Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -277.040819 |
| Energy at 298.15K | |
| HF Energy | -277.040819 |
| Nuclear repulsion energy | 127.153959 |
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/daug-cc-pVTZ
| 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 |
3208 |
2902 |
0.00 |
237.66 |
0.06 |
0.10 |
| 2 |
Ag |
1646 |
1489 |
0.00 |
5.98 |
0.75 |
0.86 |
| 3 |
Ag |
1589 |
1437 |
0.00 |
2.54 |
0.32 |
0.48 |
| 4 |
Ag |
1179 |
1066 |
0.00 |
9.11 |
0.73 |
0.84 |
| 5 |
Ag |
1154 |
1044 |
0.00 |
8.45 |
0.14 |
0.25 |
| 6 |
Ag |
497 |
449 |
0.00 |
2.31 |
0.32 |
0.49 |
| 7 |
Au |
3273 |
2961 |
63.37 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1349 |
1221 |
8.36 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
874 |
790 |
0.09 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
137 |
124 |
15.43 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3245 |
2935 |
0.00 |
100.15 |
0.75 |
0.86 |
| 12 |
Bg |
1410 |
1275 |
0.00 |
6.44 |
0.75 |
0.86 |
| 13 |
Bg |
1283 |
1160 |
0.00 |
1.01 |
0.75 |
0.86 |
| 14 |
Bu |
3212 |
2905 |
70.41 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1652 |
1494 |
4.23 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1483 |
1341 |
14.14 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1177 |
1064 |
283.31 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
312 |
282 |
22.63 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 14338.6 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 12970.7 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/daug-cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.420 |
0.629 |
0.000 |
| C2 |
-0.420 |
-0.629 |
0.000 |
| F3 |
-0.420 |
1.702 |
0.000 |
| F4 |
0.420 |
-1.702 |
0.000 |
| H5 |
1.042 |
0.678 |
0.882 |
| H6 |
1.042 |
0.678 |
-0.882 |
| H7 |
-1.042 |
-0.678 |
0.882 |
| H8 |
-1.042 |
-0.678 |
-0.882 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5119 | 1.3631 | 2.3309 | 1.0810 | 1.0810 | 2.1501 | 2.1501 |
C2 | 1.5119 | | 2.3309 | 1.3631 | 2.1501 | 2.1501 | 1.0810 | 1.0810 | F3 | 1.3631 | 2.3309 | | 3.5066 | 1.9917 | 1.9917 | 2.6134 | 2.6134 | F4 | 2.3309 | 1.3631 | 3.5066 | | 2.6134 | 2.6134 | 1.9917 | 1.9917 | H5 | 1.0810 | 2.1501 | 1.9917 | 2.6134 | | 1.7649 | 2.4865 | 3.0492 | H6 | 1.0810 | 2.1501 | 1.9917 | 2.6134 | 1.7649 | | 3.0492 | 2.4865 | H7 | 2.1501 | 1.0810 | 2.6134 | 1.9917 | 2.4865 | 3.0492 | | 1.7649 | H8 | 2.1501 | 1.0810 | 2.6134 | 1.9917 | 3.0492 | 2.4865 | 1.7649 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.227 |
|
C1 |
C2 |
H7 |
110.949 |
| C1 |
C2 |
H8 |
110.949 |
|
C2 |
C1 |
F3 |
108.227 |
| C2 |
C1 |
H5 |
110.949 |
|
C2 |
C1 |
H6 |
110.949 |
| F3 |
C1 |
H5 |
108.604 |
|
F3 |
C1 |
H6 |
108.604 |
| F4 |
C2 |
H7 |
108.604 |
|
F4 |
C2 |
H8 |
108.604 |
| H5 |
C1 |
H6 |
109.438 |
|
H7 |
C2 |
H8 |
109.438 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.044 |
|
|
|
| 2 |
C |
-0.044 |
|
|
|
| 3 |
F |
-0.954 |
|
|
|
| 4 |
F |
-0.954 |
|
|
|
| 5 |
H |
0.499 |
|
|
|
| 6 |
H |
0.499 |
|
|
|
| 7 |
H |
0.499 |
|
|
|
| 8 |
H |
0.499 |
|
|
|
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 |
-22.051 |
3.427 |
0.000 |
| y |
3.427 |
-29.617 |
0.000 |
| z |
0.000 |
0.000 |
-21.318 |
|
| Traceless |
| | x | y | z |
| x |
3.416 |
3.427 |
0.000 |
| y |
3.427 |
-7.933 |
0.000 |
| z |
0.000 |
0.000 |
4.517 |
|
| Polar |
| 3z2-r2 | 9.033 |
| x2-y2 | 7.566 |
| xy | 3.427 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.988 |
-0.014 |
0.000 |
| y |
-0.014 |
4.123 |
0.000 |
| z |
0.000 |
0.000 |
3.715 |
<r2> (average value of r
2) Å
2
| <r2> |
86.682 |
| (<r2>)1/2 |
9.310 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -277.041418 |
| Energy at 298.15K | |
| HF Energy | -277.041418 |
| Nuclear repulsion energy | 129.245928 |
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/daug-cc-pVTZ
| 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 |
3241 |
2932 |
21.54 |
76.77 |
0.75 |
0.85 |
| 2 |
A |
3204 |
2898 |
45.34 |
217.40 |
0.02 |
0.04 |
| 3 |
A |
1623 |
1469 |
0.78 |
1.14 |
0.75 |
0.86 |
| 4 |
A |
1579 |
1429 |
14.66 |
1.41 |
0.06 |
0.12 |
| 5 |
A |
1416 |
1281 |
5.74 |
7.20 |
0.66 |
0.79 |
| 6 |
A |
1235 |
1117 |
37.89 |
1.95 |
0.10 |
0.18 |
| 7 |
A |
1216 |
1100 |
85.74 |
3.56 |
0.73 |
0.85 |
| 8 |
A |
939 |
849 |
27.93 |
7.28 |
0.14 |
0.24 |
| 9 |
A |
347 |
314 |
0.29 |
0.30 |
0.27 |
0.42 |
| 10 |
A |
160 |
145 |
4.36 |
0.07 |
0.75 |
0.86 |
| 11 |
B |
3256 |
2945 |
51.81 |
10.02 |
0.75 |
0.86 |
| 12 |
B |
3190 |
2885 |
12.14 |
31.86 |
0.75 |
0.86 |
| 13 |
B |
1621 |
1466 |
7.50 |
5.30 |
0.75 |
0.86 |
| 14 |
B |
1532 |
1386 |
12.01 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1376 |
1245 |
10.85 |
1.96 |
0.75 |
0.86 |
| 16 |
B |
1197 |
1083 |
64.23 |
3.71 |
0.75 |
0.86 |
| 17 |
B |
989 |
895 |
55.37 |
2.28 |
0.75 |
0.86 |
| 18 |
B |
543 |
491 |
20.54 |
0.37 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 14332.5 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 12965.2 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 HF/daug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.260 |
0.705 |
0.504 |
| C2 |
-0.260 |
-0.705 |
0.504 |
| F3 |
-0.260 |
1.406 |
-0.540 |
| F4 |
0.260 |
-1.406 |
-0.540 |
| H5 |
-0.030 |
1.199 |
1.422 |
| H6 |
1.338 |
0.714 |
0.412 |
| H7 |
0.030 |
-1.199 |
1.422 |
| H8 |
-1.338 |
-0.714 |
0.412 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5025 | 1.3611 | 2.3549 | 1.0830 | 1.0815 | 2.1265 | 2.1391 |
C2 | 1.5025 | | 2.3549 | 1.3611 | 2.1265 | 2.1391 | 1.0830 | 1.0815 | F3 | 1.3611 | 2.3549 | | 2.8604 | 1.9864 | 1.9850 | 3.2747 | 2.5618 | F4 | 2.3549 | 1.3611 | 2.8604 | | 3.2747 | 2.5618 | 1.9864 | 1.9850 | H5 | 1.0830 | 2.1265 | 1.9864 | 3.2747 | | 1.7688 | 2.3995 | 2.5280 | H6 | 1.0815 | 2.1391 | 1.9850 | 2.5618 | 1.7688 | | 2.5280 | 3.0330 | H7 | 2.1265 | 1.0830 | 3.2747 | 1.9864 | 2.3995 | 2.5280 | | 1.7688 | H8 | 2.1391 | 1.0815 | 2.5618 | 1.9850 | 2.5280 | 3.0330 | 1.7688 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.545 |
|
C1 |
C2 |
H7 |
109.597 |
| C1 |
C2 |
H8 |
110.691 |
|
C2 |
C1 |
F3 |
110.545 |
| C2 |
C1 |
H5 |
109.597 |
|
C2 |
C1 |
H6 |
110.691 |
| F3 |
C1 |
H5 |
108.190 |
|
F3 |
C1 |
H6 |
108.164 |
| F4 |
C2 |
H7 |
108.190 |
|
F4 |
C2 |
H8 |
108.164 |
| H5 |
C1 |
H6 |
109.604 |
|
H7 |
C2 |
H8 |
109.604 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.178 |
|
|
|
| 2 |
C |
-0.178 |
|
|
|
| 3 |
F |
-0.932 |
|
|
|
| 4 |
F |
-0.932 |
|
|
|
| 5 |
H |
0.697 |
|
|
|
| 6 |
H |
0.413 |
|
|
|
| 7 |
H |
0.697 |
|
|
|
| 8 |
H |
0.413 |
|
|
|
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 |
2.889 |
2.889 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.579 |
1.807 |
0.000 |
| y |
1.807 |
-26.254 |
0.000 |
| z |
0.000 |
0.000 |
-22.434 |
|
| Traceless |
| | x | y | z |
| x |
2.764 |
1.807 |
0.000 |
| y |
1.807 |
-4.247 |
0.000 |
| z |
0.000 |
0.000 |
1.483 |
|
| Polar |
| 3z2-r2 | 2.966 |
| x2-y2 | 4.674 |
| xy | 1.807 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.823 |
0.036 |
0.000 |
| y |
0.036 |
4.087 |
0.000 |
| z |
0.000 |
0.000 |
3.947 |
<r2> (average value of r
2) Å
2
| <r2> |
78.375 |
| (<r2>)1/2 |
8.853 |