Analyzing the Setup
Welcome, fellow traveler on the path to JEE mastery. Today, we stand before a problem that might look like a tangled web of exponentials, trigonometric functions, and integrals.
We are given the equation:
f(x)+∫0x(x−t)f′(t)dt=(e2x+e−2x)cos2x+a2x
In the world of JEE Advanced, complexity is often just a mask for elegance. Our mission is to strip away that mask and find the constant a.
The Surgical Precision of Leibniz
The core challenge here is the integral term ∫0x(x−t)f′(t)dt. We have the variable x trapped both in the limit and inside the integrand.
To break this open, we reach for the
Leibniz Rule for differentiation under the integral sign. The formula is:
dxd∫u(x)v(x)g(x,t)dt=∫u(x)v(x)∂x∂g(x,t)dt+g(x,v(x))dxdv−g(x,u(x))dxdu
Taming the Left-Hand Side
Let us apply this to our left-hand side (LHS). We differentiate f(x)+∫0x(x−t)f′(t)dt with respect to x.
The derivative of f(x) is f′(x). Applying Leibniz to the integral, the partial derivative of (x−t)f′(t) with respect to x is f′(t). The upper limit term becomes (x−x)f′(x)=0, and the lower limit term is 0.
Thus, the derivative of the integral simplifies to
∫0xf′(t)dt. By the Fundamental Theorem of Calculus, this is
f(x)−f(0). Our LHS derivative is:
f′(x)+f(x)−f(0)
The Right-Hand Side and the Substitution
Now, we differentiate the right-hand side (RHS):
(e2x+e−2x)cos2x+a2x. Using the product and chain rules, we obtain:
dxdRHS=2(e2x−e−2x)cos2x−2(e2x+e−2x)sin2x+a2
Equating the two sides, we have:
f′(x)+f(x)−f(0)=2(e2x−e−2x)cos2x−2(e2x+e−2x)sin2x+a2
The Final Revelation
We are given
f′(0)=4. If we substitute
x=0 into our differentiated equation, the terms
f(x) and
f(0) cancel out, leaving:
f′(0)=a2
Since f′(0)=4, we find 4=a2, which implies a=21.
Finally, we calculate
(2a+1)5a2:
(2(21)+1)5(21)2=(1+1)5(41)=32⋅41=8
We have arrived at the answer: 8.