Integration by Parts with Complex Exponentials

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SUMMARY

The discussion focuses on solving the integral ∫xe2x cos(2x)dx using integration by parts and Euler's formula. The user aims to derive the solution ¼e2x(x cos(2x) + x sin(2x) - ½sin(2x)) + C. The application of Euler's formula, cos(2x) = (e2ix + e-2ix)/2, is crucial for transforming the integral into a more manageable form involving complex exponentials.

PREREQUISITES
  • Understanding of integration by parts
  • Familiarity with Euler's formula
  • Knowledge of complex exponentials
  • Basic proficiency in calculus
NEXT STEPS
  • Study the method of integration by parts in depth
  • Learn about the application of Euler's formula in integrals
  • Explore complex analysis techniques for solving integrals
  • Practice solving integrals involving trigonometric functions and exponentials
USEFUL FOR

Students studying calculus, particularly those focusing on integration techniques, as well as educators looking for examples of applying Euler's formula in integral calculus.

abney317
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I'm looking at this problem here. (Exam practice, move to homework if you want...)
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First part is easy, but it's the second part that I can't quite figure out.


I'm trying to get from ∫xe2x cos(2x)dx to this answer:
¼e2x(x cos(2x) + x sin(2x) - ½sin(2x))+C
 
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Do you know Euler's formula?
 
cos(2x)= \frac{e^{2ix}+ e^{-2ix}}{2}
so
\int xe^{2x} cos(2x)dx= \frac{1}{2}\int x(e^{2(1+ i)x}+ e^{2(1- i)x})dx
 
Relativistic Momentum, Mass, and Energy Momentum and mass (...), the classic equations for conserving momentum and energy are not adequate for the analysis of high-speed collisions. (...) The momentum of a particle moving with velocity ##v## is given by $$p=\cfrac{mv}{\sqrt{1-(v^2/c^2)}}\qquad{R-10}$$ ENERGY In relativistic mechanics, as in classic mechanics, the net force on a particle is equal to the time rate of change of the momentum of the particle. Considering one-dimensional...

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