Jump to
S1C2
Energy calculated at TPSSh/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -5226.735684 |
| Energy at 298.15K | |
| HF Energy | -5226.735684 |
| Nuclear repulsion energy | 414.988327 |
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 TPSSh/aug-cc-pVDZ
| 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 |
3008 |
0.00 |
164.55 |
0.02 |
0.05 |
| 2 |
Ag |
1475 |
1427 |
0.00 |
5.35 |
0.75 |
0.86 |
| 3 |
Ag |
1257 |
1216 |
0.00 |
49.00 |
0.30 |
0.47 |
| 4 |
Ag |
1072 |
1037 |
0.00 |
10.34 |
0.73 |
0.84 |
| 5 |
Ag |
643 |
622 |
0.00 |
120.37 |
0.25 |
0.41 |
| 6 |
Ag |
186 |
180 |
0.00 |
5.19 |
0.22 |
0.36 |
| 7 |
Au |
3201 |
3096 |
0.32 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1081 |
1046 |
2.33 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
748 |
723 |
2.73 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
101 |
98 |
4.67 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3179 |
3075 |
0.00 |
74.58 |
0.75 |
0.86 |
| 12 |
Bg |
1272 |
1231 |
0.00 |
1.79 |
0.75 |
0.86 |
| 13 |
Bg |
933 |
902 |
0.00 |
1.00 |
0.75 |
0.86 |
| 14 |
Bu |
3117 |
3015 |
5.66 |
0.00 |
0.02 |
0.04 |
| 15 |
Bu |
1465 |
1417 |
5.80 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1182 |
1143 |
56.59 |
0.00 |
0.33 |
0.50 |
| 17 |
Bu |
580 |
561 |
87.36 |
0.00 |
0.25 |
0.41 |
| 18 |
Bu |
172 |
167 |
7.93 |
0.00 |
0.21 |
0.35 |
Unscaled Zero Point Vibrational Energy (zpe) 12386.0 cm
-1
Scaled (by 0.9673) Zero Point Vibrational Energy (zpe) 11981.0 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 TPSSh/aug-cc-pVDZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.499 |
0.566 |
0.000 |
| C2 |
-0.499 |
-0.566 |
0.000 |
| Br3 |
-0.499 |
2.274 |
0.000 |
| Br4 |
0.499 |
-2.274 |
0.000 |
| H5 |
1.119 |
0.579 |
0.900 |
| H6 |
1.119 |
0.579 |
-0.900 |
| H7 |
-1.119 |
-0.579 |
0.900 |
| H8 |
-1.119 |
-0.579 |
-0.900 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5104 | 1.9783 | 2.8405 | 1.0927 | 1.0927 | 2.1772 | 2.1772 |
C2 | 1.5104 | | 2.8405 | 1.9783 | 2.1772 | 2.1772 | 1.0927 | 1.0927 | Br3 | 1.9783 | 2.8405 | | 4.6564 | 2.5104 | 2.5104 | 3.0549 | 3.0549 | Br4 | 2.8405 | 1.9783 | 4.6564 | | 3.0549 | 3.0549 | 2.5104 | 2.5104 | H5 | 1.0927 | 2.1772 | 2.5104 | 3.0549 | | 1.8006 | 2.5188 | 3.0963 | H6 | 1.0927 | 2.1772 | 2.5104 | 3.0549 | 1.8006 | | 3.0963 | 2.5188 | H7 | 2.1772 | 1.0927 | 3.0549 | 2.5104 | 2.5188 | 3.0963 | | 1.8006 | H8 | 2.1772 | 1.0927 | 3.0549 | 2.5104 | 3.0963 | 2.5188 | 1.8006 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.270 |
|
C1 |
C2 |
H7 |
112.531 |
| C1 |
C2 |
H8 |
112.531 |
|
C2 |
C1 |
Br3 |
108.270 |
| C2 |
C1 |
H5 |
112.531 |
|
C2 |
C1 |
H6 |
112.531 |
| Br3 |
C1 |
H5 |
106.041 |
|
Br3 |
C1 |
H6 |
106.041 |
| Br4 |
C2 |
H7 |
106.041 |
|
Br4 |
C2 |
H8 |
106.041 |
| H5 |
C1 |
H6 |
110.963 |
|
H7 |
C2 |
H8 |
110.963 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.072 |
|
|
|
| 2 |
C |
0.072 |
|
|
|
| 3 |
Br |
0.151 |
|
|
|
| 4 |
Br |
0.151 |
|
|
|
| 5 |
H |
-0.111 |
|
|
|
| 6 |
H |
-0.111 |
|
|
|
| 7 |
H |
-0.111 |
|
|
|
| 8 |
H |
-0.111 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.177 |
-1.777 |
0.000 |
| y |
-1.777 |
15.202 |
0.000 |
| z |
0.000 |
0.000 |
8.248 |
<r2> (average value of r
2) Å
2
| <r2> |
428.147 |
| (<r2>)1/2 |
20.692 |
Jump to
S1C1
Energy calculated at TPSSh/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -5226.731632 |
| Energy at 298.15K | |
| HF Energy | -5226.731632 |
| Nuclear repulsion energy | 449.959533 |
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 TPSSh/aug-cc-pVDZ
| 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 |
3155 |
3052 |
0.04 |
87.06 |
0.75 |
0.86 |
| 2 |
A |
3085 |
2985 |
17.68 |
274.15 |
0.02 |
0.04 |
| 3 |
A |
1450 |
1402 |
0.38 |
2.83 |
0.75 |
0.85 |
| 4 |
A |
1290 |
1248 |
20.02 |
4.69 |
0.15 |
0.26 |
| 5 |
A |
1175 |
1137 |
1.53 |
5.81 |
0.74 |
0.85 |
| 6 |
A |
1033 |
999 |
1.30 |
1.30 |
0.61 |
0.76 |
| 7 |
A |
898 |
869 |
6.56 |
4.51 |
0.21 |
0.34 |
| 8 |
A |
551 |
533 |
9.15 |
23.63 |
0.05 |
0.09 |
| 9 |
A |
222 |
214 |
1.23 |
1.40 |
0.21 |
0.35 |
| 10 |
A |
75 |
72 |
0.23 |
0.78 |
0.62 |
0.76 |
| 11 |
B |
3168 |
3064 |
1.41 |
30.26 |
0.75 |
0.86 |
| 12 |
B |
3078 |
2977 |
2.18 |
44.37 |
0.75 |
0.86 |
| 13 |
B |
1441 |
1394 |
10.30 |
9.32 |
0.75 |
0.86 |
| 14 |
B |
1254 |
1213 |
70.16 |
3.78 |
0.75 |
0.86 |
| 15 |
B |
1103 |
1067 |
1.45 |
1.16 |
0.75 |
0.86 |
| 16 |
B |
834 |
806 |
17.94 |
0.92 |
0.75 |
0.86 |
| 17 |
B |
581 |
562 |
17.64 |
7.96 |
0.75 |
0.86 |
| 18 |
B |
349 |
338 |
7.28 |
1.99 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12370.2 cm
-1
Scaled (by 0.9673) Zero Point Vibrational Energy (zpe) 11965.7 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 TPSSh/aug-cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.312 |
0.689 |
1.195 |
| C2 |
-0.312 |
-0.689 |
1.195 |
| Br3 |
-0.312 |
1.801 |
-0.297 |
| Br4 |
0.312 |
-1.801 |
-0.297 |
| H5 |
0.016 |
1.226 |
2.105 |
| H6 |
1.402 |
0.650 |
1.115 |
| H7 |
-0.016 |
-1.226 |
2.105 |
| H8 |
-1.402 |
-0.650 |
1.115 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5125 | 1.9632 | 2.9030 | 1.0968 | 1.0936 | 2.1449 | 2.1769 |
C2 | 1.5125 | | 2.9030 | 1.9632 | 2.1449 | 2.1769 | 1.0968 | 1.0936 | Br3 | 1.9632 | 2.9030 | | 3.6567 | 2.4912 | 2.5015 | 3.8754 | 3.0320 | Br4 | 2.9030 | 1.9632 | 3.6567 | | 3.8754 | 3.0320 | 2.4912 | 2.5015 | H5 | 1.0968 | 2.1449 | 2.4912 | 3.8754 | | 1.7974 | 2.4518 | 2.5518 | H6 | 1.0936 | 2.1769 | 2.5015 | 3.0320 | 1.7974 | | 2.5518 | 3.0913 | H7 | 2.1449 | 1.0968 | 3.8754 | 2.4912 | 2.4518 | 2.5518 | | 1.7974 | H8 | 2.1769 | 1.0936 | 3.0320 | 2.5015 | 2.5518 | 3.0913 | 1.7974 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.637 |
|
C1 |
C2 |
H7 |
109.548 |
| C1 |
C2 |
H8 |
112.301 |
|
C2 |
C1 |
Br3 |
112.637 |
| C2 |
C1 |
H5 |
109.548 |
|
C2 |
C1 |
H6 |
112.301 |
| Br3 |
C1 |
H5 |
105.480 |
|
Br3 |
C1 |
H6 |
106.336 |
| Br4 |
C2 |
H7 |
105.480 |
|
Br4 |
C2 |
H8 |
106.336 |
| H5 |
C1 |
H6 |
110.288 |
|
H7 |
C2 |
H8 |
110.288 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.008 |
|
|
|
| 2 |
C |
-0.008 |
|
|
|
| 3 |
Br |
0.187 |
|
|
|
| 4 |
Br |
0.187 |
|
|
|
| 5 |
H |
-0.080 |
|
|
|
| 6 |
H |
-0.099 |
|
|
|
| 7 |
H |
-0.080 |
|
|
|
| 8 |
H |
-0.099 |
|
|
|
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 |
2.717 |
2.717 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.545 |
-0.707 |
0.000 |
| y |
-0.707 |
12.003 |
0.000 |
| z |
0.000 |
0.000 |
10.207 |
<r2> (average value of r
2) Å
2
| <r2> |
314.264 |
| (<r2>)1/2 |
17.727 |