Analyzing the Setup
Welcome, fellow traveler of the complex plane! Today, we are going to unravel a problem that might look like a tangled mess of variables, but is actually a beautiful, symmetrical dance of complex numbers.
Imagine you are standing on the Argand plane. You have a point z1 that is moving, and a point z2 that is fixed but "not unimodular."
We are given the relationship:
w=2−z1zˉ2z1−2z2
This expression
w is unimodular, which means the distance of this complex number
w from the origin is exactly
1. We start by writing
∣w∣=1.
The Magic of Conjugates
Now, the magic begins. We cross-multiply to get ∣z1−2z2∣=∣2−z1zˉ2∣.
Squaring both sides is our next logical step, leading us to:
∣z1−2z2∣2=∣2−z1zˉ2∣2
Here is where the "Golden Key" of complex numbers comes in: the identity ∣z∣2=zzˉ. By applying this to both sides, we transform the modulus into a product of the number and its conjugate.
As we expand the expression:
(z1−2z2)(zˉ1−2zˉ2)=(2−z1zˉ2)(2−zˉ1z2)
Something miraculous happens. The cross-terms, those pesky
−2z1zˉ2 and
−2zˉ1z2, appear on both sides of the equation! They cancel out perfectly, leaving us with a clean, elegant relationship:
∣z1∣2+4∣z2∣2=4+∣z1∣2∣z2∣2
The Final Revelation
We rearrange this to factorize it into:
(∣z1∣2−4)(1−∣z2∣2)=0
Since the problem explicitly tells us that z2 is not unimodular, we know that 1−∣z2∣2 cannot be zero. Therefore, the only way for this product to be zero is if ∣z1∣2−4=0.
This simplifies to:
∣z1∣=2
And there it is! The locus of z1 is a circle of radius 2 centered at the origin. You have just navigated through the algebra to find a geometric truth.