Analyzing the Setup
Imagine a rod of fixed length l leaning against a wall. Let the floor be the x-axis and the wall be the y-axis, with the endpoints of the rod at A(a,0) and B(0,b).
As the rod slides, the values of a and b change, but the length of the rod remains constant. This provides our fundamental constraint based on the Pythagorean theorem:
This equation serves as the heartbeat of our problem, defining the boundary conditions for the motion of the rod.
The Bridge
The Section Formula
We are interested in the path traced by a point P(x,y) that divides the rod AB in the ratio 1:2. We must express the coordinates of P in terms of the variable intercepts a and b.
Using the section formula for internal division with a ratio of m:n=1:2, we calculate the x-coordinate:
Similarly, we calculate the y-coordinate:
These equations act as our bridge, connecting the position of point P to the parameters a and b.
The Elimination
Unveiling the Locus
To find the locus of point P, we must eliminate the parameters a and b using our bridge equations and the constraint equation. From the bridge equations, we isolate a and b:
Substituting these expressions into the constraint equation a2+b2=l2, we obtain:
Expanding these terms, we arrive at:
The Final Reveal
To express the path in a more elegant standard form, we multiply the entire equation by 4:
Dividing by 4l2, we can see the standard form of an ellipse:
We have successfully translated a dynamic physical motion into a static geometric shape. The path traced by point P is an ellipse.