Animated Solution for Mathematics - Complex Numbers: Find all non-zero complex numbers Z satisfying Zˉ=iZ2.
Visualized Solution
Visualizing the Equation Zˉ=iZ2
Given equation: Zˉ=iZ2
We need to find all non-zero solutions Z∈C∖{0}.
Taking the Modulus
Take modulus on both sides: ∣Zˉ∣=∣iZ2∣
Apply property: ∣z1z2∣=∣z1∣∣z2∣
Apply property: ∣Zˉ∣=∣Z∣
Simplifying the Magnitude
∣Z∣=∣i∣∣Z2∣
Since ∣i∣=1, we have ∣Z∣=∣Z∣2
The Unit Circle Constraint
Given Z=0, then ∣Z∣=0
Dividing by ∣Z∣: 1=∣Z∣
All solutions lie on the unit circle.
Using Euler's Form Z=eiθ
Let Z=eiθ
Then Zˉ=e−iθ
And Z2=(eiθ)2=ei2θ
Substituting into the Equation
Substitute into Zˉ=iZ2:
e−iθ=iei2θ
Converting i to Exponential Form
We know i=eiπ/2
Equation: e−iθ=eiπ/2ei2θ
Simplify: e−iθ=ei(π/2+2θ)
Equating the Exponents
Equate exponents: −θ=2π+2θ+2kπ
Where k∈Z
Solving for θ
Rearrange: −3θ=2π+2kπ
Divide by −3: θ=−6π−32kπ
Finding the First Root (k=0)
For k=0: θ=−6π
Z1=cos(−6π)+isin(−6π)
Z1=23−2i
Finding the Second Root (k=1)
For k=1: θ=−6π−32π=−65π
Z2=cos(−65π)+isin(−65π)
Z2=−23−2i
Finding the Third Root (k=2)
For k=2: θ=−6π−34π=−69π=−23π
Note: −23π is equivalent to 2π
Z3=cos(2π)+isin(2π)=i
Summary and Final Takeaway
Final Solutions: i,23−2i,−23−2i
Key Takeaway: Equations of the form Zˉ=aZn often lead to roots distributed symmetrically on a circle.
Challenge: Try solving Zˉ=Z3 using the same method!
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The Sigma Insight: Euler's Form and De Moivre's Theorem
Solution Diagram
Analyzing the Setup
We are tasked with solving the equation Zˉ=iZ2 for all non-zero complex numbers Z. This equation represents a fascinating intersection of algebraic manipulation and geometric rotation within the complex plane.
The Modulus Insight
When dealing with equations involving both Z and its conjugate Zˉ, the modulus is our most effective tool. By taking the modulus of both sides, we isolate the distance of the solutions from the origin:
∣Zˉ∣=∣iZ2∣
Using the properties of the modulus, where ∣Zˉ∣=∣Z∣ and ∣iZ2∣=∣i∣∣Z∣2, and knowing that ∣i∣=1, the equation simplifies to:
∣Z∣=∣Z∣2
Since we are searching for non-zero solutions, we divide by ∣Z∣ to find ∣Z∣=1. Geometrically, this confirms that all solutions must lie on the unit circle.
The Euler Transformation
With the constraint ∣Z∣=1, we can represent any solution using Euler's formula, Z=eiθ. Substituting this into the original equation, we have Zˉ=e−iθ and Z2=ei2θ.
The equation becomes:
e−iθ=iei2θ
To solve for θ, we express the imaginary unit i as eiπ/2. The equation then transforms into:
e−iθ=eiπ/2⋅ei2θ=ei(π/2+2θ)
The Periodic Dance
Because the complex exponential is periodic, we equate the exponents by accounting for the 2kπ rotation factor, where k is an integer:
−θ=2π+2θ+2kπ
Rearranging the terms to isolate θ yields:
−3θ=2π+2kπ
θ=−6π−32kπ
Final Calculation
We now evaluate the expression for k=0,1,2 to find the distinct roots: