Analyzing the Setup
Imagine you are standing on a coordinate plane, looking at two fixed points, A(3,7) and B(6,5). These points are the anchors of our universe today.
We are not just looking at one circle; we are looking at an infinite family of circles that pass through these two points. It is a beautiful, breathing structure.
Our mission is to intersect this family with a fixed circle, C0:x2+y2−4x−6y−3=0, and prove that the resulting common chords are not chaotic—they are perfectly concurrent.
The Power of the Family
To master this, we must use the most elegant tool in our arsenal: the family of circles equation, S+λL=0. Here, L=0 is the line passing through A and B.
We calculate the slope of AB as:
Using the point-slope form, we derive the line L:
For our base circle S, we choose the one where AB is the diameter, giving us:
This simplifies to:
Now, our family is defined by:
Sλ:(x2+y2−9x−12y+53)+λ(2x+3y−27)=0
This equation represents every possible circle passing through A and B.
The Radical Axis Revelation
Now, we introduce the fixed circle C0. When we intersect any circle from our family Sλ with C0, the common chord is found by simply subtracting their equations: Sλ−C0=0.
Watch the magic happen: the quadratic terms x2 and y2 cancel out perfectly! We are left with:
[(x2+y2−9x−12y+53)+λ(2x+3y−27)]−(x2+y2−4x−6y−3)=0
Grouping the terms, we get:
(−5x−6y+56)+λ(2x+3y−27)=0
The Final Concurrency
Look at the structure of this equation. It is in the form L1+λL2=0, where L1:5x+6y−56=0 and L2:2x+3y−27=0.
This is the classic equation of a family of lines passing through the intersection of L1 and L2. No matter what value λ takes, the common chord must pass through this intersection point.
Solving the system 5x+6y=56 and 2x+3y=27 (or 4x+6y=54), we subtract to find x=2. Substituting back, we find y=323.
We have proven that all these chords meet at the point (2,323). Geometry is not just about shapes; it is about the hidden order beneath the surface. You have just uncovered it.