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JEE Main 2023
Definite Integration
Definite Integration
Hard

Question

The value of α\alpha for which 4α12eαxdx=54\alpha \int\limits_{ - 1}^2 {{e^{ - \alpha \left| x \right|}}dx} = 5, is:

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Solution

Key Concepts and Formulas

  • Absolute Value Function: The definition of x|x| is crucial: x=x|x| = -x for x<0x < 0 and x=x|x| = x for x0x \ge 0. When integrating a function involving x|x| over an interval containing 00, the integral must be split at x=0x=0.
  • Integration of Exponential Functions: The general formula for integrating an exponential function is eaxdx=eaxa+C\int e^{ax} dx = \frac{e^{ax}}{a} + C.
  • Definite Integral Evaluation: The value of a definite integral abf(x)dx\int_a^b f(x) dx is found by evaluating the antiderivative F(x)F(x) at the upper and lower limits: F(b)F(a)F(b) - F(a).
  • Logarithm Properties: Key properties include ln(ek)=k\ln(e^k) = k and ln(a/b)=lnalnb\ln(a/b) = \ln a - \ln b, which can be used to simplify logarithmic expressions. Also, ex>0e^x > 0 for all real xx.

Step-by-Step Solution

We are asked to find the value of α\alpha for which 4α12eαxdx=54\alpha \int\limits_{ - 1}^2 {{e^{ - \alpha \left| x \right|}}dx} = 5.

Step 1: Handling the Absolute Value in the Integral The integrand contains x|x|. Since the interval of integration is [1,2][-1, 2], which includes 00, we must split the integral at x=0x=0. For x[1,0)x \in [-1, 0), x=x|x| = -x. So, eαx=eα(x)=eαxe^{-\alpha|x|} = e^{-\alpha(-x)} = e^{\alpha x}. For x[0,2]x \in [0, 2], x=x|x| = x. So, eαx=eαxe^{-\alpha|x|} = e^{-\alpha x}. Therefore, the integral can be rewritten as: 12eαxdx=10eαxdx+02eαxdx\int\limits_{ - 1}^2 {{e^{ - \alpha \left| x \right|}}dx} = \int\limits_{ - 1}^0 {{e^{\alpha x}}dx} + \int\limits_0^2 {{e^{ - \alpha x}}dx} The given equation becomes: 4α(10eαxdx+02eαxdx)=54\alpha \left( \int\limits_{ - 1}^0 {{e^{\alpha x}}dx} + \int\limits_0^2 {{e^{ - \alpha x}}dx} \right) = 5

Step 2: Evaluating the Integrals We apply the integration formula eaxdx=eaxa\int e^{ax} dx = \frac{e^{ax}}{a}.

For the first integral, 10eαxdx\int\limits_{ - 1}^0 {{e^{\alpha x}}dx}: [eαxα]10=eα(0)αeα(1)α=1αeαα=1eαα\left[ \frac{e^{\alpha x}}{\alpha} \right]_{ - 1}^0 = \frac{e^{\alpha(0)}}{\alpha} - \frac{e^{\alpha(-1)}}{\alpha} = \frac{1}{\alpha} - \frac{e^{-\alpha}}{\alpha} = \frac{1 - e^{-\alpha}}{\alpha}

For the second integral, 02eαxdx\int\limits_0^2 {{e^{ - \alpha x}}dx}: [eαxα]02=eα(2)αeα(0)α=e2αα1α=1e2αα\left[ \frac{e^{-\alpha x}}{-\alpha} \right]_0^2 = \frac{e^{-\alpha(2)}}{-\alpha} - \frac{e^{-\alpha(0)}}{-\alpha} = \frac{e^{-2\alpha}}{-\alpha} - \frac{1}{-\alpha} = \frac{1 - e^{-2\alpha}}{\alpha}

Substitute these results back into the main equation: 4α(1eαα+1e2αα)=54\alpha \left( \frac{1 - e^{-\alpha}}{\alpha} + \frac{1 - e^{-2\alpha}}{\alpha} \right) = 5 We can factor out 1α\frac{1}{\alpha} from the terms inside the parenthesis: 4α1α((1eα)+(1e2α))=54\alpha \cdot \frac{1}{\alpha} \left( (1 - e^{-\alpha}) + (1 - e^{-2\alpha}) \right) = 5 The α\alpha terms cancel out: 4(1eα+1e2α)=54 \left( 1 - e^{-\alpha} + 1 - e^{-2\alpha} \right) = 5

Step 3: Simplifying and Forming a Quadratic Equation Simplify the expression inside the parenthesis: 4(2eαe2α)=54 \left( 2 - e^{-\alpha} - e^{-2\alpha} \right) = 5 Distribute the 44: 84eα4e2α=58 - 4e^{-\alpha} - 4e^{-2\alpha} = 5 Rearrange the terms to form a quadratic equation in terms of eαe^{-\alpha}: 4e2α+4eα3=04e^{-2\alpha} + 4e^{-\alpha} - 3 = 0

Step 4: Solving the Quadratic Equation Let t=eαt = e^{-\alpha}. Then e2α=(eα)2=t2e^{-2\alpha} = (e^{-\alpha})^2 = t^2. Substituting this into the equation gives: 4t2+4t3=04t^2 + 4t - 3 = 0 We can solve this quadratic equation by factoring. We look for two numbers that multiply to 4×(3)=124 \times (-3) = -12 and add to 44. These numbers are 66 and 2-2. 4t2+6t2t3=04t^2 + 6t - 2t - 3 = 0 Factor by grouping: 2t(2t+3)1(2t+3)=02t(2t + 3) - 1(2t + 3) = 0 (2t1)(2t+3)=0(2t - 1)(2t + 3) = 0 This yields two possible solutions for tt: 2t1=0t=122t - 1 = 0 \Rightarrow t = \frac{1}{2} 2t+3=0t=322t + 3 = 0 \Rightarrow t = -\frac{3}{2}

Step 5: Determining the Valid Solution for α\alpha Recall that we defined t=eαt = e^{-\alpha}. Since the exponential function exe^x is always positive for any real number xx, tt must be positive. Therefore, t=32t = -\frac{3}{2} is an extraneous solution and must be rejected. The valid solution is t=12t = \frac{1}{2}. Substitute back t=eαt = e^{-\alpha}: eα=12e^{-\alpha} = \frac{1}{2} To solve for α\alpha, take the natural logarithm of both sides: ln(eα)=ln(12)\ln(e^{-\alpha}) = \ln\left(\frac{1}{2}\right) Using the property ln(ek)=k\ln(e^k) = k: α=ln(12)-\alpha = \ln\left(\frac{1}{2}\right) Using the property ln(1/b)=lnb\ln(1/b) = -\ln b: α=ln(2)-\alpha = -\ln(2) Multiply by 1-1: α=ln(2)\alpha = \ln(2) This can also be written as α=loge2\alpha = \log_e 2.

Common Mistakes & Tips

  • Absolute Value Splitting: Failing to split the integral at x=0x=0 when x|x| is involved is a common oversight.
  • Sign Errors: Be extremely careful with negative signs during integration and when evaluating definite integrals, especially with terms like eαxe^{-\alpha x}.
  • Extraneous Solutions: Always check the validity of solutions obtained from algebraic equations, particularly when dealing with exponential functions where the base is positive.

Summary

The problem requires careful handling of an integral involving an absolute value function. By splitting the integral at x=0x=0, integrating the exponential terms, and simplifying the resulting equation, we obtained a quadratic equation in terms of eαe^{-\alpha}. Solving this quadratic equation and considering the domain of the exponential function allowed us to find the unique valid value for α\alpha.

The final answer is loge2\boxed{\log_e 2}.

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