Jump to
S1C2
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -278.320066 |
Energy at 298.15K | |
HF Energy | -278.320066 |
Nuclear repulsion energy | 126.280344 |
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/Def2TZVPP
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 |
3075 |
3075 |
0.00 |
241.37 |
0.06 |
0.12 |
2 |
Ag |
1516 |
1516 |
0.00 |
10.77 |
0.72 |
0.84 |
3 |
Ag |
1452 |
1452 |
0.00 |
2.45 |
0.42 |
0.59 |
4 |
Ag |
1102 |
1102 |
0.00 |
8.11 |
0.65 |
0.79 |
5 |
Ag |
1090 |
1090 |
0.00 |
6.43 |
0.28 |
0.44 |
6 |
Ag |
462 |
462 |
0.00 |
2.66 |
0.46 |
0.63 |
7 |
Au |
3148 |
3148 |
46.06 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1240 |
1240 |
4.42 |
0.00 |
0.00 |
0.00 |
9 |
Au |
812 |
812 |
0.01 |
0.00 |
0.00 |
0.00 |
10 |
Au |
114 |
114 |
12.56 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3121 |
3121 |
0.00 |
119.41 |
0.75 |
0.86 |
12 |
Bg |
1304 |
1304 |
0.00 |
10.85 |
0.75 |
0.86 |
13 |
Bg |
1177 |
1177 |
0.00 |
2.35 |
0.75 |
0.86 |
14 |
Bu |
3082 |
3082 |
57.85 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1526 |
1526 |
3.95 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1362 |
1362 |
7.88 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
1104 |
1104 |
216.06 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
275 |
275 |
18.39 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13481.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13481.4 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 B1B95/Def2TZVPP
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.422 |
0.625 |
0.000 |
C2 |
-0.422 |
-0.625 |
0.000 |
F3 |
-0.422 |
1.716 |
0.000 |
F4 |
0.422 |
-1.716 |
0.000 |
H5 |
1.049 |
0.670 |
0.889 |
H6 |
1.049 |
0.670 |
-0.889 |
H7 |
-1.049 |
-0.670 |
0.889 |
H8 |
-1.049 |
-0.670 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5085 | 1.3788 | 2.3414 | 1.0887 | 1.0887 | 2.1521 | 2.1521 |
C2 | 1.5085 | | 2.3414 | 1.3788 | 2.1521 | 2.1521 | 1.0887 | 1.0887 | F3 | 1.3788 | 2.3414 | | 3.5343 | 2.0118 | 2.0118 | 2.6225 | 2.6225 | F4 | 2.3414 | 1.3788 | 3.5343 | | 2.6225 | 2.6225 | 2.0118 | 2.0118 | H5 | 1.0887 | 2.1521 | 2.0118 | 2.6225 | | 1.7770 | 2.4901 | 3.0591 | H6 | 1.0887 | 2.1521 | 2.0118 | 2.6225 | 1.7770 | | 3.0591 | 2.4901 | H7 | 2.1521 | 1.0887 | 2.6225 | 2.0118 | 2.4901 | 3.0591 | | 1.7770 | H8 | 2.1521 | 1.0887 | 2.6225 | 2.0118 | 3.0591 | 2.4901 | 1.7770 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.288 |
|
C1 |
C2 |
H7 |
110.881 |
C1 |
C2 |
H8 |
110.881 |
|
C2 |
C1 |
F3 |
108.288 |
C2 |
C1 |
H5 |
110.881 |
|
C2 |
C1 |
H6 |
110.881 |
F3 |
C1 |
H5 |
108.666 |
|
F3 |
C1 |
H6 |
108.666 |
F4 |
C2 |
H7 |
108.666 |
|
F4 |
C2 |
H8 |
108.666 |
H5 |
C1 |
H6 |
109.397 |
|
H7 |
C2 |
H8 |
109.397 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.051 |
|
|
|
2 |
C |
0.051 |
|
|
|
3 |
F |
-0.234 |
|
|
|
4 |
F |
-0.234 |
|
|
|
5 |
H |
0.091 |
|
|
|
6 |
H |
0.091 |
|
|
|
7 |
H |
0.091 |
|
|
|
8 |
H |
0.091 |
|
|
|
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 |
-22.022 |
2.983 |
0.000 |
y |
2.983 |
-28.952 |
0.000 |
z |
0.000 |
0.000 |
-21.459 |
|
Traceless |
| x | y | z |
x |
3.184 |
2.983 |
0.000 |
y |
2.983 |
-7.212 |
0.000 |
z |
0.000 |
0.000 |
4.028 |
|
Polar |
3z2-r2 | 8.057 |
x2-y2 | 6.931 |
xy | 2.983 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.036 |
-0.011 |
0.000 |
y |
-0.011 |
4.171 |
0.000 |
z |
0.000 |
0.000 |
3.746 |
<r2> (average value of r
2) Å
2
<r2> |
87.476 |
(<r2>)1/2 |
9.353 |
Jump to
S1C1
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -278.321739 |
Energy at 298.15K | |
HF Energy | -278.321739 |
Nuclear repulsion energy | 128.317988 |
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/Def2TZVPP
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 |
3117 |
3117 |
15.36 |
91.94 |
0.75 |
0.85 |
2 |
A |
3071 |
3071 |
34.92 |
220.76 |
0.02 |
0.04 |
3 |
A |
1490 |
1490 |
0.45 |
1.64 |
0.65 |
0.79 |
4 |
A |
1442 |
1442 |
12.85 |
2.31 |
0.33 |
0.49 |
5 |
A |
1311 |
1311 |
2.99 |
12.14 |
0.70 |
0.82 |
6 |
A |
1141 |
1141 |
90.57 |
3.07 |
0.59 |
0.74 |
7 |
A |
1131 |
1131 |
6.38 |
1.32 |
0.28 |
0.44 |
8 |
A |
883 |
883 |
21.56 |
4.94 |
0.22 |
0.36 |
9 |
A |
323 |
323 |
0.40 |
0.39 |
0.39 |
0.56 |
10 |
A |
150 |
150 |
3.64 |
0.12 |
0.74 |
0.85 |
11 |
B |
3130 |
3130 |
34.35 |
13.07 |
0.75 |
0.86 |
12 |
B |
3061 |
3061 |
9.60 |
35.57 |
0.75 |
0.86 |
13 |
B |
1489 |
1489 |
9.15 |
8.51 |
0.75 |
0.86 |
14 |
B |
1403 |
1403 |
8.10 |
0.25 |
0.75 |
0.86 |
15 |
B |
1268 |
1268 |
6.93 |
3.28 |
0.75 |
0.86 |
16 |
B |
1110 |
1110 |
60.11 |
3.57 |
0.75 |
0.86 |
17 |
B |
913 |
913 |
39.71 |
2.65 |
0.75 |
0.86 |
18 |
B |
495 |
495 |
15.44 |
0.57 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13463.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13463.1 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 B1B95/Def2TZVPP
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.265 |
0.699 |
0.505 |
C2 |
-0.265 |
-0.699 |
0.505 |
F3 |
-0.265 |
1.423 |
-0.541 |
F4 |
0.265 |
-1.423 |
-0.541 |
H5 |
-0.010 |
1.194 |
1.437 |
H6 |
1.349 |
0.698 |
0.401 |
H7 |
0.010 |
-1.194 |
1.437 |
H8 |
-1.349 |
-0.698 |
0.401 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.4957 | 1.3774 | 2.3657 | 1.0909 | 1.0893 | 2.1259 | 2.1377 |
C2 | 1.4957 | | 2.3657 | 1.3774 | 2.1259 | 2.1377 | 1.0909 | 1.0893 | F3 | 1.3774 | 2.3657 | | 2.8952 | 2.0070 | 2.0047 | 3.2918 | 2.5612 | F4 | 2.3657 | 1.3774 | 2.8952 | | 3.2918 | 2.5612 | 2.0070 | 2.0047 | H5 | 1.0909 | 2.1259 | 2.0070 | 3.2918 | | 1.7800 | 2.3882 | 2.5392 | H6 | 1.0893 | 2.1377 | 2.0047 | 2.5612 | 1.7800 | | 2.5392 | 3.0385 | H7 | 2.1259 | 1.0909 | 3.2918 | 2.0070 | 2.3882 | 2.5392 | | 1.7800 | H8 | 2.1377 | 1.0893 | 2.5612 | 2.0047 | 2.5392 | 3.0385 | 1.7800 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.789 |
|
C1 |
C2 |
H7 |
109.554 |
C1 |
C2 |
H8 |
110.585 |
|
C2 |
C1 |
F3 |
110.789 |
C2 |
C1 |
H5 |
109.554 |
|
C2 |
C1 |
H6 |
110.585 |
F3 |
C1 |
H5 |
108.249 |
|
F3 |
C1 |
H6 |
108.152 |
F4 |
C2 |
H7 |
108.249 |
|
F4 |
C2 |
H8 |
108.152 |
H5 |
C1 |
H6 |
109.463 |
|
H7 |
C2 |
H8 |
109.463 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.068 |
|
|
|
2 |
C |
0.068 |
|
|
|
3 |
F |
-0.230 |
|
|
|
4 |
F |
-0.230 |
|
|
|
5 |
H |
0.074 |
|
|
|
6 |
H |
0.089 |
|
|
|
7 |
H |
0.074 |
|
|
|
8 |
H |
0.089 |
|
|
|
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 |
2.640 |
2.640 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.646 |
1.638 |
0.000 |
y |
1.638 |
-26.014 |
0.000 |
z |
0.000 |
0.000 |
-22.306 |
|
Traceless |
| x | y | z |
x |
2.514 |
1.638 |
0.000 |
y |
1.638 |
-4.038 |
0.000 |
z |
0.000 |
0.000 |
1.524 |
|
Polar |
3z2-r2 | 3.048 |
x2-y2 | 4.368 |
xy | 1.638 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.880 |
0.047 |
0.000 |
y |
0.047 |
4.174 |
0.000 |
z |
0.000 |
0.000 |
4.011 |
<r2> (average value of r
2) Å
2
<r2> |
79.230 |
(<r2>)1/2 |
8.901 |