>0h(x) > 0 for 0<x<π/40 < x < \pi/4, and hence that

x(sin⁡2x+3cos⁡2x)−3sin⁡xcos⁡x>0x(\sin^2 x + 3 \cos^2 x) - 3 \sin x \cos x > 0

for 0<x<π/40 < x < \pi/4.

(iv) By considering F′(x)F(x)\frac{F'(x)}{F(x)}, show that F′(x)<0F'(x) < 0 for 0<x<π/40 < x < \pi/4.

Model Solution

Part (i)

We have f(x)=tan⁡x−xf(x) = \tan x - x, so f(0)=tan⁡0−0=0f(0) = \tan 0 - 0 = 0.

Differentiating:

f′(x)=sec⁡2x−1=tan⁡2x.f'(x) = \sec^2 x - 1 = \tan^2 x.

For 0<x<π/20 < x < \pi/2, we have tan⁡x>0\tan x > 0, so f′(x)=tan⁡2x>0f'(x) = \tan^2 x > 0.

Since f(0)=0f(0) = 0 and f′(x)>0f'(x) > 0 for 0<x<π/20 < x < \pi/2, the function ff is strictly increasing on [0,π/2)[0, \pi/2). Therefore f(x)>f(0)=0f(x) > f(0) = 0 for 0<x<π/20 < x < \pi/2. ■\blacksquare

Part (ii)

We have g(x)=2−2cos⁡x−xsin⁡xg(x) = 2 - 2\cos x - x\sin x, so g(0)=2−2−0=0g(0) = 2 - 2 - 0 = 0.

Differentiating:

g′(x)=2sin⁡x−sin⁡x−xcos⁡x=sin⁡x−xcos⁡x.g'(x) = 2\sin x - \sin x - x\cos x = \sin x - x\cos x.

At x=0x = 0: g′(0)=0−0=0g'(0) = 0 - 0 = 0.

Differentiating again:

g′′(x)=cos⁡x−(cos⁡x−xsin⁡x)=xsin⁡x.g''(x) = \cos x - (\cos x - x\sin x) = x\sin x.

For 0<x<π/20 < x < \pi/2, we have x>0x > 0 and sin⁡x>0\sin x > 0, so g′′(x)=xsin⁡x>0g''(x) = x\sin x > 0.

Since g′′(x)>0g''(x) > 0 for 0<x<π/20 < x < \pi/2 and g′(0)=0g'(0) = 0, the function g′g' is strictly increasing on [0,π/2)[0, \pi/2), so g′(x)>g′(0)=0g'(x) > g'(0) = 0 for 0<x<π/20 < x < \pi/2.

Since g′(x)>0g'(x) > 0 for 0<x<π/20 < x < \pi/2 and g(0)=0g(0) = 0, the function gg is strictly increasing on [0,π/2)[0, \pi/2), so g(x)>g(0)=0g(x) > g(0) = 0 for 0<x<π/20 < x < \pi/2. ■\blacksquare

Part (iii)

We have h(x)=2x+xcos⁡2x−32sin⁡2xh(x) = 2x + x\cos 2x - \tfrac{3}{2}\sin 2x, so h(0)=0+0−0=0h(0) = 0 + 0 - 0 = 0.

Differentiating:

h′(x)=2+cos⁡2x−2xsin⁡2x−3cos⁡2x=2−2cos⁡2x−2xsin⁡2x.h'(x) = 2 + \cos 2x - 2x\sin 2x - 3\cos 2x = 2 - 2\cos 2x - 2x\sin 2x.

At x=0x = 0: h′(0)=2−2−0=0h'(0) = 2 - 2 - 0 = 0.

Note that h′(x)=g(2x)h'(x) = g(2x) where gg is the function from part (ii). From part (ii), g(t)>0g(t) > 0 for 0<t<π/20 < t < \pi/2, so for 0<2x<π/20 < 2x < \pi/2, i.e.\ 0<x<π/40 < x < \pi/4, we have h′(x)=g(2x)>0h'(x) = g(2x) > 0.

Since h′(x)>0h'(x) > 0 for 0<x<π/40 < x < \pi/4 and h(0)=0h(0) = 0, the function hh is strictly increasing on [0,π/4)[0, \pi/4), so h(x)>h(0)=0h(x) > h(0) = 0 for 0<x<π/40 < x < \pi/4. ■\blacksquare

For the deduction, we need to show

x(sin⁡2x+3cos⁡2x)−3sin⁡xcos⁡x>0for 0<x<π/4.x(\sin^2 x + 3\cos^2 x) - 3\sin x\cos x > 0 \qquad \text{for } 0 < x < \pi/4.

Using the double-angle identities sin⁡xcos⁡x=12sin⁡2x\sin x\cos x = \tfrac{1}{2}\sin 2x and cos⁡2x=12(1+cos⁡2x)\cos^2 x = \tfrac{1}{2}(1 + \cos 2x):

sin⁡2x+3cos⁡2x=1+2cos⁡2x=1+(1+cos⁡2x)=2+cos⁡2x.\sin^2 x + 3\cos^2 x = 1 + 2\cos^2 x = 1 + (1 + \cos 2x) = 2 + \cos 2x.

So the left-hand side becomes:

x(2+cos⁡2x)−32sin⁡2x=2x+xcos⁡2x−32sin⁡2x=h(x).x(2 + \cos 2x) - \tfrac{3}{2}\sin 2x = 2x + x\cos 2x - \tfrac{3}{2}\sin 2x = h(x).

Since we have shown h(x)>0h(x) > 0 for 0<x<π/40 < x < \pi/4, the inequality follows immediately. ■\blacksquare

Part (iv)

We have F(x)=x(cos⁡x)1/3sin⁡xF(x) = \dfrac{x(\cos x)^{1/3}}{\sin x}, which is positive for 0<x<π/40 < x < \pi/4.

Taking logarithms:

ln⁡F(x)=ln⁡x+13ln⁡(cos⁡x)−ln⁡(sin⁡x).\ln F(x) = \ln x + \tfrac{1}{3}\ln(\cos x) - \ln(\sin x).

Differentiating:

F′(x)F(x)=1x+13⋅−sin⁡xcos⁡x−cos⁡xsin⁡x=1x−13tan⁡x−cot⁡x.\frac{F'(x)}{F(x)} = \frac{1}{x} + \frac{1}{3} \cdot \frac{-\sin x}{\cos x} - \frac{\cos x}{\sin x} = \frac{1}{x} - \frac{1}{3}\tan x - \cot x.

To show F′(x)<0F'(x) < 0, since F(x)>0F(x) > 0 it suffices to show F′(x)F(x)<0\dfrac{F'(x)}{F(x)} < 0, i.e.

1x<13tan⁡x+cot⁡x.\frac{1}{x} < \frac{1}{3}\tan x + \cot x.

Multiplying both sides by 3x>03x > 0:

3<xtan⁡x+3xcot⁡x=xsin⁡xcos⁡x+3xcos⁡xsin⁡x=xsin⁡2x+3xcos⁡2xsin⁡xcos⁡x=x(sin⁡2x+3cos⁡2x)sin⁡xcos⁡x.3 < x\tan x + 3x\cot x = \frac{x\sin x}{\cos x} + \frac{3x\cos x}{\sin x} = \frac{x\sin^2 x + 3x\cos^2 x}{\sin x\cos x} = \frac{x(\sin^2 x + 3\cos^2 x)}{\sin x\cos x}.

Multiplying both sides by sin⁡xcos⁡x>0\sin x\cos x > 0:

3sin⁡xcos⁡x<x(sin⁡2x+3cos⁡2x),3\sin x\cos x < x(\sin^2 x + 3\cos^2 x),

which is exactly the inequality established in part (iii). Therefore F′(x)F(x)<0\dfrac{F'(x)}{F(x)} < 0, and since F(x)>0F(x) > 0 for 0<x<π/40 < x < \pi/4, we conclude F′(x)<0F'(x) < 0 for 0<x<π/40 < x < \pi/4. ■\blacksquare


Topic: 向量几何 (Vector Geometry)  |  Difficulty: Challenging  |  Marks: 20

8 Points A,B,CA, B, C in three dimensions have coordinate vectors a, b, c, respectively. Show that the lines joining the vertices of the triangle ABCABC to the mid-points of the opposite sides meet at a point RR.

PP is a point which is not in the plane ABCABC. Lines are drawn through the mid-points of BCBC, CACA and ABAB parallel to PAPA, PBPB and PCPC respectively. Write down the vector equations of the lines and show by inspection that these lines meet at a common point QQ.

Prove further that the line PQPQ meets the plane ABCABC at RR.

Model Solution

Medians meeting at a point RR

The mid-point of BCBC is b+c2\frac{\mathbf{b}+\mathbf{c}}{2}, so the line from AA to this mid-point has equation

r=a+λ ⁣(b+c2−a)=(1−λ) a+λ2 b+λ2 c.(I)\mathbf{r} = \mathbf{a} + \lambda\!\left(\frac{\mathbf{b}+\mathbf{c}}{2} - \mathbf{a}\right) = (1-\lambda)\,\mathbf{a} + \frac{\lambda}{2}\,\mathbf{b} + \frac{\lambda}{2}\,\mathbf{c}. \qquad \text{(I)}

The mid-point of ACAC is a+c2\frac{\mathbf{a}+\mathbf{c}}{2}, so the line from BB to this mid-point has equation

r=b+μ ⁣(a+c2−b)=μ2 a+(1−μ) b+μ2 c.(II)\mathbf{r} = \mathbf{b} + \mu\!\left(\frac{\mathbf{a}+\mathbf{c}}{2} - \mathbf{b}\right) = \frac{\mu}{2}\,\mathbf{a} + (1-\mu)\,\mathbf{b} + \frac{\mu}{2}\,\mathbf{c}. \qquad \text{(II)}

At an intersection, equating coefficients of a\mathbf{a}, b\mathbf{b}, c\mathbf{c} (since AA, BB, CC are not collinear):

1−λ=μ2,λ2=1−μ,λ2=μ2.1-\lambda = \frac{\mu}{2}, \qquad \frac{\lambda}{2} = 1-\mu, \qquad \frac{\lambda}{2} = \frac{\mu}{2}.

From the third equation, λ=μ\lambda = \mu. Substituting into the first: 1−λ=λ/21 - \lambda = \lambda/2, giving λ=2/3\lambda = 2/3. We verify the second equation: 13=1−23=13\frac{1}{3} = 1 - \frac{2}{3} = \frac{1}{3}. ✓\checkmark

Substituting λ=2/3\lambda = 2/3 into (I):

r=13 a+13 b+13 c=a+b+c3.\mathbf{r} = \frac{1}{3}\,\mathbf{a} + \frac{1}{3}\,\mathbf{b} + \frac{1}{3}\,\mathbf{c} = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}}{3}.

The third median (from CC to the mid-point of ABAB) has equation r=(1−ν) c+ν2 a+ν2 b\mathbf{r} = (1-\nu)\,\mathbf{c} + \frac{\nu}{2}\,\mathbf{a} + \frac{\nu}{2}\,\mathbf{b}. Setting ν=2/3\nu = 2/3 gives r=a+b+c3\mathbf{r} = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}}{3}, confirming all three medians meet at

R=a+b+c3.■R = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}}{3}. \qquad \blacksquare

Lines through mid-points parallel to PAPA, PBPB, PCPC

The line through the mid-point of BCBC parallel to PAPA has direction a−p\mathbf{a} - \mathbf{p}:

ℓ1:r=b+c2+λ(a−p).(III)\ell_1:\quad \mathbf{r} = \frac{\mathbf{b}+\mathbf{c}}{2} + \lambda(\mathbf{a} - \mathbf{p}). \qquad \text{(III)}

The line through the mid-point of CACA parallel to PBPB has direction b−p\mathbf{b} - \mathbf{p}:

ℓ2:r=a+c2+μ(b−p).(IV)\ell_2:\quad \mathbf{r} = \frac{\mathbf{a}+\mathbf{c}}{2} + \mu(\mathbf{b} - \mathbf{p}). \qquad \text{(IV)}

The line through the mid-point of ABAB parallel to PCPC has direction c−p\mathbf{c} - \mathbf{p}:

ℓ3:r=a+b2+ν(c−p).(V)\ell_3:\quad \mathbf{r} = \frac{\mathbf{a}+\mathbf{b}}{2} + \nu(\mathbf{c} - \mathbf{p}). \qquad \text{(V)}

We can find a common point by inspection. Setting λ=1/2\lambda = 1/2 in (III):

r=b+c2+12(a−p)=a+b+c−p2.\mathbf{r} = \frac{\mathbf{b}+\mathbf{c}}{2} + \frac{1}{2}(\mathbf{a}-\mathbf{p}) = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-\mathbf{p}}{2}.

Setting μ=1/2\mu = 1/2 in (IV):

r=a+c2+12(b−p)=a+b+c−p2.\mathbf{r} = \frac{\mathbf{a}+\mathbf{c}}{2} + \frac{1}{2}(\mathbf{b}-\mathbf{p}) = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-\mathbf{p}}{2}.

Setting ν=1/2\nu = 1/2 in (V):

r=a+b2+12(c−p)=a+b+c−p2.\mathbf{r} = \frac{\mathbf{a}+\mathbf{b}}{2} + \frac{1}{2}(\mathbf{c}-\mathbf{p}) = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-\mathbf{p}}{2}.

All three give the same result, so all three lines meet at

Q=a+b+c−p2.■Q = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-\mathbf{p}}{2}. \qquad \blacksquare

Line PQPQ meets plane ABCABC at RR

The line PQPQ has equation

r=p+t ⁣(a+b+c−p2−p)=p+t⋅a+b+c−3p2.\mathbf{r} = \mathbf{p} + t\!\left(\frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-\mathbf{p}}{2} - \mathbf{p}\right) = \mathbf{p} + t\cdot\frac{\mathbf{a}+\mathbf{b}+\mathbf{c}-3\mathbf{p}}{2}.

A point on this line is

r=(1−3t2)p+t2 (a+b+c).\mathbf{r} = \left(1 - \frac{3t}{2}\right)\mathbf{p} + \frac{t}{2}\,(\mathbf{a}+\mathbf{b}+\mathbf{c}).

For PQPQ to meet the plane ABCABC, the coefficient of p\mathbf{p} must be zero (since PP is not in the plane, and any point in the plane is a combination of a\mathbf{a}, b\mathbf{b}, c\mathbf{c} only). Setting 1−3t2=01 - \frac{3t}{2} = 0 gives t=23t = \frac{2}{3}.

Substituting:

r=2/32 (a+b+c)=a+b+c3=R.\mathbf{r} = \frac{2/3}{2}\,(\mathbf{a}+\mathbf{b}+\mathbf{c}) = \frac{\mathbf{a}+\mathbf{b}+\mathbf{c}}{3} = R.

Therefore the line PQPQ meets the plane ABCABC at the point R=a+b+c3R = \dfrac{\mathbf{a}+\mathbf{b}+\mathbf{c}}{3}. ■\blacksquare