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TheoremProved

Integration by parts

Statement

If u=u(x)u=u(x) and v=v(x)v=v(x) are differentiable on an interval KK, then ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du, i.e. ∫u(x)v′(x) dx=u(x)v(x)−∫u′(x)v(x) dx\int u(x)v'(x)\,dx = u(x)v(x) - \int u'(x)v(x)\,dx.

Why is it true?

Integration by parts reverses the product rule: it does not remove the integral, but it shifts the derivative from one factor (vv) onto the other (uu), which is exactly the right move when uu becomes simpler after differentiating (like u=xu=x becoming u′=1u'=1) while v′v' stays easy to antidifferentiate — turning a hard product like ∫xex dx\int x e^x\,dx into an easy one.

Proof sketch

By the product rule, (uv)′=u′v+uv′(uv)' = u'v + uv'. Rearranging, uv′=(uv)′−u′vuv' = (uv)' - u'v.

Take the antiderivative (with respect to xx, on KK) of both sides. On the right, (uv)′(uv)' obviously has antiderivative uvuv itself (up to a constant, by the uniqueness theorem), so ∫uv′ dx=∫(uv)′ dx−∫u′v dx=uv−∫u′v dx\int uv'\,dx = \int (uv)'\,dx - \int u'v\,dx = uv - \int u'v\,dx.

Writing dv=v′(x) dxdv = v'(x)\,dx and du=u′(x) dxdu=u'(x)\,dx turns this into the compact mnemonic form ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du. In practice, one factor is chosen as uu (to be differentiated) and the rest as dvdv (to be antidifferentiated), typically preferring to differentiate the factor that simplifies (polynomial, logarithm) and antidifferentiate the factor that stays manageable (exe^x, sin⁡x\sin x, cos⁡x\cos x).

Topics that use this theorem

Step-by-step proofs

No step-by-step proof yet for this theorem.

References

  1. James Stewart (2015). Calculus: Early Transcendentals
  2. Michael Spivak (2008). Calculus
  3. Manuel Bronstein (1998). Symbolic Integration Tutorial