Condition for Pairs of Lines through Origin to be Harmonic Conjugates/Homogeneous Quadratic Equation Form
Theorem
Consider the two homogeneous quadratic equations:
\(\text {(E1)}: \quad\) | \(\ds a_1 x^2 + 2 h_1 x y + b_1 y^2\) | \(=\) | \(\ds 0\) | |||||||||||
\(\text {(E2)}: \quad\) | \(\ds a_2 x^2 + 2 h_2 x y + b_2 y^2\) | \(=\) | \(\ds 0\) |
each representing two straight lines through the origin.
Then the two straight lines represented by $(\text E1)$ are harmonic conjugates of the two straight lines represented by $(\text E2)$ if and only if:
- $a_1 b_2 + a_2 b_1 - 2 h_1 h_2 = 0$
Proof
From Homogeneous Quadratic Equation represents Two Straight Lines through Origin, $(\text E1)$ and $(\text E2)$ represent straight lines through the origin if and only if:
\(\ds h_1^2 - a_1 b_1\) | \(>\) | \(\ds 0\) | ||||||||||||
\(\ds h_2^2 - a_2 b_2\) | \(>\) | \(\ds 0\) |
Let the two straight lines represented by $(\text E1)$ be defined by the equations:
\(\ds y\) | \(=\) | \(\ds \lambda_1 x\) | ||||||||||||
\(\ds y\) | \(=\) | \(\ds \mu_1 x\) |
Let the two straight lines represented by $(\text E2)$ be defined by the equations:
\(\ds y\) | \(=\) | \(\ds \lambda_2 x\) | ||||||||||||
\(\ds y\) | \(=\) | \(\ds \mu_2 x\) |
Then we can write the Condition for Pairs of Lines through Origin to be Harmonic Conjugates as:
- $(1): \quad 2 \paren {\lambda_1 \mu_1 + \lambda_2 \mu_2} = \paren {\lambda_1 + \mu_1} \paren {\lambda_2 + \mu_2}$
We can express $a_1 x^2 + 2 h_1 x y + b_1 y^2 = 0$ as:
- $b_1 \paren {y - \lambda_1 x} \paren {y - \mu_1 x} = 0$
and $a_2 x^2 + 2 h_2 x y + b_2 y^2 = 0$ as:
- $b_2 \paren {y - \lambda_2 x} \paren {y - \mu_2 x} = 0$
from which we obtain via Sum of Roots of Quadratic Equation and Product of Roots of Quadratic Equation:
\(\ds \lambda_1 + \mu_1\) | \(=\) | \(\ds -\dfrac {2 h_1} {b_1}\) | ||||||||||||
\(\ds \lambda_2 + \mu_2\) | \(=\) | \(\ds -\dfrac {2 h_2} {b_2}\) | ||||||||||||
\(\ds \lambda_1 \mu_1\) | \(=\) | \(\ds \dfrac {a_1} {b_1}\) | ||||||||||||
\(\ds \lambda_2 \mu_2\) | \(=\) | \(\ds \dfrac {a_2} {b_2}\) |
Therefore $(1)$ reduces to:
\(\ds 2 \paren {\dfrac {a_1} {b_1} + \dfrac {a_2} {b_2} }\) | \(=\) | \(\ds \dfrac {4 h_1 h_2} {b_1 b_2}\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds a_1 b_2 + a_2 b_1 - 2 h_1 h_2\) | \(=\) | \(\ds 0\) |
$\blacksquare$
Sources
- 1933: D.M.Y. Sommerville: Analytical Conics (3rd ed.) ... (previous) ... (next): Chapter $\text {II}$. The Straight Line: $21$. Condition that the two pairs of lines $\ldots$ should be apolar