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Formulas/maths/M4c Conics/Chord of Circle |z| = r Joining z₁ and z₂

Chord of Circle |z| = r Joining z₁ and z₂

Equation of the chord joining two points z₁, z₂ on the circle |z|=r. When z₁→z₂, this becomes the tangent at z₁: zz̄₁ + z̄z₁ = 2r², equivalently z/z₁ + z̄/z̄₁ = 2. The chord of contact from an external point z₀ is: zz̄₀ + z̄z₀ = 2r². Connects back to: Circles chapter (chord, tangent, chord of contact).
Derivation

For the circle z=r|z| = r, every point satisfies zzˉ=r2z\bar{z} = r^2. This single identity is the key to deriving both the chord and tangent equations cleanly.

Setup

Let z1z_1 and z2z_2 be two points on z=r|z| = r. So:

z1zˉ1=r2andz2zˉ2=r2z_1\bar{z}_1 = r^2 \quad \text{and} \quad z_2\bar{z}_2 = r^2

Equation of the Chord

The equation of the line through z1z_1 and z2z_2 (from the general line formula) can be written as:

z(zˉ1+zˉ2)+zˉ(z1+z2)=2r2z(\bar{z}_1 + \bar{z}_2) + \bar{z}(z_1 + z_2) = 2r^2

Verification: Substitute z=z1z = z_1:

z1(zˉ1+zˉ2)+zˉ1(z1+z2)=z1zˉ1+z1zˉ2+zˉ1z1+zˉ1z2=2r2+z1zˉ2+zˉ1z2z_1(\bar{z}_1 + \bar{z}_2) + \bar{z}_1(z_1 + z_2) = z_1\bar{z}_1 + z_1\bar{z}_2 + \bar{z}_1 z_1 + \bar{z}_1 z_2 = 2r^2 + z_1\bar{z}_2 + \bar{z}_1 z_2

Wait — this equals 2r2+2Re(z1zˉ2)2r^2 + 2\operatorname{Re}(z_1\bar{z}_2), not 2r22r^2 in general. Let me derive more carefully.

Correct derivation: For the line through two points z1z_1, z2z_2 on z=r|z|=r, use the fact that any point zz on the chord satisfies collinearity with z1z_1, z2z_2 — i.e., (zz1)/(zˉzˉ1)(z - z_1)/(\bar{z} - \bar{z}_1) equals the complex slope (z2z1)/(zˉ2zˉ1)(z_2 - z_1)/(\bar{z}_2 - \bar{z}_1).

Since z1zˉ1=r2z_1\bar{z}_1 = r^2, we have zˉ1=r2/z1\bar{z}_1 = r^2/z_1. Substituting both zˉ1\bar{z}_1 and zˉ2\bar{z}_2:

zˉ1=r2z1,zˉ2=r2z2\bar{z}_1 = \frac{r^2}{z_1}, \qquad \bar{z}_2 = \frac{r^2}{z_2}

The chord equation reduces to:

zr2z1z2(z1+z2)+zˉ(z1+z2)=r2(z1+z2)2z1z2z \cdot \frac{r^2}{z_1 z_2}(z_1 + z_2) + \bar{z}(z_1 + z_2) = \frac{r^2(z_1+z_2)^2}{z_1 z_2} - \ldots

The cleanest route: use the parametric approach with z1=reiαz_1 = re^{i\alpha}, z2=reiβz_2 = re^{i\beta}.

The chord joining reiαre^{i\alpha} and reiβre^{i\beta} has equation:

zei(α+β)/2+zˉei(α+β)/2=2rcos ⁣αβ2z e^{-i(\alpha+\beta)/2} + \bar{z} e^{i(\alpha+\beta)/2} = 2r\cos\!\frac{\alpha-\beta}{2}

Tangent at a Point

As z2z1z_2 \to z_1 (i.e., βα\beta \to \alpha), the chord becomes the tangent. Setting α=β\alpha = \beta:

zeiα+zˉeiα=2rz e^{-i\alpha} + \bar{z} e^{i\alpha} = 2r

Multiplying through by eiαe^{i\alpha} and using z1=reiαz_1 = re^{i\alpha}, so eiα=z1/re^{i\alpha} = z_1/r:

zzˉ1r+zˉz1r=2rz \cdot \frac{\bar{z}_1}{r} + \bar{z} \cdot \frac{z_1}{r} = 2r zzˉ1+zˉz1=2r2\boxed{z\bar{z}_1 + \bar{z}z_1 = 2r^2}

Chord of Contact

For an external point z0z_0, the chord joining the two tangent points has equation:

zzˉ0+zˉz0=2r2z\bar{z}_0 + \bar{z}z_0 = 2r^2

This has the same form as the tangent equation — replacing the point on the circle z1z_1 with the external point z0z_0. This is the T=S1T = S_1 pattern in complex form, connecting back to the Circles chapter.