Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -215.860273 |
| Energy at 298.15K | |
| HF Energy | -215.860273 |
| Nuclear repulsion energy | 116.828807 |
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 B1B95/3-21G
| 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' |
3296 |
3153 |
3.73 |
44.15 |
0.69 |
0.81 |
| 2 |
A' |
3215 |
3076 |
5.59 |
128.43 |
0.16 |
0.28 |
| 3 |
A' |
3200 |
3061 |
3.21 |
28.83 |
0.44 |
0.61 |
| 4 |
A' |
3052 |
2920 |
34.61 |
140.86 |
0.12 |
0.21 |
| 5 |
A' |
1747 |
1671 |
2.57 |
11.36 |
0.11 |
0.19 |
| 6 |
A' |
1566 |
1498 |
2.41 |
23.46 |
0.64 |
0.78 |
| 7 |
A' |
1481 |
1416 |
8.86 |
11.73 |
0.52 |
0.68 |
| 8 |
A' |
1435 |
1373 |
6.22 |
14.89 |
0.59 |
0.74 |
| 9 |
A' |
1350 |
1292 |
0.08 |
15.61 |
0.43 |
0.60 |
| 10 |
A' |
1145 |
1095 |
22.80 |
2.45 |
0.73 |
0.85 |
| 11 |
A' |
1038 |
993 |
30.29 |
5.06 |
0.75 |
0.85 |
| 12 |
A' |
922 |
882 |
1.94 |
3.91 |
0.16 |
0.28 |
| 13 |
A' |
613 |
586 |
1.95 |
1.59 |
0.73 |
0.84 |
| 14 |
A' |
297 |
284 |
4.68 |
0.80 |
0.49 |
0.66 |
| 15 |
A" |
3084 |
2950 |
37.69 |
96.24 |
0.75 |
0.86 |
| 16 |
A" |
1274 |
1219 |
0.21 |
14.44 |
0.75 |
0.86 |
| 17 |
A" |
1077 |
1030 |
1.02 |
1.16 |
0.75 |
0.86 |
| 18 |
A" |
1050 |
1005 |
22.92 |
0.10 |
0.75 |
0.86 |
| 19 |
A" |
1003 |
959 |
59.34 |
0.54 |
0.75 |
0.86 |
| 20 |
A" |
591 |
566 |
16.40 |
13.46 |
0.75 |
0.86 |
| 21 |
A" |
200 |
192 |
3.72 |
6.19 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16316.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15610.0 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
-0.972 |
0.000 |
| C2 |
-0.961 |
0.175 |
0.000 |
| C3 |
-0.530 |
1.427 |
0.000 |
| F4 |
1.328 |
-0.489 |
0.000 |
| H5 |
-1.205 |
2.272 |
0.000 |
| H6 |
0.533 |
1.624 |
0.000 |
| H7 |
-2.015 |
-0.082 |
0.000 |
| H8 |
-0.154 |
-1.599 |
0.886 |
| H9 |
-0.154 |
-1.599 |
-0.886 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4970 | 2.4570 | 1.4129 | 3.4606 | 2.6506 | 2.2025 | 1.0959 | 1.0959 |
C2 | 1.4970 | | 1.3237 | 2.3833 | 2.1106 | 2.0816 | 1.0844 | 2.1407 | 2.1407 | C3 | 2.4570 | 1.3237 | | 2.6685 | 1.0812 | 1.0816 | 2.1168 | 3.1748 | 3.1748 | F4 | 1.4129 | 2.3833 | 2.6685 | | 3.7462 | 2.2573 | 3.3669 | 2.0526 | 2.0526 | H5 | 3.4606 | 2.1106 | 1.0812 | 3.7462 | | 1.8548 | 2.4895 | 4.1071 | 4.1071 | H6 | 2.6506 | 2.0816 | 1.0816 | 2.2573 | 1.8548 | | 3.0666 | 3.4123 | 3.4123 | H7 | 2.2025 | 1.0844 | 2.1168 | 3.3669 | 2.4895 | 3.0666 | | 2.5581 | 2.5581 | H8 | 1.0959 | 2.1407 | 3.1748 | 2.0526 | 4.1071 | 3.4123 | 2.5581 | | 1.7718 | H9 | 1.0959 | 2.1407 | 3.1748 | 2.0526 | 4.1071 | 3.4123 | 2.5581 | 1.7718 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.038 |
|
C1 |
C2 |
H7 |
116.212 |
| C2 |
C1 |
F4 |
109.944 |
|
C2 |
C1 |
H8 |
110.338 |
| C2 |
C1 |
H9 |
110.338 |
|
C2 |
C3 |
H5 |
122.389 |
| C2 |
C3 |
H6 |
119.520 |
|
C3 |
C2 |
H7 |
122.750 |
| F4 |
C1 |
H8 |
109.151 |
|
F4 |
C1 |
H9 |
109.151 |
| H5 |
C3 |
H6 |
118.091 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.114 |
|
|
|
| 2 |
C |
-0.282 |
|
|
|
| 3 |
C |
-0.390 |
|
|
|
| 4 |
F |
-0.303 |
|
|
|
| 5 |
H |
0.207 |
|
|
|
| 6 |
H |
0.226 |
|
|
|
| 7 |
H |
0.217 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
| 9 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.621 |
-0.674 |
0.000 |
1.755 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.496 |
1.094 |
0.000 |
| y |
1.094 |
-20.755 |
0.000 |
| z |
0.000 |
0.000 |
-24.969 |
|
| Traceless |
| | x | y | z |
| x |
-1.634 |
1.094 |
0.000 |
| y |
1.094 |
3.978 |
0.000 |
| z |
0.000 |
0.000 |
-2.344 |
|
| Polar |
| 3z2-r2 | -4.688 |
| x2-y2 | -3.741 |
| xy | 1.094 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.181 |
0.252 |
0.000 |
| y |
0.252 |
6.086 |
0.000 |
| z |
0.000 |
0.000 |
2.377 |
<r2> (average value of r
2) Å
2
| <r2> |
78.264 |
| (<r2>)1/2 |
8.847 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -215.855899 |
| Energy at 298.15K | |
| HF Energy | -215.855899 |
| Nuclear repulsion energy | 113.550312 |
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 B1B95/3-21G
| 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 |
3267 |
3125 |
10.85 |
55.48 |
0.52 |
0.69 |
| 2 |
A |
3211 |
3072 |
3.17 |
84.99 |
0.32 |
0.49 |
| 3 |
A |
3177 |
3040 |
5.50 |
64.67 |
0.11 |
0.19 |
| 4 |
A |
3107 |
2973 |
31.66 |
61.96 |
0.68 |
0.81 |
| 5 |
A |
3058 |
2925 |
32.57 |
114.04 |
0.14 |
0.24 |
| 6 |
A |
1745 |
1669 |
0.94 |
11.82 |
0.12 |
0.22 |
| 7 |
A |
1567 |
1499 |
1.53 |
14.21 |
0.69 |
0.82 |
| 8 |
A |
1510 |
1445 |
13.77 |
11.67 |
0.50 |
0.67 |
| 9 |
A |
1427 |
1366 |
14.17 |
6.85 |
0.75 |
0.86 |
| 10 |
A |
1351 |
1293 |
0.15 |
12.73 |
0.47 |
0.64 |
| 11 |
A |
1280 |
1224 |
2.54 |
18.93 |
0.73 |
0.84 |
| 12 |
A |
1191 |
1139 |
0.54 |
2.39 |
0.71 |
0.83 |
| 13 |
A |
1083 |
1036 |
49.94 |
4.83 |
0.56 |
0.72 |
| 14 |
A |
1063 |
1017 |
26.33 |
2.50 |
0.69 |
0.82 |
| 15 |
A |
1022 |
978 |
6.16 |
1.14 |
0.70 |
0.82 |
| 16 |
A |
994 |
951 |
65.39 |
0.31 |
0.42 |
0.59 |
| 17 |
A |
941 |
901 |
7.97 |
3.38 |
0.16 |
0.28 |
| 18 |
A |
639 |
612 |
11.85 |
9.48 |
0.73 |
0.84 |
| 19 |
A |
452 |
433 |
2.41 |
5.24 |
0.49 |
0.65 |
| 20 |
A |
296 |
283 |
5.99 |
3.60 |
0.75 |
0.86 |
| 21 |
A |
104 |
99 |
1.65 |
7.60 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 16241.9 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15538.6 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.585 |
0.479 |
0.234 |
| C2 |
0.639 |
-0.379 |
0.194 |
| C3 |
1.835 |
0.061 |
-0.171 |
| F4 |
-1.699 |
-0.248 |
-0.259 |
| H5 |
2.711 |
-0.573 |
-0.141 |
| H6 |
1.985 |
1.078 |
-0.518 |
| H7 |
0.495 |
-1.398 |
0.536 |
| H8 |
-0.800 |
0.772 |
1.268 |
| H9 |
-0.437 |
1.385 |
-0.359 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4951 | 2.4886 | 1.4182 | 3.4803 | 2.7441 | 2.1856 | 1.0955 | 1.0935 |
C2 | 1.4951 | | 1.3253 | 2.3848 | 2.1081 | 2.1075 | 1.0843 | 2.1328 | 2.1393 | C3 | 2.4886 | 1.3253 | | 3.5478 | 1.0824 | 1.0851 | 2.1034 | 3.0853 | 2.6363 | F4 | 1.4182 | 2.3848 | 3.5478 | | 4.4235 | 3.9233 | 2.6009 | 2.0439 | 2.0655 | H5 | 3.4803 | 2.1081 | 1.0824 | 4.4235 | | 1.8429 | 2.4603 | 4.0157 | 3.7143 | H6 | 2.7441 | 2.1075 | 1.0851 | 3.9233 | 1.8429 | | 3.0761 | 3.3229 | 2.4468 | H7 | 2.1856 | 1.0843 | 2.1034 | 2.6009 | 2.4603 | 3.0761 | | 2.6303 | 3.0681 | H8 | 1.0955 | 2.1328 | 3.0853 | 2.0439 | 4.0157 | 3.3229 | 2.6303 | | 1.7761 | H9 | 1.0935 | 2.1393 | 2.6363 | 2.0655 | 3.7143 | 2.4468 | 3.0681 | 1.7761 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.747 |
|
C1 |
C2 |
H7 |
114.913 |
| C2 |
C1 |
F4 |
109.862 |
|
C2 |
C1 |
H8 |
109.872 |
| C2 |
C1 |
H9 |
110.507 |
|
C2 |
C3 |
H5 |
121.903 |
| C2 |
C3 |
H6 |
121.617 |
|
C3 |
C2 |
H7 |
121.277 |
| F4 |
C1 |
H8 |
108.113 |
|
F4 |
C1 |
H9 |
109.973 |
| H5 |
C3 |
H6 |
116.480 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.125 |
|
|
|
| 2 |
C |
-0.246 |
|
|
|
| 3 |
C |
-0.403 |
|
|
|
| 4 |
F |
-0.310 |
|
|
|
| 5 |
H |
0.217 |
|
|
|
| 6 |
H |
0.206 |
|
|
|
| 7 |
H |
0.233 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
| 9 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.562 |
0.861 |
0.734 |
1.929 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.396 |
-1.105 |
-1.445 |
| y |
-1.105 |
-21.830 |
-0.896 |
| z |
-1.445 |
-0.896 |
-24.572 |
|
| Traceless |
| | x | y | z |
| x |
-2.195 |
-1.105 |
-1.445 |
| y |
-1.105 |
3.154 |
-0.896 |
| z |
-1.445 |
-0.896 |
-0.958 |
|
| Polar |
| 3z2-r2 | -1.917 |
| x2-y2 | -3.566 |
| xy | -1.105 |
| xz | -1.445 |
| yz | -0.896 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.926 |
0.223 |
-0.743 |
| y |
0.223 |
4.074 |
-0.514 |
| z |
-0.743 |
-0.514 |
2.694 |
<r2> (average value of r
2) Å
2
| <r2> |
90.399 |
| (<r2>)1/2 |
9.508 |