* Exactcutoff is only used by Reaction-field-zero, and is not user-selectable.
*/
enum eintmod {
- eintmodPOTSHIFT_VERLET, eintmodPOTSHIFT, eintmodNONE, eintmodPOTSWITCH, eintmodEXACTCUTOFF, eintmodNR
+ eintmodPOTSHIFT_VERLET, eintmodPOTSHIFT, eintmodNONE, eintmodPOTSWITCH, eintmodEXACTCUTOFF, eintmodFORCESWITCH, eintmodNR
};
/*
#define EEL_RF(e) ((e) == eelRF || (e) == eelGRF || (e) == eelRF_NEC || (e) == eelRF_ZERO )
#define EEL_PME(e) ((e) == eelPME || (e) == eelPMESWITCH || (e) == eelPMEUSER || (e) == eelPMEUSERSWITCH || (e) == eelP3M_AD)
-#define EEL_EWALD(e) (EEL_PME(e) || (e) == eelEWALD)
-#define EEL_FULL(e) (EEL_PME(e) || (e) == eelPOISSON || (e) == eelEWALD)
-
-#define EEL_SWITCHED(e) ((e) == eelSWITCH || (e) == eelSHIFT || (e) == eelENCADSHIFT || (e) == eelPMESWITCH || (e) == eelPMEUSERSWITCH)
+#define EEL_PME_EWALD(e) (EEL_PME(e) || (e) == eelEWALD)
+#define EEL_FULL(e) (EEL_PME_EWALD(e) || (e) == eelPOISSON)
#define EEL_USER(e) ((e) == eelUSER || (e) == eelPMEUSER || (e) == (eelPMEUSERSWITCH))
-#define EEL_IS_ZERO_AT_CUTOFF(e) (EEL_SWITCHED(e) || (e) == eelRF_ZERO)
-
-#define EEL_MIGHT_BE_ZERO_AT_CUTOFF(e) (EEL_IS_ZERO_AT_CUTOFF(e) || (e) == eelUSER || (e) == eelPMEUSER)
-
enum {
evdwCUT, evdwSWITCH, evdwSHIFT, evdwUSER, evdwENCADSHIFT,
evdwPME, evdwNR
#define EVDW_PME(e) ((e) == evdwPME)
-#define EVDW_SWITCHED(e) ((e) == evdwSWITCH || (e) == evdwSHIFT || (e) == evdwENCADSHIFT)
-
-#define EVDW_IS_ZERO_AT_CUTOFF(e) EVDW_SWITCHED(e)
-
-#define EVDW_MIGHT_BE_ZERO_AT_CUTOFF(e) (EVDW_IS_ZERO_AT_CUTOFF(e) || (e) == evdwUSER)
-
enum {
ensGRID, ensSIMPLE, ensNR
};
efptFEP, efptMASS, efptCOUL, efptVDW, efptBONDED, efptRESTRAINT, efptTEMPERATURE, efptNR
};
+/* Printing the energy to the free energy dhdl file. YES is an alias to TOTAL, and
+ * will be converted in readir, so we never have to account for it in code.
+ */
+enum {
+ edHdLPrintEnergyNO, edHdLPrintEnergyTOTAL, edHdLPrintEnergyPOTENTIAL, edHdLPrintEnergyYES, edHdLPrintEnergyNR
+};
+
/* How the lambda weights are calculated:
elamstatsMETROPOLIS = using the metropolis criteria
elamstatsBARKER = using the Barker critera for transition weights - also called unoptimized Bennett
enum eSwaptype {
eswapNO, eswapX, eswapY, eswapZ, eSwapTypesNR
};
-/* The following three enums are mainly used for indexing arrays and when
- * looping over the available ions, channels, or compartments. This hopefully
- * adds to the code's readability because it makes clear which object is dealt
- * with in a block of code.
- *
- * The two compartments for CompEL setups */
-enum eCompartment {
- eCompA, eCompB, eCompNR
-};
-/* The positive and negative ions CompEL setups, future versions of the
- * protocol might consider more than two types of ions */
-enum eIontype {
- eIonNEG, eIonPOS, eIonNR
-};
-/* The chanels that define with their COM the compartment boundaries in
- * CompEL setups. In principle one could also use modified setups with
- * more than two channels. */
-enum eChannel {
- eChan0, eChan1, eChanNR
-};
/* QMMM */
enum {
/* flat-bottom posres geometries */
enum {
efbposresZERO, efbposresSPHERE, efbposresCYLINDER, efbposresX, efbposresY, efbposresZ,
- efbposresNR
+ efbposresCYLINDERX, efbposresCYLINDERY, efbposresCYLINDERZ, efbposresNR
};
enum {
GMX_NBKERNEL_VDW_LENNARDJONES,
GMX_NBKERNEL_VDW_BUCKINGHAM,
GMX_NBKERNEL_VDW_CUBICSPLINETABLE,
+ GMX_NBKERNEL_VDW_LJEWALD,
GMX_NBKERNEL_VDW_NR
};
/* Types of interactions inside the neighborlist