Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -638.696974 |
| Energy at 298.15K | -638.701859 |
| HF Energy | -638.696974 |
| Nuclear repulsion energy | 157.585735 |
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 B1B95/6-311G*
| 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' |
3128 |
2998 |
21.20 |
|
|
|
| 2 |
A' |
3092 |
2964 |
22.19 |
|
|
|
| 3 |
A' |
1534 |
1470 |
1.86 |
|
|
|
| 4 |
A' |
1507 |
1445 |
5.24 |
|
|
|
| 5 |
A' |
1440 |
1380 |
4.68 |
|
|
|
| 6 |
A' |
1307 |
1253 |
13.65 |
|
|
|
| 7 |
A' |
1097 |
1052 |
31.33 |
|
|
|
| 8 |
A' |
1084 |
1039 |
98.41 |
|
|
|
| 9 |
A' |
787 |
754 |
48.52 |
|
|
|
| 10 |
A' |
385 |
369 |
2.62 |
|
|
|
| 11 |
A' |
236 |
226 |
12.24 |
|
|
|
| 12 |
A" |
3196 |
3063 |
14.42 |
|
|
|
| 13 |
A" |
3147 |
3017 |
19.32 |
|
|
|
| 14 |
A" |
1320 |
1265 |
0.25 |
|
|
|
| 15 |
A" |
1238 |
1187 |
0.80 |
|
|
|
| 16 |
A" |
1083 |
1038 |
4.88 |
|
|
|
| 17 |
A" |
801 |
768 |
1.08 |
|
|
|
| 18 |
A" |
132 |
126 |
10.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13256.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12707.2 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.609 |
0.000 |
| C2 |
0.989 |
-0.529 |
0.000 |
| Cl3 |
-1.662 |
-0.044 |
0.000 |
| F4 |
2.259 |
0.013 |
0.000 |
| H5 |
0.115 |
1.226 |
0.887 |
| H6 |
0.115 |
1.226 |
-0.887 |
| H7 |
0.876 |
-1.148 |
0.890 |
| H8 |
0.876 |
-1.148 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5078 | 1.7856 | 2.3367 | 1.0863 | 1.0863 | 2.1555 | 2.1555 |
C2 | 1.5078 | | 2.6953 | 1.3806 | 2.1515 | 2.1515 | 1.0901 | 1.0901 | Cl3 | 1.7856 | 2.6953 | | 3.9217 | 2.3574 | 2.3574 | 2.9072 | 2.9072 | F4 | 2.3367 | 1.3806 | 3.9217 | | 2.6182 | 2.6182 | 2.0131 | 2.0131 | H5 | 1.0863 | 2.1515 | 2.3574 | 2.6182 | | 1.7736 | 2.4924 | 3.0610 | H6 | 1.0863 | 2.1515 | 2.3574 | 2.6182 | 1.7736 | | 3.0610 | 2.4924 | H7 | 2.1555 | 1.0901 | 2.9072 | 2.0131 | 2.4924 | 3.0610 | | 1.7804 | H8 | 2.1555 | 1.0901 | 2.9072 | 2.0131 | 3.0610 | 2.4924 | 1.7804 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.916 |
|
C1 |
C2 |
H7 |
111.111 |
| C1 |
C2 |
H8 |
111.111 |
|
C2 |
C1 |
Cl3 |
109.560 |
| C2 |
C1 |
H5 |
111.023 |
|
C2 |
C1 |
H6 |
111.023 |
| Cl3 |
C1 |
H5 |
107.844 |
|
Cl3 |
C1 |
H6 |
107.844 |
| F4 |
C2 |
H7 |
108.563 |
|
F4 |
C2 |
H8 |
108.563 |
| H5 |
C1 |
H6 |
109.441 |
|
H7 |
C2 |
H8 |
109.494 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.559 |
|
|
|
| 2 |
C |
-0.098 |
|
|
|
| 3 |
Cl |
-0.079 |
|
|
|
| 4 |
F |
-0.266 |
|
|
|
| 5 |
H |
0.279 |
|
|
|
| 6 |
H |
0.279 |
|
|
|
| 7 |
H |
0.222 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.226 |
0.041 |
0.000 |
0.230 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.909 |
-0.584 |
0.000 |
| y |
-0.584 |
-29.083 |
0.000 |
| z |
0.000 |
0.000 |
-29.627 |
|
| Traceless |
| | x | y | z |
| x |
-8.554 |
-0.584 |
0.000 |
| y |
-0.584 |
4.685 |
0.000 |
| z |
0.000 |
0.000 |
3.870 |
|
| Polar |
| 3z2-r2 | 7.739 |
| x2-y2 | -8.826 |
| xy | -0.584 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.252 |
0.399 |
0.000 |
| y |
0.399 |
4.340 |
0.000 |
| z |
0.000 |
0.000 |
3.827 |
<r2> (average value of r
2) Å
2
| <r2> |
133.182 |
| (<r2>)1/2 |
11.540 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -638.696383 |
| Energy at 298.15K | -638.701373 |
| HF Energy | -638.696383 |
| Nuclear repulsion energy | 161.567851 |
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 B1B95/6-311G*
| 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 |
3183 |
3051 |
9.39 |
|
|
|
| 2 |
A |
3133 |
3003 |
33.19 |
|
|
|
| 3 |
A |
3117 |
2988 |
11.30 |
|
|
|
| 4 |
A |
3068 |
2941 |
31.77 |
|
|
|
| 5 |
A |
1516 |
1453 |
3.38 |
|
|
|
| 6 |
A |
1477 |
1416 |
11.53 |
|
|
|
| 7 |
A |
1444 |
1384 |
13.51 |
|
|
|
| 8 |
A |
1356 |
1300 |
33.43 |
|
|
|
| 9 |
A |
1296 |
1243 |
0.59 |
|
|
|
| 10 |
A |
1242 |
1191 |
2.08 |
|
|
|
| 11 |
A |
1133 |
1086 |
70.99 |
|
|
|
| 12 |
A |
1082 |
1038 |
29.03 |
|
|
|
| 13 |
A |
987 |
946 |
7.25 |
|
|
|
| 14 |
A |
866 |
831 |
8.63 |
|
|
|
| 15 |
A |
691 |
662 |
33.92 |
|
|
|
| 16 |
A |
465 |
446 |
12.90 |
|
|
|
| 17 |
A |
286 |
274 |
1.06 |
|
|
|
| 18 |
A |
129 |
124 |
2.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13235.1 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12687.2 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 B1B95/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.083 |
0.838 |
-0.293 |
| C2 |
1.197 |
0.409 |
0.360 |
| Cl3 |
-1.430 |
-0.282 |
0.064 |
| F4 |
1.661 |
-0.755 |
-0.202 |
| H5 |
-0.378 |
1.822 |
0.065 |
| H6 |
0.030 |
0.866 |
-1.374 |
| H7 |
1.952 |
1.186 |
0.205 |
| H8 |
1.062 |
0.245 |
1.430 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5006 | 1.7874 | 2.3645 | 1.0880 | 1.0870 | 2.1243 | 2.1523 |
C2 | 1.5006 | | 2.7327 | 1.3742 | 2.1366 | 2.1401 | 1.0938 | 1.0906 | Cl3 | 1.7874 | 2.7327 | | 3.1383 | 2.3525 | 2.3492 | 3.6892 | 2.8894 | F4 | 2.3645 | 1.3742 | 3.1383 | | 3.2974 | 2.5814 | 2.0046 | 2.0062 | H5 | 1.0880 | 2.1366 | 2.3525 | 3.2974 | | 1.7749 | 2.4193 | 2.5344 | H6 | 1.0870 | 2.1401 | 2.3492 | 2.5814 | 1.7749 | | 2.5078 | 3.0516 | H7 | 2.1243 | 1.0938 | 3.6892 | 2.0046 | 2.4193 | 2.5078 | | 1.7829 | H8 | 2.1523 | 1.0906 | 2.8894 | 2.0062 | 2.5344 | 3.0516 | 1.7829 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.594 |
|
C1 |
C2 |
H7 |
108.921 |
| C1 |
C2 |
H8 |
111.344 |
|
C2 |
C1 |
Cl3 |
112.134 |
| C2 |
C1 |
H5 |
110.236 |
|
C2 |
C1 |
H6 |
110.577 |
| Cl3 |
C1 |
H5 |
107.286 |
|
Cl3 |
C1 |
H6 |
107.099 |
| F4 |
C2 |
H7 |
108.092 |
|
F4 |
C2 |
H8 |
108.415 |
| H5 |
C1 |
H6 |
109.387 |
|
H7 |
C2 |
H8 |
109.412 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.552 |
|
|
|
| 2 |
C |
-0.102 |
|
|
|
| 3 |
Cl |
-0.074 |
|
|
|
| 4 |
F |
-0.255 |
|
|
|
| 5 |
H |
0.266 |
|
|
|
| 6 |
H |
0.279 |
|
|
|
| 7 |
H |
0.210 |
|
|
|
| 8 |
H |
0.228 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.965 |
2.725 |
0.314 |
2.908 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.502 |
2.369 |
0.967 |
| y |
2.369 |
-29.577 |
-0.482 |
| z |
0.967 |
-0.482 |
-29.558 |
|
| Traceless |
| | x | y | z |
| x |
-3.935 |
2.369 |
0.967 |
| y |
2.369 |
1.953 |
-0.482 |
| z |
0.967 |
-0.482 |
1.982 |
|
| Polar |
| 3z2-r2 | 3.963 |
| x2-y2 | -3.926 |
| xy | 2.369 |
| xz | 0.967 |
| yz | -0.482 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.780 |
0.995 |
-0.083 |
| y |
0.995 |
4.712 |
-0.206 |
| z |
-0.083 |
-0.206 |
4.023 |
<r2> (average value of r
2) Å
2
| <r2> |
115.555 |
| (<r2>)1/2 |
10.750 |