Jump to
S1C2
Energy calculated at B97D3/Def2TZVPP
| hartrees |
Energy at 0K | -5229.561115 |
Energy at 298.15K | |
HF Energy | -5229.561115 |
Nuclear repulsion energy | 413.775469 |
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 B97D3/Def2TZVPP
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 |
3060 |
3018 |
0.00 |
168.42 |
0.03 |
0.06 |
2 |
Ag |
1460 |
1440 |
0.00 |
7.27 |
0.75 |
0.86 |
3 |
Ag |
1243 |
1226 |
0.00 |
44.38 |
0.42 |
0.59 |
4 |
Ag |
1045 |
1030 |
0.00 |
15.11 |
0.68 |
0.81 |
5 |
Ag |
618 |
609 |
0.00 |
132.15 |
0.29 |
0.45 |
6 |
Ag |
181 |
178 |
0.00 |
5.81 |
0.29 |
0.44 |
7 |
Au |
3146 |
3103 |
1.04 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1073 |
1059 |
2.88 |
0.00 |
0.00 |
0.00 |
9 |
Au |
748 |
738 |
3.63 |
0.00 |
0.00 |
0.00 |
10 |
Au |
101 |
99 |
4.28 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3122 |
3079 |
0.00 |
79.84 |
0.75 |
0.86 |
12 |
Bg |
1259 |
1242 |
0.00 |
2.17 |
0.75 |
0.86 |
13 |
Bg |
921 |
909 |
0.00 |
2.33 |
0.75 |
0.86 |
14 |
Bu |
3069 |
3027 |
6.66 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1456 |
1436 |
5.95 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1178 |
1162 |
51.81 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
548 |
541 |
85.47 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
175 |
172 |
7.56 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12200.5 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 12033.4 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 B97D3/Def2TZVPP
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.498 |
0.564 |
0.000 |
C2 |
-0.498 |
-0.564 |
0.000 |
Br3 |
-0.498 |
2.284 |
0.000 |
Br4 |
0.498 |
-2.284 |
0.000 |
H5 |
1.118 |
0.577 |
0.895 |
H6 |
1.118 |
0.577 |
-0.895 |
H7 |
-1.118 |
-0.577 |
0.895 |
H8 |
-1.118 |
-0.577 |
-0.895 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5049 | 1.9870 | 2.8477 | 1.0885 | 1.0885 | 2.1713 | 2.1713 |
C2 | 1.5049 | | 2.8477 | 1.9870 | 2.1713 | 2.1713 | 1.0885 | 1.0885 | Br3 | 1.9870 | 2.8477 | | 4.6744 | 2.5144 | 2.5144 | 3.0610 | 3.0610 | Br4 | 2.8477 | 1.9870 | 4.6744 | | 3.0610 | 3.0610 | 2.5144 | 2.5144 | H5 | 1.0885 | 2.1713 | 2.5144 | 3.0610 | | 1.7895 | 2.5163 | 3.0877 | H6 | 1.0885 | 2.1713 | 2.5144 | 3.0610 | 1.7895 | | 3.0877 | 2.5163 | H7 | 2.1713 | 1.0885 | 3.0610 | 2.5144 | 2.5163 | 3.0877 | | 1.7895 | H8 | 2.1713 | 1.0885 | 3.0610 | 2.5144 | 3.0877 | 2.5163 | 1.7895 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.482 |
|
C1 |
C2 |
H7 |
112.706 |
C1 |
C2 |
H8 |
112.706 |
|
C2 |
C1 |
Br3 |
108.482 |
C2 |
C1 |
H5 |
112.706 |
|
C2 |
C1 |
H6 |
112.706 |
Br3 |
C1 |
H5 |
105.952 |
|
Br3 |
C1 |
H6 |
105.952 |
Br4 |
C2 |
H7 |
105.952 |
|
Br4 |
C2 |
H8 |
105.952 |
H5 |
C1 |
H6 |
110.563 |
|
H7 |
C2 |
H8 |
110.563 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.091 |
|
|
|
2 |
C |
-0.091 |
|
|
|
3 |
Br |
-0.139 |
|
|
|
4 |
Br |
-0.139 |
|
|
|
5 |
H |
0.115 |
|
|
|
6 |
H |
0.115 |
|
|
|
7 |
H |
0.115 |
|
|
|
8 |
H |
0.115 |
|
|
|
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 |
-48.736 |
1.445 |
0.000 |
y |
1.445 |
-55.913 |
0.000 |
z |
0.000 |
0.000 |
-49.299 |
|
Traceless |
| x | y | z |
x |
3.870 |
1.445 |
0.000 |
y |
1.445 |
-6.895 |
0.000 |
z |
0.000 |
0.000 |
3.025 |
|
Polar |
3z2-r2 | 6.051 |
x2-y2 | 7.177 |
xy | 1.445 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.391 |
-1.991 |
0.000 |
y |
-1.991 |
14.951 |
0.000 |
z |
0.000 |
0.000 |
7.320 |
<r2> (average value of r
2) Å
2
<r2> |
430.758 |
(<r2>)1/2 |
20.755 |
Jump to
S1C1
Energy calculated at B97D3/Def2TZVPP
| hartrees |
Energy at 0K | -5229.557468 |
Energy at 298.15K | |
HF Energy | -5229.557468 |
Nuclear repulsion energy | 446.806399 |
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 B97D3/Def2TZVPP
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 |
3098 |
3056 |
0.03 |
91.82 |
0.75 |
0.85 |
2 |
A |
3036 |
2994 |
17.34 |
281.24 |
0.02 |
0.03 |
3 |
A |
1435 |
1415 |
0.59 |
3.16 |
0.75 |
0.86 |
4 |
A |
1275 |
1257 |
18.58 |
3.90 |
0.42 |
0.59 |
5 |
A |
1158 |
1142 |
1.81 |
9.16 |
0.74 |
0.85 |
6 |
A |
1010 |
996 |
1.48 |
2.17 |
0.54 |
0.70 |
7 |
A |
882 |
870 |
7.86 |
5.92 |
0.30 |
0.47 |
8 |
A |
524 |
517 |
8.51 |
18.45 |
0.07 |
0.12 |
9 |
A |
225 |
222 |
1.38 |
1.85 |
0.31 |
0.48 |
10 |
A |
77 |
76 |
0.22 |
1.10 |
0.68 |
0.81 |
11 |
B |
3113 |
3070 |
2.18 |
26.84 |
0.75 |
0.86 |
12 |
B |
3027 |
2986 |
2.18 |
55.88 |
0.75 |
0.86 |
13 |
B |
1431 |
1412 |
10.28 |
11.09 |
0.75 |
0.86 |
14 |
B |
1241 |
1224 |
68.80 |
3.69 |
0.75 |
0.86 |
15 |
B |
1096 |
1081 |
1.64 |
2.53 |
0.75 |
0.86 |
16 |
B |
827 |
815 |
19.78 |
1.02 |
0.75 |
0.86 |
17 |
B |
556 |
548 |
18.37 |
9.41 |
0.75 |
0.86 |
18 |
B |
346 |
342 |
7.75 |
2.65 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12178.6 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 12011.7 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 B97D3/Def2TZVPP
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.314 |
0.685 |
1.187 |
C2 |
-0.314 |
-0.685 |
1.187 |
Br3 |
-0.314 |
1.826 |
-0.295 |
Br4 |
0.314 |
-1.826 |
-0.295 |
H5 |
0.032 |
1.218 |
2.098 |
H6 |
1.399 |
0.646 |
1.099 |
H7 |
-0.032 |
-1.218 |
2.098 |
H8 |
-1.399 |
-0.646 |
1.099 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5072 | 1.9721 | 2.9157 | 1.0928 | 1.0893 | 2.1387 | 2.1709 |
C2 | 1.5072 | | 2.9157 | 1.9721 | 2.1387 | 2.1709 | 1.0928 | 1.0893 | Br3 | 1.9721 | 2.9157 | | 3.7058 | 2.4928 | 2.5035 | 3.8825 | 3.0386 | Br4 | 2.9157 | 1.9721 | 3.7058 | | 3.8825 | 3.0386 | 2.4928 | 2.5035 | H5 | 1.0928 | 2.1387 | 2.4928 | 3.8825 | | 1.7868 | 2.4376 | 2.5538 | H6 | 1.0893 | 2.1709 | 2.5035 | 3.0386 | 1.7868 | | 2.5538 | 3.0816 | H7 | 2.1387 | 1.0928 | 3.8825 | 2.4928 | 2.4376 | 2.5538 | | 1.7868 | H8 | 2.1709 | 1.0893 | 3.0386 | 2.5035 | 2.5538 | 3.0816 | 1.7868 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.183 |
|
C1 |
C2 |
H7 |
109.660 |
C1 |
C2 |
H8 |
112.456 |
|
C2 |
C1 |
Br3 |
113.183 |
C2 |
C1 |
H5 |
109.660 |
|
C2 |
C1 |
H6 |
112.456 |
Br3 |
C1 |
H5 |
105.208 |
|
Br3 |
C1 |
H6 |
106.097 |
Br4 |
C2 |
H7 |
105.208 |
|
Br4 |
C2 |
H8 |
106.097 |
H5 |
C1 |
H6 |
109.936 |
|
H7 |
C2 |
H8 |
109.936 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.086 |
|
|
|
2 |
C |
-0.086 |
|
|
|
3 |
Br |
-0.125 |
|
|
|
4 |
Br |
-0.125 |
|
|
|
5 |
H |
0.105 |
|
|
|
6 |
H |
0.106 |
|
|
|
7 |
H |
0.105 |
|
|
|
8 |
H |
0.106 |
|
|
|
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 |
2.628 |
2.628 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.086 |
0.967 |
0.000 |
y |
0.967 |
-53.880 |
0.000 |
z |
0.000 |
0.000 |
-44.976 |
|
Traceless |
| x | y | z |
x |
0.342 |
0.967 |
0.000 |
y |
0.967 |
-6.849 |
0.000 |
z |
0.000 |
0.000 |
6.506 |
|
Polar |
3z2-r2 | 13.013 |
x2-y2 | 4.794 |
xy | 0.967 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.710 |
-0.766 |
0.000 |
y |
-0.766 |
11.395 |
0.000 |
z |
0.000 |
0.000 |
9.665 |
<r2> (average value of r
2) Å
2
<r2> |
319.859 |
(<r2>)1/2 |
17.885 |