Jump to
S1C2
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -148.737630 |
Energy at 298.15K | -148.739938 |
Nuclear repulsion energy | 59.446142 |
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 B1B95/6-31G(2df,p)
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' |
3587 |
3436 |
42.11 |
|
|
|
2 |
A' |
2387 |
2286 |
96.79 |
|
|
|
3 |
A' |
1624 |
1555 |
39.37 |
|
|
|
4 |
A' |
1110 |
1063 |
7.04 |
|
|
|
5 |
A' |
598 |
573 |
157.59 |
|
|
|
6 |
A' |
503 |
482 |
79.10 |
|
|
|
7 |
A" |
3685 |
3529 |
61.42 |
|
|
|
8 |
A" |
1187 |
1137 |
0.22 |
|
|
|
9 |
A" |
432 |
413 |
0.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7555.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 7236.2 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.218 |
0.000 |
N2 |
-0.036 |
1.376 |
0.000 |
N3 |
0.102 |
-1.117 |
0.000 |
H4 |
-0.233 |
-1.564 |
0.840 |
H5 |
-0.233 |
-1.564 |
-0.840 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1585 | 1.3389 | 1.9842 | 1.9842 |
N2 | 1.1585 | | 2.4968 | 3.0645 | 3.0645 | N3 | 1.3389 | 2.4968 | | 1.0088 | 1.0088 | H4 | 1.9842 | 3.0645 | 1.0088 | | 1.6794 | H5 | 1.9842 | 3.0645 | 1.0088 | 1.6794 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
114.652 |
|
C1 |
N3 |
H5 |
114.652 |
N2 |
C1 |
N3 |
177.389 |
|
H4 |
N3 |
H5 |
112.690 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.330 |
|
|
|
2 |
N |
-0.312 |
|
|
|
3 |
N |
-0.614 |
|
|
|
4 |
H |
0.298 |
|
|
|
5 |
H |
0.298 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.930 |
-4.377 |
0.000 |
4.474 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.880 |
1.886 |
0.000 |
y |
1.886 |
-17.901 |
0.000 |
z |
0.000 |
0.000 |
-14.695 |
|
Traceless |
| x | y | z |
x |
-1.582 |
1.886 |
0.000 |
y |
1.886 |
-1.614 |
0.000 |
z |
0.000 |
0.000 |
3.196 |
|
Polar |
3z2-r2 | 6.391 |
x2-y2 | 0.021 |
xy | 1.886 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.010 |
-0.006 |
0.000 |
y |
-0.006 |
4.861 |
0.000 |
z |
0.000 |
0.000 |
2.391 |
<r2> (average value of r
2) Å
2
<r2> |
39.277 |
(<r2>)1/2 |
6.267 |
Jump to
S1C1
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -148.733580 |
Energy at 298.15K | |
HF Energy | -148.733580 |
Nuclear repulsion energy | 59.669970 |
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 B1B95/6-31G(2df,p)
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 |
3674 |
3519 |
71.08 |
|
|
|
2 |
A1 |
2399 |
2298 |
126.20 |
|
|
|
3 |
A1 |
1615 |
1547 |
48.91 |
|
|
|
4 |
A1 |
1150 |
1101 |
10.68 |
|
|
|
5 |
B1 |
554 |
530 |
1.26 |
|
|
|
6 |
B1 |
424i |
406i |
254.51 |
|
|
|
7 |
B2 |
3795 |
3635 |
95.66 |
|
|
|
8 |
B2 |
1130 |
1082 |
3.07 |
|
|
|
9 |
B2 |
429 |
410 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7160.7 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 6857.8 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 B1B95/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.219 |
N2 |
0.000 |
0.000 |
1.377 |
N3 |
0.000 |
0.000 |
-1.104 |
H4 |
0.000 |
0.862 |
-1.612 |
H5 |
0.000 |
-0.862 |
-1.612 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1585 | 1.3225 | 2.0238 | 2.0238 |
N2 | 1.1585 | | 2.4810 | 3.1113 | 3.1113 | N3 | 1.3225 | 2.4810 | | 1.0009 | 1.0009 | H4 | 2.0238 | 3.1113 | 1.0009 | | 1.7242 | H5 | 2.0238 | 3.1113 | 1.0009 | 1.7242 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.531 |
|
C1 |
N3 |
H5 |
120.531 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
118.937 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.352 |
|
|
|
2 |
N |
-0.323 |
|
|
|
3 |
N |
-0.636 |
|
|
|
4 |
H |
0.303 |
|
|
|
5 |
H |
0.303 |
|
|
|
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 |
-4.746 |
4.746 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.098 |
0.000 |
0.000 |
y |
0.000 |
-14.421 |
0.000 |
z |
0.000 |
0.000 |
-17.179 |
|
Traceless |
| x | y | z |
x |
-2.297 |
0.000 |
0.000 |
y |
0.000 |
3.217 |
0.000 |
z |
0.000 |
0.000 |
-0.920 |
|
Polar |
3z2-r2 | -1.840 |
x2-y2 | -3.676 |
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 |
1.940 |
0.000 |
0.000 |
y |
0.000 |
2.354 |
0.000 |
z |
0.000 |
0.000 |
4.866 |
<r2> (average value of r
2) Å
2
<r2> |
39.124 |
(<r2>)1/2 |
6.255 |