Difference in numerical approach for PDE vs ODE

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TheCanadian
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I think I am missing something painfully obvious, but what exactly is the difference in algorithms used to solve PDEs vs ODEs? For example, I've been looking at finite difference methods and the general steps (from what I've seen, although particular approaches may vary) used to numerically solve PDEs and ODEs using this method is to set up a grid for your domain, define boundary/initial conditions, and then take the total (partial) derivative and add it to the previous step's value to find adjacent values.

For example (after initializing values), if I have a function P composed of two variables (t and z) with the total (partial) derivative operator given by Dt for the time derivative and Dz for the spatial derivative, then I set up a loop and it might look something like this:

Code:
j = 0
i = 0
while i < len(t):
    DtP = Dt(P[j,i])
    P[j,i+1] = P[j,i] + ht*DtP

    while j < len(z):
       DzP = Dz(P[j,i])
       P[j+1,i] = P[j,i] + hz*DzP
       j = j + 1

    i = i + 1

Please correct my huge misunderstanding here (or if my basic code is incredibly wrong in its approach), but how exactly is the finite difference method different for the two approaches, besides using a partial or total derivative to iterate the next step?

If you have any other methods besides finite difference methods that could also help distinguish the two approaches to solving ODEs and PDEs, that would be helpful as well.[/code]
 
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If you use the straightforward finite differencing for a PDE, you usually encounter numerically unstable behavior, which means that the numerical errors in your solution grow exponentially as a function of the time variable t. That is why there are Crank-Nicolson schemes and semi-implicit schemes for solution of PDE:s.
 
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hilbert2 said:
If you use the straightforward finite differencing for a PDE, you usually encounter numerically unstable behavior, which means that the numerical errors in your solution grow exponentially as a function of the time variable t. That is why there are Crank-Nicolson schemes and semi-implicit schemes for solution of PDE:s.

Thank you for the clarifying that. I'll definitely read more about the stability of the different approaches for PDE solvers. In case I'm misinterpreting you, why do ODE not encounter the same unstable behaviour for the different approaches?