Integration of UV Formula — ∫u dv = uv − ∫v du

#Math Formula
TL;DR
The integration of uv formula — integration by parts — is ∫u,dv=uv−∫v,du\int u,dv = uv - \int v,du, the integration counterpart of the product rule for derivatives. This article derives it from the product rule, explains the ILATE rule for choosing uu, works six examples in increasing difficulty (including the ∫ln⁡x,dx\int \ln x,dx trick), and shows the mistakes that turn a one-line problem into an endless loop.
BT
Bhanzu TeamLast updated on June 22, 20269 min read

A Formula for Products That Refuse to Integrate

Differentiating a product is easy — the product rule handles xsin⁡xx\sin x or xexxe^x in seconds. Integrating one is where students hit a wall, because there is no "product rule for integrals." The integration of uv formula is the closest thing: it doesn't integrate the product directly, it trades a hard integral for an easier one.

The integration of uv formula — also called integration by parts or the uv rule of integration — says:

;∫u,dv=uv−∫v,du;\boxed{;\int u,dv = uv - \int v,du;}

You split the integrand into a part uu (which you'll differentiate) and a part dvdv (which you'll integrate), and the formula rewrites the original integral as a product minus a new integral — one you choose your split to make simpler.

What Is the Integration of UV Formula?

The integration of uv formula is the technique for integrating a product of two functions when no straightforward antiderivative exists. It is the integral analogue of the product rule. In its most-used form:

∫u,dv=uv−∫v,du.\int u,dv = uv - \int v,du.

Here uu and vv are functions of xx; you pick uu and dvdv from the integrand, then compute dudu (by differentiating uu) and vv (by integrating dvdv). Written fully in terms of xx, with uu and ww the two factors:

∫u,w,dx=u∫w,dx−∫(u′∫w,dx)dx.\int u,w,dx = u\int w,dx - \int\left(u'\int w,dx\right)dx.

The point is never to integrate the product head-on. It is to swap the original integral for uv−∫v,duuv - \int v,du, where the new integral ∫v,du\int v,du is simpler than the one you started with. Choose the split so that differentiating uu shrinks it.

How Is the Integration of UV Formula Derived?

It comes straight from the product rule for derivatives. Start with two functions uu and vv:

ddx(uv)=udvdx+vdudx.\frac{d}{dx}(uv) = u\frac{dv}{dx} + v\frac{du}{dx}.

Integrate both sides with respect to xx. The left side integrates back to uvuv:

uv=∫u,dvdx,dx+∫v,dudx,dx=∫u,dv+∫v,du.uv = \int u,\frac{dv}{dx},dx + \int v,\frac{du}{dx},dx = \int u,dv + \int v,du.

Now rearrange to isolate the integral you want:

∫u,dv=uv−∫v,du.\int u,dv = uv - \int v,du.

That's the whole derivation. Integration by parts is the product rule run backwards and solved for one of its two integrals. (The product rule it inverts is the one from our uv differentiation formula guide — worth reading alongside this, because the contrast is the clearest way to see what each rule does.)

How Do You Choose u? The ILATE Rule

The formula only helps if the new integral ∫v,du\int v,du is easier than the original. The choice of uu decides that. The ILATE rule (also written LIATE) ranks function types by how good a choice they make for uu — pick uu from whichever type comes first:

Priority

Type

Example

I

Inverse trigonometric

arctan⁡x\arctan x, arcsin⁡x\arcsin x

L

Logarithmic

ln⁡x\ln x, log⁡x\log x

A

Algebraic

xx, x2x^2, polynomials

T

Trigonometric

sin⁡x\sin x, cos⁡x\cos x

E

Exponential

exe^x, 2x2^x

The logic: uu should get simpler when differentiated, and dvdv should stay manageable when integrated. Logarithms and inverse-trig functions simplify dramatically under differentiation (they turn into algebraic fractions), so they make excellent uu. Exponentials and trig functions barely change when integrated, so they make safe dvdv. For ∫xln⁡x,dx\int x\ln x,dx, L beats A, so u=ln⁡xu = \ln x.

Examples of the Integration of UV Formula

Example 1

Evaluate ∫x,ex,dx\int x,e^x,dx.

By ILATE, Algebraic (A) beats Exponential (E), so u=xu = x and dv=ex,dxdv = e^x,dx. Then du=dxdu = dx and v=exv = e^x:

∫x,ex,dx=uv−∫v,du=x,ex−∫ex,dx=x,ex−ex+C.\int x,e^x,dx = uv - \int v,du = x,e^x - \int e^x,dx = x,e^x - e^x + C.

Final answer: ∫x,ex,dx=ex(x−1)+C\int x,e^x,dx = e^x(x - 1) + C.

Example 2

Evaluate ∫xcos⁡x,dx\int x\cos x,dx.

The instinct here is to make the trig function uu, because trig "feels like the main function." Follow that and watch what happens.

Wrong path. Let u=cos⁡xu = \cos x and dv=x,dxdv = x,dx. Then du=−sin⁡x,dxdu = -\sin x,dx and v=x22v = \frac{x^2}{2}:

∫xcos⁡x,dx=x22cos⁡x−∫x22(−sin⁡x),dx=x22cos⁡x+12∫x2sin⁡x,dx.\int x\cos x,dx = \frac{x^2}{2}\cos x - \int \frac{x^2}{2}(-\sin x),dx = \frac{x^2}{2}\cos x + \frac12\int x^2\sin x,dx.

The new integral ∫x2sin⁡x,dx\int x^2\sin x,dx is worse than the original — the power went up from xx to x2x^2. The split made the problem harder, not easier.

The break. ILATE puts Algebraic (A) before Trigonometric (T). Choosing the trig function as uu violates the rule, and the symptom is exactly this: the algebraic power grows instead of shrinking.

The rescue. Let u=xu = x (Algebraic) and dv=cos⁡x,dxdv = \cos x,dx. Then du=dxdu = dx and v=sin⁡xv = \sin x:

∫xcos⁡x,dx=xsin⁡x−∫sin⁡x,dx=xsin⁡x+cos⁡x+C.\int x\cos x,dx = x\sin x - \int \sin x,dx = x\sin x + \cos x + C.

Final answer: ∫xcos⁡x,dx=xsin⁡x+cos⁡x+C\int x\cos x,dx = x\sin x + \cos x + C. Differentiating u=xu = x down to 11 is what collapses the new integral to something trivial.

Example 3

Evaluate ∫x2ln⁡x,dx\int x^2\ln x,dx.

By ILATE, Logarithmic (L) beats Algebraic (A), so u=ln⁡xu = \ln x and dv=x2,dxdv = x^2,dx. Then du=1x,dxdu = \frac{1}{x},dx and v=x33v = \frac{x^3}{3}:

∫x2ln⁡x,dx=x33ln⁡x−∫x33⋅1x,dx=x33ln⁡x−13∫x2,dx=x33ln⁡x−x39+C.\int x^2\ln x,dx = \frac{x^3}{3}\ln x - \int \frac{x^3}{3}\cdot\frac{1}{x},dx = \frac{x^3}{3}\ln x - \frac13\int x^2,dx = \frac{x^3}{3}\ln x - \frac{x^3}{9} + C.

Final answer: ∫x2ln⁡x,dx=x33ln⁡x−x39+C\int x^2\ln x,dx = \dfrac{x^3}{3}\ln x - \dfrac{x^3}{9} + C.

Example 4

Evaluate ∫ln⁡x,dx\int \ln x,dx (a single function, no obvious product).

The trick: write ln⁡x\ln x as a product with 11. Let u=ln⁡xu = \ln x and dv=1,dxdv = 1,dx. Then du=1x,dxdu = \frac{1}{x},dx and v=xv = x:

∫ln⁡x,dx=xln⁡x−∫x⋅1x,dx=xln⁡x−∫1,dx=xln⁡x−x+C.\int \ln x,dx = x\ln x - \int x\cdot\frac{1}{x},dx = x\ln x - \int 1,dx = x\ln x - x + C.

Final answer: ∫ln⁡x,dx=xln⁡x−x+C\int \ln x,dx = x\ln x - x + C. Integration by parts cracks "non-product" integrals like ln⁡x\ln x and arctan⁡x\arctan x by pairing them with an invisible factor of 11.

Example 5

Evaluate ∫arctan⁡x,dx\int \arctan x,dx.

Same 11-trick: u=arctan⁡xu = \arctan x (Inverse trig, top of ILATE), dv=1,dxdv = 1,dx, so du=11+x2,dxdu = \frac{1}{1 + x^2},dx and v=xv = x:

∫arctan⁡x,dx=xarctan⁡x−∫x1+x2,dx.\int \arctan x,dx = x\arctan x - \int \frac{x}{1 + x^2},dx.

The remaining integral is a standard substitution (w=1+x2w = 1 + x^2): ∫x1+x2,dx=12ln⁡(1+x2)\int \frac{x}{1+x^2},dx = \frac12\ln(1 + x^2). So:

∫arctan⁡x,dx=xarctan⁡x−12ln⁡(1+x2)+C.\int \arctan x,dx = x\arctan x - \frac12\ln(1 + x^2) + C.

Final answer: ∫arctan⁡x,dx=xarctan⁡x−12ln⁡(1+x2)+C\int \arctan x,dx = x\arctan x - \dfrac12\ln(1 + x^2) + C.

Example 6

Evaluate ∫exsin⁡x,dx\int e^x\sin x,dx (the loop that closes on itself).

Neither factor simplifies under differentiation, so apply the formula twice and let the original integral reappear. Let I=∫exsin⁡x,dxI = \int e^x\sin x,dx. With u=sin⁡xu = \sin x, dv=ex,dxdv = e^x,dx:

I=exsin⁡x−∫excos⁡x,dx.I = e^x\sin x - \int e^x\cos x,dx.

Apply parts again to ∫excos⁡x,dx\int e^x\cos x,dx with u=cos⁡xu = \cos x, dv=ex,dxdv = e^x,dx:

∫excos⁡x,dx=excos⁡x+∫exsin⁡x,dx=excos⁡x+I.\int e^x\cos x,dx = e^x\cos x + \int e^x\sin x,dx = e^x\cos x + I.

Substitute back: I=exsin⁡x−(excos⁡x+I)=exsin⁡x−excos⁡x−II = e^x\sin x - (e^x\cos x + I) = e^x\sin x - e^x\cos x - I. Solve for II:

2I=ex(sin⁡x−cos⁡x);⇒;I=ex(sin⁡x−cos⁡x)2+C.2I = e^x(\sin x - \cos x) ;\Rightarrow; I = \frac{e^x(\sin x - \cos x)}{2} + C.

Final answer: ∫exsin⁡x,dx=ex(sin⁡x−cos⁡x)2+C\int e^x\sin x,dx = \dfrac{e^x(\sin x - \cos x)}{2} + C. The reappearing integral isn't a dead end — it's solved like an algebraic unknown.

Where the Integration of UV Formula Carries Real Weight

Integration by parts is not just an exam technique — it is one of the load-bearing tools of applied mathematics.

  • Physics — quantum mechanics. Deriving expectation values and the momentum operator's action relies on integration by parts to shift a derivative off the wavefunction. The "boundary terms" that drop out are exactly the uvuv part of the formula.

  • Signal processing — the Fourier and Laplace transforms. Computing the transform of a derivative, ∫f′(t)e−st,dt\int f'(t)e^{-st},dt, uses integration by parts to convert differentiation into multiplication by ss — the property that makes Laplace transforms solve differential equations.

  • Probability and statistics. The expected value E[X]=∫0∞(1−F(x)),dxE[X] = \int_0^\infty (1 - F(x)),dx for a non-negative random variable is derived by integrating ∫xf(x),dx\int x f(x),dx by parts.

  • Engineering — the weak form of differential equations. The finite element method, behind nearly all structural and fluid simulation, rewrites differential equations in "weak form" using integration by parts so that solutions need only be once-differentiable.

For Class 12 and first-year calculus students, the immediate use is evaluating integrals like ∫xex,dx\int x e^x,dx — but the same formula reappears across physics, transforms, and the numerical methods behind modern engineering software.

Tripping Points to Avoid

Mistake 1: Choosing u and dv backwards

Where it slips in: Picking uu as the function that grows under differentiation (a trig or exponential factor) instead of the one that shrinks.

Don't do this: Choose uu by which function "looks more important." That has no bearing on whether the new integral is easier.

The correct way: Use ILATE — pick uu from the type highest on the list.

Mistake 2: Dropping the minus sign before the second integral

Where it slips in: Writing ∫u,dv=uv+∫v,du\int u,dv = uv + \int v,du — a plus where the formula needs a minus.

Don't do this: Treat the formula as symmetric. The minus sign is not optional; it comes directly from rearranging the product rule.

The correct way: Always ∫u,dv=uv−∫v,du\int u,dv = uv - \int v,du. The memorizer archetype, who recites "uv minus integral v du," still loses the sign mid-computation when the line gets long — write the minus first, before filling in the integral.

Mistake 3: Forgetting the constant of integration

Where it slips in: Reporting the final antiderivative without +C+ C, especially after a multi-step problem like Example 6.

Don't do this: Assume the constant doesn't matter because "it's just a constant." On a definite integral it cancels, but on an indefinite one it is part of the answer.

The correct way: Every indefinite integral ends in +C+ C. The silent-understander archetype does the calculus perfectly and then loses a mark on the missing constant, every single time.

Conclusion

  • The integration of uv formula is ∫u,dv=uv−∫v,du\int u,dv = uv - \int v,du — the integration counterpart of the product rule.

  • It is derived by integrating the product rule ddx(uv)=u,dv/dx+v,du/dx\frac{d}{dx}(uv) = u,dv/dx + v,du/dx and solving for one integral.

  • Use the ILATE rule (Inverse trig, Logarithmic, Algebraic, Trigonometric, Exponential) to choose uu so the new integral is simpler.

  • The pairing-with-1 trick integrates lone functions like ln⁡x\ln x and arctan⁡x\arctan x; the loop trick handles ∫exsin⁡x,dx\int e^x\sin x,dx.

  • The most common errors are choosing uu and dvdv backwards, dropping the minus sign, and forgetting +C+ C.

Practice These Before Moving On

  1. Evaluate ∫xsin⁡x,dx\int x\sin x,dx.

  2. Evaluate ∫x,ln⁡x,dx\int x,\ln x,dx.

  3. Evaluate ∫excos⁡x,dx\int e^x\cos x,dx using the loop method.

If Problem 1 gave a higher power of xx in the new integral, return to Mistake 1 — ILATE puts Algebraic before Trigonometric, so u=xu = x.

Want a live Bhanzu trainer to walk your child through integration by parts and the Class 12 calculus chapter? Book a free demo class — online globally.

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Frequently Asked Questions

What is the integration of uv formula?
It is integration by parts: ∫u,dv=uv−∫v,du\int u,dv = uv - \int v,du. It rewrites the integral of a product as a product minus a simpler integral.
How do you use the integration of uv formula?
Split the integrand into uu and dvdv (use ILATE to pick uu), compute dudu and vv, then substitute into uv−∫v,duuv - \int v,du and evaluate the new, easier integral.
What does dv mean in the formula?
dvdv is the part of the integrand you choose to integrate (together with dxdx). You integrate it to get vv, while the other part, uu, you differentiate to get dudu.
What is the ILATE rule?
ILATE — Inverse trig, Logarithmic, Algebraic, Trigonometric, Exponential — is the priority order for choosing uu. Pick uu as the function whose type appears first in the list.
How is integration by parts different from the product rule?
The product rule differentiates a product; integration by parts integrates one. In fact integration by parts is the product rule integrated and rearranged — they are inverse operations.
Can I integrate ln x or arctan x with this formula?
Yes. Pair the single function with dv=1,dxdv = 1,dx. For example, ∫ln⁡x,dx=xln⁡x−x+C\int \ln x,dx = x\ln x - x + C, taking u=ln⁡xu = \ln x and dv=1,dxdv = 1,dx.
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