Jump to
S1C2
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -278.057399 |
Energy at 298.15K | |
HF Energy | -277.847221 |
Nuclear repulsion energy | 125.338597 |
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 B2PLYP/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 |
Ag |
3079 |
2949 |
0.00 |
229.99 |
0.08 |
0.15 |
2 |
Ag |
1510 |
1446 |
0.00 |
19.22 |
0.73 |
0.85 |
3 |
Ag |
1458 |
1396 |
0.00 |
3.50 |
0.40 |
0.57 |
4 |
Ag |
1106 |
1059 |
0.00 |
8.96 |
0.52 |
0.69 |
5 |
Ag |
1077 |
1031 |
0.00 |
7.40 |
0.51 |
0.67 |
6 |
Ag |
460 |
440 |
0.00 |
3.01 |
0.51 |
0.68 |
7 |
Au |
3154 |
3020 |
65.00 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1227 |
1175 |
3.78 |
0.00 |
0.00 |
0.00 |
9 |
Au |
822 |
787 |
0.03 |
0.00 |
0.00 |
0.00 |
10 |
Au |
122 |
117 |
12.50 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3128 |
2996 |
0.00 |
140.68 |
0.75 |
0.86 |
12 |
Bg |
1298 |
1243 |
0.00 |
13.71 |
0.75 |
0.86 |
13 |
Bg |
1178 |
1128 |
0.00 |
5.29 |
0.75 |
0.86 |
14 |
Bu |
3082 |
2952 |
63.84 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1520 |
1455 |
1.39 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1356 |
1299 |
16.35 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1089 |
1043 |
194.12 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
273 |
262 |
18.17 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13469.5 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 12899.8 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 B2PLYP/cc-pVDZ
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.425 |
0.628 |
0.000 |
C2 |
-0.425 |
-0.628 |
0.000 |
F3 |
-0.425 |
1.728 |
0.000 |
F4 |
0.425 |
-1.728 |
0.000 |
H5 |
1.062 |
0.665 |
0.897 |
H6 |
1.062 |
0.665 |
-0.897 |
H7 |
-1.062 |
-0.665 |
0.897 |
H8 |
-1.062 |
-0.665 |
-0.897 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5168 | 1.3894 | 2.3564 | 1.1011 | 1.1011 | 2.1651 | 2.1651 |
C2 | 1.5168 | | 2.3564 | 1.3894 | 2.1651 | 2.1651 | 1.1011 | 1.1011 | F3 | 1.3894 | 2.3564 | | 3.5588 | 2.0357 | 2.0357 | 2.6340 | 2.6340 | F4 | 2.3564 | 1.3894 | 3.5588 | | 2.6340 | 2.6340 | 2.0357 | 2.0357 | H5 | 1.1011 | 2.1651 | 2.0357 | 2.6340 | | 1.7944 | 2.5059 | 3.0821 | H6 | 1.1011 | 2.1651 | 2.0357 | 2.6340 | 1.7944 | | 3.0821 | 2.5059 | H7 | 2.1651 | 1.1011 | 2.6340 | 2.0357 | 2.5059 | 3.0821 | | 1.7944 | H8 | 2.1651 | 1.1011 | 2.6340 | 2.0357 | 3.0821 | 2.5059 | 1.7944 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.275 |
|
C1 |
C2 |
H7 |
110.588 |
C1 |
C2 |
H8 |
110.588 |
|
C2 |
C1 |
F3 |
108.275 |
C2 |
C1 |
H5 |
110.588 |
|
C2 |
C1 |
H6 |
110.588 |
F3 |
C1 |
H5 |
109.108 |
|
F3 |
C1 |
H6 |
109.108 |
F4 |
C2 |
H7 |
109.108 |
|
F4 |
C2 |
H8 |
109.108 |
H5 |
C1 |
H6 |
109.141 |
|
H7 |
C2 |
H8 |
109.141 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.195 |
|
|
|
2 |
C |
0.195 |
|
|
|
3 |
F |
-0.261 |
|
|
|
4 |
F |
-0.261 |
|
|
|
5 |
H |
0.033 |
|
|
|
6 |
H |
0.033 |
|
|
|
7 |
H |
0.033 |
|
|
|
8 |
H |
0.033 |
|
|
|
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 |
-21.895 |
2.614 |
0.000 |
y |
2.614 |
-28.702 |
0.000 |
z |
0.000 |
0.000 |
-21.520 |
|
Traceless |
| x | y | z |
x |
3.216 |
2.614 |
0.000 |
y |
2.614 |
-6.995 |
0.000 |
z |
0.000 |
0.000 |
3.779 |
|
Polar |
3z2-r2 | 7.558 |
x2-y2 | 6.807 |
xy | 2.614 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.572 |
0.028 |
0.000 |
y |
0.028 |
3.518 |
0.000 |
z |
0.000 |
0.000 |
3.349 |
<r2> (average value of r
2) Å
2
<r2> |
88.409 |
(<r2>)1/2 |
9.403 |
Jump to
S1C1
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -278.057963 |
Energy at 298.15K | |
HF Energy | -277.847505 |
Nuclear repulsion energy | 127.401840 |
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 B2PLYP/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 |
3122 |
2990 |
21.62 |
110.14 |
0.74 |
0.85 |
2 |
A |
3071 |
2941 |
38.78 |
197.50 |
0.02 |
0.05 |
3 |
A |
1485 |
1422 |
0.34 |
1.90 |
0.69 |
0.81 |
4 |
A |
1450 |
1389 |
18.93 |
3.59 |
0.39 |
0.56 |
5 |
A |
1305 |
1250 |
1.66 |
17.84 |
0.71 |
0.83 |
6 |
A |
1136 |
1088 |
34.10 |
3.37 |
0.62 |
0.77 |
7 |
A |
1131 |
1083 |
46.58 |
2.29 |
0.51 |
0.68 |
8 |
A |
883 |
846 |
28.45 |
5.33 |
0.26 |
0.41 |
9 |
A |
322 |
309 |
0.27 |
0.34 |
0.43 |
0.60 |
10 |
A |
148 |
142 |
3.46 |
0.06 |
0.75 |
0.86 |
11 |
B |
3135 |
3002 |
48.46 |
15.24 |
0.75 |
0.86 |
12 |
B |
3059 |
2929 |
15.40 |
41.22 |
0.75 |
0.86 |
13 |
B |
1481 |
1418 |
6.45 |
14.75 |
0.75 |
0.86 |
14 |
B |
1407 |
1347 |
13.16 |
0.81 |
0.75 |
0.86 |
15 |
B |
1260 |
1207 |
6.12 |
5.10 |
0.75 |
0.86 |
16 |
B |
1097 |
1050 |
45.41 |
3.59 |
0.75 |
0.86 |
17 |
B |
911 |
873 |
40.01 |
3.43 |
0.75 |
0.86 |
18 |
B |
492 |
471 |
15.56 |
0.65 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13447.6 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 12878.8 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 B2PLYP/cc-pVDZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.267 |
0.704 |
0.510 |
C2 |
-0.267 |
-0.704 |
0.510 |
F3 |
-0.267 |
1.428 |
-0.547 |
F4 |
0.267 |
-1.428 |
-0.547 |
H5 |
-0.010 |
1.204 |
1.454 |
H6 |
1.364 |
0.694 |
0.410 |
H7 |
0.010 |
-1.204 |
1.454 |
H8 |
-1.364 |
-0.694 |
0.410 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5058 | 1.3877 | 2.3795 | 1.1032 | 1.1017 | 2.1439 | 2.1504 |
C2 | 1.5058 | | 2.3795 | 1.3877 | 2.1439 | 2.1504 | 1.1032 | 1.1017 | F3 | 1.3877 | 2.3795 | | 2.9047 | 2.0300 | 2.0279 | 3.3173 | 2.5734 | F4 | 2.3795 | 1.3877 | 2.9047 | | 3.3173 | 2.5734 | 2.0300 | 2.0279 | H5 | 1.1032 | 2.1439 | 2.0300 | 3.3173 | | 1.7990 | 2.4072 | 2.5545 | H6 | 1.1017 | 2.1504 | 2.0279 | 2.5734 | 1.7990 | | 2.5545 | 3.0608 | H7 | 2.1439 | 1.1032 | 3.3173 | 2.0300 | 2.4072 | 2.5545 | | 1.7990 | H8 | 2.1504 | 1.1017 | 2.5734 | 2.0279 | 2.5545 | 3.0608 | 1.7990 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.574 |
|
C1 |
C2 |
H7 |
109.547 |
C1 |
C2 |
H8 |
110.149 |
|
C2 |
C1 |
F3 |
110.574 |
C2 |
C1 |
H5 |
109.547 |
|
C2 |
C1 |
H6 |
110.149 |
F3 |
C1 |
H5 |
108.630 |
|
F3 |
C1 |
H6 |
108.550 |
F4 |
C2 |
H7 |
108.630 |
|
F4 |
C2 |
H8 |
108.550 |
H5 |
C1 |
H6 |
109.359 |
|
H7 |
C2 |
H8 |
109.359 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.204 |
|
|
|
2 |
C |
0.204 |
|
|
|
3 |
F |
-0.258 |
|
|
|
4 |
F |
-0.258 |
|
|
|
5 |
H |
0.019 |
|
|
|
6 |
H |
0.035 |
|
|
|
7 |
H |
0.019 |
|
|
|
8 |
H |
0.035 |
|
|
|
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 |
2.528 |
2.528 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.625 |
1.456 |
0.000 |
y |
1.456 |
-25.952 |
0.000 |
z |
0.000 |
0.000 |
-22.124 |
|
Traceless |
| x | y | z |
x |
2.413 |
1.456 |
0.000 |
y |
1.456 |
-4.078 |
0.000 |
z |
0.000 |
0.000 |
1.665 |
|
Polar |
3z2-r2 | 3.329 |
x2-y2 | 4.327 |
xy | 1.456 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.451 |
0.057 |
0.000 |
y |
0.057 |
3.602 |
0.000 |
z |
0.000 |
0.000 |
3.509 |
<r2> (average value of r
2) Å
2
<r2> |
79.941 |
(<r2>)1/2 |
8.941 |