Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -217.082518 |
| Energy at 298.15K | |
| HF Energy | -216.815703 |
| Nuclear repulsion energy | 116.592600 |
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=FULLultrafine/aug-cc-pVTZ
| 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' |
3261 |
3128 |
3.79 |
49.88 |
0.71 |
0.83 |
| 2 |
A' |
3181 |
3051 |
3.77 |
170.05 |
0.09 |
0.17 |
| 3 |
A' |
3162 |
3033 |
9.27 |
38.27 |
0.56 |
0.72 |
| 4 |
A' |
3050 |
2925 |
32.17 |
180.47 |
0.09 |
0.16 |
| 5 |
A' |
1716 |
1646 |
5.48 |
33.16 |
0.04 |
0.07 |
| 6 |
A' |
1513 |
1451 |
3.70 |
11.77 |
0.52 |
0.69 |
| 7 |
A' |
1463 |
1403 |
5.90 |
8.98 |
0.34 |
0.51 |
| 8 |
A' |
1424 |
1366 |
11.08 |
2.35 |
0.71 |
0.83 |
| 9 |
A' |
1323 |
1269 |
0.22 |
19.79 |
0.21 |
0.34 |
| 10 |
A' |
1132 |
1085 |
49.65 |
1.48 |
0.63 |
0.77 |
| 11 |
A' |
1010 |
969 |
44.69 |
4.70 |
0.67 |
0.80 |
| 12 |
A' |
916 |
878 |
3.02 |
6.55 |
0.04 |
0.07 |
| 13 |
A' |
611 |
586 |
7.38 |
1.54 |
0.69 |
0.81 |
| 14 |
A' |
266 |
255 |
2.37 |
1.24 |
0.42 |
0.59 |
| 15 |
A" |
3085 |
2959 |
18.14 |
80.23 |
0.75 |
0.86 |
| 16 |
A" |
1276 |
1224 |
0.00 |
3.48 |
0.75 |
0.86 |
| 17 |
A" |
1058 |
1015 |
11.79 |
0.85 |
0.75 |
0.86 |
| 18 |
A" |
1030 |
988 |
9.08 |
0.20 |
0.75 |
0.86 |
| 19 |
A" |
968 |
928 |
43.15 |
2.43 |
0.75 |
0.86 |
| 20 |
A" |
568 |
545 |
11.36 |
1.18 |
0.75 |
0.86 |
| 21 |
A" |
178 |
170 |
3.16 |
0.86 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16095.2 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15436.9 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=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.942 |
-0.204 |
0.000 |
| C2 |
0.000 |
0.950 |
0.000 |
| C3 |
1.323 |
0.852 |
0.000 |
| F4 |
-0.266 |
-1.418 |
0.000 |
| H5 |
1.943 |
1.734 |
0.000 |
| H6 |
1.811 |
-0.109 |
0.000 |
| H7 |
-0.479 |
1.921 |
0.000 |
| H8 |
-1.581 |
-0.185 |
0.884 |
| H9 |
-1.581 |
-0.185 |
-0.884 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4895 | 2.4987 | 1.3898 | 3.4759 | 2.7549 | 2.1749 | 1.0912 | 1.0912 |
C2 | 1.4895 | | 1.3262 | 2.3834 | 2.0957 | 2.0984 | 1.0832 | 2.1379 | 2.1379 | C3 | 2.4987 | 1.3262 | | 2.7715 | 1.0786 | 1.0787 | 2.0953 | 3.2077 | 3.2077 | F4 | 1.3898 | 2.3834 | 2.7715 | | 3.8501 | 2.4559 | 3.3466 | 2.0075 | 2.0075 | H5 | 3.4759 | 2.0957 | 1.0786 | 3.8501 | | 1.8484 | 2.4300 | 4.1095 | 4.1095 | H6 | 2.7549 | 2.0984 | 1.0787 | 2.4559 | 1.8484 | | 3.0612 | 3.5065 | 3.5065 | H7 | 2.1749 | 1.0832 | 2.0953 | 3.3466 | 2.4300 | 3.0612 | | 2.5365 | 2.5365 | H8 | 1.0912 | 2.1379 | 3.2077 | 2.0075 | 4.1095 | 3.5065 | 2.5365 | | 1.7689 | H9 | 1.0912 | 2.1379 | 3.2077 | 2.0075 | 4.1095 | 3.5065 | 2.5365 | 1.7689 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
125.002 |
|
C1 |
C2 |
H7 |
114.502 |
| C2 |
C1 |
F4 |
111.691 |
|
C2 |
C1 |
H8 |
110.931 |
| C2 |
C1 |
H9 |
110.931 |
|
C2 |
C3 |
H5 |
120.911 |
| C2 |
C3 |
H6 |
121.171 |
|
C3 |
C2 |
H7 |
120.496 |
| F4 |
C1 |
H8 |
107.414 |
|
F4 |
C1 |
H9 |
107.414 |
| H5 |
C3 |
H6 |
117.918 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.064 |
|
|
|
| 2 |
C |
-0.222 |
|
|
|
| 3 |
C |
-0.958 |
|
|
|
| 4 |
F |
-0.425 |
|
|
|
| 5 |
H |
0.454 |
|
|
|
| 6 |
H |
0.202 |
|
|
|
| 7 |
H |
0.303 |
|
|
|
| 8 |
H |
0.291 |
|
|
|
| 9 |
H |
0.291 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.916 |
1.550 |
0.000 |
1.800 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.493 |
-0.299 |
-0.000 |
| y |
-0.299 |
-25.904 |
-0.011 |
| z |
-0.000 |
-0.011 |
-25.489 |
|
| Traceless |
| | x | y | z |
| x |
4.204 |
-0.299 |
-0.000 |
| y |
-0.299 |
-2.413 |
-0.011 |
| z |
-0.000 |
-0.011 |
-1.791 |
|
| Polar |
| 3z2-r2 | -3.581 |
| x2-y2 | 4.411 |
| xy | -0.299 |
| xz | -0.000 |
| yz | -0.011 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.410 |
0.326 |
0.001 |
| y |
0.326 |
5.707 |
0.001 |
| z |
0.001 |
0.001 |
4.747 |
<r2> (average value of r
2) Å
2
| <r2> |
80.394 |
| (<r2>)1/2 |
8.966 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -217.082466 |
| Energy at 298.15K | |
| HF Energy | -216.815573 |
| Nuclear repulsion energy | 114.343443 |
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=FULLultrafine/aug-cc-pVTZ
| 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 |
3244 |
3112 |
9.04 |
59.94 |
0.56 |
0.72 |
| 2 |
A |
3179 |
3049 |
4.14 |
127.29 |
0.20 |
0.33 |
| 3 |
A |
3159 |
3030 |
8.58 |
68.70 |
0.09 |
0.17 |
| 4 |
A |
3115 |
2988 |
16.97 |
61.91 |
0.72 |
0.84 |
| 5 |
A |
3064 |
2939 |
29.25 |
134.85 |
0.07 |
0.13 |
| 6 |
A |
1711 |
1641 |
0.51 |
34.90 |
0.06 |
0.11 |
| 7 |
A |
1523 |
1460 |
3.67 |
3.41 |
0.67 |
0.80 |
| 8 |
A |
1474 |
1414 |
15.83 |
10.20 |
0.45 |
0.62 |
| 9 |
A |
1399 |
1342 |
12.92 |
3.57 |
0.21 |
0.34 |
| 10 |
A |
1324 |
1270 |
0.06 |
15.30 |
0.27 |
0.43 |
| 11 |
A |
1276 |
1224 |
4.53 |
6.91 |
0.65 |
0.79 |
| 12 |
A |
1191 |
1142 |
2.92 |
1.06 |
0.55 |
0.71 |
| 13 |
A |
1038 |
995 |
7.59 |
0.45 |
0.73 |
0.85 |
| 14 |
A |
1027 |
985 |
141.23 |
7.57 |
0.58 |
0.74 |
| 15 |
A |
996 |
956 |
3.12 |
2.26 |
0.08 |
0.15 |
| 16 |
A |
978 |
938 |
51.30 |
2.05 |
0.59 |
0.74 |
| 17 |
A |
936 |
897 |
4.14 |
4.10 |
0.11 |
0.20 |
| 18 |
A |
664 |
637 |
7.21 |
1.61 |
0.24 |
0.39 |
| 19 |
A |
436 |
418 |
2.27 |
3.47 |
0.29 |
0.46 |
| 20 |
A |
336 |
323 |
7.76 |
1.14 |
0.74 |
0.85 |
| 21 |
A |
117 |
112 |
1.06 |
2.48 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16092.9 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15434.7 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.603 |
0.428 |
0.330 |
| C2 |
0.646 |
-0.377 |
0.256 |
| C3 |
1.791 |
0.093 |
-0.223 |
| F4 |
-1.636 |
-0.225 |
-0.355 |
| H5 |
2.688 |
-0.508 |
-0.236 |
| H6 |
1.866 |
1.099 |
-0.612 |
| H7 |
0.583 |
-1.388 |
0.635 |
| H8 |
-0.942 |
0.548 |
1.359 |
| H9 |
-0.473 |
1.408 |
-0.125 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4873 | 2.4800 | 1.4014 | 3.4675 | 2.7269 | 2.1905 | 1.0899 | 1.0885 |
C2 | 1.4873 | | 1.3276 | 2.3669 | 2.1044 | 2.1027 | 1.0821 | 2.1429 | 2.1406 | C3 | 2.4800 | 1.3276 | | 3.4447 | 1.0792 | 1.0811 | 2.0955 | 3.1904 | 2.6202 | F4 | 1.4014 | 2.3669 | 3.4447 | | 4.3346 | 3.7533 | 2.6938 | 2.0047 | 2.0187 | H5 | 3.4675 | 2.1044 | 1.0792 | 4.3346 | | 1.8432 | 2.4420 | 4.1023 | 3.6976 | H6 | 2.7269 | 2.1027 | 1.0811 | 3.7533 | 1.8432 | | 3.0641 | 3.4749 | 2.4094 | H7 | 2.1905 | 1.0821 | 2.0955 | 2.6938 | 2.4420 | 3.0641 | | 2.5686 | 3.0843 | H8 | 1.0899 | 2.1429 | 3.1904 | 2.0047 | 4.1023 | 3.4749 | 2.5686 | | 1.7782 | H9 | 1.0885 | 2.1406 | 2.6202 | 2.0187 | 3.6976 | 2.4094 | 3.0843 | 1.7782 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.436 |
|
C1 |
C2 |
H7 |
116.081 |
| C2 |
C1 |
F4 |
110.006 |
|
C2 |
C1 |
H8 |
111.574 |
| C2 |
C1 |
H9 |
111.470 |
|
C2 |
C3 |
H5 |
121.597 |
| C2 |
C3 |
H6 |
121.266 |
|
C3 |
C2 |
H7 |
120.476 |
| F4 |
C1 |
H8 |
106.490 |
|
F4 |
C1 |
H9 |
107.676 |
| H5 |
C3 |
H6 |
117.136 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.016 |
|
|
|
| 2 |
C |
-0.211 |
|
|
|
| 3 |
C |
-0.928 |
|
|
|
| 4 |
F |
-0.433 |
|
|
|
| 5 |
H |
0.427 |
|
|
|
| 6 |
H |
0.257 |
|
|
|
| 7 |
H |
0.357 |
|
|
|
| 8 |
H |
0.273 |
|
|
|
| 9 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.588 |
0.768 |
0.900 |
1.980 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.178 |
-1.218 |
-2.095 |
| y |
-1.218 |
-22.881 |
-1.042 |
| z |
-2.095 |
-1.042 |
-25.101 |
|
| Traceless |
| | x | y | z |
| x |
-2.187 |
-1.218 |
-2.095 |
| y |
-1.218 |
2.758 |
-1.042 |
| z |
-2.095 |
-1.042 |
-0.572 |
|
| Polar |
| 3z2-r2 | -1.143 |
| x2-y2 | -3.296 |
| xy | -1.218 |
| xz | -2.095 |
| yz | -1.042 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.445 |
0.237 |
-0.594 |
| y |
0.237 |
5.484 |
-0.207 |
| z |
-0.594 |
-0.207 |
5.087 |
<r2> (average value of r
2) Å
2
| <r2> |
88.935 |
| (<r2>)1/2 |
9.431 |