Analyzing the Setup
Imagine you are standing on a Cartesian plane. You see two fixed anchors: point A(7,0) on the x-axis and point B(0,−5) on the y-axis. These two points define a fixed, unmoving line, AB.
Now, imagine a second line, PQ, dancing across the axes. It is not just any line; it is a line that maintains a strict, perpendicular relationship with our fixed line AB.
As PQ slides, its intercepts P(p,0) and Q(0,q) change. Consequently, the intersection point R of the lines AQ and BP traces a path. Our mission is to uncover the secret shape of this path—the locus of R.
The Fixed Foundation
First, let us respect the fixed line AB. Its slope, m1, is the gatekeeper of our perpendicularity condition. Using the slope formula:
This value is our constant. It tells us exactly how the line AB is tilted.
Any line perpendicular to it must have a slope m2 such that m1⋅m2=−1. This means m2=−57. This is the fundamental constraint governing our variable line PQ.
The Variable Dancer
Now, consider the line PQ. It cuts the x-axis at P(p,0) and the y-axis at Q(0,q). Its slope is:
Applying our perpendicularity condition, we set −pq=−57, which simplifies beautifully to 5q=7p.
This is the heartbeat of our problem—a simple, elegant relationship between the intercepts p and q that must hold true at every moment of the dance.
The Intersection
We are interested in the intersection point R(h,k) of lines AQ and BP. Using the intercept form, the equation of line AQ is:
Since R(h,k) lies on this line, we have 7h+qk=1. Rearranging this to isolate q, we find:
Similarly, the equation of line BP is px−5y=1. Substituting R(h,k) gives ph−5k=1, which leads us to:
The Algebraic Symphony
We now have p and q expressed in terms of the coordinates of R(h,k). We return to our heartbeat equation: 5q=7p.
Substituting our expressions for p and q, we get:
Notice the symmetry! We can divide both sides by 35, leaving us with:
Cross-multiplying yields k(5+k)=h(7−h), or 5k+k2=7h−h2. Rearranging everything to one side, we arrive at h2+k2−7h+5k=0.
Replacing (h,k) with (x,y), we find the locus:
Conclusion
The Circle Revealed
What we have discovered is that the point R does not wander aimlessly. It is bound to the path of a circle.
The perpendicularity of the lines AB and PQ forces the intersection point R to trace this perfect, closed curve. It is a testament to the hidden order in coordinate geometry—where seemingly independent variables p and q are locked in a dance that results in a beautiful, symmetric shape.