A complex number z=x+iy can be plotted as the point (x,y), or equivalently as the position vector from the origin O to that point, in the Argand plane (named for Jean Argand) — the x-axis is the real axis and the y-axis is the imaginary axis. This geometric picture turns algebraic facts about z into statements about points, lines and circles.
Distance and circles. Since ∣z1−z2∣ is the distance between the points z1 and z2, the equation
∣z−z0∣=r(r>0)
is exactly the set of points at distance r from the fixed point z0 — i.e. the complex form of a circle with centre z0 and radius r. Correspondingly:
- ∣z−z0∣<r describes the interior of that circle;
- ∣z−z0∣>r describes the exterior.
An equation like ∣αz−β∣=γ (α=0) is first rewritten as ∣z−(β/α)∣=γ/∣α∣ to read off centre β/α and radius γ/∣α∣.
Loci from conditions on z,z. Many geometric conditions translate directly:
- ∣z−a∣=∣z−b∣ (equidistant from two fixed points) is the perpendicular bisector of the segment joining a,b — e.g. ∣z+2∣=∣z−2∣ gives the imaginary axis, since ±2 are symmetric about it.
- Conditions like Re(iz)=k, Im[(a+ib)z+c]=0, or z=z−1 each reduce, after substituting z=x+iy and separating real/imaginary parts, to an ordinary Cartesian equation in x,y — a line, a circle, or (as with z=z−1⟺zz=1⟺x2+y2=1) the unit circle.
- An argument condition, e.g. arg(z+2z−i)=4π, fixes the angle a chord subtends and typically traces an arc of a circle; converting to Cartesian form again proceeds by writing z=x+iy, isolating the real/imaginary parts of the quotient, and using tan(angle).
The working method is always the same: substitute z=x+iy (and z=x−iy), simplify the given expression into the form (real stuff)+i(real stuff), then read off what the condition (equality of moduli, a purely real/imaginary condition, a fixed argument) forces on x and y.