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=Introduction=
 
=Introduction=
  
Feynman Integral is a powerful integration technique as we use the method of differentiating under the integral sign. Feynman's Technique of integration utilizes parametrization and a mix of other different mathematical properties in order to integrate an integral that is can't be integrated through normal processes like u-substitution or integration by parts. It primarily focuses on setting a function equal to an integral and then differentiating the function to get an integral that is easier to work with. This technique is also popularly known as the "Leibniz Integral Rule".
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When solving an integration problem in calculus, you may come across some complex problems where, when you try to solve the integration with various methods like "integration by parts," "powers of sine and cosine," "U-substitution," "trigonometric substitution," "rational functions," and "numerical integration" and still not get the desired answer and end up over-complicating the integral. To make life a bit simpler for such integrals, we can use "Feynman Integrals" which is a technique focusing on setting a function similar to the integral and then differentiating that function under the integral sign. This method of integration is also known as "Leibniz' Integral Rule".
  
 
<center>[[Image:Richard_Feynman.jpeg]]</center>
 
<center>[[Image:Richard_Feynman.jpeg]]</center>
  
Richard Philip Feynman, an American theoretical physicist, is known for this integration technique along with his other works in the theory of quantum electrodynamics, path integral formulation of quantum mechanics, the physics of the superfluidity of supercooled liquid helium, and in particle physics for which he proposed the parton model.
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Richard Philip Feynman, an American theoretical physicist, is known for this integration technique along with his other works in the theory of quantum electrodynamics, path integral formulation of quantum mechanics, the physics of the superfluidity of supercooled liquid helium, and in particle physics for which he proposed the parton model. His technique to solve integrals by using differentiation under the integral sign helps to find the derivative on the nth order of the product of two functions to be expressed with a formula's help.
  
 
[[ Walther MA271 Fall2020 topic14 | Back to Feynman Integrals]]
 
[[ Walther MA271 Fall2020 topic14 | Back to Feynman Integrals]]
  
 
[[Category:MA271Fall2020Walther]]
 
[[Category:MA271Fall2020Walther]]

Latest revision as of 03:06, 3 December 2020

Introduction

When solving an integration problem in calculus, you may come across some complex problems where, when you try to solve the integration with various methods like "integration by parts," "powers of sine and cosine," "U-substitution," "trigonometric substitution," "rational functions," and "numerical integration" and still not get the desired answer and end up over-complicating the integral. To make life a bit simpler for such integrals, we can use "Feynman Integrals" which is a technique focusing on setting a function similar to the integral and then differentiating that function under the integral sign. This method of integration is also known as "Leibniz' Integral Rule".

Richard Feynman.jpeg

Richard Philip Feynman, an American theoretical physicist, is known for this integration technique along with his other works in the theory of quantum electrodynamics, path integral formulation of quantum mechanics, the physics of the superfluidity of supercooled liquid helium, and in particle physics for which he proposed the parton model. His technique to solve integrals by using differentiation under the integral sign helps to find the derivative on the nth order of the product of two functions to be expressed with a formula's help.

Back to Feynman Integrals

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Abstract algebra continues the conceptual developments of linear algebra, on an even grander scale.

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