Description

This calculation-type keyword requests a single calculation of the forces on the nuclei (i.e., the gradient of the energy). The dipole moment is also computed (as a proper analytic derivative of the energy for MP2, CC, QCI and CI) [Raghavachari81, Wiberg92].

Options

#### EnOnly

Compute the forces by numerically differentiating the energy once. It is the default for all methods for which analytic gradients are unavailable. Note that this procedure exhibits some numerical instability, so care must be taken that an optimal step size is specified for each case.

#### Restart

Restarts numerical evaluation of the forces.

#### StepSize=N

Sets the step size used in numerical differentiation to 0.0001*N. The units are Angstroms by default unless Units=Bohr has been specified. The default step size is 0.01 Å. StepSize is valid only in conjunction with EnOnly.

#### NoStep

Can be used with large MM force calculations to avoid the O(N^{3}) work involved in computing the putative geometry optimization step.

Availability

Analytic gradients are available for all SCF wavefunctions, all DFT methods, CIS, MP2, MP3, MP4(SDQ), CID, CISD, CCD, CCSD, QCISD, BD, CASSCF, SAC-CI and all semi-empirical methods. For other methods, the forces are determined by numerical differentiation.

Examples

The forces on the nuclei appear in the output as follows (this sample is from a calculation on water):

***** AXES RESTORED TO ORIGINAL SET ***** ------------------------------------------------------------------- Center Atomic Forces (Hartrees/Bohr) Number Number X Y Z ------------------------------------------------------------------- 1 8 -.049849321 .000000000 -.028780519 2 1 .046711997 .000000000 -.023346514 3 1 .003137324 .000000000 .052127033 ------------------------------------------------------------------- MAX .052127033 RMS .031211490 ------------------------------------------------------------------- Internal Coordinate Forces (Hartree/Bohr or radian) Cent Atom N1 Length/X N2 Alpha/Y N3 Beta/Z J ------------------------------------------------------------------- 1 O 2 H 1 -.023347( 1) 3 H 1 -.023347( 2) 2 -.088273( 3) ------------------------------------------------------------------- MAX .088272874 RMS .054412682

The forces are determined in the standard orientation, but are restored to the original (Z-matrix) set of axes before printing (as noted in the output). This is followed by the corresponding derivatives with respect to the internal coordinates (lengths and angles used in the Z-matrix) when internal coordinates are in use. The forces are followed in each case by their maximum and root-mean-square values.

This calculation-type keyword requests a single calculation of the forces on the nuclei (i.e., the gradient of the energy). The dipole moment is also computed (as a proper analytic derivative of the energy for MP2, CC, QCI and CI) [Raghavachari81, Wiberg92].

#### EnOnly

Compute the forces by numerically differentiating the energy once. It is the default for all methods for which analytic gradients are unavailable. Note that this procedure exhibits some numerical instability, so care must be taken that an optimal step size is specified for each case.

#### Restart

Restarts numerical evaluation of the forces.

#### StepSize=N

Sets the step size used in numerical differentiation to 0.0001*N. The units are Angstroms by default unless Units=Bohr has been specified. The default step size is 0.01 Å. StepSize is valid only in conjunction with EnOnly.

#### NoStep

Can be used with large MM force calculations to avoid the O(N^{3}) work involved in computing the putative geometry optimization step.

Analytic gradients are available for all SCF wavefunctions, all DFT methods, CIS, MP2, MP3, MP4(SDQ), CID, CISD, CCD, CCSD, QCISD, BD, CASSCF, SAC-CI and all semi-empirical methods. For other methods, the forces are determined by numerical differentiation.

The forces on the nuclei appear in the output as follows (this sample is from a calculation on water):

***** AXES RESTORED TO ORIGINAL SET ***** ------------------------------------------------------------------- Center Atomic Forces (Hartrees/Bohr) Number Number X Y Z ------------------------------------------------------------------- 1 8 -.049849321 .000000000 -.028780519 2 1 .046711997 .000000000 -.023346514 3 1 .003137324 .000000000 .052127033 ------------------------------------------------------------------- MAX .052127033 RMS .031211490 ------------------------------------------------------------------- Internal Coordinate Forces (Hartree/Bohr or radian) Cent Atom N1 Length/X N2 Alpha/Y N3 Beta/Z J ------------------------------------------------------------------- 1 O 2 H 1 -.023347( 1) 3 H 1 -.023347( 2) 2 -.088273( 3) ------------------------------------------------------------------- MAX .088272874 RMS .054412682

The forces are determined in the standard orientation, but are restored to the original (Z-matrix) set of axes before printing (as noted in the output). This is followed by the corresponding derivatives with respect to the internal coordinates (lengths and angles used in the Z-matrix) when internal coordinates are in use. The forces are followed in each case by their maximum and root-mean-square values.

Last updated on: 05 January 2017. [G16 Rev. C.01]