Jump to
S1C2
Energy calculated at G3
| | hartrees |
| Energy at 0K | -638.386798 |
| Energy at 298.15K | -638.381153 |
| HF Energy | -636.976671 |
| Nuclear repulsion energy | 157.798252 |
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 HF/6-31G*
| 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' |
3299 |
3108 |
22.91 |
|
|
|
| 2 |
A' |
3272 |
3083 |
24.08 |
|
|
|
| 3 |
A' |
1679 |
1582 |
0.23 |
|
|
|
| 4 |
A' |
1645 |
1550 |
9.29 |
|
|
|
| 5 |
A' |
1578 |
1486 |
6.61 |
|
|
|
| 6 |
A' |
1423 |
1341 |
25.16 |
|
|
|
| 7 |
A' |
1184 |
1116 |
137.82 |
|
|
|
| 8 |
A' |
1151 |
1085 |
4.41 |
|
|
|
| 9 |
A' |
836 |
787 |
73.36 |
|
|
|
| 10 |
A' |
411 |
388 |
2.77 |
|
|
|
| 11 |
A' |
267 |
251 |
14.25 |
|
|
|
| 12 |
A" |
3367 |
3172 |
17.53 |
|
|
|
| 13 |
A" |
3325 |
3133 |
25.10 |
|
|
|
| 14 |
A" |
1426 |
1344 |
0.07 |
|
|
|
| 15 |
A" |
1342 |
1264 |
2.82 |
|
|
|
| 16 |
A" |
1175 |
1107 |
2.81 |
|
|
|
| 17 |
A" |
860 |
811 |
0.11 |
|
|
|
| 18 |
A" |
141 |
133 |
12.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14190.0 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13369.8 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 MP2=FULL/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.604 |
0.000 |
| C2 |
0.983 |
-0.545 |
0.000 |
| Cl3 |
-1.664 |
-0.029 |
0.000 |
| F4 |
2.265 |
0.003 |
0.000 |
| H5 |
0.135 |
1.220 |
0.889 |
| H6 |
0.135 |
1.220 |
-0.889 |
| H7 |
0.865 |
-1.165 |
0.892 |
| H8 |
0.865 |
-1.165 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5124 | 1.7799 | 2.3433 | 1.0896 | 1.0896 | 2.1618 | 2.1618 |
C2 | 1.5124 | | 2.6963 | 1.3944 | 2.1506 | 2.1506 | 1.0926 | 1.0926 | Cl3 | 1.7799 | 2.6963 | | 3.9285 | 2.3631 | 2.3631 | 2.9117 | 2.9117 | F4 | 2.3433 | 1.3944 | 3.9285 | | 2.6091 | 2.6091 | 2.0299 | 2.0299 | H5 | 1.0896 | 2.1506 | 2.3631 | 2.6091 | | 1.7776 | 2.4940 | 3.0646 | H6 | 1.0896 | 2.1506 | 2.3631 | 2.6091 | 1.7776 | | 3.0646 | 2.4940 | H7 | 2.1618 | 1.0926 | 2.9117 | 2.0299 | 2.4940 | 3.0646 | | 1.7842 | H8 | 2.1618 | 1.0926 | 2.9117 | 2.0299 | 3.0646 | 2.4940 | 1.7842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.455 |
|
C1 |
C2 |
H7 |
111.271 |
| C1 |
C2 |
H8 |
111.271 |
|
C2 |
C1 |
Cl3 |
109.922 |
| C2 |
C1 |
H5 |
110.927 |
|
C2 |
C1 |
H6 |
110.927 |
| Cl3 |
C1 |
H5 |
107.735 |
|
Cl3 |
C1 |
H6 |
107.735 |
| F4 |
C2 |
H7 |
108.605 |
|
F4 |
C2 |
H8 |
108.605 |
| H5 |
C1 |
H6 |
109.489 |
|
H7 |
C2 |
H8 |
109.540 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at G3
| | hartrees |
| Energy at 0K | -638.386032 |
| Energy at 298.15K | -638.391404 |
| HF Energy | -636.975419 |
| Nuclear repulsion energy | 161.937605 |
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 HF/6-31G*
| 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 |
3352 |
3159 |
11.93 |
|
|
|
| 2 |
A |
3312 |
3120 |
34.44 |
|
|
|
| 3 |
A |
3287 |
3097 |
21.92 |
|
|
|
| 4 |
A |
3246 |
3059 |
34.09 |
|
|
|
| 5 |
A |
1666 |
1569 |
0.92 |
|
|
|
| 6 |
A |
1621 |
1527 |
10.95 |
|
|
|
| 7 |
A |
1580 |
1489 |
23.56 |
|
|
|
| 8 |
A |
1480 |
1394 |
45.23 |
|
|
|
| 9 |
A |
1400 |
1319 |
0.13 |
|
|
|
| 10 |
A |
1341 |
1264 |
4.78 |
|
|
|
| 11 |
A |
1222 |
1151 |
83.50 |
|
|
|
| 12 |
A |
1174 |
1106 |
19.74 |
|
|
|
| 13 |
A |
1061 |
1000 |
4.24 |
|
|
|
| 14 |
A |
939 |
884 |
12.44 |
|
|
|
| 15 |
A |
734 |
692 |
46.35 |
|
|
|
| 16 |
A |
504 |
475 |
16.44 |
|
|
|
| 17 |
A |
305 |
288 |
0.89 |
|
|
|
| 18 |
A |
143 |
134 |
2.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14183.8 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13364.0 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 MP2=FULL/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.091 |
0.849 |
-0.294 |
| C2 |
1.199 |
0.422 |
0.358 |
| Cl3 |
-1.414 |
-0.285 |
0.066 |
| F4 |
1.634 |
-0.773 |
-0.201 |
| H5 |
-0.385 |
1.836 |
0.066 |
| H6 |
0.033 |
0.882 |
-1.377 |
| H7 |
1.965 |
1.185 |
0.180 |
| H8 |
1.070 |
0.277 |
1.433 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5069 | 1.7790 | 2.3696 | 1.0918 | 1.0903 | 2.1363 | 2.1587 |
C2 | 1.5069 | | 2.7222 | 1.3894 | 2.1431 | 2.1401 | 1.0955 | 1.0927 | Cl3 | 1.7790 | 2.7222 | | 3.0983 | 2.3574 | 2.3536 | 3.6861 | 2.8905 | F4 | 2.3696 | 1.3894 | 3.0983 | | 3.3102 | 2.5860 | 2.0219 | 2.0225 | H5 | 1.0918 | 2.1431 | 2.3574 | 3.3102 | | 1.7800 | 2.4410 | 2.5333 | H6 | 1.0903 | 2.1401 | 2.3536 | 2.5860 | 1.7800 | | 2.4991 | 3.0561 | H7 | 2.1363 | 1.0955 | 3.6861 | 2.0219 | 2.4410 | 2.4991 | | 1.7876 | H8 | 2.1587 | 1.0927 | 2.8905 | 2.0225 | 2.5333 | 3.0561 | 1.7876 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.126 |
|
C1 |
C2 |
H7 |
108.970 |
| C1 |
C2 |
H8 |
111.430 |
|
C2 |
C1 |
Cl3 |
112.069 |
| C2 |
C1 |
H5 |
110.243 |
|
C2 |
C1 |
H6 |
110.476 |
| Cl3 |
C1 |
H5 |
107.232 |
|
Cl3 |
C1 |
H6 |
107.175 |
| F4 |
C2 |
H7 |
108.198 |
|
F4 |
C2 |
H8 |
108.620 |
| H5 |
C1 |
H6 |
109.532 |
|
H7 |
C2 |
H8 |
109.436 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability