Jump to
S1C2
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -499.436495 |
| Energy at 298.15K | |
| HF Energy | -499.436495 |
| Nuclear repulsion energy | 44.729935 |
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 BLYP/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' |
3091 |
3084 |
10.54 |
|
|
|
| 2 |
A' |
1382 |
1378 |
11.15 |
|
|
|
| 3 |
A' |
786 |
784 |
36.73 |
|
|
|
| 4 |
A' |
131 |
131 |
95.26 |
|
|
|
| 5 |
A" |
3245 |
3237 |
1.97 |
|
|
|
| 6 |
A" |
984 |
981 |
1.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4809.0 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4797.0 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.005 |
1.137 |
0.000 |
| Cl2 |
-0.005 |
-0.594 |
0.000 |
| H3 |
0.060 |
1.634 |
0.962 |
| H4 |
0.060 |
1.634 |
-0.962 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7306 | 1.0847 | 1.0847 |
Cl2 | 1.7306 | | 2.4275 | 2.4275 | H3 | 1.0847 | 2.4275 | | 1.9234 | H4 | 1.0847 | 2.4275 | 1.9234 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.290 |
|
Br2 |
C1 |
H4 |
117.290 |
| H3 |
C1 |
H4 |
124.910 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.495 |
|
|
|
| 2 |
Cl |
-0.002 |
|
|
|
| 3 |
H |
0.248 |
|
|
|
| 4 |
H |
0.248 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.132 |
1.124 |
0.000 |
1.132 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.944 |
0.218 |
0.000 |
| y |
0.218 |
-17.698 |
0.000 |
| z |
0.000 |
0.000 |
-18.829 |
|
| Traceless |
| | x | y | z |
| x |
-2.681 |
0.218 |
0.000 |
| y |
0.218 |
2.188 |
0.000 |
| z |
0.000 |
0.000 |
0.493 |
|
| Polar |
| 3z2-r2 | 0.985 |
| x2-y2 | -3.246 |
| xy | 0.218 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.708 |
0.024 |
0.000 |
| y |
0.024 |
4.819 |
0.000 |
| z |
0.000 |
0.000 |
2.345 |
<r2> (average value of r
2) Å
2
| <r2> |
32.912 |
| (<r2>)1/2 |
5.737 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -499.436493 |
| Energy at 298.15K | |
| HF Energy | -499.436493 |
| Nuclear repulsion energy | 44.715738 |
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 BLYP/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 |
3093 |
3086 |
10.12 |
|
|
|
| 2 |
A1 |
1380 |
1377 |
11.31 |
|
|
|
| 3 |
A1 |
784 |
782 |
36.46 |
|
|
|
| 4 |
B1 |
99i |
99i |
98.29 |
|
|
|
| 5 |
B2 |
3248 |
3240 |
1.71 |
|
|
|
| 6 |
B2 |
982 |
980 |
1.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4694.6 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4682.9 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 BLYP/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.137 |
| Cl2 |
0.000 |
0.000 |
0.594 |
| H3 |
0.000 |
0.963 |
-1.636 |
| H4 |
0.000 |
-0.963 |
-1.636 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7312 | 1.0845 | 1.0845 |
Cl2 | 1.7312 | | 2.4288 | 2.4288 | H3 | 1.0845 | 2.4288 | | 1.9263 | H4 | 1.0845 | 2.4288 | 1.9263 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.361 |
|
Br2 |
C1 |
H4 |
117.361 |
| H3 |
C1 |
H4 |
125.279 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.495 |
|
|
|
| 2 |
Cl |
-0.003 |
|
|
|
| 3 |
H |
0.249 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
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 |
-1.130 |
1.130 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.958 |
0.000 |
0.000 |
| y |
0.000 |
-18.817 |
0.000 |
| z |
0.000 |
0.000 |
-17.681 |
|
| Traceless |
| | x | y | z |
| x |
-2.709 |
0.000 |
0.000 |
| y |
0.000 |
0.503 |
0.000 |
| z |
0.000 |
0.000 |
2.206 |
|
| Polar |
| 3z2-r2 | 4.411 |
| x2-y2 | -2.141 |
| 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 |
1.705 |
0.000 |
0.000 |
| y |
0.000 |
2.343 |
0.000 |
| z |
0.000 |
0.000 |
4.818 |
<r2> (average value of r
2) Å
2
| <r2> |
32.926 |
| (<r2>)1/2 |
5.738 |