| ▼NOpenMM | |
| CAmoebaAngleForce | This class implements an interaction between triplets of particles that varies with the angle between them |
| CAmoebaBondForce | This class implements an interaction between pairs of particles that varies with the distance between them |
| CAmoebaGeneralizedKirkwoodForce | This class implements an implicit solvation force using the generalized Kirkwood/Grycuk model |
| CAmoebaInPlaneAngleForce | This class implements an interaction at trigonal centers corresponding to the projected in-plane angle bend energy between four particles |
| CAmoebaMultipoleForce | This class implements the Amoeba multipole interaction |
| CAmoebaOutOfPlaneBendForce | This class implements the Amoeba out-of-plane bend interaction |
| CAmoebaPiTorsionForce | This class implements the Amoeba pi-torsion interaction |
| CAmoebaStretchBendForce | This class implements the Amoeba stretch-bend interaction |
| CAmoebaTorsionTorsionForce | This class implements the Amoeba torsion-torsion interaction |
| CAmoebaVdwForce | This class implements a buffered 14-7 potential used to model van der Waals forces |
| CAmoebaWcaDispersionForce | This class implements a nonbonded interaction between pairs of particles typically used along with AmoebaGeneralizedKirkwoodForce as part of an implicit solvent model |
| CAndersenThermostat | This class uses the Andersen method to maintain constant temperature |
| CBrownianIntegrator | This is an Integrator which simulates a System using Brownian dynamics |
| CCMAPTorsionForce | This class implements an interaction between pairs of dihedral angles |
| CCMMotionRemover | This class prevents the center of mass of a System from drifting |
| CContext | A Context stores the complete state of a simulation |
| CContinuous1DFunction | This is a TabulatedFunction that computes a continuous one dimensional function |
| CContinuous2DFunction | This is a TabulatedFunction that computes a continuous two dimensional function |
| CContinuous3DFunction | This is a TabulatedFunction that computes a continuous three dimensional function |
| CCustomAngleForce | This class implements interactions between sets of three particles that depend on the angle between them |
| CCustomBondForce | This class implements bonded interactions between pairs of particles |
| CCustomCompoundBondForce | This class supports a wide variety of bonded interactions |
| CCustomExternalForce | This class implements an "external" force on particles |
| CCustomGBForce | This class implements complex, multiple stage nonbonded interactions between particles |
| CCustomHbondForce | This class supports a wide variety of energy functions used to represent hydrogen bonding |
| CCustomIntegrator | This is an Integrator that can be used to implemented arbitrary, user defined integration algorithms |
| CCustomManyParticleForce | This class supports a wide variety of nonbonded N-particle interactions, where N is user specified |
| CCustomNonbondedForce | This class implements nonbonded interactions between particles |
| CCustomTorsionForce | This class implements interactions between sets of four particles that depend on the torsion angle between them |
| CDiscrete1DFunction | This is a TabulatedFunction that computes a discrete one dimensional function f(x) |
| CDiscrete2DFunction | This is a TabulatedFunction that computes a discrete two dimensional function f(x,y) |
| CDiscrete3DFunction | This is a TabulatedFunction that computes a discrete three dimensional function f(x,y,z) |
| CDrudeForce | This class implements forces that are specific to Drude oscillators |
| CDrudeLangevinIntegrator | This Integrator simulates systems that include Drude particles |
| CDrudeSCFIntegrator | This is a leap-frog Verlet Integrator that simulates systems with Drude particles |
| CForce | Force objects apply forces to the particles in a System, or alter their behavior in other ways |
| CGBSAOBCForce | This class implements an implicit solvation force using the GBSA-OBC model |
| CGBVIForce | This class implements an implicit solvation force using the GB/VI model |
| CHarmonicAngleForce | This class implements an interaction between groups of three particles that varies harmonically with the angle between them |
| CHarmonicBondForce | This class implements an interaction between pairs of particles that varies harmonically with the distance between them |
| CIntegrator | An Integrator defines a method for simulating a System by integrating the equations of motion |
| CKernel | A Kernel encapsulates a particular implementation of a calculation that can be performed on the data in a Context |
| CKernelFactory | A KernelFactory is an object that can create KernelImpls |
| CKernelImpl | A KernelImpl defines the internal implementation of a Kernel object |
| CLangevinIntegrator | This is an Integrator which simulates a System using Langevin dynamics |
| CLocalCoordinatesSite | This is a VirtualSite that uses the locations of three other particles to compute a local coordinate system, then places the virtual site at a fixed location in that coordinate system |
| CLocalEnergyMinimizer | Given a Context, this class searches for a new set of particle positions that represent a local minimum of the potential energy |
| CMonteCarloAnisotropicBarostat | This class uses a Monte Carlo algorithm to adjust the size of the periodic box, simulating the effect of constant pressure |
| CMonteCarloBarostat | This class uses a Monte Carlo algorithm to adjust the size of the periodic box, simulating the effect of constant pressure |
| CMonteCarloMembraneBarostat | This is a Monte Carlo barostat designed specifically for membrane simulations |
| CNonbondedForce | This class implements nonbonded interactions between particles, including a Coulomb force to represent electrostatics and a Lennard-Jones force to represent van der Waals interactions |
| COpenMMException | This class is used for all exceptions thrown by OpenMM |
| COutOfPlaneSite | This is a VirtualSite that computes the particle location based on three other particles' locations |
| CPeriodicTorsionForce | This class implements an interaction between groups of four particles that varies periodically with the torsion angle between them |
| CPlatform | A Platform defines an implementation of all the kernels needed to perform some calculation |
| CRBTorsionForce | This class implements an interaction between groups of four particles that varies with the torsion angle between them according to the Ryckaert-Bellemans potential |
| CRPMDIntegrator | This is an Integrator which simulates a System using ring polymer molecular dynamics (RPMD) |
| CRPMDMonteCarloBarostat | This class is very similar to MonteCarloBarostat, but it is specifically designed for use with RPMDIntegrator |
| CRPMDUpdater | This ForceImpl subclass is for forces specifically designed to work with RPMDIntegrator |
| CState | A State object records a snapshot of the current state of a simulation at a point in time |
| CSystem | This class represents a molecular system |
| CTabulatedFunction | A TabulatedFunction uses a set of tabulated values to define a mathematical function |
| CThreeParticleAverageSite | This is a VirtualSite that computes the particle location as a weighted average of three other particle's locations |
| CTwoParticleAverageSite | This is a VirtualSite that computes the particle location as a weighted average of two other particle's locations |
| CVariableLangevinIntegrator | This is an error contolled, variable time step Integrator that simulates a System using Langevin dynamics |
| CVariableVerletIntegrator | This is an error contolled, variable time step Integrator that simulates a System using the leap-frog Verlet algorithm |
| CVec3 | This class represents a three component vector |
| CVerletIntegrator | This is an Integrator which simulates a System using the leap-frog Verlet algorithm |
| CVirtualSite | A VirtualSite describes the rules for computing a particle's position based on other particles |
| CXmlSerializer | XmlSerializer is used for serializing objects as XML, and for reconstructing them again |
1.8.8 
