Jump to
S1C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -93.861053 |
| Energy at 298.15K | -93.862344 |
| HF Energy | -93.861053 |
| Nuclear repulsion energy | 28.141363 |
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 PBE1PBE/aug-cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3347 |
3219 |
1.25 |
|
|
|
| 2 |
A' |
3007 |
2891 |
44.19 |
|
|
|
| 3 |
A' |
1862 |
1790 |
34.55 |
|
|
|
| 4 |
A' |
1012 |
974 |
143.72 |
|
|
|
| 5 |
A' |
862 |
829 |
91.84 |
|
|
|
| 6 |
A" |
897 |
863 |
3.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5493.4 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 5282.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.637 |
0.000 |
| N2 |
0.112 |
-0.590 |
0.000 |
| H3 |
-0.679 |
1.410 |
0.000 |
| H4 |
-0.779 |
-1.105 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2269 | 1.1056 | 1.9569 |
N2 | 1.2269 | | 2.1502 | 1.0291 | H3 | 1.1056 | 2.1502 | | 2.5171 | H4 | 1.9569 | 1.0291 | 2.5171 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.067 |
|
H3 |
C1 |
N2 |
134.335 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.229 |
|
|
|
| 2 |
N |
-0.138 |
|
|
|
| 3 |
H |
-0.097 |
|
|
|
| 4 |
H |
0.005 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.148 |
0.460 |
0.000 |
2.196 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.379 |
0.624 |
0.000 |
| y |
0.624 |
-11.344 |
0.000 |
| z |
0.000 |
0.000 |
-12.914 |
|
| Traceless |
| | x | y | z |
| x |
-0.250 |
0.624 |
0.000 |
| y |
0.624 |
1.303 |
0.000 |
| z |
0.000 |
0.000 |
-1.053 |
|
| Polar |
| 3z2-r2 | -2.106 |
| x2-y2 | -1.035 |
| xy | 0.624 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.045 |
0.117 |
0.000 |
| y |
0.117 |
4.551 |
0.000 |
| z |
0.000 |
0.000 |
2.370 |
<r2> (average value of r
2) Å
2
| <r2> |
16.938 |
| (<r2>)1/2 |
4.116 |
Jump to
S1C1
Energy calculated at PBE1PBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -93.868570 |
| Energy at 298.15K | -93.869909 |
| HF Energy | -93.868570 |
| Nuclear repulsion energy | 28.087118 |
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 PBE1PBE/aug-cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3468 |
3335 |
9.42 |
|
|
|
| 2 |
A' |
3053 |
2935 |
21.74 |
|
|
|
| 3 |
A' |
1822 |
1752 |
34.70 |
|
|
|
| 4 |
A' |
1177 |
1132 |
13.11 |
|
|
|
| 5 |
A' |
899 |
865 |
216.36 |
|
|
|
| 6 |
A" |
970 |
933 |
107.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5694.4 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 5475.8 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.648 |
0.000 |
| N2 |
0.000 |
-0.587 |
0.000 |
| H3 |
0.903 |
1.285 |
0.000 |
| H4 |
-0.904 |
-1.066 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2352 | 1.1043 | 1.9385 |
N2 | 1.2352 | | 2.0778 | 1.0236 | H3 | 1.1043 | 2.0778 | | 2.9652 | H4 | 1.9385 | 1.0236 | 2.9652 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
117.934 |
|
H3 |
C1 |
N2 |
125.192 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.168 |
|
|
|
| 2 |
N |
-0.095 |
|
|
|
| 3 |
H |
-0.125 |
|
|
|
| 4 |
H |
0.053 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.434 |
0.229 |
0.000 |
0.490 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.562 |
3.271 |
0.000 |
| y |
3.271 |
-11.707 |
0.000 |
| z |
0.000 |
0.000 |
-12.964 |
|
| Traceless |
| | x | y | z |
| x |
0.774 |
3.271 |
0.000 |
| y |
3.271 |
0.556 |
0.000 |
| z |
0.000 |
0.000 |
-1.329 |
|
| Polar |
| 3z2-r2 | -2.659 |
| x2-y2 | 0.146 |
| xy | 3.271 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.122 |
0.184 |
0.000 |
| y |
0.184 |
4.435 |
0.000 |
| z |
0.000 |
0.000 |
2.423 |
<r2> (average value of r
2) Å
2
| <r2> |
16.896 |
| (<r2>)1/2 |
4.110 |