Jump to
S1C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -3112.425956 |
Energy at 298.15K | |
HF Energy | -3112.425956 |
Nuclear repulsion energy | 288.904508 |
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 PBE1PBE/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' |
3132 |
3011 |
6.23 |
29.51 |
0.03 |
0.06 |
2 |
A' |
3120 |
3000 |
2.01 |
145.06 |
0.03 |
0.05 |
3 |
A' |
1461 |
1405 |
0.68 |
5.62 |
0.74 |
0.85 |
4 |
A' |
1453 |
1397 |
8.04 |
0.44 |
0.74 |
0.85 |
5 |
A' |
1298 |
1248 |
0.84 |
20.58 |
0.36 |
0.53 |
6 |
A' |
1205 |
1159 |
35.06 |
2.38 |
0.27 |
0.42 |
7 |
A' |
1094 |
1052 |
1.18 |
4.69 |
0.69 |
0.82 |
8 |
A' |
757 |
728 |
30.25 |
50.70 |
0.24 |
0.39 |
9 |
A' |
659 |
634 |
56.95 |
16.26 |
0.22 |
0.36 |
10 |
A' |
252 |
243 |
0.77 |
4.55 |
0.22 |
0.36 |
11 |
A' |
195 |
187 |
7.16 |
0.20 |
0.20 |
0.33 |
12 |
A" |
3214 |
3090 |
0.15 |
5.87 |
0.75 |
0.86 |
13 |
A" |
3189 |
3066 |
0.21 |
73.17 |
0.75 |
0.86 |
14 |
A" |
1276 |
1227 |
0.02 |
2.40 |
0.75 |
0.86 |
15 |
A" |
1113 |
1070 |
1.60 |
0.03 |
0.75 |
0.86 |
16 |
A" |
968 |
931 |
0.13 |
1.02 |
0.75 |
0.86 |
17 |
A" |
760 |
731 |
3.02 |
0.00 |
0.75 |
0.86 |
18 |
A" |
111 |
106 |
5.57 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12627.8 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 12142.9 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 PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.644 |
0.000 |
C2 |
1.229 |
-0.230 |
0.000 |
Br3 |
-1.588 |
-0.492 |
0.000 |
Cl4 |
2.691 |
0.818 |
0.000 |
H5 |
-0.057 |
1.266 |
0.897 |
H6 |
-0.057 |
1.266 |
-0.897 |
H7 |
1.280 |
-0.857 |
0.896 |
H8 |
1.280 |
-0.857 |
-0.896 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5082 | 1.9517 | 2.6963 | 1.0937 | 1.0937 | 2.1664 | 2.1664 |
C2 | 1.5082 | | 2.8289 | 1.7986 | 2.1681 | 2.1681 | 1.0944 | 1.0944 | Br3 | 1.9517 | 2.8289 | | 4.4742 | 2.4974 | 2.4974 | 3.0266 | 3.0266 | Cl4 | 2.6963 | 1.7986 | 4.4742 | | 2.9254 | 2.9254 | 2.3659 | 2.3659 | H5 | 1.0937 | 2.1681 | 2.4974 | 2.9254 | | 1.7945 | 2.5094 | 3.0843 | H6 | 1.0937 | 2.1681 | 2.4974 | 2.9254 | 1.7945 | | 3.0843 | 2.5094 | H7 | 2.1664 | 1.0944 | 3.0266 | 2.3659 | 2.5094 | 3.0843 | | 1.7918 | H8 | 2.1664 | 1.0944 | 3.0266 | 2.3659 | 3.0843 | 2.5094 | 1.7918 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.933 |
|
C1 |
C2 |
H7 |
111.697 |
C1 |
C2 |
H8 |
111.697 |
|
C2 |
C1 |
Br3 |
109.020 |
C2 |
C1 |
Cl4 |
39.122 |
|
C2 |
C1 |
H6 |
111.882 |
Br3 |
C1 |
H5 |
106.769 |
|
Br3 |
C1 |
H6 |
106.769 |
Cl4 |
C2 |
H7 |
107.206 |
|
Cl4 |
C2 |
H8 |
107.206 |
H5 |
C1 |
H6 |
110.248 |
|
H7 |
C2 |
H8 |
109.892 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.020 |
|
|
|
2 |
C |
0.114 |
|
|
|
3 |
Br |
0.216 |
|
|
|
4 |
Cl |
-0.083 |
|
|
|
5 |
H |
-0.083 |
|
|
|
6 |
H |
-0.083 |
|
|
|
7 |
H |
-0.050 |
|
|
|
8 |
H |
-0.050 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.063 |
-0.018 |
0.000 |
0.065 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.299 |
-2.266 |
0.000 |
y |
-2.266 |
-43.587 |
0.000 |
z |
0.000 |
0.000 |
-43.736 |
|
Traceless |
| x | y | z |
x |
-6.638 |
-2.266 |
0.000 |
y |
-2.266 |
3.430 |
0.000 |
z |
0.000 |
0.000 |
3.208 |
|
Polar |
3z2-r2 | 6.415 |
x2-y2 | -6.712 |
xy | -2.266 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
12.287 |
1.742 |
0.000 |
y |
1.742 |
8.437 |
0.000 |
z |
0.000 |
0.000 |
7.327 |
<r2> (average value of r
2) Å
2
<r2> |
282.819 |
(<r2>)1/2 |
16.817 |
Jump to
S1C1
Energy calculated at PBE1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -3112.423137 |
Energy at 298.15K | |
HF Energy | -3112.423137 |
Nuclear repulsion energy | 305.040592 |
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 PBE1PBE/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 |
3190 |
3068 |
0.52 |
38.37 |
0.75 |
0.86 |
2 |
A |
3170 |
3048 |
0.67 |
75.68 |
0.75 |
0.86 |
3 |
A |
3111 |
2991 |
10.79 |
178.87 |
0.03 |
0.06 |
4 |
A |
3094 |
2976 |
8.68 |
111.02 |
0.15 |
0.26 |
5 |
A |
1439 |
1383 |
3.47 |
3.66 |
0.75 |
0.86 |
6 |
A |
1428 |
1374 |
12.69 |
7.39 |
0.74 |
0.85 |
7 |
A |
1315 |
1265 |
16.62 |
1.81 |
0.33 |
0.50 |
8 |
A |
1273 |
1224 |
45.04 |
3.51 |
0.38 |
0.56 |
9 |
A |
1206 |
1160 |
1.34 |
5.35 |
0.70 |
0.82 |
10 |
A |
1133 |
1089 |
0.89 |
1.28 |
0.69 |
0.81 |
11 |
A |
1059 |
1019 |
2.39 |
1.15 |
0.68 |
0.81 |
12 |
A |
931 |
896 |
8.05 |
3.86 |
0.17 |
0.29 |
13 |
A |
866 |
833 |
20.99 |
1.40 |
0.74 |
0.85 |
14 |
A |
691 |
665 |
18.53 |
8.89 |
0.25 |
0.40 |
15 |
A |
590 |
568 |
11.08 |
17.13 |
0.13 |
0.23 |
16 |
A |
390 |
375 |
7.40 |
1.60 |
0.69 |
0.82 |
17 |
A |
244 |
234 |
1.27 |
1.16 |
0.23 |
0.37 |
18 |
A |
96 |
93 |
0.53 |
0.93 |
0.65 |
0.79 |
Unscaled Zero Point Vibrational Energy (zpe) 12613.3 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 12128.9 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 PBE1PBE/aug-cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.009 |
1.100 |
-0.383 |
C2 |
1.279 |
0.900 |
0.402 |
Br3 |
-1.352 |
-0.225 |
0.036 |
Cl4 |
2.164 |
-0.577 |
-0.086 |
H5 |
-0.427 |
2.074 |
-0.131 |
H6 |
0.185 |
1.039 |
-1.461 |
H7 |
1.954 |
1.745 |
0.215 |
H8 |
1.083 |
0.820 |
1.476 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5066 | 1.9457 | 2.7469 | 1.0964 | 1.0943 | 2.1341 | 2.1654 |
C2 | 1.5066 | | 2.8850 | 1.7892 | 2.1393 | 2.1654 | 1.0978 | 1.0951 | Br3 | 1.9457 | 2.8850 | | 3.5360 | 2.4836 | 2.4905 | 3.8526 | 3.0160 | Cl4 | 2.7469 | 1.7892 | 3.5360 | | 3.7075 | 2.9014 | 2.3510 | 2.3585 | H5 | 1.0964 | 2.1393 | 2.4836 | 3.7075 | | 1.7935 | 2.4285 | 2.5372 | H6 | 1.0943 | 2.1654 | 2.4905 | 2.9014 | 1.7935 | | 2.5370 | 3.0797 | H7 | 2.1341 | 1.0978 | 3.8526 | 2.3510 | 2.4285 | 2.5370 | | 1.7907 | H8 | 2.1654 | 1.0951 | 3.0160 | 2.3585 | 2.5372 | 3.0797 | 1.7907 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.626 |
|
C1 |
C2 |
H7 |
109.042 |
C1 |
C2 |
H8 |
111.696 |
|
C2 |
C1 |
Br3 |
112.756 |
C2 |
C1 |
Cl4 |
36.958 |
|
C2 |
C1 |
H6 |
111.745 |
Br3 |
C1 |
H5 |
106.063 |
|
Br3 |
C1 |
H6 |
106.638 |
Cl4 |
C2 |
H7 |
106.576 |
|
Cl4 |
C2 |
H8 |
107.248 |
H5 |
C1 |
H6 |
109.909 |
|
H7 |
C2 |
H8 |
109.492 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.034 |
|
|
|
2 |
C |
0.046 |
|
|
|
3 |
Br |
0.241 |
|
|
|
4 |
Cl |
-0.057 |
|
|
|
5 |
H |
-0.077 |
|
|
|
6 |
H |
-0.073 |
|
|
|
7 |
H |
-0.027 |
|
|
|
8 |
H |
-0.019 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.379 |
2.694 |
0.102 |
2.722 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.972 |
2.716 |
0.479 |
y |
2.716 |
-40.616 |
-0.106 |
z |
0.479 |
-0.106 |
-43.362 |
|
Traceless |
| x | y | z |
x |
-5.983 |
2.716 |
0.479 |
y |
2.716 |
5.052 |
-0.106 |
z |
0.479 |
-0.106 |
0.932 |
|
Polar |
3z2-r2 | 1.863 |
x2-y2 | -7.357 |
xy | 2.716 |
xz | 0.479 |
yz | -0.106 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.533 |
0.182 |
-0.162 |
y |
0.182 |
9.015 |
0.033 |
z |
-0.162 |
0.033 |
7.530 |
<r2> (average value of r
2) Å
2
<r2> |
221.163 |
(<r2>)1/2 |
14.872 |