andyyee
- 2
- 0
Homework Statement
I'm working out a differential equation problem that I am supposed to solve with the formula \mathcal{L}\{t^\alpha\} = \frac{\Gamma{(\alpha + 1)}}{s^{\alpha+1}}. The problem is \mathcal{L}\{t^{\frac{1}{2}}\} (finding the Laplace transform of the given function).
Homework Equations
\mathcal{L}\{t^\alpha\} = \frac{\Gamma(\alpha + 1)}{s^{\alpha+1}}, \alpha > -1
\Gamma(\alpha) = \int^\infty_0{t^{\alpha-1}e^{-t}dt}, \alpha > 0
The Attempt at a Solution
I plug it into the equation, and get \frac{\Gamma(\frac{3}{2})}{s^\frac{3}{2}} = \frac{\int^\infty_0 {t^\frac{1}{2}e^{-t}dt}}{s^{3/2}}. That's where I run into a problem, I have no idea how to solve that integral. I can't use integration by parts, because one term will never disappear or the original integral will not appear again as \int{vdu}, so that won't work. I looked it up on Wolfram|Alpha, and it gave me \frac{1}{2}\sqrt{\pi}\text{erf}{(\sqrt{t})} - e^{-t}\sqrt{t} for the indefinite form and \frac{\sqrt{\pi}}{2} for the definite form. It also cited some stuff about integrating the normal distribution and error form, but I don't understand what it is talking about. What I am unsure about is the steps involved in solving the integral, and is there a generalized solution (for the definite integral from 0 to \infty) for other coefficient values in the power of the polynomial?
Thanks
Andrew