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III.F.2.

Completed calculations for C2H5F (fluoroethane)

Methods and basis sets for which an energy has been calculated. "e" indicates just an energy has been calculated. "o" indicates an optimized geometry. "v" indicates vibrational frequencies. "s" followed by a number indicates completed calculations for different states (for example s1ov). "c" followed by a number indicates completed calculations for different conformations (for example c2ov).
See the Calculated Energies page (section III.A.1) for more calculated properties.
Methods with predefined basis sets
semi-empirical AM1 ov
composite G1 e
G2MP2 e
G2 e
G3 e
G3B3 e
G3MP2 e
G4 e
CBS-Q e

Methods with standard basis sets
STO-3G 3-21G 3-21G* 6-31G 6-31G* 6-31G** 6-31+G** 6-311G* 6-311G** 6-31G(2df,p) 6-311+G(3df,2p) TZVP cc-pVDZ cc-pVTZ cc-pVQZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z
hartree fock HF ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov ov   ov
density functional LSDA ov ov ov ov ov ov ov ov ov ov     ov ov   ov   ov
SVWN   ov     ov   ov                      
BLYP ov ov ov ov ov ov ov ov ov ov     ov ov       ov
B1B95 ov ov ov ov ov ov ov ov ov ov     ov ov   ov   ov
B3LYP ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov ov ov
B3LYPultrafine         ov                 ov     ov  
B3PW91 ov ov ov ov ov ov ov ov ov ov     ov ov       ov
mPW1PW91 ov ov ov ov ov ov ov ov ov ov     ov ov       ov
M06-2X         ov                          
PBEPBE ov ov ov ov ov ov ov ov ov ov     ov ov     ov ov
PBEPBEultrafine         ov                          
PBE1PBE         ov                          
HSEh1PBE         ov                          
TPSSh         ov   ov                      
Moller Plesset perturbation MP2 ov ov ov ov ov ov ov ov ov ov   ov ov ov   ov   ov
MP2=FULL ov ov ov ov ov ov ov ov ov ov     ov ov       ov
MP3             o                      
MP3=FULL         ov   ov                      
MP4 ov ov     ov       ov ov                
B2PLYP         ov                 ov        
B2PLYP=FULLultrafine         ov                          
Configuration interaction CID   ov     ov         ov                
CISD   ov     ov         ov                
Quadratic configuration interaction QCISD ov ov   ov ov ov ov ov ov ov     ov ov       ov
QCISD(T)         ov       ov                  
Coupled Cluster CCD ov ov   ov ov ov ov ov ov ov     ov ov       ov
CCSD         ov       ov                  
CCSD(T)         ov       ov                  

Methods with effective core potentials (select basis sets)
CEP-31G CEP-31G* CEP-121G CEP-121G* LANL2DZ SDD
hartree fock HF ov ov ov ov ov ov
density functional B1B95 ov ov        
B3LYP ov ov ov ov ov ov
Moller Plesset perturbation MP2 ov ov ov ov ov ov

Single point energy calculations (select basis sets)
6-311+G(3df,2p) cc-pVDZ cc-pVTZ aug-cc-pVDZ aug-cc-pVTZ cc-pV(T+d)Z
Moller Plesset perturbation MP2FC// HF/6-31G* e   e     e
MP2FC// B3LYP/6-31G* e e e     e
MP2FC// MP2FC/6-31G*     e e e e
MP4// HF/6-31G* e   e     e
MP4// B3LYP/6-31G*   e e     e
MP4// MP2/6-31G*     e     e
Coupled Cluster CCSD// B3LYP/6-31G* e          
CCSD(T)// B3LYP/6-31G* e   e      
CCSD(T)//B3LYP/6-31G(2df,p)     e     e
CCSD// MP2FC/6-31G*       e e  
CCSD(T)// MP2FC/6-31G*       e e  

Barriers to internal rotation or inversion


Methods with predefined basis sets
semi-empirical AM1 s1c1t1
PM3 s1c1t1

Methods with standard basis sets
3-21G 6-31G* 6-31+G** cc-pVTZ
hartree fock HF s1c1t1 s1c1t1 s1c1t1 s1c1t1
density functional B3LYP s1c1t1 s1c1t1 s1c1t1 s1c1t1
Moller Plesset perturbation MP2 s1c1t1 s1c1t1 s1c1t1 s1c1t1
For descriptions of the methods (AM1, HF, MP2, ...) and basis sets (3-21G, 3-21G*, 6-31G, ...) see the glossary in section I.C. Predefined means the basis set used is determined by the method.