Integration using parametric derivatives

{{Short description|Method which uses known Integrals to integrate derived functions}}

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In calculus, integration by parametric derivatives, also called parametric integration,{{cite journal |last1=Zatja |first1=Aurel J. |title=Parametric Integration Techniques {{!}} Mathematical Association of America |website=www.maa.org |date=December 1989 |volume=Mathematics Magazine |url=https://www.maa.org/sites/default/files/268948443847.pdf |access-date=23 July 2019}} is a method which uses known Integrals to integrate derived functions. It is often used in Physics, and is similar to integration by substitution.

Statement of the theorem

By using the Leibniz integral rule with the upper and lower bounds fixed we get that


\frac{d}{dt}\left(\int_a^b f(x,t)dx\right)=\int_a^b \frac{\partial}{\partial t} f(x,t)dx

It is also true for non-finite bounds.

Examples

=Example One: Exponential Integral=

For example, suppose we want to find the integral

: \int_0^\infty x^2 e^{-3x} \, dx.

Since this is a product of two functions that are simple to integrate separately, repeated integration by parts is certainly one way to evaluate it. However, we may also evaluate this by starting with a simpler integral and an added parameter, which in this case is t = 3:

:

\begin{align}

& \int_0^\infty e^{-tx} \, dx = \left[ \frac{e^{-tx}}{-t} \right]_0^\infty = \left( \lim_{x \to \infty} \frac{e^{-tx}}{-t} \right) - \left( \frac{e^{-t0}}{-t} \right) \\

& = 0 - \left( \frac{1}{-t} \right) = \frac{1}{t}.

\end{align}

This converges only for t > 0, which is true of the desired integral. Now that we know

: \int_0^\infty e^{-tx} \, dx = \frac{1}{t},

we can differentiate both sides twice with respect to t (not x) in order to add the factor of x2 in the original integral.

:

\begin{align}

& \frac{d^2}{dt^2} \int_0^\infty e^{-tx} \, dx = \frac{d^2}{dt^2} \frac{1}{t} \\[10pt]

& \int_0^\infty \frac{d^2}{dt^2} e^{-tx} \, dx = \frac{d^2}{dt^2} \frac{1}{t} \\[10pt]

& \int_0^\infty \frac{d}{dt} \left (-x e^{-tx}\right) \, dx = \frac{d}{dt} \left(-\frac{1}{t^2}\right) \\[10pt]

& \int_0^\infty x^2 e^{-tx} \, dx = \frac{2}{t^3}.

\end{align}

This is the same form as the desired integral, where t = 3. Substituting that into the above equation gives the value:

: \int_0^\infty x^2 e^{-3x} \, dx = \frac{2}{3^3} = \frac{2}{27}.

=Example Two: Gaussian Integral=

Starting with the integral \int^\infty_{-\infty} e^{-x^2t}dx=\frac{\sqrt\pi}{\sqrt t},

taking the derivative with respect to t on both sides yields


\begin{align}

&\frac{d}{dt}\int^\infty_{-\infty} e^{-x^2t}dx=\frac{d}{dt}\frac{\sqrt\pi}{\sqrt t}\\

&-\int^\infty_{-\infty} x^2 e^{-x^2t} = -\frac{\sqrt \pi}{2}t^{-\frac{3}{2}}\\

&\int^\infty_{-\infty} x^2e^{-x^2t}= \frac{\sqrt{\pi}}{2}t^{-\frac{3}{2}}

\end{align}.

In general, taking the n-th derivative with respect to t gives us


\int^\infty_{-\infty} x^{2n}e^{-x^2t}= \frac{(2n-1)!!\sqrt \pi}{2^n}t^{-\frac{2n+1}{2}}.

=Example Three: A Polynomial=

Using the classical \int x^t dx=\frac{x^{t+1}}{t+1} and taking the derivative with respect to t we get


\int \ln(x)x^t= \frac{\ln(x)x^{t+1}}{t+1} - \frac{x^{t+1}}{(t+1)^2}.

=Example Four: Sums=

The method can also be applied to sums, as exemplified below.


Use the Weierstrass factorization of the sinh function:


\frac{\sinh (z)}{z}=\prod_{n=1}^\infty \left(\frac{\pi^2 n^2 + z^2}{\pi^2 n^2}\right).


Take the logarithm:


\ln(\sinh (z)) - \ln(z)=\sum_{n=1}^\infty \ln\left(\frac{\pi^2 n^2 + z^2}{\pi^2 n^2}\right).


Derive with respect to z:


\coth(z) - \frac{1}{z}= \sum^\infty_{n=1}\frac{2z}{z^2+\pi^2n^2}.


Let w=\frac{z}{\pi}:


\frac{1}{2}\frac{\coth(\pi w)}{\pi w} - \frac{1}{2}\frac{1}{z^2}=\sum^\infty_{n=1}\frac{1}{n^2+w^2}.

References

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