Jump to
S1C2
Energy calculated at PBE1PBE/daug-cc-pVDZ
| hartrees |
Energy at 0K | -216.922986 |
Energy at 298.15K | |
HF Energy | -216.922986 |
Nuclear repulsion energy | 116.245022 |
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 PBE1PBE/daug-cc-pVDZ
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' |
3277 |
3277 |
3.87 |
54.04 |
0.70 |
0.83 |
2 |
A' |
3183 |
3183 |
4.67 |
185.74 |
0.12 |
0.21 |
3 |
A' |
3170 |
3170 |
7.54 |
24.67 |
0.63 |
0.77 |
4 |
A' |
3041 |
3041 |
33.58 |
197.76 |
0.09 |
0.16 |
5 |
A' |
1736 |
1736 |
6.26 |
46.03 |
0.05 |
0.10 |
6 |
A' |
1463 |
1463 |
5.64 |
12.97 |
0.50 |
0.67 |
7 |
A' |
1433 |
1433 |
8.57 |
8.54 |
0.40 |
0.57 |
8 |
A' |
1390 |
1390 |
8.73 |
3.14 |
0.62 |
0.76 |
9 |
A' |
1305 |
1305 |
0.21 |
20.03 |
0.22 |
0.36 |
10 |
A' |
1137 |
1137 |
63.24 |
1.60 |
0.74 |
0.85 |
11 |
A' |
1006 |
1006 |
34.07 |
4.43 |
0.65 |
0.79 |
12 |
A' |
924 |
924 |
2.59 |
5.93 |
0.03 |
0.07 |
13 |
A' |
607 |
607 |
6.61 |
1.54 |
0.66 |
0.80 |
14 |
A' |
257 |
257 |
2.15 |
1.34 |
0.41 |
0.59 |
15 |
A" |
3086 |
3086 |
18.29 |
88.30 |
0.75 |
0.86 |
16 |
A" |
1250 |
1250 |
0.00 |
3.72 |
0.75 |
0.86 |
17 |
A" |
1036 |
1036 |
12.11 |
1.30 |
0.75 |
0.86 |
18 |
A" |
1011 |
1011 |
4.98 |
0.10 |
0.75 |
0.86 |
19 |
A" |
971 |
971 |
49.77 |
1.96 |
0.75 |
0.86 |
20 |
A" |
561 |
561 |
11.83 |
1.23 |
0.75 |
0.86 |
21 |
A" |
178 |
178 |
3.15 |
0.94 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16010.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16010.2 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 PBE1PBE/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.942 |
-0.205 |
0.000 |
C2 |
0.000 |
0.949 |
0.000 |
C3 |
1.329 |
0.853 |
0.000 |
F4 |
-0.270 |
-1.419 |
0.000 |
H5 |
1.955 |
1.744 |
0.000 |
H6 |
1.824 |
-0.117 |
0.000 |
H7 |
-0.486 |
1.929 |
0.000 |
H8 |
-1.589 |
-0.184 |
0.892 |
H9 |
-1.589 |
-0.184 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4900 | 2.5052 | 1.3880 | 3.4917 | 2.7675 | 2.1821 | 1.1019 | 1.1019 |
C2 | 1.4900 | | 1.3321 | 2.3842 | 2.1103 | 2.1129 | 1.0937 | 2.1463 | 2.1463 | C3 | 2.5052 | 1.3321 | | 2.7788 | 1.0890 | 1.0894 | 2.1099 | 3.2228 | 3.2228 | F4 | 1.3880 | 2.3842 | 2.7788 | | 3.8677 | 2.4662 | 3.3554 | 2.0150 | 2.0150 | H5 | 3.4917 | 2.1103 | 1.0890 | 3.8677 | | 1.8657 | 2.4483 | 4.1323 | 4.1323 | H6 | 2.7675 | 2.1129 | 1.0894 | 2.4662 | 1.8657 | | 3.0861 | 3.5285 | 3.5285 | H7 | 2.1821 | 1.0937 | 2.1099 | 3.3554 | 2.4483 | 3.0861 | | 2.5452 | 2.5452 | H8 | 1.1019 | 2.1463 | 3.2228 | 2.0150 | 4.1323 | 3.5285 | 2.5452 | | 1.7832 | H9 | 1.1019 | 2.1463 | 3.2228 | 2.0150 | 4.1323 | 3.5285 | 2.5452 | 1.7832 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
125.081 |
|
C1 |
C2 |
H7 |
114.376 |
C2 |
C1 |
F4 |
111.827 |
|
C2 |
C1 |
H8 |
110.914 |
C2 |
C1 |
H9 |
110.914 |
|
C2 |
C3 |
H5 |
120.972 |
C2 |
C3 |
H6 |
121.184 |
|
C3 |
C2 |
H7 |
120.543 |
F4 |
C1 |
H8 |
107.494 |
|
F4 |
C1 |
H9 |
107.494 |
H5 |
C3 |
H6 |
117.844 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/daug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.688 |
|
|
|
2 |
C |
1.881 |
|
|
|
3 |
C |
0.740 |
|
|
|
4 |
F |
-0.740 |
|
|
|
5 |
H |
-0.881 |
|
|
|
6 |
H |
-0.619 |
|
|
|
7 |
H |
-0.877 |
|
|
|
8 |
H |
-0.095 |
|
|
|
9 |
H |
-0.095 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.914 |
1.507 |
0.000 |
1.762 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.313 |
-0.320 |
0.000 |
y |
-0.320 |
-25.587 |
0.000 |
z |
0.000 |
0.000 |
-25.421 |
|
Traceless |
| x | y | z |
x |
4.191 |
-0.320 |
0.000 |
y |
-0.320 |
-2.220 |
0.000 |
z |
0.000 |
0.000 |
-1.971 |
|
Polar |
3z2-r2 | -3.942 |
x2-y2 | 4.274 |
xy | -0.320 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.611 |
0.365 |
0.000 |
y |
0.365 |
5.796 |
0.000 |
z |
0.000 |
0.000 |
4.805 |
<r2> (average value of r
2) Å
2
<r2> |
80.665 |
(<r2>)1/2 |
8.981 |
Jump to
S1C1
Energy calculated at PBE1PBE/daug-cc-pVDZ
| hartrees |
Energy at 0K | -216.922704 |
Energy at 298.15K | |
HF Energy | -216.922704 |
Nuclear repulsion energy | 113.970949 |
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 PBE1PBE/daug-cc-pVDZ
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 |
3259 |
3259 |
8.92 |
62.42 |
0.60 |
0.75 |
2 |
A |
3187 |
3187 |
5.64 |
114.63 |
0.22 |
0.36 |
3 |
A |
3159 |
3159 |
7.17 |
86.72 |
0.09 |
0.17 |
4 |
A |
3121 |
3121 |
17.56 |
66.54 |
0.71 |
0.83 |
5 |
A |
3057 |
3057 |
29.91 |
146.09 |
0.07 |
0.14 |
6 |
A |
1732 |
1732 |
0.46 |
47.06 |
0.07 |
0.13 |
7 |
A |
1474 |
1474 |
6.40 |
3.61 |
0.56 |
0.72 |
8 |
A |
1444 |
1444 |
16.67 |
9.81 |
0.53 |
0.69 |
9 |
A |
1364 |
1364 |
11.95 |
4.65 |
0.21 |
0.35 |
10 |
A |
1307 |
1307 |
0.10 |
13.97 |
0.31 |
0.47 |
11 |
A |
1251 |
1251 |
4.43 |
6.79 |
0.68 |
0.81 |
12 |
A |
1178 |
1178 |
2.97 |
1.11 |
0.41 |
0.58 |
13 |
A |
1048 |
1048 |
119.48 |
5.53 |
0.57 |
0.73 |
14 |
A |
1029 |
1029 |
28.58 |
2.35 |
0.68 |
0.81 |
15 |
A |
988 |
988 |
17.00 |
2.10 |
0.29 |
0.45 |
16 |
A |
981 |
981 |
44.14 |
2.32 |
0.14 |
0.25 |
17 |
A |
923 |
923 |
1.86 |
2.89 |
0.13 |
0.23 |
18 |
A |
660 |
660 |
7.84 |
1.63 |
0.28 |
0.44 |
19 |
A |
433 |
433 |
2.40 |
3.61 |
0.31 |
0.47 |
20 |
A |
331 |
331 |
7.42 |
1.24 |
0.73 |
0.85 |
21 |
A |
114 |
114 |
0.96 |
2.62 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16019.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16019.3 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 PBE1PBE/daug-cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.606 |
0.427 |
0.328 |
C2 |
0.644 |
-0.380 |
0.249 |
C3 |
1.799 |
0.094 |
-0.219 |
F4 |
-1.641 |
-0.223 |
-0.353 |
H5 |
2.703 |
-0.514 |
-0.231 |
H6 |
1.883 |
1.114 |
-0.601 |
H7 |
0.577 |
-1.405 |
0.621 |
H8 |
-0.943 |
0.546 |
1.369 |
H9 |
-0.476 |
1.418 |
-0.128 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4894 | 2.4884 | 1.3994 | 3.4849 | 2.7433 | 2.1999 | 1.1007 | 1.0987 |
C2 | 1.4894 | | 1.3334 | 2.3686 | 2.1185 | 2.1182 | 1.0928 | 2.1513 | 2.1513 | C3 | 2.4884 | 1.3334 | | 3.4577 | 1.0896 | 1.0917 | 2.1090 | 3.2004 | 2.6336 | F4 | 1.3994 | 2.3686 | 3.4577 | | 4.3557 | 3.7771 | 2.6953 | 2.0108 | 2.0256 | H5 | 3.4849 | 2.1185 | 1.0896 | 4.3557 | | 1.8598 | 2.4580 | 4.1201 | 3.7213 | H6 | 2.7433 | 2.1182 | 1.0917 | 3.7771 | 1.8598 | | 3.0891 | 3.4908 | 2.4246 | H7 | 2.1999 | 1.0928 | 2.1090 | 2.6953 | 2.4580 | 3.0891 | | 2.5835 | 3.1047 | H8 | 1.1007 | 2.1513 | 3.2004 | 2.0108 | 4.1201 | 3.4908 | 2.5835 | | 1.7941 | H9 | 1.0987 | 2.1513 | 2.6336 | 2.0256 | 3.7213 | 2.4246 | 3.1047 | 1.7941 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.563 |
|
C1 |
C2 |
H7 |
116.002 |
C2 |
C1 |
F4 |
110.112 |
|
C2 |
C1 |
H8 |
111.435 |
C2 |
C1 |
H9 |
111.562 |
|
C2 |
C3 |
H5 |
121.608 |
C2 |
C3 |
H6 |
121.401 |
|
C3 |
C2 |
H7 |
120.426 |
F4 |
C1 |
H8 |
106.471 |
|
F4 |
C1 |
H9 |
107.746 |
H5 |
C3 |
H6 |
116.990 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/daug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
1.165 |
|
|
|
2 |
C |
1.718 |
|
|
|
3 |
C |
0.803 |
|
|
|
4 |
F |
-0.434 |
|
|
|
5 |
H |
-0.810 |
|
|
|
6 |
H |
-0.755 |
|
|
|
7 |
H |
-0.842 |
|
|
|
8 |
H |
-0.222 |
|
|
|
9 |
H |
-0.623 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.547 |
0.741 |
0.878 |
1.927 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.887 |
-1.177 |
-2.066 |
y |
-1.177 |
-22.656 |
-1.048 |
z |
-2.066 |
-1.048 |
-25.027 |
|
Traceless |
| x | y | z |
x |
-2.046 |
-1.177 |
-2.066 |
y |
-1.177 |
2.801 |
-1.048 |
z |
-2.066 |
-1.048 |
-0.755 |
|
Polar |
3z2-r2 | -1.509 |
x2-y2 | -3.231 |
xy | -1.177 |
xz | -2.066 |
yz | -1.048 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.609 |
0.229 |
-0.629 |
y |
0.229 |
5.589 |
-0.222 |
z |
-0.629 |
-0.222 |
5.137 |
<r2> (average value of r
2) Å
2
<r2> |
89.334 |
(<r2>)1/2 |
9.452 |