Jump to
S1C2
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -278.309247 |
| Energy at 298.15K | |
| HF Energy | -278.309247 |
| Nuclear repulsion energy | 126.063045 |
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 B1B95/TZVP
| 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 |
3082 |
2949 |
0.00 |
239.23 |
0.07 |
0.14 |
| 2 |
Ag |
1519 |
1453 |
0.00 |
14.01 |
0.74 |
0.85 |
| 3 |
Ag |
1465 |
1402 |
0.00 |
3.12 |
0.59 |
0.75 |
| 4 |
Ag |
1099 |
1052 |
0.00 |
8.36 |
0.62 |
0.76 |
| 5 |
Ag |
1085 |
1038 |
0.00 |
7.13 |
0.41 |
0.58 |
| 6 |
Ag |
462 |
442 |
0.00 |
3.24 |
0.49 |
0.66 |
| 7 |
Au |
3157 |
3021 |
46.78 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1249 |
1195 |
4.04 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
822 |
787 |
0.00 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
116 |
111 |
14.54 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3130 |
2995 |
0.00 |
123.01 |
0.75 |
0.86 |
| 12 |
Bg |
1308 |
1251 |
0.00 |
16.29 |
0.75 |
0.86 |
| 13 |
Bg |
1184 |
1133 |
0.00 |
3.29 |
0.75 |
0.86 |
| 14 |
Bu |
3089 |
2956 |
56.74 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1529 |
1463 |
4.20 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1374 |
1315 |
9.51 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1095 |
1048 |
222.79 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
278 |
266 |
21.00 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13520.4 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 12937.7 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 B1B95/TZVP
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.422 |
0.626 |
0.000 |
| C2 |
-0.422 |
-0.626 |
0.000 |
| F3 |
-0.422 |
1.720 |
0.000 |
| F4 |
0.422 |
-1.720 |
0.000 |
| H5 |
1.049 |
0.670 |
0.890 |
| H6 |
1.049 |
0.670 |
-0.890 |
| H7 |
-1.049 |
-0.670 |
0.890 |
| H8 |
-1.049 |
-0.670 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5102 | 1.3820 | 2.3461 | 1.0893 | 1.0893 | 2.1533 | 2.1533 |
C2 | 1.5102 | | 2.3461 | 1.3820 | 2.1533 | 2.1533 | 1.0893 | 1.0893 | F3 | 1.3820 | 2.3461 | | 3.5422 | 2.0146 | 2.0146 | 2.6264 | 2.6264 | F4 | 2.3461 | 1.3820 | 3.5422 | | 2.6264 | 2.6264 | 2.0146 | 2.0146 | H5 | 1.0893 | 2.1533 | 2.0146 | 2.6264 | | 1.7794 | 2.4899 | 3.0604 | H6 | 1.0893 | 2.1533 | 2.0146 | 2.6264 | 1.7794 | | 3.0604 | 2.4899 | H7 | 2.1533 | 1.0893 | 2.6264 | 2.0146 | 2.4899 | 3.0604 | | 1.7794 | H8 | 2.1533 | 1.0893 | 2.6264 | 2.0146 | 3.0604 | 2.4899 | 1.7794 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.345 |
|
C1 |
C2 |
H7 |
110.820 |
| C1 |
C2 |
H8 |
110.820 |
|
C2 |
C1 |
F3 |
108.345 |
| C2 |
C1 |
H5 |
110.820 |
|
C2 |
C1 |
H6 |
110.820 |
| F3 |
C1 |
H5 |
108.636 |
|
F3 |
C1 |
H6 |
108.636 |
| F4 |
C2 |
H7 |
108.636 |
|
F4 |
C2 |
H8 |
108.636 |
| H5 |
C1 |
H6 |
109.522 |
|
H7 |
C2 |
H8 |
109.522 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.003 |
|
|
|
| 2 |
C |
0.003 |
|
|
|
| 3 |
F |
-0.240 |
|
|
|
| 4 |
F |
-0.240 |
|
|
|
| 5 |
H |
0.118 |
|
|
|
| 6 |
H |
0.118 |
|
|
|
| 7 |
H |
0.118 |
|
|
|
| 8 |
H |
0.118 |
|
|
|
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 |
-22.072 |
3.222 |
0.000 |
| y |
3.222 |
-29.568 |
0.000 |
| z |
0.000 |
0.000 |
-21.467 |
|
| Traceless |
| | x | y | z |
| x |
3.446 |
3.222 |
0.000 |
| y |
3.222 |
-7.798 |
0.000 |
| z |
0.000 |
0.000 |
4.353 |
|
| Polar |
| 3z2-r2 | 8.705 |
| x2-y2 | 7.496 |
| xy | 3.222 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.835 |
-0.013 |
0.000 |
| y |
-0.013 |
3.895 |
0.000 |
| z |
0.000 |
0.000 |
3.599 |
<r2> (average value of r
2) Å
2
| <r2> |
87.891 |
| (<r2>)1/2 |
9.375 |
Jump to
S1C1
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -278.310666 |
| Energy at 298.15K | |
| HF Energy | -278.310666 |
| Nuclear repulsion energy | 128.048683 |
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 B1B95/TZVP
| 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 |
3123 |
2989 |
15.14 |
97.17 |
0.74 |
0.85 |
| 2 |
A |
3075 |
2943 |
34.69 |
216.33 |
0.02 |
0.04 |
| 3 |
A |
1492 |
1428 |
0.01 |
1.73 |
0.64 |
0.78 |
| 4 |
A |
1452 |
1389 |
16.41 |
3.62 |
0.55 |
0.71 |
| 5 |
A |
1318 |
1261 |
2.30 |
17.04 |
0.72 |
0.84 |
| 6 |
A |
1137 |
1088 |
51.04 |
2.33 |
0.33 |
0.49 |
| 7 |
A |
1133 |
1084 |
45.44 |
2.80 |
0.71 |
0.83 |
| 8 |
A |
880 |
842 |
26.77 |
4.73 |
0.27 |
0.42 |
| 9 |
A |
325 |
311 |
0.29 |
0.55 |
0.34 |
0.51 |
| 10 |
A |
153 |
146 |
4.29 |
0.12 |
0.67 |
0.80 |
| 11 |
B |
3137 |
3001 |
34.79 |
12.46 |
0.75 |
0.86 |
| 12 |
B |
3066 |
2933 |
9.51 |
38.13 |
0.75 |
0.86 |
| 13 |
B |
1490 |
1425 |
10.16 |
10.93 |
0.75 |
0.86 |
| 14 |
B |
1411 |
1350 |
9.45 |
1.26 |
0.75 |
0.86 |
| 15 |
B |
1275 |
1220 |
4.90 |
4.70 |
0.75 |
0.86 |
| 16 |
B |
1106 |
1058 |
62.07 |
3.81 |
0.75 |
0.86 |
| 17 |
B |
913 |
873 |
43.06 |
3.46 |
0.75 |
0.86 |
| 18 |
B |
497 |
475 |
16.59 |
0.66 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13490.3 cm
-1
Scaled (by 0.9569) Zero Point Vibrational Energy (zpe) 12908.9 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 B1B95/TZVP
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.266 |
0.700 |
0.503 |
| C2 |
-0.266 |
-0.700 |
0.503 |
| F3 |
-0.266 |
1.432 |
-0.539 |
| F4 |
0.266 |
-1.432 |
-0.539 |
| H5 |
-0.009 |
1.190 |
1.439 |
| H6 |
1.351 |
0.696 |
0.399 |
| H7 |
0.009 |
-1.190 |
1.439 |
| H8 |
-1.351 |
-0.696 |
0.399 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4968 | 1.3799 | 2.3723 | 1.0918 | 1.0901 | 2.1244 | 2.1385 |
C2 | 1.4968 | | 2.3723 | 1.3799 | 2.1244 | 2.1385 | 1.0918 | 1.0901 | F3 | 1.3799 | 2.3723 | | 2.9119 | 2.0094 | 2.0082 | 3.2956 | 2.5662 | F4 | 2.3723 | 1.3799 | 2.9119 | | 3.2956 | 2.5662 | 2.0094 | 2.0082 | H5 | 1.0918 | 2.1244 | 2.0094 | 3.2956 | | 1.7816 | 2.3800 | 2.5381 | H6 | 1.0901 | 2.1385 | 2.0082 | 2.5662 | 1.7816 | | 2.5381 | 3.0395 | H7 | 2.1244 | 1.0918 | 3.2956 | 2.0094 | 2.3800 | 2.5381 | | 1.7816 | H8 | 2.1385 | 1.0901 | 2.5662 | 2.0082 | 2.5381 | 3.0395 | 1.7816 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
111.045 |
|
C1 |
C2 |
H7 |
109.305 |
| C1 |
C2 |
H8 |
110.530 |
|
C2 |
C1 |
F3 |
111.045 |
| C2 |
C1 |
H5 |
109.305 |
|
C2 |
C1 |
H6 |
110.530 |
| F3 |
C1 |
H5 |
108.209 |
|
F3 |
C1 |
H6 |
108.222 |
| F4 |
C2 |
H7 |
108.209 |
|
F4 |
C2 |
H8 |
108.222 |
| H5 |
C1 |
H6 |
109.483 |
|
H7 |
C2 |
H8 |
109.483 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.008 |
|
|
|
| 2 |
C |
0.008 |
|
|
|
| 3 |
F |
-0.233 |
|
|
|
| 4 |
F |
-0.233 |
|
|
|
| 5 |
H |
0.104 |
|
|
|
| 6 |
H |
0.122 |
|
|
|
| 7 |
H |
0.104 |
|
|
|
| 8 |
H |
0.122 |
|
|
|
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 |
2.839 |
2.839 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.670 |
1.769 |
0.000 |
| y |
1.769 |
-26.435 |
0.000 |
| z |
0.000 |
0.000 |
-22.375 |
|
| Traceless |
| | x | y | z |
| x |
2.735 |
1.769 |
0.000 |
| y |
1.769 |
-4.412 |
0.000 |
| z |
0.000 |
0.000 |
1.677 |
|
| Polar |
| 3z2-r2 | 3.354 |
| x2-y2 | 4.765 |
| xy | 1.769 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.715 |
0.031 |
0.000 |
| y |
0.031 |
3.918 |
0.000 |
| z |
0.000 |
0.000 |
3.818 |
<r2> (average value of r
2) Å
2
| <r2> |
79.732 |
| (<r2>)1/2 |
8.929 |