/** * @file MultiNewton.cpp * * Damped Newton solver for 1D multi-domain problems */ /* * Copyright 2001 California Institute of Technology */ #include using namespace std; #include "cantera/oneD/MultiNewton.h" #include "cantera/base/ctexceptions.h" #include "cantera/base/vec_functions.h" #include "cantera/base/stringUtils.h" #include #include #include using namespace std; namespace Cantera { // unnamed-namespace for local helpers namespace { class Indx { public: Indx(size_t nv, size_t np) : m_nv(nv), m_np(np) {} size_t m_nv, m_np; size_t operator()(size_t m, size_t j) { return j*m_nv + m; } }; /** * Return a damping coefficient that keeps the solution after taking one * Newton step between specified lower and upper bounds. This function only * considers one domain. */ doublereal bound_step(const doublereal* x, const doublereal* step, Domain1D& r, int loglevel) { char buf[100]; size_t np = r.nPoints(); size_t nv = r.nComponents(); Indx index(nv, np); doublereal above, below, val, newval; size_t m, j; doublereal fbound = 1.0; bool wroteTitle = false; for (m = 0; m < nv; m++) { above = r.upperBound(m); below = r.lowerBound(m); for (j = 0; j < np; j++) { val = x[index(m,j)]; if (loglevel > 0) { if (val > above + 1.0e-12 || val < below - 1.0e-12) { sprintf(buf, "domain %s: %20s(%s) = %10.3e (%10.3e, %10.3e)\n", int2str(r.domainIndex()).c_str(), r.componentName(m).c_str(), int2str(j).c_str(), val, below, above); writelog(string("\nERROR: solution out of bounds.\n")+buf); } } newval = val + step[index(m,j)]; if (newval > above) { fbound = std::max(0.0, std::min(fbound, (above - val)/(newval - val))); } else if (newval < below) { fbound = std::min(fbound, (val - below)/(val - newval)); } if (loglevel > 1 && (newval > above || newval < below)) { if (!wroteTitle) { writelog("\nNewton step takes solution out of bounds.\n\n"); sprintf(buf," %12s %12s %4s %10s %10s %10s %10s\n", "domain","component","pt","value","step","min","max"); wroteTitle = true; writelog(buf); } sprintf(buf, " %4s %12s %4s %10.3e %10.3e %10.3e %10.3e\n", int2str(r.domainIndex()).c_str(), r.componentName(m).c_str(), int2str(j).c_str(), val, step[index(m,j)], below, above); writelog(buf); } } } return fbound; } /** * This function computes the square of a weighted norm of a step * vector for one domain. * * @param x Solution vector for this domain. * @param step Newton step vector for this domain. * @param r Object representing the domain. Used to get tolerances, * number of components, and number of points. * * The return value is * \f[ * \sum_{n,j} \left(\frac{s_{n,j}}{w_n}\right)^2 * \f] * where the error weight for solution component \f$n\f$ is given by * \f[ * w_n = \epsilon_{r,n} \frac{\sum_j |x_{n,j}|}{J} + \epsilon_{a,n}. * \f] * Here \f$\epsilon_{r,n} \f$ is the relative error tolerance for * component n, and multiplies the average magnitude of * solution component n in the domain. The second term, * \f$\epsilon_{a,n}\f$, is the absolute error tolerance for component * n. * */ doublereal norm_square(const doublereal* x, const doublereal* step, Domain1D& r) { doublereal f, ewt, esum, sum = 0.0; size_t n, j; doublereal f2max = 0.0; size_t nv = r.nComponents(); size_t np = r.nPoints(); for (n = 0; n < nv; n++) { esum = 0.0; for (j = 0; j < np; j++) { esum += fabs(x[nv*j + n]); } ewt = r.rtol(n)*esum/np + r.atol(n); for (j = 0; j < np; j++) { f = step[nv*j + n]/ewt; sum += f*f; if (f*f > f2max) { f2max = f*f; } } } return sum; } } // end unnamed-namespace //----------------------------------------------------------- // constants //----------------------------------------------------------- const string dashedline = "-----------------------------------------------------------------"; const doublereal DampFactor = sqrt(2.0); const size_t NDAMP = 7; //----------------------------------------------------------- // MultiNewton methods //----------------------------------------------------------- MultiNewton::MultiNewton(int sz) : m_maxAge(5) { m_n = sz; m_elapsed = 0.0; } MultiNewton::~MultiNewton() { for (size_t i = 0; i < m_workarrays.size(); i++) { delete[] m_workarrays[i]; } } /** * Prepare for a new solution vector length. */ void MultiNewton::resize(size_t sz) { m_n = sz; for (size_t i = 0; i < m_workarrays.size(); i++) { delete[] m_workarrays[i]; } m_workarrays.clear(); } /** * Compute the weighted 2-norm of 'step'. */ doublereal MultiNewton::norm2(const doublereal* x, const doublereal* step, OneDim& r) const { doublereal f, sum = 0.0;//, fmx = 0.0; size_t nd = r.nDomains(); for (size_t n = 0; n < nd; n++) { f = norm_square(x + r.start(n), step + r.start(n), r.domain(n)); sum += f; } sum /= r.size(); return sqrt(sum); } /** * Compute the undamped Newton step. The residual function is * evaluated at x, but the Jacobian is not recomputed. */ void MultiNewton::step(doublereal* x, doublereal* step, OneDim& r, MultiJac& jac, int loglevel) { size_t iok; size_t sz = r.size(); r.eval(npos, x, step); #undef DEBUG_STEP #ifdef DEBUG_STEP vector_fp ssave(sz, 0.0); for (size_t n = 0; n < sz; n++) { step[n] = -step[n]; ssave[n] = step[n]; } #else for (size_t n = 0; n < sz; n++) { step[n] = -step[n]; } #endif iok = jac.solve(step, step); // if iok is non-zero, then solve failed if (iok != 0) { iok--; size_t nd = r.nDomains(); size_t n; for (n = nd-1; n != npos; n--) if (iok >= r.start(n)) { break; } Domain1D& dom = r.domain(n); size_t offset = iok - r.start(n); size_t pt = offset/dom.nComponents(); size_t comp = offset - pt*dom.nComponents(); throw CanteraError("MultiNewton::step", "Jacobian is singular for domain "+ dom.id() + ", component " +dom.componentName(comp)+" at point " +int2str(pt)+"\n(Matrix row " +int2str(iok)+") \nsee file bandmatrix.csv\n"); } else if (int(iok) < 0) throw CanteraError("MultiNewton::step", "iok = "+int2str(iok)); #ifdef DEBUG_STEP bool ok = false; Domain1D* d; if (!ok) { for (size_t n = 0; n < sz; n++) { d = r.pointDomain(n); int nvd = d->nComponents(); int pt = (n - d->loc())/nvd; cout << "step: " << pt << " " << r.pointDomain(n)->componentName(n - d->loc() - nvd*pt) << " " << x[n] << " " << ssave[n] << " " << step[n] << endl; } } #endif } /** * Return the factor by which the undamped Newton step 'step0' * must be multiplied in order to keep all solution components in * all domains between their specified lower and upper bounds. */ doublereal MultiNewton::boundStep(const doublereal* x0, const doublereal* step0, const OneDim& r, int loglevel) { doublereal fbound = 1.0; for (size_t i = 0; i < r.nDomains(); i++) { fbound = std::min(fbound, bound_step(x0 + r.start(i), step0 + r.start(i), r.domain(i), loglevel)); } return fbound; } /** * On entry, step0 must contain an undamped Newton step for the * solution x0. This method attempts to find a damping coefficient * such that the next undamped step would have a norm smaller than * that of step0. If successful, the new solution after taking the * damped step is returned in x1, and the undamped step at x1 is * returned in step1. */ int MultiNewton::dampStep(const doublereal* x0, const doublereal* step0, doublereal* x1, doublereal* step1, doublereal& s1, OneDim& r, MultiJac& jac, int loglevel, bool writetitle) { // write header if (loglevel > 0 && writetitle) { writelog("\n\nDamped Newton iteration:\n"); writelog(dashedline); sprintf(m_buf,"\n%s %9s %9s %9s %9s %9s %5s %5s\n", "m","F_damp","F_bound","log10(ss)", "log10(s0)","log10(s1)","N_jac","Age"); writelog(m_buf); writelog(dashedline+"\n"); } // compute the weighted norm of the undamped step size step0 doublereal s0 = norm2(x0, step0, r); // compute the multiplier to keep all components in bounds doublereal fbound = boundStep(x0, step0, r, loglevel-1); // if fbound is very small, then x0 is already close to the // boundary and step0 points out of the allowed domain. In // this case, the Newton algorithm fails, so return an error // condition. if (fbound < 1.e-10) { writelog("\nAt limits.\n", loglevel); return -3; } //-------------------------------------------- // Attempt damped step //-------------------------------------------- // damping coefficient starts at 1.0 doublereal damp = 1.0; doublereal ff; size_t m; for (m = 0; m < NDAMP; m++) { ff = fbound*damp; // step the solution by the damped step size for (size_t j = 0; j < m_n; j++) { x1[j] = ff*step0[j] + x0[j]; } // compute the next undamped step that would result if x1 // is accepted step(x1, step1, r, jac, loglevel-1); // compute the weighted norm of step1 s1 = norm2(x1, step1, r); // write log information if (loglevel > 0) { doublereal ss = r.ssnorm(x1,step1); sprintf(m_buf,"\n%s %9.5f %9.5f %9.5f %9.5f %9.5f %4d %d/%d", int2str(m).c_str(), damp, fbound, log10(ss+SmallNumber), log10(s0+SmallNumber), log10(s1+SmallNumber), jac.nEvals(), jac.age(), m_maxAge); writelog(m_buf); } // if the norm of s1 is less than the norm of s0, then // accept this damping coefficient. Also accept it if this // step would result in a converged solution. Otherwise, // decrease the damping coefficient and try again. if (s1 < 1.0 || s1 < s0) { break; } damp /= DampFactor; } // If a damping coefficient was found, return 1 if the // solution after stepping by the damped step would represent // a converged solution, and return 0 otherwise. If no damping // coefficient could be found, return -2. if (m < NDAMP) { if (s1 > 1.0) { return 0; } else { return 1; } } else { return -2; } } /** * Find the solution to F(X) = 0 by damped Newton iteration. On * entry, x0 contains an initial estimate of the solution. On * successful return, x1 contains the converged solution. */ int MultiNewton::solve(doublereal* x0, doublereal* x1, OneDim& r, MultiJac& jac, int loglevel) { clock_t t0 = clock(); int m = 0; bool forceNewJac = false; doublereal s1=1.e30; doublereal* x = getWorkArray(); doublereal* stp = getWorkArray(); doublereal* stp1 = getWorkArray(); copy(x0, x0 + m_n, x); bool frst = true; doublereal rdt = r.rdt(); int j0 = jac.nEvals(); int nJacReeval = 0; while (1 > 0) { // Check whether the Jacobian should be re-evaluated. if (jac.age() > m_maxAge) { writelog("\nMaximum Jacobian age reached ("+int2str(m_maxAge)+")\n", loglevel); forceNewJac = true; } if (forceNewJac) { r.eval(npos, x, stp, 0.0, 0); jac.eval(x, stp, 0.0); jac.updateTransient(rdt, DATA_PTR(r.transientMask())); forceNewJac = false; } // compute the undamped Newton step step(x, stp, r, jac, loglevel-1); // increment the Jacobian age jac.incrementAge(); // damp the Newton step m = dampStep(x, stp, x1, stp1, s1, r, jac, loglevel-1, frst); if (loglevel == 1 && m >= 0) { if (frst) { sprintf(m_buf,"\n\n %10s %10s %5s ", "log10(ss)","log10(s1)","N_jac"); writelog(m_buf); sprintf(m_buf,"\n ------------------------------------"); writelog(m_buf); } doublereal ss = r.ssnorm(x, stp); sprintf(m_buf,"\n %10.4f %10.4f %d ", log10(ss),log10(s1),jac.nEvals()); writelog(m_buf); } frst = false; // Successful step, but not converged yet. Take the damped // step, and try again. if (m == 0) { copy(x1, x1 + m_n, x); } // convergence else if (m == 1) { break; } // If dampStep fails, first try a new Jacobian if an old // one was being used. If it was a new Jacobian, then // return -1 to signify failure. else if (m < 0) { if (jac.age() > 1) { forceNewJac = true; if (nJacReeval > 3) { break; } nJacReeval++; writelog("\nRe-evaluating Jacobian, since no damping " "coefficient\ncould be found with this Jacobian.\n", loglevel); } else { break; } } } if (m < 0) { copy(x, x + m_n, x1); } if (m > 0 && jac.nEvals() == j0) { m = 100; } releaseWorkArray(x); releaseWorkArray(stp); releaseWorkArray(stp1); m_elapsed += (clock() - t0)/(1.0*CLOCKS_PER_SEC); return m; } /** * Get a pointer to an array of length m_n for temporary work * space. */ doublereal* MultiNewton::getWorkArray() { doublereal* w = 0; if (!m_workarrays.empty()) { w = m_workarrays.back(); m_workarrays.pop_back(); } else { w = new doublereal[m_n]; } return w; } /** * Release a work array by pushing its pointer onto the stack of * available arrays. */ void MultiNewton::releaseWorkArray(doublereal* work) { m_workarrays.push_back(work); } } // end namespace Cantera