Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.949676 |
| Energy at 298.15K | -93.950970 |
| HF Energy | -93.949676 |
| Nuclear repulsion energy | 28.397670 |
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 B1B95/cc-pVTZ
| 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' |
3351 |
3207 |
2.51 |
|
|
|
| 2 |
A' |
2987 |
2859 |
47.29 |
|
|
|
| 3 |
A' |
1887 |
1806 |
28.81 |
|
|
|
| 4 |
A' |
1007 |
963 |
143.12 |
|
|
|
| 5 |
A' |
862 |
825 |
116.13 |
|
|
|
| 6 |
A" |
914 |
875 |
4.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5503.7 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 5267.6 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.110 |
0.633 |
0.000 |
| N2 |
0.110 |
-0.581 |
0.000 |
| H3 |
-0.679 |
1.393 |
0.000 |
| H4 |
-0.756 |
-1.123 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2144 | 1.0956 | 1.9585 |
N2 | 1.2144 | | 2.1259 | 1.0220 | H3 | 1.0956 | 2.1259 | | 2.5169 | H4 | 1.9585 | 1.0220 | 2.5169 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.025 |
|
H3 |
C1 |
N2 |
133.875 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.112 |
|
|
|
| 2 |
N |
-0.183 |
|
|
|
| 3 |
H |
0.118 |
|
|
|
| 4 |
H |
0.177 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.121 |
0.288 |
0.000 |
2.140 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.143 |
0.572 |
0.000 |
| y |
0.572 |
-11.038 |
0.000 |
| z |
0.000 |
0.000 |
-12.607 |
|
| Traceless |
| | x | y | z |
| x |
-0.320 |
0.572 |
0.000 |
| y |
0.572 |
1.337 |
0.000 |
| z |
0.000 |
0.000 |
-1.017 |
|
| Polar |
| 3z2-r2 | -2.034 |
| x2-y2 | -1.105 |
| xy | 0.572 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.491 |
0.077 |
0.000 |
| y |
0.077 |
4.119 |
0.000 |
| z |
0.000 |
0.000 |
1.801 |
<r2> (average value of r
2) Å
2
| <r2> |
16.613 |
| (<r2>)1/2 |
4.076 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.956905 |
| Energy at 298.15K | -93.958249 |
| HF Energy | -93.956905 |
| Nuclear repulsion energy | 28.319476 |
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 B1B95/cc-pVTZ
| 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' |
3467 |
3318 |
8.32 |
|
|
|
| 2 |
A' |
3033 |
2903 |
26.68 |
|
|
|
| 3 |
A' |
1832 |
1754 |
29.18 |
|
|
|
| 4 |
A' |
1190 |
1139 |
10.55 |
|
|
|
| 5 |
A' |
907 |
868 |
222.62 |
|
|
|
| 6 |
A" |
980 |
938 |
109.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5704.6 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 5459.9 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.644 |
0.000 |
| N2 |
-0.000 |
-0.580 |
0.000 |
| H3 |
0.898 |
1.269 |
0.000 |
| H4 |
-0.892 |
-1.070 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2245 | 1.0942 | 1.9319 |
N2 | 1.2245 | | 2.0557 | 1.0170 | H3 | 1.0942 | 2.0557 | | 2.9448 | H4 | 1.9319 | 1.0170 | 2.9448 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.764 |
|
H3 |
C1 |
N2 |
124.799 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.145 |
|
|
|
| 2 |
N |
-0.191 |
|
|
|
| 3 |
H |
0.142 |
|
|
|
| 4 |
H |
0.193 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.424 |
0.108 |
0.000 |
0.438 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.295 |
3.099 |
0.000 |
| y |
3.099 |
-11.399 |
0.000 |
| z |
0.000 |
0.000 |
-12.644 |
|
| Traceless |
| | x | y | z |
| x |
0.727 |
3.099 |
0.000 |
| y |
3.099 |
0.570 |
0.000 |
| z |
0.000 |
0.000 |
-1.297 |
|
| Polar |
| 3z2-r2 | -2.595 |
| x2-y2 | 0.104 |
| xy | 3.099 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.633 |
0.384 |
0.000 |
| y |
0.384 |
3.922 |
0.000 |
| z |
0.000 |
0.000 |
1.844 |
<r2> (average value of r
2) Å
2
| <r2> |
16.560 |
| (<r2>)1/2 |
4.069 |