Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -191.875707 |
| Energy at 298.15K | |
| HF Energy | -191.875707 |
| Nuclear repulsion energy | 103.528370 |
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 B1B95/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3254 |
3124 |
6.02 |
67.54 |
0.53 |
0.69 |
| 2 |
A' |
3204 |
3076 |
1.80 |
106.32 |
0.34 |
0.50 |
| 3 |
A' |
3155 |
3029 |
5.75 |
76.02 |
0.13 |
0.23 |
| 4 |
A' |
2900 |
2785 |
105.18 |
108.40 |
0.28 |
0.44 |
| 5 |
A' |
1828 |
1755 |
243.88 |
59.30 |
0.44 |
0.61 |
| 6 |
A' |
1704 |
1636 |
2.42 |
33.03 |
0.19 |
0.32 |
| 7 |
A' |
1454 |
1396 |
13.32 |
5.88 |
0.61 |
0.76 |
| 8 |
A' |
1391 |
1336 |
7.25 |
19.51 |
0.42 |
0.60 |
| 9 |
A' |
1295 |
1243 |
4.35 |
6.63 |
0.26 |
0.41 |
| 10 |
A' |
1173 |
1126 |
36.25 |
11.21 |
0.55 |
0.71 |
| 11 |
A' |
924 |
887 |
20.49 |
1.21 |
0.06 |
0.12 |
| 12 |
A' |
575 |
552 |
6.25 |
5.35 |
0.33 |
0.50 |
| 13 |
A' |
315 |
302 |
9.88 |
0.97 |
0.36 |
0.53 |
| 14 |
A" |
1044 |
1002 |
9.14 |
1.52 |
0.75 |
0.86 |
| 15 |
A" |
1033 |
992 |
6.74 |
3.63 |
0.75 |
0.86 |
| 16 |
A" |
1001 |
961 |
47.36 |
0.81 |
0.75 |
0.86 |
| 17 |
A" |
614 |
590 |
11.02 |
2.23 |
0.75 |
0.86 |
| 18 |
A" |
172 |
165 |
4.06 |
1.33 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13517.1 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 12977.8 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.152 |
-0.742 |
0.000 |
| C2 |
0.000 |
0.719 |
0.000 |
| C3 |
1.208 |
1.275 |
0.000 |
| O4 |
-1.210 |
-1.315 |
0.000 |
| H5 |
0.806 |
-1.303 |
0.000 |
| H6 |
-0.912 |
1.304 |
0.000 |
| H7 |
1.352 |
2.347 |
0.000 |
| H8 |
2.100 |
0.658 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4687 | 2.4320 | 1.2030 | 1.1105 | 2.1822 | 3.4350 | 2.6517 |
C2 | 1.4687 | | 1.3293 | 2.3666 | 2.1769 | 1.0833 | 2.1157 | 2.1010 | C3 | 2.4320 | 1.3293 | | 3.5426 | 2.6088 | 2.1196 | 1.0816 | 1.0848 | O4 | 1.2030 | 2.3666 | 3.5426 | | 2.0159 | 2.6357 | 4.4686 | 3.8533 | H5 | 1.1105 | 2.1769 | 2.6088 | 2.0159 | | 3.1221 | 3.6902 | 2.3495 | H6 | 2.1822 | 1.0833 | 2.1196 | 2.6357 | 3.1221 | | 2.4922 | 3.0804 | H7 | 3.4350 | 2.1157 | 1.0816 | 4.4686 | 3.6902 | 2.4922 | | 1.8470 | H8 | 2.6517 | 2.1010 | 1.0848 | 3.8533 | 2.3495 | 3.0804 | 1.8470 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.650 |
|
C1 |
C2 |
H6 |
116.733 |
| C2 |
C1 |
O4 |
124.396 |
|
C2 |
C1 |
H5 |
114.420 |
| C2 |
C3 |
H7 |
122.365 |
|
C2 |
C3 |
H8 |
120.650 |
| C3 |
C2 |
H6 |
122.618 |
|
O4 |
C1 |
H5 |
121.184 |
| H7 |
C3 |
H8 |
116.985 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.190 |
|
|
|
| 2 |
C |
-0.192 |
|
|
|
| 3 |
C |
-0.192 |
|
|
|
| 4 |
O |
-0.294 |
|
|
|
| 5 |
H |
0.075 |
|
|
|
| 6 |
H |
0.135 |
|
|
|
| 7 |
H |
0.144 |
|
|
|
| 8 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.399 |
2.022 |
0.000 |
3.138 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.181 |
-2.565 |
0.000 |
| y |
-2.565 |
-23.747 |
0.000 |
| z |
0.000 |
0.000 |
-24.688 |
|
| Traceless |
| | x | y | z |
| x |
0.037 |
-2.565 |
0.000 |
| y |
-2.565 |
0.688 |
0.000 |
| z |
0.000 |
0.000 |
-0.725 |
|
| Polar |
| 3z2-r2 | -1.450 |
| x2-y2 | -0.434 |
| xy | -2.565 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.947 |
1.658 |
0.000 |
| y |
1.658 |
6.291 |
0.000 |
| z |
0.000 |
0.000 |
2.616 |
<r2> (average value of r
2) Å
2
| <r2> |
82.756 |
| (<r2>)1/2 |
9.097 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -191.873249 |
| Energy at 298.15K | |
| HF Energy | -191.873249 |
| Nuclear repulsion energy | 105.179305 |
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 B1B95/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3265 |
3135 |
2.46 |
57.54 |
0.62 |
0.76 |
| 2 |
A' |
3193 |
3066 |
10.71 |
123.72 |
0.27 |
0.43 |
| 3 |
A' |
3165 |
3039 |
5.20 |
59.35 |
0.15 |
0.25 |
| 4 |
A' |
2931 |
2814 |
149.68 |
175.56 |
0.31 |
0.47 |
| 5 |
A' |
1828 |
1755 |
122.14 |
13.73 |
0.61 |
0.76 |
| 6 |
A' |
1695 |
1627 |
66.27 |
46.27 |
0.19 |
0.33 |
| 7 |
A' |
1436 |
1379 |
34.09 |
8.02 |
0.72 |
0.83 |
| 8 |
A' |
1425 |
1368 |
13.35 |
7.85 |
0.26 |
0.41 |
| 9 |
A' |
1314 |
1262 |
2.45 |
15.74 |
0.38 |
0.55 |
| 10 |
A' |
1068 |
1026 |
5.07 |
4.48 |
0.69 |
0.82 |
| 11 |
A' |
943 |
906 |
62.48 |
4.11 |
0.18 |
0.30 |
| 12 |
A' |
686 |
659 |
11.59 |
0.79 |
0.71 |
0.83 |
| 13 |
A' |
290 |
278 |
7.20 |
3.42 |
0.45 |
0.62 |
| 14 |
A" |
1047 |
1005 |
3.30 |
8.19 |
0.75 |
0.86 |
| 15 |
A" |
1033 |
992 |
32.79 |
0.16 |
0.75 |
0.86 |
| 16 |
A" |
1016 |
975 |
18.56 |
0.29 |
0.75 |
0.86 |
| 17 |
A" |
566 |
543 |
10.94 |
3.85 |
0.75 |
0.86 |
| 18 |
A" |
180 |
173 |
7.42 |
0.47 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13540.4 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 13000.1 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.885 |
-0.288 |
0.000 |
| C2 |
0.000 |
0.898 |
0.000 |
| C3 |
1.322 |
0.761 |
0.000 |
| O4 |
-0.490 |
-1.426 |
0.000 |
| H5 |
-1.971 |
-0.070 |
0.000 |
| H6 |
-0.473 |
1.873 |
0.000 |
| H7 |
1.989 |
1.612 |
0.000 |
| H8 |
1.756 |
-0.232 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4796 | 2.4433 | 1.2039 | 1.1075 | 2.1999 | 3.4455 | 2.6413 |
C2 | 1.4796 | | 1.3287 | 2.3742 | 2.1957 | 1.0839 | 2.1136 | 2.0875 | C3 | 2.4433 | 1.3287 | | 2.8395 | 3.3958 | 2.1111 | 1.0815 | 1.0833 | O4 | 1.2039 | 2.3742 | 2.8395 | | 2.0071 | 3.2984 | 3.9208 | 2.5435 | H5 | 1.1075 | 2.1957 | 3.3958 | 2.0071 | | 2.4535 | 4.3026 | 3.7300 | H6 | 2.1999 | 1.0839 | 2.1111 | 3.2984 | 2.4535 | | 2.4760 | 3.0653 | H7 | 3.4455 | 2.1136 | 1.0815 | 3.9208 | 4.3026 | 2.4760 | | 1.8581 | H8 | 2.6413 | 2.0875 | 1.0833 | 2.5435 | 3.7300 | 3.0653 | 1.8581 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.834 |
|
C1 |
C2 |
H6 |
117.393 |
| C2 |
C1 |
O4 |
124.119 |
|
C2 |
C1 |
H5 |
115.395 |
| C2 |
C3 |
H7 |
122.218 |
|
C2 |
C3 |
H8 |
119.525 |
| C3 |
C2 |
H6 |
121.773 |
|
O4 |
C1 |
H5 |
120.485 |
| H7 |
C3 |
H8 |
118.257 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.190 |
|
|
|
| 2 |
C |
-0.240 |
|
|
|
| 3 |
C |
-0.152 |
|
|
|
| 4 |
O |
-0.292 |
|
|
|
| 5 |
H |
0.084 |
|
|
|
| 6 |
H |
0.123 |
|
|
|
| 7 |
H |
0.137 |
|
|
|
| 8 |
H |
0.150 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.208 |
2.609 |
0.000 |
2.618 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.043 |
-0.613 |
0.000 |
| y |
-0.613 |
-25.866 |
0.000 |
| z |
0.000 |
0.000 |
-24.663 |
|
| Traceless |
| | x | y | z |
| x |
5.221 |
-0.613 |
0.000 |
| y |
-0.613 |
-3.513 |
0.000 |
| z |
0.000 |
0.000 |
-1.708 |
|
| Polar |
| 3z2-r2 | -3.416 |
| x2-y2 | 5.823 |
| xy | -0.613 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.116 |
0.433 |
0.000 |
| y |
0.433 |
5.649 |
0.000 |
| z |
0.000 |
0.000 |
2.603 |
<r2> (average value of r
2) Å
2
| <r2> |
74.168 |
| (<r2>)1/2 |
8.612 |