Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.375602 |
| Energy at 298.15K | -131.374895 |
| HF Energy | -131.375602 |
| Nuclear repulsion energy | 47.134045 |
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 B3PW91/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' |
3391 |
3272 |
42.71 |
|
|
|
| 2 |
A' |
1815 |
1752 |
34.15 |
|
|
|
| 3 |
A' |
1238 |
1194 |
7.47 |
|
|
|
| 4 |
A' |
468 |
452 |
17.41 |
|
|
|
| 5 |
A' |
370 |
357 |
28.80 |
|
|
|
| 6 |
A" |
445 |
429 |
0.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3863.1 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3727.9 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 B3PW91/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.085 |
-1.224 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
-0.165 |
1.281 |
0.000 |
| H4 |
0.645 |
-2.147 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3146 | 2.5173 | 1.0793 |
C2 | 1.3146 | | 1.2043 | 2.3259 | N3 | 2.5173 | 1.2043 | | 3.5220 | H4 | 1.0793 | 2.3259 | 3.5220 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.832 |
|
C2 |
C1 |
H4 |
152.476 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.375101 |
| Energy at 298.15K | |
| HF Energy | -131.375101 |
| Nuclear repulsion energy | 47.191044 |
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 B3PW91/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 |
Σ |
3455 |
3334 |
73.35 |
|
|
|
| 2 |
Σ |
1754 |
1693 |
36.86 |
|
|
|
| 3 |
Σ |
1276 |
1231 |
5.18 |
|
|
|
| 4 |
Π |
444 |
429 |
0.24 |
|
|
|
| 4 |
Π |
444 |
429 |
0.24 |
|
|
|
| 5 |
Π |
258i |
249i |
43.27 |
|
|
|
| 5 |
Π |
258i |
249i |
43.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3428.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3308.6 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 B3PW91/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.214 |
| C2 |
0.000 |
0.000 |
0.083 |
| N3 |
0.000 |
0.000 |
1.296 |
| H4 |
0.000 |
0.000 |
-2.288 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2978 | 2.5104 | 1.0736 |
C2 | 1.2978 | | 1.2126 | 2.3713 | N3 | 2.5104 | 1.2126 | | 3.5840 | H4 | 1.0736 | 2.3713 | 3.5840 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.028 |
|
|
|
| 2 |
C |
0.034 |
|
|
|
| 3 |
N |
-0.137 |
|
|
|
| 4 |
H |
0.076 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.134 |
3.134 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.062 |
0.000 |
0.000 |
| y |
0.000 |
-17.062 |
0.000 |
| z |
0.000 |
0.000 |
-15.066 |
|
| Traceless |
| | x | y | z |
| x |
-0.998 |
0.000 |
0.000 |
| y |
0.000 |
-0.998 |
0.000 |
| z |
0.000 |
0.000 |
1.996 |
|
| Polar |
| 3z2-r2 | 3.992 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.824 |
0.000 |
0.000 |
| y |
0.000 |
1.824 |
0.000 |
| z |
0.000 |
0.000 |
6.239 |
<r2> (average value of r
2) Å
2
| <r2> |
36.123 |
| (<r2>)1/2 |
6.010 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.346360 |
| Energy at 298.15K | -131.345808 |
| HF Energy | -131.346360 |
| Nuclear repulsion energy | 46.820559 |
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 B3PW91/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' |
3071 |
2964 |
8.01 |
|
|
|
| 2 |
A' |
2111 |
2037 |
20.75 |
|
|
|
| 3 |
A' |
1096 |
1058 |
32.59 |
|
|
|
| 4 |
A' |
944 |
911 |
44.52 |
|
|
|
| 5 |
A' |
453 |
437 |
22.45 |
|
|
|
| 6 |
A" |
314 |
303 |
9.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3995.0 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3855.2 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 B3PW91/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.089 |
-1.285 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.241 |
1.252 |
0.000 |
| H4 |
1.154 |
-1.603 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3797 | 2.5586 | 1.1106 |
C2 | 1.3797 | | 1.1852 | 2.0502 | N3 | 2.5586 | 1.1852 | | 3.1778 | H4 | 1.1106 | 2.0502 | 3.1778 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.024 |
|
|
|
| 2 |
C |
0.009 |
|
|
|
| 3 |
N |
-0.108 |
|
|
|
| 4 |
H |
0.123 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.732 |
-1.258 |
0.000 |
2.140 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.701 |
-2.335 |
0.000 |
| y |
-2.335 |
-20.683 |
0.000 |
| z |
0.000 |
0.000 |
-15.701 |
|
| Traceless |
| | x | y | z |
| x |
1.492 |
-2.335 |
0.000 |
| y |
-2.335 |
-4.483 |
0.000 |
| z |
0.000 |
0.000 |
2.991 |
|
| Polar |
| 3z2-r2 | 5.982 |
| x2-y2 | 3.983 |
| xy | -2.335 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.590 |
-0.753 |
0.000 |
| y |
-0.753 |
6.155 |
0.000 |
| z |
0.000 |
0.000 |
2.310 |
<r2> (average value of r
2) Å
2
| <r2> |
36.341 |
| (<r2>)1/2 |
6.028 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -131.346360 |
| Energy at 298.15K | -131.345808 |
| HF Energy | -131.346360 |
| Nuclear repulsion energy | 46.820559 |
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 B3PW91/cc-pVDZ
Geometric Data calculated at B3PW91/cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability