Jump to
S1C2
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -377.596047 |
Energy at 298.15K | |
HF Energy | -377.596047 |
Nuclear repulsion energy | 191.629282 |
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 |
3149 |
3149 |
19.60 |
36.23 |
0.69 |
0.82 |
2 |
A |
3106 |
3106 |
25.42 |
85.74 |
0.31 |
0.48 |
3 |
A |
3085 |
3085 |
14.72 |
129.36 |
0.06 |
0.12 |
4 |
A |
1495 |
1495 |
5.00 |
4.71 |
0.73 |
0.85 |
5 |
A |
1460 |
1460 |
15.30 |
1.95 |
0.48 |
0.65 |
6 |
A |
1402 |
1402 |
18.46 |
3.03 |
0.74 |
0.85 |
7 |
A |
1345 |
1345 |
13.77 |
1.84 |
0.75 |
0.86 |
8 |
A |
1273 |
1273 |
15.10 |
5.21 |
0.71 |
0.83 |
9 |
A |
1176 |
1176 |
92.76 |
4.08 |
0.64 |
0.78 |
10 |
A |
1140 |
1140 |
52.20 |
2.06 |
0.60 |
0.75 |
11 |
A |
1135 |
1135 |
228.79 |
0.25 |
0.26 |
0.41 |
12 |
A |
1112 |
1112 |
18.78 |
5.26 |
0.43 |
0.60 |
13 |
A |
916 |
916 |
31.11 |
4.06 |
0.31 |
0.47 |
14 |
A |
583 |
583 |
3.86 |
1.79 |
0.35 |
0.52 |
15 |
A |
473 |
473 |
17.71 |
0.63 |
0.73 |
0.84 |
16 |
A |
428 |
428 |
5.42 |
1.40 |
0.49 |
0.66 |
17 |
A |
240 |
240 |
8.01 |
0.06 |
0.61 |
0.76 |
18 |
A |
115 |
115 |
8.04 |
0.03 |
0.66 |
0.80 |
Unscaled Zero Point Vibrational Energy (zpe) 11816.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11816.3 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/Def2TZVPP
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.774 |
-0.581 |
-0.286 |
C2 |
0.465 |
0.020 |
0.325 |
F3 |
-1.874 |
0.111 |
0.154 |
F4 |
1.521 |
-0.763 |
-0.005 |
F5 |
0.689 |
1.251 |
-0.181 |
H6 |
-0.714 |
-0.510 |
-1.371 |
H7 |
-0.862 |
-1.622 |
0.019 |
H8 |
0.410 |
0.102 |
1.410 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5065 | 1.3713 | 2.3196 | 2.3467 | 1.0887 | 1.0884 | 2.1790 |
C2 | 1.5065 | | 2.3464 | 1.3553 | 1.3502 | 2.1327 | 2.1327 | 1.0897 | F3 | 1.3713 | 2.3464 | | 3.5088 | 2.8247 | 2.0139 | 2.0108 | 2.6068 | F4 | 2.3196 | 1.3553 | 3.5088 | | 2.1859 | 2.6317 | 2.5334 | 1.9963 | F5 | 2.3467 | 1.3502 | 2.8247 | 2.1859 | | 2.5472 | 3.2708 | 1.9824 | H6 | 1.0887 | 2.1327 | 2.0139 | 2.6317 | 2.5472 | | 1.7856 | 3.0621 | H7 | 1.0884 | 2.1327 | 2.0108 | 2.5334 | 3.2708 | 1.7856 | | 2.5549 | H8 | 2.1790 | 1.0897 | 2.6068 | 1.9963 | 1.9824 | 3.0621 | 2.5549 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
108.187 |
|
C1 |
C2 |
F5 |
110.352 |
C1 |
C2 |
H8 |
113.164 |
|
C2 |
C1 |
F3 |
109.156 |
C2 |
C1 |
H6 |
109.480 |
|
C2 |
C1 |
H7 |
109.494 |
F3 |
C1 |
H6 |
109.360 |
|
F3 |
C1 |
H7 |
109.128 |
F4 |
C2 |
F5 |
107.794 |
|
F4 |
C2 |
H8 |
108.992 |
F5 |
C2 |
H8 |
108.212 |
|
H6 |
C1 |
H7 |
110.205 |
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 |
0.058 |
|
|
|
2 |
C |
0.277 |
|
|
|
3 |
F |
-0.220 |
|
|
|
4 |
F |
-0.196 |
|
|
|
5 |
F |
-0.189 |
|
|
|
6 |
H |
0.100 |
|
|
|
7 |
H |
0.092 |
|
|
|
8 |
H |
0.079 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.294 |
-1.438 |
0.353 |
1.509 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.164 |
1.624 |
1.485 |
y |
1.624 |
-27.779 |
0.520 |
z |
1.485 |
0.520 |
-24.736 |
|
Traceless |
| x | y | z |
x |
-5.907 |
1.624 |
1.485 |
y |
1.624 |
0.671 |
0.520 |
z |
1.485 |
0.520 |
5.236 |
|
Polar |
3z2-r2 | 10.471 |
x2-y2 | -4.385 |
xy | 1.624 |
xz | 1.485 |
yz | 0.520 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.152 |
-0.042 |
-0.005 |
y |
-0.042 |
4.058 |
0.048 |
z |
-0.005 |
0.048 |
3.858 |
<r2> (average value of r
2) Å
2
<r2> |
110.493 |
(<r2>)1/2 |
10.512 |
Jump to
S1C1
Energy calculated at B1B95/Def2TZVPP
| hartrees |
Energy at 0K | -377.594111 |
Energy at 298.15K | |
HF Energy | -377.594111 |
Nuclear repulsion energy | 194.371381 |
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' |
3085 |
3085 |
56.22 |
151.01 |
0.02 |
0.04 |
2 |
A' |
3071 |
3071 |
1.98 |
50.95 |
0.59 |
0.74 |
3 |
A' |
1490 |
1490 |
6.80 |
4.42 |
0.73 |
0.84 |
4 |
A' |
1438 |
1438 |
23.21 |
2.48 |
0.35 |
0.52 |
5 |
A' |
1416 |
1416 |
19.81 |
1.80 |
0.69 |
0.81 |
6 |
A' |
1205 |
1205 |
128.93 |
3.66 |
0.29 |
0.45 |
7 |
A' |
1128 |
1128 |
29.19 |
3.20 |
0.75 |
0.85 |
8 |
A' |
882 |
882 |
29.05 |
6.11 |
0.15 |
0.26 |
9 |
A' |
768 |
768 |
49.81 |
2.39 |
0.52 |
0.68 |
10 |
A' |
521 |
521 |
12.31 |
1.24 |
0.75 |
0.86 |
11 |
A' |
230 |
230 |
1.71 |
0.17 |
0.49 |
0.66 |
12 |
A" |
3133 |
3133 |
15.48 |
50.78 |
0.75 |
0.86 |
13 |
A" |
1392 |
1392 |
25.07 |
1.16 |
0.75 |
0.86 |
14 |
A" |
1290 |
1290 |
20.14 |
9.39 |
0.75 |
0.86 |
15 |
A" |
1153 |
1153 |
123.84 |
1.25 |
0.75 |
0.86 |
16 |
A" |
960 |
960 |
57.37 |
2.39 |
0.75 |
0.86 |
17 |
A" |
366 |
366 |
0.28 |
0.22 |
0.75 |
0.86 |
18 |
A" |
113 |
113 |
1.99 |
0.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11819.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 11819.8 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 B1B95/Def2TZVPP
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.732 |
-0.832 |
0.000 |
C2 |
0.355 |
0.625 |
0.000 |
F3 |
-0.385 |
-1.618 |
0.000 |
F4 |
-0.385 |
0.924 |
1.090 |
F5 |
-0.385 |
0.924 |
-1.090 |
H6 |
1.321 |
-1.048 |
-0.891 |
H7 |
1.321 |
-1.048 |
0.891 |
H8 |
1.242 |
1.262 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
C1 | | 1.5052 | 1.3664 | 2.3499 | 2.3499 | 1.0895 | 1.0895 | 2.1553 |
C2 | 1.5052 | | 2.3620 | 1.3514 | 1.3514 | 2.1276 | 2.1276 | 1.0921 | F3 | 1.3664 | 2.3620 | | 2.7661 | 2.7661 | 2.0073 | 2.0073 | 3.3080 | F4 | 2.3499 | 1.3514 | 2.7661 | | 2.1808 | 3.2752 | 2.6152 | 1.9876 | F5 | 2.3499 | 1.3514 | 2.7661 | 2.1808 | | 2.6152 | 3.2752 | 1.9876 | H6 | 1.0895 | 2.1276 | 2.0073 | 3.2752 | 2.6152 | | 1.7826 | 2.4776 | H7 | 1.0895 | 2.1276 | 2.0073 | 2.6152 | 3.2752 | 1.7826 | | 2.4776 | H8 | 2.1553 | 1.0921 | 3.3080 | 1.9876 | 1.9876 | 2.4776 | 2.4776 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
F4 |
110.588 |
|
C1 |
C2 |
F5 |
110.588 |
C1 |
C2 |
H8 |
111.168 |
|
C2 |
C1 |
F3 |
110.587 |
C2 |
C1 |
H6 |
109.113 |
|
C2 |
C1 |
H7 |
109.113 |
F3 |
C1 |
H6 |
109.118 |
|
F3 |
C1 |
H7 |
109.118 |
F4 |
C2 |
F5 |
107.586 |
|
F4 |
C2 |
H8 |
108.398 |
F5 |
C2 |
H8 |
108.398 |
|
H6 |
C1 |
H7 |
109.781 |
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 |
0.059 |
|
|
|
2 |
C |
0.297 |
|
|
|
3 |
F |
-0.211 |
|
|
|
4 |
F |
-0.190 |
|
|
|
5 |
F |
-0.190 |
|
|
|
6 |
H |
0.088 |
|
|
|
7 |
H |
0.088 |
|
|
|
8 |
H |
0.060 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
3.113 |
0.051 |
0.000 |
3.113 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.201 |
-0.347 |
0.000 |
y |
-0.347 |
-28.645 |
0.000 |
z |
0.000 |
0.000 |
-28.437 |
|
Traceless |
| x | y | z |
x |
3.339 |
-0.347 |
0.000 |
y |
-0.347 |
-1.826 |
0.000 |
z |
0.000 |
0.000 |
-1.513 |
|
Polar |
3z2-r2 | -3.027 |
x2-y2 | 3.443 |
xy | -0.347 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.042 |
-0.013 |
0.000 |
y |
-0.013 |
4.066 |
0.000 |
z |
0.000 |
0.000 |
3.999 |
<r2> (average value of r
2) Å
2
<r2> |
102.354 |
(<r2>)1/2 |
10.117 |