Sufficient condition for Integration by Parts

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In his textbook Calculus, Spivak presents integration by parts as follows:

If $f'$ and $g'$ are continuous then \begin{align*} \int fg'&=fg-\int f'g\\ \int f(x)g'(x)\,dx&=f(x)g(x)-\int f'(x)g(x)\,dx\\ \int_a^b f(x)g'(x)\,dx&=f(x)g(x)\bigg|_a^b-\int_a^b f'(x)g(x)\,dx\\ \end{align*} I understand that without the continuity requirement, $fg'$ and $gf'$ may not be integrable, but why isn't it enough to have $f'$ and $g'$ be integrable functions? Isn't the product of two Riemann-integrable functions necessarily Riemann-integrable?

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Spivak's statement for integration-by-parts (in the context of Riemann integration) holds when $fg’$ and $gf’$, individually, are Riemann integrable, and it is enough just that $f’$ and $g'$ be Riemann integrable when $f$ and $g$ are continuous.

The "counterexample" in the linked paper is relevant for improper integrals.

In the example, $f(x) = x^2 \sin(x^{-4})$ and $g(x) = x^2 \cos(x^{-4})$ on $[0,1]$ with $f(0), g(0) := 0$, and

$$\sin(1)\cos(1) = \int_0^1 (fg’ + gf’) \neq \int_0^1fg’ + \int_0^1 g f’,$$

since the integrals on the RHS do not exist as Riemann integrals (nor as finite Lebesgue integrals).

Rudin's theorem is correct in that $f', \, g' \in \mathcal{R}([a,b])$ requires $f'$ and $g'$ to be bounded. This is not the case in the counterexample.

For more details, note that $f$ and $g$ are differentiable with $f'(0) = g'(0) = 0.$

On $(0,1]$ we have,

$$f'(x) = 2x \sin(x^{-4}) - 4 x^{-3}\cos(x^{-4}), \\ g'(x) = 2x \cos(x^{-4}) + 4 x^{-3}\sin(x^{-4}),\\ f(x)g(x) = \frac{1}{2}x^4 \sin(2 x^{-4}), \\ (fg)'(x) = 2x^2 \sin(2x^{-4}) - 4 x^{-1}\cos(2x^{-4}) $$

Notice that $f(x)g'(x) = 2x^3\sin(x^{-4})\cos(x^{-4})- 4x^{-1} \sin^2(x^{-4})$ where the second term does not have a convergent improper integral over $[0,1]$.

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why isn't it enough to have $f'$ and $g'$ be integrable functions? $$\int_a^b f(x)g'(x)\,dx =f(x)g(x)\bigg|_a^b-\int_a^b f'(x)g(x)\,dx$$

Yes, $f′$ and $g′$ being integrable on $[a,b]$ is sufficent.

$$\int fg'=fg-\int f'g$$

For indefinite integration by parts, the only requirement is that on the intersection of their domains, $f$ and $g$ are differentiable and one of them has an antiderivative.

Proof

Without loss of generality suppose that $g$ has an antiderivative. Then $f'g$ has an antiderivative; denote it by $H.$ Then $(fg-H)$ is an antiderivative of $fg'$.

Now, by the product rule, $(fg)'=f'g+fg'.$ So, $fg=\int(f'g+fg').$

  • Therefore, $fg=\left(\int f'g\right)+\left(\int fg'\right),$ so $$\int fg'=fg-\int f'g.$$
  • By the Fundamental Theorem of Calculus, $\int_a^b(f'g+fg')=fg\bigg|_a^b\ ,$ i.e., $$\int_a^b fg'=fg\bigg|_a^b-\int_a^b f'g.$$