Jump to
S1C2
Energy calculated at B3LYP/cc-pVDZ
| hartrees |
Energy at 0K | -217.145214 |
Energy at 298.15K | |
HF Energy | -217.145214 |
Nuclear repulsion energy | 116.086982 |
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 B3LYP/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' |
3250 |
3152 |
5.58 |
61.23 |
0.72 |
0.84 |
2 |
A' |
3157 |
3062 |
4.89 |
173.37 |
0.13 |
0.22 |
3 |
A' |
3142 |
3047 |
10.53 |
34.59 |
0.70 |
0.83 |
4 |
A' |
3001 |
2911 |
42.05 |
187.08 |
0.11 |
0.19 |
5 |
A' |
1724 |
1673 |
4.38 |
19.74 |
0.15 |
0.26 |
6 |
A' |
1465 |
1421 |
3.44 |
18.09 |
0.57 |
0.73 |
7 |
A' |
1424 |
1381 |
8.62 |
13.81 |
0.55 |
0.71 |
8 |
A' |
1401 |
1359 |
12.60 |
6.50 |
0.75 |
0.86 |
9 |
A' |
1303 |
1264 |
0.20 |
18.79 |
0.37 |
0.54 |
10 |
A' |
1129 |
1095 |
50.12 |
2.03 |
0.75 |
0.86 |
11 |
A' |
1006 |
976 |
36.20 |
5.58 |
0.69 |
0.82 |
12 |
A' |
914 |
887 |
2.02 |
3.68 |
0.13 |
0.24 |
13 |
A' |
608 |
589 |
5.50 |
1.71 |
0.72 |
0.84 |
14 |
A' |
269 |
261 |
2.24 |
1.15 |
0.51 |
0.68 |
15 |
A" |
3035 |
2944 |
38.11 |
112.87 |
0.75 |
0.86 |
16 |
A" |
1247 |
1210 |
0.07 |
8.78 |
0.75 |
0.86 |
17 |
A" |
1033 |
1002 |
10.76 |
1.00 |
0.75 |
0.86 |
18 |
A" |
1016 |
986 |
6.44 |
0.00 |
0.75 |
0.86 |
19 |
A" |
949 |
920 |
32.37 |
0.62 |
0.75 |
0.86 |
20 |
A" |
561 |
544 |
8.43 |
9.74 |
0.75 |
0.86 |
21 |
A" |
186 |
181 |
2.52 |
5.34 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15909.8 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 15432.5 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 B3LYP/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.945 |
-0.205 |
0.000 |
C2 |
0.000 |
0.957 |
0.000 |
C3 |
1.329 |
0.843 |
0.000 |
F4 |
-0.267 |
-1.417 |
0.000 |
H5 |
1.973 |
1.725 |
0.000 |
H6 |
1.804 |
-0.140 |
0.000 |
H7 |
-0.480 |
1.943 |
0.000 |
H8 |
-1.599 |
-0.175 |
0.892 |
H9 |
-1.599 |
-0.175 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4976 | 2.5034 | 1.3888 | 3.4983 | 2.7496 | 2.1978 | 1.1068 | 1.1068 |
C2 | 1.4976 | | 1.3339 | 2.3895 | 2.1174 | 2.1118 | 1.0967 | 2.1531 | 2.1531 | C3 | 2.5034 | 1.3339 | | 2.7669 | 1.0922 | 1.0921 | 2.1175 | 3.2258 | 3.2258 | F4 | 1.3888 | 2.3895 | 2.7669 | | 3.8591 | 2.4334 | 3.3672 | 2.0275 | 2.0275 | H5 | 3.4983 | 2.1174 | 1.0922 | 3.8591 | | 1.8728 | 2.4632 | 4.1435 | 4.1435 | H6 | 2.7496 | 2.1118 | 1.0921 | 2.4334 | 1.8728 | | 3.0919 | 3.5182 | 3.5182 | H7 | 2.1978 | 1.0967 | 2.1175 | 3.3672 | 2.4632 | 3.0919 | | 2.5569 | 2.5569 | H8 | 1.1068 | 2.1531 | 3.2258 | 2.0275 | 4.1435 | 3.5182 | 2.5569 | | 1.7847 | H9 | 1.1068 | 2.1531 | 3.2258 | 2.0275 | 4.1435 | 3.5182 | 2.5569 | 1.7847 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.189 |
|
C1 |
C2 |
H7 |
114.928 |
C2 |
C1 |
F4 |
111.697 |
|
C2 |
C1 |
H8 |
110.630 |
C2 |
C1 |
H9 |
110.630 |
|
C2 |
C3 |
H5 |
121.238 |
C2 |
C3 |
H6 |
120.715 |
|
C3 |
C2 |
H7 |
120.883 |
F4 |
C1 |
H8 |
108.136 |
|
F4 |
C1 |
H9 |
108.136 |
H5 |
C3 |
H6 |
118.047 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.282 |
|
|
|
2 |
C |
-0.162 |
|
|
|
3 |
C |
0.034 |
|
|
|
4 |
F |
-0.239 |
|
|
|
5 |
H |
0.018 |
|
|
|
6 |
H |
0.021 |
|
|
|
7 |
H |
-0.007 |
|
|
|
8 |
H |
0.027 |
|
|
|
9 |
H |
0.027 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.889 |
1.360 |
0.000 |
1.625 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.256 |
-0.339 |
0.000 |
y |
-0.339 |
-25.102 |
0.000 |
z |
0.000 |
0.000 |
-24.870 |
|
Traceless |
| x | y | z |
x |
3.730 |
-0.339 |
0.000 |
y |
-0.339 |
-2.039 |
0.000 |
z |
0.000 |
0.000 |
-1.691 |
|
Polar |
3z2-r2 | -3.382 |
x2-y2 | 3.846 |
xy | -0.339 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.896 |
0.273 |
0.000 |
y |
0.273 |
4.803 |
0.000 |
z |
0.000 |
0.000 |
3.110 |
<r2> (average value of r
2) Å
2
<r2> |
80.430 |
(<r2>)1/2 |
8.968 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVDZ
| hartrees |
Energy at 0K | -217.143552 |
Energy at 298.15K | |
HF Energy | -217.143552 |
Nuclear repulsion energy | 113.622952 |
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 B3LYP/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 |
3229 |
3132 |
12.07 |
71.36 |
0.62 |
0.76 |
2 |
A |
3152 |
3058 |
6.65 |
136.86 |
0.24 |
0.39 |
3 |
A |
3133 |
3039 |
9.53 |
68.65 |
0.12 |
0.22 |
4 |
A |
3069 |
2976 |
31.06 |
76.61 |
0.70 |
0.82 |
5 |
A |
3014 |
2923 |
39.91 |
140.99 |
0.12 |
0.21 |
6 |
A |
1723 |
1671 |
0.56 |
19.41 |
0.16 |
0.27 |
7 |
A |
1472 |
1428 |
1.75 |
8.76 |
0.65 |
0.79 |
8 |
A |
1440 |
1397 |
18.44 |
11.53 |
0.63 |
0.77 |
9 |
A |
1377 |
1336 |
16.81 |
4.84 |
0.56 |
0.72 |
10 |
A |
1301 |
1262 |
0.23 |
14.56 |
0.46 |
0.63 |
11 |
A |
1249 |
1211 |
4.09 |
13.30 |
0.72 |
0.84 |
12 |
A |
1170 |
1135 |
2.27 |
1.74 |
0.70 |
0.82 |
13 |
A |
1047 |
1016 |
101.03 |
4.45 |
0.63 |
0.77 |
14 |
A |
1023 |
992 |
31.91 |
1.51 |
0.75 |
0.86 |
15 |
A |
981 |
951 |
2.95 |
1.27 |
0.23 |
0.37 |
16 |
A |
957 |
928 |
36.18 |
0.65 |
0.46 |
0.63 |
17 |
A |
923 |
896 |
2.86 |
2.75 |
0.20 |
0.34 |
18 |
A |
649 |
630 |
6.34 |
5.76 |
0.65 |
0.79 |
19 |
A |
435 |
422 |
2.26 |
4.75 |
0.50 |
0.67 |
20 |
A |
323 |
313 |
6.30 |
4.04 |
0.75 |
0.86 |
21 |
A |
116 |
113 |
1.04 |
6.60 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 15891.1 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 15414.4 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 B3LYP/cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.608 |
0.441 |
0.301 |
C2 |
0.645 |
-0.375 |
0.238 |
C3 |
1.816 |
0.085 |
-0.208 |
F4 |
-1.658 |
-0.233 |
-0.330 |
H5 |
2.715 |
-0.537 |
-0.202 |
H6 |
1.922 |
1.105 |
-0.590 |
H7 |
0.557 |
-1.402 |
0.611 |
H8 |
-0.915 |
0.608 |
1.350 |
H9 |
-0.475 |
1.420 |
-0.189 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4963 | 2.5025 | 1.3982 | 3.5001 | 2.7633 | 2.2017 | 1.1057 | 1.1036 |
C2 | 1.4963 | | 1.3349 | 2.3765 | 2.1225 | 2.1229 | 1.0964 | 2.1532 | 2.1584 | C3 | 2.5025 | 1.3349 | | 3.4908 | 1.0928 | 1.0949 | 2.1137 | 3.1877 | 2.6518 | F4 | 1.3982 | 2.3765 | 3.4908 | | 4.3855 | 3.8305 | 2.6754 | 2.0208 | 2.0383 | H5 | 3.5001 | 2.1225 | 1.0928 | 4.3855 | | 1.8646 | 2.4633 | 4.1107 | 3.7423 | H6 | 2.7633 | 2.1229 | 1.0949 | 3.8305 | 1.8646 | | 3.0973 | 3.4726 | 2.4500 | H7 | 2.2017 | 1.0964 | 2.1137 | 2.6754 | 2.4633 | 3.0973 | | 2.5989 | 3.1095 | H8 | 1.1057 | 2.1532 | 3.1877 | 2.0208 | 4.1107 | 3.4726 | 2.5989 | | 1.7947 | H9 | 1.1036 | 2.1584 | 2.6518 | 2.0383 | 3.7423 | 2.4500 | 3.1095 | 1.7947 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.141 |
|
C1 |
C2 |
H7 |
115.389 |
C2 |
C1 |
F4 |
110.330 |
|
C2 |
C1 |
H8 |
110.799 |
C2 |
C1 |
H9 |
111.340 |
|
C2 |
C3 |
H5 |
121.600 |
C2 |
C3 |
H6 |
121.473 |
|
C3 |
C2 |
H7 |
120.458 |
F4 |
C1 |
H8 |
107.041 |
|
F4 |
C1 |
H9 |
108.549 |
H5 |
C3 |
H6 |
116.925 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.278 |
|
|
|
2 |
C |
-0.122 |
|
|
|
3 |
C |
0.025 |
|
|
|
4 |
F |
-0.256 |
|
|
|
5 |
H |
0.026 |
|
|
|
6 |
H |
0.016 |
|
|
|
7 |
H |
-0.001 |
|
|
|
8 |
H |
0.024 |
|
|
|
9 |
H |
0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.378 |
0.701 |
0.787 |
1.735 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.495 |
-1.008 |
-1.599 |
y |
-1.008 |
-22.466 |
-0.809 |
z |
-1.599 |
-0.809 |
-24.492 |
|
Traceless |
| x | y | z |
x |
-2.016 |
-1.008 |
-1.599 |
y |
-1.008 |
2.527 |
-0.809 |
z |
-1.599 |
-0.809 |
-0.511 |
|
Polar |
3z2-r2 | -1.023 |
x2-y2 | -3.029 |
xy | -1.008 |
xz | -1.599 |
yz | -0.809 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.615 |
0.166 |
-0.880 |
y |
0.166 |
4.693 |
-0.552 |
z |
-0.880 |
-0.552 |
3.533 |
<r2> (average value of r
2) Å
2
<r2> |
89.918 |
(<r2>)1/2 |
9.482 |