Jump to
S1C2
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -377.243577 |
Energy at 298.15K | |
HF Energy | -376.976058 |
Nuclear repulsion energy | 190.237610 |
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 |
3157 |
3024 |
30.34 |
41.91 |
0.70 |
0.83 |
2 |
A |
3118 |
2986 |
31.00 |
107.34 |
0.31 |
0.47 |
3 |
A |
3088 |
2958 |
18.45 |
110.61 |
0.08 |
0.15 |
4 |
A |
1487 |
1424 |
2.95 |
8.51 |
0.74 |
0.85 |
5 |
A |
1465 |
1403 |
19.47 |
3.00 |
0.41 |
0.58 |
6 |
A |
1408 |
1348 |
24.24 |
5.10 |
0.73 |
0.85 |
7 |
A |
1339 |
1283 |
24.90 |
2.59 |
0.75 |
0.86 |
8 |
A |
1262 |
1208 |
12.08 |
8.02 |
0.73 |
0.84 |
9 |
A |
1172 |
1123 |
89.96 |
5.47 |
0.74 |
0.85 |
10 |
A |
1143 |
1095 |
21.27 |
2.10 |
0.47 |
0.64 |
11 |
A |
1124 |
1077 |
219.93 |
0.80 |
0.37 |
0.54 |
12 |
A |
1099 |
1052 |
29.25 |
5.63 |
0.54 |
0.70 |
13 |
A |
916 |
878 |
36.58 |
4.50 |
0.35 |
0.51 |
14 |
A |
577 |
553 |
4.17 |
1.96 |
0.43 |
0.60 |
15 |
A |
473 |
453 |
18.39 |
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 |
110 |
7.66 |
0.02 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 11804.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 11305.5 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 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 |
1.536 |
-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 |
0.408 |
0.101 |
1.424 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5120 | 1.3828 | 2.3323 | 2.3583 | 1.1007 | 1.1003 | 2.1902 |
C2 | 1.5120 | | 2.3601 | 1.3673 | 1.3617 | 2.1417 | 2.1452 | 1.1007 | F3 | 1.3828 | 2.3601 | | 3.5333 | 2.8360 | 2.0373 | 2.0341 | 2.6218 | F4 | 2.3323 | 1.3673 | 3.5333 | | 2.2086 | 2.6390 | 2.5451 | 2.0163 | F5 | 2.3583 | 1.3617 | 2.8360 | 2.2086 | | 2.5582 | 3.2933 | 2.0021 | H6 | 1.1007 | 2.1417 | 2.0373 | 2.6390 | 2.5582 | | 1.8027 | 3.0820 | H7 | 1.1003 | 2.1452 | 2.0341 | 2.5451 | 3.2933 | 1.8027 | | 2.5690 | H8 | 2.1902 | 1.1007 | 2.6218 | 2.0163 | 2.0021 | 3.0820 | 2.5690 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.092 |
|
C1 |
C2 |
F5 |
110.187 |
C1 |
C2 |
H8 |
112.969 |
|
C2 |
C1 |
F3 |
109.152 |
C2 |
C1 |
H6 |
109.101 |
|
C2 |
C1 |
H7 |
109.396 |
F3 |
C1 |
H6 |
109.713 |
|
F3 |
C1 |
H7 |
109.482 |
F4 |
C2 |
F5 |
108.061 |
|
F4 |
C2 |
H8 |
109.088 |
F5 |
C2 |
H8 |
108.330 |
|
H6 |
C1 |
H7 |
109.979 |
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 |
0.209 |
|
|
|
2 |
C |
0.372 |
|
|
|
3 |
F |
-0.250 |
|
|
|
4 |
F |
-0.223 |
|
|
|
5 |
F |
-0.214 |
|
|
|
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 |
-31.953 |
1.401 |
1.245 |
y |
1.401 |
-27.570 |
0.484 |
z |
1.245 |
0.484 |
-24.712 |
|
Traceless |
| x | y | z |
x |
-5.812 |
1.401 |
1.245 |
y |
1.401 |
0.762 |
0.484 |
z |
1.245 |
0.484 |
5.050 |
|
Polar |
3z2-r2 | 10.101 |
x2-y2 | -4.383 |
xy | 1.401 |
xz | 1.245 |
yz | 0.484 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.436 |
-0.026 |
0.013 |
y |
-0.026 |
3.471 |
0.050 |
z |
0.013 |
0.050 |
3.387 |
<r2> (average value of r
2) Å
2
<r2> |
111.608 |
(<r2>)1/2 |
10.564 |
Jump to
S1C1
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -377.240904 |
Energy at 298.15K | |
HF Energy | -376.973300 |
Nuclear repulsion energy | 193.051714 |
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' |
3091 |
2961 |
69.69 |
130.08 |
0.05 |
0.10 |
2 |
A' |
3073 |
2943 |
6.26 |
65.25 |
0.42 |
0.60 |
3 |
A' |
1482 |
1420 |
6.59 |
7.09 |
0.75 |
0.85 |
4 |
A' |
1446 |
1385 |
30.47 |
3.48 |
0.32 |
0.48 |
5 |
A' |
1417 |
1357 |
28.05 |
3.32 |
0.69 |
0.82 |
6 |
A' |
1194 |
1143 |
116.05 |
4.78 |
0.49 |
0.65 |
7 |
A' |
1108 |
1061 |
20.41 |
3.15 |
0.74 |
0.85 |
8 |
A' |
886 |
849 |
38.65 |
6.38 |
0.17 |
0.29 |
9 |
A' |
760 |
728 |
50.50 |
2.83 |
0.56 |
0.72 |
10 |
A' |
516 |
494 |
12.03 |
1.65 |
0.75 |
0.86 |
11 |
A' |
230 |
220 |
2.00 |
0.15 |
0.41 |
0.59 |
12 |
A" |
3139 |
3006 |
25.44 |
59.46 |
0.75 |
0.86 |
13 |
A" |
1402 |
1342 |
35.04 |
1.89 |
0.75 |
0.86 |
14 |
A" |
1283 |
1228 |
16.72 |
14.48 |
0.75 |
0.86 |
15 |
A" |
1150 |
1101 |
103.64 |
1.27 |
0.75 |
0.86 |
16 |
A" |
962 |
921 |
63.62 |
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) 11807.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 11308.4 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 Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.741 |
-0.832 |
0.000 |
C2 |
0.358 |
0.630 |
0.000 |
F3 |
-0.389 |
-1.622 |
0.000 |
F4 |
-0.389 |
0.923 |
1.102 |
F5 |
-0.389 |
0.923 |
-1.102 |
H6 |
1.337 |
-1.048 |
-0.900 |
H7 |
1.337 |
-1.048 |
0.900 |
H8 |
1.251 |
1.278 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5111 | 1.3788 | 2.3602 | 2.3602 | 1.1015 | 1.1015 | 2.1707 |
C2 | 1.5111 | | 2.3726 | 1.3631 | 1.3631 | 2.1415 | 2.1415 | 1.1032 | F3 | 1.3788 | 2.3726 | | 2.7732 | 2.7732 | 2.0301 | 2.0301 | 3.3316 | F4 | 2.3602 | 1.3631 | 2.7732 | | 2.2032 | 3.2978 | 2.6286 | 2.0074 | F5 | 2.3602 | 1.3631 | 2.7732 | 2.2032 | | 2.6286 | 3.2978 | 2.0074 | H6 | 1.1015 | 2.1415 | 2.0301 | 3.2978 | 2.6286 | | 1.8002 | 2.4960 | H7 | 1.1015 | 2.1415 | 2.0301 | 2.6286 | 3.2978 | 1.8002 | | 2.4960 | H8 | 2.1707 | 1.1032 | 3.3316 | 2.0074 | 2.0074 | 2.4960 | 2.4960 | |
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 |
111.313 |
|
C2 |
C1 |
F3 |
110.288 |
C2 |
C1 |
H6 |
109.105 |
|
C2 |
C1 |
H7 |
109.105 |
F3 |
C1 |
H6 |
109.361 |
|
F3 |
C1 |
H7 |
109.361 |
F4 |
C2 |
F5 |
107.833 |
|
F4 |
C2 |
H8 |
108.502 |
F5 |
C2 |
H8 |
108.502 |
|
H6 |
C1 |
H7 |
109.606 |
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 |
0.219 |
|
|
|
2 |
C |
0.377 |
|
|
|
3 |
F |
-0.242 |
|
|
|
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 |
|
2.984 |
0.084 |
0.000 |
2.985 |
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 |
-28.661 |
0.001 |
z |
-0.009 |
0.001 |
-28.240 |
|
Traceless |
| x | y | z |
x |
3.431 |
-0.258 |
-0.009 |
y |
-0.258 |
-2.032 |
0.001 |
z |
-0.009 |
0.001 |
-1.400 |
|
Polar |
3z2-r2 | -2.800 |
x2-y2 | 3.642 |
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 |
3.460 |
0.013 |
0.002 |
y |
0.013 |
3.430 |
-0.001 |
z |
0.002 |
-0.001 |
3.443 |
<r2> (average value of r
2) Å
2
<r2> |
103.194 |
(<r2>)1/2 |
10.158 |