Jump to
S1C2
Energy calculated at B97D3/6-31G*
| hartrees |
Energy at 0K | -148.685754 |
Energy at 298.15K | -148.688000 |
HF Energy | -148.685754 |
Nuclear repulsion energy | |
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 B97D3/6-31G*
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' |
3459 |
3391 |
24.37 |
|
|
|
2 |
A' |
2292 |
2247 |
79.26 |
|
|
|
3 |
A' |
1637 |
1605 |
41.39 |
|
|
|
4 |
A' |
1072 |
1051 |
6.01 |
|
|
|
5 |
A' |
618 |
606 |
243.97 |
|
|
|
6 |
A' |
475 |
465 |
25.17 |
|
|
|
7 |
A" |
3553 |
3483 |
38.65 |
|
|
|
8 |
A" |
1192 |
1169 |
0.18 |
|
|
|
9 |
A" |
393 |
385 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7345.2 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 7201.3 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 B97D3/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.218 |
0.000 |
N2 |
-0.011 |
1.394 |
0.000 |
N3 |
0.089 |
-1.131 |
0.000 |
H4 |
-0.273 |
-1.573 |
0.843 |
H5 |
-0.273 |
-1.573 |
-0.843 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1761 | 1.3520 | 1.9977 | 1.9977 |
N2 | 1.1761 | | 2.5271 | 3.0949 | 3.0949 | N3 | 1.3520 | 2.5271 | | 1.0181 | 1.0181 | H4 | 1.9977 | 3.0949 | 1.0181 | | 1.6860 | H5 | 1.9977 | 3.0949 | 1.0181 | 1.6860 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
114.142 |
|
C1 |
N3 |
H5 |
114.142 |
N2 |
C1 |
N3 |
176.760 |
|
H4 |
N3 |
H5 |
111.787 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.465 |
|
|
|
2 |
N |
-0.444 |
|
|
|
3 |
N |
-0.744 |
|
|
|
4 |
H |
0.362 |
|
|
|
5 |
H |
0.362 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.196 |
-4.320 |
0.000 |
4.483 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.953 |
2.161 |
0.000 |
y |
2.161 |
-18.021 |
0.000 |
z |
0.000 |
0.000 |
-14.745 |
|
Traceless |
| x | y | z |
x |
-1.570 |
2.161 |
0.000 |
y |
2.161 |
-1.672 |
0.000 |
z |
0.000 |
0.000 |
3.242 |
|
Polar |
3z2-r2 | 6.484 |
x2-y2 | 0.068 |
xy | 2.161 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.637 |
0.042 |
0.000 |
y |
0.042 |
4.982 |
0.000 |
z |
0.000 |
0.000 |
2.131 |
<r2> (average value of r
2) Å
2
<r2> |
39.975 |
(<r2>)1/2 |
6.323 |
Jump to
S1C1
Energy calculated at B97D3/6-31G*
| hartrees |
Energy at 0K | -148.683999 |
Energy at 298.15K | |
HF Energy | -148.683999 |
Nuclear repulsion energy | |
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 B97D3/6-31G*
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
3554 |
3484 |
51.30 |
|
|
|
2 |
A1 |
2295 |
2250 |
105.72 |
|
|
|
3 |
A1 |
1612 |
1581 |
50.58 |
|
|
|
4 |
A1 |
1113 |
1091 |
10.01 |
|
|
|
5 |
B1 |
506 |
497 |
0.17 |
|
|
|
6 |
B1 |
458i |
449i |
322.35 |
|
|
|
7 |
B2 |
3664 |
3592 |
72.53 |
|
|
|
8 |
B2 |
1120 |
1098 |
4.55 |
|
|
|
9 |
B2 |
391 |
383 |
0.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6898.4 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 6763.2 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 B97D3/6-31G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.218 |
N2 |
0.000 |
0.000 |
1.396 |
N3 |
0.000 |
0.000 |
-1.116 |
H4 |
0.000 |
0.869 |
-1.633 |
H5 |
0.000 |
-0.869 |
-1.633 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1780 | 1.3346 | 2.0447 | 2.0447 |
N2 | 1.1780 | | 2.5126 | 3.1510 | 3.1510 | N3 | 1.3346 | 2.5126 | | 1.0108 | 1.0108 | H4 | 2.0447 | 3.1510 | 1.0108 | | 1.7382 | H5 | 2.0447 | 3.1510 | 1.0108 | 1.7382 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.708 |
|
C1 |
N3 |
H5 |
120.708 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
118.584 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.496 |
|
|
|
2 |
N |
-0.446 |
|
|
|
3 |
N |
-0.790 |
|
|
|
4 |
H |
0.370 |
|
|
|
5 |
H |
0.370 |
|
|
|
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 |
-4.763 |
4.763 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.263 |
0.000 |
0.000 |
y |
0.000 |
-14.418 |
0.000 |
z |
0.000 |
0.000 |
-17.063 |
|
Traceless |
| x | y | z |
x |
-2.522 |
0.000 |
0.000 |
y |
0.000 |
3.245 |
0.000 |
z |
0.000 |
0.000 |
-0.723 |
|
Polar |
3z2-r2 | -1.445 |
x2-y2 | -3.845 |
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 |
1.521 |
0.000 |
0.000 |
y |
0.000 |
2.064 |
0.000 |
z |
0.000 |
0.000 |
4.999 |
<r2> (average value of r
2) Å
2
<r2> |
39.852 |
(<r2>)1/2 |
6.313 |