Jump to
S1C2
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -147.952111 |
Energy at 298.15K | -147.954544 |
Nuclear repulsion energy | 60.136608 |
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 HF/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' |
3774 |
3429 |
53.42 |
|
|
|
2 |
A' |
2592 |
2355 |
135.01 |
|
|
|
3 |
A' |
1775 |
1613 |
51.45 |
|
|
|
4 |
A' |
1152 |
1046 |
6.80 |
|
|
|
5 |
A' |
681 |
619 |
214.66 |
|
|
|
6 |
A' |
539 |
490 |
75.00 |
|
|
|
7 |
A" |
3874 |
3520 |
71.39 |
|
|
|
8 |
A" |
1312 |
1192 |
0.07 |
|
|
|
9 |
A" |
469 |
426 |
1.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8084.0 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 7344.3 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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.227 |
0.000 |
N2 |
-0.067 |
1.356 |
0.000 |
N3 |
0.123 |
-1.108 |
0.000 |
H4 |
-0.199 |
-1.550 |
0.833 |
H5 |
-0.199 |
-1.550 |
-0.833 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1315 | 1.3401 | 1.9725 | 1.9725 |
N2 | 1.1315 | | 2.4713 | 3.0263 | 3.0263 | N3 | 1.3401 | 2.4713 | | 0.9968 | 0.9968 | H4 | 1.9725 | 3.0263 | 0.9968 | | 1.6660 | H5 | 1.9725 | 3.0263 | 0.9968 | 1.6660 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
114.342 |
|
C1 |
N3 |
H5 |
114.342 |
N2 |
C1 |
N3 |
178.090 |
|
H4 |
N3 |
H5 |
113.376 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.358 |
|
|
|
2 |
N |
-0.375 |
|
|
|
3 |
N |
-0.488 |
|
|
|
4 |
H |
0.252 |
|
|
|
5 |
H |
0.252 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.953 |
-4.522 |
0.000 |
4.621 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.424 |
2.102 |
0.000 |
y |
2.102 |
-18.830 |
0.000 |
z |
0.000 |
0.000 |
-14.994 |
|
Traceless |
| x | y | z |
x |
-1.512 |
2.102 |
0.000 |
y |
2.102 |
-2.120 |
0.000 |
z |
0.000 |
0.000 |
3.633 |
|
Polar |
3z2-r2 | 7.265 |
x2-y2 | 0.405 |
xy | 2.102 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.809 |
-0.073 |
0.000 |
y |
-0.073 |
4.497 |
0.000 |
z |
0.000 |
0.000 |
2.175 |
<r2> (average value of r
2) Å
2
<r2> |
39.062 |
(<r2>)1/2 |
6.250 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -147.950492 |
Energy at 298.15K | |
HF Energy | -147.950492 |
Nuclear repulsion energy | 60.304949 |
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 HF/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 |
3838 |
3486 |
84.09 |
|
|
|
2 |
A1 |
2579 |
2343 |
174.63 |
|
|
|
3 |
A1 |
1754 |
1594 |
59.77 |
|
|
|
4 |
A1 |
1191 |
1082 |
13.44 |
|
|
|
5 |
B1 |
601 |
546 |
5.47 |
|
|
|
6 |
B1 |
466i |
424i |
327.86 |
|
|
|
7 |
B2 |
3967 |
3604 |
114.50 |
|
|
|
8 |
B2 |
1242 |
1129 |
3.05 |
|
|
|
9 |
B2 |
464 |
421 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7585.0 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 6890.9 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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.226 |
N2 |
0.000 |
0.000 |
1.359 |
N3 |
0.000 |
0.000 |
-1.098 |
H4 |
0.000 |
0.857 |
-1.595 |
H5 |
0.000 |
-0.857 |
-1.595 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1333 | 1.3236 | 2.0126 | 2.0126 |
N2 | 1.1333 | | 2.4569 | 3.0762 | 3.0762 | N3 | 1.3236 | 2.4569 | | 0.9909 | 0.9909 | H4 | 2.0126 | 3.0762 | 0.9909 | | 1.7140 | H5 | 2.0126 | 3.0762 | 0.9909 | 1.7140 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.132 |
|
C1 |
N3 |
H5 |
120.132 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
119.736 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.384 |
|
|
|
2 |
N |
-0.381 |
|
|
|
3 |
N |
-0.540 |
|
|
|
4 |
H |
0.269 |
|
|
|
5 |
H |
0.269 |
|
|
|
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 |
-4.880 |
4.880 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.556 |
0.000 |
0.000 |
y |
0.000 |
-14.728 |
0.000 |
z |
0.000 |
0.000 |
-18.155 |
|
Traceless |
| x | y | z |
x |
-2.115 |
0.000 |
0.000 |
y |
0.000 |
3.628 |
0.000 |
z |
0.000 |
0.000 |
-1.513 |
|
Polar |
3z2-r2 | -3.026 |
x2-y2 | -3.829 |
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 |
1.743 |
0.000 |
0.000 |
y |
0.000 |
2.106 |
0.000 |
z |
0.000 |
0.000 |
4.536 |
<r2> (average value of r
2) Å
2
<r2> |
38.941 |
(<r2>)1/2 |
6.240 |