Jump to
S1C2
Energy calculated at HSEh1PBE/6-31+G**
| hartrees |
Energy at 0K | -499.248961 |
Energy at 298.15K | |
HF Energy | -499.248961 |
Nuclear repulsion energy | 45.388089 |
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 HSEh1PBE/6-31+G**
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' |
3211 |
3066 |
5.96 |
108.24 |
0.11 |
0.20 |
2 |
A' |
1429 |
1364 |
11.23 |
2.21 |
0.70 |
0.83 |
3 |
A' |
865 |
826 |
40.01 |
6.78 |
0.22 |
0.36 |
4 |
A' |
231 |
220 |
102.94 |
0.15 |
0.75 |
0.86 |
5 |
A" |
3366 |
3214 |
0.08 |
50.43 |
0.75 |
0.86 |
6 |
A" |
1013 |
967 |
0.61 |
3.74 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5057.1 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 4828.5 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 HSEh1PBE/6-31+G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.000 |
1.116 |
0.000 |
Cl2 |
-0.000 |
-0.584 |
0.000 |
H3 |
0.000 |
1.620 |
0.956 |
H4 |
0.000 |
1.620 |
-0.956 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7003 | 1.0803 | 1.0803 |
Cl2 | 1.7003 | | 2.4026 | 2.4026 | H3 | 1.0803 | 2.4026 | | 1.9110 | H4 | 1.0803 | 2.4026 | 1.9110 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.812 |
|
Br2 |
C1 |
H4 |
117.812 |
H3 |
C1 |
H4 |
124.375 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.461 |
|
|
|
2 |
Cl |
0.054 |
|
|
|
3 |
H |
0.203 |
|
|
|
4 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
1.179 |
0.000 |
1.179 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.737 |
0.000 |
0.000 |
y |
0.000 |
-17.450 |
0.000 |
z |
0.000 |
0.000 |
-18.492 |
|
Traceless |
| x | y | z |
x |
-2.766 |
0.000 |
0.000 |
y |
0.000 |
2.164 |
0.000 |
z |
0.000 |
0.000 |
0.602 |
|
Polar |
3z2-r2 | 1.204 |
x2-y2 | -3.287 |
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 |
2.412 |
0.000 |
0.000 |
y |
0.000 |
4.621 |
0.000 |
z |
0.000 |
0.000 |
2.674 |
<r2> (average value of r
2) Å
2
<r2> |
32.153 |
(<r2>)1/2 |
5.670 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31+G**
| hartrees |
Energy at 0K | -499.248961 |
Energy at 298.15K | |
HF Energy | -499.248961 |
Nuclear repulsion energy | 45.397455 |
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 HSEh1PBE/6-31+G**
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 |
3211 |
3066 |
6.00 |
108.34 |
0.11 |
0.20 |
2 |
A1 |
1429 |
1365 |
11.22 |
|
|
|
3 |
A1 |
866 |
827 |
39.92 |
|
|
|
4 |
B1 |
234 |
224 |
102.88 |
|
|
|
5 |
B2 |
3365 |
3213 |
0.07 |
|
|
|
6 |
B2 |
1013 |
967 |
0.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5059.2 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 4830.5 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 HSEh1PBE/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.115 |
Cl2 |
0.000 |
0.000 |
0.584 |
H3 |
0.000 |
0.955 |
-1.620 |
H4 |
0.000 |
-0.955 |
-1.620 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.6998 | 1.0804 | 1.0804 |
Cl2 | 1.6998 | | 2.4027 | 2.4027 | H3 | 1.0804 | 2.4027 | | 1.9103 | H4 | 1.0804 | 2.4027 | 1.9103 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.861 |
|
Br2 |
C1 |
H4 |
117.861 |
H3 |
C1 |
H4 |
124.278 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.461 |
|
|
|
2 |
Cl |
0.054 |
|
|
|
3 |
H |
0.203 |
|
|
|
4 |
H |
0.203 |
|
|
|
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 |
-1.177 |
1.177 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.736 |
0.000 |
0.000 |
y |
0.000 |
-18.494 |
0.000 |
z |
0.000 |
0.000 |
-17.449 |
|
Traceless |
| x | y | z |
x |
-2.765 |
0.000 |
0.000 |
y |
0.000 |
0.598 |
0.000 |
z |
0.000 |
0.000 |
2.167 |
|
Polar |
3z2-r2 | 4.333 |
x2-y2 | -2.242 |
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 |
2.412 |
0.000 |
0.000 |
y |
0.000 |
2.673 |
0.000 |
z |
0.000 |
0.000 |
4.621 |
<r2> (average value of r
2) Å
2
<r2> |
32.146 |
(<r2>)1/2 |
5.670 |