Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -377.296267 |
Energy at 298.15K | |
HF Energy | -377.296267 |
Nuclear repulsion energy | 191.125752 |
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 HSEh1PBE/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 |
3143 |
3019 |
26.49 |
37.29 |
0.67 |
0.80 |
2 |
A |
3106 |
2983 |
28.06 |
98.63 |
0.33 |
0.50 |
3 |
A |
3077 |
2955 |
16.16 |
114.88 |
0.08 |
0.14 |
4 |
A |
1492 |
1433 |
2.94 |
7.00 |
0.74 |
0.85 |
5 |
A |
1466 |
1408 |
20.54 |
3.07 |
0.47 |
0.64 |
6 |
A |
1414 |
1358 |
21.79 |
4.64 |
0.73 |
0.85 |
7 |
A |
1347 |
1293 |
18.53 |
2.57 |
0.75 |
0.86 |
8 |
A |
1271 |
1221 |
12.55 |
7.53 |
0.73 |
0.85 |
9 |
A |
1174 |
1128 |
97.95 |
4.61 |
0.71 |
0.83 |
10 |
A |
1145 |
1100 |
11.52 |
1.76 |
0.51 |
0.68 |
11 |
A |
1131 |
1086 |
260.47 |
0.25 |
0.37 |
0.54 |
12 |
A |
1108 |
1064 |
18.43 |
5.35 |
0.54 |
0.70 |
13 |
A |
918 |
882 |
36.62 |
4.12 |
0.36 |
0.53 |
14 |
A |
583 |
560 |
4.26 |
1.91 |
0.45 |
0.62 |
15 |
A |
477 |
458 |
19.02 |
0.79 |
0.73 |
0.85 |
16 |
A |
430 |
413 |
5.61 |
1.62 |
0.54 |
0.70 |
17 |
A |
242 |
233 |
8.62 |
0.07 |
0.58 |
0.74 |
18 |
A |
117 |
112 |
8.27 |
0.02 |
0.67 |
0.80 |
Unscaled Zero Point Vibrational Energy (zpe) 11820.2 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 11352.1 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 HSEh1PBE/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.772 |
-0.585 |
-0.285 |
C2 |
0.465 |
0.021 |
0.327 |
F3 |
-1.878 |
0.108 |
0.152 |
F4 |
1.527 |
-0.762 |
-0.006 |
F5 |
0.682 |
1.258 |
-0.181 |
H6 |
-0.704 |
-0.517 |
-1.374 |
H7 |
-0.856 |
-1.630 |
0.025 |
H8 |
0.411 |
0.102 |
1.416 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5071 | 1.3761 | 2.3226 | 2.3499 | 1.0933 | 1.0930 | 2.1825 |
C2 | 1.5071 | | 2.3510 | 1.3604 | 1.3547 | 2.1329 | 2.1360 | 1.0936 | F3 | 1.3761 | 2.3510 | | 3.5177 | 2.8257 | 2.0233 | 2.0200 | 2.6146 | F4 | 2.3226 | 1.3604 | 3.5177 | | 2.1961 | 2.6288 | 2.5370 | 2.0035 | F5 | 2.3499 | 1.3547 | 2.8257 | 2.1961 | | 2.5489 | 3.2786 | 1.9898 | H6 | 1.0933 | 2.1329 | 2.0233 | 2.6288 | 2.5489 | | 1.7937 | 3.0675 | H7 | 1.0930 | 2.1360 | 2.0200 | 2.5370 | 3.2786 | 1.7937 | | 2.5574 | H8 | 2.1825 | 1.0936 | 2.6146 | 2.0035 | 1.9898 | 3.0675 | 2.5574 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.079 |
|
C1 |
C2 |
F5 |
110.278 |
C1 |
C2 |
H8 |
113.149 |
|
C2 |
C1 |
F3 |
109.172 |
C2 |
C1 |
H6 |
109.181 |
|
C2 |
C1 |
H7 |
109.442 |
F3 |
C1 |
H6 |
109.507 |
|
F3 |
C1 |
H7 |
109.259 |
F4 |
C2 |
F5 |
107.970 |
|
F4 |
C2 |
H8 |
108.978 |
F5 |
C2 |
H8 |
108.259 |
|
H6 |
C1 |
H7 |
110.262 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.023 |
|
|
|
2 |
C |
0.327 |
|
|
|
3 |
F |
-0.259 |
|
|
|
4 |
F |
-0.236 |
|
|
|
5 |
F |
-0.225 |
|
|
|
6 |
H |
0.130 |
|
|
|
7 |
H |
0.125 |
|
|
|
8 |
H |
0.114 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.246 |
-1.434 |
0.369 |
1.501 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.137 |
1.530 |
1.351 |
y |
1.530 |
-27.629 |
0.490 |
z |
1.351 |
0.490 |
-24.597 |
|
Traceless |
| x | y | z |
x |
-6.024 |
1.530 |
1.351 |
y |
1.530 |
0.738 |
0.490 |
z |
1.351 |
0.490 |
5.286 |
|
Polar |
3z2-r2 | 10.571 |
x2-y2 | -4.508 |
xy | 1.530 |
xz | 1.351 |
yz | 0.490 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.554 |
-0.019 |
0.027 |
y |
-0.019 |
3.557 |
0.061 |
z |
0.027 |
0.061 |
3.459 |
<r2> (average value of r
2) Å
2
<r2> |
110.823 |
(<r2>)1/2 |
10.527 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -377.293640 |
Energy at 298.15K | |
HF Energy | -377.293640 |
Nuclear repulsion energy | 193.890054 |
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 HSEh1PBE/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' |
3081 |
2959 |
62.40 |
127.63 |
0.05 |
0.10 |
2 |
A' |
3064 |
2943 |
4.30 |
63.34 |
0.39 |
0.56 |
3 |
A' |
1487 |
1428 |
7.71 |
5.86 |
0.75 |
0.85 |
4 |
A' |
1444 |
1387 |
30.63 |
3.07 |
0.34 |
0.51 |
5 |
A' |
1416 |
1360 |
20.20 |
2.93 |
0.72 |
0.84 |
6 |
A' |
1199 |
1151 |
130.96 |
3.91 |
0.42 |
0.59 |
7 |
A' |
1119 |
1075 |
25.09 |
3.05 |
0.74 |
0.85 |
8 |
A' |
887 |
851 |
35.01 |
5.68 |
0.18 |
0.31 |
9 |
A' |
769 |
738 |
53.41 |
2.63 |
0.58 |
0.74 |
10 |
A' |
521 |
501 |
12.76 |
1.62 |
0.75 |
0.86 |
11 |
A' |
232 |
223 |
1.98 |
0.15 |
0.44 |
0.61 |
12 |
A" |
3126 |
3002 |
20.35 |
54.20 |
0.75 |
0.86 |
13 |
A" |
1403 |
1347 |
30.20 |
1.81 |
0.75 |
0.86 |
14 |
A" |
1289 |
1238 |
17.34 |
13.22 |
0.75 |
0.86 |
15 |
A" |
1152 |
1107 |
115.93 |
1.23 |
0.75 |
0.86 |
16 |
A" |
960 |
922 |
65.05 |
2.75 |
0.75 |
0.86 |
17 |
A" |
370 |
355 |
0.16 |
0.27 |
0.75 |
0.86 |
18 |
A" |
112 |
108 |
2.04 |
0.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11815.1 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 11347.2 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.736 |
-0.830 |
0.000 |
C2 |
0.356 |
0.627 |
0.000 |
F3 |
-0.387 |
-1.618 |
0.000 |
F4 |
-0.387 |
0.922 |
1.096 |
F5 |
-0.387 |
0.922 |
-1.096 |
H6 |
1.326 |
-1.046 |
-0.896 |
H7 |
1.326 |
-1.046 |
0.896 |
H8 |
1.243 |
1.271 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5061 | 1.3720 | 2.3520 | 2.3520 | 1.0942 | 1.0942 | 2.1615 |
C2 | 1.5061 | | 2.3651 | 1.3562 | 1.3562 | 2.1316 | 2.1316 | 1.0963 | F3 | 1.3720 | 2.3651 | | 2.7666 | 2.7666 | 2.0161 | 2.0161 | 3.3175 | F4 | 2.3520 | 1.3562 | 2.7666 | | 2.1913 | 3.2825 | 2.6171 | 1.9949 | F5 | 2.3520 | 1.3562 | 2.7666 | 2.1913 | | 2.6171 | 3.2825 | 1.9949 | H6 | 1.0942 | 2.1316 | 2.0161 | 3.2825 | 2.6171 | | 1.7914 | 2.4857 | H7 | 1.0942 | 2.1316 | 2.0161 | 2.6171 | 3.2825 | 1.7914 | | 2.4857 | H8 | 2.1615 | 1.0963 | 3.3175 | 1.9949 | 1.9949 | 2.4857 | 2.4857 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.409 |
|
C1 |
C2 |
F5 |
110.409 |
C1 |
C2 |
H8 |
111.345 |
|
C2 |
C1 |
F3 |
110.442 |
C2 |
C1 |
H6 |
109.098 |
|
C2 |
C1 |
H7 |
109.098 |
F3 |
C1 |
H6 |
109.150 |
|
F3 |
C1 |
H7 |
109.150 |
F4 |
C2 |
F5 |
107.777 |
|
F4 |
C2 |
H8 |
108.397 |
F5 |
C2 |
H8 |
108.397 |
|
H6 |
C1 |
H7 |
109.893 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.034 |
|
|
|
2 |
C |
0.331 |
|
|
|
3 |
F |
-0.251 |
|
|
|
4 |
F |
-0.228 |
|
|
|
5 |
F |
-0.228 |
|
|
|
6 |
H |
0.121 |
|
|
|
7 |
H |
0.121 |
|
|
|
8 |
H |
0.099 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
3.115 |
0.089 |
0.000 |
3.116 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.972 |
-0.281 |
0.000 |
y |
-0.281 |
-28.663 |
0.000 |
z |
0.000 |
0.000 |
-28.295 |
|
Traceless |
| x | y | z |
x |
3.508 |
-0.281 |
0.000 |
y |
-0.281 |
-2.030 |
0.000 |
z |
0.000 |
0.000 |
-1.478 |
|
Polar |
3z2-r2 | -2.956 |
x2-y2 | 3.691 |
xy | -0.281 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.531 |
0.004 |
0.000 |
y |
0.004 |
3.536 |
0.000 |
z |
0.000 |
0.000 |
3.518 |
<r2> (average value of r
2) Å
2
<r2> |
102.562 |
(<r2>)1/2 |
10.127 |