Jump to
S1C2
Energy calculated at B3LYP/CEP-31G*
| | hartrees |
| Energy at 0K | -21.713673 |
| Energy at 298.15K | |
| HF Energy | -21.713673 |
| Nuclear repulsion energy | 15.718100 |
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 B3LYP/CEP-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' |
3172 |
3064 |
15.78 |
|
|
|
| 2 |
A' |
1398 |
1350 |
16.75 |
|
|
|
| 3 |
A' |
821 |
792 |
41.58 |
|
|
|
| 4 |
A' |
107 |
103 |
137.46 |
|
|
|
| 5 |
A" |
3326 |
3212 |
5.67 |
|
|
|
| 6 |
A" |
984 |
950 |
0.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4904.2 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 4736.0 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 B3LYP/CEP-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
1.141 |
0.000 |
| Cl2 |
-0.004 |
-0.596 |
0.000 |
| H3 |
0.048 |
1.643 |
0.967 |
| H4 |
0.048 |
1.643 |
-0.967 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7375 | 1.0910 | 1.0910 |
Cl2 | 1.7375 | | 2.4398 | 2.4398 | H3 | 1.0910 | 2.4398 | | 1.9348 | H4 | 1.0910 | 2.4398 | 1.9348 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.376 |
|
Br2 |
C1 |
H4 |
117.376 |
| H3 |
C1 |
H4 |
124.922 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.403 |
|
|
|
| 2 |
Cl |
-0.064 |
|
|
|
| 3 |
H |
0.234 |
|
|
|
| 4 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.127 |
1.302 |
0.000 |
1.308 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.908 |
0.215 |
0.000 |
| y |
0.215 |
-16.206 |
0.000 |
| z |
0.000 |
0.000 |
-17.583 |
|
| Traceless |
| | x | y | z |
| x |
-3.013 |
0.215 |
0.000 |
| y |
0.215 |
2.539 |
0.000 |
| z |
0.000 |
0.000 |
0.474 |
|
| Polar |
| 3z2-r2 | 0.948 |
| x2-y2 | -3.701 |
| xy | 0.215 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.565 |
0.012 |
0.000 |
| y |
0.012 |
4.517 |
0.000 |
| z |
0.000 |
0.000 |
2.041 |
<r2> (average value of r
2) Å
2
| <r2> |
26.153 |
| (<r2>)1/2 |
5.114 |
Jump to
S1C1
Energy calculated at B3LYP/CEP-31G*
| | hartrees |
| Energy at 0K | -21.713671 |
| Energy at 298.15K | |
| HF Energy | -21.713671 |
| Nuclear repulsion energy | 15.714865 |
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 B3LYP/CEP-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 |
3174 |
3065 |
15.47 |
|
|
|
| 2 |
A1 |
1397 |
1349 |
16.91 |
|
|
|
| 3 |
A1 |
819 |
791 |
41.40 |
|
|
|
| 4 |
B1 |
89i |
85i |
141.19 |
|
|
|
| 5 |
B2 |
3329 |
3215 |
5.31 |
|
|
|
| 6 |
B2 |
983 |
949 |
0.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4806.7 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 4641.8 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 B3LYP/CEP-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.142 |
| Cl2 |
0.000 |
0.000 |
0.596 |
| H3 |
0.000 |
0.968 |
-1.644 |
| H4 |
0.000 |
-0.968 |
-1.644 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7380 | 1.0908 | 1.0908 |
Cl2 | 1.7380 | | 2.4405 | 2.4405 | H3 | 1.0908 | 2.4405 | | 1.9368 | H4 | 1.0908 | 2.4405 | 1.9368 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.409 |
|
Br2 |
C1 |
H4 |
117.409 |
| H3 |
C1 |
H4 |
125.183 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.405 |
|
|
|
| 2 |
Cl |
-0.064 |
|
|
|
| 3 |
H |
0.235 |
|
|
|
| 4 |
H |
0.235 |
|
|
|
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 |
-1.307 |
1.307 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.917 |
0.000 |
0.000 |
| y |
0.000 |
-17.575 |
0.000 |
| z |
0.000 |
0.000 |
-16.194 |
|
| Traceless |
| | x | y | z |
| x |
-3.033 |
0.000 |
0.000 |
| y |
0.000 |
0.481 |
0.000 |
| z |
0.000 |
0.000 |
2.552 |
|
| Polar |
| 3z2-r2 | 5.104 |
| x2-y2 | -2.343 |
| 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 |
1.564 |
0.000 |
0.000 |
| y |
0.000 |
2.038 |
0.000 |
| z |
0.000 |
0.000 |
4.517 |
<r2> (average value of r
2) Å
2
| <r2> |
26.160 |
| (<r2>)1/2 |
5.115 |