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Definite Integration question

2014 · Shift 2 · Q36
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Definite Integration question

2014 · Shift 2 · Q36

JEE AdvancedMathematicsDefinite IntegrationMCQ+3 / −1
The following integral ∫π4π2(2csc⁡  x)17dx\int\limits_{{\pi \over 4}}^{{\pi \over 2}} {{{\left( {2\csc\,\,x} \right)}^{17}}dx}4π​∫2π​​(2cscx)17dx is equal to
  1. A
    ∫0log⁡(1+2)2(eu+e−u)16 du\int\limits_0^{\log \left( {1 + \sqrt 2 } \right)} {2{{\left( {{e^u} + {e^{ - u}}} \right)}^{16}}\,du}0∫log(1+2​)​2(eu+e−u)16du
  2. B
    ∫0log⁡(1+2)(eu+e−u)17 du\int\limits_0^{\log \left( {1 + \sqrt 2 } \right)} {{{\left( {{e^u} + {e^{ - u}}} \right)}^{17}}\,du}0∫log(1+2​)​(eu+e−u)17du
  3. C
    ∫0log⁡(1+2)(eu−e−u)17 du\int\limits_0^{\log \left( {1 + \sqrt 2 } \right)} {{{\left( {{e^u} - {e^{ - u}}} \right)}^{17}}\,du}0∫log(1+2​)​(eu−e−u)17du
  4. D
    ∫0log⁡(1+2)2(eu−e−u)16 du\int\limits_0^{\log \left( {1 + \sqrt 2 } \right)} {2{{\left( {{e^u} - {e^{ - u}}} \right)}^{16}}\,du}0∫log(1+2​)​2(eu−e−u)16du
View written solutionFree

Correct answer: A

The user wants me to solve the definite integral: I=∫π/4π/2(2csc⁡ x)17dxI = \int\limits_{{\pi / 4}}^{{\pi / 2}} {{{\left( {2\csc\,x} \right)}^{17}}dx}I=π/4∫π/2​(2cscx)17dx and match it with one of the given options. The options are integrals in terms of a variable u with exponential functions, which suggests that a substitution is required to transform the trigonometric integral into one with exponential functions.

Step-by-step solution:

  1. Choosing the substitution: The options have limits of integration from 000 to log⁡(1+2)\log(1+\sqrt{2})log(1+2​) and involve terms like eu+e−ue^u + e^{-u}eu+e−u. This hints at a standard substitution used for integrals involving csc⁡x\csc xcscx. Let's try the substitution: u=log⁡(csc⁡x+cot⁡x)u = \log(\csc x + \cot x)u=log(cscx+cotx)

  2. Changing the limits of integration: We need to find the new limits for the variable uuu corresponding to the original limits for xxx.

    • Lower limit: When x=π/4x = \pi/4x=π/4, u=log⁡(csc⁡(π/4)+cot⁡(π/4))=log⁡(2+1)u = \log(\csc(\pi/4) + \cot(\pi/4)) = \log(\sqrt{2} + 1)u=log(csc(π/4)+cot(π/4))=log(2​+1)
    • Upper limit: When x=π/2x = \pi/2x=π/2, u=log⁡(csc⁡(π/2)+cot⁡(π/2))=log⁡(1+0)=log⁡(1)=0u = \log(\csc(\pi/2) + \cot(\pi/2)) = \log(1 + 0) = \log(1) = 0u=log(csc(π/2)+cot(π/2))=log(1+0)=log(1)=0 So, the integration will be from log⁡(1+2)\log(1+\sqrt{2})log(1+2​) to 000.
  3. Expressing the integrand in terms of u: From our substitution, we have eu=csc⁡x+cot⁡xe^u = \csc x + \cot xeu=cscx+cotx. Then, e−u=1csc⁡x+cot⁡xe^{-u} = \frac{1}{\csc x + \cot x}e−u=cscx+cotx1​. Rationalizing the denominator gives: e−u=1csc⁡x+cot⁡x×csc⁡x−cot⁡xcsc⁡x−cot⁡x=csc⁡x−cot⁡xcsc⁡2x−cot⁡2x=csc⁡x−cot⁡xe^{-u} = \frac{1}{\csc x + \cot x} \times \frac{\csc x - \cot x}{\csc x - \cot x} = \frac{\csc x - \cot x}{\csc^2 x - \cot^2 x} = \csc x - \cot xe−u=cscx+cotx1​×cscx−cotxcscx−cotx​=csc2x−cot2xcscx−cotx​=cscx−cotx Now, we can find an expression for csc⁡x\csc xcscx by adding eue^ueu and e−ue^{-u}e−u: eu+e−u=(csc⁡x+cot⁡x)+(csc⁡x−cot⁡x)=2csc⁡xe^u + e^{-u} = (\csc x + \cot x) + (\csc x - \cot x) = 2\csc xeu+e−u=(cscx+cotx)+(cscx−cotx)=2cscx The term in the integrand is (2csc⁡x)17(2\csc x)^{17}(2cscx)17, which becomes: (2csc⁡x)17=(eu+e−u)17(2\csc x)^{17} = (e^u + e^{-u})^{17}(2cscx)17=(eu+e−u)17

  4. Finding dx in terms of du: We differentiate the substitution u=log⁡(csc⁡x+cot⁡x)u = \log(\csc x + \cot x)u=log(cscx+cotx) with respect to xxx: dudx=1csc⁡x+cot⁡x⋅ddx(csc⁡x+cot⁡x)\frac{du}{dx} = \frac{1}{\csc x + \cot x} \cdot \frac{d}{dx}(\csc x + \cot x)dxdu​=cscx+cotx1​⋅dxd​(cscx+cotx) dudx=1csc⁡x+cot⁡x⋅(−csc⁡xcot⁡x−csc⁡2x)\frac{du}{dx} = \frac{1}{\csc x + \cot x} \cdot (-\csc x \cot x - \csc^2 x)dxdu​=cscx+cotx1​⋅(−cscxcotx−csc2x) dudx=−csc⁡x(cot⁡x+csc⁡x)csc⁡x+cot⁡x=−csc⁡x\frac{du}{dx} = \frac{-\csc x (\cot x + \csc x)}{\csc x + \cot x} = -\csc xdxdu​=cscx+cotx−cscx(cotx+cscx)​=−cscx So, du=−csc⁡x dxdu = -\csc x \, dxdu=−cscxdx. This gives dx=−ducsc⁡xdx = -\frac{du}{\csc x}dx=−cscxdu​. From step 3, we know csc⁡x=eu+e−u2\csc x = \frac{e^u + e^{-u}}{2}cscx=2eu+e−u​. Substituting this into the expression for dxdxdx: dx=−du(eu+e−u2)=−2 dueu+e−udx = -\frac{du}{(\frac{e^u + e^{-u}}{2})} = -\frac{2 \, du}{e^u + e^{-u}}dx=−(2eu+e−u​)du​=−eu+e−u2du​

  5. Substituting into the integral and simplifying: Now we substitute the new limits, the new integrand, and the new differential into the original integral: I=∫log⁡(1+2)0(eu+e−u)17(−2 dueu+e−u)I = \int\limits_{\log(1+\sqrt{2})}^{0} (e^u + e^{-u})^{17} \left( -\frac{2 \, du}{e^u + e^{-u}} \right)I=log(1+2​)∫0​(eu+e−u)17(−eu+e−u2du​) I=−2∫log⁡(1+2)0(eu+e−u)17eu+e−u duI = -2 \int\limits_{\log(1+\sqrt{2})}^{0} \frac{(e^u + e^{-u})^{17}}{e^u + e^{-u}} \, duI=−2log(1+2​)∫0​eu+e−u(eu+e−u)17​du I=−2∫log⁡(1+2)0(eu+e−u)16 duI = -2 \int\limits_{\log(1+\sqrt{2})}^{0} (e^u + e^{-u})^{16} \, duI=−2log(1+2​)∫0​(eu+e−u)16du Using the property of definite integrals ∫abf(x)dx=−∫baf(x)dx\int_a^b f(x)dx = -\int_b^a f(x)dx∫ab​f(x)dx=−∫ba​f(x)dx, we can flip the limits of integration and remove the negative sign: I=2∫0log⁡(1+2)(eu+e−u)16 duI = 2 \int\limits_{0}^{\log(1+\sqrt{2})} (e^u + e^{-u})^{16} \, duI=20∫log(1+2​)​(eu+e−u)16du

  6. Comparing with the options: The calculated integral is: I=∫0log⁡(1+2)2(eu+e−u)16 duI = \int\limits_0^{\log \left( {1 + \sqrt 2 } \right)} {2{{\left( {{e^u} + {e^{ - u}}} \right)}^{16}}\,du}I=0∫log(1+2​)​2(eu+e−u)16du This matches option A exactly.

Conclusion

The correct option is A.

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