Jump to
S1C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -93.869294 |
| Energy at 298.15K | -93.870564 |
| HF Energy | -93.869294 |
| Nuclear repulsion energy | 28.046716 |
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 PBEPBE/6-311G**
| 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' |
3169 |
3141 |
16.84 |
|
|
|
| 2 |
A' |
2871 |
2845 |
67.31 |
|
|
|
| 3 |
A' |
1818 |
1801 |
18.49 |
|
|
|
| 4 |
A' |
956 |
948 |
146.93 |
|
|
|
| 5 |
A' |
852 |
844 |
101.45 |
|
|
|
| 6 |
A" |
873 |
865 |
4.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5269.5 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 5221.6 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 PBEPBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.640 |
0.000 |
| N2 |
0.112 |
-0.588 |
0.000 |
| H3 |
-0.683 |
1.415 |
0.000 |
| H4 |
-0.768 |
-1.139 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2285 | 1.1096 | 1.9850 |
N2 | 1.2285 | | 2.1549 | 1.0380 | H3 | 1.1096 | 2.1549 | | 2.5554 | H4 | 1.9850 | 1.0380 | 2.5554 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.049 |
|
H3 |
C1 |
N2 |
134.275 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.036 |
|
|
|
| 2 |
N |
-0.281 |
|
|
|
| 3 |
H |
0.124 |
|
|
|
| 4 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.167 |
0.213 |
0.000 |
2.177 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.181 |
0.542 |
0.000 |
| y |
0.542 |
-11.186 |
0.000 |
| z |
0.000 |
0.000 |
-12.597 |
|
| Traceless |
| | x | y | z |
| x |
-0.289 |
0.542 |
0.000 |
| y |
0.542 |
1.202 |
0.000 |
| z |
0.000 |
0.000 |
-0.913 |
|
| Polar |
| 3z2-r2 | -1.827 |
| x2-y2 | -0.994 |
| xy | 0.542 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.268 |
0.102 |
0.000 |
| y |
0.102 |
4.180 |
0.000 |
| z |
0.000 |
0.000 |
1.453 |
<r2> (average value of r
2) Å
2
| <r2> |
16.887 |
| (<r2>)1/2 |
4.109 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -93.876900 |
| Energy at 298.15K | -93.878231 |
| HF Energy | -93.876900 |
| Nuclear repulsion energy | 27.959259 |
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 PBEPBE/6-311G**
| 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' |
3322 |
3292 |
1.70 |
|
|
|
| 2 |
A' |
2925 |
2899 |
34.49 |
|
|
|
| 3 |
A' |
1757 |
1741 |
18.46 |
|
|
|
| 4 |
A' |
1170 |
1160 |
9.22 |
|
|
|
| 5 |
A' |
892 |
884 |
203.07 |
|
|
|
| 6 |
A" |
955 |
946 |
112.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5510.9 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 5460.8 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 PBEPBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.654 |
0.000 |
| N2 |
-0.001 |
-0.588 |
0.000 |
| H3 |
0.922 |
1.266 |
0.000 |
| H4 |
-0.910 |
-1.074 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2412 | 1.1077 | 1.9520 |
N2 | 1.2412 | | 2.0708 | 1.0310 | H3 | 1.1077 | 2.0708 | | 2.9719 | H4 | 1.9520 | 1.0310 | 2.9719 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.131 |
|
H3 |
C1 |
N2 |
123.579 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.076 |
|
|
|
| 2 |
N |
-0.275 |
|
|
|
| 3 |
H |
0.139 |
|
|
|
| 4 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.444 |
0.002 |
0.000 |
0.444 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.228 |
3.112 |
0.000 |
| y |
3.112 |
-11.600 |
0.000 |
| z |
0.000 |
0.000 |
-12.638 |
|
| Traceless |
| | x | y | z |
| x |
0.891 |
3.112 |
0.000 |
| y |
3.112 |
0.333 |
0.000 |
| z |
0.000 |
0.000 |
-1.224 |
|
| Polar |
| 3z2-r2 | -2.448 |
| x2-y2 | 0.372 |
| xy | 3.112 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.445 |
0.500 |
0.000 |
| y |
0.500 |
3.838 |
0.000 |
| z |
0.000 |
0.000 |
1.533 |
<r2> (average value of r
2) Å
2
| <r2> |
16.798 |
| (<r2>)1/2 |
4.099 |