Jump to
S1C2
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -276.922121 |
| Energy at 298.15K | -276.927320 |
| HF Energy | -276.922121 |
| Nuclear repulsion energy | 126.953999 |
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/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3263 |
2932 |
0.00 |
193.58 |
0.10 |
0.18 |
| 2 |
Ag |
1680 |
1510 |
0.00 |
19.19 |
0.74 |
0.85 |
| 3 |
Ag |
1618 |
1454 |
0.00 |
3.01 |
0.51 |
0.67 |
| 4 |
Ag |
1193 |
1072 |
0.00 |
11.34 |
0.73 |
0.84 |
| 5 |
Ag |
1170 |
1051 |
0.00 |
8.57 |
0.23 |
0.37 |
| 6 |
Ag |
497 |
447 |
0.00 |
2.59 |
0.46 |
0.63 |
| 7 |
Au |
3331 |
2993 |
90.18 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1356 |
1218 |
6.93 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
881 |
792 |
0.71 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
145 |
130 |
15.82 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3305 |
2970 |
0.00 |
123.72 |
0.75 |
0.86 |
| 12 |
Bg |
1420 |
1276 |
0.00 |
18.17 |
0.75 |
0.86 |
| 13 |
Bg |
1296 |
1164 |
0.00 |
4.65 |
0.75 |
0.86 |
| 14 |
Bu |
3265 |
2934 |
73.00 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1687 |
1516 |
3.23 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1499 |
1347 |
28.40 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1196 |
1075 |
253.52 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
306 |
275 |
23.50 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 14554.1 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13076.9 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 HF/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.422 |
0.627 |
0.000 |
| C2 |
-0.422 |
-0.627 |
0.000 |
| F3 |
-0.422 |
1.704 |
0.000 |
| F4 |
0.422 |
-1.704 |
0.000 |
| H5 |
1.046 |
0.672 |
0.882 |
| H6 |
1.046 |
0.672 |
-0.882 |
| H7 |
-1.046 |
-0.672 |
0.882 |
| H8 |
-1.046 |
-0.672 |
-0.882 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5118 | 1.3683 | 2.3307 | 1.0813 | 1.0813 | 2.1496 | 2.1496 |
C2 | 1.5118 | | 2.3307 | 1.3683 | 2.1496 | 2.1496 | 1.0813 | 1.0813 | F3 | 1.3683 | 2.3307 | | 3.5104 | 1.9997 | 1.9997 | 2.6096 | 2.6096 | F4 | 2.3307 | 1.3683 | 3.5104 | | 2.6096 | 2.6096 | 1.9997 | 1.9997 | H5 | 1.0813 | 2.1496 | 1.9997 | 2.6096 | | 1.7640 | 2.4864 | 3.0486 | H6 | 1.0813 | 2.1496 | 1.9997 | 2.6096 | 1.7640 | | 3.0486 | 2.4864 | H7 | 2.1496 | 1.0813 | 2.6096 | 1.9997 | 2.4864 | 3.0486 | | 1.7640 | H8 | 2.1496 | 1.0813 | 2.6096 | 1.9997 | 3.0486 | 2.4864 | 1.7640 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.939 |
|
C1 |
C2 |
H7 |
110.891 |
| C1 |
C2 |
H8 |
110.891 |
|
C2 |
C1 |
F3 |
107.939 |
| C2 |
C1 |
H5 |
110.891 |
|
C2 |
C1 |
H6 |
110.891 |
| F3 |
C1 |
H5 |
108.876 |
|
F3 |
C1 |
H6 |
108.876 |
| F4 |
C2 |
H7 |
108.876 |
|
F4 |
C2 |
H8 |
108.876 |
| H5 |
C1 |
H6 |
109.313 |
|
H7 |
C2 |
H8 |
109.313 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.069 |
|
|
|
| 2 |
C |
0.069 |
|
|
|
| 3 |
F |
-0.407 |
|
|
|
| 4 |
F |
-0.407 |
|
|
|
| 5 |
H |
0.169 |
|
|
|
| 6 |
H |
0.169 |
|
|
|
| 7 |
H |
0.169 |
|
|
|
| 8 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.664 |
3.029 |
0.000 |
| y |
3.029 |
-29.149 |
0.000 |
| z |
0.000 |
0.000 |
-21.271 |
|
| Traceless |
| | x | y | z |
| x |
3.546 |
3.029 |
0.000 |
| y |
3.029 |
-7.681 |
0.000 |
| z |
0.000 |
0.000 |
4.135 |
|
| Polar |
| 3z2-r2 | 8.271 |
| x2-y2 | 7.484 |
| xy | 3.029 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.274 |
0.050 |
0.000 |
| y |
0.050 |
3.151 |
0.000 |
| z |
0.000 |
0.000 |
3.219 |
<r2> (average value of r
2) Å
2
| <r2> |
86.612 |
| (<r2>)1/2 |
9.307 |
Jump to
S1C1
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -276.921403 |
| Energy at 298.15K | |
| HF Energy | -276.921403 |
| Nuclear repulsion energy | 129.202758 |
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/6-31G*
| 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 |
3300 |
2965 |
27.57 |
|
|
|
| 2 |
A |
3258 |
2927 |
44.61 |
|
|
|
| 3 |
A |
1662 |
1494 |
0.07 |
|
|
|
| 4 |
A |
1607 |
1443 |
26.20 |
|
|
|
| 5 |
A |
1424 |
1280 |
2.84 |
|
|
|
| 6 |
A |
1251 |
1124 |
24.46 |
|
|
|
| 7 |
A |
1230 |
1106 |
84.21 |
|
|
|
| 8 |
A |
956 |
859 |
31.30 |
|
|
|
| 9 |
A |
348 |
312 |
0.28 |
|
|
|
| 10 |
A |
150 |
135 |
4.41 |
|
|
|
| 11 |
B |
3314 |
2977 |
69.78 |
|
|
|
| 12 |
B |
3242 |
2913 |
21.47 |
|
|
|
| 13 |
B |
1658 |
1490 |
4.05 |
|
|
|
| 14 |
B |
1563 |
1404 |
21.67 |
|
|
|
| 15 |
B |
1383 |
1243 |
7.59 |
|
|
|
| 16 |
B |
1211 |
1088 |
48.03 |
|
|
|
| 17 |
B |
1002 |
900 |
51.50 |
|
|
|
| 18 |
B |
541 |
486 |
20.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14549.6 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13072.9 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 HF/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.262 |
0.705 |
0.511 |
| C2 |
-0.262 |
-0.705 |
0.511 |
| F3 |
-0.262 |
1.395 |
-0.546 |
| F4 |
0.262 |
-1.395 |
-0.546 |
| H5 |
-0.027 |
1.210 |
1.425 |
| H6 |
1.340 |
0.709 |
0.421 |
| H7 |
0.027 |
-1.210 |
1.425 |
| H8 |
-1.340 |
-0.709 |
0.421 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5036 | 1.3661 | 2.3505 | 1.0833 | 1.0817 | 2.1344 | 2.1379 |
C2 | 1.5036 | | 2.3505 | 1.3661 | 2.1344 | 2.1379 | 1.0833 | 1.0817 | F3 | 1.3661 | 2.3505 | | 2.8385 | 1.9931 | 1.9922 | 3.2787 | 2.5538 | F4 | 2.3505 | 1.3661 | 2.8385 | | 3.2787 | 2.5538 | 1.9931 | 1.9922 | H5 | 1.0833 | 2.1344 | 1.9931 | 3.2787 | | 1.7680 | 2.4197 | 2.5322 | H6 | 1.0817 | 2.1379 | 1.9922 | 2.5538 | 1.7680 | | 2.5322 | 3.0312 | H7 | 2.1344 | 1.0833 | 3.2787 | 1.9931 | 2.4197 | 2.5322 | | 1.7680 | H8 | 2.1379 | 1.0817 | 2.5538 | 1.9922 | 2.5322 | 3.0312 | 1.7680 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.893 |
|
C1 |
C2 |
H7 |
110.127 |
| C1 |
C2 |
H8 |
110.509 |
|
C2 |
C1 |
F3 |
109.893 |
| C2 |
C1 |
H5 |
110.127 |
|
C2 |
C1 |
H6 |
110.509 |
| F3 |
C1 |
H5 |
108.370 |
|
F3 |
C1 |
H6 |
108.392 |
| F4 |
C2 |
H7 |
108.370 |
|
F4 |
C2 |
H8 |
108.392 |
| H5 |
C1 |
H6 |
109.502 |
|
H7 |
C2 |
H8 |
109.502 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.076 |
|
|
|
| 2 |
C |
0.076 |
|
|
|
| 3 |
F |
-0.401 |
|
|
|
| 4 |
F |
-0.401 |
|
|
|
| 5 |
H |
0.153 |
|
|
|
| 6 |
H |
0.172 |
|
|
|
| 7 |
H |
0.153 |
|
|
|
| 8 |
H |
0.172 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.877 |
2.877 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.388 |
1.647 |
0.005 |
| y |
1.647 |
-25.953 |
-0.006 |
| z |
0.005 |
-0.006 |
-21.993 |
|
| Traceless |
| | x | y | z |
| x |
2.586 |
1.647 |
0.005 |
| y |
1.647 |
-4.262 |
-0.006 |
| z |
0.005 |
-0.006 |
1.677 |
|
| Polar |
| 3z2-r2 | 3.353 |
| x2-y2 | 4.565 |
| xy | 1.647 |
| xz | 0.005 |
| yz | -0.006 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.242 |
0.019 |
-0.001 |
| y |
0.019 |
3.241 |
0.008 |
| z |
-0.001 |
0.008 |
3.231 |
<r2> (average value of r
2) Å
2
| <r2> |
77.901 |
| (<r2>)1/2 |
8.826 |