Integration techniques MOC

Integration by parts

Integration by parts is basically an integral version of the product rule.12 By beginning with the product rule, and integrating by π‘₯, we get the following:

𝑑𝑑π‘₯(𝑒𝑣)=𝑣𝑑𝑒𝑑π‘₯+𝑒𝑑𝑣𝑑π‘₯βŸΉπ‘’π‘£=βˆ«π‘£π‘‘π‘’+βˆ«π‘’π‘‘π‘£

which can be rearranged to get the product rule

βˆ«π‘’π‘‘π‘£=π‘’π‘£βˆ’βˆ«π‘£π‘‘π‘’

Or in function notation

βˆ«π‘“(π‘₯)𝑔′(π‘₯)𝑑π‘₯=𝑓(π‘₯)𝑔(π‘₯)βˆ’βˆ«π‘”(π‘₯)𝑓′(π‘₯)𝑑π‘₯

It applies to the situation in which you are called upon to integrate the product of one function (𝑓) and the derivative of another (𝑔); it says you can transfer the derivative from 𝑔 to 𝑓, at the cost of a minus sign and a boundary term.

Higher order derivatives

It follows

βˆ«π‘π‘Žπ‘‘π‘›π‘“π‘‘π‘₯𝑛𝑔𝑑π‘₯=[π‘›βˆ‘π‘—=1π‘‘π‘›βˆ’π‘—π‘“π‘‘π‘₯π‘›βˆ’π‘—π‘‘π‘—βˆ’1𝑔𝑑π‘₯π‘—βˆ’1]π‘₯=𝑏π‘₯=π‘Ž+(βˆ’1)π‘›βˆ«π‘π‘Žπ‘“π‘‘π‘›π‘”π‘‘π‘₯𝑛𝑑π‘₯

Generalizations

By exploiting different generalisations of the Fundamental theorem of calculus along with different generalisations of the product rule, we can generalise integration by parts for vector valued functions.3

Divergence

  1. Scaling
βˆ­Ξ©π‘“(βƒ—βˆ‡β‹…βƒ—π†)π‘‘πœ=βŠ‚βŠƒβˆ¬πœ•Ξ©π‘“βƒ—π†β‹…π‘‘βƒ—πšβˆ’βˆ­Ξ©βƒ—π†β‹…(βƒ—βˆ‡π‘“)π‘‘πœ

Curl

  1. Scaling
βˆ­Ξ©π‘“(βƒ—βˆ‡Γ—βƒ—π†)π‘‘πœ=βˆ’βŠ‚βŠƒβˆ¬πœ•Ξ©π‘“βƒ—π†Γ—π‘‘βƒ—πšβˆ’βˆ­Ξ©(βƒ—βˆ‡π‘“)Γ—βƒ—π†π‘‘πœ

Semi-Riemannian geometry

To covariantly integrate by parts we can use ^P1.

Practice problems


tidy | en | SemBr

Footnotes

  1. 2022. MATH1011: Multivariable calculus, pp. 94–95 (Β§6.3.6) ↩

  2. 2016. Calculus, pp. 512–516 (Β§7.1) ↩

  3. 2013. Introduction to electrodynamics, p. 37 (eqn 1.59) ↩