Jump to
S1C2
Energy calculated at B3LYP/CEP-31G
| | hartrees |
| Energy at 0K | -16.622434 |
| Energy at 298.15K | -16.623670 |
| HF Energy | -16.622434 |
| Nuclear repulsion energy | 15.319545 |
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 B3LYP/CEP-31G
| 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 |
3217 |
4.82 |
|
|
|
| 2 |
A' |
2970 |
2876 |
70.21 |
|
|
|
| 3 |
A' |
1784 |
1728 |
25.85 |
|
|
|
| 4 |
A' |
961 |
931 |
72.48 |
|
|
|
| 5 |
A' |
756 |
732 |
255.37 |
|
|
|
| 6 |
A" |
886 |
858 |
7.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5338.9 cm
-1
Scaled (by 0.9684) Zero Point Vibrational Energy (zpe) 5170.2 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 B3LYP/CEP-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.107 |
0.660 |
0.000 |
| N2 |
0.107 |
-0.594 |
0.000 |
| H3 |
-0.686 |
1.441 |
0.000 |
| H4 |
-0.704 |
-1.242 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2548 | 1.1126 | 2.0677 |
N2 | 1.2548 | | 2.1846 | 1.0375 | H3 | 1.1126 | 2.1846 | | 2.6832 | H4 | 2.0677 | 1.0375 | 2.6832 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
128.606 |
|
H3 |
C1 |
N2 |
134.587 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.372 |
|
|
|
| 2 |
N |
-0.074 |
|
|
|
| 3 |
H |
0.187 |
|
|
|
| 4 |
H |
0.259 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.836 |
0.260 |
0.000 |
2.848 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.488 |
0.535 |
0.000 |
| y |
0.535 |
-10.780 |
0.000 |
| z |
0.000 |
0.000 |
-12.713 |
|
| Traceless |
| | x | y | z |
| x |
-0.741 |
0.535 |
0.000 |
| y |
0.535 |
1.821 |
0.000 |
| z |
0.000 |
0.000 |
-1.079 |
|
| Polar |
| 3z2-r2 | -2.158 |
| x2-y2 | -1.708 |
| xy | 0.535 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.707 |
0.254 |
0.000 |
| y |
0.254 |
4.201 |
0.000 |
| z |
0.000 |
0.000 |
1.358 |
<r2> (average value of r
2) Å
2
| <r2> |
15.690 |
| (<r2>)1/2 |
3.961 |
Jump to
S1C1
Energy calculated at B3LYP/CEP-31G
| | hartrees |
| Energy at 0K | -16.633115 |
| Energy at 298.15K | -16.634445 |
| HF Energy | -16.633115 |
| Nuclear repulsion energy | 15.289741 |
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 B3LYP/CEP-31G
| 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' |
3452 |
3343 |
1.48 |
|
|
|
| 2 |
A' |
3063 |
2967 |
36.07 |
|
|
|
| 3 |
A' |
1705 |
1652 |
26.00 |
|
|
|
| 4 |
A' |
1177 |
1140 |
10.68 |
|
|
|
| 5 |
A' |
887 |
859 |
277.27 |
|
|
|
| 6 |
A" |
979 |
948 |
166.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5631.7 cm
-1
Scaled (by 0.9684) Zero Point Vibrational Energy (zpe) 5453.8 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 B3LYP/CEP-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.672 |
0.000 |
| N2 |
-0.002 |
-0.598 |
0.000 |
| H3 |
0.911 |
1.299 |
0.000 |
| H4 |
-0.881 |
-1.140 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2701 | 1.1078 | 2.0135 |
N2 | 1.2701 | | 2.1056 | 1.0323 | H3 | 1.1078 | 2.1056 | | 3.0263 | H4 | 2.0135 | 1.0323 | 3.0263 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
121.636 |
|
H3 |
C1 |
N2 |
124.485 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.379 |
|
|
|
| 2 |
N |
-0.083 |
|
|
|
| 3 |
H |
0.193 |
|
|
|
| 4 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.458 |
0.134 |
0.000 |
0.477 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.363 |
3.868 |
0.000 |
| y |
3.868 |
-11.494 |
0.000 |
| z |
0.000 |
0.000 |
-12.808 |
|
| Traceless |
| | x | y | z |
| x |
0.788 |
3.868 |
0.000 |
| y |
3.868 |
0.591 |
0.000 |
| z |
0.000 |
0.000 |
-1.379 |
|
| Polar |
| 3z2-r2 | -2.759 |
| x2-y2 | 0.131 |
| xy | 3.868 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.075 |
0.246 |
0.000 |
| y |
0.246 |
4.009 |
0.000 |
| z |
0.000 |
0.000 |
1.437 |
<r2> (average value of r
2) Å
2
| <r2> |
15.612 |
| (<r2>)1/2 |
3.951 |