Jump to
S1C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -218.238219 |
| Energy at 298.15K | -218.232118 |
| HF Energy | -218.386686 |
| Nuclear repulsion energy | 127.943952 |
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 B3LYP/6-31G(2df,p)
| 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' |
3112 |
3003 |
27.34 |
|
|
|
| 2 |
A' |
3039 |
2933 |
43.55 |
|
|
|
| 3 |
A' |
3033 |
2927 |
11.93 |
|
|
|
| 4 |
A' |
3007 |
2902 |
33.49 |
|
|
|
| 5 |
A' |
1524 |
1471 |
2.32 |
|
|
|
| 6 |
A' |
1507 |
1454 |
2.64 |
|
|
|
| 7 |
A' |
1492 |
1440 |
0.33 |
|
|
|
| 8 |
A' |
1438 |
1387 |
15.31 |
|
|
|
| 9 |
A' |
1412 |
1363 |
0.25 |
|
|
|
| 10 |
A' |
1335 |
1288 |
2.49 |
|
|
|
| 11 |
A' |
1137 |
1097 |
4.77 |
|
|
|
| 12 |
A' |
1085 |
1047 |
93.02 |
|
|
|
| 13 |
A' |
1038 |
1002 |
3.72 |
|
|
|
| 14 |
A' |
899 |
867 |
7.26 |
|
|
|
| 15 |
A' |
449 |
434 |
5.15 |
|
|
|
| 16 |
A' |
264 |
255 |
2.46 |
|
|
|
| 17 |
A" |
3102 |
2994 |
65.40 |
|
|
|
| 18 |
A" |
3076 |
2968 |
11.25 |
|
|
|
| 19 |
A" |
3044 |
2937 |
22.15 |
|
|
|
| 20 |
A" |
1502 |
1449 |
5.46 |
|
|
|
| 21 |
A" |
1316 |
1269 |
0.06 |
|
|
|
| 22 |
A" |
1272 |
1228 |
0.50 |
|
|
|
| 23 |
A" |
1201 |
1159 |
1.31 |
|
|
|
| 24 |
A" |
893 |
862 |
1.56 |
|
|
|
| 25 |
A" |
764 |
737 |
1.61 |
|
|
|
| 26 |
A" |
233 |
225 |
0.00 |
|
|
|
| 27 |
A" |
127 |
123 |
2.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21149.8 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 20409.5 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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.130 |
-0.790 |
0.000 |
| C2 |
0.000 |
0.725 |
0.000 |
| C3 |
-1.462 |
1.180 |
0.000 |
| F4 |
1.462 |
-1.153 |
0.000 |
| H5 |
-0.346 |
-1.226 |
0.889 |
| H6 |
-0.346 |
-1.226 |
-0.889 |
| H7 |
0.522 |
1.119 |
-0.880 |
| H8 |
0.522 |
1.119 |
0.880 |
| H9 |
-1.531 |
2.272 |
0.000 |
| H10 |
-1.995 |
0.814 |
-0.884 |
| H11 |
-1.995 |
0.814 |
0.884 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5206 | 2.5332 | 1.3810 | 1.0986 | 1.0986 | 2.1384 | 2.1384 | 3.4833 | 2.8053 | 2.8053 |
C2 | 1.5206 | | 1.5312 | 2.3804 | 2.1715 | 2.1715 | 1.0962 | 1.0962 | 2.1763 | 2.1839 | 2.1839 | C3 | 2.5332 | 1.5312 | | 3.7414 | 2.7975 | 2.7975 | 2.1708 | 2.1708 | 1.0934 | 1.0956 | 1.0956 | F4 | 1.3810 | 2.3804 | 3.7414 | | 2.0162 | 2.0162 | 2.6122 | 2.6122 | 4.5487 | 4.0748 | 4.0748 | H5 | 1.0986 | 2.1715 | 2.7975 | 2.0162 | | 1.7784 | 3.0628 | 2.5003 | 3.7983 | 3.1662 | 2.6229 | H6 | 1.0986 | 2.1715 | 2.7975 | 2.0162 | 1.7784 | | 2.5003 | 3.0628 | 3.7983 | 2.6229 | 3.1662 | H7 | 2.1384 | 1.0962 | 2.1708 | 2.6122 | 3.0628 | 2.5003 | | 1.7595 | 2.5130 | 2.5350 | 3.0883 | H8 | 2.1384 | 1.0962 | 2.1708 | 2.6122 | 2.5003 | 3.0628 | 1.7595 | | 2.5130 | 3.0883 | 2.5350 | H9 | 3.4833 | 2.1763 | 1.0934 | 4.5487 | 3.7983 | 3.7983 | 2.5130 | 2.5130 | | 1.7670 | 1.7670 | H10 | 2.8053 | 2.1839 | 1.0956 | 4.0748 | 3.1662 | 2.6229 | 2.5350 | 3.0883 | 1.7670 | | 1.7686 | H11 | 2.8053 | 2.1839 | 1.0956 | 4.0748 | 2.6229 | 3.1662 | 3.0883 | 2.5350 | 1.7670 | 1.7686 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.192 |
|
C1 |
C2 |
H7 |
108.530 |
| C1 |
C2 |
H8 |
108.530 |
|
C2 |
C1 |
F4 |
110.150 |
| C2 |
C1 |
H5 |
110.989 |
|
C2 |
C1 |
H6 |
110.989 |
| C2 |
C3 |
H9 |
110.925 |
|
C2 |
C3 |
H10 |
111.402 |
| C2 |
C3 |
H11 |
111.402 |
|
C3 |
C2 |
H7 |
110.326 |
| C3 |
C2 |
H8 |
110.326 |
|
F4 |
C1 |
H5 |
108.270 |
| F4 |
C1 |
H6 |
108.270 |
|
H5 |
C1 |
H6 |
108.076 |
| H7 |
C2 |
H8 |
106.760 |
|
H9 |
C3 |
H10 |
107.647 |
| H9 |
C3 |
H11 |
107.647 |
|
H10 |
C3 |
H11 |
107.634 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.038 |
|
|
|
| 2 |
C |
-0.191 |
|
|
|
| 3 |
C |
-0.385 |
|
|
|
| 4 |
F |
-0.160 |
|
|
|
| 5 |
H |
0.097 |
|
|
|
| 6 |
H |
0.097 |
|
|
|
| 7 |
H |
0.110 |
|
|
|
| 8 |
H |
0.110 |
|
|
|
| 9 |
H |
0.123 |
|
|
|
| 10 |
H |
0.119 |
|
|
|
| 11 |
H |
0.119 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.530 |
0.713 |
0.000 |
1.688 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
103.350 |
| (<r2>)1/2 |
10.166 |
Jump to
S1C1
Energy calculated at G4
| | hartrees |
| Energy at 0K | -5621.140673 |
| Energy at 298.15K | -5621.134661 |
| HF Energy | -218.387314 |
| Nuclear repulsion energy | 130.449488 |
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 B3LYP/6-31G(2df,p)
| 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 |
3123 |
3014 |
23.24 |
|
|
|
| 2 |
A |
3105 |
2997 |
41.47 |
|
|
|
| 3 |
A |
3070 |
2962 |
36.54 |
|
|
|
| 4 |
A |
3056 |
2949 |
43.58 |
|
|
|
| 5 |
A |
3038 |
2931 |
20.84 |
|
|
|
| 6 |
A |
3028 |
2922 |
12.09 |
|
|
|
| 7 |
A |
3011 |
2906 |
40.81 |
|
|
|
| 8 |
A |
1516 |
1463 |
1.02 |
|
|
|
| 9 |
A |
1509 |
1456 |
5.62 |
|
|
|
| 10 |
A |
1495 |
1443 |
5.04 |
|
|
|
| 11 |
A |
1476 |
1424 |
1.32 |
|
|
|
| 12 |
A |
1435 |
1384 |
13.60 |
|
|
|
| 13 |
A |
1405 |
1356 |
3.48 |
|
|
|
| 14 |
A |
1381 |
1332 |
1.17 |
|
|
|
| 15 |
A |
1302 |
1256 |
1.00 |
|
|
|
| 16 |
A |
1277 |
1232 |
1.24 |
|
|
|
| 17 |
A |
1182 |
1141 |
1.48 |
|
|
|
| 18 |
A |
1127 |
1088 |
19.54 |
|
|
|
| 19 |
A |
1089 |
1051 |
40.63 |
|
|
|
| 20 |
A |
987 |
953 |
33.25 |
|
|
|
| 21 |
A |
920 |
888 |
2.69 |
|
|
|
| 22 |
A |
874 |
843 |
3.13 |
|
|
|
| 23 |
A |
770 |
743 |
0.45 |
|
|
|
| 24 |
A |
478 |
462 |
2.90 |
|
|
|
| 25 |
A |
311 |
300 |
1.05 |
|
|
|
| 26 |
A |
217 |
209 |
1.56 |
|
|
|
| 27 |
A |
143 |
138 |
1.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21162.4 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 20421.7 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 B3LYP/6-31G(2df,p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.808 |
0.510 |
0.291 |
| C2 |
-0.593 |
0.667 |
-0.276 |
| C3 |
-1.523 |
-0.484 |
0.118 |
| F4 |
1.377 |
-0.665 |
-0.171 |
| H5 |
1.456 |
1.343 |
-0.009 |
| H6 |
0.786 |
0.465 |
1.389 |
| H7 |
-0.521 |
0.735 |
-1.368 |
| H8 |
-0.995 |
1.626 |
0.073 |
| H9 |
-2.510 |
-0.372 |
-0.339 |
| H10 |
-1.102 |
-1.440 |
-0.206 |
| H11 |
-1.658 |
-0.529 |
1.204 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 1.5201 | 2.5399 | 1.3847 | 1.0974 | 1.0987 | 2.1377 | 2.1320 | 3.4908 | 2.7744 | 2.8278 |
C2 | 1.5201 | | 1.5308 | 2.3806 | 2.1745 | 2.1716 | 1.0967 | 1.0974 | 2.1811 | 2.1681 | 2.1808 | C3 | 2.5399 | 1.5308 | | 2.9198 | 3.4967 | 2.8014 | 2.1677 | 2.1760 | 1.0937 | 1.0932 | 1.0958 | F4 | 1.3847 | 2.3806 | 2.9198 | | 2.0164 | 2.0147 | 2.6447 | 3.3071 | 3.9019 | 2.5977 | 3.3351 | H5 | 1.0974 | 2.1745 | 3.4967 | 2.0164 | | 1.7812 | 2.4747 | 2.4683 | 4.3336 | 3.7852 | 3.8308 | H6 | 1.0987 | 2.1716 | 2.8014 | 2.0147 | 1.7812 | | 3.0630 | 2.5004 | 3.8147 | 3.1207 | 2.6454 | H7 | 2.1377 | 1.0967 | 2.1677 | 2.6447 | 2.4747 | 3.0630 | | 1.7600 | 2.4988 | 2.5333 | 3.0839 | H8 | 2.1320 | 1.0974 | 2.1760 | 3.3071 | 2.4683 | 2.5004 | 1.7600 | | 2.5416 | 3.0807 | 2.5231 | H9 | 3.4908 | 2.1811 | 1.0937 | 3.9019 | 4.3336 | 3.8147 | 2.4988 | 2.5416 | | 1.7719 | 1.7697 | H10 | 2.7744 | 2.1681 | 1.0932 | 2.5977 | 3.7852 | 3.1207 | 2.5333 | 3.0807 | 1.7719 | | 1.7686 | H11 | 2.8278 | 2.1808 | 1.0958 | 3.3351 | 3.8308 | 2.6454 | 3.0839 | 2.5231 | 1.7697 | 1.7686 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.704 |
|
C1 |
C2 |
H7 |
108.482 |
| C1 |
C2 |
H8 |
107.996 |
|
C2 |
C1 |
F4 |
109.982 |
| C2 |
C1 |
H5 |
111.308 |
|
C2 |
C1 |
H6 |
111.018 |
| C2 |
C3 |
H9 |
111.300 |
|
C2 |
C3 |
H10 |
110.346 |
| C2 |
C3 |
H11 |
111.166 |
|
C3 |
C2 |
H7 |
110.087 |
| C3 |
C2 |
H8 |
110.683 |
|
F4 |
C1 |
H5 |
108.126 |
| F4 |
C1 |
H6 |
107.900 |
|
H5 |
C1 |
H6 |
108.393 |
| H7 |
C2 |
H8 |
106.672 |
|
H9 |
C3 |
H10 |
108.259 |
| H9 |
C3 |
H11 |
107.841 |
|
H10 |
C3 |
H11 |
107.796 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.036 |
|
|
|
| 2 |
C |
-0.193 |
|
|
|
| 3 |
C |
-0.369 |
|
|
|
| 4 |
F |
-0.167 |
|
|
|
| 5 |
H |
0.098 |
|
|
|
| 6 |
H |
0.097 |
|
|
|
| 7 |
H |
0.110 |
|
|
|
| 8 |
H |
0.099 |
|
|
|
| 9 |
H |
0.114 |
|
|
|
| 10 |
H |
0.133 |
|
|
|
| 11 |
H |
0.114 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.834 |
1.276 |
0.393 |
1.574 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
91.176 |
| (<r2>)1/2 |
9.549 |