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STEP2 2005 -- Pure Mathematics

Exam: STEP2  |  Year: 2005  |  Questions: Q1—Q8  |  Total marks per question: 20

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

QTopicDifficultyKey Techniques
1微积分 Calculus(求导与多项式构造)Standard乘积法则求导,提取公因式,构造微分方程求多项式
2数论 Number Theory(Euler totient 函数)Standard素因数分解,构造反例,代数恒等式
3微积分 Calculus(定积分与不等式)Challenging分部积分,三角恒等式降幂,不等式放缩
4三角函数 Trigonometry(反三角函数恒等式)Challenging反正切加法公式,代数化简,参数赋值验证
5几何 Geometry(圆与三角形)Challenging切线长相等性质,配方法求最值,面积比计算
6幂级数 Power SeriesChallenging二项式级数展开,代入法求和,逐项微分
7向量与三维几何 Vectors and 3D GeometryChallenging位置向量几何描述,标量积求夹角,三角不等式求时间区间
8微分方程与曲线描绘 Differential Equations and Curve SketchingChallenging分离变量法,换元积分,渐近展开,曲线渐近行为分析

Topic: 微积分 Calculus(求导与多项式构造)  |  Difficulty: Standard  |  Marks: 20

1 Find the three values of xx for which the derivative of x2e−x2x^2e^{-x^2} is zero.

Given that aa and bb are distinct positive numbers, find a polynomial P(x)P(x) such that the derivative of P(x)e−x2P(x)e^{-x^2} is zero for x=0x = 0, x=±ax = \pm a and x=±bx = \pm b, but for no other values of xx.

Hint

Differentiation leads to f’(x) = 2xe^{-x^2} - 2x^3e^{-x^2}. Since e^{-x^2} is not equal to 0 for any finite x then f’(x) = 0 implies x - x^3 = 0, so x = 0, 1, -1.

For the rest of the question, observe first that P’(x) - 2xP(x) = x(x^2 - a^2)(x^2 - b^2) () within a multiplicative non-zero constant. Thus P(x) can take the form -x^4/2 + px^2 + q and hence substitution into () plus equating the coefficient of x^2 and constant terms leads to a possible result for P(x).

A similar argument based on setting P(x) = sum c_i x^i is feasible, but it involves more working and so is correspondingly more error prone.

Alternatively, one can multiply (*) by e^{-x^2} and then integrate with respect to x to obtain P(x)e^{-x^2} = integral of x(x^2 - a^2)(x^2 - b^2)e^{-x^2} dx. From integral of xe^{-x^2} dx = -(1/2)e^{-x^2} the integrals of x^3e^{-x^2} dx and x^5e^{-x^2} dx can be evaluated by use of the integration by parts rule. It then only remains to cancel out the factor e^{-x^2} to obtain P(x) = -x^4/2 + (a^2/2 + b^2/2 - 1)x^2 - 1 + a^2/2 + b^2/2 - a^2b^2/2.

Model Solution

Part 1: Find the three values of xx for which the derivative of x2e−x2x^2 e^{-x^2} is zero.

Let f(x)=x2e−x2f(x) = x^2 e^{-x^2}. By the product rule:

f′(x)=2x⋅e−x2+x2⋅(−2x)e−x2=2x e−x2−2x3e−x2=2x e−x2(1−x2).f'(x) = 2x \cdot e^{-x^2} + x^2 \cdot (-2x)e^{-x^2} = 2x\,e^{-x^2} - 2x^3 e^{-x^2} = 2x\,e^{-x^2}(1 - x^2) \text{.}

Since e−x2>0e^{-x^2} > 0 for all real xx, the derivative is zero if and only if:

2x(1−x2)=0,2x(1 - x^2) = 0 \text{,}

which gives x=0x = 0 or x2=1x^2 = 1. Hence the three values are:

x=0,x=1,x=−1.□x = 0, \quad x = 1, \quad x = -1 \text{.} \qquad \square

Part 2: Find a polynomial P(x)P(x) such that ddx ⁣[P(x)e−x2]=0\frac{d}{dx}\!\left[P(x)e^{-x^2}\right] = 0 at x=0,±a,±bx = 0, \pm a, \pm b only.

We compute:

ddx ⁣[P(x)e−x2]=[P′(x)−2xP(x)]e−x2.\frac{d}{dx}\!\left[P(x)e^{-x^2}\right] = \left[P'(x) - 2xP(x)\right]e^{-x^2} \text{.}

Since e−x2≠0e^{-x^2} \neq 0, this is zero if and only if P′(x)−2xP(x)=0P'(x) - 2xP(x) = 0. We need this to hold at exactly x=0,±a,±bx = 0, \pm a, \pm b, so we require:

P′(x)−2xP(x)=kx(x2−a2)(x2−b2)(*)P'(x) - 2xP(x) = kx(x^2 - a^2)(x^2 - b^2) \qquad \text{(*)}

for some non-zero constant kk. The right side is a degree 55 polynomial, so PP must have degree 44. Since the right side is an odd function, we try P(x)=αx4+βx2+γP(x) = \alpha x^4 + \beta x^2 + \gamma (an even polynomial). Then:

P′(x)−2xP(x)=(4αx3+2βx)−2x(αx4+βx2+γ)=−2αx5+(4α−2β)x3+(2β−2γ)x.P'(x) - 2xP(x) = (4\alpha x^3 + 2\beta x) - 2x(\alpha x^4 + \beta x^2 + \gamma) = -2\alpha x^5 + (4\alpha - 2\beta)x^3 + (2\beta - 2\gamma)x \text{.}

Expanding the right side of (∗)(*):

kx(x2−a2)(x2−b2)=kx5−k(a2+b2)x3+ka2b2x.kx(x^2 - a^2)(x^2 - b^2) = kx^5 - k(a^2 + b^2)x^3 + ka^2b^2 x \text{.}

Matching coefficients of each power of xx:

x5x^5: −2α=k-2\alpha = k, so α=−k2\alpha = -\dfrac{k}{2}.

x3x^3: 4α−2β=−k(a2+b2)4\alpha - 2\beta = -k(a^2 + b^2), so β=2α+k(a2+b2)2=k(a2+b2−2)2\beta = 2\alpha + \dfrac{k(a^2 + b^2)}{2} = \dfrac{k(a^2 + b^2 - 2)}{2}.

x1x^1: 2β−2γ=ka2b22\beta - 2\gamma = ka^2b^2, so γ=β−ka2b22=k(a2+b2−a2b2−2)2\gamma = \beta - \dfrac{ka^2b^2}{2} = \dfrac{k(a^2 + b^2 - a^2b^2 - 2)}{2}.

Setting k=−2k = -2 for a clean leading coefficient:

P(x)=x4−(a2+b2−2)x2+(a2+b2−a2b2−2).P(x) = x^4 - (a^2 + b^2 - 2)x^2 + (a^2 + b^2 - a^2b^2 - 2) \text{.}

Verification. We check (∗)(*) with k=−2k = -2:

P′(x)−2xP(x)=4x3−2(a2+b2−2)x−2x5+2(a2+b2−2)x3−2(a2+b2−a2b2−2)xP'(x) - 2xP(x) = 4x^3 - 2(a^2 + b^2 - 2)x - 2x^5 + 2(a^2 + b^2 - 2)x^3 - 2(a^2 + b^2 - a^2b^2 - 2)x

=−2x5+2(a2+b2)x3−2a2b2x=−2x(x2−a2)(x2−b2).= -2x^5 + 2(a^2 + b^2)x^3 - 2a^2b^2 x = -2x(x^2 - a^2)(x^2 - b^2) \text{.}

Since aa and bb are distinct positive numbers, the five zeros x=0,±a,±bx = 0, \pm a, \pm b are all distinct, and a degree 55 polynomial has at most 55 real zeros. Hence ddx[P(x)e−x2]=0\frac{d}{dx}[P(x)e^{-x^2}] = 0 at exactly x=0,±a,±bx = 0, \pm a, \pm b. □\qquad \square

Note: Any non-zero scalar multiple of P(x)P(x) also satisfies the requirements (since the equation P′−2xP=kx(x2−a2)(x2−b2)P' - 2xP = kx(x^2-a^2)(x^2-b^2) holds for any non-zero kk). The choice k=−2k = -2 gives the simplest integer coefficients.


Topic: 数论 Number Theory(Euler totient 函数)  |  Difficulty: Standard  |  Marks: 20

2 For any positive integer NN, the function f(N)f(N) is defined by

f(N)=N(1−1p1)(1−1p2)⋯(1−1pk)f(N) = N \left( 1 - \frac{1}{p_1} \right) \left( 1 - \frac{1}{p_2} \right) \cdots \left( 1 - \frac{1}{p_k} \right)

where p1,p2,…,pkp_1, p_2, \dots, p_k are the only prime numbers that are factors of NN. Thus f(80)=80(1−12)(1−15)f(80) = 80(1 - \frac{1}{2})(1 - \frac{1}{5}).

(a) (i) Evaluate f(12)f(12) and f(180)f(180).

(ii) Show that f(N)f(N) is an integer for all NN.

(b) Prove, or disprove by means of a counterexample, each of the following:

(i) f(m)f(n)=f(mn)f(m)f(n) = f(mn);

(ii) f(p)f(q)=f(pq)f(p)f(q) = f(pq) if pp and qq are distinct prime numbers;

(iii) f(p)f(q)=f(pq)f(p)f(q) = f(pq) only if pp and qq are distinct prime numbers.

(c) Find a positive integer mm and a prime number pp such that f(pm)=146410f(p^m) = 146410.

Hint

(a) (i) Following the definition of f(N), it is immediate that f(12) = 12(1 - 1/2)(1 - 1/3) = 4, and f(180) = 180(1 - 1/2)(1 - 1/3)(1 - 1/5) = 48.

(ii) The result may seem obvious but care must be taken in order to construct a complete proof. For example, N = p_1^{alpha_1} … p_k^{alpha_k} implies f(N) = p_1^{alpha_1-1} … p_k^{alpha_k-1}(p_1 - 1) … (p_k - 1). Thus as p_i is a positive integer and alpha_i - 1 is a non-negative integer for 1 <= i <= k, then f(N) is an integer.

(b) In each of (i), (ii), (iii), the conclusion must be made clear.

(i) As f(3)f(9) = 2 x 6 = 12 is not equal to f(27) = 18, then the statement is false.

(ii) For any two primes p and q, f(p)f(q) = p(1 - 1/p)q(1 - 1/q) = pq(1 - 1/p)(1 - 1/q) = f(pq). Hence the statement is true.

(iii) Consider f(5) = 4, f(6) = 2, f(30) = 8 = 2 x 4. Then as 6 is not a prime it is clear that the statement is false.

(c) Start with p^{m-1}(p - 1) = 146410, then without difficulty it will be found that p = 11 and m = 5 (not 4).

Model Solution

Part (a)(i) Evaluate f(12)f(12) and f(180)f(180).

For N=12=22×3N = 12 = 2^2 \times 3, the prime factors are 22 and 33:

f(12)=12(1−12) ⁣(1−13)=12⋅12⋅23=4.f(12) = 12\left(1 - \frac{1}{2}\right)\!\left(1 - \frac{1}{3}\right) = 12 \cdot \frac{1}{2} \cdot \frac{2}{3} = 4 \text{.}

For N=180=22×32×5N = 180 = 2^2 \times 3^2 \times 5, the prime factors are 22, 33, and 55:

f(180)=180(1−12) ⁣(1−13) ⁣(1−15)=180⋅12⋅23⋅45=48.f(180) = 180\left(1 - \frac{1}{2}\right)\!\left(1 - \frac{1}{3}\right)\!\left(1 - \frac{1}{5}\right) = 180 \cdot \frac{1}{2} \cdot \frac{2}{3} \cdot \frac{4}{5} = 48 \text{.}

Part (a)(ii) Show that f(N)f(N) is an integer for all NN.

Write N=p1α1p2α2⋯pkαkN = p_1^{\alpha_1} p_2^{\alpha_2} \cdots p_k^{\alpha_k} where p1,p2,…,pkp_1, p_2, \dots, p_k are distinct primes and αi⩾1\alpha_i \geqslant 1. Then:

f(N)=p1α1p2α2⋯pkαk⋅(1−1p1) ⁣(1−1p2)⋯(1−1pk)f(N) = p_1^{\alpha_1} p_2^{\alpha_2} \cdots p_k^{\alpha_k} \cdot \left(1 - \frac{1}{p_1}\right)\!\left(1 - \frac{1}{p_2}\right)\cdots\left(1 - \frac{1}{p_k}\right)

=p1α1p2α2⋯pkαk⋅p1−1p1⋅p2−1p2⋯pk−1pk= p_1^{\alpha_1} p_2^{\alpha_2} \cdots p_k^{\alpha_k} \cdot \frac{p_1 - 1}{p_1} \cdot \frac{p_2 - 1}{p_2} \cdots \frac{p_k - 1}{p_k}

=p1α1−1p2α2−1⋯pkαk−1⋅(p1−1)(p2−1)⋯(pk−1).= p_1^{\alpha_1 - 1} p_2^{\alpha_2 - 1} \cdots p_k^{\alpha_k - 1} \cdot (p_1 - 1)(p_2 - 1) \cdots (p_k - 1) \text{.}

Since each αi⩾1\alpha_i \geqslant 1, every exponent αi−1⩾0\alpha_i - 1 \geqslant 0, and each pi−1⩾1p_i - 1 \geqslant 1. All factors are positive integers, so f(N)f(N) is a positive integer. □\qquad \square

Part (b)(i) Disprove: f(m)f(n)=f(mn)f(m)f(n) = f(mn) for all m,nm, n.

Counterexample. Take m=3m = 3, n=9n = 9. Then mn=27=33mn = 27 = 3^3.

f(3)=3(1−13)=2,f(9)=9(1−13)=6,f(27)=27(1−13)=18.f(3) = 3\left(1 - \frac{1}{3}\right) = 2, \qquad f(9) = 9\left(1 - \frac{1}{3}\right) = 6, \qquad f(27) = 27\left(1 - \frac{1}{3}\right) = 18 \text{.}

Since f(3)f(9)=2×6=12≠18=f(27)f(3)f(9) = 2 \times 6 = 12 \neq 18 = f(27), the statement is false. □\qquad \square

Part (b)(ii) Prove: f(p)f(q)=f(pq)f(p)f(q) = f(pq) if pp and qq are distinct primes.

Since pp and qq are distinct primes, pqpq has prime factors pp and qq:

f(pq)=pq(1−1p) ⁣(1−1q)=p(1−1p)⋅q(1−1q)=f(p)⋅f(q).f(pq) = pq\left(1 - \frac{1}{p}\right)\!\left(1 - \frac{1}{q}\right) = p\left(1 - \frac{1}{p}\right) \cdot q\left(1 - \frac{1}{q}\right) = f(p) \cdot f(q) \text{.}

The statement is true. □\qquad \square

Part (b)(iii) Disprove: f(p)f(q)=f(pq)f(p)f(q) = f(pq) only if pp and qq are distinct primes.

We need a counterexample where f(m)f(n)=f(mn)f(m)f(n) = f(mn) but at least one of m,nm, n is not prime.

Counterexample. Take m=5m = 5 (prime), n=6=2×3n = 6 = 2 \times 3 (not prime). Then mn=30=2×3×5mn = 30 = 2 \times 3 \times 5.

f(5)=5⋅45=4,f(6)=6⋅12⋅23=2,f(30)=30⋅12⋅23⋅45=8.f(5) = 5 \cdot \frac{4}{5} = 4, \qquad f(6) = 6 \cdot \frac{1}{2} \cdot \frac{2}{3} = 2, \qquad f(30) = 30 \cdot \frac{1}{2} \cdot \frac{2}{3} \cdot \frac{4}{5} = 8 \text{.}

Since f(5)f(6)=4×2=8=f(30)f(5)f(6) = 4 \times 2 = 8 = f(30), yet 66 is not prime, the statement is false. □\qquad \square

Part (c) Find mm and prime pp such that f(pm)=146410f(p^m) = 146410.

For a prime power pmp^m, the only prime factor is pp, so:

f(pm)=pm(1−1p)=pm−1(p−1)=146410.f(p^m) = p^m\left(1 - \frac{1}{p}\right) = p^{m-1}(p - 1) = 146410 \text{.}

We factor 146410146410: since 146410=10×14641146410 = 10 \times 14641 and 14641=11414641 = 11^4, we get 146410=2×5×114146410 = 2 \times 5 \times 11^4.

Since pp must be prime and p−1p - 1 must divide 146410146410, we try p=11p = 11:

pm−1(p−1)=11m−1×10=146410  ⟹  11m−1=14641=114  ⟹  m=5.p^{m-1}(p - 1) = 11^{m-1} \times 10 = 146410 \implies 11^{m-1} = 14641 = 11^4 \implies m = 5 \text{.}

Verification: f(115)=114×(11−1)=14641×10=146410f(11^5) = 11^4 \times (11 - 1) = 14641 \times 10 = 146410. ✓\checkmark

Therefore p=11p = 11 and m=5m = 5. □\qquad \square

Note: No other solution exists. If p=2p = 2, then p−1=1p - 1 = 1 and pm−1=146410p^{m-1} = 146410, but 146410146410 is not a power of 22. If p=5p = 5, then p−1=4p - 1 = 4 and pm−1=36602.5p^{m-1} = 36602.5, which is not an integer. For p>11p > 11, we would need pm−1(p−1)=146410p^{m-1}(p-1) = 146410, but p−1⩾12p - 1 \geqslant 12 would require pm−1⩽12200p^{m-1} \leqslant 12200, and checking small values of mm yields no prime solutions.


Topic: 微积分 Calculus(定积分与不等式)  |  Difficulty: Challenging  |  Marks: 20

3 Give a sketch, for 0⩽x⩽π/20 \leqslant x \leqslant \pi/2, of the curve

y=(sin⁡x−xcos⁡x) ,y = (\sin x - x \cos x) \text{ ,}

and show that 0⩽y⩽10 \leqslant y \leqslant 1.

Show that:

(i) ∫0π/2y dx=2−π2\int_0^{\pi/2} y \, dx = 2 - \frac{\pi}{2} ;

(ii) ∫0π/2y2 dx=π348−π8\int_0^{\pi/2} y^2 \, dx = \frac{\pi^3}{48} - \frac{\pi}{8} .

Deduce that π3+18π<96\pi^3 + 18\pi < 96.

Hint

Here dy/dx = x sin x which is zero at x = 0 and is positive for 0 < x <= pi/2. A further differentiation will show that d^2y/dx^2 = 0 at x = 0 and positive for 0 < x <= pi/2. Also, as y(0) = 0 and y(pi/2) = 1, then 0 <= y <= 1 for 0 <= x <= pi/2, and the sketch can now be completed consistently with the above conclusions.

(i) integral from 0 to pi/2 of sin x dx = 1 and use of the integration by parts rule will show that integral from 0 to pi/2 of x cos x dx = pi/2 - 1. The displayed result for integral from 0 to pi/2 of y dx then follows immediately.

(ii) Start with integral from 0 to pi/2 of y^2 dx = integral of sin^2 x dx - integral of x sin 2x dx + integral of x^2 cos^2 x dx.

Next, express sin^2 x and cos^2 x in terms of cos 2x so that now there are only two essentially different integrals involving trigonometric terms, namely, integral of x sin 2x dx and integral of x^2 cos 2x dx. The second of these can be obtained from the first, again by application of the integration by parts rule. A correct application of this rule to the first integral and the careful collection of terms will lead to the displayed result.

For the final result, begin with the observation that y^2 < y for 0 < x < pi/2. From this, it is immediate that integral of y^2 dx < integral of y dx and hence that pi^3/48 - pi/8 < 2 - pi/2. The final displayed result can then be obtained without difficulty.

Model Solution

We have y=sin⁡x−xcos⁡xy = \sin x - x\cos x for 0⩽x⩽π/20 \leqslant x \leqslant \pi/2.

Derivative. By the product rule,

dydx=cos⁡x−(cos⁡x−xsin⁡x)=xsin⁡x.\frac{dy}{dx} = \cos x - (\cos x - x\sin x) = x\sin x \text{.}

For 0<x⩽π/20 < x \leqslant \pi/2, we have x>0x > 0 and sin⁡x>0\sin x > 0, so dydx>0\frac{dy}{dx} > 0. At x=0x = 0, dydx=0\frac{dy}{dx} = 0. Thus yy is non-decreasing on [0,π/2][0, \pi/2] with y(0)=sin⁡0−0⋅cos⁡0=0y(0) = \sin 0 - 0\cdot\cos 0 = 0 and y(π/2)=sin⁡(π/2)−π2cos⁡(π/2)=1y(\pi/2) = \sin(\pi/2) - \frac{\pi}{2}\cos(\pi/2) = 1. Since yy increases from 00 to 11, we have 0⩽y⩽10 \leqslant y \leqslant 1.

The second derivative is d2ydx2=sin⁡x+xcos⁡x\frac{d^2y}{dx^2} = \sin x + x\cos x, which is positive for 0<x⩽π/20 < x \leqslant \pi/2, so the curve is concave up throughout. The sketch shows a curve starting at the origin with zero gradient, increasing monotonically with increasing slope, reaching y=1y = 1 at x=π/2x = \pi/2.

Part (i)

∫0π/2y dx=∫0π/2sin⁡x dx−∫0π/2xcos⁡x dx.\int_0^{\pi/2} y\,dx = \int_0^{\pi/2} \sin x\,dx - \int_0^{\pi/2} x\cos x\,dx \text{.}

The first integral is ∫0π/2sin⁡x dx=[−cos⁡x]0π/2=0−(−1)=1\int_0^{\pi/2} \sin x\,dx = [-\cos x]_0^{\pi/2} = 0-(-1) = 1.

For the second integral, integrate by parts with u=xu = x, dv=cos⁡x dxdv = \cos x\,dx (so du=dxdu = dx, v=sin⁡xv = \sin x):

∫0π/2xcos⁡x dx=[xsin⁡x]0π/2−∫0π/2sin⁡x dx=π2−1.\int_0^{\pi/2} x\cos x\,dx = [x\sin x]_0^{\pi/2} - \int_0^{\pi/2} \sin x\,dx = \frac{\pi}{2} - 1 \text{.}

Therefore

∫0π/2y dx=1−(π2−1)=2−π2.□\int_0^{\pi/2} y\,dx = 1 - \left(\frac{\pi}{2} - 1\right) = 2 - \frac{\pi}{2} \text{.} \qquad \square

Part (ii) We expand y2y^2:

y2=sin⁡2x−2xsin⁡xcos⁡x+x2cos⁡2x=sin⁡2x−xsin⁡2x+x2cos⁡2x.y^2 = \sin^2 x - 2x\sin x\cos x + x^2\cos^2 x = \sin^2 x - x\sin 2x + x^2\cos^2 x \text{.}

Using sin⁡2x=1−cos⁡2x2\sin^2 x = \frac{1-\cos 2x}{2} and cos⁡2x=1+cos⁡2x2\cos^2 x = \frac{1+\cos 2x}{2}:

∫0π/2y2 dx=∫0π/21−cos⁡2x2 dx⏟I1−∫0π/2xsin⁡2x dx⏟I2+∫0π/2x2(1+cos⁡2x)2 dx⏟I3.\int_0^{\pi/2} y^2\,dx = \underbrace{\int_0^{\pi/2} \frac{1-\cos 2x}{2}\,dx}_{I_1} - \underbrace{\int_0^{\pi/2} x\sin 2x\,dx}_{I_2} + \underbrace{\int_0^{\pi/2} \frac{x^2(1+\cos 2x)}{2}\,dx}_{I_3} \text{.}

Evaluating I1I_1:

I1=12 ⁣[x−sin⁡2x2]0π/2=12⋅π2=π4.I_1 = \frac{1}{2}\!\left[x - \frac{\sin 2x}{2}\right]_0^{\pi/2} = \frac{1}{2}\cdot\frac{\pi}{2} = \frac{\pi}{4} \text{.}

Evaluating I2I_2: Integrate by parts with u=xu = x, dv=sin⁡2x dxdv = \sin 2x\,dx (so du=dxdu = dx, v=−cos⁡2x2v = -\frac{\cos 2x}{2}):

I2=[−xcos⁡2x2]0π/2+∫0π/2cos⁡2x2 dx=−π2⋅(−1)2+[sin⁡2x4]0π/2=π4+0=π4.I_2 = \left[-\frac{x\cos 2x}{2}\right]_0^{\pi/2} + \int_0^{\pi/2} \frac{\cos 2x}{2}\,dx = -\frac{\frac{\pi}{2}\cdot(-1)}{2} + \left[\frac{\sin 2x}{4}\right]_0^{\pi/2} = \frac{\pi}{4} + 0 = \frac{\pi}{4} \text{.}

Evaluating I3I_3:

I3=12∫0π/2x2 dx+12∫0π/2x2cos⁡2x dx=π348+12∫0π/2x2cos⁡2x dx.I_3 = \frac{1}{2}\int_0^{\pi/2} x^2\,dx + \frac{1}{2}\int_0^{\pi/2} x^2\cos 2x\,dx = \frac{\pi^3}{48} + \frac{1}{2}\int_0^{\pi/2} x^2\cos 2x\,dx \text{.}

For ∫0π/2x2cos⁡2x dx\int_0^{\pi/2} x^2\cos 2x\,dx, integrate by parts with u=x2u = x^2, dv=cos⁡2x dxdv = \cos 2x\,dx (so du=2x dxdu = 2x\,dx, v=sin⁡2x2v = \frac{\sin 2x}{2}):

∫0π/2x2cos⁡2x dx=[x2sin⁡2x2]0π/2−∫0π/2xsin⁡2x dx=0−I2=−π4.\int_0^{\pi/2} x^2\cos 2x\,dx = \left[\frac{x^2\sin 2x}{2}\right]_0^{\pi/2} - \int_0^{\pi/2} x\sin 2x\,dx = 0 - I_2 = -\frac{\pi}{4} \text{.}

Therefore I3=π348+12 ⁣(−π4)=π348−π8I_3 = \frac{\pi^3}{48} + \frac{1}{2}\!\left(-\frac{\pi}{4}\right) = \frac{\pi^3}{48} - \frac{\pi}{8}.

Combining:

∫0π/2y2 dx=I1−I2+I3=π4−π4+π348−π8=π348−π8.□\int_0^{\pi/2} y^2\,dx = I_1 - I_2 + I_3 = \frac{\pi}{4} - \frac{\pi}{4} + \frac{\pi^3}{48} - \frac{\pi}{8} = \frac{\pi^3}{48} - \frac{\pi}{8} \text{.} \qquad \square

Deduction. For 0<x<π/20 < x < \pi/2 we have 0<y<10 < y < 1, so y2<yy^2 < y. Integrating over [0,π/2][0, \pi/2]:

∫0π/2y2 dx<∫0π/2y dx\int_0^{\pi/2} y^2\,dx < \int_0^{\pi/2} y\,dx

π348−π8<2−π2\frac{\pi^3}{48} - \frac{\pi}{8} < 2 - \frac{\pi}{2}

Multiplying both sides by 4848:

π3−6π<96−24π\pi^3 - 6\pi < 96 - 24\pi

π3+18π<96.□\pi^3 + 18\pi < 96 \text{.} \qquad \square


Topic: 三角函数 Trigonometry(反三角函数恒等式)  |  Difficulty: Challenging  |  Marks: 20

4 The positive numbers aa, bb and cc satisfy bc=a2+1bc = a^2 + 1. Prove that

arctan⁡(1a+b)+arctan⁡(1a+c)=arctan⁡(1a).\arctan \left( \frac{1}{a+b} \right) + \arctan \left( \frac{1}{a+c} \right) = \arctan \left( \frac{1}{a} \right) .

The positive numbers p,q,r,s,t,up, q, r, s, t, u and vv satisfy

st=(p+q)2+1,uv=(p+r)2+1,qr=p2+1.st = (p + q)^2 + 1 , \quad uv = (p + r)^2 + 1 , \quad qr = p^2 + 1 .

Prove that

arctan⁡(1p+q+s)+arctan⁡(1p+q+t)+arctan⁡(1p+r+u)+arctan⁡(1p+r+v)=arctan⁡(1p).\arctan \left( \frac{1}{p + q + s} \right) + \arctan \left( \frac{1}{p + q + t} \right) + \arctan \left( \frac{1}{p + r + u} \right) + \arctan \left( \frac{1}{p + r + v} \right) = \arctan \left( \frac{1}{p} \right) .

Hence show that

arctan⁡(113)+arctan⁡(121)+arctan⁡(182)+arctan⁡(1187)=arctan⁡(17).\arctan \left( \frac{1}{13} \right) + \arctan \left( \frac{1}{21} \right) + \arctan \left( \frac{1}{82} \right) + \arctan \left( \frac{1}{187} \right) = \arctan \left( \frac{1}{7} \right) .

[Note that arctan⁡x\arctan x is another notation for tan⁡−1x\tan^{-1} x.]

Hint

The first two parts of this question depend on the identity tan^{-1} A + tan^{-1} B = tan^{-1}[(A + B)/(1 - AB)] which is simply another way of writing tan(alpha + beta) = [tan alpha + tan beta]/[1 - tan alpha tan beta].

In the second part, it follows from the data that

tan^{-1}[1/(p + q + s)] + tan^{-1}[1/(p + q + t)] = tan^{-1}[1/(p + q)]

and

tan^{-1}[1/(p + r + u)] + tan^{-1}[1/(p + r + v)] = tan^{-1}[1/(p + r)].

As also from the data,

tan^{-1}[1/(p + q)] + tan^{-1}[1/(p + r)] = tan^{-1}(1/p),

then the proof is complete.

For the final part, it is clear that p=7p = 7 and this leads to st=(7+q)2+1st = (7 + q)^2 + 1, uv=(7+r)2+1uv = (7 + r)^2 + 1, qr=50qr = 50. Pair the smaller targets with rr: from p+r+u=13p+r+u = 13 and p+r+v=21p+r+v = 21, we have r+u=6r+u = 6 and r+v=14r+v = 14, so (6−r)(14−r)=(7+r)2+1(6-r)(14-r) = (7+r)^2 + 1, which gives r=1r = 1, and hence u=5u = 5, v=13v = 13. Similarly, pairing the larger targets with qq gives q+s=75q+s = 75, q+t=180q+t = 180, so (75−q)(180−q)=(7+q)2+1(75-q)(180-q) = (7+q)^2 + 1, giving q=50q = 50, s=25s = 25, t=130t = 130.

The solution given above is not unique. Moreover, other plausible strategies may lead to incorrect solutions. It is important, therefore, to check that the solution obtained not only satisfies the displayed identity, but also the given conditions.

Model Solution

We use the identity arctan⁡A+arctan⁡B=arctan⁡ ⁣A+B1−AB\arctan A + \arctan B = \arctan\!\dfrac{A+B}{1-AB}, valid when AB<1AB < 1.

Part 1. Let A=1a+bA = \dfrac{1}{a+b} and B=1a+cB = \dfrac{1}{a+c}. Then:

A+B=a+c+a+b(a+b)(a+c)=2a+b+c(a+b)(a+c)A + B = \frac{a+c+a+b}{(a+b)(a+c)} = \frac{2a+b+c}{(a+b)(a+c)}

1−AB=1−1(a+b)(a+c)=(a+b)(a+c)−1(a+b)(a+c)=a2+ab+ac+bc−1(a+b)(a+c)1 - AB = 1 - \frac{1}{(a+b)(a+c)} = \frac{(a+b)(a+c)-1}{(a+b)(a+c)} = \frac{a^2+ab+ac+bc-1}{(a+b)(a+c)}

Using bc=a2+1bc = a^2+1:

a2+ab+ac+bc−1=a2+ab+ac+a2+1−1=2a2+ab+ac=a(2a+b+c)a^2 + ab + ac + bc - 1 = a^2 + ab + ac + a^2 + 1 - 1 = 2a^2 + ab + ac = a(2a+b+c)

Therefore:

A+B1−AB=2a+b+ca(2a+b+c)=1a\frac{A+B}{1-AB} = \frac{2a+b+c}{a(2a+b+c)} = \frac{1}{a}

Since a,b,c>0a, b, c > 0, we have AB=1(a+b)(a+c)<1AB = \frac{1}{(a+b)(a+c)} < 1 (as (a+b)(a+c)>1(a+b)(a+c) > 1), so:

arctan⁡1a+b+arctan⁡1a+c=arctan⁡1a.□\arctan\frac{1}{a+b} + \arctan\frac{1}{a+c} = \arctan\frac{1}{a} \text{.} \qquad \square

Part 2. We group the four terms into two pairs and apply the result from Part 1.

First pair: arctan⁡1p+q+s+arctan⁡1p+q+t\arctan\dfrac{1}{p+q+s} + \arctan\dfrac{1}{p+q+t}.

This has the form arctan⁡1a′+b′+arctan⁡1a′+c′\arctan\dfrac{1}{a'+b'} + \arctan\dfrac{1}{a'+c'} with a′=p+qa' = p+q, b′=sb' = s, c′=tc' = t. The condition b′c′=a′2+1b'c' = a'^2+1 becomes st=(p+q)2+1st = (p+q)^2+1, which holds by hypothesis. By Part 1:

arctan⁡1p+q+s+arctan⁡1p+q+t=arctan⁡1p+q.(*)\arctan\frac{1}{p+q+s} + \arctan\frac{1}{p+q+t} = \arctan\frac{1}{p+q} \text{.} \qquad \text{(*)}

Second pair: arctan⁡1p+r+u+arctan⁡1p+r+v\arctan\dfrac{1}{p+r+u} + \arctan\dfrac{1}{p+r+v}.

Similarly, with a′=p+ra' = p+r, b′=ub' = u, c′=vc' = v and uv=(p+r)2+1uv = (p+r)^2+1:

arctan⁡1p+r+u+arctan⁡1p+r+v=arctan⁡1p+r.(**)\arctan\frac{1}{p+r+u} + \arctan\frac{1}{p+r+v} = \arctan\frac{1}{p+r} \text{.} \qquad \text{(**)}

Combining: Adding (∗)(*) and (∗∗)(**), we need arctan⁡1p+q+arctan⁡1p+r\arctan\dfrac{1}{p+q} + \arctan\dfrac{1}{p+r}. Applying Part 1 once more with a=pa = p, b=qb = q, c=rc = r and the condition qr=p2+1qr = p^2+1:

arctan⁡1p+q+arctan⁡1p+r=arctan⁡1p.□\arctan\frac{1}{p+q} + \arctan\frac{1}{p+r} = \arctan\frac{1}{p} \text{.} \qquad \square

Numerical verification. We seek p,q,r,s,t,u,vp, q, r, s, t, u, v satisfying the three constraints and matching the four target arguments. Setting p=7p = 7 and assigning:

p+r+u=13,p+r+v=21,p+q+s=82,p+q+t=187.p+r+u = 13, \quad p+r+v = 21, \quad p+q+s = 82, \quad p+q+t = 187.

First pair (with a′=p+ra' = p+r): r+u=6r+u = 6 and r+v=14r+v = 14, so u=6−ru = 6-r and v=14−rv = 14-r. From uv=(7+r)2+1uv = (7+r)^2+1:

(6−r)(14−r)=(7+r)2+1(6-r)(14-r) = (7+r)^2+1

r2−20r+84=r2+14r+50r^2 - 20r + 84 = r^2 + 14r + 50

34=34r  ⟹  r=134 = 34r \implies r = 1

So u=5u = 5 and v=13v = 13.

Second pair (with a′=p+qa' = p+q): q+s=75q+s = 75 and q+t=180q+t = 180, so s=75−qs = 75-q and t=180−qt = 180-q. From st=(7+q)2+1st = (7+q)^2+1:

(75−q)(180−q)=(7+q)2+1(75-q)(180-q) = (7+q)^2+1

q2−255q+13500=q2+14q+50q^2 - 255q + 13500 = q^2 + 14q + 50

13450=269q  ⟹  q=5013450 = 269q \implies q = 50

So s=25s = 25 and t=130t = 130.

Verification of all three constraints:

  • qr=50×1=50=72+1qr = 50 \times 1 = 50 = 7^2 + 1 ✓\checkmark
  • st=25×130=3250=(7+50)2+1=3250st = 25 \times 130 = 3250 = (7+50)^2 + 1 = 3250 ✓\checkmark
  • uv=5×13=65=(7+1)2+1=65uv = 5 \times 13 = 65 = (7+1)^2 + 1 = 65 ✓\checkmark

Verification of all four arguments:

  • p+r+u=7+1+5=13p+r+u = 7+1+5 = 13 ✓\checkmark
  • p+r+v=7+1+13=21p+r+v = 7+1+13 = 21 ✓\checkmark
  • p+q+s=7+50+25=82p+q+s = 7+50+25 = 82 ✓\checkmark
  • p+q+t=7+50+130=187p+q+t = 7+50+130 = 187 ✓\checkmark

Since addition is commutative, the four-term sum equals arctan⁡113+arctan⁡121+arctan⁡182+arctan⁡1187\arctan\frac{1}{13}+\arctan\frac{1}{21}+\arctan\frac{1}{82}+\arctan\frac{1}{187}, which by the proved identity equals arctan⁡17\arctan\frac{1}{7}. □\qquad \square

Note: The correct assignment pairs the smaller targets (1313, 2121) with r=1r = 1 and the larger targets (8282, 187187) with q=50q = 50. All seven values p=7p=7, q=50q=50, r=1r=1, s=25s=25, t=130t=130, u=5u=5, v=13v=13 are positive, as required.


Topic: 几何 Geometry(圆与三角形)  |  Difficulty: Challenging  |  Marks: 20

5 The angle AA of triangle ABCABC is a right angle and the sides BC,CABC, CA and ABAB are of lengths aa, bb and cc, respectively. Each side of the triangle is tangent to the circle S1S_1 which is of radius rr. Show that 2r=b+c−a2r = b + c - a.

Each vertex of the triangle lies on the circle S2S_2. The ratio of the area of the region between S1S_1 and the triangle to the area of S2S_2 is denoted by RR. Show that

πR=−(π−1)q2+2πq−(π+1),\pi R = -(\pi - 1)q^2 + 2\pi q - (\pi + 1) ,

where q=b+caq = \frac{b+c}{a}. Deduce that

R≤1π(π−1).R \le \frac{1}{\pi(\pi - 1)} .

Hint

At the outset it should be emphasised that a large, well annotated diagram will enable insight into this question.

The first result may be obtained expeditiously by observing that if S_1 touches the sides BC, CA, AB at P, Q, R, respectively, then AQ = AR = r implies BR = c - r, CQ = b - r. Thus b - r + c - r = a implies 2r = b + c - a.

This result leads to r = a(q - 1)/2 which is the key to the remainder of the question. In fact R = [2bc - pi a^2(q - 1)^2]/(pi a^2) (*).

From the data a^2 = b^2 + c^2 implies 2bc = (a + b + c)(b + c - a) implies bc/a^2 = (q^2 - 1)/2 which together with (*) leads to the second displayed result.

The obtaining of the turning value of a quadratic function is routine. In this context the method of completion of the square is to be preferred to the use of the calculus. Where the critical value of q is obtained from dR/dq = 0, it is important to give a reason as to why this defines an upper bound for R.

Model Solution

Show that 2r=b+c−a2r = b + c - a.

Let S1S_1 touch BCBC, CACA, ABAB at PP, QQ, RR respectively. Since the two tangents from an external point to a circle are equal in length:

AQ=AR=r,BQ=BP,CP=CQ.AQ = AR = r, \quad BQ = BP, \quad CP = CQ.

From these:

BR=AB−AR=c−r,CQ=CA−AQ=b−r.BR = AB - AR = c - r, \quad CQ = CA - AQ = b - r.

Since BP=BRBP = BR and CP=CQCP = CQ:

a=BC=BP+CP=BR+CQ=(c−r)+(b−r)=b+c−2r.a = BC = BP + CP = BR + CQ = (c - r) + (b - r) = b + c - 2r.

Therefore 2r=b+c−a2r = b + c - a. □\qquad \square

Show that πR=−(π−1)q2+2πq−(π+1)\pi R = -(\pi - 1)q^2 + 2\pi q - (\pi + 1).

Since AA is a right angle, by Pythagoras a2=b2+c2a^2 = b^2 + c^2, so BCBC is the diameter of the circumcircle S2S_2. The circumradius is a/2a/2, giving:

Area(S2)=π(a2)2=πa24.\text{Area}(S_2) = \pi \left(\frac{a}{2}\right)^2 = \frac{\pi a^2}{4}.

The area of triangle ABCABC is 12bc\frac{1}{2}bc, and the area of S1S_1 is πr2\pi r^2. Thus:

R=12bc−πr2πa24=2bc−πa2(q−1)2πa2R = \frac{\frac{1}{2}bc - \pi r^2}{\frac{\pi a^2}{4}} = \frac{2bc - \pi a^2(q-1)^2}{\pi a^2}

where we substituted r=a(q−1)2r = \frac{a(q-1)}{2} from 2r=b+c−a=a(q−1)2r = b + c - a = a(q - 1).

We now express bc/a2bc/a^2 in terms of qq. From a2=b2+c2a^2 = b^2 + c^2:

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

⟹2bc=(b+c)2−a2=a2q2−a2=a2(q2−1)\Longrightarrow \quad 2bc = (b+c)^2 - a^2 = a^2q^2 - a^2 = a^2(q^2 - 1)

⟹bca2=q2−12.\Longrightarrow \quad \frac{bc}{a^2} = \frac{q^2 - 1}{2}.

Substituting into the expression for πR\pi R:

πR=2bca2−π(q−1)2=(q2−1)−π(q−1)2.\pi R = \frac{2bc}{a^2} - \pi(q-1)^2 = (q^2 - 1) - \pi(q-1)^2.

Expanding (q−1)2=q2−2q+1(q-1)^2 = q^2 - 2q + 1:

πR=q2−1−πq2+2πq−π=−(π−1)q2+2πq−(π+1).□\pi R = q^2 - 1 - \pi q^2 + 2\pi q - \pi = -(\pi - 1)q^2 + 2\pi q - (\pi + 1). \qquad \square

Deduce that R⩽1π(π−1)R \leqslant \frac{1}{\pi(\pi - 1)}.

We have πR=−(π−1)q2+2πq−(π+1)\pi R = -(\pi - 1)q^2 + 2\pi q - (\pi + 1). Since π−1>0\pi - 1 > 0, this is a downward-opening quadratic in qq with a maximum. Completing the square:

πR=−(π−1) ⁣[q2−2ππ−1 q]−(π+1)\pi R = -(\pi - 1)\!\left[q^2 - \frac{2\pi}{\pi - 1}\,q\right] - (\pi + 1)

=−(π−1) ⁣[q−ππ−1]2+π2π−1−(π+1).= -(\pi - 1)\!\left[q - \frac{\pi}{\pi - 1}\right]^2 + \frac{\pi^2}{\pi - 1} - (\pi + 1).

The constant term simplifies:

π2π−1−(π+1)=π2−(π+1)(π−1)π−1=π2−(π2−1)π−1=1π−1.\frac{\pi^2}{\pi - 1} - (\pi + 1) = \frac{\pi^2 - (\pi + 1)(\pi - 1)}{\pi - 1} = \frac{\pi^2 - (\pi^2 - 1)}{\pi - 1} = \frac{1}{\pi - 1}.

So:

πR=−(π−1) ⁣[q−ππ−1]2+1π−1.\pi R = -(\pi - 1)\!\left[q - \frac{\pi}{\pi - 1}\right]^2 + \frac{1}{\pi - 1}.

Since the squared term is non-negative, πR⩽1π−1\pi R \leqslant \frac{1}{\pi - 1}, and therefore:

R⩽1π(π−1).□R \leqslant \frac{1}{\pi(\pi - 1)}. \qquad \square

The completed square gives the required upper bound; the unconstrained vertex q=ππ−1q = \frac{\pi}{\pi - 1} lies outside the feasible range 1<q⩽21 < q \leqslant \sqrt{2} for a right triangle with legs b,cb, c.


Topic: 幂级数 Power Series  |  Difficulty: Challenging  |  Marks: 20

6 (i) Write down the general term in the expansion in powers of xx of (1−x)−1(1 - x)^{-1}, (1−x)−2(1 - x)^{-2} and (1−x)−3(1 - x)^{-3}, where ∣x∣<1|x| < 1.

Evaluate ∑n=1∞n2−n\displaystyle \sum_{n=1}^{\infty} n 2^{-n} and ∑n=1∞n22−n.\displaystyle \sum_{n=1}^{\infty} n^2 2^{-n} .

(ii) Show that (1−x)−12=∑n=0∞(2n)!(n!)2xn22n\displaystyle (1 - x)^{-\frac{1}{2}} = \sum_{n=0}^{\infty} \frac{(2n)!}{(n!)^2} \frac{x^n}{2^{2n}}, for ∣x∣<1|x| < 1.

Evaluate ∑n=0∞(2n)!(n!)222n3n\displaystyle \sum_{n=0}^{\infty} \frac{(2n)!}{(n!)^2 2^{2n} 3^n} and ∑n=1∞n(2n)!(n!)222n3n.\displaystyle \sum_{n=1}^{\infty} \frac{n(2n)!}{(n!)^2 2^{2n} 3^n} .

Hint

(i) The power series representations of (1+x)−k(1 + x)^{-k} for k=1,2,3k = 1, 2, 3 are standard and should be well known by any candidate for this examination. In fact the general terms of these three series are xnx^n, (n+1)xn(n + 1)x^n, (1/2)(n+1)(n+2)xn(1/2)(n + 1)(n + 2)x^n, respectively.

The displayed series may be summed by using the general terms obtained. Thus, ∑n=1∞n2−n=(1/2)(1−1/2)−2=2\sum_{n=1}^{\infty} n 2^{-n} = (1/2)(1 - 1/2)^{-2} = 2, and as ∑n=1∞n(n+1)2−n=8\sum_{n=1}^{\infty} n(n + 1)2^{-n} = 8, then ∑n=1∞n22−n=8−2=6\sum_{n=1}^{\infty} n^2 2^{-n} = 8 - 2 = 6.

(ii) The obtaining of the general term of the power series for (1−x)−1/2(1 - x)^{-1/2} is a straightforward application of the binomial series for a general exponent.

To sum the penultimate series, put x=1/3x = 1/3 and to sum the final series, first differentiate with respect to xx and then put x=1/3x = 1/3. The sums will be found to be 3/2\sqrt{3/2} and (1/4)3/2(1/4)\sqrt{3/2}, respectively.

Model Solution

Part (i)

The general terms in the expansions of (1−x)−k(1-x)^{-k} for ∣x∣<1|x| < 1:

For (1−x)−1(1 - x)^{-1}: the nnth term (starting at n=0n = 0) is xnx^n.

For (1−x)−2(1 - x)^{-2}: using the identity (1−x)−2=ddx(1−x)−1(1-x)^{-2} = \frac{d}{dx}(1-x)^{-1}, the nnth term is (n+1)xn(n+1)x^n.

For (1−x)−3(1 - x)^{-3}: using (1−x)−3=12d2dx2(1−x)−1(1-x)^{-3} = \frac{1}{2}\frac{d^2}{dx^2}(1-x)^{-1}, the nnth term is 12(n+1)(n+2)xn\frac{1}{2}(n+1)(n+2)x^n.

Evaluate ∑n=1∞n 2−n\displaystyle\sum_{n=1}^{\infty} n\,2^{-n}.

From the expansion (1−x)−2=∑n=0∞(n+1)xn(1-x)^{-2} = \sum_{n=0}^{\infty}(n+1)x^n, we have:

∑n=0∞(n+1)xn=1(1−x)2\sum_{n=0}^{\infty}(n+1)x^n = \frac{1}{(1-x)^2}

⟹∑n=0∞nxn+∑n=0∞xn=1(1−x)2\Longrightarrow \quad \sum_{n=0}^{\infty} nx^n + \sum_{n=0}^{\infty} x^n = \frac{1}{(1-x)^2}

⟹∑n=1∞nxn=1(1−x)2−11−x=x(1−x)2.\Longrightarrow \quad \sum_{n=1}^{\infty} nx^n = \frac{1}{(1-x)^2} - \frac{1}{1-x} = \frac{x}{(1-x)^2}.

Setting x=12x = \frac{1}{2}:

∑n=1∞n2n=12(12)2=1214=2.(a)\sum_{n=1}^{\infty} \frac{n}{2^n} = \frac{\frac{1}{2}}{\left(\frac{1}{2}\right)^2} = \frac{\frac{1}{2}}{\frac{1}{4}} = 2. \qquad \text{(a)}

Evaluate ∑n=1∞n2 2−n\displaystyle\sum_{n=1}^{\infty} n^2\,2^{-n}.

From the expansion (1−x)−3=∑n=0∞12(n+1)(n+2)xn(1-x)^{-3} = \sum_{n=0}^{\infty}\frac{1}{2}(n+1)(n+2)x^n:

∑n=0∞12(n+1)(n+2)xn=1(1−x)3\sum_{n=0}^{\infty}\frac{1}{2}(n+1)(n+2)x^n = \frac{1}{(1-x)^3}

⟹∑n=0∞(n+1)(n+2)xn=2(1−x)3.\Longrightarrow \quad \sum_{n=0}^{\infty}(n+1)(n+2)x^n = \frac{2}{(1-x)^3}.

Expanding (n+1)(n+2)=n2+3n+2(n+1)(n+2) = n^2 + 3n + 2:

∑n=1∞n2xn+3∑n=1∞nxn+2∑n=0∞xn=2(1−x)3\sum_{n=1}^{\infty} n^2 x^n + 3\sum_{n=1}^{\infty} nx^n + 2\sum_{n=0}^{\infty} x^n = \frac{2}{(1-x)^3}

⟹∑n=1∞n2xn=2(1−x)3−3x(1−x)2−21−x.\Longrightarrow \quad \sum_{n=1}^{\infty} n^2 x^n = \frac{2}{(1-x)^3} - \frac{3x}{(1-x)^2} - \frac{2}{1-x}.

Setting x=12x = \frac{1}{2}:

∑n=1∞n22n=2(12)3−3⋅12(12)2−212=16−6−4=6.(b)\sum_{n=1}^{\infty} \frac{n^2}{2^n} = \frac{2}{\left(\frac{1}{2}\right)^3} - \frac{3 \cdot \frac{1}{2}}{\left(\frac{1}{2}\right)^2} - \frac{2}{\frac{1}{2}} = 16 - 6 - 4 = 6. \qquad \text{(b)}

Part (ii)

Show that (1−x)−1/2=∑n=0∞(2n)!(n!)2xn22n\displaystyle (1-x)^{-1/2} = \sum_{n=0}^{\infty}\frac{(2n)!}{(n!)^2}\frac{x^n}{2^{2n}}.

Using the general binomial expansion for (1−x)α(1-x)^{\alpha} with α=−12\alpha = -\frac{1}{2}:

(1−x)−1/2=∑n=0∞(−1/2n)(−x)n=∑n=0∞(−1/2n)(−1)nxn.(1-x)^{-1/2} = \sum_{n=0}^{\infty}\binom{-1/2}{n}(-x)^n = \sum_{n=0}^{\infty}\binom{-1/2}{n}(-1)^n x^n.

We compute:

(−1/2n)=(−12)(−12−1)(−12−2)⋯(−12−n+1)n!\binom{-1/2}{n} = \frac{(-\tfrac{1}{2})(-\tfrac{1}{2} - 1)(-\tfrac{1}{2} - 2)\cdots(-\tfrac{1}{2} - n + 1)}{n!}

=(−1)n⋅12⋅32⋅52⋯2n−12n!=(−1)n2n⋅n!⋅1⋅3⋅5⋯(2n−1).= \frac{(-1)^n \cdot \frac{1}{2} \cdot \frac{3}{2} \cdot \frac{5}{2} \cdots \frac{2n-1}{2}}{n!} = \frac{(-1)^n}{2^n \cdot n!}\cdot 1 \cdot 3 \cdot 5 \cdots (2n-1).

Therefore:

(−1/2n)(−1)n=1⋅3⋅5⋯(2n−1)2n⋅n!.\binom{-1/2}{n}(-1)^n = \frac{1 \cdot 3 \cdot 5 \cdots (2n-1)}{2^n \cdot n!}.

The product 1⋅3⋅5⋯(2n−1)1 \cdot 3 \cdot 5 \cdots (2n-1) equals (2n)!2n⋅n!\frac{(2n)!}{2^n \cdot n!}, since (2n)!=[1⋅3⋅5⋯(2n−1)]⋅[2⋅4⋅6⋯2n]=[1⋅3⋯(2n−1)]⋅2n⋅n!(2n)! = [1 \cdot 3 \cdot 5 \cdots (2n-1)] \cdot [2 \cdot 4 \cdot 6 \cdots 2n] = [1 \cdot 3 \cdots (2n-1)] \cdot 2^n \cdot n!.

So:

(−1/2n)(−1)n=(2n)!2n⋅n!⋅2n⋅n!=(2n)!4n(n!)2=(2n)!(n!)2⋅22n.\binom{-1/2}{n}(-1)^n = \frac{(2n)!}{2^n \cdot n! \cdot 2^n \cdot n!} = \frac{(2n)!}{4^n(n!)^2} = \frac{(2n)!}{(n!)^2 \cdot 2^{2n}}.

Thus:

(1−x)−1/2=∑n=0∞(2n)!(n!)2xn22nfor ∣x∣<1.□(1-x)^{-1/2} = \sum_{n=0}^{\infty}\frac{(2n)!}{(n!)^2}\frac{x^n}{2^{2n}} \qquad \text{for } |x| < 1. \qquad \square

Evaluate ∑n=0∞(2n)!(n!)2 22n 3n\displaystyle\sum_{n=0}^{\infty}\frac{(2n)!}{(n!)^2\,2^{2n}\,3^n}.

Setting x=13x = \frac{1}{3} in the expansion:

∑n=0∞(2n)!(n!)2 22n⋅13n=(1−13)−1/2=(23)−1/2=(32)1/2.\sum_{n=0}^{\infty}\frac{(2n)!}{(n!)^2\,2^{2n}} \cdot \frac{1}{3^n} = \left(1 - \frac{1}{3}\right)^{-1/2} = \left(\frac{2}{3}\right)^{-1/2} = \left(\frac{3}{2}\right)^{1/2}.

∑n=0∞(2n)!(n!)2 22n 3n=32.(c)\sum_{n=0}^{\infty}\frac{(2n)!}{(n!)^2\,2^{2n}\,3^n} = \sqrt{\frac{3}{2}}. \qquad \text{(c)}

Evaluate ∑n=1∞n(2n)!(n!)2 22n 3n\displaystyle\sum_{n=1}^{\infty}\frac{n(2n)!}{(n!)^2\,2^{2n}\,3^n}.

Differentiating the expansion term by term with respect to xx:

ddx(1−x)−1/2=12(1−x)−3/2=∑n=1∞n(2n)!(n!)2 22n xn−1.\frac{d}{dx}(1-x)^{-1/2} = \frac{1}{2}(1-x)^{-3/2} = \sum_{n=1}^{\infty}\frac{n(2n)!}{(n!)^2\,2^{2n}}\,x^{n-1}.

Multiplying both sides by xx:

x2(1−x)−3/2=∑n=1∞n(2n)!(n!)2 22n xn.\frac{x}{2}(1-x)^{-3/2} = \sum_{n=1}^{\infty}\frac{n(2n)!}{(n!)^2\,2^{2n}}\,x^{n}.

Setting x=13x = \frac{1}{3}:

∑n=1∞n(2n)!(n!)2 22n 3n=12⋅13⋅(23)−3/2=16(32)3/2.\sum_{n=1}^{\infty}\frac{n(2n)!}{(n!)^2\,2^{2n}\,3^n} = \frac{1}{2}\cdot\frac{1}{3}\cdot\left(\frac{2}{3}\right)^{-3/2} = \frac{1}{6}\left(\frac{3}{2}\right)^{3/2}.

Since (32)3/2=32⋅32\left(\frac{3}{2}\right)^{3/2} = \frac{3}{2}\cdot\sqrt{\frac{3}{2}}:

∑n=1∞n(2n)!(n!)2 22n 3n=16⋅32⋅32=1432.(d)\sum_{n=1}^{\infty}\frac{n(2n)!}{(n!)^2\,2^{2n}\,3^n} = \frac{1}{6}\cdot\frac{3}{2}\cdot\sqrt{\frac{3}{2}} = \frac{1}{4}\sqrt{\frac{3}{2}}. \qquad \text{(d)}


Topic: 向量与三维几何 Vectors and 3D Geometry  |  Difficulty: Challenging  |  Marks: 20

7 The position vectors, relative to an origin OO, at time tt of the particles PP and QQ are

cos⁡ti+sin⁡tj+0kandcos⁡(t+14π)[32i+332k]+3sin⁡(t+14π)j ,\cos t \mathbf{i} + \sin t \mathbf{j} + 0 \mathbf{k} \quad \text{and} \quad \cos(t + \frac{1}{4}\pi) \left[ \frac{3}{2}\mathbf{i} + \frac{3\sqrt{3}}{2}\mathbf{k} \right] + 3 \sin(t + \frac{1}{4}\pi) \mathbf{j} \text{ ,}

respectively, where 0⩽t⩽2π0 \leqslant t \leqslant 2\pi.

(i) Give a geometrical description of the motion of PP and QQ.

(ii) Let θ\theta be the angle POQPOQ at time tt that satisfies 0⩽θ⩽2π0 \leqslant \theta \leqslant 2\pi. Show that

cos⁡θ=328−14cos⁡(2t+14π).\cos \theta = \frac{3\sqrt{2}}{8} - \frac{1}{4} \cos(2t + \frac{1}{4}\pi) \text{.}

(iii) Show that the total time for which θ⩾14π\theta \geqslant \frac{1}{4}\pi is 32π\frac{3}{2}\pi.

Hint

(i) The absence of a k component in the specification of the locus of P, shows immediately that its motion takes place in the plane z=0z = 0, i.e. in the x−yx - y plane. Also, it is obvious that x2+y2=1x^2 + y^2 = 1. Hence P describes a circle centre O and radius 1 in the x−yx - y plane.

For the locus of Q, it is helpful to write x=(3/2)cos⁡(t+π/4)x = (3/2) \cos(t + \pi/4), y=3sin⁡(t+π/4)y = 3 \sin(t + \pi/4), z=(33/2)cos⁡(t+π/4)z = (3\sqrt{3}/2) \cos(t + \pi/4). It is then evident that 3x−z=0\sqrt{3}x - z = 0 and so this defines the plane in which the motion of Q takes place. Furthermore, it is clear that x2+y2+z2=9x^2 + y^2 + z^2 = 9 which shows that the distance of Q from O is constant and equal to 3. Hence Q describes the circle centre O and radius 3 in the plane 3x−z=0\sqrt{3}x - z = 0.

(ii) Use of the scalar product leads to cos⁡θ=∣(1/2)cos⁡tcos⁡(t+π/4)+sin⁡tsin⁡(t+π/4)∣=...=∣3/(42)−(1/4)cos⁡(2t+π/4)∣\cos \theta = |(1/2) \cos t \cos(t + \pi/4) + \sin t \sin(t + \pi/4)| = ... = |3/(4\sqrt{2}) - (1/4) \cos(2t + \pi/4)|.

(iii) From the result just obtained, it is immediate that θ≥π/4⇒−1/2≤3/(42)−c/4≤1/2\theta \geq \pi/4 \Rightarrow -1/\sqrt{2} \leq 3/(4\sqrt{2}) - c/4 \leq 1/\sqrt{2} where c≡cos⁡(2t+π/4)c \equiv \cos(2t + \pi/4), so that cc is restricted to the interval −1/2≤c≤1-1/\sqrt{2} \leq c \leq 1, and as c≤1c \le 1, then t∉[π/4,π/2]t \notin [\pi/4, \pi/2] and t∉[5π/4,3π/2]t \notin [5\pi/4, 3\pi/2] are required. Hence T=3π/2T = 3\pi/2.

Model Solution

Part (i)

The position vector of PP is p=cos⁡t i+sin⁡t j\mathbf{p} = \cos t\,\mathbf{i} + \sin t\,\mathbf{j}, which has no k\mathbf{k} component. Thus PP moves in the plane z=0z = 0 (the xyxy-plane). Since x2+y2=cos⁡2t+sin⁡2t=1x^2 + y^2 = \cos^2 t + \sin^2 t = 1, the particle PP describes a circle of centre OO and radius 11 in the xyxy-plane.

The position vector of QQ is q=32cos⁡(t+π4) i+3sin⁡(t+π4) j+332cos⁡(t+π4) k\mathbf{q} = \tfrac{3}{2}\cos(t + \tfrac{\pi}{4})\,\mathbf{i} + 3\sin(t + \tfrac{\pi}{4})\,\mathbf{j} + \tfrac{3\sqrt{3}}{2}\cos(t + \tfrac{\pi}{4})\,\mathbf{k}. We compute:

x2+y2+z2=94cos⁡2(t+π4)+9sin⁡2(t+π4)+274cos⁡2(t+π4)=9cos⁡2(t+π4)+9sin⁡2(t+π4)=9,x^2 + y^2 + z^2 = \tfrac{9}{4}\cos^2(t+\tfrac{\pi}{4}) + 9\sin^2(t+\tfrac{\pi}{4}) + \tfrac{27}{4}\cos^2(t+\tfrac{\pi}{4}) = 9\cos^2(t+\tfrac{\pi}{4}) + 9\sin^2(t+\tfrac{\pi}{4}) = 9 \text{,}

so QQ remains at distance 33 from OO. Also, the ratio z/x=33/23/2=3z/x = \tfrac{3\sqrt{3}/2}{3/2} = \sqrt{3} (when cos⁡(t+π4)≠0\cos(t+\tfrac{\pi}{4}) \neq 0), so z=3 xz = \sqrt{3}\,x. Therefore QQ describes a circle of centre OO and radius 33 in the plane 3 x−z=0\sqrt{3}\,x - z = 0.

Part (ii)

We compute cos⁡θ\cos\theta using cos⁡θ=p⋅q∣p∣∣q∣\cos\theta = \dfrac{\mathbf{p}\cdot\mathbf{q}}{|\mathbf{p}||\mathbf{q}|}.

Since ∣p∣=1|\mathbf{p}| = 1 and ∣q∣=3|\mathbf{q}| = 3:

p⋅q=32cos⁡tcos⁡(t+π4)+3sin⁡tsin⁡(t+π4)+0.\mathbf{p}\cdot\mathbf{q} = \tfrac{3}{2}\cos t\cos(t+\tfrac{\pi}{4}) + 3\sin t\sin(t+\tfrac{\pi}{4}) + 0 \text{.}

Using the product-to-sum identities cos⁡Acos⁡B=12[cos⁡(A−B)+cos⁡(A+B)]\cos A\cos B = \tfrac{1}{2}[\cos(A-B)+\cos(A+B)] and sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)]\sin A\sin B = \tfrac{1}{2}[\cos(A-B)-\cos(A+B)]:

cos⁡tcos⁡(t+π4)=12[cos⁡(−π4)+cos⁡(2t+π4)]=12[cos⁡π4+cos⁡(2t+π4)]\cos t\cos(t+\tfrac{\pi}{4}) = \tfrac{1}{2}[\cos(-\tfrac{\pi}{4}) + \cos(2t+\tfrac{\pi}{4})] = \tfrac{1}{2}[\cos\tfrac{\pi}{4} + \cos(2t+\tfrac{\pi}{4})]

sin⁡tsin⁡(t+π4)=12[cos⁡(−π4)−cos⁡(2t+π4)]=12[cos⁡π4−cos⁡(2t+π4)]\sin t\sin(t+\tfrac{\pi}{4}) = \tfrac{1}{2}[\cos(-\tfrac{\pi}{4}) - \cos(2t+\tfrac{\pi}{4})] = \tfrac{1}{2}[\cos\tfrac{\pi}{4} - \cos(2t+\tfrac{\pi}{4})]

Substituting:

p⋅q=32⋅12[cos⁡π4+cos⁡(2t+π4)]+3⋅12[cos⁡π4−cos⁡(2t+π4)]\mathbf{p}\cdot\mathbf{q} = \tfrac{3}{2}\cdot\tfrac{1}{2}[\cos\tfrac{\pi}{4} + \cos(2t+\tfrac{\pi}{4})] + 3\cdot\tfrac{1}{2}[\cos\tfrac{\pi}{4} - \cos(2t+\tfrac{\pi}{4})]

=34cos⁡π4+34cos⁡(2t+π4)+32cos⁡π4−32cos⁡(2t+π4)= \tfrac{3}{4}\cos\tfrac{\pi}{4} + \tfrac{3}{4}\cos(2t+\tfrac{\pi}{4}) + \tfrac{3}{2}\cos\tfrac{\pi}{4} - \tfrac{3}{2}\cos(2t+\tfrac{\pi}{4})

=94cos⁡π4−34cos⁡(2t+π4)=928−34cos⁡(2t+π4).= \tfrac{9}{4}\cos\tfrac{\pi}{4} - \tfrac{3}{4}\cos(2t+\tfrac{\pi}{4}) = \tfrac{9\sqrt{2}}{8} - \tfrac{3}{4}\cos(2t+\tfrac{\pi}{4}) \text{.}

Therefore:

cos⁡θ=p⋅q3=328−14cos⁡(2t+π4).□\cos\theta = \frac{\mathbf{p}\cdot\mathbf{q}}{3} = \frac{3\sqrt{2}}{8} - \frac{1}{4}\cos(2t+\tfrac{\pi}{4}) \text{.} \qquad \square

Part (iii)

Since θ∈[0,π]\theta \in [0, \pi], the condition θ⩾π4\theta \geqslant \tfrac{\pi}{4} is equivalent to cos⁡θ⩽cos⁡π4=22\cos\theta \leqslant \cos\tfrac{\pi}{4} = \tfrac{\sqrt{2}}{2}. Substituting:

328−14cos⁡(2t+π4)⩽22\frac{3\sqrt{2}}{8} - \frac{1}{4}\cos(2t+\tfrac{\pi}{4}) \leqslant \frac{\sqrt{2}}{2}

−14cos⁡(2t+π4)⩽22−328=28-\frac{1}{4}\cos(2t+\tfrac{\pi}{4}) \leqslant \frac{\sqrt{2}}{2} - \frac{3\sqrt{2}}{8} = \frac{\sqrt{2}}{8}

cos⁡(2t+π4)⩾−22.\cos(2t+\tfrac{\pi}{4}) \geqslant -\frac{\sqrt{2}}{2} \text{.}

We now find the values of t∈[0,2π]t \in [0, 2\pi] for which this fails, i.e., where cos⁡(2t+π4)<−22\cos(2t+\tfrac{\pi}{4}) < -\tfrac{\sqrt{2}}{2}. Setting φ=2t+π4\varphi = 2t + \tfrac{\pi}{4}, the condition cos⁡φ<−22\cos\varphi < -\tfrac{\sqrt{2}}{2} holds when φ∈(3π4+2kπ,5π4+2kπ)\varphi \in (\tfrac{3\pi}{4} + 2k\pi, \tfrac{5\pi}{4} + 2k\pi) for integer kk.

For t∈[0,2π]t \in [0, 2\pi], we have φ∈[π4,17π4]\varphi \in [\tfrac{\pi}{4}, \tfrac{17\pi}{4}]. The excluded intervals are:

  • k=0k = 0: φ∈(3π4,5π4)\varphi \in (\tfrac{3\pi}{4}, \tfrac{5\pi}{4}), giving t∈(π4,π2)t \in (\tfrac{\pi}{4}, \tfrac{\pi}{2}).
  • k=1k = 1: φ∈(11π4,13π4)\varphi \in (\tfrac{11\pi}{4}, \tfrac{13\pi}{4}), giving t∈(5π4,3π2)t \in (\tfrac{5\pi}{4}, \tfrac{3\pi}{2}).

The total excluded time is:

(π2−π4)+(3π2−5π4)=π4+π4=π2.(\tfrac{\pi}{2} - \tfrac{\pi}{4}) + (\tfrac{3\pi}{2} - \tfrac{5\pi}{4}) = \tfrac{\pi}{4} + \tfrac{\pi}{4} = \tfrac{\pi}{2} \text{.}

Hence the total time for which θ⩾π4\theta \geqslant \tfrac{\pi}{4} is:

2π−π2=32π.□2\pi - \frac{\pi}{2} = \frac{3}{2}\pi \text{.} \qquad \square


Topic: 微分方程与曲线描绘 Differential Equations and Curve Sketching  |  Difficulty: Challenging  |  Marks: 20

8 For x⩾0x \geqslant 0 the curve CC is defined by

dydx=x3y2(1+x2)5/2\frac{\mathrm{d}y}{\mathrm{d}x} = \frac{x^3 y^2}{(1 + x^2)^{5/2}}

with y=1y = 1 when x=0x = 0. Show that

1y=2+3x23(1+x2)3/2+13\frac{1}{y} = \frac{2 + 3x^2}{3(1 + x^2)^{3/2}} + \frac{1}{3}

and hence that for large positive xx

y≈3−9x.y \approx 3 - \frac{9}{x} \text{.}

Draw a sketch of CC.

On a separate diagram draw a sketch of the two curves defined for x⩾0x \geqslant 0 by

dzdx=x3z32(1+x2)5/2\frac{\mathrm{d}z}{\mathrm{d}x} = \frac{x^3 z^3}{2(1 + x^2)^{5/2}}

with z=1z = 1 at x=0x = 0 on one curve, and z=−1z = -1 at x=0x = 0 on the other.

Hint

Separation of variables will lead to A−1/y=∫x3(1+x2)−5/2 dx,A - 1/y = \int x^3(1 + x^2)^{-5/2} \, dx, where A is a constant. There are several possible strategies for the evaluation of the integral on the right; by parts, or by any of such substitutions as w=1+x2w = 1 + x^2, x=tan⁡tx = \tan t, x=sinh⁡vx = \sinh v. One way or another, the result of this integration correctly carried out will lead to the equivalent of A−1/y=−(1/3)x2(1+x2)−3/2−(2/3)(1+x2)−1/2.A - 1/y = -(1/3)x^2(1 + x^2)^{-3/2} - (2/3)(1 + x^2)^{-1/2}.

Use of the initial condition y(0)=1y(0) = 1 will then show that A=1/3A = 1/3 and the required result follows at once: 1/y=1/3+(2+3x2)/[3(1+x2)3/2].1/y = 1/3 + (2 + 3x^2)/[3(1 + x^2)^{3/2}].

To obtain the required approximation for yy for large positive xx, first write 1/y≈1/3+(2+3x2)(1−3/2x2)/3x3,1/y \approx 1/3 + (2 + 3x^2)(1 - 3/2x^2)/3x^3, from which it follows that 1/y=1/3+1/x+O(1/x3)1/y = 1/3 + 1/x + O(1/x^3) and this can easily be worked to the displayed approximation for yy.

For the sketch, the main features are that it has a zero gradient at x=0x = 0 and that for x>0x > 0, it is monotonically increasing and has exactly one point of inflexion and that it is asymptotic to the line y=3y = 3.

The two given differential equations are related by y=z2y = z^2. Thus it is unnecessary to solve the second differential equation independently of the first. In any case, the question does not require a formal solution for zz. Nevertheless, it is helpful to obtain the approximation z≈±3∓33/(2x)z \approx \pm\sqrt{3} \mp 3\sqrt{3}/(2x) from y≈3−9/xy \approx 3 - 9/x, for large positive xx.

All the main features of the x−zx - z sketch may be derived from those listed above for the x−yx - y sketch. The two curves which make up the sketch of zz are reflections of each other in the xx-axis. They start at (0,±1)(0, \pm 1) and are asymptotic to the lines z=±3z = \pm\sqrt{3}.

Model Solution

Show that 1y=2+3x23(1+x2)3/2+13\dfrac{1}{y} = \dfrac{2 + 3x^2}{3(1 + x^2)^{3/2}} + \dfrac{1}{3}.

We separate variables in dydx=x3y2(1+x2)5/2\dfrac{dy}{dx} = \dfrac{x^3 y^2}{(1+x^2)^{5/2}}:

dyy2=x3(1+x2)5/2 dx\frac{dy}{y^2} = \frac{x^3}{(1+x^2)^{5/2}}\,dx

Integrating both sides:

−1y=∫x3(1+x2)5/2 dx+C.-\frac{1}{y} = \int \frac{x^3}{(1+x^2)^{5/2}}\,dx + C \text{.}

For the integral on the right, substitute w=1+x2w = 1 + x^2, so dw=2x dxdw = 2x\,dx and x2=w−1x^2 = w - 1:

∫x3(1+x2)5/2 dx=∫x2⋅x(1+x2)5/2 dx=∫w−12w5/2 dw=12∫(w−3/2−w−5/2)dw\int \frac{x^3}{(1+x^2)^{5/2}}\,dx = \int \frac{x^2 \cdot x}{(1+x^2)^{5/2}}\,dx = \int \frac{w - 1}{2w^{5/2}}\,dw = \frac{1}{2}\int \left(w^{-3/2} - w^{-5/2}\right) dw

=12[−2w−1/2+23w−3/2]=−w−1/2+13w−3/2=−(1+x2)−1/2+13(1+x2)−3/2.= \frac{1}{2}\left[-2w^{-1/2} + \frac{2}{3}w^{-3/2}\right] = -w^{-1/2} + \frac{1}{3}w^{-3/2} = -(1+x^2)^{-1/2} + \frac{1}{3}(1+x^2)^{-3/2} \text{.}

So:

−1y=−(1+x2)−1/2+13(1+x2)−3/2+C.-\frac{1}{y} = -(1+x^2)^{-1/2} + \frac{1}{3}(1+x^2)^{-3/2} + C \text{.}

Using the initial condition y=1y = 1 when x=0x = 0:

−1=−1+13+C  ⟹  C=−13.-1 = -1 + \frac{1}{3} + C \implies C = -\frac{1}{3} \text{.}

Therefore:

1y=(1+x2)−1/2−13(1+x2)−3/2+13.\frac{1}{y} = (1+x^2)^{-1/2} - \frac{1}{3}(1+x^2)^{-3/2} + \frac{1}{3} \text{.}

Writing (1+x2)−1/2=1+x2(1+x2)3/2(1+x^2)^{-1/2} = \dfrac{1+x^2}{(1+x^2)^{3/2}} to combine the first two terms:

1y=1+x2(1+x2)3/2−13(1+x2)3/2+13=3(1+x2)−13(1+x2)3/2+13\frac{1}{y} = \frac{1+x^2}{(1+x^2)^{3/2}} - \frac{1}{3(1+x^2)^{3/2}} + \frac{1}{3} = \frac{3(1+x^2) - 1}{3(1+x^2)^{3/2}} + \frac{1}{3}

=2+3x23(1+x2)3/2+13.□= \frac{2 + 3x^2}{3(1+x^2)^{3/2}} + \frac{1}{3} \text{.} \qquad \square

Show that y≈3−9xy \approx 3 - \dfrac{9}{x} for large positive xx.

For large xx:

(1+x2)3/2=x3(1+1x2)3/2=x3(1+32x2+O(x−4)),(1+x^2)^{3/2} = x^3\left(1 + \frac{1}{x^2}\right)^{3/2} = x^3\left(1 + \frac{3}{2x^2} + O(x^{-4})\right) \text{,}

so:

2+3x23(1+x2)3/2=3x2+23x3(1+32x2+⋯ )=(1x+23x3)(1−32x2+⋯ )=1x+O(x−3).\frac{2 + 3x^2}{3(1+x^2)^{3/2}} = \frac{3x^2 + 2}{3x^3\left(1 + \frac{3}{2x^2} + \cdots\right)} = \left(\frac{1}{x} + \frac{2}{3x^3}\right)\left(1 - \frac{3}{2x^2} + \cdots\right) = \frac{1}{x} + O(x^{-3}) \text{.}

Therefore:

1y=13+1x+O(x−3).\frac{1}{y} = \frac{1}{3} + \frac{1}{x} + O(x^{-3}) \text{.}

Inverting:

y=113+1x+O(x−3)=3xx+3+O(x−2)=31+3x+O(x−3)y = \frac{1}{\frac{1}{3} + \frac{1}{x} + O(x^{-3})} = \frac{3x}{x + 3 + O(x^{-2})} = \frac{3}{1 + \frac{3}{x} + O(x^{-3})}

=3(1−3x+O(x−2))=3−9x+O(x−2).= 3\left(1 - \frac{3}{x} + O(x^{-2})\right) = 3 - \frac{9}{x} + O(x^{-2}) \text{.}

Hence y≈3−9xy \approx 3 - \dfrac{9}{x} for large positive xx. □\qquad \square

Sketch of CC.

Key features:

  • At x=0x = 0: y=1y = 1, and dydx=0\dfrac{dy}{dx} = 0 (zero gradient at the origin).
  • For x>0x > 0: dydx=x3y2(1+x2)5/2>0\dfrac{dy}{dx} = \dfrac{x^3 y^2}{(1+x^2)^{5/2}} > 0, so yy is strictly increasing.
  • As x→∞x \to \infty: y→3y \to 3 asymptotically, with y≈3−9/xy \approx 3 - 9/x.
  • The curve has one point of inflection (the gradient increases from 00, reaches a maximum, then decreases toward 00 as y→3y \to 3).

The sketch shows a curve starting at (0,1)(0, 1) with zero slope, rising monotonically, bending to approach the horizontal asymptote y=3y = 3 from below.

The zz-equation and its two curves.

Observe that if y=z2y = z^2, then dydx=2zdzdx\dfrac{dy}{dx} = 2z\dfrac{dz}{dx}. The given zz-equation is:

dzdx=x3z32(1+x2)5/2,\frac{dz}{dx} = \frac{x^3 z^3}{2(1+x^2)^{5/2}} \text{,}

so 2zdzdx=x3z4(1+x2)5/2=x3y2(1+x2)5/2=dydx2z\dfrac{dz}{dx} = \dfrac{x^3 z^4}{(1+x^2)^{5/2}} = \dfrac{x^3 y^2}{(1+x^2)^{5/2}} = \dfrac{dy}{dx}.

Therefore y=z2y = z^2 satisfies the yy-equation. Both initial conditions z=1z = 1 and z=−1z = -1 at x=0x = 0 give y=1y = 1 at x=0x = 0, the same initial condition as before.

The two curves are therefore z=+yz = +\sqrt{y} and z=−yz = -\sqrt{y}, where yy is the solution found above.

For large positive xx, using y≈3−9/xy \approx 3 - 9/x:

z=±y≈±3−9x=±31−3x≈±3(1−32x)=±3∓332x.z = \pm\sqrt{y} \approx \pm\sqrt{3 - \frac{9}{x}} = \pm\sqrt{3}\sqrt{1 - \frac{3}{x}} \approx \pm\sqrt{3}\left(1 - \frac{3}{2x}\right) = \pm\sqrt{3} \mp \frac{3\sqrt{3}}{2x} \text{.}

Key features of the zz-sketch:

  • The two curves are reflections of each other in the xx-axis.
  • The upper curve starts at (0,1)(0, 1) with zero gradient, increases monotonically, and is asymptotic to z=3z = \sqrt{3}.
  • The lower curve starts at (0,−1)(0, -1) with zero gradient, decreases monotonically, and is asymptotic to z=−3z = -\sqrt{3}.
  • Each curve has one point of inflection, with the same structure as CC but reflected/scaled appropriately.