The only thing complicated about that integral is your way of doing it. Instead, do it by parts:
\int cos(\omega x)e^{ax}dx
Let u= cos(\omega x, dv= e^{ax}dx so that du= -\omega sin(\omega x)dx and v= (1/a)e^{ax} so we have
\int udv= uv- \int vdu= \frac{1}{a}e^{ax}cos(\omega x)+ \frac{\omega}{a}\int e^{ax}sin(\omega x)dx
Now, do it again. Let u= sin(\omega x) and dv= e^{ax} so that du= \omega cos(\omega x)dx and v= (1/a) e^{ax}.
Now you have
\int e^{ax}cos(\omega x) dx= \frac{1}{a}e^{ax}cos(\omega x)+\frac{\omega}{a^2}e^{ax}sin(\omega x)- \frac{\omega^2}{a^2}\int e^{ax}cos(\omega x)dx
Add \int e^{ax}cos(\omega x) dx to both sides and divide by 2.
#4
michaelbarret
2
0
Thanks HallsofIvy for your reply.
I think the biggest thing I'm unsure on is how my original signal can be generalised to ∫cos(wx) e^ax dx. In my case does w=w, x=t(1-qt) and dx=dt?
Also sorry If it's obvious but I don't really understand why I should add ∫e^ax cos(ωx)dx to both sides and divide by 2.
I can't figure out how to integrate the complex exponential associated with the FT either, ∫e^-jwt dt
#5
algebrat
428
1
Yeah last helper might not have noticed the squaring of t in the original problem, it also looks like you didn't write it after the first line. But it looks like you were close to done, I like what you have worked out on the PDF. I think the next goal might be to complete the square and use some substitutions and move things around so you almost have that thing that's equal to root pi over a.
I'm reviewing Meirovitch's "Methods of Analytical Dynamics," and I don't understand the commutation of the derivative from r to dr:
$$
\mathbf{F} \cdot d\mathbf{r} = m \ddot{\mathbf{r}} \cdot d\mathbf{r} = m\mathbf{\dot{r}} \cdot d\mathbf{\dot{r}}
$$