Jump to
S1C2
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -217.128252 |
| Energy at 298.15K | |
| HF Energy | -217.128252 |
| Nuclear repulsion energy | 116.979812 |
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/TZVP
| 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' |
3272 |
3131 |
3.92 |
52.61 |
0.71 |
0.83 |
| 2 |
A' |
3184 |
3047 |
4.20 |
174.03 |
0.14 |
0.24 |
| 3 |
A' |
3171 |
3035 |
8.48 |
27.64 |
0.72 |
0.84 |
| 4 |
A' |
3047 |
2916 |
33.43 |
185.45 |
0.11 |
0.20 |
| 5 |
A' |
1741 |
1666 |
5.25 |
29.37 |
0.09 |
0.16 |
| 6 |
A' |
1499 |
1434 |
6.39 |
13.87 |
0.61 |
0.76 |
| 7 |
A' |
1451 |
1388 |
6.39 |
11.89 |
0.46 |
0.63 |
| 8 |
A' |
1419 |
1358 |
12.16 |
9.12 |
0.72 |
0.84 |
| 9 |
A' |
1322 |
1265 |
0.20 |
17.55 |
0.28 |
0.44 |
| 10 |
A' |
1146 |
1096 |
57.27 |
2.09 |
0.75 |
0.85 |
| 11 |
A' |
1020 |
976 |
42.48 |
5.20 |
0.71 |
0.83 |
| 12 |
A' |
922 |
882 |
1.75 |
4.11 |
0.08 |
0.15 |
| 13 |
A' |
618 |
591 |
6.32 |
1.89 |
0.74 |
0.85 |
| 14 |
A' |
264 |
253 |
2.41 |
1.30 |
0.55 |
0.71 |
| 15 |
A" |
3085 |
2952 |
24.15 |
91.68 |
0.75 |
0.86 |
| 16 |
A" |
1272 |
1217 |
0.05 |
8.87 |
0.75 |
0.86 |
| 17 |
A" |
1048 |
1003 |
14.88 |
1.30 |
0.75 |
0.86 |
| 18 |
A" |
1025 |
981 |
8.01 |
0.03 |
0.75 |
0.86 |
| 19 |
A" |
966 |
925 |
52.04 |
1.12 |
0.75 |
0.86 |
| 20 |
A" |
563 |
539 |
11.86 |
5.07 |
0.75 |
0.86 |
| 21 |
A" |
176 |
168 |
3.46 |
2.41 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16104.6 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 15410.5 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 B1B95/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.937 |
-0.206 |
0.000 |
| C2 |
0.000 |
0.948 |
0.000 |
| C3 |
1.317 |
0.847 |
0.000 |
| F4 |
-0.265 |
-1.411 |
0.000 |
| H5 |
1.945 |
1.726 |
0.000 |
| H6 |
1.802 |
-0.119 |
0.000 |
| H7 |
-0.482 |
1.920 |
0.000 |
| H8 |
-1.580 |
-0.181 |
0.884 |
| H9 |
-1.580 |
-0.181 |
-0.884 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4865 | 2.4881 | 1.3800 | 3.4696 | 2.7411 | 2.1741 | 1.0931 | 1.0931 |
C2 | 1.4865 | | 1.3212 | 2.3740 | 2.0946 | 2.0947 | 1.0848 | 2.1334 | 2.1334 | C3 | 2.4881 | 1.3212 | | 2.7571 | 1.0802 | 1.0807 | 2.0949 | 3.1984 | 3.1984 | F4 | 1.3800 | 2.3740 | 2.7571 | | 3.8373 | 2.4381 | 3.3382 | 2.0057 | 2.0057 | H5 | 3.4696 | 2.0946 | 1.0802 | 3.8373 | | 1.8504 | 2.4343 | 4.1036 | 4.1036 | H6 | 2.7411 | 2.0947 | 1.0807 | 2.4381 | 1.8504 | | 3.0619 | 3.4963 | 3.4963 | H7 | 2.1741 | 1.0848 | 2.0949 | 3.3382 | 2.4343 | 3.0619 | | 2.5301 | 2.5301 | H8 | 1.0931 | 2.1334 | 3.1984 | 2.0057 | 4.1036 | 3.4963 | 2.5301 | | 1.7682 | H9 | 1.0931 | 2.1334 | 3.1984 | 2.0057 | 4.1036 | 3.4963 | 2.5301 | 1.7682 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
124.685 |
|
C1 |
C2 |
H7 |
114.553 |
| C2 |
C1 |
F4 |
111.768 |
|
C2 |
C1 |
H8 |
110.663 |
| C2 |
C1 |
H9 |
110.663 |
|
C2 |
C3 |
H5 |
121.112 |
| C2 |
C3 |
H6 |
121.079 |
|
C3 |
C2 |
H7 |
120.763 |
| F4 |
C1 |
H8 |
107.821 |
|
F4 |
C1 |
H9 |
107.821 |
| H5 |
C3 |
H6 |
117.808 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.010 |
|
|
|
| 2 |
C |
-0.133 |
|
|
|
| 3 |
C |
-0.262 |
|
|
|
| 4 |
F |
-0.244 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
0.142 |
|
|
|
| 7 |
H |
0.135 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
| 9 |
H |
0.116 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.938 |
1.595 |
0.000 |
1.851 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.104 |
-0.301 |
0.000 |
| y |
-0.301 |
-25.465 |
0.000 |
| z |
0.000 |
0.000 |
-25.216 |
|
| Traceless |
| | x | y | z |
| x |
4.237 |
-0.301 |
0.000 |
| y |
-0.301 |
-2.304 |
0.000 |
| z |
0.000 |
0.000 |
-1.932 |
|
| Polar |
| 3z2-r2 | -3.865 |
| x2-y2 | 4.361 |
| xy | -0.301 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.129 |
0.269 |
0.000 |
| y |
0.269 |
4.955 |
0.000 |
| z |
0.000 |
0.000 |
3.886 |
<r2> (average value of r
2) Å
2
| <r2> |
79.690 |
| (<r2>)1/2 |
8.927 |
Jump to
S1C1
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -217.127623 |
| Energy at 298.15K | |
| HF Energy | -217.127623 |
| Nuclear repulsion energy | 114.631404 |
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/TZVP
| 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 |
3254 |
3114 |
10.12 |
62.25 |
0.59 |
0.74 |
| 2 |
A |
3185 |
3048 |
6.10 |
114.37 |
0.24 |
0.39 |
| 3 |
A |
3162 |
3026 |
8.13 |
77.85 |
0.13 |
0.23 |
| 4 |
A |
3116 |
2982 |
22.40 |
71.85 |
0.71 |
0.83 |
| 5 |
A |
3060 |
2928 |
32.62 |
137.77 |
0.09 |
0.16 |
| 6 |
A |
1739 |
1664 |
0.46 |
29.75 |
0.10 |
0.18 |
| 7 |
A |
1504 |
1439 |
3.07 |
6.31 |
0.66 |
0.79 |
| 8 |
A |
1466 |
1402 |
21.88 |
9.80 |
0.56 |
0.72 |
| 9 |
A |
1401 |
1340 |
13.64 |
5.42 |
0.48 |
0.65 |
| 10 |
A |
1321 |
1264 |
0.08 |
13.87 |
0.36 |
0.53 |
| 11 |
A |
1277 |
1222 |
3.57 |
11.67 |
0.69 |
0.81 |
| 12 |
A |
1187 |
1136 |
2.49 |
1.29 |
0.72 |
0.84 |
| 13 |
A |
1061 |
1015 |
127.95 |
5.60 |
0.57 |
0.72 |
| 14 |
A |
1040 |
995 |
27.71 |
1.75 |
0.69 |
0.81 |
| 15 |
A |
993 |
950 |
2.56 |
1.56 |
0.12 |
0.22 |
| 16 |
A |
979 |
937 |
58.37 |
0.94 |
0.46 |
0.63 |
| 17 |
A |
933 |
893 |
3.01 |
2.29 |
0.14 |
0.25 |
| 18 |
A |
664 |
635 |
7.76 |
3.01 |
0.60 |
0.75 |
| 19 |
A |
435 |
416 |
2.59 |
3.99 |
0.48 |
0.65 |
| 20 |
A |
330 |
315 |
6.90 |
2.31 |
0.75 |
0.86 |
| 21 |
A |
116 |
111 |
1.11 |
4.37 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16110.7 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 15416.4 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 B1B95/TZVP
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.602 |
0.425 |
0.318 |
| C2 |
0.644 |
-0.379 |
0.242 |
| C3 |
1.792 |
0.093 |
-0.214 |
| F4 |
-1.639 |
-0.222 |
-0.343 |
| H5 |
2.690 |
-0.509 |
-0.225 |
| H6 |
1.878 |
1.105 |
-0.590 |
| H7 |
0.571 |
-1.397 |
0.607 |
| H8 |
-0.921 |
0.557 |
1.354 |
| H9 |
-0.467 |
1.405 |
-0.140 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4853 | 2.4750 | 1.3899 | 3.4647 | 2.7268 | 2.1871 | 1.0921 | 1.0902 |
C2 | 1.4853 | | 1.3223 | 2.3624 | 2.1022 | 2.1014 | 1.0840 | 2.1364 | 2.1365 | C3 | 2.4750 | 1.3223 | | 3.4480 | 1.0808 | 1.0830 | 2.0937 | 3.1682 | 2.6135 | F4 | 1.3899 | 2.3624 | 3.4480 | | 4.3400 | 3.7669 | 2.6782 | 2.0008 | 2.0156 | H5 | 3.4647 | 2.1022 | 1.0808 | 4.3400 | | 1.8431 | 2.4428 | 4.0830 | 3.6926 | H6 | 2.7268 | 2.1014 | 1.0830 | 3.7669 | 1.8431 | | 3.0658 | 3.4518 | 2.4061 | H7 | 2.1871 | 1.0840 | 2.0937 | 2.6782 | 2.4428 | 3.0658 | | 2.5706 | 3.0808 | H8 | 1.0921 | 2.1364 | 3.1682 | 2.0008 | 4.0830 | 3.4518 | 2.5706 | | 1.7775 | H9 | 1.0902 | 2.1365 | 2.6135 | 2.0156 | 3.6926 | 2.4061 | 3.0808 | 1.7775 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
123.555 |
|
C1 |
C2 |
H7 |
115.813 |
| C2 |
C1 |
F4 |
110.455 |
|
C2 |
C1 |
H8 |
111.056 |
| C2 |
C1 |
H9 |
111.174 |
|
C2 |
C3 |
H5 |
121.722 |
| C2 |
C3 |
H6 |
121.463 |
|
C3 |
C2 |
H7 |
120.622 |
| F4 |
C1 |
H8 |
106.825 |
|
F4 |
C1 |
H9 |
108.110 |
| H5 |
C3 |
H6 |
116.815 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.018 |
|
|
|
| 2 |
C |
-0.083 |
|
|
|
| 3 |
C |
-0.277 |
|
|
|
| 4 |
F |
-0.242 |
|
|
|
| 5 |
H |
0.124 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.148 |
|
|
|
| 8 |
H |
0.110 |
|
|
|
| 9 |
H |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.601 |
0.783 |
0.911 |
2.002 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.868 |
-1.223 |
-2.011 |
| y |
-1.223 |
-22.424 |
-1.026 |
| z |
-2.011 |
-1.026 |
-24.835 |
|
| Traceless |
| | x | y | z |
| x |
-2.238 |
-1.223 |
-2.011 |
| y |
-1.223 |
2.927 |
-1.026 |
| z |
-2.011 |
-1.026 |
-0.689 |
|
| Polar |
| 3z2-r2 | -1.378 |
| x2-y2 | -3.444 |
| xy | -1.223 |
| xz | -2.011 |
| yz | -1.026 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.912 |
0.290 |
-0.771 |
| y |
0.290 |
4.905 |
-0.381 |
| z |
-0.771 |
-0.381 |
4.243 |
<r2> (average value of r
2) Å
2
| <r2> |
88.568 |
| (<r2>)1/2 |
9.411 |