The Geometric Dance of the Normal
Welcome, fellow traveler on the path to JEE mastery. Today, we are not just solving a problem; we are witnessing a beautiful, elegant dance between algebra and geometry.
We are looking at a parabola, that iconic curve defined by y2=4bx, and we are exploring the behavior of its normal lines. Imagine you are standing on this curve at a point P. You draw a tangent, and then, with a sharp turn, you draw a line perfectly perpendicular to it—the normal.
This line cuts through the interior of the parabola and, like a boomerang, strikes the curve again at a new point Q. Our mission is to find the secret relationship between the parameters of these two points, t1 and t2.
Phase 1
Defining the Players
Let us ground ourselves. We define our parabola as y2=4bx. Any point on this curve can be described by a single parameter t.
For our starting point P, we choose the parameter t1, giving us the coordinates (bt12,2bt1). This is our anchor.
Now, consider the normal line at P. The standard equation for a normal to this parabola at any parameter t is given by the elegant expression y=−tx+2bt+bt3. By substituting our specific parameter t1, the equation of our normal line becomes:
This line is our path. It starts at P and travels across the parabola to find its second home at Q.
Phase 2
The Intersection
Now, let us turn our attention to point Q. Since Q also lies on the parabola, it must have its own parameter, t2, and thus its coordinates are (bt22,2bt2).
The magic happens here: because the normal line passes through Q, the coordinates of Q must satisfy the equation of the normal. This is the moment where geometry yields to algebra. We substitute x=bt22 and y=2bt2 into our normal equation:
2bt2=−t1(bt22)+2bt1+bt13
Look at this equation. It looks a bit cluttered, but notice the constant b in every single term. Since b is the scale factor of our parabola and is non-zero, we can divide the entire equation by b. This simple act of cleaning up reveals the structure beneath:
Phase 3
The Algebraic Unveiling
We are close. Our goal is to find the relationship between t1 and t2. Let us group the terms to see if we can factorize. We move the linear terms to one side:
On the left, we factor out a 2, giving us 2(t2−t1). On the right, we factor out a −t1, which leaves us with (t22−t12). The equation now stands as:
2(t2−t1)=−t1(t22−t12)
Do you see it? The term (t22−t12) is a classic difference of squares, which expands to (t2−t1)(t2+t1). Substituting this back, we get:
2(t2−t1)=−t1(t2−t1)(t2+t1)
The Grand Finale
Here is the moment of truth. We have a common factor of (t2−t1) on both sides. Because P and Q are distinct points, $t_2
eq t_1$, meaning $(t_2 - t_1)
eq 0$.
We can safely divide both sides by this factor. The equation collapses into something remarkably simple:
Now, we just need to isolate t2. Dividing by −t1, we get t2+t1=−t12. Finally, subtracting t1 from both sides, we arrive at our destination:
This is the beautiful, universal condition for the normal at t1 to intersect the parabola again at t2. It is a result that appears simple, but it encapsulates the entire geometric journey we just took.
Remember this result, but more importantly, remember the process—the way we translated geometry into algebra and simplified it until the truth revealed itself. Keep practicing, keep questioning, and keep falling in love with the physics and math behind these problems.