Jump to
S1C2
Energy calculated at B1B95/6-311G**
| hartrees |
Energy at 0K | -377.534034 |
Energy at 298.15K | |
HF Energy | -377.534034 |
Nuclear repulsion energy | 191.460785 |
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 B1B95/6-311G**
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 |
3154 |
3028 |
26.46 |
36.93 |
0.68 |
0.81 |
2 |
A |
3117 |
2993 |
27.52 |
98.26 |
0.33 |
0.50 |
3 |
A |
3087 |
2964 |
16.19 |
113.45 |
0.08 |
0.14 |
4 |
A |
1496 |
1436 |
2.91 |
6.98 |
0.74 |
0.85 |
5 |
A |
1469 |
1410 |
20.34 |
2.95 |
0.47 |
0.64 |
6 |
A |
1416 |
1360 |
22.73 |
4.63 |
0.73 |
0.85 |
7 |
A |
1348 |
1294 |
19.96 |
2.52 |
0.75 |
0.86 |
8 |
A |
1273 |
1223 |
13.51 |
7.51 |
0.73 |
0.84 |
9 |
A |
1178 |
1131 |
100.10 |
4.62 |
0.71 |
0.83 |
10 |
A |
1146 |
1100 |
21.46 |
2.06 |
0.57 |
0.72 |
11 |
A |
1136 |
1090 |
251.65 |
0.22 |
0.21 |
0.35 |
12 |
A |
1112 |
1068 |
18.07 |
5.24 |
0.52 |
0.68 |
13 |
A |
919 |
883 |
35.78 |
4.22 |
0.36 |
0.53 |
14 |
A |
582 |
559 |
4.42 |
1.89 |
0.45 |
0.62 |
15 |
A |
473 |
454 |
19.01 |
0.78 |
0.73 |
0.84 |
16 |
A |
428 |
411 |
5.97 |
1.60 |
0.54 |
0.70 |
17 |
A |
238 |
228 |
8.90 |
0.07 |
0.58 |
0.74 |
18 |
A |
115 |
110 |
8.40 |
0.02 |
0.67 |
0.80 |
Unscaled Zero Point Vibrational Energy (zpe) 11843.9 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 11371.3 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 B1B95/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.770 |
-0.586 |
-0.285 |
C2 |
0.465 |
0.021 |
0.327 |
F3 |
-1.874 |
0.107 |
0.152 |
F4 |
1.526 |
-0.759 |
-0.006 |
F5 |
0.679 |
1.256 |
-0.181 |
H6 |
-0.703 |
-0.516 |
-1.371 |
H7 |
-0.854 |
-1.628 |
0.024 |
H8 |
0.411 |
0.102 |
1.413 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5051 | 1.3741 | 2.3190 | 2.3454 | 1.0903 | 1.0901 | 2.1792 |
C2 | 1.5051 | | 2.3464 | 1.3582 | 1.3525 | 2.1287 | 2.1326 | 1.0906 | F3 | 1.3741 | 2.3464 | | 3.5116 | 2.8188 | 2.0194 | 2.0159 | 2.6096 | F4 | 2.3190 | 1.3582 | 3.5116 | | 2.1930 | 2.6242 | 2.5338 | 1.9994 | F5 | 2.3454 | 1.3525 | 2.8188 | 2.1930 | | 2.5425 | 3.2722 | 1.9857 | H6 | 1.0903 | 2.1287 | 2.0194 | 2.6242 | 2.5425 | | 1.7898 | 3.0610 | H7 | 1.0901 | 2.1326 | 2.0159 | 2.5338 | 3.2722 | 1.7898 | | 2.5537 | H8 | 2.1792 | 1.0906 | 2.6096 | 1.9994 | 1.9857 | 3.0610 | 2.5537 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.065 |
|
C1 |
C2 |
F5 |
110.204 |
C1 |
C2 |
H8 |
113.214 |
|
C2 |
C1 |
F3 |
109.080 |
C2 |
C1 |
H6 |
109.158 |
|
C2 |
C1 |
H7 |
109.484 |
F3 |
C1 |
H6 |
109.513 |
|
F3 |
C1 |
H7 |
109.241 |
F4 |
C2 |
F5 |
107.994 |
|
F4 |
C2 |
H8 |
108.976 |
F5 |
C2 |
H8 |
108.259 |
|
H6 |
C1 |
H7 |
110.344 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.022 |
|
|
|
2 |
C |
0.324 |
|
|
|
3 |
F |
-0.260 |
|
|
|
4 |
F |
-0.237 |
|
|
|
5 |
F |
-0.226 |
|
|
|
6 |
H |
0.133 |
|
|
|
7 |
H |
0.126 |
|
|
|
8 |
H |
0.117 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.250 |
-1.450 |
0.373 |
1.518 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.102 |
1.552 |
1.374 |
y |
1.552 |
-27.568 |
0.499 |
z |
1.374 |
0.499 |
-24.509 |
|
Traceless |
| x | y | z |
x |
-6.063 |
1.552 |
1.374 |
y |
1.552 |
0.737 |
0.499 |
z |
1.374 |
0.499 |
5.326 |
|
Polar |
3z2-r2 | 10.652 |
x2-y2 | -4.534 |
xy | 1.552 |
xz | 1.374 |
yz | 0.499 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.533 |
-0.018 |
0.026 |
y |
-0.018 |
3.535 |
0.059 |
z |
0.026 |
0.059 |
3.437 |
<r2> (average value of r
2) Å
2
<r2> |
110.441 |
(<r2>)1/2 |
10.509 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| hartrees |
Energy at 0K | -377.531408 |
Energy at 298.15K | |
HF Energy | -377.531408 |
Nuclear repulsion energy | 194.315555 |
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 B1B95/6-311G**
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' |
3092 |
2968 |
61.42 |
124.37 |
0.06 |
0.11 |
2 |
A' |
3075 |
2952 |
4.70 |
65.38 |
0.36 |
0.53 |
3 |
A' |
1491 |
1432 |
7.26 |
5.89 |
0.75 |
0.85 |
4 |
A' |
1447 |
1389 |
30.91 |
2.98 |
0.34 |
0.51 |
5 |
A' |
1418 |
1361 |
21.50 |
2.85 |
0.73 |
0.84 |
6 |
A' |
1202 |
1154 |
132.85 |
4.03 |
0.43 |
0.60 |
7 |
A' |
1124 |
1079 |
25.12 |
2.96 |
0.74 |
0.85 |
8 |
A' |
888 |
853 |
34.06 |
5.92 |
0.18 |
0.31 |
9 |
A' |
768 |
737 |
53.73 |
2.61 |
0.59 |
0.74 |
10 |
A' |
520 |
499 |
13.24 |
1.60 |
0.75 |
0.86 |
11 |
A' |
225 |
216 |
2.06 |
0.14 |
0.45 |
0.62 |
12 |
A" |
3137 |
3012 |
20.55 |
53.91 |
0.75 |
0.86 |
13 |
A" |
1406 |
1350 |
31.61 |
1.77 |
0.75 |
0.86 |
14 |
A" |
1292 |
1240 |
18.07 |
13.22 |
0.75 |
0.86 |
15 |
A" |
1157 |
1111 |
117.86 |
1.19 |
0.75 |
0.86 |
16 |
A" |
962 |
924 |
62.95 |
2.79 |
0.75 |
0.86 |
17 |
A" |
366 |
351 |
0.15 |
0.26 |
0.75 |
0.86 |
18 |
A" |
107 |
103 |
2.10 |
0.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11838.2 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 11365.9 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.737 |
-0.828 |
0.000 |
C2 |
0.356 |
0.627 |
0.000 |
F3 |
-0.387 |
-1.612 |
0.000 |
F4 |
-0.387 |
0.918 |
1.094 |
F5 |
-0.387 |
0.918 |
-1.094 |
H6 |
1.324 |
-1.045 |
-0.894 |
H7 |
1.324 |
-1.045 |
0.894 |
H8 |
1.239 |
1.272 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5040 | 1.3696 | 2.3472 | 2.3472 | 1.0912 | 1.0912 | 2.1597 |
C2 | 1.5040 | | 2.3584 | 1.3540 | 1.3540 | 2.1285 | 2.1285 | 1.0933 | F3 | 1.3696 | 2.3584 | | 2.7562 | 2.7562 | 2.0118 | 2.0118 | 3.3103 | F4 | 2.3472 | 1.3540 | 2.7562 | | 2.1874 | 3.2760 | 2.6120 | 1.9908 | F5 | 2.3472 | 1.3540 | 2.7562 | 2.1874 | | 2.6120 | 3.2760 | 1.9908 | H6 | 1.0912 | 2.1285 | 2.0118 | 3.2760 | 2.6120 | | 1.7874 | 2.4851 | H7 | 1.0912 | 2.1285 | 2.0118 | 2.6120 | 3.2760 | 1.7874 | | 2.4851 | H8 | 2.1597 | 1.0933 | 3.3103 | 1.9908 | 1.9908 | 2.4851 | 2.4851 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.318 |
|
C1 |
C2 |
F5 |
110.318 |
C1 |
C2 |
H8 |
111.531 |
|
C2 |
C1 |
F3 |
110.221 |
C2 |
C1 |
H6 |
109.171 |
|
C2 |
C1 |
H7 |
109.171 |
F3 |
C1 |
H6 |
109.151 |
|
F3 |
C1 |
H7 |
109.151 |
F4 |
C2 |
F5 |
107.755 |
|
F4 |
C2 |
H8 |
108.405 |
F5 |
C2 |
H8 |
108.405 |
|
H6 |
C1 |
H7 |
109.966 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.033 |
|
|
|
2 |
C |
0.328 |
|
|
|
3 |
F |
-0.252 |
|
|
|
4 |
F |
-0.229 |
|
|
|
5 |
F |
-0.229 |
|
|
|
6 |
H |
0.123 |
|
|
|
7 |
H |
0.123 |
|
|
|
8 |
H |
0.102 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
3.153 |
0.091 |
0.000 |
3.154 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.894 |
-0.287 |
0.000 |
y |
-0.287 |
-28.563 |
0.000 |
z |
0.000 |
0.000 |
-28.245 |
|
Traceless |
| x | y | z |
x |
3.510 |
-0.287 |
0.000 |
y |
-0.287 |
-1.994 |
0.000 |
z |
0.000 |
0.000 |
-1.516 |
|
Polar |
3z2-r2 | -3.033 |
x2-y2 | 3.669 |
xy | -0.287 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.508 |
0.001 |
0.000 |
y |
0.001 |
3.516 |
0.000 |
z |
0.000 |
0.000 |
3.497 |
<r2> (average value of r
2) Å
2
<r2> |
102.068 |
(<r2>)1/2 |
10.103 |