Jump to
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| hartrees |
Energy at 0K | -5227.153470 |
Energy at 298.15K | |
HF Energy | -5227.153470 |
Nuclear repulsion energy | 418.191914 |
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 wB97X-D/cc-pVTZ
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 |
3124 |
2986 |
0.00 |
159.71 |
0.04 |
0.08 |
2 |
Ag |
1497 |
1431 |
0.00 |
9.66 |
0.74 |
0.85 |
3 |
Ag |
1308 |
1251 |
0.00 |
33.03 |
0.44 |
0.61 |
4 |
Ag |
1074 |
1027 |
0.00 |
10.02 |
0.72 |
0.84 |
5 |
Ag |
702 |
671 |
0.00 |
77.88 |
0.26 |
0.42 |
6 |
Ag |
195 |
186 |
0.00 |
3.99 |
0.28 |
0.44 |
7 |
Au |
3206 |
3065 |
0.28 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1122 |
1073 |
2.98 |
0.00 |
0.00 |
0.00 |
9 |
Au |
765 |
732 |
4.32 |
0.00 |
0.00 |
0.00 |
10 |
Au |
103 |
98 |
4.46 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3184 |
3044 |
0.00 |
79.15 |
0.75 |
0.86 |
12 |
Bg |
1300 |
1242 |
0.00 |
2.51 |
0.75 |
0.86 |
13 |
Bg |
958 |
916 |
0.00 |
3.13 |
0.75 |
0.86 |
14 |
Bu |
3131 |
2993 |
6.61 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1492 |
1427 |
8.97 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1229 |
1175 |
51.67 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
628 |
600 |
62.24 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
185 |
177 |
6.02 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12600.5 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 12046.1 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 wB97X-D/cc-pVTZ
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.489 |
0.573 |
0.000 |
C2 |
-0.489 |
-0.573 |
0.000 |
Br3 |
-0.489 |
2.261 |
0.000 |
Br4 |
0.489 |
-2.261 |
0.000 |
H5 |
1.112 |
0.577 |
0.888 |
H6 |
1.112 |
0.577 |
-0.888 |
H7 |
-1.112 |
-0.577 |
0.888 |
H8 |
-1.112 |
-0.577 |
-0.888 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5069 | 1.9509 | 2.8344 | 1.0847 | 1.0847 | 2.1620 | 2.1620 |
C2 | 1.5069 | | 2.8344 | 1.9509 | 2.1620 | 2.1620 | 1.0847 | 1.0847 | Br3 | 1.9509 | 2.8344 | | 4.6270 | 2.4874 | 2.4874 | 3.0385 | 3.0385 | Br4 | 2.8344 | 1.9509 | 4.6270 | | 3.0385 | 3.0385 | 2.4874 | 2.4874 | H5 | 1.0847 | 2.1620 | 2.4874 | 3.0385 | | 1.7761 | 2.5053 | 3.0710 | H6 | 1.0847 | 2.1620 | 2.4874 | 3.0385 | 1.7761 | | 3.0710 | 2.5053 | H7 | 2.1620 | 1.0847 | 3.0385 | 2.4874 | 2.5053 | 3.0710 | | 1.7761 | H8 | 2.1620 | 1.0847 | 3.0385 | 2.4874 | 3.0710 | 2.5053 | 1.7761 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
109.446 |
|
C1 |
C2 |
H7 |
112.048 |
C1 |
C2 |
H8 |
112.048 |
|
C2 |
C1 |
Br3 |
109.446 |
C2 |
C1 |
H5 |
112.048 |
|
C2 |
C1 |
H6 |
112.048 |
Br3 |
C1 |
H5 |
106.541 |
|
Br3 |
C1 |
H6 |
106.541 |
Br4 |
C2 |
H7 |
106.541 |
|
Br4 |
C2 |
H8 |
106.541 |
H5 |
C1 |
H6 |
109.917 |
|
H7 |
C2 |
H8 |
109.917 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.147 |
|
|
|
2 |
C |
-0.147 |
|
|
|
3 |
Br |
-0.124 |
|
|
|
4 |
Br |
-0.124 |
|
|
|
5 |
H |
0.135 |
|
|
|
6 |
H |
0.135 |
|
|
|
7 |
H |
0.135 |
|
|
|
8 |
H |
0.135 |
|
|
|
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 |
-48.812 |
1.337 |
0.000 |
y |
1.337 |
-55.781 |
0.000 |
z |
0.000 |
0.000 |
-49.402 |
|
Traceless |
| x | y | z |
x |
3.779 |
1.337 |
0.000 |
y |
1.337 |
-6.673 |
0.000 |
z |
0.000 |
0.000 |
2.894 |
|
Polar |
3z2-r2 | 5.789 |
x2-y2 | 6.968 |
xy | 1.337 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.727 |
-1.910 |
0.000 |
y |
-1.910 |
13.357 |
0.000 |
z |
0.000 |
0.000 |
6.585 |
<r2> (average value of r
2) Å
2
<r2> |
422.963 |
(<r2>)1/2 |
20.566 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVTZ
| hartrees |
Energy at 0K | -5227.150460 |
Energy at 298.15K | |
HF Energy | -5227.150460 |
Nuclear repulsion energy | 451.131257 |
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 wB97X-D/cc-pVTZ
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 |
3170 |
3031 |
0.04 |
89.50 |
0.75 |
0.85 |
2 |
A |
3111 |
2974 |
14.67 |
232.21 |
0.02 |
0.03 |
3 |
A |
1477 |
1412 |
0.85 |
3.53 |
0.70 |
0.83 |
4 |
A |
1325 |
1266 |
19.20 |
2.79 |
0.37 |
0.53 |
5 |
A |
1211 |
1157 |
1.26 |
7.81 |
0.74 |
0.85 |
6 |
A |
1047 |
1001 |
1.06 |
1.59 |
0.66 |
0.79 |
7 |
A |
920 |
879 |
7.97 |
5.44 |
0.36 |
0.53 |
8 |
A |
580 |
554 |
6.96 |
18.97 |
0.06 |
0.11 |
9 |
A |
232 |
221 |
1.15 |
1.51 |
0.42 |
0.59 |
10 |
A |
79 |
75 |
0.27 |
1.15 |
0.70 |
0.82 |
11 |
B |
3182 |
3042 |
0.91 |
27.10 |
0.75 |
0.86 |
12 |
B |
3104 |
2967 |
2.40 |
40.03 |
0.75 |
0.86 |
13 |
B |
1474 |
1409 |
13.26 |
10.29 |
0.75 |
0.86 |
14 |
B |
1295 |
1238 |
62.61 |
3.08 |
0.75 |
0.86 |
15 |
B |
1140 |
1090 |
1.84 |
3.09 |
0.75 |
0.86 |
16 |
B |
860 |
822 |
18.44 |
1.26 |
0.75 |
0.86 |
17 |
B |
616 |
589 |
14.14 |
9.16 |
0.75 |
0.86 |
18 |
B |
364 |
348 |
5.53 |
2.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12592.0 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 12038.0 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 wB97X-D/cc-pVTZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.309 |
0.688 |
1.170 |
C2 |
-0.309 |
-0.688 |
1.170 |
Br3 |
-0.309 |
1.810 |
-0.291 |
Br4 |
0.309 |
-1.810 |
-0.291 |
H5 |
0.028 |
1.208 |
2.083 |
H6 |
1.391 |
0.646 |
1.095 |
H7 |
-0.028 |
-1.208 |
2.083 |
H8 |
-1.391 |
-0.646 |
1.095 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5075 | 1.9435 | 2.8938 | 1.0874 | 1.0853 | 2.1310 | 2.1614 |
C2 | 1.5075 | | 2.8938 | 1.9435 | 2.1310 | 2.1614 | 1.0874 | 1.0853 | Br3 | 1.9435 | 2.8938 | | 3.6721 | 2.4723 | 2.4826 | 3.8504 | 3.0205 | Br4 | 2.8938 | 1.9435 | 3.6721 | | 3.8504 | 3.0205 | 2.4723 | 2.4826 | H5 | 1.0874 | 2.1310 | 2.4723 | 3.8504 | | 1.7742 | 2.4174 | 2.5355 | H6 | 1.0853 | 2.1614 | 2.4826 | 3.0205 | 1.7742 | | 2.5355 | 3.0666 | H7 | 2.1310 | 1.0874 | 3.8504 | 2.4723 | 2.4174 | 2.5355 | | 1.7742 | H8 | 2.1614 | 1.0853 | 3.0205 | 2.4826 | 2.5355 | 3.0666 | 1.7742 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.373 |
|
C1 |
C2 |
H7 |
109.349 |
C1 |
C2 |
H8 |
111.919 |
|
C2 |
C1 |
Br3 |
113.373 |
C2 |
C1 |
H5 |
109.349 |
|
C2 |
C1 |
H6 |
111.919 |
Br3 |
C1 |
H5 |
105.829 |
|
Br3 |
C1 |
H6 |
106.644 |
Br4 |
C2 |
H7 |
105.829 |
|
Br4 |
C2 |
H8 |
106.644 |
H5 |
C1 |
H6 |
109.493 |
|
H7 |
C2 |
H8 |
109.493 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.155 |
|
|
|
2 |
C |
-0.155 |
|
|
|
3 |
Br |
-0.107 |
|
|
|
4 |
Br |
-0.107 |
|
|
|
5 |
H |
0.129 |
|
|
|
6 |
H |
0.133 |
|
|
|
7 |
H |
0.129 |
|
|
|
8 |
H |
0.133 |
|
|
|
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 |
2.634 |
2.634 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.183 |
0.918 |
0.000 |
y |
0.918 |
-53.803 |
0.000 |
z |
0.000 |
0.000 |
-45.063 |
|
Traceless |
| x | y | z |
x |
0.250 |
0.918 |
0.000 |
y |
0.918 |
-6.680 |
0.000 |
z |
0.000 |
0.000 |
6.430 |
|
Polar |
3z2-r2 | 12.861 |
x2-y2 | 4.620 |
xy | 0.918 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.016 |
-0.767 |
0.000 |
y |
-0.767 |
10.376 |
0.000 |
z |
0.000 |
0.000 |
8.995 |
<r2> (average value of r
2) Å
2
<r2> |
314.695 |
(<r2>)1/2 |
17.740 |