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- // -*- mode: c++; coding: utf-8 -*-
- // ra-ra/examples - Maxwell, 4-vector potential vacuum field equations
- // After Chaitin1986, p. 14. Attempt at straight translation from APL.
- // (c) Daniel Llorens - 2016-2023
- // This library is free software; you can redistribute it and/or modify it under
- // the terms of the GNU Lesser General Public License as published by the Free
- // Software Foundation; either version 3 of the License, or (at your option) any
- // later version.
- #include <iostream>
- #include <thread>
- #include <string>
- #include "ra/test.hh"
- #include "ra/ra.hh"
- #include "ra/bench.hh"
- #include <numbers>
- using real = double;
- template <class T, int rank> using array = ra::Big<T, rank>;
- using ra::iota;
- auto H = ra::all;
- template <int n> constexpr ra::dots_t<n> HH = ra::dots<n>;
- constexpr auto PI = std::numbers::pi_v<double>;
- using std::cout, std::endl, ra::TestRecorder;
- using ra::int_c;
- int main()
- {
- TestRecorder tr(cout);
- real delta = 1;
- int o=20, n=20, m=2, l=2;
- array<real, 5> A({o, n, m, l, 4}, 0.);
- array<real, 6> DA({o, n, m, l, 4, 4}, 0.);
- array<real, 6> F({o, n, m, l, 4, 4}, 0.);
- array<real, 4> divA({o, n, m, l}, 0.);
- array<real, 4> X({n, m, l, 4}, 0.), Y({n, m, l, 4}, 0.);
- A(0, H, H, H, 2) = -cos(iota(n)*(2*PI/n))/(2*PI/n);
- A(1, H, H, H, 2) = -cos((iota(n)-delta)*(2*PI/n))/(2*PI/n);
- auto t0 = Benchmark::clock::now();
- // FIXME this is painful without a roll operator, but we need a roll operator without temps.
- for (int t=1; t+1<o; ++t) {
- // X←(1⌽[0]A[T;;;;])+(1⌽[1]A[T;;;;])+(1⌽[2]A[T;;;;])
- X(iota(n-1)) = A(t, iota(n-1, 1));
- X(n-1) = A(t, 0);
- X(H, iota(m-1)) += A(t, H, iota(m-1, 1));
- X(H, m-1) += A(t, H, 0);
- X(H, H, iota(l-1)) += A(t, H, H, iota(l-1, 1));
- X(H, H, l-1) += A(t, H, H, 0);
- // Y←(¯1⌽[0]A[T;;;;])+(¯1⌽[1]A[T;;;;])+(¯1⌽[2]A[T;;;;])
- Y(iota(n-1, 1)) = A(t, iota(n-1));
- Y(0) = A(t, n-1);
- Y(H, iota(m-1, 1)) += A(t, H, iota(m-1));
- Y(H, 0) += A(t, H, m-1);
- Y(H, H, iota(l-1, 1)) += A(t, H, H, iota(l-1));
- Y(H, H, 0) += A(t, H, H, l-1);
- A(t+1) = X + Y - A(t-1) - 4*A(t);
- }
- auto time_A = Benchmark::clock::now()-t0;
- // FIXME should try to traverse the array once, e.g. explode() = pack(...), but we need to wrap around boundaries.
- auto diff = [&DA, &A, &delta](auto k_, real factor)
- {
- constexpr int k = k_;
- const int o = DA.len(k);
- if (o>=2) {
- DA(HH<k>, iota(o-2, 1), HH<4-k>, k) = (A(HH<k>, iota(o-2, 2)) - A(HH<k>, iota(o-2, 0)));
- DA(HH<k>, 0, HH<4-k>, k) = (A(HH<k>, 1) - A(HH<k>, o-1));
- DA(HH<k>, o-1, HH<4-k>, k) = (A(HH<k>, 0) - A(HH<k>, o-2));
- DA(HH<5>, k) *= factor;
- }
- };
- t0 = Benchmark::clock::now();
- diff(int_c<0>(), +1/(2*delta));
- diff(int_c<1>(), -1/(2*delta));
- diff(int_c<2>(), -1/(2*delta));
- diff(int_c<3>(), -1/(2*delta));
- auto time_DA = Benchmark::clock::now()-t0;
- F = ra::transpose<0, 1, 2, 3, 5, 4>(DA) - DA;
- // abuse shape matching to reduce last axis.
- divA += ra::transpose<0, 1, 2, 3, 4, 4>(DA);
- tr.info("Lorentz test max div A (1)").test_eq(0., amax(divA));
- // an alternative without a temporary.
- tr.info("Lorentz test max div A (2)")
- .test_eq(0., amax(map([](auto && a) { return sum(a); },
- iter<1>(ra::transpose<0, 1, 2, 3, 4, 4>(DA)))));
- tr.quiet().test_eq(0.3039588939177449, F(19, 0, 0, 0, 2, 1));
- auto show = [&tr, &delta](char const * name, int t, auto && F)
- {
- tr.quiet().test(amin(F)>=-1);
- tr.quiet().test(amax(F)<=+1);
- cout << name << "(0)=" << std::setprecision(10) << std::setw(12) << F(0) << " t=" << (t*delta) << ":\n";
- for_each([](auto && F) { cout << std::string(int(round(20*(clamp(F, -1., 1.)+1))), ' ') << "*\n"; }, F);
- };
- for (int t=0; t<o; ++t) {
- show("Ey", t, F(t, H, 0, 0, 2, 0));
- show("Bz", t, F(t, H, 0, 0, 2, 1));
- std::this_thread::sleep_for(std::chrono::milliseconds(50));
- cout << endl;
- }
- cout << Benchmark::toseconds(time_A)/1e-6 << " μs time_A" << endl;
- cout << Benchmark::toseconds(time_DA)/1e-6 << " μs time_DA" << endl;
- return tr.summary();
- }
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