Jump to
S1C2
Energy calculated at B2PLYP/6-311G*
| hartrees |
Energy at 0K | -3112.289833 |
Energy at 298.15K | |
HF Energy | -3112.110971 |
Nuclear repulsion energy | 287.509663 |
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 B2PLYP/6-311G*
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' |
3143 |
3143 |
13.10 |
10.89 |
0.08 |
0.14 |
2 |
A' |
3134 |
3134 |
1.54 |
146.18 |
0.08 |
0.15 |
3 |
A' |
1518 |
1518 |
1.17 |
12.87 |
0.72 |
0.84 |
4 |
A' |
1517 |
1517 |
6.28 |
2.70 |
0.72 |
0.84 |
5 |
A' |
1361 |
1361 |
3.27 |
14.74 |
0.62 |
0.77 |
6 |
A' |
1267 |
1267 |
50.28 |
3.12 |
0.52 |
0.69 |
7 |
A' |
1080 |
1080 |
1.01 |
9.66 |
0.74 |
0.85 |
8 |
A' |
745 |
745 |
28.15 |
56.22 |
0.30 |
0.46 |
9 |
A' |
645 |
645 |
61.05 |
12.87 |
0.25 |
0.40 |
10 |
A' |
249 |
249 |
0.83 |
5.01 |
0.38 |
0.55 |
11 |
A' |
197 |
197 |
7.56 |
0.19 |
0.31 |
0.48 |
12 |
A" |
3218 |
3218 |
3.91 |
2.79 |
0.75 |
0.86 |
13 |
A" |
3195 |
3195 |
0.47 |
96.78 |
0.75 |
0.86 |
14 |
A" |
1325 |
1325 |
0.21 |
5.67 |
0.75 |
0.86 |
15 |
A" |
1165 |
1165 |
4.77 |
0.09 |
0.75 |
0.86 |
16 |
A" |
1003 |
1003 |
0.20 |
6.47 |
0.75 |
0.86 |
17 |
A" |
783 |
783 |
4.83 |
0.03 |
0.75 |
0.86 |
18 |
A" |
117 |
117 |
5.84 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12831.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12831.6 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 B2PLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.644 |
0.000 |
C2 |
1.239 |
-0.222 |
0.000 |
Br3 |
-1.595 |
-0.505 |
0.000 |
Cl4 |
2.701 |
0.842 |
0.000 |
H5 |
-0.062 |
1.264 |
0.890 |
H6 |
-0.062 |
1.264 |
-0.890 |
H7 |
1.295 |
-0.844 |
0.889 |
H8 |
1.295 |
-0.844 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5114 | 1.9659 | 2.7079 | 1.0860 | 1.0860 | 2.1637 | 2.1637 |
C2 | 1.5114 | | 2.8473 | 1.8080 | 2.1656 | 2.1656 | 1.0863 | 1.0863 | Br3 | 1.9659 | 2.8473 | | 4.5016 | 2.5047 | 2.5047 | 3.0419 | 3.0419 | Cl4 | 2.7079 | 1.8080 | 4.5016 | | 2.9325 | 2.9325 | 2.3681 | 2.3681 | H5 | 1.0860 | 2.1656 | 2.5047 | 2.9325 | | 1.7791 | 2.5068 | 3.0735 | H6 | 1.0860 | 2.1656 | 2.5047 | 2.9325 | 1.7791 | | 3.0735 | 2.5068 | H7 | 2.1637 | 1.0863 | 3.0419 | 2.3681 | 2.5068 | 3.0735 | | 1.7776 | H8 | 2.1637 | 1.0863 | 3.0419 | 2.3681 | 3.0735 | 2.5068 | 1.7776 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.999 |
|
C1 |
C2 |
H7 |
111.753 |
C1 |
C2 |
H8 |
111.753 |
|
C2 |
C1 |
Br3 |
109.237 |
C2 |
C1 |
Cl4 |
39.147 |
|
C2 |
C1 |
H6 |
111.933 |
Br3 |
C1 |
H5 |
106.734 |
|
Br3 |
C1 |
H6 |
106.734 |
Cl4 |
C2 |
H7 |
107.158 |
|
Cl4 |
C2 |
H8 |
107.158 |
H5 |
C1 |
H6 |
109.997 |
|
H7 |
C2 |
H8 |
109.803 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.499 |
|
|
|
2 |
C |
-0.474 |
|
|
|
3 |
Br |
-0.045 |
|
|
|
4 |
Cl |
-0.085 |
|
|
|
5 |
H |
0.276 |
|
|
|
6 |
H |
0.276 |
|
|
|
7 |
H |
0.275 |
|
|
|
8 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.194 |
-0.067 |
0.000 |
0.205 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-51.384 |
-2.390 |
-0.009 |
y |
-2.390 |
-44.088 |
-0.003 |
z |
-0.009 |
-0.003 |
-44.172 |
|
Traceless |
| x | y | z |
x |
-7.254 |
-2.390 |
-0.009 |
y |
-2.390 |
3.690 |
-0.003 |
z |
-0.009 |
-0.003 |
3.564 |
|
Polar |
3z2-r2 | 7.129 |
x2-y2 | -7.296 |
xy | -2.390 |
xz | -0.009 |
yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.486 |
2.280 |
0.000 |
y |
2.280 |
6.428 |
0.000 |
z |
0.000 |
0.000 |
4.832 |
<r2> (average value of r
2) Å
2
<r2> |
286.187 |
(<r2>)1/2 |
16.917 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| hartrees |
Energy at 0K | -3112.286642 |
Energy at 298.15K | |
HF Energy | -3112.107597 |
Nuclear repulsion energy | 303.249336 |
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 B2PLYP/6-311G*
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 |
3192 |
3192 |
4.12 |
36.39 |
0.75 |
0.86 |
2 |
A |
3174 |
3174 |
1.96 |
94.16 |
0.75 |
0.86 |
3 |
A |
3121 |
3121 |
17.44 |
164.96 |
0.04 |
0.07 |
4 |
A |
3106 |
3106 |
10.35 |
94.88 |
0.26 |
0.41 |
5 |
A |
1501 |
1501 |
2.03 |
6.23 |
0.69 |
0.82 |
6 |
A |
1495 |
1495 |
10.93 |
12.95 |
0.73 |
0.85 |
7 |
A |
1375 |
1375 |
28.18 |
3.38 |
0.74 |
0.85 |
8 |
A |
1332 |
1332 |
50.43 |
1.88 |
0.58 |
0.73 |
9 |
A |
1243 |
1243 |
5.21 |
13.90 |
0.74 |
0.85 |
10 |
A |
1176 |
1176 |
3.31 |
5.65 |
0.74 |
0.85 |
11 |
A |
1060 |
1060 |
1.13 |
2.61 |
0.74 |
0.85 |
12 |
A |
954 |
954 |
10.37 |
7.03 |
0.43 |
0.60 |
13 |
A |
891 |
891 |
24.13 |
2.01 |
0.74 |
0.85 |
14 |
A |
683 |
683 |
23.27 |
10.51 |
0.43 |
0.61 |
15 |
A |
578 |
578 |
12.20 |
15.94 |
0.21 |
0.34 |
16 |
A |
390 |
390 |
7.28 |
2.73 |
0.71 |
0.83 |
17 |
A |
247 |
247 |
1.19 |
1.51 |
0.53 |
0.69 |
18 |
A |
101 |
101 |
0.54 |
1.94 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12809.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12809.2 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 B2PLYP/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.015 |
1.101 |
-0.385 |
C2 |
1.288 |
0.900 |
0.405 |
Br3 |
-1.365 |
-0.225 |
0.036 |
Cl4 |
2.186 |
-0.577 |
-0.086 |
H5 |
-0.416 |
2.071 |
-0.141 |
H6 |
0.191 |
1.038 |
-1.455 |
H7 |
1.954 |
1.744 |
0.224 |
H8 |
1.090 |
0.819 |
1.470 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5115 | 1.9592 | 2.7600 | 1.0888 | 1.0867 | 2.1321 | 2.1629 |
C2 | 1.5115 | | 2.9053 | 1.7970 | 2.1380 | 2.1636 | 1.0902 | 1.0871 | Br3 | 1.9592 | 2.9053 | | 3.5704 | 2.4905 | 2.4980 | 3.8639 | 3.0294 | Cl4 | 2.7600 | 1.7970 | 3.5704 | | 3.7124 | 2.9088 | 2.3531 | 2.3608 | H5 | 1.0888 | 2.1380 | 2.4905 | 3.7124 | | 1.7781 | 2.4201 | 2.5361 | H6 | 1.0867 | 2.1636 | 2.4980 | 2.9088 | 1.7781 | | 2.5352 | 3.0686 | H7 | 2.1321 | 1.0902 | 3.8639 | 2.3531 | 2.4201 | 2.5352 | | 1.7762 | H8 | 2.1629 | 1.0871 | 3.0294 | 2.3608 | 2.5361 | 3.0686 | 1.7762 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.787 |
|
C1 |
C2 |
H7 |
109.002 |
C1 |
C2 |
H8 |
111.639 |
|
C2 |
C1 |
Br3 |
113.039 |
C2 |
C1 |
Cl4 |
36.889 |
|
C2 |
C1 |
H6 |
111.724 |
Br3 |
C1 |
H5 |
106.037 |
|
Br3 |
C1 |
H6 |
106.659 |
Cl4 |
C2 |
H7 |
106.604 |
|
Cl4 |
C2 |
H8 |
107.309 |
H5 |
C1 |
H6 |
109.632 |
|
H7 |
C2 |
H8 |
109.334 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.502 |
|
|
|
2 |
C |
-0.471 |
|
|
|
3 |
Br |
-0.033 |
|
|
|
4 |
Cl |
-0.071 |
|
|
|
5 |
H |
0.263 |
|
|
|
6 |
H |
0.277 |
|
|
|
7 |
H |
0.263 |
|
|
|
8 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.274 |
2.799 |
0.114 |
2.815 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.639 |
2.933 |
0.396 |
y |
2.933 |
-41.142 |
-0.087 |
z |
0.396 |
-0.087 |
-43.819 |
|
Traceless |
| x | y | z |
x |
-6.159 |
2.933 |
0.396 |
y |
2.933 |
5.087 |
-0.087 |
z |
0.396 |
-0.087 |
1.072 |
|
Polar |
3z2-r2 | 2.144 |
x2-y2 | -7.497 |
xy | 2.933 |
xz | 0.396 |
yz | -0.087 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.270 |
0.262 |
-0.328 |
y |
0.262 |
7.323 |
0.077 |
z |
-0.328 |
0.077 |
5.179 |
<r2> (average value of r
2) Å
2
<r2> |
224.461 |
(<r2>)1/2 |
14.982 |