Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a problem; we are witnessing a beautiful, silent dance between two mathematical curves. Imagine two paths crossing each other in the coordinate plane.
Usually, they might cross at any arbitrary angle, but today, we are dealing with a special case: orthogonality. When two curves intersect at 90∘, they are locked in a perfect perpendicular embrace.
Our mission is to uncover the hidden relationship between the constants a,b,c, and d that govern these curves. Let us begin by looking at our two protagonists:
ax2+by2=1andcx2+dy2=1
Phase 1
The Calculus of Slopes
To understand how these curves behave at their intersection point P(x,y), we need to know their direction. In calculus, direction is synonymous with the slope of the tangent.
Let us take the first curve, ax2+by2=1, and differentiate it with respect to x. Applying the power rule and the chain rule, we get:
With a quick algebraic shuffle, we isolate the slope m1:
Now, we repeat this elegant process for the second curve, cx2+dy2=1. The derivative yields c2x+d2ydxdy=0, which gives us our second slope:
Phase 2
The Orthogonality Condition
Now, we invoke the condition of orthogonality. If these curves meet at 90∘, their tangents must be perpendicular. The condition for perpendicularity is simple yet profound: m1⋅m2=−1.
Let us substitute our expressions:
The negative signs vanish, leaving us with acy2bdx2=−1. By cross-multiplying, we arrive at a vital intermediate relation:
Phase 3
The Algebraic Alchemy
We have the slopes and the condition, but we still have x and y cluttering our equation. We need to eliminate them by using the original equations themselves.
Subtracting the second equation from the first, the constants on the right side cancel out:
(ax2+by2)−(cx2+dy2)=1−1=0
This leaves us with:
x2(a1−c1)+y2(b1−d1)=0
Simplifying the fractions, we obtain:
The Grand Finale
Now, we substitute our orthogonality condition acx2=−bdy2 into the equation above. The expression becomes:
(−bdy2)(c−a)+y2(bdd−b)=0
Since y is not zero at the intersection, we can divide the entire equation by bdy2. We are left with:
Expanding this, we get −c+a+d−b=0. Rearranging the terms, we arrive at the final, elegant result:
You have just navigated the intersection of geometry and algebra. This is the essence of JEE Advanced—not just calculating, but seeing the structure beneath the surface.