Jump to
S1C2
Energy calculated at TPSSh/aug-cc-pVDZ
| hartrees |
Energy at 0K | -3112.909961 |
Energy at 298.15K | |
HF Energy | -3112.909961 |
Nuclear repulsion energy | 286.839469 |
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' |
3114 |
3012 |
7.63 |
29.68 |
0.03 |
0.06 |
2 |
A' |
3103 |
3001 |
2.20 |
145.73 |
0.03 |
0.06 |
3 |
A' |
1478 |
1430 |
0.53 |
5.69 |
0.74 |
0.85 |
4 |
A' |
1469 |
1421 |
5.30 |
0.55 |
0.75 |
0.86 |
5 |
A' |
1285 |
1243 |
1.13 |
22.86 |
0.34 |
0.51 |
6 |
A' |
1198 |
1159 |
43.43 |
2.88 |
0.26 |
0.41 |
7 |
A' |
1071 |
1036 |
0.94 |
5.97 |
0.72 |
0.84 |
8 |
A' |
713 |
689 |
33.73 |
64.93 |
0.25 |
0.40 |
9 |
A' |
622 |
602 |
68.64 |
18.74 |
0.22 |
0.37 |
10 |
A' |
242 |
234 |
0.80 |
5.42 |
0.22 |
0.36 |
11 |
A' |
186 |
180 |
8.26 |
0.24 |
0.20 |
0.33 |
12 |
A" |
3195 |
3091 |
1.16 |
5.59 |
0.75 |
0.86 |
13 |
A" |
3170 |
3066 |
0.37 |
75.77 |
0.75 |
0.86 |
14 |
A" |
1275 |
1234 |
0.02 |
2.34 |
0.75 |
0.86 |
15 |
A" |
1101 |
1065 |
1.49 |
0.05 |
0.75 |
0.86 |
16 |
A" |
959 |
928 |
0.14 |
1.16 |
0.75 |
0.86 |
17 |
A" |
756 |
731 |
2.27 |
0.00 |
0.75 |
0.86 |
18 |
A" |
108 |
105 |
5.81 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12523.1 cm
-1
Scaled (by 0.9673) Zero Point Vibrational Energy (zpe) 12113.6 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 Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.653 |
0.000 |
C2 |
1.234 |
-0.224 |
0.000 |
Br3 |
-1.594 |
-0.512 |
0.000 |
Cl4 |
2.701 |
0.852 |
0.000 |
H5 |
-0.070 |
1.269 |
0.900 |
H6 |
-0.070 |
1.269 |
-0.900 |
H7 |
1.297 |
-0.843 |
0.899 |
H8 |
1.297 |
-0.843 |
-0.899 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5135 | 1.9741 | 2.7088 | 1.0928 | 1.0928 | 2.1747 | 2.1747 |
C2 | 1.5135 | | 2.8419 | 1.8200 | 2.1768 | 2.1768 | 1.0935 | 1.0935 | Br3 | 1.9741 | 2.8419 | | 4.5065 | 2.5102 | 2.5102 | 3.0451 | 3.0451 | Cl4 | 2.7088 | 1.8200 | 4.5065 | | 2.9440 | 2.9440 | 2.3782 | 2.3782 | H5 | 1.0928 | 2.1768 | 2.5102 | 2.9440 | | 1.8004 | 2.5160 | 3.0930 | H6 | 1.0928 | 2.1768 | 2.5102 | 2.9440 | 1.8004 | | 3.0930 | 2.5160 | H7 | 2.1747 | 1.0935 | 3.0451 | 2.3782 | 2.5160 | 3.0930 | | 1.7977 | H8 | 2.1747 | 1.0935 | 3.0451 | 2.3782 | 3.0930 | 2.5160 | 1.7977 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.350 |
|
C1 |
C2 |
H7 |
112.051 |
C1 |
C2 |
H8 |
112.051 |
|
C2 |
C1 |
Br3 |
108.425 |
C2 |
C1 |
Cl4 |
39.623 |
|
C2 |
C1 |
H6 |
112.264 |
Br3 |
C1 |
H5 |
106.284 |
|
Br3 |
C1 |
H6 |
106.284 |
Cl4 |
C2 |
H7 |
106.754 |
|
Cl4 |
C2 |
H8 |
106.754 |
H5 |
C1 |
H6 |
110.924 |
|
H7 |
C2 |
H8 |
110.569 |
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 |
0.088 |
|
|
|
2 |
C |
0.165 |
|
|
|
3 |
Br |
0.162 |
|
|
|
4 |
Cl |
-0.105 |
|
|
|
5 |
H |
-0.091 |
|
|
|
6 |
H |
-0.091 |
|
|
|
7 |
H |
-0.063 |
|
|
|
8 |
H |
-0.063 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.057 |
-0.016 |
0.000 |
0.059 |
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 |
12.735 |
1.887 |
0.000 |
y |
1.887 |
8.620 |
0.000 |
z |
0.000 |
0.000 |
7.436 |
<r2> (average value of r
2) Å
2
<r2> |
286.416 |
(<r2>)1/2 |
16.924 |
Jump to
S1C1
Energy calculated at TPSSh/aug-cc-pVDZ
| hartrees |
Energy at 0K | -3112.906570 |
Energy at 298.15K | |
HF Energy | -3112.906570 |
Nuclear repulsion energy | 303.147649 |
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 |
3167 |
3064 |
1.98 |
38.14 |
0.75 |
0.86 |
2 |
A |
3147 |
3044 |
1.27 |
79.49 |
0.75 |
0.86 |
3 |
A |
3088 |
2987 |
14.64 |
193.40 |
0.03 |
0.06 |
4 |
A |
3071 |
2971 |
9.73 |
114.57 |
0.18 |
0.30 |
5 |
A |
1455 |
1407 |
1.88 |
3.84 |
0.75 |
0.86 |
6 |
A |
1444 |
1397 |
8.88 |
7.98 |
0.74 |
0.85 |
7 |
A |
1308 |
1265 |
18.87 |
1.86 |
0.32 |
0.48 |
8 |
A |
1268 |
1227 |
54.06 |
3.77 |
0.37 |
0.55 |
9 |
A |
1191 |
1152 |
1.99 |
5.72 |
0.70 |
0.82 |
10 |
A |
1122 |
1086 |
0.86 |
1.35 |
0.69 |
0.82 |
11 |
A |
1038 |
1004 |
2.33 |
1.19 |
0.73 |
0.85 |
12 |
A |
922 |
891 |
7.78 |
3.95 |
0.20 |
0.33 |
13 |
A |
856 |
828 |
19.17 |
1.13 |
0.74 |
0.85 |
14 |
A |
662 |
641 |
23.43 |
10.32 |
0.25 |
0.40 |
15 |
A |
565 |
547 |
13.14 |
18.53 |
0.13 |
0.22 |
16 |
A |
378 |
365 |
8.42 |
1.86 |
0.69 |
0.82 |
17 |
A |
235 |
227 |
1.28 |
1.27 |
0.22 |
0.37 |
18 |
A |
92 |
89 |
0.54 |
0.97 |
0.64 |
0.78 |
Unscaled Zero Point Vibrational Energy (zpe) 12504.4 cm
-1
Scaled (by 0.9673) Zero Point Vibrational Energy (zpe) 12095.5 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 C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.013 |
1.113 |
-0.388 |
C2 |
1.285 |
0.911 |
0.407 |
Br3 |
-1.359 |
-0.227 |
0.036 |
Cl4 |
2.175 |
-0.582 |
-0.087 |
H5 |
-0.432 |
2.082 |
-0.134 |
H6 |
0.186 |
1.043 |
-1.465 |
H7 |
1.967 |
1.749 |
0.217 |
H8 |
1.088 |
0.824 |
1.480 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5132 | 1.9643 | 2.7637 | 1.0962 | 1.0935 | 2.1420 | 2.1747 |
C2 | 1.5132 | | 2.9021 | 1.8075 | 2.1474 | 2.1749 | 1.0975 | 1.0942 | Br3 | 1.9643 | 2.9021 | | 3.5539 | 2.4936 | 2.5012 | 3.8731 | 3.0296 | Cl4 | 2.7637 | 1.8075 | 3.5539 | | 3.7279 | 2.9148 | 2.3608 | 2.3692 | H5 | 1.0962 | 2.1474 | 2.4936 | 3.7279 | | 1.7986 | 2.4473 | 2.5495 | H6 | 1.0935 | 2.1749 | 2.5012 | 2.9148 | 1.7986 | | 2.5493 | 3.0883 | H7 | 2.1420 | 1.0975 | 3.8731 | 2.3608 | 2.4473 | 2.5493 | | 1.7958 | H8 | 2.1747 | 1.0942 | 3.0296 | 2.3692 | 2.5495 | 3.0883 | 1.7958 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.360 |
|
C1 |
C2 |
H7 |
109.224 |
C1 |
C2 |
H8 |
112.031 |
|
C2 |
C1 |
Br3 |
112.491 |
C2 |
C1 |
Cl4 |
37.217 |
|
C2 |
C1 |
H6 |
112.089 |
Br3 |
C1 |
H5 |
105.600 |
|
Br3 |
C1 |
H6 |
106.249 |
Cl4 |
C2 |
H7 |
106.123 |
|
Cl4 |
C2 |
H8 |
106.881 |
H5 |
C1 |
H6 |
110.450 |
|
H7 |
C2 |
H8 |
110.035 |
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 |
0.023 |
|
|
|
2 |
C |
0.094 |
|
|
|
3 |
Br |
0.189 |
|
|
|
4 |
Cl |
-0.080 |
|
|
|
5 |
H |
-0.081 |
|
|
|
6 |
H |
-0.079 |
|
|
|
7 |
H |
-0.035 |
|
|
|
8 |
H |
-0.031 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.393 |
2.754 |
0.103 |
2.784 |
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 |
10.777 |
0.181 |
-0.163 |
y |
0.181 |
9.179 |
0.035 |
z |
-0.163 |
0.035 |
7.636 |
<r2> (average value of r
2) Å
2
<r2> |
223.327 |
(<r2>)1/2 |
14.944 |