Still, I'll use the implementation of the 1D FDTD method (you can simply understand it as a kind of explicit finite difference scheme for the Maxwell's equation) as the example. Just for completeness, here is the 1D Maxwell's equation:
$$\mu \frac{\partial H_y}{\partial t}=\frac{\partial E_z}{\partial x}$$ $$\epsilon \frac{\partial E_z}{\partial t}=\frac{\partial H_y}{\partial x}$$
and the corresponding finite difference equation:
$$H_y^{q+\frac{1}{2}}\left[m+\frac{1}{2}\right]\text{==}H_y^{q-\frac{1}{2}}\left[m+\frac{1}{2}\right]+\frac{\Delta _t}{\mu \Delta _x}\left(E_z^q[m+1]-E_z^q[m]\right)$$ $$E_z^{q+1}[m]==E_z^q[m]+\frac{\Delta _t}{\epsilon \Delta _x}\left(H_y^{q+\frac{1}{2}}\left[m+\frac{1}{2}\right]-H_y^{q+\frac{1}{2}}\left[m-\frac{1}{2}\right]\right)$$
The toy code I've repeatedly used in several posts implementing the difference scheme is:
ie = 200;
ez = ConstantArray[0., {ie + 1}];
hy = ConstantArray[0., {ie}];
fdtd1d = Compile[{{steps}},
Module[{ie = ie, ez = ez, hy = hy},
Do[ez[[2 ;; ie]] += (hy[[2 ;; ie]] - hy[[1 ;; ie - 1]]);
ez[[1]] = Sin[n/10];
hy[[1 ;; ie]] += (ez[[2 ;; ie + 1]] - ez[[1 ;; ie]]), {n,
steps}]; ez]];
result = fdtd1d[10000]; // AbsoluteTiming
Notice that constants like $\mu$, $\Delta _t$ are omitted for simplicity.
Personally I think it's a typical example for the implementation of finite difference method (FDM), so here's the question: has this piece of code (at least almost) touched the speed limit of Mathematica? In fact several months ago, I found that if the code is rewrited with Julia, it'll be 4 times faster.
Indeed, I know this might be the case that one should use the best-suited tool for a specific job, but since I've already gained some stupid pride on using Mathematica and am unwilling to spend time to learn a new programming language (Wolfram is almost my first programming language, I used to learn some VB, but already gave it back to my teacher when started to use Mathematica), I still want to make sure if the Mathematica version of the code can be faster.
If it's the limitation, I'd like to know why there's such a big difference.
Any help would be appreciated.
CompilePrint[fdtd1d]
we find that the first three instructions in the compiled function are calls toMainEvaluate
. If you addCompilationOptions -> {"InlineExternalDefinitions" -> True}
and repeat, the first two instructions are nowCopyTensor
, although there is virtually no difference in the timings between the two functions. This may mean nothing, or it may be something worth investigating. $\endgroup$"InlineExternalDefinitions" -> True
or changing the beginning part toWith[{ie2 = ie, ez2 = ez, hy2 = hy}, Compile[{{steps}}, Module[{ie = ie2, ez = ez2, hy = hy2}, …
orWith[{ie = 200}, Compile[{{steps}}, Module[{ez = Table[0., {ie + 1}], hy = Table[0., {ie}]}, …
doesn't help, the bottleneck is insideDo
. $\endgroup$"CompileOptions"
(-O3
,-Ofast
, etc.) but didn't get a speed-up… Could you give an example? (BTW-Ofast
does help in speeding up this code :D) $\endgroup$