Jump to
S1C2
Energy calculated at B3PW91/cc-pVTZ-PP
| | hartrees |
| Energy at 0K | -912.588429 |
| Energy at 298.15K | |
| HF Energy | -912.588429 |
| Nuclear repulsion energy | 278.668858 |
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 B3PW91/cc-pVTZ-PP
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3110 |
3110 |
0.00 |
159.44 |
0.03 |
0.07 |
| 2 |
Ag |
1482 |
1482 |
0.00 |
7.99 |
0.75 |
0.86 |
| 3 |
Ag |
1272 |
1272 |
0.00 |
39.28 |
0.44 |
0.61 |
| 4 |
Ag |
1077 |
1077 |
0.00 |
12.61 |
0.68 |
0.81 |
| 5 |
Ag |
669 |
669 |
0.00 |
97.36 |
0.27 |
0.42 |
| 6 |
Ag |
188 |
188 |
0.00 |
4.31 |
0.27 |
0.42 |
| 7 |
Au |
3194 |
3194 |
0.11 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1095 |
1095 |
3.17 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
757 |
757 |
4.44 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
101 |
101 |
4.06 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3170 |
3170 |
0.00 |
78.44 |
0.75 |
0.86 |
| 12 |
Bg |
1281 |
1281 |
0.00 |
2.23 |
0.75 |
0.86 |
| 13 |
Bg |
939 |
939 |
0.00 |
3.36 |
0.75 |
0.86 |
| 14 |
Bu |
3119 |
3119 |
5.06 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1477 |
1477 |
8.02 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1200 |
1200 |
49.55 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
601 |
601 |
70.06 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
175 |
175 |
6.62 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12452.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12452.9 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 B3PW91/cc-pVTZ-PP
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.492 |
0.567 |
0.000 |
| C2 |
-0.492 |
-0.567 |
0.000 |
| Br3 |
-0.492 |
2.264 |
0.000 |
| Br4 |
0.492 |
-2.264 |
0.000 |
| H5 |
1.113 |
0.577 |
0.890 |
| H6 |
1.113 |
0.577 |
-0.890 |
| H7 |
-1.113 |
-0.577 |
0.890 |
| H8 |
-1.113 |
-0.577 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5008 | 1.9611 | 2.8309 | 1.0858 | 1.0858 | 2.1624 | 2.1624 |
C2 | 1.5008 | | 2.8309 | 1.9611 | 2.1624 | 2.1624 | 1.0858 | 1.0858 | Br3 | 1.9611 | 2.8309 | | 4.6332 | 2.4926 | 2.4926 | 3.0412 | 3.0412 | Br4 | 2.8309 | 1.9611 | 4.6332 | | 3.0412 | 3.0412 | 2.4926 | 2.4926 | H5 | 1.0858 | 2.1624 | 2.4926 | 3.0412 | | 1.7804 | 2.5075 | 3.0753 | H6 | 1.0858 | 2.1624 | 2.4926 | 3.0412 | 1.7804 | | 3.0753 | 2.5075 | H7 | 2.1624 | 1.0858 | 3.0412 | 2.4926 | 2.5075 | 3.0753 | | 1.7804 | H8 | 2.1624 | 1.0858 | 3.0412 | 2.4926 | 3.0753 | 2.5075 | 1.7804 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.994 |
|
C1 |
C2 |
H7 |
112.448 |
| C1 |
C2 |
H8 |
112.448 |
|
C2 |
C1 |
Br3 |
108.994 |
| C2 |
C1 |
H5 |
112.448 |
|
C2 |
C1 |
H6 |
112.448 |
| Br3 |
C1 |
H5 |
106.207 |
|
Br3 |
C1 |
H6 |
106.207 |
| Br4 |
C2 |
H7 |
106.207 |
|
Br4 |
C2 |
H8 |
106.207 |
| H5 |
C1 |
H6 |
110.144 |
|
H7 |
C2 |
H8 |
110.144 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ-PP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.187 |
|
|
|
| 2 |
C |
-0.187 |
|
|
|
| 3 |
Br |
-0.100 |
|
|
|
| 4 |
Br |
-0.100 |
|
|
|
| 5 |
H |
0.143 |
|
|
|
| 6 |
H |
0.143 |
|
|
|
| 7 |
H |
0.143 |
|
|
|
| 8 |
H |
0.143 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.088 |
1.230 |
0.000 |
| y |
1.230 |
-54.665 |
0.000 |
| z |
0.000 |
0.000 |
-48.696 |
|
| Traceless |
| | x | y | z |
| x |
3.592 |
1.230 |
0.000 |
| y |
1.230 |
-6.272 |
0.000 |
| z |
0.000 |
0.000 |
2.681 |
|
| Polar |
| 3z2-r2 | 5.361 |
| x2-y2 | 6.576 |
| xy | 1.230 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.925 |
-1.847 |
0.000 |
| y |
-1.847 |
13.856 |
0.000 |
| z |
0.000 |
0.000 |
6.873 |
<r2> (average value of r
2) Å
2
| <r2> |
316.082 |
| (<r2>)1/2 |
17.779 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVTZ-PP
| | hartrees |
| Energy at 0K | -912.584722 |
| Energy at 298.15K | |
| HF Energy | -912.584722 |
| Nuclear repulsion energy | 295.084699 |
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 B3PW91/cc-pVTZ-PP
| 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 |
3150 |
3150 |
0.00 |
89.00 |
0.75 |
0.86 |
| 2 |
A |
3090 |
3090 |
13.49 |
249.81 |
0.02 |
0.03 |
| 3 |
A |
1458 |
1458 |
0.89 |
3.07 |
0.75 |
0.86 |
| 4 |
A |
1301 |
1301 |
18.75 |
3.37 |
0.38 |
0.55 |
| 5 |
A |
1186 |
1186 |
1.57 |
9.06 |
0.75 |
0.86 |
| 6 |
A |
1040 |
1040 |
1.26 |
2.03 |
0.54 |
0.70 |
| 7 |
A |
904 |
904 |
7.96 |
5.89 |
0.35 |
0.51 |
| 8 |
A |
564 |
564 |
6.90 |
18.73 |
0.06 |
0.11 |
| 9 |
A |
225 |
225 |
1.15 |
1.55 |
0.33 |
0.49 |
| 10 |
A |
76 |
76 |
0.21 |
1.02 |
0.69 |
0.82 |
| 11 |
B |
3164 |
3164 |
0.73 |
26.52 |
0.75 |
0.86 |
| 12 |
B |
3082 |
3082 |
1.97 |
48.32 |
0.75 |
0.86 |
| 13 |
B |
1454 |
1454 |
12.90 |
10.48 |
0.75 |
0.86 |
| 14 |
B |
1269 |
1269 |
63.06 |
3.41 |
0.75 |
0.86 |
| 15 |
B |
1117 |
1117 |
1.89 |
3.01 |
0.75 |
0.86 |
| 16 |
B |
844 |
844 |
19.72 |
1.10 |
0.75 |
0.86 |
| 17 |
B |
596 |
596 |
14.84 |
8.56 |
0.75 |
0.86 |
| 18 |
B |
353 |
353 |
5.69 |
2.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12436.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12436.3 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 B3PW91/cc-pVTZ-PP
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.309 |
0.685 |
1.176 |
| C2 |
-0.309 |
-0.685 |
1.176 |
| Br3 |
-0.309 |
1.808 |
-0.293 |
| Br4 |
0.309 |
-1.808 |
-0.293 |
| H5 |
0.028 |
1.214 |
2.086 |
| H6 |
1.392 |
0.646 |
1.097 |
| H7 |
-0.028 |
-1.214 |
2.086 |
| H8 |
-1.392 |
-0.646 |
1.097 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5025 | 1.9498 | 2.8930 | 1.0895 | 1.0865 | 2.1319 | 2.1617 |
C2 | 1.5025 | | 2.8930 | 1.9498 | 2.1319 | 2.1617 | 1.0895 | 1.0865 | Br3 | 1.9498 | 2.8930 | | 3.6684 | 2.4748 | 2.4850 | 3.8557 | 3.0210 | Br4 | 2.8930 | 1.9498 | 3.6684 | | 3.8557 | 3.0210 | 2.4748 | 2.4850 | H5 | 1.0895 | 2.1319 | 2.4748 | 3.8557 | | 1.7782 | 2.4278 | 2.5407 | H6 | 1.0865 | 2.1617 | 2.4850 | 3.0210 | 1.7782 | | 2.5407 | 3.0700 | H7 | 2.1319 | 1.0895 | 3.8557 | 2.4748 | 2.4278 | 2.5407 | | 1.7782 | H8 | 2.1617 | 1.0865 | 3.0210 | 2.4850 | 2.5407 | 3.0700 | 1.7782 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.226 |
|
C1 |
C2 |
H7 |
109.640 |
| C1 |
C2 |
H8 |
112.228 |
|
C2 |
C1 |
Br3 |
113.226 |
| C2 |
C1 |
H5 |
109.640 |
|
C2 |
C1 |
H6 |
112.228 |
| Br3 |
C1 |
H5 |
105.511 |
|
Br3 |
C1 |
H6 |
106.353 |
| Br4 |
C2 |
H7 |
105.511 |
|
Br4 |
C2 |
H8 |
106.353 |
| H5 |
C1 |
H6 |
109.605 |
|
H7 |
C2 |
H8 |
109.605 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ-PP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.192 |
|
|
|
| 2 |
C |
-0.192 |
|
|
|
| 3 |
Br |
-0.082 |
|
|
|
| 4 |
Br |
-0.082 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
| 6 |
H |
0.141 |
|
|
|
| 7 |
H |
0.134 |
|
|
|
| 8 |
H |
0.141 |
|
|
|
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 |
2.531 |
2.531 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.460 |
0.852 |
0.000 |
| y |
0.852 |
-52.848 |
0.000 |
| z |
0.000 |
0.000 |
-44.365 |
|
| Traceless |
| | x | y | z |
| x |
0.147 |
0.852 |
0.000 |
| y |
0.852 |
-6.436 |
0.000 |
| z |
0.000 |
0.000 |
6.289 |
|
| Polar |
| 3z2-r2 | 12.578 |
| x2-y2 | 4.389 |
| xy | 0.852 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.254 |
-0.729 |
0.000 |
| y |
-0.729 |
10.692 |
0.000 |
| z |
0.000 |
0.000 |
9.150 |
<r2> (average value of r
2) Å
2
| <r2> |
244.960 |
| (<r2>)1/2 |
15.651 |