Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -79.784000 |
Energy at 298.15K | -79.789866 |
HF Energy | -79.784000 |
Nuclear repulsion energy | 41.893057 |
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 BLYP/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 |
A1g |
2954 |
2947 |
0.00 |
245.83 |
0.01 |
0.02 |
2 |
A1g |
1398 |
1394 |
0.00 |
4.43 |
0.75 |
0.86 |
3 |
A1g |
966 |
963 |
0.00 |
8.96 |
0.29 |
0.44 |
4 |
A1u |
299 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
5 |
A2u |
2955 |
2948 |
74.05 |
0.00 |
0.00 |
0.00 |
6 |
A2u |
1388 |
1385 |
1.66 |
0.00 |
0.00 |
0.00 |
7 |
Eg |
2993 |
2986 |
0.00 |
157.68 |
0.75 |
0.86 |
7 |
Eg |
2993 |
2986 |
0.00 |
157.68 |
0.75 |
0.86 |
8 |
Eg |
1487 |
1483 |
0.00 |
28.19 |
0.75 |
0.86 |
8 |
Eg |
1487 |
1483 |
0.00 |
28.19 |
0.75 |
0.86 |
9 |
Eg |
1195 |
1192 |
0.00 |
1.01 |
0.75 |
0.86 |
9 |
Eg |
1195 |
1192 |
0.00 |
1.01 |
0.75 |
0.86 |
10 |
Eu |
3020 |
3012 |
92.10 |
0.00 |
0.00 |
0.00 |
10 |
Eu |
3020 |
3012 |
92.10 |
0.00 |
0.00 |
0.00 |
11 |
Eu |
1490 |
1487 |
11.27 |
0.00 |
0.00 |
0.00 |
11 |
Eu |
1490 |
1487 |
11.27 |
0.00 |
0.00 |
0.00 |
12 |
Eu |
813 |
811 |
4.43 |
0.00 |
0.00 |
0.00 |
12 |
Eu |
813 |
811 |
4.43 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 15977.9 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 15937.9 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 BLYP/6-311G*
Point Group is D3d
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.770 |
C2 |
0.000 |
0.000 |
-0.770 |
H3 |
0.000 |
1.024 |
1.173 |
H4 |
-0.887 |
-0.512 |
1.173 |
H5 |
0.887 |
-0.512 |
1.173 |
H6 |
0.000 |
-1.024 |
-1.173 |
H7 |
-0.887 |
0.512 |
-1.173 |
H8 |
0.887 |
0.512 |
-1.173 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5403 | 1.1004 | 1.1004 | 1.1004 | 2.1965 | 2.1965 | 2.1965 |
C2 | 1.5403 | | 2.1965 | 2.1965 | 2.1965 | 1.1004 | 1.1004 | 1.1004 | H3 | 1.1004 | 2.1965 | | 1.7737 | 1.7737 | 3.1143 | 2.5599 | 2.5599 | H4 | 1.1004 | 2.1965 | 1.7737 | | 1.7737 | 2.5599 | 2.5599 | 3.1143 | H5 | 1.1004 | 2.1965 | 1.7737 | 1.7737 | | 2.5599 | 3.1143 | 2.5599 | H6 | 2.1965 | 1.1004 | 3.1143 | 2.5599 | 2.5599 | | 1.7737 | 1.7737 | H7 | 2.1965 | 1.1004 | 2.5599 | 2.5599 | 3.1143 | 1.7737 | | 1.7737 | H8 | 2.1965 | 1.1004 | 2.5599 | 3.1143 | 2.5599 | 1.7737 | 1.7737 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H6 |
111.478 |
|
C1 |
C2 |
H7 |
111.478 |
C1 |
C2 |
H8 |
111.478 |
|
C2 |
C1 |
H3 |
111.478 |
C2 |
C1 |
H4 |
111.478 |
|
C2 |
C1 |
H5 |
111.478 |
H3 |
C1 |
H4 |
107.392 |
|
H3 |
C1 |
H5 |
107.392 |
H4 |
C1 |
H5 |
107.392 |
|
H6 |
C2 |
H7 |
107.392 |
H6 |
C2 |
H8 |
107.392 |
|
H7 |
C2 |
H8 |
107.392 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.582 |
|
|
|
2 |
C |
-0.582 |
|
|
|
3 |
H |
0.194 |
|
|
|
4 |
H |
0.194 |
|
|
|
5 |
H |
0.194 |
|
|
|
6 |
H |
0.194 |
|
|
|
7 |
H |
0.194 |
|
|
|
8 |
H |
0.194 |
|
|
|
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 |
-15.202 |
0.000 |
0.000 |
y |
0.000 |
-15.202 |
0.000 |
z |
0.000 |
0.000 |
-15.908 |
|
Traceless |
| x | y | z |
x |
0.353 |
0.000 |
0.000 |
y |
0.000 |
0.353 |
0.000 |
z |
0.000 |
0.000 |
-0.706 |
|
Polar |
3z2-r2 | -1.412 |
x2-y2 | 0.000 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.670 |
0.000 |
0.000 |
y |
0.000 |
3.670 |
0.000 |
z |
0.000 |
0.000 |
4.060 |
<r2> (average value of r
2) Å
2
<r2> |
31.307 |
(<r2>)1/2 |
5.595 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -79.779893 |
Energy at 298.15K | |
HF Energy | -79.779893 |
Nuclear repulsion energy | 41.726226 |
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 BLYP/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 |
A1' |
2971 |
2963 |
0.00 |
|
|
|
2 |
A1' |
1422 |
1419 |
0.00 |
|
|
|
3 |
A1' |
961 |
958 |
0.00 |
|
|
|
4 |
A1" |
291i |
290i |
0.00 |
|
|
|
5 |
A2" |
2964 |
2956 |
75.53 |
|
|
|
6 |
A2" |
1388 |
1384 |
1.61 |
|
|
|
7 |
E' |
3028 |
3020 |
79.16 |
|
|
|
7 |
E' |
3028 |
3020 |
79.17 |
|
|
|
8 |
E' |
1497 |
1493 |
12.43 |
|
|
|
8 |
E' |
1497 |
1493 |
12.43 |
|
|
|
9 |
E' |
887 |
885 |
4.27 |
|
|
|
9 |
E' |
887 |
885 |
4.27 |
|
|
|
10 |
E" |
3004 |
2996 |
0.00 |
|
|
|
10 |
E" |
3004 |
2996 |
0.00 |
|
|
|
11 |
E" |
1488 |
1484 |
0.00 |
|
|
|
11 |
E" |
1488 |
1484 |
0.00 |
|
|
|
12 |
E" |
1148 |
1145 |
0.00 |
|
|
|
12 |
E" |
1148 |
1145 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15757.9 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 15718.5 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 BLYP/6-311G*
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.777 |
C2 |
0.000 |
0.000 |
-0.777 |
H3 |
0.000 |
1.020 |
1.188 |
H4 |
-0.883 |
-0.510 |
1.188 |
H5 |
0.883 |
-0.510 |
1.188 |
H6 |
0.000 |
1.020 |
-1.188 |
H7 |
0.883 |
-0.510 |
-1.188 |
H8 |
-0.883 |
-0.510 |
-1.188 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5548 | 1.0992 | 1.0992 | 1.0992 | 2.2141 | 2.2141 | 2.2141 |
C2 | 1.5548 | | 2.2141 | 2.2141 | 2.2141 | 1.0992 | 1.0992 | 1.0992 | H3 | 1.0992 | 2.2141 | | 1.7661 | 1.7661 | 2.3760 | 2.9605 | 2.9605 | H4 | 1.0992 | 2.2141 | 1.7661 | | 1.7661 | 2.9605 | 2.9605 | 2.3760 | H5 | 1.0992 | 2.2141 | 1.7661 | 1.7661 | | 2.9605 | 2.3760 | 2.9605 | H6 | 2.2141 | 1.0992 | 2.3760 | 2.9605 | 2.9605 | | 1.7661 | 1.7661 | H7 | 2.2141 | 1.0992 | 2.9605 | 2.9605 | 2.3760 | 1.7661 | | 1.7661 | H8 | 2.2141 | 1.0992 | 2.9605 | 2.3760 | 2.9605 | 1.7661 | 1.7661 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H6 |
111.934 |
|
C1 |
C2 |
H7 |
111.934 |
C1 |
C2 |
H8 |
111.934 |
|
C2 |
C1 |
H3 |
111.934 |
C2 |
C1 |
H4 |
111.934 |
|
C2 |
C1 |
H5 |
111.934 |
H3 |
C1 |
H4 |
106.900 |
|
H3 |
C1 |
H5 |
106.900 |
H4 |
C1 |
H5 |
106.900 |
|
H6 |
C2 |
H7 |
106.900 |
H6 |
C2 |
H8 |
106.900 |
|
H7 |
C2 |
H8 |
106.900 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.595 |
|
|
|
2 |
C |
-0.595 |
|
|
|
3 |
H |
0.198 |
|
|
|
4 |
H |
0.198 |
|
|
|
5 |
H |
0.198 |
|
|
|
6 |
H |
0.198 |
|
|
|
7 |
H |
0.198 |
|
|
|
8 |
H |
0.198 |
|
|
|
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 |
-15.194 |
0.000 |
0.000 |
y |
0.000 |
-15.194 |
0.000 |
z |
0.000 |
0.000 |
-15.852 |
|
Traceless |
| x | y | z |
x |
0.329 |
0.000 |
0.000 |
y |
0.000 |
0.329 |
0.000 |
z |
0.000 |
0.000 |
-0.658 |
|
Polar |
3z2-r2 | -1.317 |
x2-y2 | 0.000 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.605 |
0.000 |
0.000 |
y |
0.000 |
3.605 |
0.000 |
z |
0.000 |
0.000 |
3.969 |
<r2> (average value of r
2) Å
2
<r2> |
31.585 |
(<r2>)1/2 |
5.620 |