Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/cc-pVDZ
| hartrees |
Energy at 0K | -377.246899 |
Energy at 298.15K | |
HF Energy | -376.976080 |
Nuclear repulsion energy | 190.274570 |
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=FULLultrafine/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 |
3159 |
3027 |
30.18 |
41.98 |
0.70 |
0.83 |
2 |
A |
3119 |
2989 |
31.05 |
107.07 |
0.31 |
0.47 |
3 |
A |
3090 |
2961 |
18.41 |
110.53 |
0.08 |
0.15 |
4 |
A |
1488 |
1426 |
2.96 |
8.50 |
0.74 |
0.85 |
5 |
A |
1466 |
1404 |
19.50 |
3.00 |
0.41 |
0.58 |
6 |
A |
1409 |
1350 |
24.22 |
5.10 |
0.73 |
0.85 |
7 |
A |
1340 |
1284 |
24.87 |
2.58 |
0.75 |
0.86 |
8 |
A |
1262 |
1210 |
12.04 |
8.01 |
0.73 |
0.84 |
9 |
A |
1173 |
1124 |
89.85 |
5.47 |
0.74 |
0.85 |
10 |
A |
1144 |
1096 |
21.43 |
2.09 |
0.47 |
0.64 |
11 |
A |
1125 |
1077 |
219.95 |
0.79 |
0.37 |
0.54 |
12 |
A |
1099 |
1053 |
29.14 |
5.62 |
0.54 |
0.70 |
13 |
A |
917 |
879 |
36.58 |
4.49 |
0.35 |
0.51 |
14 |
A |
577 |
553 |
4.16 |
1.95 |
0.43 |
0.60 |
15 |
A |
473 |
453 |
18.38 |
0.78 |
0.73 |
0.85 |
16 |
A |
427 |
409 |
5.31 |
1.66 |
0.54 |
0.70 |
17 |
A |
239 |
229 |
8.17 |
0.06 |
0.58 |
0.74 |
18 |
A |
115 |
111 |
7.66 |
0.02 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 11810.6 cm
-1
Scaled (by 0.9582) Zero Point Vibrational Energy (zpe) 11316.9 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 B2PLYP=FULLultrafine/cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.773 |
-0.588 |
-0.287 |
C2 |
0.467 |
0.021 |
0.328 |
F3 |
-1.885 |
0.106 |
0.153 |
F4 |
1.535 |
-0.764 |
-0.006 |
F5 |
0.681 |
1.265 |
-0.182 |
H6 |
-0.702 |
-0.520 |
-1.383 |
H7 |
-0.853 |
-1.642 |
0.020 |
H8 |
0.407 |
0.101 |
1.424 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5116 | 1.3826 | 2.3318 | 2.3577 | 1.1004 | 1.1000 | 2.1896 |
C2 | 1.5116 | | 2.3597 | 1.3671 | 1.3614 | 2.1411 | 2.1446 | 1.1005 | F3 | 1.3826 | 2.3597 | | 3.5326 | 2.8354 | 2.0369 | 2.0337 | 2.6213 | F4 | 2.3318 | 1.3671 | 3.5326 | | 2.2083 | 2.6383 | 2.5446 | 2.0159 | F5 | 2.3577 | 1.3614 | 2.8354 | 2.2083 | | 2.5577 | 3.2926 | 2.0017 | H6 | 1.1004 | 2.1411 | 2.0369 | 2.6383 | 2.5577 | | 1.8021 | 3.0811 | H7 | 1.1000 | 2.1446 | 2.0337 | 2.5446 | 3.2926 | 1.8021 | | 2.5683 | H8 | 2.1896 | 1.1005 | 2.6213 | 2.0159 | 2.0017 | 3.0811 | 2.5683 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.094 |
|
C1 |
C2 |
F5 |
110.187 |
C1 |
C2 |
H8 |
112.965 |
|
C2 |
C1 |
F3 |
109.155 |
C2 |
C1 |
H6 |
109.099 |
|
C2 |
C1 |
H7 |
109.396 |
F3 |
C1 |
H6 |
109.716 |
|
F3 |
C1 |
H7 |
109.486 |
F4 |
C2 |
F5 |
108.063 |
|
F4 |
C2 |
H8 |
109.088 |
F5 |
C2 |
H8 |
108.330 |
|
H6 |
C1 |
H7 |
109.972 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.209 |
|
|
|
2 |
C |
0.372 |
|
|
|
3 |
F |
-0.249 |
|
|
|
4 |
F |
-0.223 |
|
|
|
5 |
F |
-0.213 |
|
|
|
6 |
H |
0.043 |
|
|
|
7 |
H |
0.036 |
|
|
|
8 |
H |
0.026 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.234 |
-1.370 |
0.345 |
1.432 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.950 |
1.400 |
1.245 |
y |
1.400 |
-27.569 |
0.484 |
z |
1.245 |
0.484 |
-24.712 |
|
Traceless |
| x | y | z |
x |
-5.810 |
1.400 |
1.245 |
y |
1.400 |
0.762 |
0.484 |
z |
1.245 |
0.484 |
5.048 |
|
Polar |
3z2-r2 | 10.096 |
x2-y2 | -4.381 |
xy | 1.400 |
xz | 1.245 |
yz | 0.484 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.435 |
-0.026 |
0.013 |
y |
-0.026 |
3.470 |
0.050 |
z |
0.013 |
0.050 |
3.386 |
<r2> (average value of r
2) Å
2
<r2> |
111.570 |
(<r2>)1/2 |
10.563 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/cc-pVDZ
| hartrees |
Energy at 0K | -377.244228 |
Energy at 298.15K | |
HF Energy | -376.973323 |
Nuclear repulsion energy | 193.089387 |
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=FULLultrafine/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' |
3093 |
2964 |
69.62 |
130.16 |
0.05 |
0.10 |
2 |
A' |
3075 |
2947 |
6.23 |
64.95 |
0.43 |
0.60 |
3 |
A' |
1483 |
1421 |
6.60 |
7.09 |
0.75 |
0.85 |
4 |
A' |
1447 |
1387 |
30.56 |
3.48 |
0.32 |
0.48 |
5 |
A' |
1418 |
1358 |
27.93 |
3.31 |
0.69 |
0.82 |
6 |
A' |
1194 |
1144 |
115.98 |
4.78 |
0.49 |
0.65 |
7 |
A' |
1108 |
1062 |
20.41 |
3.15 |
0.74 |
0.85 |
8 |
A' |
887 |
850 |
38.66 |
6.37 |
0.17 |
0.29 |
9 |
A' |
760 |
728 |
50.49 |
2.82 |
0.56 |
0.72 |
10 |
A' |
516 |
494 |
12.03 |
1.64 |
0.75 |
0.86 |
11 |
A' |
230 |
221 |
2.00 |
0.15 |
0.41 |
0.59 |
12 |
A" |
3141 |
3010 |
25.35 |
59.39 |
0.75 |
0.86 |
13 |
A" |
1402 |
1344 |
35.02 |
1.89 |
0.75 |
0.86 |
14 |
A" |
1283 |
1230 |
16.70 |
14.46 |
0.75 |
0.86 |
15 |
A" |
1150 |
1102 |
103.73 |
1.27 |
0.75 |
0.86 |
16 |
A" |
962 |
922 |
63.57 |
2.96 |
0.75 |
0.86 |
17 |
A" |
367 |
352 |
0.08 |
0.24 |
0.75 |
0.86 |
18 |
A" |
110 |
106 |
1.87 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11813.6 cm
-1
Scaled (by 0.9582) Zero Point Vibrational Energy (zpe) 11319.8 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=FULLultrafine/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.740 |
-0.831 |
0.000 |
C2 |
0.358 |
0.630 |
0.000 |
F3 |
-0.389 |
-1.621 |
0.000 |
F4 |
-0.389 |
0.923 |
1.101 |
F5 |
-0.389 |
0.923 |
-1.101 |
H6 |
1.337 |
-1.048 |
-0.900 |
H7 |
1.337 |
-1.048 |
0.900 |
H8 |
1.250 |
1.278 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5107 | 1.3786 | 2.3597 | 2.3597 | 1.1012 | 1.1012 | 2.1701 |
C2 | 1.5107 | | 2.3721 | 1.3629 | 1.3629 | 2.1410 | 2.1410 | 1.1029 | F3 | 1.3786 | 2.3721 | | 2.7726 | 2.7726 | 2.0298 | 2.0298 | 3.3309 | F4 | 2.3597 | 1.3629 | 2.7726 | | 2.2029 | 3.2971 | 2.6280 | 2.0070 | F5 | 2.3597 | 1.3629 | 2.7726 | 2.2029 | | 2.6280 | 3.2971 | 2.0070 | H6 | 1.1012 | 2.1410 | 2.0298 | 3.2971 | 2.6280 | | 1.7997 | 2.4952 | H7 | 1.1012 | 2.1410 | 2.0298 | 2.6280 | 3.2971 | 1.7997 | | 2.4952 | H8 | 2.1701 | 1.1029 | 3.3309 | 2.0070 | 2.0070 | 2.4952 | 2.4952 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.297 |
|
C1 |
C2 |
F5 |
110.297 |
C1 |
C2 |
H8 |
111.310 |
|
C2 |
C1 |
F3 |
110.289 |
C2 |
C1 |
H6 |
109.105 |
|
C2 |
C1 |
H7 |
109.105 |
F3 |
C1 |
H6 |
109.364 |
|
F3 |
C1 |
H7 |
109.364 |
F4 |
C2 |
F5 |
107.834 |
|
F4 |
C2 |
H8 |
108.503 |
F5 |
C2 |
H8 |
108.503 |
|
H6 |
C1 |
H7 |
109.600 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.219 |
|
|
|
2 |
C |
0.376 |
|
|
|
3 |
F |
-0.241 |
|
|
|
4 |
F |
-0.215 |
|
|
|
5 |
F |
-0.215 |
|
|
|
6 |
H |
0.033 |
|
|
|
7 |
H |
0.033 |
|
|
|
8 |
H |
0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.983 |
0.084 |
0.000 |
2.984 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.019 |
-0.258 |
-0.009 |
y |
-0.258 |
-28.659 |
0.001 |
z |
-0.009 |
0.001 |
-28.238 |
|
Traceless |
| x | y | z |
x |
3.430 |
-0.258 |
-0.009 |
y |
-0.258 |
-2.031 |
0.001 |
z |
-0.009 |
0.001 |
-1.399 |
|
Polar |
3z2-r2 | -2.799 |
x2-y2 | 3.640 |
xy | -0.258 |
xz | -0.009 |
yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.459 |
0.013 |
0.002 |
y |
0.013 |
3.428 |
-0.001 |
z |
0.002 |
-0.001 |
3.441 |
<r2> (average value of r
2) Å
2
<r2> |
103.158 |
(<r2>)1/2 |
10.157 |