Jump to
S1C2
Energy calculated at HSEh1PBE/STO-3G
| hartrees |
Energy at 0K | -3078.451918 |
Energy at 298.15K | |
HF Energy | -3078.451918 |
Nuclear repulsion energy | 286.395411 |
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 HSEh1PBE/STO-3G
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' |
3396 |
2999 |
1.27 |
4.76 |
0.17 |
0.30 |
2 |
A' |
3389 |
2993 |
0.01 |
66.62 |
0.11 |
0.20 |
3 |
A' |
1653 |
1460 |
3.28 |
7.26 |
0.75 |
0.86 |
4 |
A' |
1634 |
1443 |
1.00 |
15.89 |
0.75 |
0.86 |
5 |
A' |
1444 |
1275 |
0.41 |
14.86 |
0.32 |
0.48 |
6 |
A' |
1342 |
1185 |
27.83 |
0.03 |
0.63 |
0.77 |
7 |
A' |
1135 |
1002 |
1.03 |
10.37 |
0.74 |
0.85 |
8 |
A' |
869 |
767 |
21.86 |
28.88 |
0.30 |
0.46 |
9 |
A' |
794 |
701 |
25.78 |
5.44 |
0.36 |
0.53 |
10 |
A' |
262 |
231 |
0.77 |
4.08 |
0.41 |
0.58 |
11 |
A' |
194 |
172 |
8.12 |
0.01 |
0.72 |
0.84 |
12 |
A" |
3522 |
3110 |
0.43 |
4.51 |
0.75 |
0.86 |
13 |
A" |
3505 |
3095 |
0.00 |
49.60 |
0.75 |
0.86 |
14 |
A" |
1393 |
1230 |
0.02 |
16.84 |
0.75 |
0.86 |
15 |
A" |
1223 |
1080 |
0.59 |
0.07 |
0.75 |
0.86 |
16 |
A" |
1045 |
923 |
0.07 |
8.78 |
0.75 |
0.86 |
17 |
A" |
809 |
714 |
3.34 |
0.02 |
0.75 |
0.86 |
18 |
A" |
100 |
88 |
6.40 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13853.9 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 12234.4 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 HSEh1PBE/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.628 |
0.000 |
C2 |
1.226 |
-0.311 |
0.000 |
Br3 |
-1.629 |
-0.401 |
0.000 |
Cl4 |
2.772 |
0.675 |
0.000 |
H5 |
0.021 |
1.272 |
0.894 |
H6 |
0.021 |
1.272 |
-0.894 |
H7 |
1.247 |
-0.948 |
0.901 |
H8 |
1.247 |
-0.948 |
-0.901 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5448 | 1.9269 | 2.7720 | 1.1018 | 1.1018 | 2.2022 | 2.2022 |
C2 | 1.5448 | | 2.8566 | 1.8333 | 2.1813 | 2.1813 | 1.1031 | 1.1031 | Br3 | 1.9269 | 2.8566 | | 4.5302 | 2.5143 | 2.5143 | 3.0625 | 3.0625 | Cl4 | 2.7720 | 1.8333 | 4.5302 | | 2.9529 | 2.9529 | 2.4022 | 2.4022 | H5 | 1.1018 | 2.1813 | 2.5143 | 2.9529 | | 1.7877 | 2.5357 | 3.1065 | H6 | 1.1018 | 2.1813 | 2.5143 | 2.9529 | 1.7877 | | 3.1065 | 2.5357 | H7 | 2.2022 | 1.1031 | 3.0625 | 2.4022 | 2.5357 | 3.1065 | | 1.8015 | H8 | 2.2022 | 1.1031 | 3.0625 | 2.4022 | 3.1065 | 2.5357 | 1.8015 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.988 |
|
C1 |
C2 |
H7 |
111.447 |
C1 |
C2 |
H8 |
111.447 |
|
C2 |
C1 |
Br3 |
110.249 |
C2 |
C1 |
Cl4 |
38.429 |
|
C2 |
C1 |
H6 |
109.881 |
Br3 |
C1 |
H5 |
109.175 |
|
Br3 |
C1 |
H6 |
109.175 |
Cl4 |
C2 |
H7 |
107.151 |
|
Cl4 |
C2 |
H8 |
107.151 |
H5 |
C1 |
H6 |
108.446 |
|
H7 |
C2 |
H8 |
109.475 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.187 |
|
|
|
2 |
C |
-0.104 |
|
|
|
3 |
Br |
-0.009 |
|
|
|
4 |
Cl |
-0.160 |
|
|
|
5 |
H |
0.112 |
|
|
|
6 |
H |
0.112 |
|
|
|
7 |
H |
0.118 |
|
|
|
8 |
H |
0.118 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.823 |
-0.387 |
0.000 |
0.909 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.095 |
-2.929 |
0.000 |
y |
-2.929 |
-39.896 |
0.000 |
z |
0.000 |
0.000 |
-39.713 |
|
Traceless |
| x | y | z |
x |
-9.290 |
-2.929 |
0.000 |
y |
-2.929 |
4.507 |
0.000 |
z |
0.000 |
0.000 |
4.783 |
|
Polar |
3z2-r2 | 9.566 |
x2-y2 | -9.198 |
xy | -2.929 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.102 |
1.601 |
0.000 |
y |
1.601 |
2.533 |
0.000 |
z |
0.000 |
0.000 |
1.668 |
<r2> (average value of r
2) Å
2
<r2> |
286.964 |
(<r2>)1/2 |
16.940 |
Jump to
S1C1
Energy calculated at HSEh1PBE/STO-3G
| hartrees |
Energy at 0K | -3078.449746 |
Energy at 298.15K | |
HF Energy | -3078.449746 |
Nuclear repulsion energy | 303.178129 |
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 HSEh1PBE/STO-3G
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 |
3508 |
3098 |
0.89 |
27.92 |
0.74 |
0.85 |
2 |
A |
3491 |
3083 |
0.29 |
42.91 |
0.75 |
0.86 |
3 |
A |
3384 |
2988 |
0.23 |
56.65 |
0.10 |
0.18 |
4 |
A |
3374 |
2980 |
0.06 |
43.54 |
0.17 |
0.28 |
5 |
A |
1637 |
1446 |
1.55 |
11.12 |
0.74 |
0.85 |
6 |
A |
1620 |
1431 |
3.07 |
17.15 |
0.74 |
0.85 |
7 |
A |
1450 |
1281 |
11.80 |
6.58 |
0.52 |
0.68 |
8 |
A |
1426 |
1259 |
39.91 |
0.85 |
0.65 |
0.79 |
9 |
A |
1309 |
1156 |
0.34 |
17.43 |
0.75 |
0.86 |
10 |
A |
1240 |
1095 |
0.78 |
7.02 |
0.75 |
0.86 |
11 |
A |
1125 |
993 |
2.67 |
4.06 |
0.75 |
0.85 |
12 |
A |
1020 |
900 |
6.06 |
5.82 |
0.51 |
0.67 |
13 |
A |
949 |
838 |
12.64 |
2.24 |
0.62 |
0.76 |
14 |
A |
779 |
688 |
9.55 |
9.96 |
0.44 |
0.61 |
15 |
A |
698 |
617 |
4.66 |
11.65 |
0.21 |
0.35 |
16 |
A |
400 |
354 |
6.51 |
2.46 |
0.75 |
0.86 |
17 |
A |
234 |
207 |
1.13 |
1.00 |
0.45 |
0.62 |
18 |
A |
88 |
78 |
1.14 |
1.21 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 13866.3 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 12245.4 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 HSEh1PBE/STO-3G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.038 |
1.107 |
-0.383 |
C2 |
1.288 |
0.937 |
0.396 |
Br3 |
-1.351 |
-0.233 |
0.038 |
Cl4 |
2.176 |
-0.587 |
-0.086 |
H5 |
-0.450 |
2.099 |
-0.131 |
H6 |
0.166 |
1.085 |
-1.465 |
H7 |
1.963 |
1.784 |
0.177 |
H8 |
1.113 |
0.881 |
1.484 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5463 | 1.9220 | 2.8025 | 1.1038 | 1.1019 | 2.1845 | 2.2040 |
C2 | 1.5463 | | 2.9082 | 1.8287 | 2.1557 | 2.1781 | 1.1043 | 1.1032 | Br3 | 1.9220 | 2.9082 | | 3.5461 | 2.5054 | 2.5088 | 3.8810 | 3.0660 | Cl4 | 2.8025 | 1.8287 | 3.5461 | | 3.7564 | 2.9553 | 2.3945 | 2.3979 | H5 | 1.1038 | 2.1557 | 2.5054 | 3.7564 | | 1.7857 | 2.4526 | 2.5562 | H6 | 1.1019 | 2.1781 | 2.5088 | 2.9553 | 1.7857 | | 2.5325 | 3.1040 | H7 | 2.1845 | 1.1043 | 3.8810 | 2.3945 | 2.4526 | 2.5325 | | 1.8012 | H8 | 2.2040 | 1.1032 | 3.0660 | 2.3979 | 2.5562 | 3.1040 | 1.8012 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
111.997 |
|
C1 |
C2 |
H7 |
109.883 |
C1 |
C2 |
H8 |
111.483 |
|
C2 |
C1 |
Br3 |
113.524 |
C2 |
C1 |
Cl4 |
37.232 |
|
C2 |
C1 |
H6 |
109.523 |
Br3 |
C1 |
H5 |
108.756 |
|
Br3 |
C1 |
H6 |
109.097 |
Cl4 |
C2 |
H7 |
106.836 |
|
Cl4 |
C2 |
H8 |
107.128 |
H5 |
C1 |
H6 |
108.104 |
|
H7 |
C2 |
H8 |
109.355 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.189 |
|
|
|
2 |
C |
-0.105 |
|
|
|
3 |
Br |
-0.004 |
|
|
|
4 |
Cl |
-0.156 |
|
|
|
5 |
H |
0.107 |
|
|
|
6 |
H |
0.112 |
|
|
|
7 |
H |
0.116 |
|
|
|
8 |
H |
0.118 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.228 |
2.838 |
0.219 |
2.856 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-44.761 |
2.911 |
0.717 |
y |
2.911 |
-37.968 |
-0.029 |
z |
0.717 |
-0.029 |
-39.450 |
|
Traceless |
| x | y | z |
x |
-6.052 |
2.911 |
0.717 |
y |
2.911 |
4.137 |
-0.029 |
z |
0.717 |
-0.029 |
1.914 |
|
Polar |
3z2-r2 | 3.828 |
x2-y2 | -6.793 |
xy | 2.911 |
xz | 0.717 |
yz | -0.029 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.489 |
0.232 |
-0.400 |
y |
0.232 |
3.516 |
0.036 |
z |
-0.400 |
0.036 |
1.819 |
<r2> (average value of r
2) Å
2
<r2> |
221.325 |
(<r2>)1/2 |
14.877 |