\item {\em Restraints}: position restraints, angle restraints,
distance restraints, orientation restraints and dihedral restraints, all
based on fixed lists.
+%\ifthenelse{\equal{\gmxlite}{1}}{}{
+\item {\em Applied Forces}:
+externally applied forces, see \chref{special}.
+%}
\end{enumerate}
\section{Non-bonded interactions}
pages = {1986--1994}
}
+@article{Caleman2008a,
+ author = {Caleman, C and van der Spoel, D},
+ title = {{Picosecond Melting of Ice by an Infrared Laser Pulse - A simulation
+ study}},
+ journal = {Angew. Chem., Int. Ed. Engl.},
+ year = {2008},
+ volume = {47},
+ pages = {1417--1420}
+}
+
@article{Wolf2010,
author = {Wolf, M.G. and Hoefling, M. and Aponte-Santamar\'{i}a, C. and Grubm\"{u}ller, H. and Groenhof, G.},
title = {{g\_membed}: Efficient insertion of a membrane protein into an equilibrated lipid bilayer with minimal perturbation},
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+&
local rotation axis of the slab and the Gaussian-weighted positions.
+\section{\normindex{Electric fields}}
+A pulsed and oscillating electric field can be applied according to:
+\begin{equation}
+E(t) = E_0 \exp\left[-\frac{(t-t_0)^2}{2\sigma^2}\right]\cos\left[\omega (t-t_0)\right]
+\label{eq_efield}
+\end{equation}
+where $E_0$ is the field strength, the angular frequency \mbox{$\omega = 2\pi c/\lambda$}, $t_0$ is
+the time at of the peak in the field strength and $\sigma$ is the with
+of the pulse. Special cases occur when $\sigma$ = 0 (non-pulsed field)
+and for $\omega$ is 0 (static field).
+
+This simulated \normindex{laser}-pulse was applied to
+simulations of melting ice~\cite{Caleman2008a}. A pulsed electric field may
+look ike Fig.~\ref{fig:field}. In the supporting
+information of that paper the impact of an applied electric field on a
+system under periodic boundary conditions is analyzed. It is described
+that the effective electric field under PBC is larger than the applied
+field, by a factor depending on the size of the box and the dielectric
+properties of molecules in the box. For a system with static dielectric
+properties this factor can be corrected for. But for a system where
+the dielectric varies over time, for example a membrane protein with
+a pore that opens and closes during the simulatippn, this way of applying
+an electric field is not useful. In such cases one can use the computational
+electrophysiology protocol described in the next section (\secref{compel}).
+\begin{figure}[ht]
+\centerline{\includegraphics[width=8cm]{plots/field}}
+\caption {A simulated laser pulse in GROMACS.}
+\label{fig:field}
+\end{figure}
+
+Electric fields are applied when the following options are specified
+in the {\tt grompp.mdp} file. You specify, in order, $E_0$, $\omega$,
+$t_0$ and $\sigma$:
+\begin{verbatim}
+ElectricField-x = 0.04 0 0 0
+\end{verbatim}
+yields a static field with $E_0$ = 0.04 V/nm in the X-direction. In contrast,
+\begin{verbatim}
+ElectricField-x = 2.0 150 5 0
+\end{verbatim}
+yields an oscillating electric field with $E_0$ = 2 V/nm, $\omega$ = 150/ps and
+$t_0$ = 5 ps. Finally
+\begin{verbatim}
+ElectricField-x = 2.0 150 5 1
+\end{verbatim}
+yields an pulsed-oscillating electric field with $E_0$ = 2 V/nm, $\omega$ = 150/ps and
+$t_0$ = 5 ps and $\sigma$ = 1 ps. Read more in ref.~\cite{Caleman2008a}.
+Note that the input file format is changed from the undocumented older
+version. A figure like Fig.~\ref{fig:field} may be produced by passing
+the {\tt -field} option to {\tt gmx mdrun}.
+
+
\section{\normindex{Computational Electrophysiology}}
\label{sec:compel}
add_subdirectory(gmxlib)
add_subdirectory(mdlib)
+add_subdirectory(applied-forces)
add_subdirectory(listed-forces)
add_subdirectory(commandline)
add_subdirectory(domdec)
--- /dev/null
+#
+# This file is part of the GROMACS molecular simulation package.
+#
+# Copyright (c) 2015,2016, by the GROMACS development team, led by
+# Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
+# and including many others, as listed in the AUTHORS file in the
+# top-level source directory and at http://www.gromacs.org.
+#
+# GROMACS 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 2.1
+# of the License, or (at your option) any later version.
+#
+# GROMACS is distributed in the hope that it will be useful,
+# but WITHOUT ANY WARRANTY; without even the implied warranty of
+# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
+# Lesser General Public License for more details.
+#
+# You should have received a copy of the GNU Lesser General Public
+# License along with GROMACS; if not, see
+# http://www.gnu.org/licenses, or write to the Free Software Foundation,
+# Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+#
+# If you want to redistribute modifications to GROMACS, please
+# consider that scientific software is very special. Version
+# control is crucial - bugs must be traceable. We will be happy to
+# consider code for inclusion in the official distribution, but
+# derived work must not be called official GROMACS. Details are found
+# in the README & COPYING files - if they are missing, get the
+# official version at http://www.gromacs.org.
+#
+# To help us fund GROMACS development, we humbly ask that you cite
+# the research papers on the package. Check out http://www.gromacs.org.
+
+gmx_add_libgromacs_sources(
+ electricfield.cpp
+ )
+
+if (BUILD_TESTING)
+ add_subdirectory(tests)
+endif()
--- /dev/null
+/*
+ * This file is part of the GROMACS molecular simulation package.
+ *
+ * Copyright (c) 2015,2016, by the GROMACS development team, led by
+ * Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
+ * and including many others, as listed in the AUTHORS file in the
+ * top-level source directory and at http://www.gromacs.org.
+ *
+ * GROMACS 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 2.1
+ * of the License, or (at your option) any later version.
+ *
+ * GROMACS is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
+ * Lesser General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public
+ * License along with GROMACS; if not, see
+ * http://www.gnu.org/licenses, or write to the Free Software Foundation,
+ * Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+ *
+ * If you want to redistribute modifications to GROMACS, please
+ * consider that scientific software is very special. Version
+ * control is crucial - bugs must be traceable. We will be happy to
+ * consider code for inclusion in the official distribution, but
+ * derived work must not be called official GROMACS. Details are found
+ * in the README & COPYING files - if they are missing, get the
+ * official version at http://www.gromacs.org.
+ *
+ * To help us fund GROMACS development, we humbly ask that you cite
+ * the research papers on the package. Check out http://www.gromacs.org.
+ */
+/*! \internal \file
+ * \brief
+ * Declares data structure and utilities for electric fields
+ *
+ * \author David van der Spoel <david.vanderspoel@icm.uu.se>
+ * \ingroup module_applied_forces
+ */
+#include "gmxpre.h"
+
+#include "electricfield.h"
+
+#include <cmath>
+
+#include "gromacs/commandline/filenm.h"
+#include "gromacs/fileio/gmxfio.h"
+#include "gromacs/fileio/gmxfio-xdr.h"
+#include "gromacs/fileio/readinp.h"
+#include "gromacs/fileio/warninp.h"
+#include "gromacs/fileio/xvgr.h"
+#include "gromacs/gmxlib/network.h"
+#include "gromacs/math/units.h"
+#include "gromacs/math/vec.h"
+#include "gromacs/mdtypes/commrec.h"
+#include "gromacs/mdtypes/forcerec.h"
+#include "gromacs/mdtypes/inputrec.h"
+#include "gromacs/mdtypes/mdatom.h"
+#include "gromacs/utility/compare.h"
+#include "gromacs/utility/exceptions.h"
+#include "gromacs/utility/fatalerror.h"
+#include "gromacs/utility/pleasecite.h"
+#include "gromacs/utility/strconvert.h"
+#include "gromacs/utility/stringutil.h"
+#include "gromacs/utility/txtdump.h"
+
+namespace gmx
+{
+
+namespace
+{
+
+/*! \internal
+ * \brief Declaration of storage unit for fields
+ */
+class ElectricFieldData
+{
+ public:
+ ElectricFieldData() : a_(0), omega_(0), t0_(0), sigma_(0)
+ {
+ }
+
+ /*! \brief Evaluates this field component at given time.
+ *
+ * \param[in] t The time to evualate at
+ * \return The electric field
+ */
+ real evaluate(real t) const
+ {
+ if (sigma_ > 0)
+ {
+ return a_ * (std::cos(omega_*(t-t0_))
+ * std::exp(-square(t-t0_)/(2.0*square(sigma_))));
+ }
+ else
+ {
+ return a_ * std::cos(omega_*t);
+ }
+ }
+
+ /*! \brief Initiate the field values
+ *
+ * \param[in] a Amplitude
+ * \param[in] omega Frequency
+ * \param[in] t0 Peak of the pulse
+ * \param[in] sigma Width of the pulse
+ */
+ void setField(real a, real omega, real t0, real sigma)
+ {
+ a_ = a;
+ omega_ = omega;
+ t0_ = t0;
+ sigma_ = sigma;
+ }
+
+ //! Return the amplitude
+ real a() const { return a_; }
+ //! Return the frequency
+ real omega() const { return omega_; }
+ //! Return the time for the peak of the pulse
+ real t0() const { return t0_; }
+ //! Return the width of the pulse (0 means inifinite)
+ real sigma() const { return sigma_; }
+
+ private:
+ //! Coeffient (V / nm)
+ real a_;
+ //! Frequency (1/ps)
+ real omega_;
+ //! Central time point (ps) for pulse
+ real t0_;
+ //! Width of pulse (ps, if zero there is no pulse)
+ real sigma_;
+};
+
+/*! \internal
+ * \brief Describe time dependent electric field
+ *
+ * Class that implements a force to be evaluated in mdrun.
+ * The electric field can be pulsed and oscillating, simply
+ * oscillating, or static, in each of X,Y,Z directions.
+ */
+class ElectricField : public IInputRecExtension, public IForceProvider
+{
+ public:
+ ElectricField() : fpField_(nullptr) {}
+
+ // From IInputRecExtension
+ virtual void doTpxIO(t_fileio *fio, bool bRead);
+ virtual void readMdp(int *ninp_p, t_inpfile **inp_p, warninp *wi);
+ virtual void broadCast(const t_commrec *cr);
+ virtual void compare(FILE *fp,
+ const IInputRecExtension *field2,
+ real reltol,
+ real abstol);
+ virtual void printParameters(FILE *fp, int indent);
+ virtual void initOutput(FILE *fplog, int nfile, const t_filenm fnm[],
+ bool bAppendFiles, const gmx_output_env_t *oenv);
+ virtual void finishOutput();
+ virtual void initForcerec(t_forcerec *fr);
+
+ // From IForceProvider
+ virtual void calculateForces(const t_commrec *cr,
+ const t_mdatoms *atoms,
+ PaddedRVecVector *force,
+ double t);
+
+ private:
+ /*! \brief Extract relevant fields from an mdp file
+ *
+ * \todo Remove this when new tests are in place.
+ * \param[in] dim The direction XX, YY, or ZZ
+ * \param[in] staticField Static components of the field
+ * \param[in] dynamicField Dynamic components of the field
+ * \param[in] wi Warning control structure
+ */
+ void decodeMdp(int dim,
+ const char *staticField,
+ const char *dynamicField,
+ warninp *wi);
+
+ //! Return whether or not to apply a field
+ bool isActive() const;
+
+ /*! \brief Add a component to the electric field
+ *
+ * The electric field has three spatial dimensions that are
+ * added to the data structure one at a time.
+ * \param[in] dim Dimension, XX, YY, ZZ (0, 1, 2)
+ * \param[in] a Amplitude of the field in V/nm
+ * \param[in] omega Frequency (1/ps)
+ * \param[in] t0 Time of pulse peak (ps)
+ * \param[in] sigma Width of peak (ps)
+ */
+ void setFieldTerm(int dim, real a, real omega, real t0, real sigma);
+
+ /*! \brief Return the field strength
+ *
+ * \param[in] dim The spatial direction
+ * \param[in] t The time (ps)
+ * \return The field strength in V/nm units
+ */
+ real field(int dim, real t) const;
+
+ /*! \brief Return amplitude of field
+ *
+ * \param[in] dim Direction of the field (XX, YY, ZZ)
+ * \return Amplitude of the field
+ */
+ real a(int dim) const { return efield_[dim].a(); }
+ /*! \brief Return frequency of field (1/ps)
+ *
+ * \param[in] dim Direction of the field (XX, YY, ZZ)
+ * \return Frequency of the field
+ */
+ real omega(int dim) const { return efield_[dim].omega(); }
+ /*! \brief Return time of pulse peak
+ *
+ * \param[in] dim Direction of the field (XX, YY, ZZ)
+ * \return Time of pulse peak
+ */
+ real t0(int dim) const { return efield_[dim].t0(); }
+ /*! \brief Return width of the pulse
+ *
+ * \param[in] dim Direction of the field (XX, YY, ZZ)
+ * \return Width of the pulse
+ */
+ real sigma(int dim) const { return efield_[dim].sigma(); }
+
+ /*! \brief Print the field components to a file
+ *
+ * \param[in] t The time
+ * Will throw and exit with fatal error if file is not open.
+ */
+ void printComponents(double t) const;
+
+ //! The field strength in each dimension
+ ElectricFieldData efield_[DIM];
+ //! File pointer for electric field
+ FILE *fpField_;
+};
+
+void ElectricField::doTpxIO(t_fileio *fio, bool bRead)
+{
+ // The content of the tpr file for this feature has
+ // been the same since gromacs 4.0 that was used for
+ // developing.
+ for (int j = 0; (j < DIM); j++)
+ {
+ int n = 0, nt = 0;
+ if (!bRead)
+ {
+ n = 1;
+ if (omega(j) != 0 || sigma(j) != 0 || t0(j) != 0)
+ {
+ nt = 1;
+ }
+ }
+ gmx_fio_do_int(fio, n);
+ gmx_fio_do_int(fio, nt);
+ std::vector<real> aa, phi, at, phit;
+ if (!bRead)
+ {
+ aa.push_back(a(j));
+ phi.push_back(t0(j));
+ at.push_back(omega(j));
+ phit.push_back(sigma(j));
+ }
+ else
+ {
+ aa.resize(n+1);
+ phi.resize(nt+1);
+ at.resize(nt+1);
+ phit.resize(nt+1);
+ }
+ gmx_fio_ndo_real(fio, aa.data(), n);
+ gmx_fio_ndo_real(fio, phi.data(), n);
+ gmx_fio_ndo_real(fio, at.data(), nt);
+ gmx_fio_ndo_real(fio, phit.data(), nt);
+ if (bRead && n > 0)
+ {
+ setFieldTerm(j, aa[0], at[0], phi[0], phit[0]);
+ if (n > 1 || nt > 1)
+ {
+ gmx_fatal(FARGS, "Can not handle tpr files with more than one electric field term per direction.");
+ }
+ }
+ }
+}
+
+void ElectricField::readMdp(int *ninp_p, t_inpfile **inp_p, warninp_t wi)
+{
+ // Old style MDP. Will be removed later.
+ char efield_x[STRLEN], efield_xt[STRLEN], efield_y[STRLEN],
+ efield_yt[STRLEN], efield_z[STRLEN], efield_zt[STRLEN];
+ efield_x[0] = '\0';
+ efield_xt[0] = '\0';
+ efield_y[0] = '\0';
+ efield_yt[0] = '\0';
+ efield_z[0] = '\0';
+ efield_zt[0] = '\0';
+
+ const char *tmp;
+ int ninp = *ninp_p;
+ t_inpfile *inp = *inp_p;
+
+ CCTYPE("Electric fields");
+ // Old style inputs for backward compatibility
+ STYPE ("E-x", efield_x, NULL);
+ STYPE ("E-xt", efield_xt, NULL);
+ STYPE ("E-y", efield_y, NULL);
+ STYPE ("E-yt", efield_yt, NULL);
+ STYPE ("E-z", efield_z, NULL);
+ STYPE ("E-zt", efield_zt, NULL);
+
+ *ninp_p = ninp;
+ *inp_p = inp;
+
+ // Extract mdp parameters
+ decodeMdp(XX, efield_x, efield_xt, wi);
+ decodeMdp(YY, efield_y, efield_yt, wi);
+ decodeMdp(ZZ, efield_z, efield_zt, wi);
+}
+
+void ElectricField::decodeMdp(int dim,
+ const char *staticField,
+ const char *dynamicField,
+ warninp_t wi)
+{
+ char warn_buf[STRLEN];
+ // TODO: Better context for the exceptions from the converters (possibly
+ // also convert them to warning_errors).
+ std::vector<std::string> sx = splitString(staticField);
+ if (sx.empty())
+ {
+ return;
+ }
+ // Old style for backwards compatibility
+ int n = fromString<int>(sx[0]);
+ if (n <= 0)
+ {
+ return;
+ }
+ if (n != 1)
+ {
+ sprintf(warn_buf, "Only one electric field term supported for each dimension");
+ warning_error(wi, warn_buf);
+ }
+ if (sx.size() != 3)
+ {
+ sprintf(warn_buf, "Expected exactly one electric field amplitude value");
+ warning_error(wi, warn_buf);
+ }
+ real E0 = fromString<real>(sx[1]);
+
+ std::vector<std::string> sxt = splitString(dynamicField);
+ if (!sxt.empty())
+ {
+ real omega = 0, t0 = 0, sigma = 0;
+ int n = fromString<int>(sxt[0]);
+ switch (n)
+ {
+ case 1:
+ if (sxt.size() != 3)
+ {
+ sprintf(warn_buf, "Please specify 1 omega 0 for non-pulsed fields");
+ warning_error(wi, warn_buf);
+ }
+ omega = fromString<real>(sxt[1]);
+ break;
+ case 3:
+ if (sxt.size() != 7)
+ {
+ sprintf(warn_buf, "Please specify 1 omega 0 t0 0 sigma 0 for pulsed fields");
+ warning_error(wi, warn_buf);
+ }
+ omega = fromString<real>(sxt[1]);
+ t0 = fromString<real>(sxt[3]);
+ sigma = fromString<real>(sxt[5]);
+ break;
+ default:
+ sprintf(warn_buf, "Incomprehensible input for electric field");
+ warning_error(wi, warn_buf);
+ }
+ setFieldTerm(dim, E0, omega, t0, sigma);
+ }
+ else
+ {
+ setFieldTerm(dim, E0, 0, 0, 0);
+ }
+}
+
+void ElectricField::broadCast(const t_commrec *cr)
+{
+ rvec a1, omega1, sigma1, t01;
+
+ if (MASTER(cr))
+ {
+ // Load the parameters read from tpr into temp vectors
+ for (int m = 0; m < DIM; m++)
+ {
+ a1[m] = a(m);
+ omega1[m] = omega(m);
+ sigma1[m] = sigma(m);
+ t01[m] = t0(m);
+ }
+ }
+ // Broadcasting the parameters
+ gmx_bcast(DIM*sizeof(a1[0]), a1, cr);
+ gmx_bcast(DIM*sizeof(omega1[0]), omega1, cr);
+ gmx_bcast(DIM*sizeof(t01[0]), t01, cr);
+ gmx_bcast(DIM*sizeof(sigma1[0]), sigma1, cr);
+
+ // And storing them locally
+ if (!MASTER(cr))
+ {
+ for (int m = 0; m < DIM; m++)
+ {
+ setFieldTerm(m, a1[m], omega1[m], t01[m], sigma1[m]);
+ }
+ }
+}
+
+void ElectricField::initOutput(FILE *fplog, int nfile, const t_filenm fnm[],
+ bool bAppendFiles, const gmx_output_env_t *oenv)
+{
+ if (isActive())
+ {
+ please_cite(fplog, "Caleman2008a");
+
+ // Optional outpuf file showing the field, see manual.
+ if (opt2bSet("-field", nfile, fnm))
+ {
+ if (bAppendFiles)
+ {
+ fpField_ = gmx_fio_fopen(opt2fn("-field", nfile, fnm), "a+");
+ }
+ else
+ {
+ fpField_ = xvgropen(opt2fn("-field", nfile, fnm),
+ "Applied electric field", "Time (ps)",
+ "E (V/nm)", oenv);
+ }
+ }
+ }
+}
+
+void ElectricField::finishOutput()
+{
+ if (fpField_ != nullptr)
+ {
+ // This is opened sometimes with xvgropen, sometimes with
+ // gmx_fio_fopen, so we use the least common denominator for closing.
+ gmx_fio_fclose(fpField_);
+ fpField_ = nullptr;
+ }
+}
+
+void ElectricField::initForcerec(t_forcerec *fr)
+{
+ if (isActive())
+ {
+ fr->bF_NoVirSum = TRUE;
+ fr->efield = this;
+ }
+}
+
+void ElectricField::printParameters(FILE *fp, int indent)
+{
+ const char *const dimension[DIM] = { "X", "Y", "Z" };
+ indent = pr_title(fp, indent, "ElectricField");
+ for (int m = 0; m < DIM; m++)
+ {
+ pr_indent(fp, indent);
+ fprintf(fp, "-%s E0 = %g omega = %g t0 = %g sigma = %g\n",
+ dimension[m], a(m), omega(m), t0(m), sigma(m));
+ }
+}
+
+void ElectricField::setFieldTerm(int dim, real a, real omega, real t0, real sigma)
+{
+ range_check(dim, 0, DIM);
+ efield_[dim].setField(a, omega, t0, sigma);
+}
+
+real ElectricField::field(int dim, real t) const
+{
+ return efield_[dim].evaluate(t);
+}
+
+bool ElectricField::isActive() const
+{
+ return (efield_[XX].a() != 0 ||
+ efield_[YY].a() != 0 ||
+ efield_[ZZ].a() != 0);
+}
+
+void ElectricField::compare(FILE *fp,
+ const IInputRecExtension *other,
+ real reltol,
+ real abstol)
+{
+ GMX_ASSERT(dynamic_cast<const ElectricField *>(other) != nullptr,
+ "Invalid other type");
+ const ElectricField *f2 = static_cast<const ElectricField *>(other);
+ for (int m = 0; (m < DIM); m++)
+ {
+ char buf[256];
+
+ sprintf(buf, "inputrec->field[%d]", m);
+ cmp_real(fp, buf, -1, a(m), f2->a(m), reltol, abstol);
+ cmp_real(fp, buf, -1, omega(m), f2->omega(m), reltol, abstol);
+ cmp_real(fp, buf, -1, t0(m), f2->t0(m), reltol, abstol);
+ cmp_real(fp, buf, -1, sigma(m), f2->sigma(m), reltol, abstol);
+ }
+}
+
+void ElectricField::printComponents(double t) const
+{
+ fprintf(fpField_, "%10g %10g %10g %10g\n", t,
+ field(XX, t), field(YY, t), field(ZZ, t));
+}
+
+void ElectricField::calculateForces(const t_commrec *cr,
+ const t_mdatoms *mdatoms,
+ PaddedRVecVector *force,
+ double t)
+{
+ if (isActive())
+ {
+ rvec *f = as_rvec_array(force->data());
+
+ for (int m = 0; (m < DIM); m++)
+ {
+ real Ext = FIELDFAC*field(m, t);
+
+ if (Ext != 0)
+ {
+ // TODO: Check parallellism
+ for (int i = 0; i < mdatoms->homenr; ++i)
+ {
+ // NOTE: Not correct with perturbed charges
+ f[i][m] += mdatoms->chargeA[i]*Ext;
+ }
+ }
+ }
+ if (MASTER(cr) && fpField_ != nullptr)
+ {
+ printComponents(t);
+ }
+ }
+}
+
+} // namespace
+
+std::unique_ptr<IInputRecExtension> createElectricFieldModule()
+{
+ return std::unique_ptr<IInputRecExtension>(new ElectricField());
+}
+
+} // namespace gmx
--- /dev/null
+/*
+ * This file is part of the GROMACS molecular simulation package.
+ *
+ * Copyright (c) 2015,2016, by the GROMACS development team, led by
+ * Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
+ * and including many others, as listed in the AUTHORS file in the
+ * top-level source directory and at http://www.gromacs.org.
+ *
+ * GROMACS 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 2.1
+ * of the License, or (at your option) any later version.
+ *
+ * GROMACS is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
+ * Lesser General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public
+ * License along with GROMACS; if not, see
+ * http://www.gnu.org/licenses, or write to the Free Software Foundation,
+ * Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+ *
+ * If you want to redistribute modifications to GROMACS, please
+ * consider that scientific software is very special. Version
+ * control is crucial - bugs must be traceable. We will be happy to
+ * consider code for inclusion in the official distribution, but
+ * derived work must not be called official GROMACS. Details are found
+ * in the README & COPYING files - if they are missing, get the
+ * official version at http://www.gromacs.org.
+ *
+ * To help us fund GROMACS development, we humbly ask that you cite
+ * the research papers on the package. Check out http://www.gromacs.org.
+ */
+#ifndef GMX_APPLIED_FORCES_ELECTRICFIELD_H
+#define GMX_APPLIED_FORCES_ELECTRICFIELD_H
+
+#include <memory>
+
+namespace gmx
+{
+
+class IInputRecExtension;
+
+/*! \brief
+ * Creates a module for an external electric field.
+ *
+ * The returned class describes the time dependent electric field that can
+ * be applied to all charges in a simulation. The field is described
+ * by the following:
+ * E(t) = A cos(omega*(t-t0))*exp(-sqr(t-t0)/(2.0*sqr(sigma)));
+ * If sigma = 0 there is no pulse and we have instead
+ * E(t) = A cos(omega*t)
+ *
+ * force is kJ mol^-1 nm^-1 = e * kJ mol^-1 nm^-1 / e
+ *
+ * WARNING:
+ * There can be problems with the virial.
+ * Since the field is not self-consistent this is unavoidable.
+ * For neutral molecules the virial is correct within this approximation.
+ * For neutral systems with many charged molecules the error is small.
+ * But for systems with a net charge or a few charged molecules
+ * the error can be significant when the field is high.
+ * Solution: implement a self-consistent electric field into PME.
+ */
+std::unique_ptr<IInputRecExtension> createElectricFieldModule();
+
+} // namespace gmx
+
+#endif
--- /dev/null
+#
+# This file is part of the GROMACS molecular simulation package.
+#
+# Copyright (c) 2015,2016, by the GROMACS development team, led by
+# Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
+# and including many others, as listed in the AUTHORS file in the
+# top-level source directory and at http://www.gromacs.org.
+#
+# GROMACS 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 2.1
+# of the License, or (at your option) any later version.
+#
+# GROMACS is distributed in the hope that it will be useful,
+# but WITHOUT ANY WARRANTY; without even the implied warranty of
+# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
+# Lesser General Public License for more details.
+#
+# You should have received a copy of the GNU Lesser General Public
+# License along with GROMACS; if not, see
+# http://www.gnu.org/licenses, or write to the Free Software Foundation,
+# Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+#
+# If you want to redistribute modifications to GROMACS, please
+# consider that scientific software is very special. Version
+# control is crucial - bugs must be traceable. We will be happy to
+# consider code for inclusion in the official distribution, but
+# derived work must not be called official GROMACS. Details are found
+# in the README & COPYING files - if they are missing, get the
+# official version at http://www.gromacs.org.
+#
+# To help us fund GROMACS development, we humbly ask that you cite
+# the research papers on the package. Check out http://www.gromacs.org.
+
+gmx_add_unit_test(AppliedForcesUnitTest applied-forces-test
+ electricfield.cpp
+ )
--- /dev/null
+/*
+ * This file is part of the GROMACS molecular simulation package.
+ *
+ * Copyright (c) 2015,2016, by the GROMACS development team, led by
+ * Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
+ * and including many others, as listed in the AUTHORS file in the
+ * top-level source directory and at http://www.gromacs.org.
+ *
+ * GROMACS 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 2.1
+ * of the License, or (at your option) any later version.
+ *
+ * GROMACS is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
+ * Lesser General Public License for more details.
+ *
+ * You should have received a copy of the GNU Lesser General Public
+ * License along with GROMACS; if not, see
+ * http://www.gnu.org/licenses, or write to the Free Software Foundation,
+ * Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+ *
+ * If you want to redistribute modifications to GROMACS, please
+ * consider that scientific software is very special. Version
+ * control is crucial - bugs must be traceable. We will be happy to
+ * consider code for inclusion in the official distribution, but
+ * derived work must not be called official GROMACS. Details are found
+ * in the README & COPYING files - if they are missing, get the
+ * official version at http://www.gromacs.org.
+ *
+ * To help us fund GROMACS development, we humbly ask that you cite
+ * the research papers on the package. Check out http://www.gromacs.org.
+ */
+/*! \internal \file
+ * \brief
+ * Tests for functionality of the "angle" trajectory analysis module.
+ *
+ * \author David van der Spoel <david.vanderspoel@icm.uu.se>
+ * \ingroup module_applied_forces
+ */
+#include "gmxpre.h"
+
+#include "gromacs/applied-forces/electricfield.h"
+
+#include <gtest/gtest.h>
+
+#include "gromacs/fileio/readinp.h"
+#include "gromacs/fileio/warninp.h"
+#include "gromacs/gmxlib/network.h"
+#include "gromacs/math/vec.h"
+#include "gromacs/mdlib/forcerec.h"
+#include "gromacs/mdrunutility/mdmodules.h"
+#include "gromacs/mdtypes/forcerec.h"
+#include "gromacs/mdtypes/inputrec.h"
+#include "gromacs/mdtypes/mdatom.h"
+#include "gromacs/utility/cstringutil.h"
+#include "gromacs/utility/real.h"
+#include "gromacs/utility/smalloc.h"
+
+#include "testutils/testasserts.h"
+
+namespace
+{
+
+/********************************************************************
+ * ElectricFieldTest
+ */
+
+class ElectricFieldTest : public ::testing::Test
+{
+ public:
+ ElectricFieldTest() {}
+
+ void test(int dim,
+ real E0,
+ real omega,
+ real t0,
+ real sigma,
+ real expectedValue)
+ {
+ gmx::test::FloatingPointTolerance tolerance(
+ gmx::test::relativeToleranceAsFloatingPoint(1.0, 0.005));
+ gmx::MDModules module;
+ t_inputrec *inputrec = module.inputrec();
+ // Prepare MDP inputs
+ int ninp = 0;
+ t_inpfile *inp = NULL;
+ char name[128];
+ char value[128];
+ const char *dimXYZ[3] = { "X", "Y", "Z" };
+ GMX_RELEASE_ASSERT((dim >= 0 && dim < 3), "Dimension should be 0, 1 or 2");
+ t_inpfile tmp;
+ tmp.bObsolete = FALSE;
+ tmp.bSet = TRUE;
+ tmp.inp_count = 0;
+ tmp.count = 0;
+ tmp.name = NULL;
+ tmp.value = NULL;
+
+ ninp = 2;
+ snew(inp, ninp);
+ inp[0] = tmp;
+ snprintf(name, sizeof(name), "E%s", dimXYZ[dim]);
+ snprintf(value, sizeof(value), "1 %g 0", E0);
+ inp[0].name = gmx_strdup(name);
+ inp[0].value = gmx_strdup(value);
+
+ inp[1] = tmp;
+ inp[1].count = 1;
+ snprintf(name, sizeof(name), "E%s-t", dimXYZ[dim]);
+ snprintf(value, sizeof(value), "3 %g 0 %g 0 %g 0", omega, t0, sigma);
+ inp[1].name = gmx_strdup(name);
+ inp[1].value = gmx_strdup(value);
+
+ warninp_t wi = init_warning(TRUE, 0);
+
+ inputrec->efield->readMdp(&ninp, &inp, wi);
+ t_mdatoms md;
+ PaddedRVecVector f = { { 0, 0, 0 } };
+ md.homenr = 1;
+ snew(md.chargeA, md.homenr);
+ md.chargeA[0] = 1;
+
+ t_commrec *cr = init_commrec();
+ t_forcerec *forcerec = mk_forcerec();
+ inputrec->efield->initForcerec(forcerec);
+ forcerec->efield->calculateForces(cr, &md, &f, 0);
+
+ EXPECT_REAL_EQ_TOL(f[0][dim], expectedValue, tolerance);
+ for (int i = 0; i < ninp; i++)
+ {
+ sfree(inp[i].name);
+ sfree(inp[i].value);
+ }
+ done_warning(wi, 0, "no file", 0);
+ }
+};
+
+TEST_F(ElectricFieldTest, Static)
+{
+ test(0, 1, 0, 0, 0, 96.4853363);
+}
+
+TEST_F(ElectricFieldTest, Oscillating)
+{
+ test(0, 1, 5, 0.2, 0, 96.4853363);
+}
+
+TEST_F(ElectricFieldTest, Pulsed)
+{
+ test(0, 1, 5, 0.5, 1, -68.215782);
+}
+
+} // namespace
*
* Copyright (c) 1991-2000, University of Groningen, The Netherlands.
* Copyright (c) 2001-2004, The GROMACS development team.
- * Copyright (c) 2013,2014,2015, by the GROMACS development team, led by
+ * Copyright (c) 2013,2014,2015,2016, by the GROMACS development team, led by
* Mark Abraham, David van der Spoel, Berk Hess, and Erik Lindahl,
* and including many others, as listed in the AUTHORS file in the
* top-level source directory and at http://www.gromacs.org.
#include "gromacs/fileio/warninp.h"
#include "gromacs/utility/basedefinitions.h"
-typedef struct {
+typedef struct t_inpfile {
int count; /* sort order for output */
gmx_bool bObsolete; /* whether it is an obsolete param value */
gmx_bool bSet; /* whether it it has been read out */
ir->wall_ewald_zfac = 3;
}
/* Cosine stuff for electric fields */
- for (j = 0; (j < DIM); j++)
- {
- gmx_fio_do_int(fio, ir->ex[j].n);
- gmx_fio_do_int(fio, ir->et[j].n);
- if (bRead)
- {
- snew(ir->ex[j].a, ir->ex[j].n);
- snew(ir->ex[j].phi, ir->ex[j].n);
- snew(ir->et[j].a, ir->et[j].n);
- snew(ir->et[j].phi, ir->et[j].n);
- }
- gmx_fio_ndo_real(fio, ir->ex[j].a, ir->ex[j].n);
- gmx_fio_ndo_real(fio, ir->ex[j].phi, ir->ex[j].n);
- gmx_fio_ndo_real(fio, ir->et[j].a, ir->et[j].n);
- gmx_fio_ndo_real(fio, ir->et[j].phi, ir->et[j].n);
- }
+ ir->efield->doTpxIO(fio, bRead);
/* Swap ions */
if (file_version >= tpxv_ComputationalElectrophysiology)
char QMmethod[STRLEN], QMbasis[STRLEN], QMcharge[STRLEN], QMmult[STRLEN],
bSH[STRLEN], CASorbitals[STRLEN], CASelectrons[STRLEN], SAon[STRLEN],
SAoff[STRLEN], SAsteps[STRLEN], bTS[STRLEN], bOPT[STRLEN];
- char efield_x[STRLEN], efield_xt[STRLEN], efield_y[STRLEN],
- efield_yt[STRLEN], efield_z[STRLEN], efield_zt[STRLEN];
} gmx_inputrec_strings;
}
/* Electric fields */
- CCTYPE("Electric fields");
- CTYPE ("Format is number of terms (int) and for all terms an amplitude (real)");
- CTYPE ("and a phase angle (real)");
- STYPE ("E-x", is->efield_x, NULL);
- CTYPE ("Time dependent (pulsed) electric field. Format is omega, time for pulse");
- CTYPE ("peak, and sigma (width) for pulse. Sigma = 0 removes pulse, leaving");
- CTYPE ("the field to be a cosine function.");
- STYPE ("E-xt", is->efield_xt, NULL);
- STYPE ("E-y", is->efield_y, NULL);
- STYPE ("E-yt", is->efield_yt, NULL);
- STYPE ("E-z", is->efield_z, NULL);
- STYPE ("E-zt", is->efield_zt, NULL);
+ ir->efield->readMdp(&ninp, &inp, wi);
/* Ion/water position swapping ("computational electrophysiology") */
CCTYPE("Ion/water position swapping for computational electrophysiology setups");
sfree(nrdf_vcm_sub);
}
-static void decode_cos(char *s, t_cosines *cosine)
-{
- char *t;
- char format[STRLEN], f1[STRLEN];
- double a, phi;
- int i;
-
- t = gmx_strdup(s);
- trim(t);
-
- cosine->n = 0;
- cosine->a = NULL;
- cosine->phi = NULL;
- if (strlen(t))
- {
- if (sscanf(t, "%d", &(cosine->n)) != 1)
- {
- gmx_fatal(FARGS, "Cannot parse cosine multiplicity from string '%s'", t);
- }
- if (cosine->n <= 0)
- {
- cosine->n = 0;
- }
- else
- {
- snew(cosine->a, cosine->n);
- snew(cosine->phi, cosine->n);
-
- sprintf(format, "%%*d");
- for (i = 0; (i < cosine->n); i++)
- {
- double gmx_unused canary;
-
- strcpy(f1, format);
- strcat(f1, "%lf%lf%lf");
- if (sscanf(t, f1, &a, &phi, &canary) != 2)
- {
- gmx_fatal(FARGS, "Invalid input for electric field shift: '%s'", t);
- }
- cosine->a[i] = a;
- cosine->phi[i] = phi;
- strcat(format, "%*lf%*lf");
- }
- }
- }
- sfree(t);
-}
-
static gmx_bool do_egp_flag(t_inputrec *ir, gmx_groups_t *groups,
const char *option, const char *val, int flag)
{
gmx_fatal(FARGS, "Can only have energy group pair tables in combination with user tables for VdW and/or Coulomb");
}
- decode_cos(is->efield_x, &(ir->ex[XX]));
- decode_cos(is->efield_xt, &(ir->et[XX]));
- decode_cos(is->efield_y, &(ir->ex[YY]));
- decode_cos(is->efield_yt, &(ir->et[YY]));
- decode_cos(is->efield_z, &(ir->ex[ZZ]));
- decode_cos(is->efield_zt, &(ir->et[ZZ]));
-
for (i = 0; (i < grps->nr); i++)
{
sfree(gnames[i]);
}
}
-static void bc_cosines(const t_commrec *cr, t_cosines *cs)
-{
- block_bc(cr, cs->n);
- snew_bc(cr, cs->a, cs->n);
- snew_bc(cr, cs->phi, cs->n);
- if (cs->n > 0)
- {
- nblock_bc(cr, cs->n, cs->a);
- nblock_bc(cr, cs->n, cs->phi);
- }
-}
-
static void bc_pull_group(const t_commrec *cr, t_pull_group *pgrp)
{
block_bc(cr, *pgrp);
static void bc_inputrec(const t_commrec *cr, t_inputrec *inputrec)
{
- int i;
-
+ /* The statement below is dangerous. It overwrites all structures in inputrec.
+ * If something is added to inputrec, like efield it will need to be
+ * treated here.
+ */
+ gmx::IInputRecExtension *eptr = inputrec->efield;
block_bc(cr, *inputrec);
+ inputrec->efield = eptr;
bc_grpopts(cr, &(inputrec->opts));
snew_bc(cr, inputrec->imd, 1);
bc_imd(cr, inputrec->imd);
}
- for (i = 0; (i < DIM); i++)
- {
- bc_cosines(cr, &(inputrec->ex[i]));
- bc_cosines(cr, &(inputrec->et[i]));
- }
+ inputrec->efield->broadCast(cr);
if (inputrec->eSwapCoords != eswapNO)
{
snew_bc(cr, inputrec->swap, 1);
std::vector<real> *lambda, struct t_graph *graph,
t_forcerec *fr,
gmx_vsite_t *vsite, rvec mu_tot,
- double t, FILE *field, struct gmx_edsam *ed,
+ double t, struct gmx_edsam *ed,
gmx_bool bBornRadii,
int flags);
fr->bF_NoVirSum = (EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype) ||
gmx_mtop_ftype_count(mtop, F_POSRES) > 0 ||
- gmx_mtop_ftype_count(mtop, F_FBPOSRES) > 0 ||
- inputrecElecField(ir)
- );
+ gmx_mtop_ftype_count(mtop, F_FBPOSRES) > 0);
+
+ /* Initialization call after setting bF_NoVirSum,
+ * since it efield->initForcerec also sets this to true.
+ */
+ ir->efield->initForcerec(fr);
+
if (fr->bF_NoVirSum)
{
fr->forceBufferNoVirialSummation = new PaddedRVecVector;
int elamstats;
int simulation_part;
FILE *fp_dhdl;
- FILE *fp_field;
int natoms_global;
int natoms_x_compressed;
gmx_groups_t *groups; /* for compressed position writing */
of->tng = NULL;
of->tng_low_prec = NULL;
of->fp_dhdl = NULL;
- of->fp_field = NULL;
of->eIntegrator = ir->eI;
of->bExpanded = ir->bExpanded;
}
}
- if (opt2bSet("-field", nfile, fnm) &&
- (ir->ex[XX].n || ir->ex[YY].n || ir->ex[ZZ].n))
- {
- if (bAppendFiles)
- {
- of->fp_field = gmx_fio_fopen(opt2fn("-field", nfile, fnm),
- filemode);
- }
- else
- {
- of->fp_field = xvgropen(opt2fn("-field", nfile, fnm),
- "Applied electric field", "Time (ps)",
- "E (V/nm)", oenv);
- }
- }
+ ir->efield->initOutput(fplog, nfile, fnm, bAppendFiles, oenv);
/* Set up atom counts so they can be passed to actual
trajectory-writing routines later. Also, XTC writing needs
return of;
}
-FILE *mdoutf_get_fp_field(gmx_mdoutf_t of)
-{
- return of->fp_field;
-}
-
ener_file_t mdoutf_get_fp_ene(gmx_mdoutf_t of)
{
return of->fp_ene;
}
}
-void done_mdoutf(gmx_mdoutf_t of)
+void done_mdoutf(gmx_mdoutf_t of, const t_inputrec *ir)
{
if (of->fp_ene != NULL)
{
{
gmx_fio_fclose(of->fp_dhdl);
}
- if (of->fp_field != NULL)
- {
- /* This is opened sometimes with xvgropen, sometimes with
- * gmx_fio_fopen, so we use the least common denominator for closing.
- */
- gmx_fio_fclose(of->fp_field);
- }
+ ir->efield->finishOutput();
if (of->f_global != NULL)
{
sfree(of->f_global);
const gmx_output_env_t *oenv,
gmx_wallcycle_t wcycle);
-/*! \brief Getter for file pointer */
-FILE *mdoutf_get_fp_field(gmx_mdoutf_t of);
-
/*! \brief Getter for file pointer */
ener_file_t mdoutf_get_fp_ene(gmx_mdoutf_t of);
void mdoutf_tng_close(gmx_mdoutf_t of);
/*! \brief Close all open output files and free the of pointer */
-void done_mdoutf(gmx_mdoutf_t of);
+void done_mdoutf(gmx_mdoutf_t of, const t_inputrec *ir);
/*! \brief Routine that writes trajectory-like frames.
*
}
//! Finalize the minimization
-static void finish_em(t_commrec *cr, gmx_mdoutf_t outf,
+static void finish_em(t_commrec *cr, gmx_mdoutf_t outf, const t_inputrec *ir,
gmx_walltime_accounting_t walltime_accounting,
gmx_wallcycle_t wcycle)
{
gmx_pme_send_finish(cr);
}
- done_mdoutf(outf);
+ done_mdoutf(outf, ir);
em_time_end(walltime_accounting, wcycle);
}
count, nrnb, wcycle, top, &top_global->groups,
ems->s.box, &ems->s.x, &ems->s.hist,
&ems->f, force_vir, mdatoms, enerd, fcd,
- &ems->s.lambda, graph, fr, vsite, mu_tot, t, NULL, NULL, TRUE,
+ &ems->s.lambda, graph, fr, vsite, mu_tot, t, NULL, TRUE,
GMX_FORCE_STATECHANGED | GMX_FORCE_ALLFORCES |
GMX_FORCE_VIRIAL | GMX_FORCE_ENERGY |
(bNS ? GMX_FORCE_NS : 0));
fprintf(fplog, "\nPerformed %d energy evaluations in total.\n", neval);
}
- finish_em(cr, outf, walltime_accounting, wcycle);
+ finish_em(cr, outf, inputrec, walltime_accounting, wcycle);
/* To print the actual number of steps we needed somewhere */
walltime_accounting_set_nsteps_done(walltime_accounting, step);
fprintf(fplog, "\nPerformed %d energy evaluations in total.\n", neval);
}
- finish_em(cr, outf, walltime_accounting, wcycle);
+ finish_em(cr, outf, inputrec, walltime_accounting, wcycle);
/* To print the actual number of steps we needed somewhere */
walltime_accounting_set_nsteps_done(walltime_accounting, step);
s_min, sqrtNumAtoms);
}
- finish_em(cr, outf, walltime_accounting, wcycle);
+ finish_em(cr, outf, inputrec, walltime_accounting, wcycle);
/* To print the actual number of steps we needed somewhere */
inputrec->nsteps = count;
&state_work.s, &state_work.f, vir, mdatoms,
nrnb, wcycle, graph, &top_global->groups,
shellfc, fr, bBornRadii, t, mu_tot,
- vsite, NULL);
+ vsite);
bNS = false;
step++;
}
gmx_mtxio_write(ftp2fn(efMTX, nfile, fnm), sz, sz, full_matrix, sparse_matrix);
}
- finish_em(cr, outf, walltime_accounting, wcycle);
+ finish_em(cr, outf, inputrec, walltime_accounting, wcycle);
walltime_accounting_set_nsteps_done(walltime_accounting, atom_index.size()*2);
t_forcerec *fr,
gmx_bool bBornRadii,
double t, rvec mu_tot,
- gmx_vsite_t *vsite,
- FILE *fp_field)
+ gmx_vsite_t *vsite)
{
int nshell;
t_shell *shell;
state->box, &state->x, &state->hist,
force[Min], force_vir, md, enerd, fcd,
&state->lambda, graph,
- fr, vsite, mu_tot, t, fp_field, NULL, bBornRadii,
+ fr, vsite, mu_tot, t, NULL, bBornRadii,
(bDoNS ? GMX_FORCE_NS : 0) | force_flags);
sf_dir = 0;
top, groups, state->box, pos[Try], &state->hist,
force[Try], force_vir,
md, enerd, fcd, &state->lambda, graph,
- fr, vsite, mu_tot, t, fp_field, NULL, bBornRadii,
+ fr, vsite, mu_tot, t, NULL, bBornRadii,
force_flags);
if (gmx_debug_at)
t_forcerec *fr,
gmx_bool bBornRadii,
double t, rvec mu_tot,
- gmx_vsite_t *vsite,
- FILE *fp_field);
+ gmx_vsite_t *vsite);
/* Print some final output */
void done_shellfc(FILE *fplog, gmx_shellfc_t *shellfc, gmx_int64_t numSteps);
}
}
-/*
- * calc_f_el calculates forces due to an electric field.
- *
- * force is kJ mol^-1 nm^-1 = e * kJ mol^-1 nm^-1 / e
- *
- * Et[] contains the parameters for the time dependent
- * part of the field.
- * Ex[] contains the parameters for
- * the spatial dependent part of the field.
- * The function should return the energy due to the electric field
- * (if any) but for now returns 0.
- *
- * WARNING:
- * There can be problems with the virial.
- * Since the field is not self-consistent this is unavoidable.
- * For neutral molecules the virial is correct within this approximation.
- * For neutral systems with many charged molecules the error is small.
- * But for systems with a net charge or a few charged molecules
- * the error can be significant when the field is high.
- * Solution: implement a self-consistent electric field into PME.
- */
-static void calc_f_el(FILE *fp, int start, int homenr,
- real charge[], rvec f[],
- t_cosines Ex[], t_cosines Et[], double t)
-{
- rvec Ext;
- real t0;
- int i, m;
-
- for (m = 0; (m < DIM); m++)
- {
- if (Et[m].n > 0)
- {
- if (Et[m].n == 3)
- {
- t0 = Et[m].a[1];
- Ext[m] = std::cos(Et[m].a[0]*(t-t0))*std::exp(-gmx::square(t-t0)/(2.0*gmx::square(Et[m].a[2])));
- }
- else
- {
- Ext[m] = std::cos(Et[m].a[0]*t);
- }
- }
- else
- {
- Ext[m] = 1.0;
- }
- if (Ex[m].n > 0)
- {
- /* Convert the field strength from V/nm to MD-units */
- Ext[m] *= Ex[m].a[0]*FIELDFAC;
- for (i = start; (i < start+homenr); i++)
- {
- f[i][m] += charge[i]*Ext[m];
- }
- }
- else
- {
- Ext[m] = 0;
- }
- }
- if (fp != NULL)
- {
- fprintf(fp, "%10g %10g %10g %10g #FIELD\n", t,
- Ext[XX]/FIELDFAC, Ext[YY]/FIELDFAC, Ext[ZZ]/FIELDFAC);
- }
-}
-
static void calc_virial(int start, int homenr, rvec x[], rvec f[],
tensor vir_part, t_graph *graph, matrix box,
t_nrnb *nrnb, const t_forcerec *fr, int ePBC)
real *lambda, t_graph *graph,
t_forcerec *fr, interaction_const_t *ic,
gmx_vsite_t *vsite, rvec mu_tot,
- double t, FILE *field, gmx_edsam_t ed,
+ double t, gmx_edsam_t ed,
gmx_bool bBornRadii,
int flags)
{
int cg1, i, j;
- int start, homenr;
double mu[2*DIM];
gmx_bool bStateChanged, bNS, bFillGrid, bCalcCGCM;
gmx_bool bDoForces, bUseGPU, bUseOrEmulGPU;
cycles_wait_gpu = 0;
nbv = fr->nbv;
- start = 0;
- homenr = mdatoms->homenr;
+ const int start = 0;
+ const int homenr = mdatoms->homenr;
clear_mat(vir_force);
if (bDoForces)
{
- if (inputrecElecField(inputrec))
+ /* Compute forces due to electric field */
+ if (fr->efield != nullptr)
{
- /* Compute forces due to electric field */
- calc_f_el(MASTER(cr) ? field : NULL,
- start, homenr, mdatoms->chargeA,
- as_rvec_array(fr->f_novirsum->data()),
- inputrec->ex, inputrec->et, t);
+ fr->efield->calculateForces(cr, mdatoms, fr->f_novirsum, t);
}
/* If we have NoVirSum forces, but we do not calculate the virial,
gmx_enerdata_t *enerd, t_fcdata *fcd,
real *lambda, t_graph *graph,
t_forcerec *fr, gmx_vsite_t *vsite, rvec mu_tot,
- double t, FILE *field, gmx_edsam_t ed,
+ double t, gmx_edsam_t ed,
gmx_bool bBornRadii,
int flags)
{
int cg0, cg1, i, j;
- int start, homenr;
double mu[2*DIM];
gmx_bool bStateChanged, bNS, bFillGrid, bCalcCGCM;
gmx_bool bDoForces;
float cycles_pme, cycles_force;
- start = 0;
- homenr = mdatoms->homenr;
+ const int start = 0;
+ const int homenr = mdatoms->homenr;
clear_mat(vir_force);
if (bDoForces)
{
- if (inputrecElecField(inputrec))
+ /* Compute forces due to electric field */
+ if (fr->efield != nullptr)
{
- /* Compute forces due to electric field */
- calc_f_el(MASTER(cr) ? field : NULL,
- start, homenr, mdatoms->chargeA,
- as_rvec_array(fr->f_novirsum->data()),
- inputrec->ex, inputrec->et, t);
+ fr->efield->calculateForces(cr, mdatoms, fr->f_novirsum, t);
}
/* Communicate the forces */
std::vector<real> *lambda, t_graph *graph,
t_forcerec *fr,
gmx_vsite_t *vsite, rvec mu_tot,
- double t, FILE *field, gmx_edsam_t ed,
+ double t, gmx_edsam_t ed,
gmx_bool bBornRadii,
int flags)
{
lambda->data(), graph,
fr, fr->ic,
vsite, mu_tot,
- t, field, ed,
+ t, ed,
bBornRadii,
flags);
break;
enerd, fcd,
lambda->data(), graph,
fr, vsite, mu_tot,
- t, field, ed,
+ t, ed,
bBornRadii,
flags);
break;
please_cite(fplog, "Goga2012");
}
}
- if ((ir->et[XX].n > 0) || (ir->et[YY].n > 0) || (ir->et[ZZ].n > 0))
- {
- please_cite(fplog, "Caleman2008a");
- }
init_nrnb(nrnb);
if (nfile != -1)
state_global->box, &state_global->x, &state_global->hist,
&f, force_vir, mdatoms, enerd, fcd,
&state_global->lambda,
- NULL, fr, NULL, mu_tot, t, NULL, NULL, FALSE,
+ NULL, fr, NULL, mu_tot, t, NULL, FALSE,
GMX_FORCE_NONBONDED | GMX_FORCE_ENERGY |
(bNS ? GMX_FORCE_DYNAMICBOX | GMX_FORCE_NS : 0) |
(bStateChanged ? GMX_FORCE_STATECHANGED : 0));
#include "mdmodules.h"
+#include "gromacs/applied-forces/electricfield.h"
#include "gromacs/mdtypes/inputrec.h"
#include "gromacs/utility/smalloc.h"
{
if (ir_ == nullptr)
{
+ field_ = createElectricFieldModule();
snew(ir_, 1);
snew(ir_->fepvals, 1);
snew(ir_->expandedvals, 1);
snew(ir_->simtempvals, 1);
+ ir_->efield = field_.get();
}
}
- t_inputrec *ir_;
+ std::unique_ptr<IInputRecExtension> field_;
+ t_inputrec *ir_;
};
MDModules::MDModules() : impl_(new Impl)
*
* This class acts as a central place for constructing t_inputrec (and possibly
* other mdrun structures in the future) and wiring up dependencies between
- * modules that are referenced from these structures.
+ * modules that are referenced from these structures. This class owns all such
+ * modules, and needs to remain in existence as long as the returned data
+ * structures are in use. Ideally, it is also the only place that creates
+ * instances of these modules (outside test code).
+ *
+ * The general idea is that each module takes care of its own data rather than
+ * mdrun having to know about all the details of each type of force calculation.
+ * Initially this is applied for simple things like electric field calculations
+ * but later more complex forces will be supported too.
+ *
+ * The current approach uses t_inputrec and IInputRecExtension to pass
+ * references to the modules to other code to avoid changing many function
+ * signatures. Also, the current usage means that nearly every use of
+ * t_inputrec (in particular, reading it from mdp or tpr files) needs to be
+ * initialized through MDModules for correct functionality. For the future, a
+ * better approach would be to pass around a reference to MDModules instead and
+ * call it directly for cases that are not related to t_inputrec functionality.
+ * This (and other refactoring) would allow simplifying IInputRecExtension.
+ * IForceProvider is the other interface currently used to interact with these
+ * modules. Also, all the places where these interfaces are used should become
+ * loops over a container of these interfaces, instead of the current single
+ * pointer.
*
* \inlibraryapi
* \ingroup module_mdrunutility
#ifdef __cplusplus
extern "C" {
-#endif
-#if 0
-} /* fixes auto-indentation problems */
+
+struct t_mdatoms;
+struct t_commrec;
+
+/*! \libinternal \brief
+ * Interface for a component that provides forces during MD.
+ *
+ * This is typically part of a larger structure/class managing its own
+ * data, such that it has the information on what to do stored locally.
+ * \todo Implement returning of energy and dH/dlambda.
+ * \inlibraryapi
+ */
+struct IForceProvider
+{
+ public:
+ /*! \brief Compute forces
+ *
+ * \todo This is specific for electric fields and needs to be generalized.
+ * \param[in] cr Communication record for parallel operations
+ * \param[in] mdatoms Atom information
+ * \param[inout] force The forces
+ * \param[in] t The actual time in the simulation (ps)
+ */
+ virtual void calculateForces(const t_commrec *cr,
+ const t_mdatoms *mdatoms,
+ PaddedRVecVector *force,
+ double t) = 0;
+
+ protected:
+ ~IForceProvider() {}
+};
#endif
/* Abstract type for PME that is defined only in the routine that use them. */
struct bonded_threading_t *bonded_threading;
/* Ewald correction thread local virial and energy data */
- int nthread_ewc;
- ewald_corr_thread_t *ewc_t;
+ int nthread_ewc;
+ ewald_corr_thread_t *ewc_t;
+
+ struct IForceProvider *efield;
} t_forcerec;
/* Important: Starting with Gromacs-4.6, the values of c6 and c12 in the nbfp array have
void done_inputrec(t_inputrec *ir)
{
- int m;
-
- for (m = 0; (m < DIM); m++)
- {
- if (ir->ex[m].a)
- {
- sfree(ir->ex[m].a);
- }
- if (ir->ex[m].phi)
- {
- sfree(ir->ex[m].phi);
- }
- if (ir->et[m].a)
- {
- sfree(ir->et[m].a);
- }
- if (ir->et[m].phi)
- {
- sfree(ir->et[m].phi);
- }
- }
-
sfree(ir->opts.nrdf);
sfree(ir->opts.ref_t);
sfree(ir->opts.annealing);
}
}
-static void pr_cosine(FILE *fp, int indent, const char *title, const t_cosines *cos,
- gmx_bool bMDPformat)
-{
- int j;
-
- if (bMDPformat)
- {
- fprintf(fp, "%s = %d\n", title, cos->n);
- }
- else
- {
- indent = pr_title(fp, indent, title);
- pr_indent(fp, indent);
- fprintf(fp, "n = %d\n", cos->n);
- if (cos->n > 0)
- {
- pr_indent(fp, indent+2);
- fprintf(fp, "a =");
- for (j = 0; (j < cos->n); j++)
- {
- fprintf(fp, " %e", cos->a[j]);
- }
- fprintf(fp, "\n");
- pr_indent(fp, indent+2);
- fprintf(fp, "phi =");
- for (j = 0; (j < cos->n); j++)
- {
- fprintf(fp, " %e", cos->phi[j]);
- }
- fprintf(fp, "\n");
- }
- }
-}
-
#define PS(t, s) pr_str(fp, indent, t, s)
#define PI(t, s) pr_int(fp, indent, t, s)
#define PSTEP(t, s) pr_int64(fp, indent, t, s)
}
/* ELECTRIC FIELDS */
- pr_cosine(fp, indent, "E-x", &(ir->ex[XX]), bMDPformat);
- pr_cosine(fp, indent, "E-xt", &(ir->et[XX]), bMDPformat);
- pr_cosine(fp, indent, "E-y", &(ir->ex[YY]), bMDPformat);
- pr_cosine(fp, indent, "E-yt", &(ir->et[YY]), bMDPformat);
- pr_cosine(fp, indent, "E-z", &(ir->ex[ZZ]), bMDPformat);
- pr_cosine(fp, indent, "E-zt", &(ir->et[ZZ]), bMDPformat);
+ ir->efield->printParameters(fp, indent);
/* ION/WATER SWAPPING FOR COMPUTATIONAL ELECTROPHYSIOLOGY */
PS("swapcoords", ESWAPTYPE(ir->eSwapCoords));
}
}
-
-static void cmp_cosines(FILE *fp, const char *s, const t_cosines c1[DIM], const t_cosines c2[DIM], real ftol, real abstol)
-{
- int i, m;
- char buf[256];
-
- for (m = 0; (m < DIM); m++)
- {
- sprintf(buf, "inputrec->%s[%d]", s, m);
- cmp_int(fp, buf, 0, c1->n, c2->n);
- for (i = 0; (i < std::min(c1->n, c2->n)); i++)
- {
- cmp_real(fp, buf, i, c1->a[i], c2->a[i], ftol, abstol);
- cmp_real(fp, buf, i, c1->phi[i], c2->phi[i], ftol, abstol);
- }
- }
-}
static void cmp_pull(FILE *fp)
{
fprintf(fp, "WARNING: Both files use COM pulling, but comparing of the pull struct is not implemented (yet). The pull parameters could be the same or different.\n");
cmp_real(fp, "inputrec->userreal3", -1, ir1->userreal3, ir2->userreal3, ftol, abstol);
cmp_real(fp, "inputrec->userreal4", -1, ir1->userreal4, ir2->userreal4, ftol, abstol);
cmp_grpopts(fp, &(ir1->opts), &(ir2->opts), ftol, abstol);
- cmp_cosines(fp, "ex", ir1->ex, ir2->ex, ftol, abstol);
- cmp_cosines(fp, "et", ir1->et, ir2->et, ftol, abstol);
+ ir1->efield->compare(fp, ir2->efield, ftol, abstol);
}
void comp_pull_AB(FILE *fp, pull_params_t *pull, real ftol, real abstol)
(ir->ewald_geometry == eewg3DC || ir->epsilon_surface != 0));
}
-gmx_bool inputrecElecField(const t_inputrec *ir)
-{
- return (ir->ex[XX].n > 0 || ir->ex[YY].n > 0 || ir->ex[ZZ].n > 0);
-}
-
gmx_bool inputrecExclForces(const t_inputrec *ir)
{
return (EEL_FULL(ir->coulombtype) || (EEL_RF(ir->coulombtype)) ||
#include "gromacs/utility/basedefinitions.h"
#include "gromacs/utility/real.h"
-struct pull_params_t;
+#define EGP_EXCL (1<<0)
+#define EGP_TABLE (1<<1)
-typedef struct {
- //! Number of terms
- int n;
- //! Coeffients (V / nm)
- real *a;
- //! Phase angles
- real *phi;
-} t_cosines;
+struct gmx_output_env_t;
+struct pull_params_t;
+struct t_commrec;
+struct t_fileio;
+struct t_filenm;
+struct t_forcerec;
+struct t_inpfile;
+struct warninp;
+
+namespace gmx
+{
-typedef struct {
- real E0; /* Field strength (V/nm) */
- real omega; /* Frequency (1/ps) */
- real t0; /* Centre of the Gaussian pulse (ps) */
- real sigma; /* Width of the Gaussian pulse (FWHM) (ps) */
-} t_efield;
+/*! \libinternal \brief
+ * Inputrec extension interface for a mdrun module.
+ *
+ * This interface provides a mechanism for additional modules to contribute
+ * data that traditionally has been kept in t_inputrec. This is essentially
+ * parameters read from an mdp file and subsequently stored in a tpr file.
+ * The functionality to broadcast, compare, and print these parameters
+ * currently needs to be provided separately, but this should simplify
+ * significantly if/when we move to a more structured file format (both for mdp
+ * and tpr) that allows a generic representation for code that does not need to
+ * know the interpretation of the values.
+ *
+ * For now, this interface also includes some unrelated methods (initOutput(),
+ * finishOutput(), initForcerec()), because t_inputrec is used as a container
+ * to pass references to the modules around.
+ * See MDModules for more information on the general approach and future
+ * considerations.
+ */
+class IInputRecExtension
+{
+ public:
+ virtual ~IInputRecExtension() {}
+
+ /*! \brief Read or write tpr file
+ *
+ * Read or write the necessary data from a tpr file. The routine is responsible
+ * for consistency, such that all data belonging to this module is read or written.
+ * \param[inout] fio Gromacs file descriptor
+ * \param[in] bRead boolean determines whether we are reading or writing
+ */
+ virtual void doTpxIO(t_fileio *fio, bool bRead) = 0;
+
+ /*! \brief
+ * Extracts parameters from mdp file.
+ *
+ * \param[inout] ninp_p Number of inpfile elements before and after processing
+ * \param[inout] inp_p The inpfile elements corresponding to lines in the mdp
+ * \param[inout] wi Structure for managing warnings in grompp
+ */
+ virtual void readMdp(int *ninp_p, t_inpfile **inp_p, warninp *wi) = 0;
+
+ /*! \brief Broadcast input parameters to all ranks
+ *
+ * \param[in] cr Communication record, gromacs structure
+ */
+ virtual void broadCast(const t_commrec *cr) = 0;
+
+ /*! \brief compare a section of two input record structures
+ *
+ * Routine is used in gmx check.
+ * \param[in] fp File pointer
+ * \param[inout] field2 Electric field
+ * \param[in] reltol Relative tolerance
+ * \param[in] abstol Absolute tolerance
+ */
+ virtual void compare(FILE *fp,
+ const gmx::IInputRecExtension *field2,
+ real reltol,
+ real abstol) = 0;
+
+ /*! \brief Print parameters belonging to this class to a file
+ *
+ * \param[in] fp File pointer
+ * \param[in] indent Initial indentation level for printing
+ */
+ virtual void printParameters(FILE *fp, int indent) = 0;
+
+ /*! \brief Initiate output parameters
+ *
+ * \param[in] fplog File pointer for log messages
+ * \param[in] nfile Number of files
+ * \param[in] fnm Array of filenames and properties
+ * \param[in] bAppendFiles Whether or not we should append to files
+ * \param[in] oenv The output environment for xvg files
+ */
+ virtual void initOutput(FILE *fplog, int nfile, const t_filenm fnm[],
+ bool bAppendFiles, const gmx_output_env_t *oenv) = 0;
+
+ //! Finalize output
+ virtual void finishOutput() = 0;
+
+ /*! \brief Set/initiate relevant options in the forcerec structure
+ *
+ * \param[inout] fr The forcerec structure
+ */
+ virtual void initForcerec(t_forcerec *fr) = 0;
+};
-#define EGP_EXCL (1<<0)
-#define EGP_TABLE (1<<1)
+} // namespace gmx
typedef struct t_grpopts {
int ngtc; /* # T-Coupl groups */
struct pull_t *pull_work; /* The COM pull force calculation data structure; TODO this pointer should live somewhere else */
/* Enforced rotation data */
- gmx_bool bRot; /* Calculate enforced rotation potential(s)? */
- t_rot *rot; /* The data for enforced rotation potentials */
-
- int eSwapCoords; /* Do ion/water position exchanges (CompEL)? */
- t_swapcoords *swap;
-
- gmx_bool bIMD; /* Allow interactive MD sessions for this .tpr? */
- t_IMD *imd; /* Interactive molecular dynamics */
-
- real cos_accel; /* Acceleration for viscosity calculation */
- tensor deform; /* Triclinic deformation velocities (nm/ps) */
- int userint1; /* User determined parameters */
- int userint2;
- int userint3;
- int userint4;
- real userreal1;
- real userreal2;
- real userreal3;
- real userreal4;
- t_grpopts opts; /* Group options */
- t_cosines ex[DIM]; /* Electric field stuff (spatial part) */
- t_cosines et[DIM]; /* Electric field stuff (time part) */
- gmx_bool bQMMM; /* QM/MM calculation */
- int QMconstraints; /* constraints on QM bonds */
- int QMMMscheme; /* Scheme: ONIOM or normal */
- real scalefactor; /* factor for scaling the MM charges in QM calc.*/
+ gmx_bool bRot; /* Calculate enforced rotation potential(s)? */
+ t_rot *rot; /* The data for enforced rotation potentials */
+
+ int eSwapCoords; /* Do ion/water position exchanges (CompEL)? */
+ t_swapcoords *swap;
+
+ gmx_bool bIMD; /* Allow interactive MD sessions for this .tpr? */
+ t_IMD *imd; /* Interactive molecular dynamics */
+
+ real cos_accel; /* Acceleration for viscosity calculation */
+ tensor deform; /* Triclinic deformation velocities (nm/ps) */
+ int userint1; /* User determined parameters */
+ int userint2;
+ int userint3;
+ int userint4;
+ real userreal1;
+ real userreal2;
+ real userreal3;
+ real userreal4;
+ t_grpopts opts; /* Group options */
+ gmx::IInputRecExtension *efield; /* Applied electric field */
+ gmx_bool bQMMM; /* QM/MM calculation */
+ int QMconstraints; /* constraints on QM bonds */
+ int QMMMscheme; /* Scheme: ONIOM or normal */
+ real scalefactor; /* factor for scaling the MM charges in QM calc.*/
/* Fields for removed features go here (better caching) */
gmx_bool bAdress; // Whether AdResS is enabled - always false if a valid .tpr was read
gmx_bool inputrecTwinRange(const t_inputrec *ir);
-gmx_bool inputrecElecField(const t_inputrec *ir);
-
gmx_bool inputrecExclForces(const t_inputrec *ir);
gmx_bool inputrecNptTrotter(const t_inputrec *ir);
state, &f, force_vir, mdatoms,
nrnb, wcycle, graph, groups,
shellfc, fr, bBornRadii, t, mu_tot,
- vsite, mdoutf_get_fp_field(outf));
+ vsite);
}
else
{
state->box, &state->x, &state->hist,
&f, force_vir, mdatoms, enerd, fcd,
&state->lambda, graph,
- fr, vsite, mu_tot, t, mdoutf_get_fp_field(outf), ed, bBornRadii,
+ fr, vsite, mu_tot, t, ed, bBornRadii,
(bNS ? GMX_FORCE_NS : 0) | force_flags);
}
}
}
- done_mdoutf(outf);
+ done_mdoutf(outf, ir);
if (bPMETune)
{