Jump to
S1C2
Energy calculated at BLYP/6-311G**
| hartrees |
Energy at 0K | -93.960998 |
Energy at 298.15K | -93.962268 |
HF Energy | -93.960998 |
Nuclear repulsion energy | 28.030259 |
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 BLYP/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' |
3120 |
3108 |
21.50 |
|
|
|
2 |
A' |
2839 |
2828 |
72.96 |
|
|
|
3 |
A' |
1800 |
1793 |
17.28 |
|
|
|
4 |
A' |
956 |
952 |
159.14 |
|
|
|
5 |
A' |
864 |
860 |
92.48 |
|
|
|
6 |
A" |
865 |
861 |
4.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5221.6 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 5201.2 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.112 |
0.642 |
0.000 |
N2 |
0.112 |
-0.587 |
0.000 |
H3 |
-0.687 |
1.411 |
0.000 |
H4 |
-0.763 |
-1.149 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2292 | 1.1087 | 1.9930 |
N2 | 1.2292 | | 2.1519 | 1.0394 | H3 | 1.1087 | 2.1519 | | 2.5611 | H4 | 1.9930 | 1.0394 | 2.5611 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
122.709 |
|
H3 |
C1 |
N2 |
133.930 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.034 |
|
|
|
2 |
N |
-0.266 |
|
|
|
3 |
H |
0.111 |
|
|
|
4 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.140 |
0.182 |
0.000 |
2.148 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.259 |
0.522 |
0.000 |
y |
0.522 |
-11.279 |
0.000 |
z |
0.000 |
0.000 |
-12.622 |
|
Traceless |
| x | y | z |
x |
-0.308 |
0.522 |
0.000 |
y |
0.522 |
1.161 |
0.000 |
z |
0.000 |
0.000 |
-0.853 |
|
Polar |
3z2-r2 | -1.706 |
x2-y2 | -0.980 |
xy | 0.522 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.274 |
0.112 |
0.000 |
y |
0.112 |
4.209 |
0.000 |
z |
0.000 |
0.000 |
1.451 |
<r2> (average value of r
2) Å
2
<r2> |
16.942 |
(<r2>)1/2 |
4.116 |
Jump to
S1C1
Energy calculated at BLYP/6-311G**
| hartrees |
Energy at 0K | -93.968599 |
Energy at 298.15K | -93.969932 |
HF Energy | -93.968599 |
Nuclear repulsion energy | 27.932854 |
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 BLYP/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' |
3284 |
3271 |
0.97 |
|
|
|
2 |
A' |
2897 |
2885 |
38.74 |
|
|
|
3 |
A' |
1732 |
1725 |
17.32 |
|
|
|
4 |
A' |
1179 |
1174 |
9.88 |
|
|
|
5 |
A' |
902 |
899 |
200.56 |
|
|
|
6 |
A" |
950 |
946 |
112.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5471.5 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 5450.1 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.001 |
0.655 |
0.000 |
N2 |
-0.001 |
-0.588 |
0.000 |
H3 |
0.922 |
1.265 |
0.000 |
H4 |
-0.907 |
-1.081 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
H3 |
H4 |
C1 | | 1.2427 | 1.1066 | 1.9581 |
N2 | 1.2427 | | 2.0700 | 1.0317 | H3 | 1.1066 | 2.0700 | | 2.9748 | H4 | 1.9581 | 1.0317 | 2.9748 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N2 |
H4 |
118.548 |
|
H3 |
C1 |
N2 |
123.447 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.070 |
|
|
|
2 |
N |
-0.263 |
|
|
|
3 |
H |
0.125 |
|
|
|
4 |
H |
0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.432 |
-0.018 |
0.000 |
0.432 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.315 |
3.062 |
0.000 |
y |
3.062 |
-11.676 |
0.000 |
z |
0.000 |
0.000 |
-12.659 |
|
Traceless |
| x | y | z |
x |
0.852 |
3.062 |
0.000 |
y |
3.062 |
0.311 |
0.000 |
z |
0.000 |
0.000 |
-1.164 |
|
Polar |
3z2-r2 | -2.327 |
x2-y2 | 0.361 |
xy | 3.062 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.454 |
0.525 |
0.000 |
y |
0.525 |
3.843 |
0.000 |
z |
0.000 |
0.000 |
1.534 |
<r2> (average value of r
2) Å
2
<r2> |
16.856 |
(<r2>)1/2 |
4.106 |