Jump to
S1C2
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -92.708505 |
| Energy at 298.15K | -92.709761 |
| HF Energy | -92.708505 |
| Nuclear repulsion energy | 27.430084 |
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 mPW1PW91/STO-3G
| 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' |
3378 |
2969 |
0.99 |
|
|
|
| 2 |
A' |
3286 |
2888 |
3.09 |
|
|
|
| 3 |
A' |
1866 |
1640 |
6.55 |
|
|
|
| 4 |
A' |
1076 |
946 |
122.64 |
|
|
|
| 5 |
A' |
918 |
806 |
76.33 |
|
|
|
| 6 |
A" |
947 |
833 |
2.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5735.4 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 5040.9 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 mPW1PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.117 |
0.652 |
0.000 |
| N2 |
0.117 |
-0.609 |
0.000 |
| H3 |
-0.673 |
1.434 |
0.000 |
| H4 |
-0.847 |
-1.083 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2609 | 1.1115 | 1.9851 |
N2 | 1.2609 | | 2.1905 | 1.0745 | H3 | 1.1115 | 2.1905 | | 2.5236 | H4 | 1.9851 | 1.0745 | 2.5236 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
116.194 |
|
H3 |
C1 |
N2 |
134.736 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.017 |
|
|
|
| 2 |
N |
-0.288 |
|
|
|
| 3 |
H |
0.089 |
|
|
|
| 4 |
H |
0.182 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.939 |
0.588 |
0.000 |
2.026 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.540 |
0.788 |
0.000 |
| y |
0.788 |
-10.705 |
0.000 |
| z |
0.000 |
0.000 |
-11.183 |
|
| Traceless |
| | x | y | z |
| x |
0.404 |
0.788 |
0.000 |
| y |
0.788 |
0.156 |
0.000 |
| z |
0.000 |
0.000 |
-0.560 |
|
| Polar |
| 3z2-r2 | -1.121 |
| x2-y2 | 0.165 |
| xy | 0.788 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.896 |
0.165 |
0.000 |
| y |
0.165 |
2.238 |
0.000 |
| z |
0.000 |
0.000 |
0.473 |
<r2> (average value of r
2) Å
2
| <r2> |
16.476 |
| (<r2>)1/2 |
4.059 |
Jump to
S1C1
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -92.720183 |
| Energy at 298.15K | -92.721508 |
| HF Energy | -92.720183 |
| Nuclear repulsion energy | 27.326641 |
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 mPW1PW91/STO-3G
| 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' |
3512 |
3087 |
1.27 |
|
|
|
| 2 |
A' |
3320 |
2918 |
0.29 |
|
|
|
| 3 |
A' |
1812 |
1592 |
7.95 |
|
|
|
| 4 |
A' |
1320 |
1160 |
15.39 |
|
|
|
| 5 |
A' |
977 |
859 |
159.62 |
|
|
|
| 6 |
A" |
1052 |
925 |
64.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5996.5 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 5270.3 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 mPW1PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.002 |
0.669 |
0.000 |
| N2 |
0.002 |
-0.606 |
0.000 |
| H3 |
0.955 |
1.247 |
0.000 |
| H4 |
-0.982 |
-1.021 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2750 | 1.1145 | 1.9562 |
N2 | 1.2750 | | 2.0833 | 1.0683 | H3 | 1.1145 | 2.0833 | | 2.9829 | H4 | 1.9562 | 1.0683 | 2.9829 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
112.899 |
|
H3 |
C1 |
N2 |
121.207 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.000 |
|
|
|
| 2 |
N |
-0.279 |
|
|
|
| 3 |
H |
0.089 |
|
|
|
| 4 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.667 |
0.312 |
0.000 |
0.736 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.877 |
2.266 |
0.000 |
| y |
2.266 |
-11.118 |
0.000 |
| z |
0.000 |
0.000 |
-11.213 |
|
| Traceless |
| | x | y | z |
| x |
1.289 |
2.266 |
0.000 |
| y |
2.266 |
-0.573 |
0.000 |
| z |
0.000 |
0.000 |
-0.715 |
|
| Polar |
| 3z2-r2 | -1.430 |
| x2-y2 | 1.241 |
| xy | 2.266 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.203 |
0.503 |
0.000 |
| y |
0.503 |
2.208 |
0.000 |
| z |
0.000 |
0.000 |
0.513 |
<r2> (average value of r
2) Å
2
| <r2> |
16.436 |
| (<r2>)1/2 |
4.054 |