Jump to
S1C2
Energy calculated at mPW1PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.938851 |
| Energy at 298.15K | -93.940148 |
| HF Energy | -93.938851 |
| Nuclear repulsion energy | 28.132702 |
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/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' |
3319 |
3181 |
5.24 |
|
|
|
| 2 |
A' |
3002 |
2876 |
50.01 |
|
|
|
| 3 |
A' |
1879 |
1801 |
27.51 |
|
|
|
| 4 |
A' |
1021 |
978 |
147.06 |
|
|
|
| 5 |
A' |
876 |
839 |
91.75 |
|
|
|
| 6 |
A" |
908 |
870 |
3.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5502.3 cm
-1
Scaled (by 0.9583) Zero Point Vibrational Energy (zpe) 5272.8 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 mPW1PW91/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.113 |
0.636 |
0.000 |
| N2 |
0.113 |
-0.591 |
0.000 |
| H3 |
-0.675 |
1.415 |
0.000 |
| H4 |
-0.789 |
-1.094 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2264 | 1.1078 | 1.9508 |
N2 | 1.2264 | | 2.1546 | 1.0327 | H3 | 1.1078 | 2.1546 | | 2.5116 | H4 | 1.9508 | 1.0327 | 2.5116 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.184 |
|
H3 |
C1 |
N2 |
134.690 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.049 |
|
|
|
| 2 |
N |
-0.145 |
|
|
|
| 3 |
H |
0.076 |
|
|
|
| 4 |
H |
0.118 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.111 |
0.386 |
0.000 |
2.146 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.887 |
0.595 |
0.000 |
| y |
0.595 |
-10.997 |
0.000 |
| z |
0.000 |
0.000 |
-12.393 |
|
| Traceless |
| | x | y | z |
| x |
-0.192 |
0.595 |
0.000 |
| y |
0.595 |
1.143 |
0.000 |
| z |
0.000 |
0.000 |
-0.951 |
|
| Polar |
| 3z2-r2 | -1.901 |
| x2-y2 | -0.890 |
| xy | 0.595 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.078 |
0.061 |
0.000 |
| y |
0.061 |
3.802 |
0.000 |
| z |
0.000 |
0.000 |
1.335 |
<r2> (average value of r
2) Å
2
| <r2> |
16.654 |
| (<r2>)1/2 |
4.081 |
Jump to
S1C1
Energy calculated at mPW1PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -93.946131 |
| Energy at 298.15K | -93.947473 |
| HF Energy | -93.946131 |
| Nuclear repulsion energy | 28.064053 |
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/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' |
3443 |
3300 |
6.46 |
|
|
|
| 2 |
A' |
3045 |
2918 |
27.72 |
|
|
|
| 3 |
A' |
1834 |
1757 |
27.31 |
|
|
|
| 4 |
A' |
1202 |
1152 |
9.21 |
|
|
|
| 5 |
A' |
907 |
869 |
214.90 |
|
|
|
| 6 |
A" |
976 |
935 |
110.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5703.5 cm
-1
Scaled (by 0.9583) Zero Point Vibrational Energy (zpe) 5465.6 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 mPW1PW91/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.649 |
0.000 |
| N2 |
0.000 |
-0.588 |
0.000 |
| H3 |
0.913 |
1.274 |
0.000 |
| H4 |
-0.915 |
-1.053 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2361 | 1.1067 | 1.9323 |
N2 | 1.2361 | | 2.0732 | 1.0271 | H3 | 1.1067 | 2.0732 | | 2.9594 | H4 | 1.9323 | 1.0271 | 2.9594 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
116.950 |
|
H3 |
C1 |
N2 |
124.387 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.085 |
|
|
|
| 2 |
N |
-0.140 |
|
|
|
| 3 |
H |
0.090 |
|
|
|
| 4 |
H |
0.136 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.466 |
0.140 |
0.000 |
0.486 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.040 |
2.971 |
0.000 |
| y |
2.971 |
-11.305 |
0.000 |
| z |
0.000 |
0.000 |
-12.420 |
|
| Traceless |
| | x | y | z |
| x |
0.823 |
2.971 |
0.000 |
| y |
2.971 |
0.425 |
0.000 |
| z |
0.000 |
0.000 |
-1.248 |
|
| Polar |
| 3z2-r2 | -2.496 |
| x2-y2 | 0.265 |
| xy | 2.971 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.285 |
0.501 |
0.000 |
| y |
0.501 |
3.634 |
0.000 |
| z |
0.000 |
0.000 |
1.386 |
<r2> (average value of r
2) Å
2
| <r2> |
16.582 |
| (<r2>)1/2 |
4.072 |