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Home > Integration by parts


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Calculus

Topics in Calculus
Fundamental theorem | Function | Limits of functions | Continuity | Calculus with polynomials
Differentiation
Product rule | Quotient rule | Chain rule | Implicit differentiation | Taylor's theorem
Integration
Integration by substitution | Integration by parts | Integration by trigonometric substitution | Solids of revolution | Integration by disks | Integration by cylindrical shells | Lists of integrals
Vector Calculus
Vector | Vector field | Matrix | Partial Derivative | Gradient | Flux | Divergence | Divergence Theorem | Del | Curl | Green's Theorem | Stokes' Theorem
Tensor Calculus
Tensor | Tensor field | Tensor product | Exterior power | Exterior Derivative | Covariant derivative | Manifold

In calculus, and more generally in mathematical analysis, integration by parts is a rule that transforms the integral of products of functions into other, possibly simpler, integrals. The rule arises from the product rule of differentiation.

Suppose f(x) and g(x) are two continuously differentiable functions. Then the integration by parts rule states that for endpoints a, b

where we use the common notation

The rule is shown to be true by using the product rule for derivatives and the fundamental theorem of calculus. Thus


In the traditional calculus curriculum, this rule is often stated using indefinite integrals in the form

or in an even shorter form, if we let u = f(x), v = g(x) and the differentials du = f′(x) dx and dv = g′(x) dx, then it is in the form in which it is most often seen:

One can also formulate a discrete analogue for sequences, called summation by parts.

Note that the original integral contains the derivative of g; in order to be able to apply the rule, you need to find its antiderivative g and then you still have to evaluate the resulting integral of ∫g f ' dx.

An alternative notation has the advantage that the factors of the original expression are identified as f and g, but the drawback of a nested integral:

This formula is valid whenever f is continuously differentiable and g is continuous.



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