Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -148.759817 |
Energy at 298.15K | -148.762107 |
Nuclear repulsion energy | 59.448140 |
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 B3PW91/6-311G*
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' |
3577 |
3444 |
33.65 |
|
|
|
2 |
A' |
2374 |
2285 |
104.29 |
|
|
|
3 |
A' |
1679 |
1616 |
55.15 |
|
|
|
4 |
A' |
1109 |
1068 |
7.29 |
|
|
|
5 |
A' |
585 |
563 |
197.79 |
|
|
|
6 |
A' |
500 |
482 |
97.66 |
|
|
|
7 |
A" |
3670 |
3533 |
48.21 |
|
|
|
8 |
A" |
1216 |
1170 |
0.64 |
|
|
|
9 |
A" |
420 |
405 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7564.9 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 7282.7 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.219 |
0.000 |
N2 |
-0.021 |
1.377 |
0.000 |
N3 |
0.087 |
-1.116 |
0.000 |
H4 |
-0.232 |
-1.571 |
0.843 |
H5 |
-0.232 |
-1.571 |
-0.843 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1578 | 1.3382 | 1.9919 | 1.9919 |
N2 | 1.1578 | | 2.4953 | 3.0728 | 3.0728 | N3 | 1.3382 | 2.4953 | | 1.0096 | 1.0096 | H4 | 1.9919 | 3.0728 | 1.0096 | | 1.6856 | H5 | 1.9919 | 3.0728 | 1.0096 | 1.6856 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
115.372 |
|
C1 |
N3 |
H5 |
115.372 |
N2 |
C1 |
N3 |
177.295 |
|
H4 |
N3 |
H5 |
113.197 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.341 |
|
|
|
2 |
N |
-0.313 |
|
|
|
3 |
N |
-0.785 |
|
|
|
4 |
H |
0.378 |
|
|
|
5 |
H |
0.378 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.066 |
-4.522 |
0.000 |
4.646 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.338 |
2.003 |
0.000 |
y |
2.003 |
-18.252 |
0.000 |
z |
0.000 |
0.000 |
-14.825 |
|
Traceless |
| x | y | z |
x |
-1.799 |
2.003 |
0.000 |
y |
2.003 |
-1.671 |
0.000 |
z |
0.000 |
0.000 |
3.470 |
|
Polar |
3z2-r2 | 6.940 |
x2-y2 | -0.085 |
xy | 2.003 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.845 |
0.000 |
0.000 |
y |
0.000 |
4.896 |
0.000 |
z |
0.000 |
0.000 |
2.225 |
<r2> (average value of r
2) Å
2
<r2> |
39.500 |
(<r2>)1/2 |
6.285 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -148.758722 |
Energy at 298.15K | |
HF Energy | -148.758722 |
Nuclear repulsion energy | 59.579180 |
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 B3PW91/6-311G*
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
3640 |
3505 |
55.40 |
|
|
|
2 |
A1 |
2373 |
2285 |
129.65 |
|
|
|
3 |
A1 |
1652 |
1591 |
60.53 |
|
|
|
4 |
A1 |
1141 |
1099 |
10.46 |
|
|
|
5 |
B1 |
543 |
523 |
0.65 |
|
|
|
6 |
B1 |
405i |
390i |
332.77 |
|
|
|
7 |
B2 |
3754 |
3614 |
76.98 |
|
|
|
8 |
B2 |
1153 |
1110 |
4.71 |
|
|
|
9 |
B2 |
415 |
400 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7133.7 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 6867.6 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 B3PW91/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.220 |
N2 |
0.000 |
0.000 |
1.379 |
N3 |
0.000 |
0.000 |
-1.105 |
H4 |
0.000 |
0.864 |
-1.617 |
H5 |
0.000 |
-0.864 |
-1.617 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1593 | 1.3246 | 2.0294 | 2.0294 |
N2 | 1.1593 | | 2.4839 | 3.1176 | 3.1176 | N3 | 1.3246 | 2.4839 | | 1.0041 | 1.0041 | H4 | 2.0294 | 3.1176 | 1.0041 | | 1.7280 | H5 | 2.0294 | 3.1176 | 1.0041 | 1.7280 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.632 |
|
C1 |
N3 |
H5 |
120.632 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
118.736 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.363 |
|
|
|
2 |
N |
-0.320 |
|
|
|
3 |
N |
-0.820 |
|
|
|
4 |
H |
0.388 |
|
|
|
5 |
H |
0.388 |
|
|
|
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 |
-4.881 |
4.881 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.567 |
0.000 |
0.000 |
y |
0.000 |
-14.576 |
0.000 |
z |
0.000 |
0.000 |
-17.496 |
|
Traceless |
| x | y | z |
x |
-2.531 |
0.000 |
0.000 |
y |
0.000 |
3.455 |
0.000 |
z |
0.000 |
0.000 |
-0.924 |
|
Polar |
3z2-r2 | -1.849 |
x2-y2 | -3.991 |
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 |
1.776 |
0.000 |
0.000 |
y |
0.000 |
2.154 |
0.000 |
z |
0.000 |
0.000 |
4.924 |
<r2> (average value of r
2) Å
2
<r2> |
39.409 |
(<r2>)1/2 |
6.278 |