here are some last minute pointers
remember that
F(s) = int( f(t)*exp(-st) dt) from 0 to ??
if f(t) has no singularities this is an easy integral
ie. if f(t) is a constant K then we have
F(s) = lim (a-> ??) K*[exp(-s*0)/s + K*exp(-s*a)] = K/s
if (t) is a polynomial, you can do it term by term by doing integration by parts. I won't bore you with the details but for a polynomial f(t) = t^n you get F(s) = n!/s^(n+1)
sin's and cos's (as well as their hyperbolic counterparts) also shouldn't be a problem, again do it by parts. For example, for f(t) = sin(bt)
F(s) = b/(s^2+b^2). If you know a bit of complex calculus, you can solve the integral int(exp(ibt+st)) and easily obtain the transform for cos(bt) and sin(bt): Re(int) and Im(int) respectively.
You might have to understand some transforms for generalized functions such as the Dirac delta or the step function. Just memorize those, they're easy to remember anyways.
Convolution is a major pain in the ass, don't use it if at all possible. Otherwise, memorize the form and try applying it.
Also, the nth derivative of f(t) becomes s^nF(s) - s^(n-1)f(0) - s^(n-2)f'(n) - ... - d^(n-1)f/(dt)^(n-1) evaluated at 0 in the S-domain.
For anything that has a singularity on the real axis (ie f(t) = 1/t) you need contour integrals in the complex plane so I'm guessing he hasn't shown you that.
The Laplace inverse is, at your level, just going to be identifying the forms that I stated above and reversing the operation. You'll likely be using a lot of partial fractions, so make sure you revise those.
The PDE's you've learned in your course are probably nothing too complicated here are the 2 cases you'll robably see:
1) take the Laplace with respect to one variable to obtain an ODE in the S-domain with respect to the other variable. Solve using the techniques you know, take the Laplace inverse to get the answer in the time domain. Plug in ICs and BVPs to get rid of constants and you're done. This is how you'll solve the heat equation for simple cases like a heated bar.
2) Assume the variables can be separated, that is, that you can obtain f(x,t) = F(x)G(t). Once you make that assumption there are a lot of things that simplify out pretty nicely and you should be able to obtain a solution using a Fourier expansion for the different modes of vibration.
Fourier expansions are 1/(2Pi)*int(f(t)*exp(-iwt) dt) from -?? to ?? which is easy to evaluate in the complex plane. More than likely however, you can just find the expansion in the region you're looking at since you'll have a string of finite length and of fixed ends and you won't have any singularites.
If you still have time to look at another book, check out Nagle, Saff, and Snider it covers all these topics in detail.
Anyhow, I hope this helps you, let me know if you want a little more detail about something and best of luck on your final
BTW, we did almost everything you covered in our introduction to DE Eq. class though we didn't solve too many heat equations. Although, the dude teaching us did go nuts with the series stuff though and shoed us a ton of stuff with gamma and bessel functions.