Jump to
S1C2
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -214.739368 |
Energy at 298.15K | |
HF Energy | -214.739368 |
Nuclear repulsion energy | 117.121513 |
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 HF/3-21G*
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' |
3424 |
3091 |
5.15 |
45.80 |
0.74 |
0.85 |
2 |
A' |
3350 |
3024 |
7.80 |
131.75 |
0.14 |
0.24 |
3 |
A' |
3331 |
3007 |
6.13 |
31.49 |
0.68 |
0.81 |
4 |
A' |
3224 |
2910 |
36.86 |
135.58 |
0.13 |
0.23 |
5 |
A' |
1870 |
1688 |
1.28 |
17.54 |
0.15 |
0.26 |
6 |
A' |
1687 |
1523 |
0.67 |
22.71 |
0.67 |
0.81 |
7 |
A' |
1603 |
1447 |
6.55 |
13.15 |
0.53 |
0.69 |
8 |
A' |
1553 |
1402 |
11.75 |
9.99 |
0.56 |
0.72 |
9 |
A' |
1458 |
1316 |
0.31 |
20.77 |
0.38 |
0.55 |
10 |
A' |
1229 |
1109 |
21.17 |
2.91 |
0.73 |
0.84 |
11 |
A' |
1118 |
1009 |
44.33 |
5.57 |
0.75 |
0.86 |
12 |
A' |
953 |
860 |
3.58 |
8.29 |
0.16 |
0.28 |
13 |
A' |
659 |
595 |
5.61 |
1.93 |
0.74 |
0.85 |
14 |
A' |
313 |
283 |
5.53 |
1.05 |
0.57 |
0.73 |
15 |
A" |
3256 |
2939 |
41.97 |
94.22 |
0.75 |
0.86 |
16 |
A" |
1380 |
1245 |
0.02 |
13.62 |
0.75 |
0.86 |
17 |
A" |
1188 |
1072 |
0.62 |
4.28 |
0.75 |
0.86 |
18 |
A" |
1141 |
1030 |
54.52 |
0.05 |
0.75 |
0.86 |
19 |
A" |
1136 |
1025 |
43.11 |
0.86 |
0.75 |
0.86 |
20 |
A" |
644 |
581 |
14.55 |
15.15 |
0.75 |
0.86 |
21 |
A" |
194 |
175 |
5.37 |
7.24 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17354.8 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15664.4 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 HF/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.954 |
-0.189 |
0.000 |
C2 |
0.000 |
0.968 |
0.000 |
C3 |
1.303 |
0.808 |
0.000 |
F4 |
-0.242 |
-1.401 |
0.000 |
H5 |
1.976 |
1.643 |
0.000 |
H6 |
1.734 |
-0.172 |
0.000 |
H7 |
-0.455 |
1.941 |
0.000 |
H8 |
-1.586 |
-0.165 |
0.878 |
H9 |
-1.586 |
-0.165 |
-0.878 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4996 | 2.4672 | 1.4052 | 3.4551 | 2.6877 | 2.1880 | 1.0818 | 1.0818 |
C2 | 1.4996 | | 1.3125 | 2.3810 | 2.0877 | 2.0752 | 1.0745 | 2.1375 | 2.1375 | C3 | 2.4672 | 1.3125 | | 2.6953 | 1.0720 | 1.0711 | 2.0916 | 3.1719 | 3.1719 | F4 | 1.4052 | 2.3810 | 2.6953 | | 3.7656 | 2.3263 | 3.3487 | 2.0256 | 2.0256 | H5 | 3.4551 | 2.0877 | 1.0720 | 3.7656 | | 1.8311 | 2.4493 | 4.0893 | 4.0893 | H6 | 2.6877 | 2.0752 | 1.0711 | 2.3263 | 1.8311 | | 3.0430 | 3.4336 | 3.4336 | H7 | 2.1880 | 1.0745 | 2.0916 | 3.3487 | 2.4493 | 3.0430 | | 2.5466 | 2.5466 | H8 | 1.0818 | 2.1375 | 3.1719 | 2.0256 | 4.0893 | 3.4336 | 2.5466 | | 1.7557 | H9 | 1.0818 | 2.1375 | 3.1719 | 2.0256 | 4.0893 | 3.4336 | 2.5466 | 1.7557 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
122.504 |
|
C1 |
C2 |
H7 |
115.429 |
C2 |
C1 |
F4 |
110.058 |
|
C2 |
C1 |
H8 |
110.750 |
C2 |
C1 |
H9 |
110.750 |
|
C2 |
C3 |
H5 |
121.893 |
C2 |
C3 |
H6 |
120.726 |
|
C3 |
C2 |
H7 |
122.066 |
F4 |
C1 |
H8 |
108.369 |
|
F4 |
C1 |
H9 |
108.369 |
H5 |
C3 |
H6 |
117.381 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.003 |
|
|
|
2 |
C |
-0.328 |
|
|
|
3 |
C |
-0.392 |
|
|
|
4 |
F |
-0.405 |
|
|
|
5 |
H |
0.217 |
|
|
|
6 |
H |
0.244 |
|
|
|
7 |
H |
0.232 |
|
|
|
8 |
H |
0.215 |
|
|
|
9 |
H |
0.215 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.001 |
1.832 |
0.000 |
2.088 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.451 |
-0.301 |
0.000 |
y |
-0.301 |
-25.823 |
0.000 |
z |
0.000 |
0.000 |
-25.310 |
|
Traceless |
| x | y | z |
x |
5.116 |
-0.301 |
0.000 |
y |
-0.301 |
-2.943 |
0.000 |
z |
0.000 |
0.000 |
-2.174 |
|
Polar |
3z2-r2 | -4.347 |
x2-y2 | 5.373 |
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 |
6.131 |
0.051 |
0.000 |
y |
0.051 |
3.923 |
0.000 |
z |
0.000 |
0.000 |
2.266 |
<r2> (average value of r
2) Å
2
<r2> |
78.722 |
(<r2>)1/2 |
8.873 |
Jump to
S1C1
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -214.736007 |
Energy at 298.15K | |
HF Energy | -214.736007 |
Nuclear repulsion energy | 114.158925 |
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 HF/3-21G*
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 |
3395 |
3065 |
14.22 |
56.54 |
0.47 |
0.64 |
2 |
A |
3352 |
3025 |
2.43 |
85.60 |
0.38 |
0.55 |
3 |
A |
3314 |
2991 |
9.05 |
69.08 |
0.12 |
0.21 |
4 |
A |
3280 |
2961 |
30.09 |
58.45 |
0.71 |
0.83 |
5 |
A |
3233 |
2918 |
33.55 |
109.57 |
0.15 |
0.26 |
6 |
A |
1867 |
1685 |
0.86 |
18.67 |
0.16 |
0.28 |
7 |
A |
1687 |
1523 |
0.56 |
12.26 |
0.72 |
0.84 |
8 |
A |
1621 |
1463 |
15.63 |
13.49 |
0.51 |
0.67 |
9 |
A |
1539 |
1389 |
22.89 |
5.03 |
0.75 |
0.86 |
10 |
A |
1452 |
1311 |
0.02 |
16.68 |
0.40 |
0.57 |
11 |
A |
1382 |
1247 |
2.29 |
19.11 |
0.73 |
0.84 |
12 |
A |
1274 |
1150 |
1.98 |
2.57 |
0.68 |
0.81 |
13 |
A |
1179 |
1064 |
7.42 |
6.63 |
0.72 |
0.83 |
14 |
A |
1151 |
1039 |
66.88 |
6.02 |
0.62 |
0.76 |
15 |
A |
1127 |
1017 |
93.82 |
0.62 |
0.67 |
0.80 |
16 |
A |
1097 |
991 |
9.03 |
0.87 |
0.59 |
0.74 |
17 |
A |
992 |
896 |
11.20 |
5.79 |
0.14 |
0.25 |
18 |
A |
686 |
619 |
11.83 |
11.68 |
0.71 |
0.83 |
19 |
A |
491 |
443 |
3.17 |
5.94 |
0.46 |
0.63 |
20 |
A |
332 |
300 |
8.05 |
3.36 |
0.75 |
0.86 |
21 |
A |
100 |
91 |
2.74 |
9.21 |
0.75 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 17275.4 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15592.8 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 HF/3-21G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.585 |
0.491 |
0.213 |
C2 |
0.639 |
-0.373 |
0.182 |
C3 |
1.833 |
0.057 |
-0.156 |
F4 |
-1.693 |
-0.257 |
-0.237 |
H5 |
2.694 |
-0.582 |
-0.124 |
H6 |
2.004 |
1.066 |
-0.484 |
H7 |
0.482 |
-1.386 |
0.501 |
H8 |
-0.798 |
0.810 |
1.224 |
H9 |
-0.471 |
1.361 |
-0.416 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4989 | 2.4848 | 1.4099 | 3.4668 | 2.7427 | 2.1784 | 1.0812 | 1.0795 |
C2 | 1.4989 | | 1.3136 | 2.3723 | 2.0881 | 2.0926 | 1.0736 | 2.1333 | 2.1439 | C3 | 2.4848 | 1.3136 | | 3.5411 | 1.0725 | 1.0750 | 2.0833 | 3.0654 | 2.6601 | F4 | 1.4099 | 2.3723 | 3.5411 | | 4.4004 | 3.9345 | 2.5597 | 2.0180 | 2.0352 | H5 | 3.4668 | 2.0881 | 1.0725 | 4.4004 | | 1.8229 | 2.4351 | 3.9939 | 3.7250 | H6 | 2.7427 | 2.0926 | 1.0750 | 3.9345 | 1.8229 | | 3.0499 | 3.2915 | 2.4933 | H7 | 2.1784 | 1.0736 | 2.0833 | 2.5597 | 2.4351 | 3.0499 | | 2.6429 | 3.0488 | H8 | 1.0812 | 2.1333 | 3.0654 | 2.0180 | 3.9939 | 3.2915 | 2.6429 | | 1.7602 | H9 | 1.0795 | 2.1439 | 2.6601 | 2.0352 | 3.7250 | 2.4933 | 3.0488 | 1.7602 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
124.004 |
|
C1 |
C2 |
H7 |
114.726 |
C2 |
C1 |
F4 |
109.251 |
|
C2 |
C1 |
H8 |
110.501 |
C2 |
C1 |
H9 |
111.465 |
|
C2 |
C3 |
H5 |
121.789 |
C2 |
C3 |
H6 |
122.034 |
|
C3 |
C2 |
H7 |
121.226 |
F4 |
C1 |
H8 |
107.473 |
|
F4 |
C1 |
H9 |
108.959 |
H5 |
C3 |
H6 |
116.177 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.010 |
|
|
|
2 |
C |
-0.290 |
|
|
|
3 |
C |
-0.412 |
|
|
|
4 |
F |
-0.408 |
|
|
|
5 |
H |
0.227 |
|
|
|
6 |
H |
0.213 |
|
|
|
7 |
H |
0.253 |
|
|
|
8 |
H |
0.216 |
|
|
|
9 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.871 |
1.094 |
0.788 |
2.306 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.482 |
-1.388 |
-1.558 |
y |
-1.388 |
-22.071 |
-0.916 |
z |
-1.558 |
-0.916 |
-24.968 |
|
Traceless |
| x | y | z |
x |
-2.963 |
-1.388 |
-1.558 |
y |
-1.388 |
3.655 |
-0.916 |
z |
-1.558 |
-0.916 |
-0.691 |
|
Polar |
3z2-r2 | -1.383 |
x2-y2 | -4.412 |
xy | -1.388 |
xz | -1.558 |
yz | -0.916 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.876 |
0.345 |
-0.766 |
y |
0.345 |
3.917 |
-0.516 |
z |
-0.766 |
-0.516 |
2.547 |
<r2> (average value of r
2) Å
2
<r2> |
90.233 |
(<r2>)1/2 |
9.499 |