review Algebraic form: z = a + b i ( a , b ∈ R ) , a = ℜ ( z ) , b = ℑ ( z ) z=a+bi(a,b\in R),a=\Re(z),b=\Im(z) z = a + bi ( a , b ∈ R ) , a = ℜ ( z ) , b = ℑ ( z ) Trigonometric form: z = r ( cos θ + i sin θ ) , ( r ≥ 0 ) z=r(\cos\theta+i\sin\theta),(r\ge0) z = r ( cos θ + i sin θ ) , ( r ≥ 0 ) -arg ( z ) ∈ [ 0 , 2 π ) \arg(z)\in[0,2\pi) arg ( z ) ∈ [ 0 , 2 π ) represents the main value of the argument, A r g ( z ) ∈ R Arg(z)\in\R A r g ( z ) ∈ R represents the argumentz 1 z 2 = r 1 r 2 [ cos ( θ 1 + θ 2 ) + i sin ( θ 1 + θ 2 ) z_1z_2=r_1r_2[\cos(\theta_1+\theta_2)+i\sin(\theta_1+\theta_2) z 1 z 2 = r 1 r 2 [ cos ( θ 1 + θ 2 ) + i sin ( θ 1 + θ 2 ) z 1 z 2 = r 1 r 2 [ cos ( θ 1 − θ 2 ) + i sin ( θ 1 − θ 2 ) \frac{z_1}{z_2}=\frac{r_1}{r_2}[\cos(\theta_1-\theta_2)+i\sin(\theta_1-\theta_2) z 2 z 1 = r 2 r 1 [ cos ( θ 1 − θ 2 ) + i sin ( θ 1 − θ 2 ) z n = r n ( cos n θ + i sin n θ ) z^n=r^n(\cos n\theta+i\sin n\theta) z n = r n ( cos n θ + i sin n θ ) z n = r n ( cos θ + 2 k π n + i sin θ + 2 k π n ) , k = 0 , 1 , 2 , . . . , n − 1 \sqrt[n]{z}=\sqrt[n]{r}(\cos\frac{\theta+2k\pi}{n}+i\sin\frac{\theta+2k\pi}{n}),k=0,1,2,...,n-1 n z = n r ( cos n θ + 2 k π + i sin n θ + 2 k π ) , k = 0 , 1 , 2 , ... , n − 1 Exponential form: e i θ = cos θ + i sin θ e^{i\theta}=\cos\theta+i\sin\theta e i θ = cos θ + i sin θ Application of plural numbers S △ = 1 2 ∣ I m ( z 1 ‾ z 2 + z 2 ‾ z 3 + z 3 ‾ z 1 ) ∣ S_\triangle=\frac{1}{2}|Im(\overline{z_1}z_2+\overline{z_2}z_3+\overline{z_3}z_1)| S △ = 2 1 ∣ I m ( z 1 z 2 + z 2 z 3 + z 3 z 1 ) ∣ Necessary and sufficient conditions for four points to be a circle: z 3 − z 1 z 4 − z 1 : z 3 − z 2 z 4 − z 2 ∈ R \frac{z_3-z_1}{z_4-z_1}:\frac{z_3-z_2}{z_4-z_2}\in R z 4 − z 1 z 3 − z 1 : z 4 − z 2 z 3 − z 2 ∈ R △ z 1 z 2 z 3 , △ w 1 w 2 w 3 \triangle z_1z_2z_3,\triangle w_1w_2w_3 △ z 1 z 2 z 3 , △ w 1 w 2 w 3 Similar necessary and sufficient conditions: z 3 − z 2 z 2 − z 1 = w 3 − w 2 w 2 − w 1 \frac{z_3-z_2}{z_2-z_1}=\frac{w_3-w_2}{w_2-w_1} z 2 − z 1 z 3 − z 2 = w 2 − w 1 w 3 − w 2 brush questions Example 1 If z ∈ C , ∣ z − 2 ∣ ≤ 1 z\in C,|z-2|\le1 z ∈ C , ∣ z − 2∣ ≤ 1 , find the maximum and minimum values of ∣ z ∣ |z| ∣ z ∣ , and the range of arg ( z ) \arg(z) arg ( z )
Solution: The point represented by z z z in the complex plane is on a circle with center ( 2 , 0 ) (2,0) ( 2 , 0 ) and radius 1 1 1 .
Since there is ∣ ∣ z ∣ − 2 ∣ ≤ ∣ z − 2 ∣ ≤ ∣ z ∣ + ∣ 2 ∣ ||z|-2|\le|z-2|\le|z|+|2| ∣∣ z ∣ − 2∣ ≤ ∣ z − 2∣ ≤ ∣ z ∣ + ∣2∣ :
So − 1 ≤ ∣ z ∣ − 2 ≤ 1 , 1 ≤ ∣ z ∣ ≤ 3 -1\le|z|-2\le1,1\le|z|\le3 − 1 ≤ ∣ z ∣ − 2 ≤ 1 , 1 ≤ ∣ z ∣ ≤ 3
Combining numbers and shapes, arg ( z ) ∈ [ 0 , π 6 ] ∪ [ 11 6 π , 2 π ) \arg(z)\in[0,\frac{\pi}{6}]\cup[\frac{11}{6}\pi,2\pi) arg ( z ) ∈ [ 0 , 6 π ] ∪ [ 6 11 π , 2 π )
Example 2 The complex number z z z satisfies arg ( z + 3 ) = 6 5 π \arg(z+3)=\frac{6}{5}\pi arg ( z + 3 ) = 5 6 π , find min ∣ z + 6 ∣ + ∣ z − 3 i ∣ \min|z+6|+|z-3i| min ∣ z + 6∣ + ∣ z − 3 i ∣ .
Solution: It is easy to know that the trajectory represented by arg ( z + 3 ) = 6 5 π \arg(z+3)=\frac{6}{5}\pi arg ( z + 3 ) = 5 6 π is y = − 1 2 ( x + 3 ) ( x < − 3 ) y=-\frac{1}{2}(x+3)(x\lt-3) y = − 2 1 ( x + 3 ) ( x < − 3 )
The obtained ∣ z + 6 ∣ + ∣ z − 3 i ∣ |z+6|+|z-3i| ∣ z + 6∣ + ∣ z − 3 i ∣ is equivalent to the sum of the distances from the corresponding points of z z z to ( − 6 , 0 ) , ( 0 , 3 ) (-6,0),(0,3) ( − 6 , 0 ) , ( 0 , 3 ) in the complex plane.
Obviously min ∣ z + 6 ∣ + ∣ z − 3 i ∣ = 6 2 + 3 2 = 3 5 \min |z+6|+|z-3i|=\sqrt{6^2+3^2}=3\sqrt{5} min ∣ z + 6∣ + ∣ z − 3 i ∣ = 6 2 + 3 2 = 3 5 (the shortest line segment between two points).
Example 3 Given ∣ z − 2 i ∣ ≤ 1 |z-2i|\le1 ∣ z − 2 i ∣ ≤ 1 , find max arg ( z − 4 i ) \max\arg(z-4i) max arg ( z − 4 i ) Apparently max arg ( z − 4 i ) = 5 3 π \max\arg(z-4i)=\frac{5}{3}\pi max arg ( z − 4 i ) = 3 5 π
Example 4 A line l l l passes through the origin. The parabola C C C has its vertex at the origin and its focus on the positive x x x -axis. The reflections of A ( − 1 , 0 ) A(-1,0) A ( − 1 , 0 ) and B ( 0 , 8 ) B(0,8) B ( 0 , 8 ) across l l l both lie on C C C . Find the equations of l l l and C C C .
Let parabola C : y 2 = 2 p x ( p > 0 ) C:y^2=2px(p\gt0) C : y 2 = 2 p x ( p > 0 ) and straight line l : y = k x l:y=kx l : y = k x .
If you consider calculating the symmetry point coordinates and then bringing them into the parabola, the calculation will be extremely complicated.
We establish a complex plane and assume that O A ′ ⃗ , O B ′ ⃗ \vec{OA'},\vec{OB'} O A ′ , O B ′ corresponds to the complex number x 1 + y 1 i , x 2 + y 2 i x_1+y_1i,x_2+y_2i x 1 + y 1 i , x 2 + y 2 i .
Apparently O A ′ ⃗ ⊥ O B ′ ⃗ , ∣ O A ′ ∣ = 1 , ∣ O B ′ ∣ = 8 \vec{OA'}\perp\vec{OB'},|OA'|=1,|OB'|=8 O A ′ ⊥ O B ′ , ∣ O A ′ ∣ = 1 , ∣ O B ′ ∣ = 8
Therefore x 2 + y 2 i = 8 i ( x 1 + y 1 ) x_2+y_2i=8i(x_1+y_1) x 2 + y 2 i = 8 i ( x 1 + y 1 ) , then { x 2 = − 8 y 1 , y 2 = 8 x 1 \begin{cases} x_2=-8y_1,\\ y_2=8x_1 \end{cases} { x 2 = − 8 y 1 , y 2 = 8 x 1
Bringing A ′ , B ′ A',B' A ′ , B ′ into the parabola:
y 1 2 = 2 p x 1 ( 1 ) y 2 2 = 2 p x 2 ( 2 ) x 2 = − 8 y 1 ( 3 ) y 2 = 8 x 1 ( 4 ) ( 1 ) ( 2 ) ( 3 ) ( 4 ) : − y 1 y 2 = 4 p 2 ( 1 ) ( 4 ) : y 1 2 = p 4 y 2 y 1 = − p , y 2 = 4 p x 1 = p 2 x 1 2 + y 1 2 = ( p 2 ) 2 + p 2 = 1 , p = 2 5 5 C : y 2 = 4 5 5 x \begin{gathered} y_1^2=2px_1 (1)\\ y_2^2=2px_2 (2)\\ x_2=-8y_1 (3)\\ y_2=8x_1 (4)\\ \frac{(1)(2)}{(3)(4)}:-y_1y_2=4p^2\\ (1)(4):y_1^2=\frac{p}{4}y_2\\ y_1=-p,y_2=4p\\ x_1=\frac{p}{2}\\ x_1^2+y_1^2=(\frac{p}{2})^2+p^2=1,p=\frac{2\sqrt{5}}{5}\\ C:y^2=\frac{4\sqrt{5}}{5}x\\ \end{gathered} y 1 2 = 2 p x 1 ( 1 ) y 2 2 = 2 p x 2 ( 2 ) x 2 = − 8 y 1 ( 3 ) y 2 = 8 x 1 ( 4 ) ( 3 ) ( 4 ) ( 1 ) ( 2 ) : − y 1 y 2 = 4 p 2 ( 1 ) ( 4 ) : y 1 2 = 4 p y 2 y 1 = − p , y 2 = 4 p x 1 = 2 p x 1 2 + y 1 2 = ( 2 p ) 2 + p 2 = 1 , p = 5 2 5 C : y 2 = 5 4 5 x
Find the equation of the straight line below:
x 1 = 5 5 , y 1 = − 2 5 5 − 1 k = y 1 − 0 x 1 − ( − 1 ) k = x 1 + 1 − y 1 = p 2 + 1 p = 1 + 5 2 l : y = 1 + 5 2 x \begin{gathered} x_1=\frac{\sqrt{5}}{5},y_1=-\frac{2\sqrt{5}}{5}\\ -\frac{1}{k}=\frac{y_1-0}{x_1-(-1)}\\ k=\frac{x_1+1}{-y_1}=\frac{\frac{p}{2}+1}{p}=\frac{1+\sqrt{5}}{2}\\ l:y=\frac{1+\sqrt{5}}{2}x \end{gathered} x 1 = 5 5 , y 1 = − 5 2 5 − k 1 = x 1 − ( − 1 ) y 1 − 0 k = − y 1 x 1 + 1 = p 2 p + 1 = 2 1 + 5 l : y = 2 1 + 5 x
Example 5 If point A ( 3 , 0 ) , B A(3,0),B A ( 3 , 0 ) , B is on ellipse x 2 4 + y 2 = 1 \frac{x^2}{4}+y^2=1 4 x 2 + y 2 = 1 , point A , B , C A,B,C A , B , C and three points are arranged in a clockwise direction, and △ A B C \triangle ABC △ A B C is an equilateral triangle, find the trajectory of point C C C .
Assume C ( x , y ) C(x,y) C ( x , y ) , then the geometric relationship [ ( x − 3 ) + y i ] ( cos 60 ∘ + i sin 60 ∘ ) = ( x B − 3 ) + y B i [(x-3)+yi](\cos60\degree+i\sin60\degree)=(x_B-3)+y_Bi [( x − 3 ) + y i ] ( cos 6 0 ∘ + i sin 6 0 ∘ ) = ( x B − 3 ) + y B i
Then { x B = 3 + x − 3 2 − 3 2 y = x − 3 y + 3 2 y B = 3 ( x − 3 ) 2 + y 2 = 3 x + y − 3 3 2 \begin{cases} x_B=3+\frac{x-3}{2}-\frac{\sqrt{3}}{2}y=\frac{x-\sqrt{3}y+3}{2}\\ y_B=\frac{\sqrt{3}(x-3)}{2}+\frac{y}{2}=\frac{\sqrt{3}x+y-3\sqrt{3}}{2} \end{cases} { x B = 3 + 2 x − 3 − 2 3 y = 2 x − 3 y + 3 y B = 2 3 ( x − 3 ) + 2 y = 2 3 x + y − 3 3
Enter the elliptic equation: ( x − 3 y + 3 2 ) 2 + 4 ( 3 x + y − 3 3 2 ) 2 = 4 (\frac{x-\sqrt{3}y+3}{2})^2+4(\frac{\sqrt{3}x+y-3\sqrt{3}}{2})^2=4 ( 2 x − 3 y + 3 ) 2 + 4 ( 2 3 x + y − 3 3 ) 2 = 4
Further simplify the coefficients:
( x − 3 y + 3 ) 2 + 4 ( 3 x + y − 3 3 ) 2 = 16 (x-\sqrt{3}y+3)^2+4(\sqrt{3}x+y-3\sqrt{3})^2=16 ( x − 3 y + 3 ) 2 + 4 ( 3 x + y − 3 3 ) 2 = 16
Example 6 Assume x , y ∈ R x, y \in R x , y ∈ R , z 1 = 2 − 3 x + x i z_1 = 2 - \sqrt{3}x + xi z 1 = 2 − 3 x + x i , z 2 = 3 y − 1 + ( 3 − y ) i z_2 = \sqrt{3}y - 1 + (\sqrt{3} - y)i z 2 = 3 y − 1 + ( 3 − y ) i , known ∣ z 1 ∣ = ∣ z 2 ∣ |z_1| = |z_2| ∣ z 1 ∣ = ∣ z 2 ∣ , arg z 1 z 2 = π 2 \arg \frac{z_1}{z_2} = \frac{\pi}{2} arg z 2 z 1 = 2 π ,
(1) Find ( z 1 + z 2 2 ) 100 \left( \frac{z_1 + z_2}{2} \right)^{100} ( 2 z 1 + z 2 ) 100
(2) Assume z = z 1 + z 2 2 z = \frac{z_1 + z_2}{2} z = 2 z 1 + z 2 , find the number of elements in the set A = { x ∣ x = z 2 k + z − 2 k , k ∈ Z } A = \left\{ x \mid x = z^{2k} + z^{-2k}, k \in \Z \right\} A = { x ∣ x = z 2 k + z − 2 k , k ∈ Z } .
(1)
Because arg ( z 1 z 2 ) = π 2 , ∣ z 1 ∣ = ∣ z 2 ∣ \arg(\frac{z_1}{z_2})=\frac{\pi}{2},|z_1|=|z_2| arg ( z 2 z 1 ) = 2 π , ∣ z 1 ∣ = ∣ z 2 ∣
So z 1 = i z 2 z_1=iz_2 z 1 = i z 2
( 2 − 3 x ) + x i = i [ ( 3 y − 1 ) + ( 3 − y ) i ] (2-\sqrt{3}x)+xi=i[(\sqrt{3}y-1)+(\sqrt{3}-y)i] ( 2 − 3 x ) + x i = i [( 3 y − 1 ) + ( 3 − y ) i ]
This gives: { 2 − 3 x = y − 3 , x = 3 y − 1 \begin{cases} 2-\sqrt{3}x=y-\sqrt{3},\\ x=\sqrt{3}y-1 \end{cases} { 2 − 3 x = y − 3 , x = 3 y − 1
Solving gives: { x = 1 + 3 2 y = 1 + 3 2 \begin{cases} x=\frac{1+\sqrt{3}}{2}\\ y=\frac{1+\sqrt{3}}{2} \end{cases} { x = 2 1 + 3 y = 2 1 + 3
Therefore: { z 1 = 1 − 3 2 + 1 + 3 2 i z 2 = 1 + 3 2 + 3 − 1 2 i \begin{cases} z_1=\frac{1-\sqrt{3}}{2}+\frac{1+\sqrt{3}}{2}i\\ z_2=\frac{1+\sqrt{3}}{2}+\frac{\sqrt{3}-1}{2}i \end{cases} { z 1 = 2 1 − 3 + 2 1 + 3 i z 2 = 2 1 + 3 + 2 3 − 1 i
Hence: ( z 1 + z 2 2 ) 100 = ( 1 2 + 3 2 i ) 100 = ( cos 60 ∘ + i sin 60 ∘ ) 100 = cos 6000 ∘ + i sin 6000 ∘ = cos 240 ∘ + i sin 240 ∘ = − 1 2 − 3 2 i \begin{gathered} \left( \frac{z_1 + z_2}{2} \right)^{100}\\ =(\frac{1}{2}+\frac{\sqrt{3}}{2}i)^{100}\\ =(\cos60\degree+i\sin60\degree)^{100}\\ =\cos6000\degree+i\sin6000\degree\\ =\cos240\degree+i\sin240\degree\\ =-\frac{1}{2}-\frac{\sqrt{3}}{2}i \end{gathered} ( 2 z 1 + z 2 ) 100 = ( 2 1 + 2 3 i ) 100 = ( cos 6 0 ∘ + i sin 6 0 ∘ ) 100 = cos 600 0 ∘ + i sin 600 0 ∘ = cos 24 0 ∘ + i sin 24 0 ∘ = − 2 1 − 2 3 i
Consider ( 1 2 + 3 2 i ) 3 = − 1 (\frac{1}{2}+\frac{\sqrt{3}}{2}i)^{3}=-1 ( 2 1 + 2 3 i ) 3 = − 1 for easier calculation.
(2)
x = z 2 k + z − 2 k = ( cos 60 ∘ + i sin 60 ∘ ) 2 k + ( cos 60 ∘ + i sin 60 ∘ ) − 2 k = 2 cos ( 120 k ) ∘ \begin{gathered} x=z^{2k}+z^{-2k}\\ =(\cos60\degree+i\sin60\degree)^{2k}+(\cos60\degree+i\sin60\degree)^{-2k}\\ =2\cos(120k)\degree \end{gathered} x = z 2 k + z − 2 k = ( cos 6 0 ∘ + i sin 6 0 ∘ ) 2 k + ( cos 6 0 ∘ + i sin 6 0 ∘ ) − 2 k = 2 cos ( 120 k ) ∘ Considering k ∈ Z k\in\Z k ∈ Z , there are 2 possible x = 2 cos ( 120 k ) x=2\cos(120k) x = 2 cos ( 120 k ) . ∣ A ∣ = 2 |A|=2 ∣ A ∣ = 2
Let ω = − 1 2 + 3 2 i \omega=-\frac{1}{2}+\frac{\sqrt{3}}{2}i ω = − 2 1 + 2 3 i
There is z = − w ‾ z=-\overline{w} z = − w
x = z 2 k + z − 2 k = ( − ω ‾ ) 2 k + ( − ω ‾ ) − 2 k = ( ω ‾ ) 2 k + ( ω ‾ ) − 2 k = ω k + ω − k \begin{gathered} x=z^{2k}+z^{-2k}\\ =(-\overline{\omega})^{2k}+(-\overline{\omega})^{-2k}\\ =(\overline{\omega})^{2k}+(\overline{\omega})^{-2k}\\ =\omega^k+\omega^{-k} \end{gathered} x = z 2 k + z − 2 k = ( − ω ) 2 k + ( − ω ) − 2 k = ( ω ) 2 k + ( ω ) − 2 k = ω k + ω − k
Considering k = 3 m , 3 m + 1 , 3 m + 2 k=3m,3m+1,3m+2 k = 3 m , 3 m + 1 , 3 m + 2 , we get that x x x has two possible values.
Example 7 Assume complex numbers z = cos θ + i sin θ ( 0 < θ < π ) z = \cos\theta + i\sin\theta(0 < \theta < \pi) z = cos θ + i sin θ ( 0 < θ < π ) , w = 1 − ( z ‾ ) 4 1 + z 4 w = \frac{1 - (\overline{z})^4}{1 + z^4} w = 1 + z 4 1 − ( z ) 4 , and ∣ w ∣ = 3 3 |w| = \frac{\sqrt{3}}{3} ∣ w ∣ = 3 3 , arg w < π 2 \arg w < \frac{\pi}{2} arg w < 2 π , and find θ \theta θ .
w = ( 1 − cos 4 θ ) + i sin 4 θ ( 1 + cos 4 θ ) + i sin 4 θ = 2 sin 2 2 θ + 2 sin 2 θ cos 2 θ i 2 cos 2 2 θ + 2 sin 2 θ cos 2 θ i = tan 2 θ sin 2 θ + i cos 2 θ cos 2 θ + i sin 2 θ = tan 2 θ cos ( π 2 − 2 θ ) + i sin ( π 2 − 2 θ ) cos 2 θ + i sin 2 θ = tan 2 θ [ cos ( π 2 − 4 θ ) + i sin ( π 2 − 4 θ ) ] \begin{gathered} w\\ =\frac{(1-\cos4\theta)+i\sin4\theta}{(1+\cos4\theta)+i\sin4\theta}\\ =\frac{2\sin^{2}2\theta+2\sin2\theta\cos2\theta i}{2\cos^{2}2\theta+2\sin2\theta\cos2\theta i}\\ =\tan2\theta\frac{\sin2\theta+i\cos2\theta}{\cos2\theta+i\sin2\theta}\\ =\tan2\theta\frac{\cos(\frac{\pi}{2}-2\theta)+i\sin(\frac{\pi}{2}-2\theta)}{\cos2\theta+i\sin2\theta}\\ =\tan2\theta[\cos(\frac{\pi}{2}-4\theta)+i\sin(\frac{\pi}{2}-4\theta)] \end{gathered} w = ( 1 + cos 4 θ ) + i sin 4 θ ( 1 − cos 4 θ ) + i sin 4 θ = 2 cos 2 2 θ + 2 sin 2 θ cos 2 θ i 2 sin 2 2 θ + 2 sin 2 θ cos 2 θ i = tan 2 θ cos 2 θ + i sin 2 θ sin 2 θ + i cos 2 θ = tan 2 θ cos 2 θ + i sin 2 θ cos ( 2 π − 2 θ ) + i sin ( 2 π − 2 θ ) = tan 2 θ [ cos ( 2 π − 4 θ ) + i sin ( 2 π − 4 θ )]
Requirements: ∣ tan 2 θ ∣ = ∣ w ∣ = 3 3 , 2 θ = ± 1 6 π + k π |\tan2\theta|=|w|=\frac{\sqrt{3}}{3},2\theta=\pm\frac{1}{6}\pi+k\pi ∣ tan 2 θ ∣ = ∣ w ∣ = 3 3 , 2 θ = ± 6 1 π + k π
Case 1 tan 2 θ = 3 3 \tan2\theta=\frac{\sqrt{3}}{3} tan 2 θ = 3 3 θ = 1 12 π or 7 12 π \theta=\frac{1}{12}\pi\text{ or }\frac{7}{12}\pi θ = 12 1 π or 12 7 π w = 3 3 ( cos π 6 + i sin π 6 ) , arg ( w ) = π 3 < π 2 w=\frac{\sqrt{3}}{3}(\cos\frac{\pi}{6}+i\sin\frac{\pi}{6}),\arg(w)=\frac{\pi}{3}\lt\frac{\pi}{2} w = 3 3 ( cos 6 π + i sin 6 π ) , arg ( w ) = 3 π < 2 π
Situation 2 tan 2 θ = − 3 3 \tan2\theta=-\frac{\sqrt{3}}{3} tan 2 θ = − 3 3 θ = 5 12 π or 11 12 π \theta=\frac{5}{12}\pi\text{ or }\frac{11}{12}\pi θ = 12 5 π or 12 11 π w = − 3 3 ( cos 5 6 π + i sin 5 6 π ) = 3 3 ( cos 11 π 6 + i sin 11 π 6 ) arg ( w ) > π 2 w=-\frac{\sqrt{3}}{3}(\cos\frac{5}{6}\pi+i\sin\frac{5}{6}\pi)=\frac{\sqrt{3}}{3}(\cos\frac{11\pi}{6}+i\sin\frac{11\pi}{6})\\ \arg(w)\gt\frac{\pi}{2} w = − 3 3 ( cos 6 5 π + i sin 6 5 π ) = 3 3 ( cos 6 11 π + i sin 6 11 π ) arg ( w ) > 2 π
To sum up, θ = 1 12 π or 7 12 π \theta=\frac{1}{12}\pi\text{ or }\frac{7}{12}\pi θ = 12 1 π or 12 7 π
Example 8 Proof: cos π 7 − cos 2 π 7 + cos 3 π 7 = 1 2 \cos\frac{\pi}{7} - \cos\frac{2\pi}{7} + \cos\frac{3\pi}{7} = \frac{1}{2} cos 7 π − cos 7 2 π + cos 7 3 π = 2 1
Construct an equation: z 7 − 1 = 0 z^7-1=0 z 7 − 1 = 0
By de Mauve's formula: z k = cos 2 k π 7 + i sin 2 k π 7 , k = 0 , 1 , 2 , . . . , 6 z_k=\cos\frac{2k\pi}{7}+i\sin\frac{2k\pi}{7},k=0,1,2,...,6 z k = cos 7 2 k π + i sin 7 2 k π , k = 0 , 1 , 2 , ... , 6
According to Vedic theorem: z 0 + z 1 + z 2 + . . . + z 6 = 0 z_0+z_1+z_2+...+z_6=0 z 0 + z 1 + z 2 + ... + z 6 = 0
The real part is equal to 0:
1 + cos 2 7 π + cos 4 7 π + cos 6 7 π + cos 8 7 π + cos 10 7 π + cos 12 7 π = 1 − 2 ( cos π 7 − cos 2 π 7 + cos 3 π 7 ) = 0 \begin{gathered} 1+\cos\frac{2}{7}\pi+\cos\frac{4}{7}\pi+\cos\frac{6}{7}\pi+\cos\frac{8}{7}\pi+\cos\frac{10}{7}\pi+\cos\frac{12}{7}\pi\\ =1-2(\cos\frac{\pi}{7} - \cos\frac{2\pi}{7} + \cos\frac{3\pi}{7})=0 \end{gathered} 1 + cos 7 2 π + cos 7 4 π + cos 7 6 π + cos 7 8 π + cos 7 10 π + cos 7 12 π = 1 − 2 ( cos 7 π − cos 7 2 π + cos 7 3 π ) = 0
Q.E.D
If you consider using trigonometric identity transformation:
cos π 7 − cos 2 π 7 + cos 3 π 7 = cos π 7 + cos 3 π 7 + cos 5 π 7 \begin{gathered} \cos\frac{\pi}{7} - \cos\frac{2\pi}{7} + \cos\frac{3\pi}{7}\\ =\cos\frac{\pi}{7}+\cos\frac{3\pi}{7}+\cos\frac{5\pi}{7} \end{gathered} cos 7 π − cos 7 2 π + cos 7 3 π = cos 7 π + cos 7 3 π + cos 7 5 π
For the sum of trigonometric functions of equal angles, the solution is: multiply by ** twice the sine of half the difference angle **
2 sin π 7 ( cos π 7 + cos 3 π 7 + cos 5 π 7 ) = sin 2 π 7 + sin 0 + sin 4 π 7 − sin − 2 π 7 + sin 6 π 7 − sin 4 π 7 = sin π 7 \begin{gathered} 2\sin\frac{\pi}{7}(\cos\frac{\pi}{7}+\cos\frac{3\pi}{7}+\cos\frac{5\pi}{7})\\ =\sin\frac{2\pi}{7}+\sin0+\sin\frac{4\pi}{7}-\sin\frac{-2\pi}{7}+\sin\frac{6\pi}{7}-\sin\frac{4\pi}{7}\\ =\sin\frac{\pi}{7} \end{gathered} 2 sin 7 π ( cos 7 π + cos 7 3 π + cos 7 5 π ) = sin 7 2 π + sin 0 + sin 7 4 π − sin 7 − 2 π + sin 7 6 π − sin 7 4 π = sin 7 π
Q.E.D
Example 9 Simplify sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x \frac{\sin x + \sin 3x + \sin 5x + \cdots + \sin(2n-1)x}{\cos x + \cos 3x + \cos 5x + \cdots + \cos(2n-1)x} c o s x + c o s 3 x + c o s 5 x + ⋯ + c o s ( 2 n − 1 ) x s i n x + s i n 3 x + s i n 5 x + ⋯ + s i n ( 2 n − 1 ) x .
sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x = 2 sin x [ sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x ] 2 sin x [ cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x ] = − [ ( cos 2 x − cos 0 ) + ( cos 4 x − cos 2 x ) + ( cos 6 x − cos 4 x ) + . . . + ( cos 2 n x − cos ( 2 n − 2 ) x ] ( sin 2 x − sin 0 ) + ( sin 4 x − sin 2 x ) + ( sin 6 x − sin 4 x ) + . . . + ( sin 2 n x − sin ( 2 n − 2 ) x ) = 1 − cos 2 n x sin 2 n x = 2 sin 2 n x 2 sin n x cos n x = tan n x \begin{gathered} \frac{\sin x + \sin 3x + \sin 5x + \cdots + \sin(2n-1)x}{\cos x + \cos 3x + \cos 5x + \cdots + \cos(2n-1)x}\\ =\frac{2\sin x[\sin x + \sin 3x + \sin 5x + \cdots + \sin(2n-1)x]}{2\sin x[\cos x + \cos 3x + \cos 5x + \cdots + \cos(2n-1)x]}\\ =\frac{-[(\cos2x-\cos0)+(\cos4x-\cos2x)+(\cos6x-\cos4x)+...+(\cos2nx-\cos(2n-2)x]}{(\sin2x-\sin0)+(\sin4x-\sin2x)+(\sin6x-\sin4x)+...+(\sin2nx-\sin(2n-2)x)}\\ =\frac{1-\cos2nx}{\sin2nx}\\ =\frac{2\sin^2nx}{2\sin nx\cos nx}\\ =\tan{nx} \end{gathered} cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x = 2 sin x [ cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x ] 2 sin x [ sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x ] = ( sin 2 x − sin 0 ) + ( sin 4 x − sin 2 x ) + ( sin 6 x − sin 4 x ) + ... + ( sin 2 n x − sin ( 2 n − 2 ) x ) − [( cos 2 x − cos 0 ) + ( cos 4 x − cos 2 x ) + ( cos 6 x − cos 4 x ) + ... + ( cos 2 n x − cos ( 2 n − 2 ) x ] = sin 2 n x 1 − cos 2 n x = 2 sin n x cos n x 2 sin 2 n x = tan n x
How to consider complex numbers: let z = cos x + i sin x z=\cos x+i\sin x z = cos x + i sin x
So there are: { cos n x = z n + z ‾ n 2 , sin n x = z n − z ‾ n 2 i \begin{cases} \cos nx=\frac{z^n+\overline{z}^n}{2},\\ \sin nx=\frac{z^n-\overline{z}^n}{2i} \end{cases} { cos n x = 2 z n + z n , sin n x = 2 i z n − z n
So the numerator:
sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x = 1 2 i [ ( z + z 3 + . . . + z 2 n − 1 ) − ( z ‾ + z ‾ 3 + . . . + z ‾ 2 n − 1 ) ] = 1 2 i [ z 2 n + 1 − z z 2 − 1 − z ‾ 2 n + 1 − z ‾ z ‾ 2 − 1 ] = 1 2 i [ z 2 n + 1 − z z 2 − z z ‾ − z ‾ 2 n + 1 − z ‾ z ‾ 2 − z z ‾ ] = 1 2 i [ ( z 2 n − 1 ) + ( z ‾ 2 n − 1 ) z − z ‾ ] = 1 2 i ( z n − z ‾ n ) 2 z − z ‾ = ( z n − z ‾ n 2 i ) 2 2 i z − z ‾ = sin 2 n x sin x \begin{gathered} \sin x + \sin 3x + \sin 5x + \cdots + \sin(2n-1)x\\ =\frac{1}{2i}[(z+z^3+...+z^{2n-1})-(\overline{z}+\overline{z}^3+...+\overline{z}^{2n-1})]\\ =\frac{1}{2i}[\frac{z^{2n+1}-z}{z^2-1}-\frac{\overline{z}^{2n+1}-\overline{z}}{\overline{z}^2-1}]\\ =\frac{1}{2i}[\frac{z^{2n+1}-z}{z^2-z\overline{z}}-\frac{\overline{z}^{2n+1}-\overline{z}}{\overline{z}^2-z\overline{z}}]\\ =\frac{1}{2i}[\frac{(z^{2n}-1)+(\overline{z}^{2n}-1)}{z-\overline{z}}]\\ =\frac{1}{2i}\frac{(z^n-\overline{z}^n)^2}{z-\overline{z}}=(\frac{z^n-\overline{z}^n}{2i})^2\frac{2i}{z-\overline{z}}=\frac{\sin^2 nx}{\sin x} \end{gathered} sin x + sin 3 x + sin 5 x + ⋯ + sin ( 2 n − 1 ) x = 2 i 1 [( z + z 3 + ... + z 2 n − 1 ) − ( z + z 3 + ... + z 2 n − 1 )] = 2 i 1 [ z 2 − 1 z 2 n + 1 − z − z 2 − 1 z 2 n + 1 − z ] = 2 i 1 [ z 2 − z z z 2 n + 1 − z − z 2 − z z z 2 n + 1 − z ] = 2 i 1 [ z − z ( z 2 n − 1 ) + ( z 2 n − 1 ) ] = 2 i 1 z − z ( z n − z n ) 2 = ( 2 i z n − z n ) 2 z − z 2 i = sin x sin 2 n x
The same denominator:
cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x = 1 2 [ ( z + z 3 + . . . + z 2 n − 1 ) + ( z ‾ + z ‾ 3 + . . . + z ‾ 2 n − 1 ) ] = 1 2 [ ( z 2 n − 1 ) − ( z ‾ 2 n − 1 ) z − z ‾ ] = 1 2 [ ( z n + z ‾ n ) ( z n − z ‾ n ) z − z ‾ ] = ( z n + z ‾ n 2 ) ( z n − z ‾ n 2 ) ( 2 i z − z ‾ ) = sin n x cos n x sin x \begin{gathered} \cos x + \cos 3x + \cos 5x + \cdots + \cos(2n-1)x\\ =\frac{1}{2}[(z+z^3+...+z^{2n-1})+(\overline{z}+\overline{z}^3+...+\overline{z}^{2n-1})]\\ =\frac{1}{2}[\frac{(z^{2n}-1)-(\overline{z}^{2n}-1)}{z-\overline{z}}]\\ =\frac{1}{2}[\frac{(z^n+\overline{z}^n)(z^n-\overline{z}^n)}{z-\overline{z}}]\\ =(\frac{z^n+\overline{z}^n}{2})(\frac{z^n-\overline{z}^n}{2})(\frac{2i}{z-\overline{z}})=\frac{\sin nx\cos nx}{\sin x} \end{gathered} cos x + cos 3 x + cos 5 x + ⋯ + cos ( 2 n − 1 ) x = 2 1 [( z + z 3 + ... + z 2 n − 1 ) + ( z + z 3 + ... + z 2 n − 1 )] = 2 1 [ z − z ( z 2 n − 1 ) − ( z 2 n − 1 ) ] = 2 1 [ z − z ( z n + z n ) ( z n − z n ) ] = ( 2 z n + z n ) ( 2 z n − z n ) ( z − z 2 i ) = sin x sin n x cos n x
Divide to get tan n x \tan nx tan n x
Example 10 Familiar: tan α 2 = 1 − cos α sin α = sin α 1 + cos α \tan\frac{\alpha}{2}=\frac{1-\cos\alpha}{\sin\alpha}=\frac{\sin\alpha}{1+\cos\alpha} tan 2 α = s i n α 1 − c o s α = 1 + c o s α s i n α
Use the sum ratio theorem:
1 + sin α − cos α 1 + sin α + cos α = tan α 2 \frac{1 + \sin\alpha - \cos\alpha}{1 + \sin\alpha + \cos\alpha} = \tan\frac{\alpha}{2} 1 + sin α + cos α 1 + sin α − cos α = tan 2 α
1 + 2 sin α − cos α 1 + sin α + 2 cos α = tan α 2 \frac{1 + 2\sin\alpha - \cos\alpha}{1 + \sin\alpha + 2\cos\alpha} = \tan\frac{\alpha}{2} 1 + sin α + 2 cos α 1 + 2 sin α − cos α = tan 2 α
3 + 2 sin α − 3 cos α 2 + 3 sin α + 2 cos α = tan α 2 \frac{\sqrt{3} + \sqrt{2}\sin\alpha - \sqrt{3}\cos\alpha}{\sqrt{2} + \sqrt{3}\sin\alpha + \sqrt{2}\cos\alpha} = \tan\frac{\alpha}{2} 2 + 3 sin α + 2 cos α 3 + 2 sin α − 3 cos α = tan 2 α