Jump to
S1C2
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -499.476062 |
Energy at 298.15K | |
HF Energy | -499.476062 |
Nuclear repulsion energy | 45.098863 |
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 B3LYPultrafine/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' |
3169 |
3062 |
10.00 |
103.35 |
0.15 |
0.26 |
2 |
A' |
1422 |
1374 |
11.50 |
2.09 |
0.71 |
0.83 |
3 |
A' |
823 |
796 |
39.54 |
7.52 |
0.33 |
0.50 |
4 |
A' |
119 |
115 |
95.65 |
0.17 |
0.11 |
0.20 |
5 |
A" |
3324 |
3212 |
0.98 |
53.55 |
0.75 |
0.86 |
6 |
A" |
1010 |
976 |
1.00 |
3.89 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4933.4 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4767.1 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 B3LYPultrafine/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.004 |
1.126 |
0.000 |
Cl2 |
-0.004 |
-0.589 |
0.000 |
H3 |
0.049 |
1.624 |
0.955 |
H4 |
0.049 |
1.624 |
-0.955 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7152 | 1.0782 | 1.0782 |
Cl2 | 1.7152 | | 2.4109 | 2.4109 | H3 | 1.0782 | 2.4109 | | 1.9096 | H4 | 1.0782 | 2.4109 | 1.9096 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.507 |
|
Br2 |
C1 |
H4 |
117.507 |
H3 |
C1 |
H4 |
124.647 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.509 |
|
|
|
2 |
Cl |
-0.011 |
|
|
|
3 |
H |
0.260 |
|
|
|
4 |
H |
0.260 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.108 |
1.215 |
0.000 |
1.220 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.854 |
0.178 |
0.000 |
y |
0.178 |
-17.570 |
0.000 |
z |
0.000 |
0.000 |
-18.717 |
|
Traceless |
| x | y | z |
x |
-2.710 |
0.178 |
0.000 |
y |
0.178 |
2.216 |
0.000 |
z |
0.000 |
0.000 |
0.494 |
|
Polar |
3z2-r2 | 0.989 |
x2-y2 | -3.284 |
xy | 0.178 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.676 |
0.019 |
0.000 |
y |
0.019 |
4.614 |
0.000 |
z |
0.000 |
0.000 |
2.283 |
<r2> (average value of r
2) Å
2
<r2> |
32.508 |
(<r2>)1/2 |
5.702 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -499.476061 |
Energy at 298.15K | |
HF Energy | -499.476061 |
Nuclear repulsion energy | 45.104195 |
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 B3LYPultrafine/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 |
3170 |
3063 |
9.77 |
103.08 |
0.15 |
0.26 |
2 |
A1 |
1422 |
1374 |
11.58 |
|
|
|
3 |
A1 |
824 |
796 |
39.25 |
|
|
|
4 |
B1 |
72i |
70i |
97.72 |
|
|
|
5 |
B2 |
3326 |
3214 |
0.89 |
|
|
|
6 |
B2 |
1009 |
975 |
1.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4839.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4676.0 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 B3LYPultrafine/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.126 |
Cl2 |
0.000 |
0.000 |
0.589 |
H3 |
0.000 |
0.955 |
-1.626 |
H4 |
0.000 |
-0.955 |
-1.626 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7148 | 1.0780 | 1.0780 |
Cl2 | 1.7148 | | 2.4116 | 2.4116 | H3 | 1.0780 | 2.4116 | | 1.9107 | H4 | 1.0780 | 2.4116 | 1.9107 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.599 |
|
Br2 |
C1 |
H4 |
117.599 |
H3 |
C1 |
H4 |
124.801 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.510 |
|
|
|
2 |
Cl |
-0.011 |
|
|
|
3 |
H |
0.260 |
|
|
|
4 |
H |
0.260 |
|
|
|
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 |
-1.216 |
1.216 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.861 |
0.000 |
0.000 |
y |
0.000 |
-18.711 |
0.000 |
z |
0.000 |
0.000 |
-17.559 |
|
Traceless |
| x | y | z |
x |
-2.726 |
0.000 |
0.000 |
y |
0.000 |
0.499 |
0.000 |
z |
0.000 |
0.000 |
2.227 |
|
Polar |
3z2-r2 | 4.454 |
x2-y2 | -2.150 |
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 |
1.674 |
0.000 |
0.000 |
y |
0.000 |
2.281 |
0.000 |
z |
0.000 |
0.000 |
4.613 |
<r2> (average value of r
2) Å
2
<r2> |
32.505 |
(<r2>)1/2 |
5.701 |