Analyzing the Setup
Imagine you are standing on a Cartesian plane with a fixed anchor point at (2,3). A line is pinned to this point, but it is free to rotate like a propeller.
As it rotates, it carves out different intercepts on the x and y axes, which we call P and Q. The rectangle OPRQ forms as the line pivots, and our goal is to find the equation of the path traced by the corner R.
The Power of Intercepts
To solve this, we use the intercept form of a line. Since the line cuts the axes at P(h,0) and Q(0,k), the equation of the line is:
This equation is the heartbeat of our solution. Because the line is forced to pass through our fixed anchor (2,3), these coordinates must satisfy the equation.
Substituting x=2 and y=3, we obtain the constraint:
This equation represents the mathematical "DNA" of our line.
The Birth of the Locus
Now, consider the rectangle OPRQ. With O at (0,0), P at (h,0), and Q at (0,k), the vertex R must be at (h,k).
This is the point whose path we are tracking. To find the locus, we transition from the specific variables h and k to the general coordinates (x,y) of any point on the path.
Substituting h=x and k=y into our constraint, we get:
The Final Elegance
To express this in a standard form, we multiply the entire expression by xy to clear the denominators:
This simplifies beautifully to:
Rearranging the terms, we arrive at the final equation of the locus:
If you were to graph this, you would see a hyperbola. It is fascinating to observe that a simple, rotating straight line, constrained by a single point, creates such an elegant curve. You have successfully mapped the motion of R.