Analyzing the Setup
We begin with the parabola y2=4x. This is our canvas, a standard rightward-opening parabola where the axis of symmetry is the x-axis, defined by the equation y=0.
The Power of Parametric Coordinates
We are given two distinct points, A and B, on this parabola. To avoid the algebraic burden of Cartesian coordinates, we utilize parametric coordinates.
For a parabola y2=4ax with a=1, any point can be represented as (t2,2t). Thus, we define our points as A=(t12,2t1) and B=(t22,2t2).
The Circle's Dance
Consider a circle with AB as its diameter. The center of this circle, C, is the midpoint of the segment AB. Using the midpoint formula, the coordinates of C are:
C=(2t12+t22,22t1+2t2)=(2t12+t22,t1+t2)
We are told that this circle touches the x-axis. Geometrically, this means the perpendicular distance from the center C to the x-axis is exactly equal to the radius r.
The distance from a point (x,y) to the x-axis is ∣y∣. Therefore, we have the condition:
This implies that t1+t2=±r. This result serves as the bridge between our geometric setup and our final answer.
The Algebraic Symphony
Next, we determine the slope m of the line joining A and B. Using the slope formula m=x2−x1y2−y1, we substitute our parametric coordinates:
The denominator is a difference of squares, which factors as (t2−t1)(t2+t1). Since A and B are distinct points, $t_1
eq t_2$, allowing us to simplify:
m=(t2−t1)(t2+t1)2(t2−t1)=t1+t22
Final Calculation
Substituting the tangency condition t1+t2=±r into our slope equation, we obtain:
The possible values for the slope are r2 and −r2. We have successfully navigated the geometry and simplified the algebra to reach this elegant conclusion.