All results from a given calculation for C4H2N2 (Fumaronitrile)
using model chemistry: CCSD=FULL/aug-cc-pVTZ
19 10 17 12 22
States and conformations
| State |
Conformation |
minimum conformation |
conformer description |
state description |
| 1 |
1 |
yes |
C2H |
1Ag |
Energy calculated at CCSD=FULL/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -262.689595 |
| Energy at 298.15K | |
| HF Energy | -261.583457 |
| Nuclear repulsion energy | 163.043389 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at CCSD=FULL/aug-cc-pVTZ
Geometric Data calculated at CCSD=FULL/aug-cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.335 |
0.575 |
0.000 |
| C2 |
0.335 |
-0.575 |
0.000 |
| C3 |
0.335 |
1.833 |
0.000 |
| C4 |
-0.335 |
-1.833 |
0.000 |
| N5 |
0.858 |
2.858 |
0.000 |
| N6 |
-0.858 |
-2.858 |
0.000 |
| H7 |
-1.412 |
0.594 |
0.000 |
| H8 |
1.412 |
-0.594 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
N5 |
N6 |
H7 |
H8 |
| C1 | | 1.3309 | 1.4255 | 2.4077 | 2.5767 | 3.4729 | 1.0767 | 2.1018 |
C2 | 1.3309 | | 2.4077 | 1.4255 | 3.4729 | 2.5767 | 2.1018 | 1.0767 | C3 | 1.4255 | 2.4077 | | 3.7266 | 1.1513 | 4.8408 | 2.1418 | 2.6548 | C4 | 2.4077 | 1.4255 | 3.7266 | | 4.8408 | 1.1513 | 2.6548 | 2.1418 | N5 | 2.5767 | 3.4729 | 1.1513 | 4.8408 | | 5.9691 | 3.2066 | 3.4963 | N6 | 3.4729 | 2.5767 | 4.8408 | 1.1513 | 5.9691 | | 3.4963 | 3.2066 | H7 | 1.0767 | 2.1018 | 2.1418 | 2.6548 | 3.2066 | 3.4963 | | 3.0631 | H8 | 2.1018 | 1.0767 | 2.6548 | 2.1418 | 3.4963 | 3.2066 | 3.0631 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
121.700 |
|
C1 |
C2 |
H8 |
121.256 |
| C1 |
C3 |
N5 |
178.972 |
|
C2 |
C1 |
C3 |
121.700 |
| C2 |
C1 |
H7 |
121.256 |
|
C2 |
C4 |
N6 |
178.972 |
| C3 |
C1 |
H7 |
117.044 |
|
C4 |
C2 |
H8 |
117.044 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability