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JEE Main 2024
Definite Integration
Definite Integration
Hard

Question

If f:RRf: \mathbb{R} \rightarrow \mathbb{R} be a continuous function satisfying \int_\limits{0}^{\frac{\pi}{2}} f(\sin 2 x) \sin x d x+\alpha \int_\limits{0}^{\frac{\pi}{4}} f(\cos 2 x) \cos x d x=0, then the value of α\alpha is :

Options

Solution

Key Concepts and Formulas

  • King's Property of Definite Integrals: For a continuous function f(x)f(x) on [a,b][a, b], abf(x)dx=abf(a+bx)dx\int_a^b f(x) \, dx = \int_a^b f(a+b-x) \, dx.
  • Trigonometric Identities:
    • sin(π2θ)=cosθ\sin(\frac{\pi}{2} - \theta) = \cos \theta
    • sin(π2+θ)=cosθ\sin(\frac{\pi}{2} + \theta) = \cos \theta
    • sin(AB)+sin(A+B)=2sinAcosB\sin(A-B) + \sin(A+B) = 2 \sin A \cos B
  • Integral Properties:
    • abf(x)dx+bcf(x)dx=acf(x)dx\int_a^b f(x) \, dx + \int_b^c f(x) \, dx = \int_a^c f(x) \, dx
    • Constants can be factored out of integrals.

Step-by-Step Solution

We are given the equation: 0π2f(sin2x)sinxdx+α0π4f(cos2x)cosxdx=0()\int\limits_0^{\frac{\pi}{2}} f(\sin 2 x) \sin x d x+\alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2 x) \cos x d x=0 \quad (*) Let I1=0π2f(sin2x)sinxdxI_1 = \int\limits_0^{\frac{\pi}{2}} f(\sin 2 x) \sin x d x and I2=0π4f(cos2x)cosxdxI_2 = \int\limits_0^{\frac{\pi}{4}} f(\cos 2 x) \cos x d x. The equation is I1+αI2=0I_1 + \alpha I_2 = 0.

Step 1: Splitting the first integral (I1I_1) To unify the limits of integration with I2I_2, we split I1I_1 at x=π4x = \frac{\pi}{4}. I1=0π4f(sin2x)sinxdx+π4π2f(sin2x)sinxdxI_1 = \int\limits_0^{\frac{\pi}{4}} f(\sin 2 x) \sin x d x + \int\limits_{\frac{\pi}{4}}^{\frac{\pi}{2}} f(\sin 2 x) \sin x d x Let I1a=0π4f(sin2x)sinxdxI_{1a} = \int\limits_0^{\frac{\pi}{4}} f(\sin 2 x) \sin x d x and I1b=π4π2f(sin2x)sinxdxI_{1b} = \int\limits_{\frac{\pi}{4}}^{\frac{\pi}{2}} f(\sin 2 x) \sin x d x. The equation becomes I1a+I1b+αI2=0I_{1a} + I_{1b} + \alpha I_2 = 0.

Step 2: Transforming I1aI_{1a} using King's Property We apply King's Property abg(x)dx=abg(a+bx)dx\int_a^b g(x) dx = \int_a^b g(a+b-x) dx to I1aI_{1a} with a=0a=0 and b=π4b=\frac{\pi}{4}. Replace xx with π4x\frac{\pi}{4}-x. I1a=0π4f(sin(2(π4x)))sin(π4x)dxI_{1a} = \int\limits_0^{\frac{\pi}{4}} f\left(\sin \left(2\left(\frac{\pi}{4}-x\right)\right)\right) \sin\left(\frac{\pi}{4}-x\right) d x Simplify the argument of ff: sin(2(π4x))=sin(π22x)=cos2x\sin\left(2\left(\frac{\pi}{4}-x\right)\right) = \sin\left(\frac{\pi}{2}-2x\right) = \cos 2x. Thus, I1a=0π4f(cos2x)sin(π4x)dxI_{1a} = \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \sin\left(\frac{\pi}{4}-x\right) d x

Step 3: Transforming I1bI_{1b} using substitution We want to change the limits of I1bI_{1b} from [π4,π2][\frac{\pi}{4}, \frac{\pi}{2}] to [0,π4][0, \frac{\pi}{4}]. Let x=π2ux = \frac{\pi}{2} - u. Then dx=dudx = -du. When x=π4x = \frac{\pi}{4}, u=π2π4=π4u = \frac{\pi}{2} - \frac{\pi}{4} = \frac{\pi}{4}. When x=π2x = \frac{\pi}{2}, u=π2π2=0u = \frac{\pi}{2} - \frac{\pi}{2} = 0. Substitute into I1bI_{1b}: I1b=π40f(sin(2(π2u)))sin(π2u)(du)I_{1b} = \int\limits_{\frac{\pi}{4}}^{0} f\left(\sin \left(2\left(\frac{\pi}{2}-u\right)\right)\right) \sin\left(\frac{\pi}{2}-u\right) (-du) Swap the limits and absorb the negative sign: I1b=0π4f(sin(π2u))sin(π2u)duI_{1b} = \int\limits_0^{\frac{\pi}{4}} f\left(\sin \left(\pi-2u\right)\right) \sin\left(\frac{\pi}{2}-u\right) du Simplify the trigonometric terms: sin(π2u)=sin(2u)\sin(\pi-2u) = \sin(2u) sin(π2u)=cosu\sin(\frac{\pi}{2}-u) = \cos u So, I1b=0π4f(sin2u)cosuduI_{1b} = \int\limits_0^{\frac{\pi}{4}} f(\sin 2u) \cos u \, du Replace the dummy variable uu with xx: I1b=0π4f(sin2x)cosxdxI_{1b} = \int\limits_0^{\frac{\pi}{4}} f(\sin 2x) \cos x \, dx

Step 4: Combining the transformed integrals Substitute the transformed I1aI_{1a} and I1bI_{1b} back into the original equation (from Step 1): 0π4f(cos2x)sin(π4x)dx+0π4f(sin2x)cosxdx+α0π4f(cos2x)cosxdx=0\int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \sin\left(\frac{\pi}{4}-x\right) d x + \int\limits_0^{\frac{\pi}{4}} f(\sin 2x) \cos x \, dx + \alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x d x = 0 This approach seems to have led to a complication as the argument of ff is different in the second integral. Let's re-evaluate the transformation of I1bI_{1b}.

Alternative Step 3: Transforming I1bI_{1b} using substitution (Revised) Let's use the substitution x=π4+tx = \frac{\pi}{4} + t for I1b=π4π2f(sin2x)sinxdxI_{1b} = \int\limits_{\frac{\pi}{4}}^{\frac{\pi}{2}} f(\sin 2x) \sin x \, dx. When x=π4x = \frac{\pi}{4}, t=0t = 0. When x=π2x = \frac{\pi}{2}, t=π4t = \frac{\pi}{4}. dx=dtdx = dt. sin(2x)=sin(2(π4+t))=sin(π2+2t)=cos2t\sin(2x) = \sin\left(2\left(\frac{\pi}{4}+t\right)\right) = \sin\left(\frac{\pi}{2}+2t\right) = \cos 2t sinx=sin(π4+t)\sin x = \sin\left(\frac{\pi}{4}+t\right) So, I1b=0π4f(cos2t)sin(π4+t)dtI_{1b} = \int\limits_0^{\frac{\pi}{4}} f(\cos 2t) \sin\left(\frac{\pi}{4}+t\right) dt Replacing tt with xx: I1b=0π4f(cos2x)sin(π4+x)dxI_{1b} = \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \sin\left(\frac{\pi}{4}+x\right) dx

Step 4: Combining the transformed integrals (Revised) Now substitute the transformed I1aI_{1a} and I1bI_{1b} back into the equation I1a+I1b+αI2=0I_{1a} + I_{1b} + \alpha I_2 = 0: 0π4f(cos2x)sin(π4x)dx+0π4f(cos2x)sin(π4+x)dx+α0π4f(cos2x)cosxdx=0\int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \sin\left(\frac{\pi}{4}-x\right) d x + \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \sin\left(\frac{\pi}{4}+x\right) d x + \alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x d x = 0 Combine the first two integrals as they have the same integrand argument for ff and the same limits: 0π4f(cos2x)[sin(π4x)+sin(π4+x)]dx+α0π4f(cos2x)cosxdx=0\int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \left[ \sin\left(\frac{\pi}{4}-x\right) + \sin\left(\frac{\pi}{4}+x\right) \right] dx + \alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x d x = 0 Use the sum-to-product identity sin(AB)+sin(A+B)=2sinAcosB\sin(A-B) + \sin(A+B) = 2 \sin A \cos B with A=π4A=\frac{\pi}{4} and B=xB=x: sin(π4x)+sin(π4+x)=2sin(π4)cosx=212cosx=2cosx\sin\left(\frac{\pi}{4}-x\right) + \sin\left(\frac{\pi}{4}+x\right) = 2 \sin\left(\frac{\pi}{4}\right) \cos x = 2 \cdot \frac{1}{\sqrt{2}} \cos x = \sqrt{2} \cos x Substitute this back into the equation: 0π4f(cos2x)[2cosx]dx+α0π4f(cos2x)cosxdx=0\int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \left[ \sqrt{2} \cos x \right] dx + \alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x d x = 0 This can be written as: 20π4f(cos2x)cosxdx+α0π4f(cos2x)cosxdx=0\sqrt{2} \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x \, dx + \alpha \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x \, dx = 0 Factor out the common integral: (2+α)0π4f(cos2x)cosxdx=0(\sqrt{2} + \alpha) \int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x \, dx = 0

Step 5: Determining the value of α\alpha For this equation to hold true for any continuous function ff, the coefficient of the integral must be zero, because the integral itself is not necessarily zero. For example, if f(u)=1f(u)=1, then 0π4cosxdx=[sinx]0π4=120\int_0^{\frac{\pi}{4}} \cos x \, dx = [\sin x]_0^{\frac{\pi}{4}} = \frac{1}{\sqrt{2}} \neq 0. Therefore, we must have: 2+α=0\sqrt{2} + \alpha = 0 Solving for α\alpha: α=2\alpha = -\sqrt{2}


Common Mistakes & Tips

  • Incorrect Substitution: Ensure that when performing substitutions, the limits of integration are correctly transformed and that all occurrences of the original variable are replaced.
  • Algebraic Errors in Trigonometric Simplification: Carefully apply trigonometric identities to avoid mistakes in simplifying expressions like sin(π4x)+sin(π4+x)\sin(\frac{\pi}{4}-x) + \sin(\frac{\pi}{4}+x).
  • Assuming the Integral is Zero: Do not assume that 0π4f(cos2x)cosxdx=0\int\limits_0^{\frac{\pi}{4}} f(\cos 2x) \cos x \, dx = 0. This integral depends on the function ff and is not generally zero for all continuous functions. The equation must hold for arbitrary ff.

Summary The problem was solved by strategically splitting the first integral and applying the King's Property and a suitable substitution to transform its parts. This allowed all terms in the equation to be expressed with the same integration limits and the same functional argument (f(cos2x)f(\cos 2x)). After combining these transformed integrals and using a trigonometric sum-to-product identity, the equation simplified to a form where a common integral term could be factored out. For the equation to be true for an arbitrary continuous function ff, the remaining coefficient must be zero, leading to the value of α\alpha.

The final answer is 2\boxed{-\sqrt{2}}, which corresponds to option (C).

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