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JEE Main 2023
Definite Integration
Definite Integration
Hard

Question

The value of 0πecosxsinx(1+cos2x)(ecosx+ecosx)dx\int\limits_0^\pi {{{{e^{\cos x}}\sin x} \over {(1 + {{\cos }^2}x)({e^{\cos x}} + {e^{ - \cos x}})}}dx} is equal to:

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Solution

Key Concepts and Formulas

  • Substitution Method for Definite Integrals: This technique is used to simplify integrals by changing the variable of integration. It is essential to update the limits of integration according to the substitution.
  • Properties of Definite Integrals: Specifically, the property abf(x)dx=baf(x)dx\int_a^b f(x) dx = -\int_b^a f(x) dx is used to reverse the limits of integration, and the property aaf(x)dx=aaf(x)dx\int_{-a}^a f(x) dx = \int_{-a}^a f(-x) dx is useful for integrals with symmetric limits.
  • Algebraic Simplification: Basic algebraic manipulation of exponents and fractions is required.

Step-by-Step Solution

Step 1: Analyze the Integral and Apply Substitution

The given integral is: I=0πecosxsinx(1+cos2x)(ecosx+ecosx)dxI = \int\limits_0^\pi {{{{e^{\cos x}}\sin x} \over {(1 + {{\cos }^2}x)({e^{\cos x}} + {e^{ - \cos x}})}}dx} We observe that the numerator contains sinxdx\sin x \, dx, and the terms in the integrand are functions of cosx\cos x. This suggests using the substitution t=cosxt = \cos x.

Let t=cosxt = \cos x. Differentiating both sides with respect to xx, we get dtdx=sinx\frac{dt}{dx} = -\sin x, which implies dt=sinxdxdt = -\sin x \, dx, or sinxdx=dt\sin x \, dx = -dt.

Now, we must change the limits of integration: When x=0x = 0, t=cos(0)=1t = \cos(0) = 1. When x=πx = \pi, t=cos(π)=1t = \cos(\pi) = -1.

Substituting these into the integral, we get: I=11et(dt)(1+t2)(et+et)I = \int\limits_1^{-1} {{{{e^t}(-dt)} \over {(1 + {t^2})({e^t} + {e^{ - t}})}}} I=11et(1+t2)(et+et)dtI = - \int\limits_1^{-1} {{{{e^t}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}}dt} Using the property abf(x)dx=baf(x)dx\int_a^b f(x) dx = -\int_b^a f(x) dx, we can swap the limits of integration and remove the negative sign: I=11et(1+t2)(et+et)dt... (Equation 1)I = \int\limits_{-1}^1 {{{{e^t}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}}dt} \quad \text{... (Equation 1)}

Step 2: Apply the Property of Definite Integrals for Symmetric Limits

The integral in Equation 1 has symmetric limits from 1-1 to 11. We can use the property aaf(t)dt=aaf(t)dt\int_{-a}^a f(t) \, dt = \int_{-a}^a f(-t) \, dt. Let f(t)=et(1+t2)(et+et)f(t) = {{{e^t}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}}. Then, f(t)=et(1+(t)2)(et+e(t))=et(1+t2)(et+et)f(-t) = {{{e^{-t}}} \over {(1 + {(-t)^2})({e^{-t}} + {e^{ - (-t)}})}} = {{{e^{-t}}} \over {(1 + {t^2})({e^{-t}} + {e^t})}}.

Therefore, we can also write the integral II as: I=11et(1+t2)(et+et)dt... (Equation 2)I = \int\limits_{-1}^1 {{{{e^{-t}}} \over {(1 + {t^2})({e^{-t}} + {e^t})}}dt} \quad \text{... (Equation 2)}

Step 3: Combine the Two Forms of the Integral

Now, we add Equation 1 and Equation 2: I+I=11et(1+t2)(et+et)dt+11et(1+t2)(et+et)dtI + I = \int\limits_{-1}^1 {{{{e^t}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}}dt} + \int\limits_{-1}^1 {{{{e^{-t}}} \over {(1 + {t^2})({e^{-t}} + {e^t})}}dt} 2I=11(et(1+t2)(et+et)+et(1+t2)(et+et))dt2I = \int\limits_{-1}^1 {\left( {{{e^t}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}} + {{{e^{-t}}} \over {(1 + {t^2})({e^{-t}} + {e^t})}} \right)} dt Since the denominators are the same, we can combine the numerators: 2I=11et+et(1+t2)(et+et)dt2I = \int\limits_{-1}^1 {{{{e^t} + {e^{-t}}} \over {(1 + {t^2})({e^t} + {e^{ - t}})}} dt} Notice that the term (et+et)(e^t + e^{-t}) appears in both the numerator and the denominator. We can cancel this term, provided et+et0e^t + e^{-t} \neq 0, which is always true for real tt. 2I=111(1+t2)dt2I = \int\limits_{-1}^1 {{{{1}} \over {(1 + {t^2})}} dt}

Step 4: Evaluate the Simplified Integral

The integral is now a standard form: 2I=1111+t2dt2I = \int\limits_{-1}^1 \frac{1}{1+t^2} dt The antiderivative of 11+t2\frac{1}{1+t^2} is tan1(t)\tan^{-1}(t). 2I=[tan1(t)]112I = \left[ \tan^{-1}(t) \right]_{-1}^1 Now, we evaluate the definite integral using the limits: 2I=tan1(1)tan1(1)2I = \tan^{-1}(1) - \tan^{-1}(-1) We know that tan1(1)=π4\tan^{-1}(1) = \frac{\pi}{4} and tan1(1)=π4\tan^{-1}(-1) = -\frac{\pi}{4}. 2I=π4(π4)2I = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) 2I=π4+π42I = \frac{\pi}{4} + \frac{\pi}{4} 2I=2π42I = \frac{2\pi}{4} 2I=π22I = \frac{\pi}{2}

Step 5: Solve for I

Finally, we solve for II by dividing by 2: I=12×π2I = \frac{1}{2} \times \frac{\pi}{2} I=π4I = \frac{\pi}{4}

Common Mistakes & Tips

  • Forgetting to change limits: When using substitution in definite integrals, always update the limits of integration to correspond to the new variable.
  • Sign errors with substitution: The derivative of cosx\cos x is sinx-\sin x, so remember to include the negative sign when performing the substitution dt=sinxdxdt = -\sin x \, dx.
  • Misapplying the symmetric limit property: Ensure the integrand is indeed an even function of the variable tt when using aaf(t)dt=aaf(t)dt\int_{-a}^a f(t) dt = \int_{-a}^a f(-t) dt or an odd function for aaf(t)dt=0\int_{-a}^a f(t) dt = 0. In this case, we used the property to get an alternative form of the integral and then added them.

Summary

The problem is solved by first applying a trigonometric substitution to simplify the integrand and transform the limits of integration. The resulting integral has symmetric limits, allowing us to use a property of definite integrals to obtain a second form of the integral. By adding the original and transformed integrals, the expression simplifies significantly. The final step involves evaluating a standard integral of 11+t2\frac{1}{1+t^2} and solving for the value of the original integral.

The final answer is π4\boxed{{\frac{\pi}{4}}}.

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