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Completed calculations for CH3CH2OH (Ethanol)

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
composite G1 c1e
G2MP2 c1e
G2 c1e
G3 c1e
G3B3 c1e
G3MP2 c1e
G4 c1e
CBS-Q c1e

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 aug-cc-pVQZ cc-pV(T+d)Z aug-cc-pCVTZ Sadlej_pVTZ daug-cc-pVDZ daug-cc-pVTZ
hartree fock HF c1ov c1ov c1ov c1ov c1ov c2ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov c1ov
density functional BLYP c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov     c1ov c1ov
B1B95 c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov     c1o c1ov
B3LYP c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov c1ov
B3LYPultrafine   c1ov     c1ov c1ov c1ov c1ov   c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
B3PW91 c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov     c1ov c1ov
mPW1PW91 c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov     c1ov c1ov
M06-2X c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
PBEPBE c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov   c1ov   c1ov c1ov c1ov
PBEPBEultrafine   c1ov     c1ov c1ov c1ov c1ov   c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
PBE1PBE c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
HSEh1PBE c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
TPSSh c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov       c1ov c1ov
wB97X-D c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov       c1ov c1ov
B97D3 c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov       c1ov c1ov
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 aug-cc-pVQZ cc-pV(T+d)Z aug-cc-pCVTZ Sadlej_pVTZ daug-cc-pVDZ daug-cc-pVTZ
Moller Plesset perturbation MP2 c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c2ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov c1ov
MP2=FULL c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov     c1ov c1ov c1ov
MP3         c1ov   c1ov                                
MP3=FULL         c1ov   c1ov                                
MP4   c1ov c1o   c1ov                 c1ov                  
B2PLYP c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov c2ov         c1ov c1o
B2PLYP=FULL c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov   c1ov c1ov         c1ov c1ov
B2PLYP=FULLultrafine         c1ov                       c1ov     c1o      
Configuration interaction CID         c1ov                                    
CISD         c1ov                                    
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 aug-cc-pVQZ cc-pV(T+d)Z aug-cc-pCVTZ Sadlej_pVTZ daug-cc-pVDZ daug-cc-pVTZ
Quadratic configuration interaction QCISD   c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov c1ov     c1ov c1ov     c1ov            
QCISD(T)         c1ov                                    
Coupled Cluster CCD   c1ov c1ov c1ov c1ov c1ov c1ov c1ov         c1ov                    
CCSD         c1ov         c1ov       c1ov     c1ov            
CCSD=FULL         c1ov         c1ov       c1ov     c1ov            
CCSD(T)         c1ov c1ov                                  
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 aug-cc-pVQZ cc-pV(T+d)Z aug-cc-pCVTZ Sadlej_pVTZ daug-cc-pVDZ daug-cc-pVTZ

Methods with effective core potentials (select basis sets)
CEP-31G CEP-31G* CEP-121G CEP-121G* LANL2DZ SDD cc-pVTZ-PP aug-cc-pVTZ-PP Def2TZVPP
hartree fock HF   c1ov c1ov c1ov c1ov c1ov     c1ov
density functional BLYP                 c1ov
B1B95 c1ov c1ov             c1ov
B3LYP c1ov c1ov c1ov c1ov c1ov c1ov     c1ov
B3LYPultrafine                 c1ov
B3PW91                 c1ov
mPW1PW91                 c1ov
M06-2X                 c1ov
PBEPBE                 c1ov
PBEPBEultrafine                 c1ov
PBE1PBE                 c1ov
HSEh1PBE                 c1ov
TPSSh                 c1ov
wB97X-D c1ov c1ov c1ov c1ov c1ov c1ov     c1ov
B97D3                 c1ov
Moller Plesset perturbation MP2 c1ov c1ov c1ov c1ov c1ov c1ov     c1ov
MP2=FULL                 c1ov
B2PLYP                 c1ov
B2PLYP=FULL                 c1ov

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* c1e c1e c1e c1e c1e c1e
MP2FC// B3LYP/6-31G* c1e c1e c1e c1e c1e c1e
MP2FC// MP2FC/6-31G*   c1e c1e c1e c1e c1e
MP4// HF/6-31G* c1e c1e c1e     c1e
MP4// B3LYP/6-31G*   c1e c1e     c1e
MP4// MP2/6-31G*     c1e     c1e
Coupled Cluster CCSD// HF/6-31G* c1e c1e c1e c1e   c1e
CCSD(T)// HF/6-31G* c1e c1e c1e c1e   c1e
CCSD// B3LYP/6-31G* c1e c1e c1e     c1e
CCSD(T)// B3LYP/6-31G* c1e c1e c1e     c1e
CCSD(T)//B3LYP/6-31G(2df,p)     c1e     c1e
CCSD// MP2FC/6-31G*   c1e c1e c1e c1e c1e
CCSD(T)// MP2FC/6-31G*   c1e c1e c1e c1e c1e

Barriers to internal rotation or inversion


Methods with predefined basis sets
semi-empirical AM1 s1c1t2
PM3 s1c1t2
molecular mechanics DREIDING s1c1t2

Methods with standard basis sets
3-21G 6-31G* 6-31+G** cc-pVTZ aug-cc-pVTZ aug-cc-pCVTZ
hartree fock HF s1c1t2 s1c1t2 s1c1t2 s1c1t2    
density functional B3LYP s1c1t2 s1c1t2 s1c1t2 s1c1t2    
wB97X-D   s1c1t1   s1c1t1    
3-21G 6-31G* 6-31+G** cc-pVTZ aug-cc-pVTZ aug-cc-pCVTZ
Moller Plesset perturbation MP2 s1c1t2 s1c1t2 s1c1t2 s1c1t2 s1c1t1  
B2PLYP         s1c1t1  
B2PLYP=FULLultrafine           s1c1t1
Coupled Cluster CCSD   s1c1t1   s1c1t1    
3-21G 6-31G* 6-31+G** cc-pVTZ aug-cc-pVTZ aug-cc-pCVTZ
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.