Analyzing the Setup
Welcome, fellow traveler on the path to JEE Advanced mastery. Today, we are not just solving a problem; we are uncovering the hidden symmetry between a simple algebraic relation and the power of calculus.
We are given the equation y2=P(x), where P(x) is a polynomial of degree 3. Our mission is to evaluate the expression 2dxd(y3y′′).
At first glance, this looks like a daunting task involving high-order derivatives. However, as we peel back the layers, you will see how the structure of the polynomial guides us to a surprisingly elegant solution.
The Foundation
We begin with our anchor: y2=P(x). In the world of JEE, whenever you see a function defined by a polynomial, you should immediately think about its derivatives.
If P(x) is a cubic, then P′(x) is a quadratic, P′′(x) is linear, and P′′′(x) is a constant. This is our geometric roadmap. We need to find y′′, so let us start by differentiating our anchor with respect to x.
Applying the chain rule, the derivative of y2 is 2yy′. Thus, we get:
This is our first key relation. It connects the velocity of our function y to the slope of the polynomial P(x).
The Second Derivative
To reach the second derivative y′′, we must differentiate again. We apply the product rule to the left side of our equation 2yy′=P′(x).
The derivative of 2yy′ is 2(y′)2+2yy′′. On the right side, the derivative of P′(x) is simply P′′(x). So, we arrive at:
Now, look closely at what we have. We have a term 2yy′′, but our target expression requires y3y′′.
We need to transform 2yy′′ into 4y3y′′. The most logical step is to multiply the entire equation by 2y2. This scales the 2yy′′ term perfectly to 4y3y′′ and allows us to substitute y2 with P(x) later.
The Algebraic Bridge
Multiplying our equation 2(y′)2+2yy′′=P′′(x) by 2y2, we get:
4y2(y′)2+4y3y′′=2y2P′′(x)
Now, let us perform the substitution. We know from our first step that 2yy′=P′(x), which implies 4y2(y′)2=(P′(x))2.
Substituting y2=P(x) and the squared derivative into our equation, we get:
(P′(x))2+4y3y′′=2P(x)P′′(x)
Rearranging to isolate our target term, 4y3y′′, we find:
4y3y′′=2P(x)P′′(x)−(P′(x))2
The Final Act
We are now at the threshold of the solution. We need to find 2dxd(y3y′′).
Let us differentiate our isolated expression with respect to x. The left side becomes dxd(4y3y′′), which is 4dxd(y3y′′).
On the right side, we apply the product rule to 2P(x)P′′(x) and the chain rule to (P′(x))2:
dxd[2P(x)P′′(x)−(P′(x))2]=[2P′(x)P′′(x)+2P(x)P′′′(x)]−2P′(x)P′′(x)
Look at the magic happening here! The terms 2P′(x)P′′(x) and −2P′(x)P′′(x) cancel out perfectly. We are left with:
4dxd(y3y′′)=2P(x)P′′′(x)
Dividing both sides by 2, we finally obtain the result:
Conclusion
And there it is. The complexity of the derivatives has vanished, leaving us with a clean, elegant relationship.
Because P(x) is a cubic polynomial, P′′′(x) is a constant, making the final expression a simple multiple of the original polynomial. This problem teaches us that in calculus, if you follow the logical steps and trust the algebraic structure, the most intimidating expressions often simplify into something beautiful.