The Geometry of Orthogonality
A Journey into Homogeneous Equations
Imagine you are standing at the origin of a coordinate plane. You have two lines, both passing through your feet, stretching out into the infinite expanse of the xy-plane.
You want these lines to be perfectly perpendicular—a perfect cross, a symbol of absolute balance. We can force this condition using the elegant world of homogeneous equations of the second degree.
The Canvas
Homogeneous Equations
We start with the given equation:
At first glance, this might look like just another jumble of variables. However, every term here is of degree 2.
The x2 term, the xy term, and the y2 term all share the same weight. This is a homogeneous equation of degree 2, which is the geometric signature of a pair of straight lines passing through the origin (0,0).
The Condition of Perpendicularity
To understand how these lines behave, we compare our equation to the standard form:
By matching the coefficients, we identify our players: A=3a, 2H=5, and B=a2−2.
The condition for these two lines to be perpendicular is:
This occurs because if the slopes of the lines are m1 and m2, they must satisfy m1m2=−1. When you derive the relationship between the coefficients and the slopes, the H term vanishes, leaving us with the requirement that the sum of the coefficients of x2 and y2 must be zero.
The Algebraic Resolution
Now, we substitute our values into the condition A+B=0:
Rearranging this, we find a quadratic equation in a:
To determine how many values of a satisfy this, we calculate the discriminant D=b2−4ac, where b=3, a=1, and c=−2.
Since D=17, which is strictly greater than zero, we know with absolute certainty that this quadratic equation yields two distinct, real roots.
The Final Insight
We started with a general equation, identified its geometric nature, and applied the condition for perpendicularity. Because the discriminant is positive, we conclude that there are exactly two values of a for which these lines will stand at a perfect 90∘ angle to each other.