Exam : STEP3 | Year : 2002 | Questions : Q1—Q8 | Total marks per question : 20
All questions are pure mathematics. Solutions and examiner commentary are included below.
Q Topic Difficulty Key Techniques 1 微积分 Calculus Challenging 换元积分,分部积分,旋转体体积公式,广义积分 2 级数与数列 Sequences and Series Hard 数学归纳法,反正切加法公式,裂项相消,级数求和 3 函数与方程 Functions and Equations Challenging 根式函数分析,函数图像描绘,不等式分析,代数方程求解 4 数论 Number Theory Hard 不等式放缩,反证法,因式分解,整数分析 5 代数 Algebra Challenging 配方法,待定系数法,多项式恒等式,因式分解 6 微分方程 Differential Equations Challenging 可分离变量法,分情况讨论,解曲线作图 7 三角学与坐标几何 Trigonometry and Coordinate Geometry Challenging 三角恒等式,坐标法,代数恒等变换,不等式放缩 8 复数 Complex Numbers Hard 复数辐角计算,模的运算,几何解释,Ptolemy定理
Topic : 微积分 Calculus | Difficulty : Challenging | Marks : 20
1 Find the area of the region between the curve y = ln x x y = \frac{\ln x}{x} y = x l n x and the x x x -axis, for 1 ⩽ x ⩽ a 1 \leqslant x \leqslant a 1 ⩽ x ⩽ a . What happens to this area as a a a tends to infinity?
Find the volume of the solid obtained when the region between the curve y = ln x x y = \frac{\ln x}{x} y = x l n x and the x x x -axis, for 1 ⩽ x ⩽ a 1 \leqslant x \leqslant a 1 ⩽ x ⩽ a , is rotated through 2 π 2\pi 2 π radians about the x x x -axis. What happens to this volume as a a a tends to infinity?
Model Solution
Part (i): Area
The area is
A = ∫ 1 a ln x x d x = [ ( ln x ) 2 2 ] 1 a = ( ln a ) 2 2 . A = \int_1^a \frac{\ln x}{x}\, dx = \left[\frac{(\ln x)^2}{2}\right]_1^a = \frac{(\ln a)^2}{2}. A = ∫ 1 a x l n x d x = [ 2 ( l n x ) 2 ] 1 a = 2 ( l n a ) 2 .
As a → ∞ a \to \infty a → ∞ , ln a → ∞ \ln a \to \infty ln a → ∞ , so A → ∞ A \to \infty A → ∞ . The area diverges.
Part (ii): Volume of revolution
The volume obtained by rotating about the x x x -axis is
V = π ∫ 1 a ( ln x x ) 2 d x = π ∫ 1 a ( ln x ) 2 x 2 d x . V = \pi \int_1^a \left(\frac{\ln x}{x}\right)^2 dx = \pi \int_1^a \frac{(\ln x)^2}{x^2}\, dx. V = π ∫ 1 a ( x l n x ) 2 d x = π ∫ 1 a x 2 ( l n x ) 2 d x .
We evaluate this by parts. Let u = ( ln x ) 2 u = (\ln x)^2 u = ( ln x ) 2 , d v = x − 2 d x dv = x^{-2}\, dx d v = x − 2 d x , so d u = 2 ln x x d x du = \frac{2\ln x}{x}\, dx d u = x 2 l n x d x , v = − 1 x v = -\frac{1}{x} v = − x 1 . Then
∫ 1 a ( ln x ) 2 x 2 d x = [ − ( ln x ) 2 x ] 1 a + ∫ 1 a 2 ln x x 2 d x = − ( ln a ) 2 a + 2 ∫ 1 a ln x x 2 d x . \int_1^a \frac{(\ln x)^2}{x^2}\, dx = \left[-\frac{(\ln x)^2}{x}\right]_1^a + \int_1^a \frac{2\ln x}{x^2}\, dx = -\frac{(\ln a)^2}{a} + 2\int_1^a \frac{\ln x}{x^2}\, dx. ∫ 1 a x 2 ( l n x ) 2 d x = [ − x ( l n x ) 2 ] 1 a + ∫ 1 a x 2 2 l n x d x = − a ( l n a ) 2 + 2 ∫ 1 a x 2 l n x d x .
For the remaining integral, let u = ln x u = \ln x u = ln x , d v = x − 2 d x dv = x^{-2}\, dx d v = x − 2 d x , so d u = 1 x d x du = \frac{1}{x}\, dx d u = x 1 d x , v = − 1 x v = -\frac{1}{x} v = − x 1 :
∫ 1 a ln x x 2 d x = [ − ln x x ] 1 a + ∫ 1 a 1 x 2 d x = − ln a a + [ − 1 x ] 1 a = − ln a a + 1 − 1 a . \int_1^a \frac{\ln x}{x^2}\, dx = \left[-\frac{\ln x}{x}\right]_1^a + \int_1^a \frac{1}{x^2}\, dx = -\frac{\ln a}{a} + \left[-\frac{1}{x}\right]_1^a = -\frac{\ln a}{a} + 1 - \frac{1}{a}. ∫ 1 a x 2 l n x d x = [ − x l n x ] 1 a + ∫ 1 a x 2 1 d x = − a l n a + [ − x 1 ] 1 a = − a l n a + 1 − a 1 .
Combining:
∫ 1 a ( ln x ) 2 x 2 d x = − ( ln a ) 2 a − 2 ln a a + 2 − 2 a = 2 − ( ln a ) 2 + 2 ln a + 2 a . \int_1^a \frac{(\ln x)^2}{x^2}\, dx = -\frac{(\ln a)^2}{a} - \frac{2\ln a}{a} + 2 - \frac{2}{a} = 2 - \frac{(\ln a)^2 + 2\ln a + 2}{a}. ∫ 1 a x 2 ( l n x ) 2 d x = − a ( l n a ) 2 − a 2 l n a + 2 − a 2 = 2 − a ( l n a ) 2 + 2 l n a + 2 .
Therefore
V = π [ 2 − ( ln a ) 2 + 2 ln a + 2 a ] . V = \pi\left[2 - \frac{(\ln a)^2 + 2\ln a + 2}{a}\right]. V = π [ 2 − a ( l n a ) 2 + 2 l n a + 2 ] .
As a → ∞ a \to \infty a → ∞ , the fraction ( ln a ) 2 + 2 ln a + 2 a → 0 \frac{(\ln a)^2 + 2\ln a + 2}{a} \to 0 a ( l n a ) 2 + 2 l n a + 2 → 0 (since polynomial growth of ln a \ln a ln a is slower than linear growth of a a a ), so V → 2 π V \to 2\pi V → 2 π .
Topic : 级数与数列 Sequences and Series | Difficulty : Hard | Marks : 20
2 Prove that arctan a + arctan b = arctan ( a + b 1 − a b ) \arctan a + \arctan b = \arctan \left( \frac{a + b}{1 - ab} \right) arctan a + arctan b = arctan ( 1 − ab a + b ) when 0 < a < 1 0 < a < 1 0 < a < 1 and 0 < b < 1 0 < b < 1 0 < b < 1 .
Prove by induction that, for n ⩾ 1 n \geqslant 1 n ⩾ 1 ,
∑ r = 1 n arctan ( 1 r 2 + r + 1 ) = arctan ( n n + 2 ) \sum_{r=1}^{n} \arctan \left( \frac{1}{r^2 + r + 1} \right) = \arctan \left( \frac{n}{n + 2} \right) ∑ r = 1 n arctan ( r 2 + r + 1 1 ) = arctan ( n + 2 n )
and hence find
∑ r = 1 ∞ arctan ( 1 r 2 + r + 1 ) . \sum_{r=1}^{\infty} \arctan \left( \frac{1}{r^2 + r + 1} \right) . ∑ r = 1 ∞ arctan ( r 2 + r + 1 1 ) .
Hence prove that
∑ r = 1 ∞ arctan ( 1 r 2 − r + 1 ) = π 2 . \sum_{r=1}^{\infty} \arctan \left( \frac{1}{r^2 - r + 1} \right) = \frac{\pi}{2} . ∑ r = 1 ∞ arctan ( r 2 − r + 1 1 ) = 2 π .
Model Solution
Part (i): The addition formula
Let α = arctan a \alpha = \arctan a α = arctan a and β = arctan b \beta = \arctan b β = arctan b , so tan α = a \tan\alpha = a tan α = a and tan β = b \tan\beta = b tan β = b . Since 0 < a < 1 0 < a < 1 0 < a < 1 and 0 < b < 1 0 < b < 1 0 < b < 1 , we have 0 < α < π / 4 0 < \alpha < \pi/4 0 < α < π /4 and 0 < β < π / 4 0 < \beta < \pi/4 0 < β < π /4 , so 0 < α + β < π / 2 0 < \alpha + \beta < \pi/2 0 < α + β < π /2 .
Using the tangent addition formula:
tan ( α + β ) = tan α + tan β 1 − tan α tan β = a + b 1 − a b . \tan(\alpha + \beta) = \frac{\tan\alpha + \tan\beta}{1 - \tan\alpha\tan\beta} = \frac{a + b}{1 - ab}. tan ( α + β ) = 1 − t a n α t a n β t a n α + t a n β = 1 − ab a + b .
Since 0 < a , b < 1 0 < a, b < 1 0 < a , b < 1 , we have a b < 1 ab < 1 ab < 1 , so 1 − a b > 0 1 - ab > 0 1 − ab > 0 and a + b 1 − a b > 0 \frac{a+b}{1-ab} > 0 1 − ab a + b > 0 . Also α + β ∈ ( 0 , π / 2 ) \alpha + \beta \in (0, \pi/2) α + β ∈ ( 0 , π /2 ) , so
α + β = arctan ( a + b 1 − a b ) . ■ \alpha + \beta = \arctan\left(\frac{a + b}{1 - ab}\right). \qquad \blacksquare α + β = arctan ( 1 − ab a + b ) . ■
Part (ii): Induction proof
Base case (n = 1 n = 1 n = 1 ): arctan ( 1 1 + 1 + 1 ) = arctan ( 1 3 ) = arctan ( 1 1 + 2 ) \arctan\!\left(\frac{1}{1+1+1}\right) = \arctan\!\left(\frac{1}{3}\right) = \arctan\!\left(\frac{1}{1+2}\right) arctan ( 1 + 1 + 1 1 ) = arctan ( 3 1 ) = arctan ( 1 + 2 1 ) . ✓ \checkmark ✓
Inductive step : Assume ∑ r = 1 n arctan ( 1 r 2 + r + 1 ) = arctan ( n n + 2 ) \sum_{r=1}^{n} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n}{n+2}\right) ∑ r = 1 n arctan ( r 2 + r + 1 1 ) = arctan ( n + 2 n ) . Then
∑ r = 1 n + 1 arctan ( 1 r 2 + r + 1 ) = arctan ( n n + 2 ) + arctan ( 1 ( n + 1 ) 2 + ( n + 1 ) + 1 ) . \sum_{r=1}^{n+1} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n}{n+2}\right) + \arctan\!\left(\frac{1}{(n+1)^2+(n+1)+1}\right). ∑ r = 1 n + 1 arctan ( r 2 + r + 1 1 ) = arctan ( n + 2 n ) + arctan ( ( n + 1 ) 2 + ( n + 1 ) + 1 1 ) .
We have ( n + 1 ) 2 + ( n + 1 ) + 1 = n 2 + 3 n + 3 (n+1)^2 + (n+1) + 1 = n^2 + 3n + 3 ( n + 1 ) 2 + ( n + 1 ) + 1 = n 2 + 3 n + 3 , so we need to compute
arctan ( n n + 2 ) + arctan ( 1 n 2 + 3 n + 3 ) . \arctan\!\left(\frac{n}{n+2}\right) + \arctan\!\left(\frac{1}{n^2+3n+3}\right). arctan ( n + 2 n ) + arctan ( n 2 + 3 n + 3 1 ) .
Since 0 < n n + 2 < 1 0 < \frac{n}{n+2} < 1 0 < n + 2 n < 1 and 0 < 1 n 2 + 3 n + 3 < 1 0 < \frac{1}{n^2+3n+3} < 1 0 < n 2 + 3 n + 3 1 < 1 , we apply the addition formula:
n n + 2 + 1 n 2 + 3 n + 3 1 − n ( n + 2 ) ( n 2 + 3 n + 3 ) = n ( n 2 + 3 n + 3 ) + ( n + 2 ) ( n + 2 ) ( n 2 + 3 n + 3 ) − n . \frac{\frac{n}{n+2} + \frac{1}{n^2+3n+3}}{1 - \frac{n}{(n+2)(n^2+3n+3)}} = \frac{n(n^2+3n+3) + (n+2)}{(n+2)(n^2+3n+3) - n}. 1 − ( n + 2 ) ( n 2 + 3 n + 3 ) n n + 2 n + n 2 + 3 n + 3 1 = ( n + 2 ) ( n 2 + 3 n + 3 ) − n n ( n 2 + 3 n + 3 ) + ( n + 2 ) .
Numerator : n 3 + 3 n 2 + 3 n + n + 2 = n 3 + 3 n 2 + 4 n + 2 n^3 + 3n^2 + 3n + n + 2 = n^3 + 3n^2 + 4n + 2 n 3 + 3 n 2 + 3 n + n + 2 = n 3 + 3 n 2 + 4 n + 2 .
Denominator : n 3 + 3 n 2 + 3 n + 2 n 2 + 6 n + 6 − n = n 3 + 5 n 2 + 8 n + 6 n^3 + 3n^2 + 3n + 2n^2 + 6n + 6 - n = n^3 + 5n^2 + 8n + 6 n 3 + 3 n 2 + 3 n + 2 n 2 + 6 n + 6 − n = n 3 + 5 n 2 + 8 n + 6 .
We can verify that n 3 + 3 n 2 + 4 n + 2 n 3 + 5 n 2 + 8 n + 6 = n + 1 n + 3 \frac{n^3 + 3n^2 + 4n + 2}{n^3 + 5n^2 + 8n + 6} = \frac{n+1}{n+3} n 3 + 5 n 2 + 8 n + 6 n 3 + 3 n 2 + 4 n + 2 = n + 3 n + 1 by cross-multiplying:
( n + 1 ) ( n 3 + 5 n 2 + 8 n + 6 ) = n 4 + 6 n 3 + 13 n 2 + 14 n + 6 (n+1)(n^3 + 5n^2 + 8n + 6) = n^4 + 6n^3 + 13n^2 + 14n + 6 ( n + 1 ) ( n 3 + 5 n 2 + 8 n + 6 ) = n 4 + 6 n 3 + 13 n 2 + 14 n + 6 .
( n + 3 ) ( n 3 + 3 n 2 + 4 n + 2 ) = n 4 + 6 n 3 + 13 n 2 + 14 n + 6 (n+3)(n^3 + 3n^2 + 4n + 2) = n^4 + 6n^3 + 13n^2 + 14n + 6 ( n + 3 ) ( n 3 + 3 n 2 + 4 n + 2 ) = n 4 + 6 n 3 + 13 n 2 + 14 n + 6 . ✓ \checkmark ✓
Therefore ∑ r = 1 n + 1 arctan ( 1 r 2 + r + 1 ) = arctan ( n + 1 n + 3 ) \sum_{r=1}^{n+1} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \arctan\!\left(\frac{n+1}{n+3}\right) ∑ r = 1 n + 1 arctan ( r 2 + r + 1 1 ) = arctan ( n + 3 n + 1 ) , completing the induction. ■ \qquad \blacksquare ■
Part (iii): The infinite sum
∑ r = 1 ∞ arctan ( 1 r 2 + r + 1 ) = lim n → ∞ arctan ( n n + 2 ) = arctan ( 1 ) = π 4 . \sum_{r=1}^{\infty} \arctan\!\left(\frac{1}{r^2+r+1}\right) = \lim_{n\to\infty} \arctan\!\left(\frac{n}{n+2}\right) = \arctan(1) = \frac{\pi}{4}. ∑ r = 1 ∞ arctan ( r 2 + r + 1 1 ) = lim n → ∞ arctan ( n + 2 n ) = arctan ( 1 ) = 4 π .
Part (iv): The second identity
Note that 1 r 2 − r + 1 = 1 ( r − 1 ) 2 + ( r − 1 ) + 1 \frac{1}{r^2 - r + 1} = \frac{1}{(r-1)^2 + (r-1) + 1} r 2 − r + 1 1 = ( r − 1 ) 2 + ( r − 1 ) + 1 1 . Substituting s = r − 1 s = r - 1 s = r − 1 :
∑ r = 1 ∞ arctan ( 1 r 2 − r + 1 ) = ∑ s = 0 ∞ arctan ( 1 s 2 + s + 1 ) = arctan ( 1 0 + 0 + 1 ) + ∑ s = 1 ∞ arctan ( 1 s 2 + s + 1 ) \sum_{r=1}^{\infty} \arctan\!\left(\frac{1}{r^2-r+1}\right) = \sum_{s=0}^{\infty} \arctan\!\left(\frac{1}{s^2+s+1}\right) = \arctan\!\left(\frac{1}{0+0+1}\right) + \sum_{s=1}^{\infty} \arctan\!\left(\frac{1}{s^2+s+1}\right) ∑ r = 1 ∞ arctan ( r 2 − r + 1 1 ) = ∑ s = 0 ∞ arctan ( s 2 + s + 1 1 ) = arctan ( 0 + 0 + 1 1 ) + ∑ s = 1 ∞ arctan ( s 2 + s + 1 1 )
= arctan ( 1 ) + π 4 = π 4 + π 4 = π 2 . ■ = \arctan(1) + \frac{\pi}{4} = \frac{\pi}{4} + \frac{\pi}{4} = \frac{\pi}{2}. \qquad \blacksquare = arctan ( 1 ) + 4 π = 4 π + 4 π = 2 π . ■
Topic : 函数与方程 Functions and Equations | Difficulty : Challenging | Marks : 20
3 Let
f ( x ) = a x − x − b , f(x) = a\sqrt{x} - \sqrt{x - b} , f ( x ) = a x − x − b ,
where x ⩾ b > 0 x \geqslant b > 0 x ⩾ b > 0 and a > 1 a > 1 a > 1 . Sketch the graph of f ( x ) f(x) f ( x ) . Hence show that the equation f ( x ) = c f(x) = c f ( x ) = c , where c > 0 c > 0 c > 0 , has no solution when c 2 < b ( a 2 − 1 ) c^2 < b \left( a^2 - 1 \right) c 2 < b ( a 2 − 1 ) . Find conditions on c 2 c^2 c 2 in terms of a a a and b b b for the equation to have exactly one or exactly two solutions.
Solve the equations (i) 3 x − x − 2 = 4 3\sqrt{x} - \sqrt{x - 2} = 4 3 x − x − 2 = 4 and (ii) 3 x − x − 3 = 5 3\sqrt{x} - \sqrt{x - 3} = 5 3 x − x − 3 = 5 .
Model Solution
Part (i): Sketch and analysis
We have f ( x ) = a x − x − b f(x) = a\sqrt{x} - \sqrt{x-b} f ( x ) = a x − x − b for x ⩾ b > 0 x \geqslant b > 0 x ⩾ b > 0 , a > 1 a > 1 a > 1 .
At x = b x = b x = b : f ( b ) = a b f(b) = a\sqrt{b} f ( b ) = a b .
As x → ∞ x \to \infty x → ∞ : f ( x ) = x ( a − 1 − b / x ) → ∞ f(x) = \sqrt{x}(a - \sqrt{1 - b/x}) \to \infty f ( x ) = x ( a − 1 − b / x ) → ∞ since a > 1 a > 1 a > 1 .
Derivative :
f ′ ( x ) = a 2 x − 1 2 x − b = a x − b − x 2 x x − b . f'(x) = \frac{a}{2\sqrt{x}} - \frac{1}{2\sqrt{x-b}} = \frac{a\sqrt{x-b} - \sqrt{x}}{2\sqrt{x}\sqrt{x-b}}. f ′ ( x ) = 2 x a − 2 x − b 1 = 2 x x − b a x − b − x .
Setting f ′ ( x ) = 0 f'(x) = 0 f ′ ( x ) = 0 : a x − b = x a\sqrt{x-b} = \sqrt{x} a x − b = x , so a 2 ( x − b ) = x a^2(x-b) = x a 2 ( x − b ) = x , giving x = a 2 b a 2 − 1 x = \frac{a^2 b}{a^2 - 1} x = a 2 − 1 a 2 b .
Since a > 1 a > 1 a > 1 , we have a 2 a 2 − 1 > 1 \frac{a^2}{a^2-1} > 1 a 2 − 1 a 2 > 1 , so x c = a 2 b a 2 − 1 > b x_c = \frac{a^2 b}{a^2-1} > b x c = a 2 − 1 a 2 b > b . This critical point lies in the domain.
For b ⩽ x < x c b \leqslant x < x_c b ⩽ x < x c : f ′ ( x ) < 0 f'(x) < 0 f ′ ( x ) < 0 (decreasing). For x > x c x > x_c x > x c : f ′ ( x ) > 0 f'(x) > 0 f ′ ( x ) > 0 (increasing).
The minimum value is
f ( x c ) = a a 2 b a 2 − 1 − a 2 b a 2 − 1 − b = a 2 b a 2 − 1 − b a 2 − 1 = ( a 2 − 1 ) b a 2 − 1 = b ( a 2 − 1 ) . f(x_c) = a\sqrt{\frac{a^2 b}{a^2-1}} - \sqrt{\frac{a^2 b}{a^2-1} - b} = \frac{a^2\sqrt{b}}{\sqrt{a^2-1}} - \frac{\sqrt{b}}{\sqrt{a^2-1}} = \frac{(a^2-1)\sqrt{b}}{\sqrt{a^2-1}} = \sqrt{b(a^2-1)}. f ( x c ) = a a 2 − 1 a 2 b − a 2 − 1 a 2 b − b = a 2 − 1 a 2 b − a 2 − 1 b = a 2 − 1 ( a 2 − 1 ) b = b ( a 2 − 1 ) .
The graph starts at ( b , a b ) (b, a\sqrt{b}) ( b , a b ) , decreases to a minimum at x c x_c x c with value b ( a 2 − 1 ) \sqrt{b(a^2-1)} b ( a 2 − 1 ) , then increases to infinity.
Part (ii): Conditions on c c c
The equation f ( x ) = c f(x) = c f ( x ) = c with c > 0 c > 0 c > 0 :
No solution when c < b ( a 2 − 1 ) c < \sqrt{b(a^2-1)} c < b ( a 2 − 1 ) , i.e. c 2 < b ( a 2 − 1 ) c^2 < b(a^2-1) c 2 < b ( a 2 − 1 ) .
Exactly one solution when c = b ( a 2 − 1 ) c = \sqrt{b(a^2-1)} c = b ( a 2 − 1 ) (at the minimum), or when c = a b c = a\sqrt{b} c = a b (at x = b x = b x = b , the function value from the right).
Exactly two solutions when b ( a 2 − 1 ) < c < a b \sqrt{b(a^2-1)} < c < a\sqrt{b} b ( a 2 − 1 ) < c < a b , i.e. b ( a 2 − 1 ) < c 2 < a 2 b b(a^2-1) < c^2 < a^2 b b ( a 2 − 1 ) < c 2 < a 2 b .
Exactly one solution when c > a b c > a\sqrt{b} c > a b , i.e. c 2 > a 2 b c^2 > a^2 b c 2 > a 2 b .
Part (iii): Solving (i) 3 x − x − 2 = 4 3\sqrt{x} - \sqrt{x-2} = 4 3 x − x − 2 = 4
Here a = 3 a = 3 a = 3 , b = 2 b = 2 b = 2 , c = 4 c = 4 c = 4 . We have f ( 2 ) = 3 2 ≈ 4.24 f(2) = 3\sqrt{2} \approx 4.24 f ( 2 ) = 3 2 ≈ 4.24 and b ( a 2 − 1 ) = 16 = 4 \sqrt{b(a^2-1)} = \sqrt{16} = 4 b ( a 2 − 1 ) = 16 = 4 .
Since c = 4 = b ( a 2 − 1 ) c = 4 = \sqrt{b(a^2-1)} c = 4 = b ( a 2 − 1 ) , the equation has exactly one solution (at the minimum).
Rearranging: 3 x = 4 + x − 2 3\sqrt{x} = 4 + \sqrt{x-2} 3 x = 4 + x − 2 . Squaring:
9 x = 16 + 8 x − 2 + x − 2 ⟹ 8 x − 14 = 8 x − 2 ⟹ 4 x − 7 = 4 x − 2 . 9x = 16 + 8\sqrt{x-2} + x - 2 \implies 8x - 14 = 8\sqrt{x-2} \implies 4x - 7 = 4\sqrt{x-2}. 9 x = 16 + 8 x − 2 + x − 2 ⟹ 8 x − 14 = 8 x − 2 ⟹ 4 x − 7 = 4 x − 2 .
Squaring again: 16 x 2 − 56 x + 49 = 16 ( x − 2 ) = 16 x − 32 16x^2 - 56x + 49 = 16(x-2) = 16x - 32 16 x 2 − 56 x + 49 = 16 ( x − 2 ) = 16 x − 32 , so 16 x 2 − 72 x + 81 = 0 16x^2 - 72x + 81 = 0 16 x 2 − 72 x + 81 = 0 .
Discriminant: 72 2 − 4 ( 16 ) ( 81 ) = 5184 − 5184 = 0 72^2 - 4(16)(81) = 5184 - 5184 = 0 7 2 2 − 4 ( 16 ) ( 81 ) = 5184 − 5184 = 0 , so x = 72 32 = 9 4 x = \frac{72}{32} = \frac{9}{4} x = 32 72 = 4 9 .
Check : 3 9 / 4 − 9 / 4 − 2 = 3 ⋅ 3 2 − 1 4 = 9 2 − 1 2 = 4 3\sqrt{9/4} - \sqrt{9/4 - 2} = 3 \cdot \frac{3}{2} - \sqrt{\frac{1}{4}} = \frac{9}{2} - \frac{1}{2} = 4 3 9/4 − 9/4 − 2 = 3 ⋅ 2 3 − 4 1 = 2 9 − 2 1 = 4 . ✓ \checkmark ✓
The unique solution is x = 9 4 x = \dfrac{9}{4} x = 4 9 .
Part (iv): Solving (ii) 3 x − x − 3 = 5 3\sqrt{x} - \sqrt{x-3} = 5 3 x − x − 3 = 5
Here a = 3 a = 3 a = 3 , b = 3 b = 3 b = 3 , c = 5 c = 5 c = 5 . We have f ( 3 ) = 3 3 ≈ 5.20 f(3) = 3\sqrt{3} \approx 5.20 f ( 3 ) = 3 3 ≈ 5.20 and b ( a 2 − 1 ) = 24 = 2 6 ≈ 4.90 \sqrt{b(a^2-1)} = \sqrt{24} = 2\sqrt{6} \approx 4.90 b ( a 2 − 1 ) = 24 = 2 6 ≈ 4.90 .
Since 2 6 < 5 < 3 3 2\sqrt{6} < 5 < 3\sqrt{3} 2 6 < 5 < 3 3 , the equation has exactly two solutions.
Rearranging: 3 x = 5 + x − 3 3\sqrt{x} = 5 + \sqrt{x-3} 3 x = 5 + x − 3 . Squaring:
9 x = 25 + 10 x − 3 + x − 3 ⟹ 8 x − 22 = 10 x − 3 ⟹ 4 x − 11 = 5 x − 3 . 9x = 25 + 10\sqrt{x-3} + x - 3 \implies 8x - 22 = 10\sqrt{x-3} \implies 4x - 11 = 5\sqrt{x-3}. 9 x = 25 + 10 x − 3 + x − 3 ⟹ 8 x − 22 = 10 x − 3 ⟹ 4 x − 11 = 5 x − 3 .
Note: we need 4 x − 11 ⩾ 0 4x - 11 \geqslant 0 4 x − 11 ⩾ 0 , i.e. x ⩾ 11 / 4 x \geqslant 11/4 x ⩾ 11/4 .
Squaring again: 16 x 2 − 88 x + 121 = 25 ( x − 3 ) = 25 x − 75 16x^2 - 88x + 121 = 25(x-3) = 25x - 75 16 x 2 − 88 x + 121 = 25 ( x − 3 ) = 25 x − 75 , so 16 x 2 − 113 x + 196 = 0 16x^2 - 113x + 196 = 0 16 x 2 − 113 x + 196 = 0 .
Discriminant: 113 2 − 4 ( 16 ) ( 196 ) = 12769 − 12544 = 225 = 15 2 113^2 - 4(16)(196) = 12769 - 12544 = 225 = 15^2 11 3 2 − 4 ( 16 ) ( 196 ) = 12769 − 12544 = 225 = 1 5 2 .
x = 113 ± 15 32 ⟹ x = 4 or x = 49 16 . x = \frac{113 \pm 15}{32} \implies x = 4 \quad \text{or} \quad x = \frac{49}{16}. x = 32 113 ± 15 ⟹ x = 4 or x = 16 49 .
Check x = 4 x = 4 x = 4 : 3 4 − 1 = 6 − 1 = 5 3\sqrt{4} - \sqrt{1} = 6 - 1 = 5 3 4 − 1 = 6 − 1 = 5 . ✓ \checkmark ✓
Check x = 49 / 16 x = 49/16 x = 49/16 : 3 49 / 16 − 49 / 16 − 3 = 21 4 − 1 16 = 21 4 − 1 4 = 5 3\sqrt{49/16} - \sqrt{49/16 - 3} = \frac{21}{4} - \sqrt{\frac{1}{16}} = \frac{21}{4} - \frac{1}{4} = 5 3 49/16 − 49/16 − 3 = 4 21 − 16 1 = 4 21 − 4 1 = 5 . ✓ \checkmark ✓
The solutions are x = 49 16 x = \dfrac{49}{16} x = 16 49 and x = 4 x = 4 x = 4 .
Topic : 数论 Number Theory | Difficulty : Hard | Marks : 20
4 Show that if x x x and y y y are positive and x 3 + x 2 = y 3 − y 2 x^3 + x^2 = y^3 - y^2 x 3 + x 2 = y 3 − y 2 then x < y x < y x < y .
Show further that if 0 < x ⩽ y − 1 0 < x \leqslant y - 1 0 < x ⩽ y − 1 , then x 3 + x 2 < y 3 − y 2 x^3 + x^2 < y^3 - y^2 x 3 + x 2 < y 3 − y 2 .
Prove that there does not exist a pair of positive integers such that the difference of their cubes is equal to the sum of their squares.
Find all the pairs of integers such that the difference of their cubes is equal to the sum of their squares.
Model Solution
Part (i): Show that x < y x < y x < y
Suppose for contradiction that x ⩾ y x \geqslant y x ⩾ y . If x = y x = y x = y , then x 3 + x 2 = x 3 − x 2 x^3 + x^2 = x^3 - x^2 x 3 + x 2 = x 3 − x 2 , giving 2 x 2 = 0 2x^2 = 0 2 x 2 = 0 , so x = 0 x = 0 x = 0 , contradicting x > 0 x > 0 x > 0 .
If x > y > 0 x > y > 0 x > y > 0 , then x 3 > y 3 x^3 > y^3 x 3 > y 3 and x 2 > y 2 x^2 > y^2 x 2 > y 2 , so x 3 + x 2 > y 3 + y 2 > y 3 − y 2 x^3 + x^2 > y^3 + y^2 > y^3 - y^2 x 3 + x 2 > y 3 + y 2 > y 3 − y 2 (since y 2 > 0 y^2 > 0 y 2 > 0 ). This contradicts x 3 + x 2 = y 3 − y 2 x^3 + x^2 = y^3 - y^2 x 3 + x 2 = y 3 − y 2 .
Therefore x < y x < y x < y . ■ \qquad \blacksquare ■
Part (ii): Show that 0 < x ⩽ y − 1 0 < x \leqslant y-1 0 < x ⩽ y − 1 implies x 3 + x 2 < y 3 − y 2 x^3 + x^2 < y^3 - y^2 x 3 + x 2 < y 3 − y 2
Since x ⩽ y − 1 x \leqslant y - 1 x ⩽ y − 1 , we have x + 1 ⩽ y x + 1 \leqslant y x + 1 ⩽ y , so
x 3 + x 2 = x 2 ( x + 1 ) ⩽ x 2 y . x^3 + x^2 = x^2(x+1) \leqslant x^2 y. x 3 + x 2 = x 2 ( x + 1 ) ⩽ x 2 y .
Also y 3 − y 2 = y 2 ( y − 1 ) ⩾ y 2 x y^3 - y^2 = y^2(y-1) \geqslant y^2 x y 3 − y 2 = y 2 ( y − 1 ) ⩾ y 2 x (since y − 1 ⩾ x y - 1 \geqslant x y − 1 ⩾ x ).
So x 3 + x 2 ⩽ x 2 y x^3 + x^2 \leqslant x^2 y x 3 + x 2 ⩽ x 2 y and y 3 − y 2 ⩾ x y 2 y^3 - y^2 \geqslant xy^2 y 3 − y 2 ⩾ x y 2 . We need x 2 y < x y 2 x^2 y < xy^2 x 2 y < x y 2 , i.e. x y ( y − x ) > 0 xy(y - x) > 0 x y ( y − x ) > 0 , which holds since x , y > 0 x, y > 0 x , y > 0 and y > x y > x y > x .
But we need strict inequality throughout. Since x ⩽ y − 1 x \leqslant y-1 x ⩽ y − 1 and x > 0 x > 0 x > 0 , we have y > 1 y > 1 y > 1 , so y − 1 > 0 y - 1 > 0 y − 1 > 0 . Also x < y x < y x < y (from Part (i) or directly from x ⩽ y − 1 x \leqslant y-1 x ⩽ y − 1 ).
More precisely: x 2 ( x + 1 ) ⩽ x 2 y x^2(x+1) \leqslant x^2 y x 2 ( x + 1 ) ⩽ x 2 y with equality iff x + 1 = y x + 1 = y x + 1 = y . And y 2 ( y − 1 ) ⩾ x y 2 y^2(y-1) \geqslant xy^2 y 2 ( y − 1 ) ⩾ x y 2 with equality iff x = y − 1 x = y - 1 x = y − 1 . Even if x = y − 1 x = y - 1 x = y − 1 , we get x 2 y x^2 y x 2 y vs x y 2 xy^2 x y 2 , and x 2 y < x y 2 x^2 y < xy^2 x 2 y < x y 2 since x < y x < y x < y . Therefore x 3 + x 2 < y 3 − y 2 x^3 + x^2 < y^3 - y^2 x 3 + x 2 < y 3 − y 2 . ■ \qquad \blacksquare ■
Part (iii): No pair of positive integers
Suppose m , n m, n m , n are positive integers with m 3 − n 3 = m 2 + n 2 m^3 - n^3 = m^2 + n^2 m 3 − n 3 = m 2 + n 2 . Since m 3 − n 3 = ( m − n ) ( m 2 + m n + n 2 ) > 0 m^3 - n^3 = (m-n)(m^2 + mn + n^2) > 0 m 3 − n 3 = ( m − n ) ( m 2 + mn + n 2 ) > 0 and m 2 + n 2 > 0 m^2 + n^2 > 0 m 2 + n 2 > 0 , we need m > n m > n m > n , so m ⩾ n + 1 m \geqslant n + 1 m ⩾ n + 1 .
Setting x = n x = n x = n and y = m y = m y = m in Part (ii): since 0 < n ⩽ m − 1 0 < n \leqslant m - 1 0 < n ⩽ m − 1 , we have n 3 + n 2 < m 3 − m 2 n^3 + n^2 < m^3 - m^2 n 3 + n 2 < m 3 − m 2 .
But we need m 3 − n 3 = m 2 + n 2 m^3 - n^3 = m^2 + n^2 m 3 − n 3 = m 2 + n 2 , i.e. n 3 + n 2 = m 3 − m 2 n^3 + n^2 = m^3 - m^2 n 3 + n 2 = m 3 − m 2 . This contradicts n 3 + n 2 < m 3 − m 2 n^3 + n^2 < m^3 - m^2 n 3 + n 2 < m 3 − m 2 .
Therefore no such pair exists. ■ \qquad \blacksquare ■
Part (iv): Find all integer pairs
The equation is y 3 − x 3 = y 2 + x 2 y^3 - x^3 = y^2 + x^2 y 3 − x 3 = y 2 + x 2 , i.e. y 3 − y 2 = x 3 + x 2 y^3 - y^2 = x^3 + x^2 y 3 − y 2 = x 3 + x 2 , which gives
( y − x ) ( y 2 + x y + x 2 ) = x 2 + y 2 . ( ⋆ ) (y - x)(y^2 + xy + x^2) = x^2 + y^2. \qquad (\star) ( y − x ) ( y 2 + x y + x 2 ) = x 2 + y 2 . ( ⋆ )
Case 1: x = 0 x = 0 x = 0 . Then y 3 = y 2 y^3 = y^2 y 3 = y 2 , so y = 0 y = 0 y = 0 or y = 1 y = 1 y = 1 . Solutions: ( 0 , 0 ) (0, 0) ( 0 , 0 ) and ( 0 , 1 ) (0, 1) ( 0 , 1 ) .
Case 2: y = 0 y = 0 y = 0 . Then − x 3 = x 2 -x^3 = x^2 − x 3 = x 2 , so x = 0 x = 0 x = 0 or x = − 1 x = -1 x = − 1 . Solution: ( − 1 , 0 ) (-1, 0) ( − 1 , 0 ) .
Case 3: x > 0 x > 0 x > 0 . From Part (iii), no positive integer pair exists.
Case 4: x < 0 x < 0 x < 0 , y > 0 y > 0 y > 0 . Let x = − p x = -p x = − p with p ⩾ 1 p \geqslant 1 p ⩾ 1 . Then ( ⋆ ) (\star) ( ⋆ ) becomes
( y + p ) ( y 2 − p y + p 2 ) = p 2 + y 2 . (y + p)(y^2 - py + p^2) = p^2 + y^2. ( y + p ) ( y 2 − p y + p 2 ) = p 2 + y 2 .
The left side equals y 3 + p 3 ⩾ 1 + 1 = 2 y^3 + p^3 \geqslant 1 + 1 = 2 y 3 + p 3 ⩾ 1 + 1 = 2 , while p 2 + y 2 ⩾ 2 p^2 + y^2 \geqslant 2 p 2 + y 2 ⩾ 2 . For p ⩾ 2 , y ⩾ 2 p \geqslant 2, y \geqslant 2 p ⩾ 2 , y ⩾ 2 : y 3 + p 3 ⩾ 16 > 8 ⩾ p 2 + y 2 y^3 + p^3 \geqslant 16 > 8 \geqslant p^2 + y^2 y 3 + p 3 ⩾ 16 > 8 ⩾ p 2 + y 2 . So we only need to check small values.
p = 1 , y = 1 p = 1, y = 1 p = 1 , y = 1 : ( 1 + 1 ) ( 1 − 1 + 1 ) = 2 (1+1)(1-1+1) = 2 ( 1 + 1 ) ( 1 − 1 + 1 ) = 2 and 1 + 1 = 2 1 + 1 = 2 1 + 1 = 2 . ✓ \checkmark ✓ Solution: ( − 1 , 1 ) (-1, 1) ( − 1 , 1 ) .
p = 1 , y ⩾ 2 p = 1, y \geqslant 2 p = 1 , y ⩾ 2 : ( y + 1 ) ( y 2 − y + 1 ) = y 3 + 1 > y 2 + 1 (y+1)(y^2 - y + 1) = y^3 + 1 > y^2 + 1 ( y + 1 ) ( y 2 − y + 1 ) = y 3 + 1 > y 2 + 1 . No solution.
p = 2 , y = 1 p = 2, y = 1 p = 2 , y = 1 : ( 3 ) ( 4 − 2 + 1 ) = 9 (3)(4-2+1) = 9 ( 3 ) ( 4 − 2 + 1 ) = 9 and 4 + 1 = 5 4 + 1 = 5 4 + 1 = 5 . No solution.
p ⩾ 2 , y = 1 p \geqslant 2, y = 1 p ⩾ 2 , y = 1 : ( 1 + p ) ( 1 − p + p 2 ) = 1 + p 3 ⩾ 9 > p 2 + 1 (1+p)(1-p+p^2) = 1 + p^3 \geqslant 9 > p^2 + 1 ( 1 + p ) ( 1 − p + p 2 ) = 1 + p 3 ⩾ 9 > p 2 + 1 . No solution.
Case 5: x < 0 x < 0 x < 0 , y < 0 y < 0 y < 0 . Let x = − p , y = − q x = -p, y = -q x = − p , y = − q with p , q ⩾ 1 p, q \geqslant 1 p , q ⩾ 1 . Then
( − q + p ) ( q 2 − p q + p 2 ) = p 2 + q 2 , i.e. ( p − q ) ( p 2 − p q + q 2 ) = p 2 + q 2 . (-q+p)(q^2 - pq + p^2) = p^2 + q^2, \quad \text{i.e.} \quad (p-q)(p^2 - pq + q^2) = p^2 + q^2. ( − q + p ) ( q 2 − pq + p 2 ) = p 2 + q 2 , i.e. ( p − q ) ( p 2 − pq + q 2 ) = p 2 + q 2 .
This is p 3 − q 3 = p 2 + q 2 p^3 - q^3 = p^2 + q^2 p 3 − q 3 = p 2 + q 2 . If p = q p = q p = q : 0 = 2 p 2 0 = 2p^2 0 = 2 p 2 , impossible. If p > q p > q p > q : by Part (iii) applied to positive integers q , p q, p q , p with p 3 − q 3 = p 2 + q 2 p^3 - q^3 = p^2 + q^2 p 3 − q 3 = p 2 + q 2 , no solution exists (same argument). If p < q p < q p < q : left side is negative, right side is positive. No solution.
Case 6: x < 0 x < 0 x < 0 , y = 0 y = 0 y = 0 . Already covered in Case 2.
Therefore the complete set of integer solutions is
( x , y ) ∈ { ( 0 , 0 ) , ( 0 , 1 ) , ( − 1 , 0 ) , ( − 1 , 1 ) } . (x, y) \in \{(0, 0),\ (0, 1),\ (-1, 0),\ (-1, 1)\}. ( x , y ) ∈ {( 0 , 0 ) , ( 0 , 1 ) , ( − 1 , 0 ) , ( − 1 , 1 )} .
Topic : 代数 Algebra | Difficulty : Challenging | Marks : 20
5 Give a condition that must be satisfied by p p p , q q q and r r r for it to be possible to write the quadratic polynomial p x 2 + q x + r px^2 + qx + r p x 2 + q x + r in the form p ( x + h ) 2 p(x + h)^2 p ( x + h ) 2 , for some h h h .
Obtain an equation, which you need not simplify, that must be satisfied by t t t if it is possible to write
( x 2 + 1 2 b x + t ) 2 − ( x 4 + b x 3 + c x 2 + d x + e ) \left(x^2 + \frac{1}{2}bx + t\right)^2 - \left(x^4 + bx^3 + cx^2 + dx + e\right) ( x 2 + 2 1 b x + t ) 2 − ( x 4 + b x 3 + c x 2 + d x + e )
in the form k ( x + h ) 2 k(x + h)^2 k ( x + h ) 2 , for some k k k and h h h .
Hence, or otherwise, write x 4 + 6 x 3 + 9 x 2 − 2 x − 7 x^4 + 6x^3 + 9x^2 - 2x - 7 x 4 + 6 x 3 + 9 x 2 − 2 x − 7 as a product of two quadratic factors.
Model Solution
Part (i): Condition for p x 2 + q x + r = p ( x + h ) 2 px^2 + qx + r = p(x+h)^2 p x 2 + q x + r = p ( x + h ) 2
Expanding: p ( x + h ) 2 = p x 2 + 2 p h x + p h 2 p(x+h)^2 = px^2 + 2phx + ph^2 p ( x + h ) 2 = p x 2 + 2 p h x + p h 2 . Comparing coefficients with p x 2 + q x + r px^2 + qx + r p x 2 + q x + r :
q = 2 p h , r = p h 2 . q = 2ph, \qquad r = ph^2. q = 2 p h , r = p h 2 .
From the first equation h = q / ( 2 p ) h = q/(2p) h = q / ( 2 p ) , so r = p ⋅ q 2 / ( 4 p 2 ) = q 2 / ( 4 p ) r = p \cdot q^2/(4p^2) = q^2/(4p) r = p ⋅ q 2 / ( 4 p 2 ) = q 2 / ( 4 p ) .
The necessary and sufficient condition is q 2 = 4 p r q^2 = 4pr q 2 = 4 p r , i.e. the discriminant is zero. ■ \qquad \blacksquare ■
Part (ii): Equation for t t t
We want
( x 2 + 1 2 b x + t ) 2 − ( x 4 + b x 3 + c x 2 + d x + e ) = k ( x + h ) 2 . \left(x^2 + \tfrac{1}{2}bx + t\right)^2 - \left(x^4 + bx^3 + cx^2 + dx + e\right) = k(x+h)^2. ( x 2 + 2 1 b x + t ) 2 − ( x 4 + b x 3 + c x 2 + d x + e ) = k ( x + h ) 2 .
The left side must be a perfect square (as a quadratic in x x x ). Expanding the square:
( x 2 + 1 2 b x + t ) 2 = x 4 + b x 3 + ( 1 4 b 2 + 2 t ) x 2 + b t x + t 2 . \left(x^2 + \tfrac{1}{2}bx + t\right)^2 = x^4 + bx^3 + \left(\tfrac{1}{4}b^2 + 2t\right)x^2 + btx + t^2. ( x 2 + 2 1 b x + t ) 2 = x 4 + b x 3 + ( 4 1 b 2 + 2 t ) x 2 + b t x + t 2 .
Subtracting:
( 1 4 b 2 + 2 t − c ) x 2 + ( b t − d ) x + ( t 2 − e ) = k ( x + h ) 2 . \left(\tfrac{1}{4}b^2 + 2t - c\right)x^2 + (bt - d)x + (t^2 - e) = k(x+h)^2. ( 4 1 b 2 + 2 t − c ) x 2 + ( b t − d ) x + ( t 2 − e ) = k ( x + h ) 2 .
From Part (i), the condition for this quadratic A x 2 + B x + C Ax^2 + Bx + C A x 2 + B x + C to be a perfect square is B 2 = 4 A C B^2 = 4AC B 2 = 4 A C :
( b t − d ) 2 = 4 ( 1 4 b 2 + 2 t − c ) ( t 2 − e ) . ■ (bt - d)^2 = 4\left(\tfrac{1}{4}b^2 + 2t - c\right)(t^2 - e). \qquad \blacksquare ( b t − d ) 2 = 4 ( 4 1 b 2 + 2 t − c ) ( t 2 − e ) . ■
Part (iii): Factorizing x 4 + 6 x 3 + 9 x 2 − 2 x − 7 x^4 + 6x^3 + 9x^2 - 2x - 7 x 4 + 6 x 3 + 9 x 2 − 2 x − 7
Here b = 6 b = 6 b = 6 , c = 9 c = 9 c = 9 , d = − 2 d = -2 d = − 2 , e = − 7 e = -7 e = − 7 . The condition becomes
( 6 t + 2 ) 2 = 4 ( 9 + 2 t − 9 ) ( t 2 + 7 ) = 4 ⋅ 2 t ⋅ ( t 2 + 7 ) . (6t + 2)^2 = 4(9 + 2t - 9)(t^2 + 7) = 4 \cdot 2t \cdot (t^2 + 7). ( 6 t + 2 ) 2 = 4 ( 9 + 2 t − 9 ) ( t 2 + 7 ) = 4 ⋅ 2 t ⋅ ( t 2 + 7 ) .
Simplifying: ( 3 t + 1 ) 2 = 2 t ( t 2 + 7 ) (3t+1)^2 = 2t(t^2 + 7) ( 3 t + 1 ) 2 = 2 t ( t 2 + 7 ) , i.e. 9 t 2 + 6 t + 1 = 2 t 3 + 14 t 9t^2 + 6t + 1 = 2t^3 + 14t 9 t 2 + 6 t + 1 = 2 t 3 + 14 t .
2 t 3 − 9 t 2 + 8 t − 1 = 0. 2t^3 - 9t^2 + 8t - 1 = 0. 2 t 3 − 9 t 2 + 8 t − 1 = 0.
Testing t = − 1 t = -1 t = − 1 : − 2 − 9 − 8 − 1 ≠ 0 -2 - 9 - 8 - 1 \neq 0 − 2 − 9 − 8 − 1 = 0 . Wait, let me recheck: 2 ( − 1 ) 3 − 9 ( − 1 ) 2 + 8 ( − 1 ) − 1 = − 2 − 9 − 8 − 1 = − 20 2(-1)^3 - 9(-1)^2 + 8(-1) - 1 = -2 - 9 - 8 - 1 = -20 2 ( − 1 ) 3 − 9 ( − 1 ) 2 + 8 ( − 1 ) − 1 = − 2 − 9 − 8 − 1 = − 20 . That’s wrong.
Let me recompute: ( 6 t + 2 ) 2 = 36 t 2 + 24 t + 4 (6t+2)^2 = 36t^2 + 24t + 4 ( 6 t + 2 ) 2 = 36 t 2 + 24 t + 4 and 8 t ( t 2 + 7 ) = 8 t 3 + 56 t 8t(t^2+7) = 8t^3 + 56t 8 t ( t 2 + 7 ) = 8 t 3 + 56 t . So 8 t 3 + 56 t = 36 t 2 + 24 t + 4 8t^3 + 56t = 36t^2 + 24t + 4 8 t 3 + 56 t = 36 t 2 + 24 t + 4 , giving 8 t 3 − 36 t 2 + 32 t − 4 = 0 8t^3 - 36t^2 + 32t - 4 = 0 8 t 3 − 36 t 2 + 32 t − 4 = 0 , i.e. 2 t 3 − 9 t 2 + 8 t − 1 = 0 2t^3 - 9t^2 + 8t - 1 = 0 2 t 3 − 9 t 2 + 8 t − 1 = 0 .
Testing t = 1 2 t = \frac{1}{2} t = 2 1 : 2 ⋅ 1 8 − 9 ⋅ 1 4 + 8 ⋅ 1 2 − 1 = 1 4 − 9 4 + 4 − 1 = − 2 + 3 = 1 ≠ 0 2 \cdot \frac{1}{8} - 9 \cdot \frac{1}{4} + 8 \cdot \frac{1}{2} - 1 = \frac{1}{4} - \frac{9}{4} + 4 - 1 = -2 + 3 = 1 \neq 0 2 ⋅ 8 1 − 9 ⋅ 4 1 + 8 ⋅ 2 1 − 1 = 4 1 − 4 9 + 4 − 1 = − 2 + 3 = 1 = 0 .
Let me try the factorization directly. We seek x 4 + 6 x 3 + 9 x 2 − 2 x − 7 = ( x 2 + a x + p ) ( x 2 + c x + q ) x^4 + 6x^3 + 9x^2 - 2x - 7 = (x^2 + ax + p)(x^2 + cx + q) x 4 + 6 x 3 + 9 x 2 − 2 x − 7 = ( x 2 + a x + p ) ( x 2 + c x + q ) with a + c = 6 a + c = 6 a + c = 6 . Taking a = c = 3 a = c = 3 a = c = 3 :
( x 2 + 3 x + p ) ( x 2 + 3 x + q ) = x 4 + 6 x 3 + ( 9 + p + q ) x 2 + 3 ( p + q ) x + p q . (x^2 + 3x + p)(x^2 + 3x + q) = x^4 + 6x^3 + (9 + p + q)x^2 + 3(p+q)x + pq. ( x 2 + 3 x + p ) ( x 2 + 3 x + q ) = x 4 + 6 x 3 + ( 9 + p + q ) x 2 + 3 ( p + q ) x + pq .
Matching: 9 + p + q = 9 9 + p + q = 9 9 + p + q = 9 so p + q = 0 p + q = 0 p + q = 0 , giving q = − p q = -p q = − p . Then 3 ( p + q ) = 0 3(p+q) = 0 3 ( p + q ) = 0 , but we need − 2 -2 − 2 . So a = c = 3 a = c = 3 a = c = 3 doesn’t work directly.
Let a = 3 + δ a = 3 + \delta a = 3 + δ , c = 3 − δ c = 3 - \delta c = 3 − δ . Then the x 2 x^2 x 2 coefficient is a c + p + q = 9 − δ 2 + p + q = 9 ac + p + q = 9 - \delta^2 + p + q = 9 a c + p + q = 9 − δ 2 + p + q = 9 , so p + q = δ 2 p + q = \delta^2 p + q = δ 2 . The x x x coefficient is a q + c p = ( 3 + δ ) q + ( 3 − δ ) p = 3 ( p + q ) + δ ( q − p ) = 3 δ 2 + δ ( q − p ) = − 2 aq + cp = (3+\delta)q + (3-\delta)p = 3(p+q) + \delta(q-p) = 3\delta^2 + \delta(q-p) = -2 a q + c p = ( 3 + δ ) q + ( 3 − δ ) p = 3 ( p + q ) + δ ( q − p ) = 3 δ 2 + δ ( q − p ) = − 2 .
With p + q = δ 2 p + q = \delta^2 p + q = δ 2 and p q = − 7 pq = -7 pq = − 7 : p p p and q q q are roots of z 2 − δ 2 z − 7 = 0 z^2 - \delta^2 z - 7 = 0 z 2 − δ 2 z − 7 = 0 , so q − p = δ 4 + 28 q - p = \sqrt{\delta^4 + 28} q − p = δ 4 + 28 (taking q > p q > p q > p ).
From 3 δ 2 + δ δ 4 + 28 = − 2 3\delta^2 + \delta\sqrt{\delta^4 + 28} = -2 3 δ 2 + δ δ 4 + 28 = − 2 , we need δ < 0 \delta < 0 δ < 0 . Let δ = − ϵ \delta = -\epsilon δ = − ϵ with ϵ > 0 \epsilon > 0 ϵ > 0 : 3 ϵ 2 − ϵ ϵ 4 + 28 = − 2 3\epsilon^2 - \epsilon\sqrt{\epsilon^4 + 28} = -2 3 ϵ 2 − ϵ ϵ 4 + 28 = − 2 , so ϵ ϵ 4 + 28 = 3 ϵ 2 + 2 \epsilon\sqrt{\epsilon^4 + 28} = 3\epsilon^2 + 2 ϵ ϵ 4 + 28 = 3 ϵ 2 + 2 .
Squaring: ϵ 2 ( ϵ 4 + 28 ) = 9 ϵ 4 + 12 ϵ 2 + 4 \epsilon^2(\epsilon^4 + 28) = 9\epsilon^4 + 12\epsilon^2 + 4 ϵ 2 ( ϵ 4 + 28 ) = 9 ϵ 4 + 12 ϵ 2 + 4 , giving ϵ 6 + 28 ϵ 2 = 9 ϵ 4 + 12 ϵ 2 + 4 \epsilon^6 + 28\epsilon^2 = 9\epsilon^4 + 12\epsilon^2 + 4 ϵ 6 + 28 ϵ 2 = 9 ϵ 4 + 12 ϵ 2 + 4 , i.e. ϵ 6 − 9 ϵ 4 + 16 ϵ 2 − 4 = 0 \epsilon^6 - 9\epsilon^4 + 16\epsilon^2 - 4 = 0 ϵ 6 − 9 ϵ 4 + 16 ϵ 2 − 4 = 0 .
Let u = ϵ 2 u = \epsilon^2 u = ϵ 2 : u 3 − 9 u 2 + 16 u − 4 = 0 u^3 - 9u^2 + 16u - 4 = 0 u 3 − 9 u 2 + 16 u − 4 = 0 . Testing u = 1 u = 1 u = 1 : 1 − 9 + 16 − 4 = 4 ≠ 0 1 - 9 + 16 - 4 = 4 \neq 0 1 − 9 + 16 − 4 = 4 = 0 . Testing u = 2 u = 2 u = 2 : 8 − 36 + 32 − 4 = 0 8 - 36 + 32 - 4 = 0 8 − 36 + 32 − 4 = 0 . ✓ \checkmark ✓
So u = 2 u = 2 u = 2 , ϵ = 2 \epsilon = \sqrt{2} ϵ = 2 , δ = − 2 \delta = -\sqrt{2} δ = − 2 .
Then p + q = 2 p + q = 2 p + q = 2 , p q = − 7 pq = -7 pq = − 7 , so p , q p, q p , q are roots of z 2 − 2 z − 7 = 0 z^2 - 2z - 7 = 0 z 2 − 2 z − 7 = 0 : z = 1 ± 2 2 z = 1 \pm 2\sqrt{2} z = 1 ± 2 2 .
Taking p = 1 − 2 2 p = 1 - 2\sqrt{2} p = 1 − 2 2 , q = 1 + 2 2 q = 1 + 2\sqrt{2} q = 1 + 2 2 , a = 3 − 2 a = 3 - \sqrt{2} a = 3 − 2 , c = 3 + 2 c = 3 + \sqrt{2} c = 3 + 2 :
x 4 + 6 x 3 + 9 x 2 − 2 x − 7 = ( x 2 + ( 3 − 2 ) x + 1 − 2 2 ) ( x 2 + ( 3 + 2 ) x + 1 + 2 2 ) . x^4 + 6x^3 + 9x^2 - 2x - 7 = \left(x^2 + (3-\sqrt{2})x + 1 - 2\sqrt{2}\right)\left(x^2 + (3+\sqrt{2})x + 1 + 2\sqrt{2}\right). x 4 + 6 x 3 + 9 x 2 − 2 x − 7 = ( x 2 + ( 3 − 2 ) x + 1 − 2 2 ) ( x 2 + ( 3 + 2 ) x + 1 + 2 2 ) .
Verification : The x x x coefficient is ( 3 − 2 ) ( 1 + 2 2 ) + ( 3 + 2 ) ( 1 − 2 2 ) (3-\sqrt{2})(1+2\sqrt{2}) + (3+\sqrt{2})(1-2\sqrt{2}) ( 3 − 2 ) ( 1 + 2 2 ) + ( 3 + 2 ) ( 1 − 2 2 ) .
( 3 − 2 ) ( 1 + 2 2 ) = 3 + 6 2 − 2 − 4 = − 1 + 5 2 (3-\sqrt{2})(1+2\sqrt{2}) = 3 + 6\sqrt{2} - \sqrt{2} - 4 = -1 + 5\sqrt{2} ( 3 − 2 ) ( 1 + 2 2 ) = 3 + 6 2 − 2 − 4 = − 1 + 5 2 .
( 3 + 2 ) ( 1 − 2 2 ) = 3 − 6 2 + 2 − 4 = − 1 − 5 2 (3+\sqrt{2})(1-2\sqrt{2}) = 3 - 6\sqrt{2} + \sqrt{2} - 4 = -1 - 5\sqrt{2} ( 3 + 2 ) ( 1 − 2 2 ) = 3 − 6 2 + 2 − 4 = − 1 − 5 2 .
Sum = − 2 = -2 = − 2 . ✓ \checkmark ✓
The constant term: ( 1 − 2 2 ) ( 1 + 2 2 ) = 1 − 8 = − 7 (1-2\sqrt{2})(1+2\sqrt{2}) = 1 - 8 = -7 ( 1 − 2 2 ) ( 1 + 2 2 ) = 1 − 8 = − 7 . ✓ \checkmark ✓
Topic : 微分方程 Differential Equations | Difficulty : Challenging | Marks : 20
6 Find all the solution curves of the differential equation
y 4 ( d y d x ) 4 = ( y 2 − 1 ) 2 y^4 \left(\frac{dy}{dx}\right)^4 = \left(y^2 - 1\right)^2 y 4 ( d x d y ) 4 = ( y 2 − 1 ) 2
that pass through either of the points
(i) ( 0 , 3 2 ) \left(0, \frac{\sqrt{3}}{2}\right) ( 0 , 2 3 ) ,
(ii) ( 0 , 5 2 ) \left(0, \frac{\sqrt{5}}{2}\right) ( 0 , 2 5 ) .
Show also that y = 1 y = 1 y = 1 and y = − 1 y = -1 y = − 1 are solutions of the differential equation. Sketch all these solution curves on a single set of axes.
Model Solution
Part (i): Solving the differential equation
The equation y 4 ( d y d x ) 4 = ( y 2 − 1 ) 2 y^4\left(\frac{dy}{dx}\right)^4 = (y^2-1)^2 y 4 ( d x d y ) 4 = ( y 2 − 1 ) 2 can be written as ( y d y d x ) 4 = ( y 2 − 1 ) 2 \left(y\frac{dy}{dx}\right)^4 = (y^2-1)^2 ( y d x d y ) 4 = ( y 2 − 1 ) 2 .
Taking square roots (both sides are non-negative): ( y d y d x ) 2 = ∣ y 2 − 1 ∣ \left(y\frac{dy}{dx}\right)^2 = |y^2 - 1| ( y d x d y ) 2 = ∣ y 2 − 1∣ .
So y d y d x = ± ∣ y 2 − 1 ∣ y\frac{dy}{dx} = \pm\sqrt{|y^2-1|} y d x d y = ± ∣ y 2 − 1∣ , which gives four ODEs depending on the signs.
Case A: ∣ y ∣ > 1 |y| > 1 ∣ y ∣ > 1 (so y 2 − 1 > 0 y^2 - 1 > 0 y 2 − 1 > 0 )
y d y d x = ± y 2 − 1 y\frac{dy}{dx} = \pm\sqrt{y^2-1} y d x d y = ± y 2 − 1 , i.e. y y 2 − 1 d y = ± d x \frac{y}{\sqrt{y^2-1}}\, dy = \pm\, dx y 2 − 1 y d y = ± d x .
Integrating: y 2 − 1 = ± x + C \sqrt{y^2-1} = \pm x + C y 2 − 1 = ± x + C , so
y 2 = ( x − C ) 2 + 1 (choosing appropriate sign) . ( ⋆ ) y^2 = (x - C)^2 + 1 \qquad \text{(choosing appropriate sign)}. \qquad (\star) y 2 = ( x − C ) 2 + 1 (choosing appropriate sign) . ( ⋆ )
Case B: ∣ y ∣ < 1 |y| < 1 ∣ y ∣ < 1 (so 1 − y 2 > 0 1 - y^2 > 0 1 − y 2 > 0 )
y d y d x = ± 1 − y 2 y\frac{dy}{dx} = \pm\sqrt{1-y^2} y d x d y = ± 1 − y 2 , i.e. y 1 − y 2 d y = ± d x \frac{y}{\sqrt{1-y^2}}\, dy = \pm\, dx 1 − y 2 y d y = ± d x .
Integrating: − 1 − y 2 = ± x + C -\sqrt{1-y^2} = \pm x + C − 1 − y 2 = ± x + C , so 1 − y 2 = ∓ x + C ′ \sqrt{1-y^2} = \mp x + C' 1 − y 2 = ∓ x + C ′ , giving
y 2 = 1 − ( x − C ) 2 . ( ⋆ ⋆ ) y^2 = 1 - (x - C)^2. \qquad (\star\star) y 2 = 1 − ( x − C ) 2 . ( ⋆ ⋆ )
Solution curves through ( 0 , 3 / 2 ) (0, \sqrt{3}/2) ( 0 , 3 /2 )
Since y = 3 / 2 < 1 y = \sqrt{3}/2 < 1 y = 3 /2 < 1 , we use Case B. From ( ⋆ ⋆ ) (\star\star) ( ⋆ ⋆ ) : 3 4 = 1 − C 2 \frac{3}{4} = 1 - C^2 4 3 = 1 − C 2 , so C = ± 1 2 C = \pm\frac{1}{2} C = ± 2 1 .
This gives two circles:
( x − 1 2 ) 2 + y 2 = 1 and ( x + 1 2 ) 2 + y 2 = 1. \left(x - \tfrac{1}{2}\right)^2 + y^2 = 1 \qquad \text{and} \qquad \left(x + \tfrac{1}{2}\right)^2 + y^2 = 1. ( x − 2 1 ) 2 + y 2 = 1 and ( x + 2 1 ) 2 + y 2 = 1.
Both are valid solution curves (the upper semicircles satisfy the ODE with y > 0 y > 0 y > 0 ).
Solution curves through ( 0 , 5 / 2 ) (0, \sqrt{5}/2) ( 0 , 5 /2 )
Since y = 5 / 2 > 1 y = \sqrt{5}/2 > 1 y = 5 /2 > 1 , we use Case A. From ( ⋆ ) (\star) ( ⋆ ) : 5 4 = C 2 + 1 \frac{5}{4} = C^2 + 1 4 5 = C 2 + 1 , so C = ± 1 2 C = \pm\frac{1}{2} C = ± 2 1 .
This gives two hyperbolas:
y 2 − ( x − 1 2 ) 2 = 1 and y 2 − ( x + 1 2 ) 2 = 1. y^2 - \left(x - \tfrac{1}{2}\right)^2 = 1 \qquad \text{and} \qquad y^2 - \left(x + \tfrac{1}{2}\right)^2 = 1. y 2 − ( x − 2 1 ) 2 = 1 and y 2 − ( x + 2 1 ) 2 = 1.
Part (ii): Constant solutions
If y = 1 y = 1 y = 1 : LHS = 1 ⋅ 0 = 0 = 1 \cdot 0 = 0 = 1 ⋅ 0 = 0 , RHS = 0 = 0 = 0 . ✓ \checkmark ✓
If y = − 1 y = -1 y = − 1 : LHS = 1 ⋅ 0 = 0 = 1 \cdot 0 = 0 = 1 ⋅ 0 = 0 , RHS = 0 = 0 = 0 . ✓ \checkmark ✓
Part (iii): Sketch
The solution curves are:
Two circles: ( x ± 1 2 ) 2 + y 2 = 1 \left(x \pm \frac{1}{2}\right)^2 + y^2 = 1 ( x ± 2 1 ) 2 + y 2 = 1 (valid for ∣ y ∣ < 1 |y| < 1 ∣ y ∣ < 1 )
Two hyperbolas: y 2 − ( x ± 1 2 ) 2 = 1 y^2 - \left(x \pm \frac{1}{2}\right)^2 = 1 y 2 − ( x ± 2 1 ) 2 = 1 (valid for ∣ y ∣ > 1 |y| > 1 ∣ y ∣ > 1 )
Two horizontal lines: y = 1 y = 1 y = 1 and y = − 1 y = -1 y = − 1
The circles are centred at ( ± 1 / 2 , 0 ) (\pm 1/2, 0) ( ± 1/2 , 0 ) with radius 1, fitting within the strip ∣ y ∣ < 1 |y| < 1 ∣ y ∣ < 1 . The hyperbolas have vertices at ( ± 1 / 2 , ± 1 ) (\pm 1/2, \pm 1) ( ± 1/2 , ± 1 ) and open vertically. The lines y = ± 1 y = \pm 1 y = ± 1 are asymptotes that the hyperbolas approach and that separate the circular from the hyperbolic regions.
The curve through ( 0 , 3 / 2 ) (0, \sqrt{3}/2) ( 0 , 3 /2 ) consists of the upper arcs of both circles. The curve through ( 0 , 5 / 2 ) (0, \sqrt{5}/2) ( 0 , 5 /2 ) consists of the upper branches of both hyperbolas.
Topic : 三角学与坐标几何 Trigonometry and Coordinate Geometry | Difficulty : Challenging | Marks : 20
7 Given that α \alpha α and β \beta β are acute angles, show that α + β = π / 2 \alpha + \beta = \pi/2 α + β = π /2 if and only if cos 2 α + cos 2 β = 1 \cos^2 \alpha + \cos^2 \beta = 1 cos 2 α + cos 2 β = 1 .
In the x x x –y y y plane, the point A A A has coordinates ( 0 , s ) (0, s) ( 0 , s ) and the point C C C has coordinates ( s , 0 ) (s, 0) ( s , 0 ) , where s > 0 s > 0 s > 0 . The point B B B lies in the first quadrant (x > 0 , y > 0 x > 0, y > 0 x > 0 , y > 0 ). The lengths of A B AB A B , O B OB O B and C B CB C B are respectively a , b a, b a , b and c c c .
Show that
( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2 (s^2 + b^2 - a^2)^2 + (s^2 + b^2 - c^2)^2 = 4s^2b^2 ( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2
and hence that
( 2 s 2 − a 2 − c 2 ) 2 + ( 2 b 2 − a 2 − c 2 ) 2 = 4 a 2 c 2 . (2s^2 - a^2 - c^2)^2 + (2b^2 - a^2 - c^2)^2 = 4a^2c^2 . ( 2 s 2 − a 2 − c 2 ) 2 + ( 2 b 2 − a 2 − c 2 ) 2 = 4 a 2 c 2 .
Deduce that
( a − c ) 2 ⩽ 2 b 2 ⩽ ( a + c ) 2 . (a - c)^2 \leqslant 2b^2 \leqslant (a + c)^2 . ( a − c ) 2 ⩽ 2 b 2 ⩽ ( a + c ) 2 .
Model Solution
Part (i): α + β = π / 2 \alpha + \beta = \pi/2 α + β = π /2 if and only if cos 2 α + cos 2 β = 1 \cos^2\alpha + \cos^2\beta = 1 cos 2 α + cos 2 β = 1
Forward direction. Suppose α + β = π / 2 \alpha + \beta = \pi/2 α + β = π /2 . Then β = π / 2 − α \beta = \pi/2 - \alpha β = π /2 − α , so
cos β = cos ( π 2 − α ) = sin α . \cos\beta = \cos\!\left(\frac{\pi}{2} - \alpha\right) = \sin\alpha. cos β = cos ( 2 π − α ) = sin α .
Since α \alpha α is acute, both sin α \sin\alpha sin α and cos α \cos\alpha cos α are non-negative, so cos 2 β = sin 2 α \cos^2\beta = \sin^2\alpha cos 2 β = sin 2 α . Therefore
cos 2 α + cos 2 β = cos 2 α + sin 2 α = 1. \cos^2\alpha + \cos^2\beta = \cos^2\alpha + \sin^2\alpha = 1. cos 2 α + cos 2 β = cos 2 α + sin 2 α = 1.
Reverse direction. Suppose cos 2 α + cos 2 β = 1 \cos^2\alpha + \cos^2\beta = 1 cos 2 α + cos 2 β = 1 . Using cos 2 α = 1 − sin 2 α \cos^2\alpha = 1 - \sin^2\alpha cos 2 α = 1 − sin 2 α , we get sin 2 α + cos 2 β = 1 \sin^2\alpha + \cos^2\beta = 1 sin 2 α + cos 2 β = 1 , so cos 2 β = sin 2 α \cos^2\beta = \sin^2\alpha cos 2 β = sin 2 α .
Since α \alpha α and β \beta β are acute, cos β > 0 \cos\beta > 0 cos β > 0 and sin α > 0 \sin\alpha > 0 sin α > 0 , so cos β = sin α = cos ( π / 2 − α ) \cos\beta = \sin\alpha = \cos(\pi/2 - \alpha) cos β = sin α = cos ( π /2 − α ) . Since cos \cos cos is strictly decreasing on [ 0 , π ] [0, \pi] [ 0 , π ] and both β \beta β and π / 2 − α \pi/2 - \alpha π /2 − α lie in ( 0 , π / 2 ) (0, \pi/2) ( 0 , π /2 ) , we conclude β = π / 2 − α \beta = \pi/2 - \alpha β = π /2 − α , i.e. α + β = π / 2 \alpha + \beta = \pi/2 α + β = π /2 . ■ \qquad \blacksquare ■
Part (ii): The first identity
Let B = ( x , y ) B = (x, y) B = ( x , y ) with x > 0 , y > 0 x > 0, y > 0 x > 0 , y > 0 . Let θ = ∠ B O x \theta = \angle BOx θ = ∠ B O x , so x = b cos θ x = b\cos\theta x = b cos θ and y = b sin θ y = b\sin\theta y = b sin θ .
Using A = ( 0 , s ) A = (0, s) A = ( 0 , s ) , C = ( s , 0 ) C = (s, 0) C = ( s , 0 ) , O = ( 0 , 0 ) O = (0, 0) O = ( 0 , 0 ) :
a 2 = ∣ A B ∣ 2 = x 2 + ( y − s ) 2 = x 2 + y 2 − 2 s y + s 2 = b 2 + s 2 − 2 s b sin θ a^2 = |AB|^2 = x^2 + (y - s)^2 = x^2 + y^2 - 2sy + s^2 = b^2 + s^2 - 2sb\sin\theta a 2 = ∣ A B ∣ 2 = x 2 + ( y − s ) 2 = x 2 + y 2 − 2 sy + s 2 = b 2 + s 2 − 2 s b sin θ
c 2 = ∣ C B ∣ 2 = ( x − s ) 2 + y 2 = x 2 − 2 s x + s 2 + y 2 = b 2 + s 2 − 2 s b cos θ c^2 = |CB|^2 = (x - s)^2 + y^2 = x^2 - 2sx + s^2 + y^2 = b^2 + s^2 - 2sb\cos\theta c 2 = ∣ C B ∣ 2 = ( x − s ) 2 + y 2 = x 2 − 2 s x + s 2 + y 2 = b 2 + s 2 − 2 s b cos θ
Therefore
s 2 + b 2 − a 2 = 2 s b sin θ , s 2 + b 2 − c 2 = 2 s b cos θ . s^2 + b^2 - a^2 = 2sb\sin\theta, \qquad s^2 + b^2 - c^2 = 2sb\cos\theta. s 2 + b 2 − a 2 = 2 s b sin θ , s 2 + b 2 − c 2 = 2 s b cos θ .
Squaring and adding:
( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2 sin 2 θ + 4 s 2 b 2 cos 2 θ = 4 s 2 b 2 . ■ (s^2 + b^2 - a^2)^2 + (s^2 + b^2 - c^2)^2 = 4s^2b^2\sin^2\theta + 4s^2b^2\cos^2\theta = 4s^2b^2. \qquad \blacksquare ( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2 sin 2 θ + 4 s 2 b 2 cos 2 θ = 4 s 2 b 2 . ■
Part (iii): The second identity
From Part (ii), a 2 = s 2 + b 2 − 2 s b sin θ a^2 = s^2 + b^2 - 2sb\sin\theta a 2 = s 2 + b 2 − 2 s b sin θ and c 2 = s 2 + b 2 − 2 s b cos θ c^2 = s^2 + b^2 - 2sb\cos\theta c 2 = s 2 + b 2 − 2 s b cos θ , so
a 2 + c 2 = 2 ( s 2 + b 2 ) − 2 s b ( sin θ + cos θ ) . a^2 + c^2 = 2(s^2 + b^2) - 2sb(\sin\theta + \cos\theta). a 2 + c 2 = 2 ( s 2 + b 2 ) − 2 s b ( sin θ + cos θ ) .
Hence
2 s 2 − a 2 − c 2 = 2 s 2 − 2 ( s 2 + b 2 ) + 2 s b ( sin θ + cos θ ) = 2 s b ( sin θ + cos θ ) − 2 b 2 2s^2 - a^2 - c^2 = 2s^2 - 2(s^2 + b^2) + 2sb(\sin\theta + \cos\theta) = 2sb(\sin\theta + \cos\theta) - 2b^2 2 s 2 − a 2 − c 2 = 2 s 2 − 2 ( s 2 + b 2 ) + 2 s b ( sin θ + cos θ ) = 2 s b ( sin θ + cos θ ) − 2 b 2
2 b 2 − a 2 − c 2 = 2 b 2 − 2 ( s 2 + b 2 ) + 2 s b ( sin θ + cos θ ) = 2 s b ( sin θ + cos θ ) − 2 s 2 . 2b^2 - a^2 - c^2 = 2b^2 - 2(s^2 + b^2) + 2sb(\sin\theta + \cos\theta) = 2sb(\sin\theta + \cos\theta) - 2s^2. 2 b 2 − a 2 − c 2 = 2 b 2 − 2 ( s 2 + b 2 ) + 2 s b ( sin θ + cos θ ) = 2 s b ( sin θ + cos θ ) − 2 s 2 .
Wait — let me redo this more cleanly. Define u = a 2 + c 2 u = a^2 + c^2 u = a 2 + c 2 and v = a 2 − c 2 v = a^2 - c^2 v = a 2 − c 2 . Then
u = 2 ( s 2 + b 2 ) − 2 s b ( sin θ + cos θ ) , v = 2 s b ( cos θ − sin θ ) . u = 2(s^2 + b^2) - 2sb(\sin\theta + \cos\theta), \qquad v = 2sb(\cos\theta - \sin\theta). u = 2 ( s 2 + b 2 ) − 2 s b ( sin θ + cos θ ) , v = 2 s b ( cos θ − sin θ ) .
So
2 s 2 − u = 2 s b ( sin θ + cos θ ) − 2 b 2 , 2 b 2 − u = 2 s b ( sin θ + cos θ ) − 2 s 2 . 2s^2 - u = 2sb(\sin\theta + \cos\theta) - 2b^2, \qquad 2b^2 - u = 2sb(\sin\theta + \cos\theta) - 2s^2. 2 s 2 − u = 2 s b ( sin θ + cos θ ) − 2 b 2 , 2 b 2 − u = 2 s b ( sin θ + cos θ ) − 2 s 2 .
Let w = sin θ + cos θ w = \sin\theta + \cos\theta w = sin θ + cos θ . Then 2 s 2 − u = 2 s b w − 2 b 2 = 2 b ( s w − b ) 2s^2 - u = 2sbw - 2b^2 = 2b(sw - b) 2 s 2 − u = 2 s b w − 2 b 2 = 2 b ( s w − b ) and 2 b 2 − u = 2 s b w − 2 s 2 = 2 s ( b w − s ) 2b^2 - u = 2sbw - 2s^2 = 2s(bw - s) 2 b 2 − u = 2 s b w − 2 s 2 = 2 s ( b w − s ) .
Computing the left side:
( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = 4 b 2 ( s w − b ) 2 + 4 s 2 ( b w − s ) 2 . (2s^2 - u)^2 + (2b^2 - u)^2 = 4b^2(sw - b)^2 + 4s^2(bw - s)^2. ( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = 4 b 2 ( s w − b ) 2 + 4 s 2 ( b w − s ) 2 .
Expanding:
= 4 b 2 ( s 2 w 2 − 2 s b w + b 2 ) + 4 s 2 ( b 2 w 2 − 2 s b w + s 2 ) = 4b^2(s^2w^2 - 2sbw + b^2) + 4s^2(b^2w^2 - 2sbw + s^2) = 4 b 2 ( s 2 w 2 − 2 s b w + b 2 ) + 4 s 2 ( b 2 w 2 − 2 s b w + s 2 )
= 4 s 2 b 2 w 2 − 8 s 2 b 2 w + 4 b 4 + 4 s 2 b 2 w 2 − 8 s 2 b 2 w + 4 s 4 = 4s^2b^2w^2 - 8s^2b^2w + 4b^4 + 4s^2b^2w^2 - 8s^2b^2w + 4s^4 = 4 s 2 b 2 w 2 − 8 s 2 b 2 w + 4 b 4 + 4 s 2 b 2 w 2 − 8 s 2 b 2 w + 4 s 4
Wait, that has w 2 w^2 w 2 and w w w terms that don’t simplify neatly. Let me try a direct computation instead.
( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = 4 s 4 − 4 s 2 u + u 2 + 4 b 4 − 4 b 2 u + u 2 (2s^2 - u)^2 + (2b^2 - u)^2 = 4s^4 - 4s^2u + u^2 + 4b^4 - 4b^2u + u^2 ( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = 4 s 4 − 4 s 2 u + u 2 + 4 b 4 − 4 b 2 u + u 2
= 2 u 2 − 4 u ( s 2 + b 2 ) + 4 ( s 4 + b 4 ) = 2u^2 - 4u(s^2 + b^2) + 4(s^4 + b^4) = 2 u 2 − 4 u ( s 2 + b 2 ) + 4 ( s 4 + b 4 )
= 2 [ u 2 − 2 u ( s 2 + b 2 ) + 2 ( s 4 + b 4 ) ] = 2[u^2 - 2u(s^2 + b^2) + 2(s^4 + b^4)] = 2 [ u 2 − 2 u ( s 2 + b 2 ) + 2 ( s 4 + b 4 )]
= 2 [ ( s 2 + b 2 − u ) 2 + ( s 4 + b 4 ) − ( s 2 + b 2 ) 2 + 2 ( s 4 + b 4 ) − 2 ( s 4 + b 4 ) ] = 2[(s^2 + b^2 - u)^2 + (s^4 + b^4) - (s^2 + b^2)^2 + 2(s^4 + b^4) - 2(s^4 + b^4)] = 2 [( s 2 + b 2 − u ) 2 + ( s 4 + b 4 ) − ( s 2 + b 2 ) 2 + 2 ( s 4 + b 4 ) − 2 ( s 4 + b 4 )]
This is getting circular. Let me use the identity from Part (ii) directly.
From Part (ii): ( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2 (s^2 + b^2 - a^2)^2 + (s^2 + b^2 - c^2)^2 = 4s^2b^2 ( s 2 + b 2 − a 2 ) 2 + ( s 2 + b 2 − c 2 ) 2 = 4 s 2 b 2 .
Now compute 4 a 2 c 2 4a^2c^2 4 a 2 c 2 . We have a 2 c 2 = ( s 2 + b 2 − 2 s b sin θ ) ( s 2 + b 2 − 2 s b cos θ ) a^2c^2 = (s^2 + b^2 - 2sb\sin\theta)(s^2 + b^2 - 2sb\cos\theta) a 2 c 2 = ( s 2 + b 2 − 2 s b sin θ ) ( s 2 + b 2 − 2 s b cos θ ) .
Let m = s 2 + b 2 m = s^2 + b^2 m = s 2 + b 2 . Then
a 2 c 2 = ( m − 2 s b sin θ ) ( m − 2 s b cos θ ) = m 2 − 2 s b m ( sin θ + cos θ ) + 4 s 2 b 2 sin θ cos θ . a^2c^2 = (m - 2sb\sin\theta)(m - 2sb\cos\theta) = m^2 - 2sbm(\sin\theta + \cos\theta) + 4s^2b^2\sin\theta\cos\theta. a 2 c 2 = ( m − 2 s b sin θ ) ( m − 2 s b cos θ ) = m 2 − 2 s bm ( sin θ + cos θ ) + 4 s 2 b 2 sin θ cos θ .
Also, u = 2 m − 2 s b ( sin θ + cos θ ) u = 2m - 2sb(\sin\theta + \cos\theta) u = 2 m − 2 s b ( sin θ + cos θ ) , so u 2 = 4 m 2 − 8 s b m ( sin θ + cos θ ) + 4 s 2 b 2 ( sin θ + cos θ ) 2 u^2 = 4m^2 - 8sbm(\sin\theta + \cos\theta) + 4s^2b^2(\sin\theta + \cos\theta)^2 u 2 = 4 m 2 − 8 s bm ( sin θ + cos θ ) + 4 s 2 b 2 ( sin θ + cos θ ) 2 .
And v 2 = 4 s 2 b 2 ( cos θ − sin θ ) 2 v^2 = 4s^2b^2(\cos\theta - \sin\theta)^2 v 2 = 4 s 2 b 2 ( cos θ − sin θ ) 2 .
Therefore
u 2 − v 2 = 4 m 2 − 8 s b m ( sin θ + cos θ ) + 4 s 2 b 2 [ ( sin θ + cos θ ) 2 − ( cos θ − sin θ ) 2 ] . u^2 - v^2 = 4m^2 - 8sbm(\sin\theta + \cos\theta) + 4s^2b^2[(\sin\theta + \cos\theta)^2 - (\cos\theta - \sin\theta)^2]. u 2 − v 2 = 4 m 2 − 8 s bm ( sin θ + cos θ ) + 4 s 2 b 2 [( sin θ + cos θ ) 2 − ( cos θ − sin θ ) 2 ] .
Since ( sin θ + cos θ ) 2 − ( cos θ − sin θ ) 2 = 4 sin θ cos θ (\sin\theta + \cos\theta)^2 - (\cos\theta - \sin\theta)^2 = 4\sin\theta\cos\theta ( sin θ + cos θ ) 2 − ( cos θ − sin θ ) 2 = 4 sin θ cos θ :
u 2 − v 2 = 4 [ m 2 − 2 s b m ( sin θ + cos θ ) + 4 s 2 b 2 sin θ cos θ ] = 4 a 2 c 2 . u^2 - v^2 = 4[m^2 - 2sbm(\sin\theta + \cos\theta) + 4s^2b^2\sin\theta\cos\theta] = 4a^2c^2. u 2 − v 2 = 4 [ m 2 − 2 s bm ( sin θ + cos θ ) + 4 s 2 b 2 sin θ cos θ ] = 4 a 2 c 2 .
Since u 2 − v 2 = ( a 2 + c 2 ) 2 − ( a 2 − c 2 ) 2 = 4 a 2 c 2 u^2 - v^2 = (a^2 + c^2)^2 - (a^2 - c^2)^2 = 4a^2c^2 u 2 − v 2 = ( a 2 + c 2 ) 2 − ( a 2 − c 2 ) 2 = 4 a 2 c 2 , this is just the identity ( u + v ) ( u − v ) = 4 a 2 c 2 (u+v)(u-v) = 4a^2c^2 ( u + v ) ( u − v ) = 4 a 2 c 2 , which is always true. So I need a different approach to connect to the left side.
Let me instead directly compute ( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 (2s^2 - u)^2 + (2b^2 - u)^2 ( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 and compare with 4 a 2 c 2 4a^2c^2 4 a 2 c 2 .
( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = ( 2 s 2 − a 2 − c 2 ) 2 + ( 2 b 2 − a 2 − c 2 ) 2 (2s^2 - u)^2 + (2b^2 - u)^2 = (2s^2 - a^2 - c^2)^2 + (2b^2 - a^2 - c^2)^2 ( 2 s 2 − u ) 2 + ( 2 b 2 − u ) 2 = ( 2 s 2 − a 2 − c 2 ) 2 + ( 2 b 2 − a 2 − c 2 ) 2
= [ 2 s 2 − 2 m + 2 s b w ] 2 + [ 2 b 2 − 2 m + 2 s b w ] 2 = [2s^2 - 2m + 2sbw]^2 + [2b^2 - 2m + 2sbw]^2 = [ 2 s 2 − 2 m + 2 s b w ] 2 + [ 2 b 2 − 2 m + 2 s b w ] 2 where w = sin θ + cos θ w = \sin\theta + \cos\theta w = sin θ + cos θ
= [ − 2 b 2 + 2 s b w ] 2 + [ − 2 s 2 + 2 s b w ] 2 = [-2b^2 + 2sbw]^2 + [-2s^2 + 2sbw]^2 = [ − 2 b 2 + 2 s b w ] 2 + [ − 2 s 2 + 2 s b w ] 2
= 4 b 2 ( s w − b ) 2 + 4 s 2 ( b w − s ) 2 = 4b^2(sw - b)^2 + 4s^2(bw - s)^2 = 4 b 2 ( s w − b ) 2 + 4 s 2 ( b w − s ) 2
= 4 [ b 2 ( s 2 w 2 − 2 b s w + b 2 ) + s 2 ( b 2 w 2 − 2 b s w + s 2 ) ] = 4[b^2(s^2w^2 - 2bsw + b^2) + s^2(b^2w^2 - 2bsw + s^2)] = 4 [ b 2 ( s 2 w 2 − 2 b s w + b 2 ) + s 2 ( b 2 w 2 − 2 b s w + s 2 )]
= 4 [ s 2 b 2 w 2 − 2 b 3 s w + b 4 + s 2 b 2 w 2 − 2 s 3 b w + s 4 ] = 4[s^2b^2w^2 - 2b^3sw + b^4 + s^2b^2w^2 - 2s^3bw + s^4] = 4 [ s 2 b 2 w 2 − 2 b 3 s w + b 4 + s 2 b 2 w 2 − 2 s 3 b w + s 4 ]
= 4 [ 2 s 2 b 2 w 2 − 2 s b w ( b 2 + s 2 ) + s 4 + b 4 ] = 4[2s^2b^2w^2 - 2sbw(b^2 + s^2) + s^4 + b^4] = 4 [ 2 s 2 b 2 w 2 − 2 s b w ( b 2 + s 2 ) + s 4 + b 4 ]
= 4 [ 2 s 2 b 2 w 2 − 2 s b w m + m 2 − 2 s 2 b 2 ] = 4[2s^2b^2w^2 - 2sbwm + m^2 - 2s^2b^2] = 4 [ 2 s 2 b 2 w 2 − 2 s b w m + m 2 − 2 s 2 b 2 ]
Now 4 a 2 c 2 = 4 [ m 2 − 2 s b m w + 4 s 2 b 2 sin θ cos θ ] 4a^2c^2 = 4[m^2 - 2sbmw + 4s^2b^2\sin\theta\cos\theta] 4 a 2 c 2 = 4 [ m 2 − 2 s bm w + 4 s 2 b 2 sin θ cos θ ] .
So we need: 2 s 2 b 2 w 2 − 2 s b w m + m 2 − 2 s 2 b 2 = m 2 − 2 s b m w + 4 s 2 b 2 sin θ cos θ 2s^2b^2w^2 - 2sbwm + m^2 - 2s^2b^2 = m^2 - 2sbmw + 4s^2b^2\sin\theta\cos\theta 2 s 2 b 2 w 2 − 2 s b w m + m 2 − 2 s 2 b 2 = m 2 − 2 s bm w + 4 s 2 b 2 sin θ cos θ .
Simplifying: 2 s 2 b 2 w 2 − 2 s 2 b 2 = 4 s 2 b 2 sin θ cos θ 2s^2b^2w^2 - 2s^2b^2 = 4s^2b^2\sin\theta\cos\theta 2 s 2 b 2 w 2 − 2 s 2 b 2 = 4 s 2 b 2 sin θ cos θ .
w 2 − 1 = ( sin θ + cos θ ) 2 − 1 = sin 2 θ + 2 sin θ cos θ + cos 2 θ − 1 = 2 sin θ cos θ w^2 - 1 = (\sin\theta + \cos\theta)^2 - 1 = \sin^2\theta + 2\sin\theta\cos\theta + \cos^2\theta - 1 = 2\sin\theta\cos\theta w 2 − 1 = ( sin θ + cos θ ) 2 − 1 = sin 2 θ + 2 sin θ cos θ + cos 2 θ − 1 = 2 sin θ cos θ .
So 2 s 2 b 2 ( w 2 − 1 ) = 4 s 2 b 2 sin θ cos θ 2s^2b^2(w^2 - 1) = 4s^2b^2\sin\theta\cos\theta 2 s 2 b 2 ( w 2 − 1 ) = 4 s 2 b 2 sin θ cos θ . This is true! ■ \qquad \blacksquare ■
OK so the approach works but the write-up is messy. Let me restructure it cleanly.
Part (iv): The deduction
From Part (ii), rearranging: ( 2 b 2 − a 2 − c 2 ) 2 = 4 a 2 c 2 − ( 2 s 2 − a 2 − c 2 ) 2 (2b^2 - a^2 - c^2)^2 = 4a^2c^2 - (2s^2 - a^2 - c^2)^2 ( 2 b 2 − a 2 − c 2 ) 2 = 4 a 2 c 2 − ( 2 s 2 − a 2 − c 2 ) 2 .
Since ( 2 s 2 − a 2 − c 2 ) 2 ⩾ 0 (2s^2 - a^2 - c^2)^2 \geqslant 0 ( 2 s 2 − a 2 − c 2 ) 2 ⩾ 0 , we have
( 2 b 2 − a 2 − c 2 ) 2 ⩽ 4 a 2 c 2 , (2b^2 - a^2 - c^2)^2 \leqslant 4a^2c^2, ( 2 b 2 − a 2 − c 2 ) 2 ⩽ 4 a 2 c 2 ,
so ∣ 2 b 2 − a 2 − c 2 ∣ ⩽ 2 a c |2b^2 - a^2 - c^2| \leqslant 2ac ∣2 b 2 − a 2 − c 2 ∣ ⩽ 2 a c . This gives
− 2 a c ⩽ 2 b 2 − a 2 − c 2 ⩽ 2 a c . -2ac \leqslant 2b^2 - a^2 - c^2 \leqslant 2ac. − 2 a c ⩽ 2 b 2 − a 2 − c 2 ⩽ 2 a c .
Adding a 2 + c 2 a^2 + c^2 a 2 + c 2 throughout: a 2 + c 2 − 2 a c ⩽ 2 b 2 ⩽ a 2 + c 2 + 2 a c a^2 + c^2 - 2ac \leqslant 2b^2 \leqslant a^2 + c^2 + 2ac a 2 + c 2 − 2 a c ⩽ 2 b 2 ⩽ a 2 + c 2 + 2 a c , i.e.
( a − c ) 2 ⩽ 2 b 2 ⩽ ( a + c ) 2 . ■ (a - c)^2 \leqslant 2b^2 \leqslant (a + c)^2. \qquad \blacksquare ( a − c ) 2 ⩽ 2 b 2 ⩽ ( a + c ) 2 . ■
Topic : 复数 Complex Numbers | Difficulty : Hard | Marks : 20
8 Four complex numbers u 1 , u 2 , u 3 u_1, u_2, u_3 u 1 , u 2 , u 3 and u 4 u_4 u 4 have unit modulus, and arguments θ 1 , θ 2 , θ 3 \theta_1, \theta_2, \theta_3 θ 1 , θ 2 , θ 3 and θ 4 \theta_4 θ 4 , respectively, with − π < θ 1 < θ 2 < θ 3 < θ 4 < π -\pi < \theta_1 < \theta_2 < \theta_3 < \theta_4 < \pi − π < θ 1 < θ 2 < θ 3 < θ 4 < π .
Show that
arg ( u 1 − u 2 ) = 1 2 ( θ 1 + θ 2 − π ) + 2 n π \arg (u_1 - u_2) = \frac{1}{2} (\theta_1 + \theta_2 - \pi) + 2n\pi arg ( u 1 − u 2 ) = 2 1 ( θ 1 + θ 2 − π ) + 2 nπ
where n = 0 n = 0 n = 0 or 1 1 1 . Deduce that
arg ( ( u 1 − u 2 ) ( u 4 − u 3 ) ) = arg ( ( u 1 − u 4 ) ( u 3 − u 2 ) ) + 2 n π \arg ((u_1 - u_2) (u_4 - u_3)) = \arg ((u_1 - u_4) (u_3 - u_2)) + 2n\pi arg (( u 1 − u 2 ) ( u 4 − u 3 )) = arg (( u 1 − u 4 ) ( u 3 − u 2 )) + 2 nπ
for some integer n n n .
Prove that
∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ + ∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = ∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣ . | (u_1 - u_2) (u_4 - u_3) | + | (u_1 - u_4) (u_3 - u_2) | = | (u_1 - u_3) (u_4 - u_2) | . ∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ + ∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = ∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣.
Model Solution
Part (i): Argument of u 1 − u 2 u_1 - u_2 u 1 − u 2
Write u k = e i θ k u_k = e^{i\theta_k} u k = e i θ k . Then
u 1 − u 2 = e i θ 1 − e i θ 2 = e i ( θ 1 + θ 2 ) / 2 ( e i ( θ 1 − θ 2 ) / 2 − e − i ( θ 1 − θ 2 ) / 2 ) = 2 i sin ( θ 1 − θ 2 2 ) e i ( θ 1 + θ 2 ) / 2 . u_1 - u_2 = e^{i\theta_1} - e^{i\theta_2} = e^{i(\theta_1+\theta_2)/2}\left(e^{i(\theta_1-\theta_2)/2} - e^{-i(\theta_1-\theta_2)/2}\right) = 2i\sin\!\left(\frac{\theta_1-\theta_2}{2}\right)e^{i(\theta_1+\theta_2)/2}. u 1 − u 2 = e i θ 1 − e i θ 2 = e i ( θ 1 + θ 2 ) /2 ( e i ( θ 1 − θ 2 ) /2 − e − i ( θ 1 − θ 2 ) /2 ) = 2 i sin ( 2 θ 1 − θ 2 ) e i ( θ 1 + θ 2 ) /2 .
Since θ 1 < θ 2 \theta_1 < \theta_2 θ 1 < θ 2 , we have θ 1 − θ 2 2 < 0 \frac{\theta_1-\theta_2}{2} < 0 2 θ 1 − θ 2 < 0 , so sin ( θ 1 − θ 2 2 ) < 0 \sin\!\left(\frac{\theta_1-\theta_2}{2}\right) < 0 sin ( 2 θ 1 − θ 2 ) < 0 . Thus
u 1 − u 2 = 2 ∣ sin ( θ 1 − θ 2 2 ) ∣ ⋅ i ⋅ ( − 1 ) ⋅ e i ( θ 1 + θ 2 ) / 2 = 2 ∣ sin ( θ 1 − θ 2 2 ) ∣ e i ( θ 1 + θ 2 ) / 2 ⋅ e − i π / 2 ⋅ e i π . u_1 - u_2 = 2\left|\sin\!\left(\frac{\theta_1-\theta_2}{2}\right)\right| \cdot i \cdot (-1) \cdot e^{i(\theta_1+\theta_2)/2} = 2\left|\sin\!\left(\frac{\theta_1-\theta_2}{2}\right)\right| e^{i(\theta_1+\theta_2)/2} \cdot e^{-i\pi/2} \cdot e^{i\pi}. u 1 − u 2 = 2 sin ( 2 θ 1 − θ 2 ) ⋅ i ⋅ ( − 1 ) ⋅ e i ( θ 1 + θ 2 ) /2 = 2 sin ( 2 θ 1 − θ 2 ) e i ( θ 1 + θ 2 ) /2 ⋅ e − iπ /2 ⋅ e iπ .
Therefore
arg ( u 1 − u 2 ) = θ 1 + θ 2 2 + π 2 + π ( m o d 2 π ) = θ 1 + θ 2 2 + 3 π 2 ( m o d 2 π ) . \arg(u_1 - u_2) = \frac{\theta_1+\theta_2}{2} + \frac{\pi}{2} + \pi \pmod{2\pi} = \frac{\theta_1+\theta_2}{2} + \frac{3\pi}{2} \pmod{2\pi}. arg ( u 1 − u 2 ) = 2 θ 1 + θ 2 + 2 π + π ( mod 2 π ) = 2 θ 1 + θ 2 + 2 3 π ( mod 2 π ) .
Wait — let me redo this more carefully. We have i ⋅ sin α i \cdot \sin\alpha i ⋅ sin α where α < 0 \alpha < 0 α < 0 and sin α < 0 \sin\alpha < 0 sin α < 0 . So i sin α = ∣ sin α ∣ ⋅ i ⋅ ( − 1 ) = ∣ sin α ∣ ⋅ e i π ⋅ e i π / 2 = ∣ sin α ∣ ⋅ e i 3 π / 2 i\sin\alpha = |\sin\alpha| \cdot i \cdot (-1) = |\sin\alpha| \cdot e^{i\pi} \cdot e^{i\pi/2} = |\sin\alpha| \cdot e^{i3\pi/2} i sin α = ∣ sin α ∣ ⋅ i ⋅ ( − 1 ) = ∣ sin α ∣ ⋅ e iπ ⋅ e iπ /2 = ∣ sin α ∣ ⋅ e i 3 π /2 .
Thus u 1 − u 2 = 2 ∣ sin α ∣ ⋅ e i ( θ 1 + θ 2 ) / 2 ⋅ e i 3 π / 2 u_1 - u_2 = 2|\sin\alpha| \cdot e^{i(\theta_1+\theta_2)/2} \cdot e^{i3\pi/2} u 1 − u 2 = 2∣ sin α ∣ ⋅ e i ( θ 1 + θ 2 ) /2 ⋅ e i 3 π /2 , giving
arg ( u 1 − u 2 ) = θ 1 + θ 2 2 + 3 π 2 = θ 1 + θ 2 2 − π 2 ( m o d 2 π ) . \arg(u_1 - u_2) = \frac{\theta_1+\theta_2}{2} + \frac{3\pi}{2} = \frac{\theta_1+\theta_2}{2} - \frac{\pi}{2} \pmod{2\pi}. arg ( u 1 − u 2 ) = 2 θ 1 + θ 2 + 2 3 π = 2 θ 1 + θ 2 − 2 π ( mod 2 π ) .
Since θ 1 + θ 2 − π 2 \frac{\theta_1+\theta_2-\pi}{2} 2 θ 1 + θ 2 − π is equivalent to θ 1 + θ 2 2 − π 2 \frac{\theta_1+\theta_2}{2} - \frac{\pi}{2} 2 θ 1 + θ 2 − 2 π , we have
arg ( u 1 − u 2 ) = 1 2 ( θ 1 + θ 2 − π ) + 2 n π , n = 0 or 1. ■ \arg(u_1 - u_2) = \frac{1}{2}(\theta_1 + \theta_2 - \pi) + 2n\pi, \qquad n = 0 \text{ or } 1. \qquad \blacksquare arg ( u 1 − u 2 ) = 2 1 ( θ 1 + θ 2 − π ) + 2 nπ , n = 0 or 1. ■
Part (ii): Argument of products
Using the result from Part (i):
arg ( u 1 − u 2 ) = θ 1 + θ 2 − π 2 , arg ( u 4 − u 3 ) = θ 3 + θ 4 − π 2 , \arg(u_1 - u_2) = \frac{\theta_1+\theta_2-\pi}{2}, \qquad \arg(u_4 - u_3) = \frac{\theta_3+\theta_4-\pi}{2}, arg ( u 1 − u 2 ) = 2 θ 1 + θ 2 − π , arg ( u 4 − u 3 ) = 2 θ 3 + θ 4 − π ,
arg ( u 1 − u 4 ) = θ 1 + θ 4 − π 2 , arg ( u 3 − u 2 ) = θ 2 + θ 3 − π 2 . \arg(u_1 - u_4) = \frac{\theta_1+\theta_4-\pi}{2}, \qquad \arg(u_3 - u_2) = \frac{\theta_2+\theta_3-\pi}{2}. arg ( u 1 − u 4 ) = 2 θ 1 + θ 4 − π , arg ( u 3 − u 2 ) = 2 θ 2 + θ 3 − π .
Therefore
arg ( ( u 1 − u 2 ) ( u 4 − u 3 ) ) = θ 1 + θ 2 + θ 3 + θ 4 − 2 π 2 ( m o d 2 π ) , \arg((u_1-u_2)(u_4-u_3)) = \frac{\theta_1+\theta_2+\theta_3+\theta_4 - 2\pi}{2} \pmod{2\pi}, arg (( u 1 − u 2 ) ( u 4 − u 3 )) = 2 θ 1 + θ 2 + θ 3 + θ 4 − 2 π ( mod 2 π ) ,
arg ( ( u 1 − u 4 ) ( u 3 − u 2 ) ) = θ 1 + θ 2 + θ 3 + θ 4 − 2 π 2 ( m o d 2 π ) . \arg((u_1-u_4)(u_3-u_2)) = \frac{\theta_1+\theta_2+\theta_3+\theta_4 - 2\pi}{2} \pmod{2\pi}. arg (( u 1 − u 4 ) ( u 3 − u 2 )) = 2 θ 1 + θ 2 + θ 3 + θ 4 − 2 π ( mod 2 π ) .
These are equal modulo 2 π 2\pi 2 π , so
arg ( ( u 1 − u 2 ) ( u 4 − u 3 ) ) = arg ( ( u 1 − u 4 ) ( u 3 − u 2 ) ) + 2 n π . ■ \arg((u_1-u_2)(u_4-u_3)) = \arg((u_1-u_4)(u_3-u_2)) + 2n\pi. \qquad \blacksquare arg (( u 1 − u 2 ) ( u 4 − u 3 )) = arg (( u 1 − u 4 ) ( u 3 − u 2 )) + 2 nπ . ■
Part (iii): The magnitude identity
Since all u k u_k u k lie on the unit circle, ∣ u i − u j ∣ = 2 ∣ sin θ i − θ j 2 ∣ |u_i - u_j| = 2\left|\sin\frac{\theta_i-\theta_j}{2}\right| ∣ u i − u j ∣ = 2 sin 2 θ i − θ j . With the ordering − π < θ 1 < θ 2 < θ 3 < θ 4 < π -\pi < \theta_1 < \theta_2 < \theta_3 < \theta_4 < \pi − π < θ 1 < θ 2 < θ 3 < θ 4 < π , all differences θ j − θ i \theta_j - \theta_i θ j − θ i for i < j i < j i < j are positive and less than 2 π 2\pi 2 π , so ∣ u i − u j ∣ = 2 sin θ j − θ i 2 |u_i - u_j| = 2\sin\frac{\theta_j-\theta_i}{2} ∣ u i − u j ∣ = 2 sin 2 θ j − θ i .
Let α = θ 2 − θ 1 > 0 \alpha = \theta_2 - \theta_1 > 0 α = θ 2 − θ 1 > 0 , β = θ 3 − θ 2 > 0 \beta = \theta_3 - \theta_2 > 0 β = θ 3 − θ 2 > 0 , γ = θ 4 − θ 3 > 0 \gamma = \theta_4 - \theta_3 > 0 γ = θ 4 − θ 3 > 0 . Then
∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ = 4 sin α 2 sin γ 2 , |(u_1-u_2)(u_4-u_3)| = 4\sin\frac{\alpha}{2}\sin\frac{\gamma}{2}, ∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ = 4 sin 2 α sin 2 γ ,
∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = 4 sin α + β + γ 2 sin β 2 , |(u_1-u_4)(u_3-u_2)| = 4\sin\frac{\alpha+\beta+\gamma}{2}\sin\frac{\beta}{2}, ∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = 4 sin 2 α + β + γ sin 2 β ,
∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣ = 4 sin α + β 2 sin β + γ 2 . |(u_1-u_3)(u_4-u_2)| = 4\sin\frac{\alpha+\beta}{2}\sin\frac{\beta+\gamma}{2}. ∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣ = 4 sin 2 α + β sin 2 β + γ .
We need to show:
sin α 2 sin γ 2 + sin α + β + γ 2 sin β 2 = sin α + β 2 sin β + γ 2 . ( † ) \sin\frac{\alpha}{2}\sin\frac{\gamma}{2} + \sin\frac{\alpha+\beta+\gamma}{2}\sin\frac{\beta}{2} = \sin\frac{\alpha+\beta}{2}\sin\frac{\beta+\gamma}{2}. \qquad (\dagger) sin 2 α sin 2 γ + sin 2 α + β + γ sin 2 β = sin 2 α + β sin 2 β + γ . ( † )
Let A = α / 2 A = \alpha/2 A = α /2 , B = β / 2 B = \beta/2 B = β /2 , C = γ / 2 C = \gamma/2 C = γ /2 . Then ( † ) (\dagger) ( † ) becomes
sin A sin C + sin ( A + B + C ) sin B = sin ( A + B ) sin ( B + C ) . \sin A\sin C + \sin(A+B+C)\sin B = \sin(A+B)\sin(B+C). sin A sin C + sin ( A + B + C ) sin B = sin ( A + B ) sin ( B + C ) .
Using the product-to-sum formula sin X sin Y = 1 2 [ cos ( X − Y ) − cos ( X + Y ) ] \sin X \sin Y = \frac{1}{2}[\cos(X-Y) - \cos(X+Y)] sin X sin Y = 2 1 [ cos ( X − Y ) − cos ( X + Y )] :
RHS : sin ( A + B ) sin ( B + C ) = 1 2 [ cos ( A − C ) − cos ( A + 2 B + C ) ] \sin(A+B)\sin(B+C) = \frac{1}{2}[\cos(A-C) - \cos(A+2B+C)] sin ( A + B ) sin ( B + C ) = 2 1 [ cos ( A − C ) − cos ( A + 2 B + C )] .
LHS : sin A sin C = 1 2 [ cos ( A − C ) − cos ( A + C ) ] \sin A\sin C = \frac{1}{2}[\cos(A-C) - \cos(A+C)] sin A sin C = 2 1 [ cos ( A − C ) − cos ( A + C )] and
sin ( A + B + C ) sin B = 1 2 [ cos ( A + C ) − cos ( A + 2 B + C ) ] \sin(A+B+C)\sin B = \frac{1}{2}[\cos(A+C) - \cos(A+2B+C)] sin ( A + B + C ) sin B = 2 1 [ cos ( A + C ) − cos ( A + 2 B + C )] .
Adding: LHS = 1 2 [ cos ( A − C ) − cos ( A + 2 B + C ) ] = RHS \text{LHS} = \frac{1}{2}[\cos(A-C) - \cos(A+2B+C)] = \text{RHS} LHS = 2 1 [ cos ( A − C ) − cos ( A + 2 B + C )] = RHS . ■ \qquad \blacksquare ■
Geometric interpretation : The four points u 1 , u 2 , u 3 , u 4 u_1, u_2, u_3, u_4 u 1 , u 2 , u 3 , u 4 lie in order on the unit circle, forming a cyclic quadrilateral. The identity ∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ + ∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = ∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣ |(u_1-u_2)(u_4-u_3)| + |(u_1-u_4)(u_3-u_2)| = |(u_1-u_3)(u_4-u_2)| ∣ ( u 1 − u 2 ) ( u 4 − u 3 ) ∣ + ∣ ( u 1 − u 4 ) ( u 3 − u 2 ) ∣ = ∣ ( u 1 − u 3 ) ( u 4 − u 2 ) ∣ is precisely Ptolemy’s theorem : for a cyclic quadrilateral, the sum of the products of opposite sides equals the product of the diagonals.