Jump to
S1C2
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -213.931127 |
| Energy at 298.15K | |
| HF Energy | -213.865125 |
| Nuclear repulsion energy | 114.473808 |
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/STO-3G
| 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' |
3592 |
3592 |
0.12 |
31.38 |
0.71 |
0.83 |
| 2 |
A' |
3488 |
3488 |
1.79 |
53.62 |
0.27 |
0.43 |
| 3 |
A' |
3435 |
3435 |
13.97 |
27.30 |
0.15 |
0.26 |
| 4 |
A' |
3268 |
3268 |
10.93 |
57.31 |
0.12 |
0.22 |
| 5 |
A' |
1849 |
1849 |
0.85 |
3.82 |
0.19 |
0.31 |
| 6 |
A' |
1683 |
1683 |
0.52 |
18.40 |
0.73 |
0.84 |
| 7 |
A' |
1567 |
1567 |
0.57 |
9.44 |
0.60 |
0.75 |
| 8 |
A' |
1527 |
1527 |
22.22 |
6.58 |
0.60 |
0.75 |
| 9 |
A' |
1407 |
1407 |
1.78 |
16.44 |
0.56 |
0.72 |
| 10 |
A' |
1252 |
1252 |
7.74 |
2.57 |
0.74 |
0.85 |
| 11 |
A' |
1094 |
1094 |
4.45 |
4.94 |
0.73 |
0.84 |
| 12 |
A' |
958 |
958 |
1.82 |
5.80 |
0.24 |
0.39 |
| 13 |
A' |
611 |
611 |
1.01 |
1.55 |
0.75 |
0.85 |
| 14 |
A' |
235 |
235 |
0.58 |
0.76 |
0.52 |
0.69 |
| 15 |
A" |
3359 |
3359 |
10.40 |
45.83 |
0.75 |
0.86 |
| 16 |
A" |
1336 |
1336 |
1.32 |
9.08 |
0.75 |
0.86 |
| 17 |
A" |
1118 |
1118 |
7.83 |
0.13 |
0.75 |
0.86 |
| 18 |
A" |
1101 |
1101 |
1.41 |
0.43 |
0.75 |
0.86 |
| 19 |
A" |
1006 |
1006 |
16.92 |
0.09 |
0.75 |
0.86 |
| 20 |
A" |
584 |
584 |
4.11 |
6.56 |
0.75 |
0.86 |
| 21 |
A" |
132 |
132 |
0.78 |
2.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17300.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17300.4 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
-0.985 |
0.000 |
| C2 |
-0.962 |
0.229 |
0.000 |
| C3 |
-0.534 |
1.496 |
0.000 |
| F4 |
1.347 |
-0.585 |
0.000 |
| H5 |
-1.225 |
2.345 |
0.000 |
| H6 |
0.538 |
1.725 |
0.000 |
| H7 |
-2.033 |
-0.015 |
0.000 |
| H8 |
-0.213 |
-1.618 |
0.897 |
| H9 |
-0.213 |
-1.618 |
-0.897 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5493 | 2.5376 | 1.4053 | 3.5480 | 2.7631 | 2.2526 | 1.1181 | 1.1181 |
C2 | 1.5493 | | 1.3367 | 2.4484 | 2.1316 | 2.1183 | 1.0987 | 2.1858 | 2.1858 | C3 | 2.5376 | 1.3367 | | 2.8046 | 1.0949 | 1.0960 | 2.1286 | 3.2560 | 3.2560 | F4 | 1.4053 | 2.4484 | 2.8046 | | 3.8984 | 2.4475 | 3.4278 | 2.0750 | 2.0750 | H5 | 3.5480 | 2.1316 | 1.0949 | 3.8984 | | 1.8688 | 2.4944 | 4.1870 | 4.1870 | H6 | 2.7631 | 2.1183 | 1.0960 | 2.4475 | 1.8688 | | 3.1048 | 3.5418 | 3.5418 | H7 | 2.2526 | 1.0987 | 2.1286 | 3.4278 | 2.4944 | 3.1048 | | 2.5856 | 2.5856 | H8 | 1.1181 | 2.1858 | 3.2560 | 2.0750 | 4.1870 | 3.5418 | 2.5856 | | 1.7935 | H9 | 1.1181 | 2.1858 | 3.2560 | 2.0750 | 4.1870 | 3.5418 | 2.5856 | 1.7935 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
122.933 |
|
C1 |
C2 |
H7 |
115.517 |
| C2 |
C1 |
F4 |
111.830 |
|
C2 |
C1 |
H8 |
108.988 |
| C2 |
C1 |
H9 |
108.988 |
|
C2 |
C3 |
H5 |
122.158 |
| C2 |
C3 |
H6 |
120.770 |
|
C3 |
C2 |
H7 |
121.550 |
| F4 |
C1 |
H8 |
110.117 |
|
F4 |
C1 |
H9 |
110.117 |
| H5 |
C3 |
H6 |
117.072 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.015 |
|
|
|
| 2 |
C |
-0.077 |
|
|
|
| 3 |
C |
-0.150 |
|
|
|
| 4 |
F |
-0.111 |
|
|
|
| 5 |
H |
0.072 |
|
|
|
| 6 |
H |
0.076 |
|
|
|
| 7 |
H |
0.070 |
|
|
|
| 8 |
H |
0.067 |
|
|
|
| 9 |
H |
0.067 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.888 |
-0.353 |
0.000 |
0.956 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.378 |
0.656 |
0.002 |
| y |
0.656 |
-20.649 |
0.006 |
| z |
0.002 |
0.006 |
-22.570 |
|
| Traceless |
| | x | y | z |
| x |
-0.768 |
0.656 |
0.002 |
| y |
0.656 |
1.825 |
0.006 |
| z |
0.002 |
0.006 |
-1.057 |
|
| Polar |
| 3z2-r2 | -2.114 |
| x2-y2 | -1.729 |
| xy | 0.656 |
| xz | 0.002 |
| yz | 0.006 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.699 |
0.208 |
-0.000 |
| y |
0.208 |
3.781 |
-0.000 |
| z |
-0.000 |
-0.000 |
1.212 |
<r2> (average value of r
2) Å
2
| <r2> |
81.220 |
| (<r2>)1/2 |
9.012 |
Jump to
S1C1
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -213.930446 |
| Energy at 298.15K | |
| HF Energy | -213.864426 |
| Nuclear repulsion energy | 112.047619 |
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/STO-3G
| 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 |
3585 |
3585 |
0.04 |
33.42 |
0.71 |
0.83 |
| 2 |
A |
3488 |
3488 |
2.24 |
48.58 |
0.27 |
0.43 |
| 3 |
A |
3431 |
3431 |
12.28 |
30.37 |
0.14 |
0.24 |
| 4 |
A |
3381 |
3381 |
9.28 |
32.54 |
0.75 |
0.86 |
| 5 |
A |
3276 |
3276 |
11.69 |
44.12 |
0.15 |
0.26 |
| 6 |
A |
1843 |
1843 |
0.31 |
5.14 |
0.19 |
0.33 |
| 7 |
A |
1677 |
1677 |
0.30 |
12.94 |
0.75 |
0.86 |
| 8 |
A |
1594 |
1594 |
4.56 |
10.13 |
0.49 |
0.66 |
| 9 |
A |
1507 |
1507 |
21.98 |
5.22 |
0.73 |
0.85 |
| 10 |
A |
1413 |
1413 |
3.42 |
14.30 |
0.57 |
0.73 |
| 11 |
A |
1352 |
1352 |
3.87 |
15.32 |
0.75 |
0.85 |
| 12 |
A |
1233 |
1233 |
1.11 |
2.83 |
0.54 |
0.70 |
| 13 |
A |
1218 |
1218 |
11.79 |
4.27 |
0.63 |
0.77 |
| 14 |
A |
1118 |
1118 |
7.83 |
0.30 |
0.73 |
0.85 |
| 15 |
A |
1030 |
1030 |
1.00 |
0.91 |
0.33 |
0.50 |
| 16 |
A |
1012 |
1012 |
15.95 |
0.15 |
0.47 |
0.64 |
| 17 |
A |
980 |
980 |
4.00 |
3.17 |
0.23 |
0.37 |
| 18 |
A |
684 |
684 |
4.06 |
4.33 |
0.62 |
0.76 |
| 19 |
A |
427 |
427 |
0.27 |
2.35 |
0.51 |
0.68 |
| 20 |
A |
340 |
340 |
1.97 |
3.18 |
0.75 |
0.86 |
| 21 |
A |
88 |
88 |
0.28 |
3.35 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17337.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17337.2 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/STO-3G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.637 |
0.416 |
0.343 |
| C2 |
0.682 |
-0.389 |
0.263 |
| C3 |
1.823 |
0.105 |
-0.234 |
| F4 |
-1.675 |
-0.219 |
-0.371 |
| H5 |
2.744 |
-0.488 |
-0.270 |
| H6 |
1.887 |
1.129 |
-0.619 |
| H7 |
0.637 |
-1.420 |
0.641 |
| H8 |
-0.938 |
0.523 |
1.414 |
| H9 |
-0.464 |
1.441 |
-0.061 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5478 | 2.5457 | 1.4104 | 3.5529 | 2.7940 | 2.2545 | 1.1179 | 1.1153 |
C2 | 1.5478 | | 1.3385 | 2.4467 | 2.1316 | 2.1297 | 1.0990 | 2.1871 | 2.1838 | C3 | 2.5457 | 1.3385 | | 3.5154 | 1.0958 | 1.0963 | 2.1207 | 3.2421 | 2.6543 | F4 | 1.4104 | 2.4467 | 3.5154 | | 4.4280 | 3.8169 | 2.7948 | 2.0691 | 2.0776 | H5 | 3.5529 | 2.1316 | 1.0958 | 4.4280 | | 1.8628 | 2.4777 | 4.1729 | 3.7490 | H6 | 2.7940 | 2.1297 | 1.0963 | 3.8169 | 1.8628 | | 3.1065 | 3.5327 | 2.4367 | H7 | 2.2545 | 1.0990 | 2.1207 | 2.7948 | 2.4777 | 3.1065 | | 2.6180 | 3.1450 | H8 | 1.1179 | 2.1871 | 3.2421 | 2.0691 | 4.1729 | 3.5327 | 2.6180 | | 1.8010 | H9 | 1.1153 | 2.1838 | 2.6543 | 2.0776 | 3.7490 | 2.4367 | 3.1450 | 1.8010 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.609 |
|
C1 |
C2 |
H7 |
115.782 |
| C2 |
C1 |
F4 |
111.516 |
|
C2 |
C1 |
H8 |
109.199 |
| C2 |
C1 |
H9 |
109.101 |
|
C2 |
C3 |
H5 |
121.929 |
| C2 |
C3 |
H6 |
121.692 |
|
C3 |
C2 |
H7 |
120.608 |
| F4 |
C1 |
H8 |
109.295 |
|
F4 |
C1 |
H9 |
110.138 |
| H5 |
C3 |
H6 |
116.378 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.017 |
|
|
|
| 2 |
C |
-0.075 |
|
|
|
| 3 |
C |
-0.144 |
|
|
|
| 4 |
F |
-0.111 |
|
|
|
| 5 |
H |
0.074 |
|
|
|
| 6 |
H |
0.070 |
|
|
|
| 7 |
H |
0.072 |
|
|
|
| 8 |
H |
0.066 |
|
|
|
| 9 |
H |
0.066 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.709 |
0.398 |
0.503 |
0.956 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.934 |
-0.568 |
-1.029 |
| y |
-0.568 |
-21.050 |
-0.530 |
| z |
-1.029 |
-0.530 |
-22.340 |
|
| Traceless |
| | x | y | z |
| x |
-1.239 |
-0.568 |
-1.029 |
| y |
-0.568 |
1.587 |
-0.530 |
| z |
-1.029 |
-0.530 |
-0.348 |
|
| Polar |
| 3z2-r2 | -0.696 |
| x2-y2 | -1.884 |
| xy | -0.568 |
| xz | -1.029 |
| yz | -0.530 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.742 |
0.244 |
-0.579 |
| y |
0.244 |
2.400 |
-0.390 |
| z |
-0.579 |
-0.390 |
1.637 |
<r2> (average value of r
2) Å
2
| <r2> |
90.690 |
| (<r2>)1/2 |
9.523 |