The Geometry of Motion
Unveiling the Locus
Welcome, fellow traveler in the world of mathematics. Today, we are going to dissect a problem that, at first glance, might seem like a dry exercise in coordinate geometry.
But I want you to pause and look at the problem statement again. We have an ellipse, a circle, a vertical line, and a point R dancing between them.
This is not just algebra; this is the study of how shapes transform and relate to one another. Let us embark on this journey together.
Phase 1
The Auxiliary Circle and the Eccentric Angle
Every ellipse, defined by the equation
has a secret companion: the auxiliary circle, x2+y2=a2. Imagine the ellipse as a circle that has been squashed along the y-axis.
This relationship is the key to our entire solution. When we define point P on the ellipse, we could use standard Cartesian coordinates (x,y), but that would lead us into a labyrinth of square roots.
Instead, we use the eccentric angle θ. By setting P=(acosθ,bsinθ), we are essentially saying that P is a projection of a point on the auxiliary circle.
This is the first step in mastering JEE-level geometry: choosing the right coordinate system to make the math work for you, not against you.
Phase 2
The Vertical Constraint
Now, consider the line PQ. The problem tells us it is parallel to the y-axis. This is a gift!
A vertical line means that the x-coordinate is constant for every point on that line. If P has an x-coordinate of acosθ, then Q must also have an x-coordinate of acosθ.
Since Q lies on the auxiliary circle x2+y2=a2, we substitute our x-value: (acosθ)2+yQ2=a2. Solving for yQ, we find yQ=asinθ.
We now have the coordinates of both points: P=(acosθ,bsinθ) and Q=(acosθ,asinθ). Notice how the x-coordinates are identical, while the y-coordinates capture the difference between the ellipse and the circle.
Phase 3
The Section Formula
We introduce point R(h,k), which divides the segment PQ in the ratio r:s. This is where the physics of the problem meets the algebra.
The section formula is our bridge. For the x-coordinate h, we have
Look at that! Because the x-coordinates of P and Q are the same, the ratio doesn't even matter for the x-component. It simplifies beautifully to h=acosθ.
Now, for the y-coordinate k, we apply the formula with more care:
Here, the ratio matters deeply. We factor out the sinθ to get
This is the heart of the problem. We have successfully expressed the coordinates of R in terms of the parameter θ.
Phase 4
The Final Elimination
We are almost there. We have h=acosθ and k=r+s(ar+bs)sinθ. To find the locus, we need to eliminate θ.
We isolate the trigonometric functions: cosθ=ah and sinθ=ar+bsk(r+s). Now, we invoke the most powerful identity in trigonometry: cos2θ+sin2θ=1.
Substituting our expressions, we get:
Replacing h and k with the general variables x and y, we arrive at our final equation:
a2x2+(bs+ar)2y2(r+s)2=1
Conclusion
The Elegance of the Result
Look at the final equation. It is still an ellipse! The ratio r:s has effectively modified the semi-minor axis of the original ellipse.
This is the beauty of coordinate geometry: even as we move points and change ratios, the fundamental structure—the elliptical nature of the path—remains invariant.
You have successfully navigated the geometry, applied the section formula, and used trigonometric identities to reveal the hidden path. Take a moment to appreciate this. You didn't just solve for an equation; you uncovered a geometric truth. Keep this mindset, and no problem will ever be too daunting.