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JEE Main 2021
Definite Integration
Definite Integration
Hard

Question

Let ff be a continuous function satisfying \int_\limits{0}^{t^{2}}\left(f(x)+x^{2}\right) d x=\frac{4}{3} t^{3}, \forall t > 0. Then f(π24)f\left(\frac{\pi^{2}}{4}\right) is equal to :

Options

Solution

Key Concepts and Formulas

  • Leibniz Integral Rule: If G(t)=a(t)b(t)g(x)dxG(t) = \int_{a(t)}^{b(t)} g(x) \, dx, then G(t)=g(b(t))b(t)g(a(t))a(t)G'(t) = g(b(t)) \cdot b'(t) - g(a(t)) \cdot a'(t), provided g(x)g(x) is continuous and a(t),b(t)a(t), b(t) are differentiable.
  • Differentiation of Powers: ddt(tn)=ntn1\frac{d}{dt}(t^n) = nt^{n-1}.
  • Substitution: If y=x2y = x^2, then x=yx = \sqrt{y} for x>0x>0.

Step-by-Step Solution

Step 1: Apply the Leibniz Integral Rule to Differentiate the Given Equation

We are given the equation: 0t2(f(x)+x2)dx=43t3,t>0\int\limits_0^{t^{2}}\left(f(x)+x^{2}\right) d x=\frac{4}{3} t^{3}, \quad \forall t > 0 The purpose of this step is to eliminate the integral and obtain an equation involving f(t2)f(t^2) and tt. We will differentiate both sides of the equation with respect to tt.

The left-hand side (LHS) is an integral of the form a(t)b(t)g(x)dx\int_{a(t)}^{b(t)} g(x) \, dx, where:

  • g(x)=f(x)+x2g(x) = f(x) + x^2
  • b(t)=t2b(t) = t^2 (upper limit)
  • a(t)=0a(t) = 0 (lower limit)

Using the Leibniz Integral Rule, the derivative of the LHS with respect to tt is: ddt[0t2(f(x)+x2)dx]=g(b(t))b(t)g(a(t))a(t)\frac{d}{dt} \left[ \int\limits_0^{t^{2}}\left(f(x)+x^{2}\right) d x \right] = g(b(t)) \cdot b'(t) - g(a(t)) \cdot a'(t) First, find the derivatives of the limits:

  • b(t)=ddt(t2)=2tb'(t) = \frac{d}{dt}(t^2) = 2t
  • a(t)=ddt(0)=0a'(t) = \frac{d}{dt}(0) = 0

Next, substitute the limits into the integrand g(x)=f(x)+x2g(x) = f(x) + x^2:

  • g(b(t))=g(t2)=f(t2)+(t2)2=f(t2)+t4g(b(t)) = g(t^2) = f(t^2) + (t^2)^2 = f(t^2) + t^4
  • g(a(t))=g(0)=f(0)+(0)2=f(0)g(a(t)) = g(0) = f(0) + (0)^2 = f(0)

Now, apply the Leibniz Rule formula: ddt[LHS]=(f(t2)+t4)(2t)(f(0))(0)=2t(f(t2)+t4)\frac{d}{dt} \left[ \text{LHS} \right] = (f(t^2) + t^4) \cdot (2t) - (f(0)) \cdot (0) = 2t(f(t^2) + t^4) The right-hand side (RHS) is 43t3\frac{4}{3} t^3. Its derivative with respect to tt is: ddt(43t3)=433t2=4t2\frac{d}{dt} \left( \frac{4}{3} t^3 \right) = \frac{4}{3} \cdot 3t^2 = 4t^2 Equating the derivatives of the LHS and RHS: 2t(f(t2)+t4)=4t22t(f(t^2) + t^4) = 4t^2

Step 2: Solve for f(t2)f(t^2)

We have the equation: 2t(f(t2)+t4)=4t22t(f(t^2) + t^4) = 4t^2 Since the problem states t>0t > 0, we can divide both sides by 2t2t: f(t2)+t4=4t22tf(t^2) + t^4 = \frac{4t^2}{2t} f(t2)+t4=2tf(t^2) + t^4 = 2t Now, isolate f(t2)f(t^2): f(t2)=2tt4f(t^2) = 2t - t^4 This equation expresses the value of the function ff when its argument is t2t^2.

Step 3: Evaluate f(π24)f\left(\frac{\pi^{2}}{4}\right)

We need to find the value of ff at the specific point π24\frac{\pi^2}{4}. From the equation f(t2)=2tt4f(t^2) = 2t - t^4, we need to find the value of tt such that t2=π24t^2 = \frac{\pi^2}{4}. t2=π24t^2 = \frac{\pi^2}{4} Since t>0t > 0, we take the positive square root: t=π24=π2t = \sqrt{\frac{\pi^2}{4}} = \frac{\pi}{2} Now, substitute t=π2t = \frac{\pi}{2} into the expression for f(t2)f(t^2): f((π2)2)=2(π2)(π2)4f\left(\left(\frac{\pi}{2}\right)^2\right) = 2\left(\frac{\pi}{2}\right) - \left(\frac{\pi}{2}\right)^4 f(π24)=ππ416f\left(\frac{\pi^2}{4}\right) = \pi - \frac{\pi^4}{16} To match the format of the options, we can factor out π\pi: f(π24)=π(1π316)f\left(\frac{\pi^2}{4}\right) = \pi \left(1 - \frac{\pi^3}{16}\right)

Common Mistakes & Tips

  • Chain Rule Application: Ensure the derivative of the upper limit (2t2t) is correctly multiplied with the integrand evaluated at the upper limit. Forgetting this is a common error.
  • Substitution Errors: When solving for tt, remember that t>0t>0 is given, so only the positive root is considered.
  • Algebraic Manipulation: Pay close attention to signs and exponents when simplifying the equation after differentiation.

Summary

The problem was solved by applying the Leibniz Integral Rule to differentiate the given integral equation, which allowed us to obtain an explicit expression for f(t2)f(t^2). By setting t2t^2 equal to the desired argument π24\frac{\pi^2}{4}, we found the corresponding value of tt and substituted it into the derived expression for f(t2)f(t^2) to find f(π24)f\left(\frac{\pi^{2}}{4}\right).

The final answer is π(1π316)\boxed{\pi\left(1-\frac{\pi^{3}}{16}\right)}, which corresponds to option (B).

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