Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -191.869596 |
| Energy at 298.15K | |
| HF Energy | -191.869596 |
| Nuclear repulsion energy | 103.500076 |
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' |
3255 |
3120 |
9.24 |
65.70 |
0.54 |
0.70 |
| 2 |
A' |
3206 |
3073 |
2.83 |
104.73 |
0.34 |
0.51 |
| 3 |
A' |
3159 |
3028 |
8.35 |
72.40 |
0.14 |
0.24 |
| 4 |
A' |
2909 |
2788 |
113.15 |
106.51 |
0.29 |
0.45 |
| 5 |
A' |
1831 |
1755 |
246.90 |
60.57 |
0.44 |
0.61 |
| 6 |
A' |
1710 |
1639 |
2.33 |
31.08 |
0.19 |
0.32 |
| 7 |
A' |
1467 |
1406 |
12.62 |
5.94 |
0.60 |
0.75 |
| 8 |
A' |
1402 |
1344 |
7.60 |
19.73 |
0.44 |
0.61 |
| 9 |
A' |
1304 |
1250 |
3.88 |
7.06 |
0.25 |
0.40 |
| 10 |
A' |
1180 |
1131 |
36.04 |
11.38 |
0.54 |
0.70 |
| 11 |
A' |
929 |
891 |
21.59 |
1.17 |
0.06 |
0.11 |
| 12 |
A' |
575 |
552 |
6.27 |
5.37 |
0.34 |
0.50 |
| 13 |
A' |
316 |
303 |
9.87 |
0.97 |
0.37 |
0.54 |
| 14 |
A" |
1042 |
999 |
11.02 |
1.48 |
0.75 |
0.86 |
| 15 |
A" |
1028 |
985 |
8.30 |
3.90 |
0.75 |
0.86 |
| 16 |
A" |
994 |
953 |
48.52 |
0.90 |
0.75 |
0.86 |
| 17 |
A" |
611 |
586 |
11.55 |
2.45 |
0.75 |
0.86 |
| 18 |
A" |
172 |
165 |
3.88 |
1.36 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13545.1 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12984.3 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.152 |
-0.742 |
0.000 |
| C2 |
0.000 |
0.718 |
0.000 |
| C3 |
1.206 |
1.278 |
0.000 |
| O4 |
-1.209 |
-1.317 |
0.000 |
| H5 |
0.804 |
-1.308 |
0.000 |
| H6 |
-0.913 |
1.303 |
0.000 |
| H7 |
1.348 |
2.350 |
0.000 |
| H8 |
2.104 |
0.667 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4685 | 2.4339 | 1.2029 | 1.1107 | 2.1822 | 3.4371 | 2.6597 |
C2 | 1.4685 | | 1.3295 | 2.3669 | 2.1799 | 1.0840 | 2.1167 | 2.1043 | C3 | 2.4339 | 1.3295 | | 3.5442 | 2.6164 | 2.1192 | 1.0823 | 1.0853 | O4 | 1.2029 | 2.3669 | 3.5442 | | 2.0127 | 2.6363 | 4.4703 | 3.8610 | H5 | 1.1107 | 2.1799 | 2.6164 | 2.0127 | | 3.1247 | 3.6985 | 2.3643 | H6 | 2.1822 | 1.0840 | 2.1192 | 2.6363 | 3.1247 | | 2.4916 | 3.0828 | H7 | 3.4371 | 2.1167 | 1.0823 | 4.4703 | 3.6985 | 2.4916 | | 1.8451 | H8 | 2.6597 | 2.1043 | 1.0853 | 3.8610 | 2.3643 | 3.0828 | 1.8451 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.806 |
|
C1 |
C2 |
H6 |
116.701 |
| C2 |
C1 |
O4 |
124.464 |
|
C2 |
C1 |
H5 |
114.677 |
| C2 |
C3 |
H7 |
122.389 |
|
C2 |
C3 |
H8 |
120.914 |
| C3 |
C2 |
H6 |
122.493 |
|
O4 |
C1 |
H5 |
120.859 |
| H7 |
C3 |
H8 |
116.697 |
|
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 |
0.104 |
|
|
|
| 2 |
C |
-0.246 |
|
|
|
| 3 |
C |
-0.416 |
|
|
|
| 4 |
O |
-0.297 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
| 6 |
H |
0.227 |
|
|
|
| 7 |
H |
0.239 |
|
|
|
| 8 |
H |
0.231 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.403 |
2.041 |
0.000 |
3.153 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.128 |
-2.574 |
0.000 |
| y |
-2.574 |
-23.697 |
0.000 |
| z |
0.000 |
0.000 |
-24.833 |
|
| Traceless |
| | x | y | z |
| x |
0.137 |
-2.574 |
0.000 |
| y |
-2.574 |
0.784 |
0.000 |
| z |
0.000 |
0.000 |
-0.921 |
|
| Polar |
| 3z2-r2 | -1.842 |
| x2-y2 | -0.431 |
| xy | -2.574 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.893 |
1.662 |
0.000 |
| y |
1.662 |
6.252 |
0.000 |
| z |
0.000 |
0.000 |
2.530 |
<r2> (average value of r
2) Å
2
| <r2> |
82.846 |
| (<r2>)1/2 |
9.102 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -191.867120 |
| Energy at 298.15K | |
| HF Energy | -191.867120 |
| Nuclear repulsion energy | 105.141440 |
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' |
3268 |
3132 |
4.48 |
55.24 |
0.64 |
0.78 |
| 2 |
A' |
3196 |
3063 |
13.24 |
124.87 |
0.27 |
0.42 |
| 3 |
A' |
3169 |
3038 |
7.82 |
54.40 |
0.17 |
0.29 |
| 4 |
A' |
2938 |
2816 |
161.16 |
172.32 |
0.32 |
0.48 |
| 5 |
A' |
1832 |
1756 |
123.53 |
14.03 |
0.61 |
0.76 |
| 6 |
A' |
1701 |
1630 |
67.69 |
45.67 |
0.20 |
0.33 |
| 7 |
A' |
1447 |
1387 |
36.11 |
8.30 |
0.74 |
0.85 |
| 8 |
A' |
1437 |
1377 |
11.51 |
7.96 |
0.25 |
0.40 |
| 9 |
A' |
1323 |
1268 |
2.45 |
15.71 |
0.37 |
0.54 |
| 10 |
A' |
1076 |
1031 |
5.45 |
4.45 |
0.69 |
0.81 |
| 11 |
A' |
945 |
906 |
61.93 |
4.03 |
0.18 |
0.31 |
| 12 |
A' |
689 |
660 |
11.54 |
0.82 |
0.71 |
0.83 |
| 13 |
A' |
289 |
277 |
7.08 |
3.38 |
0.46 |
0.63 |
| 14 |
A" |
1041 |
998 |
5.54 |
8.40 |
0.75 |
0.86 |
| 15 |
A" |
1032 |
989 |
32.25 |
0.26 |
0.75 |
0.86 |
| 16 |
A" |
1008 |
966 |
20.80 |
0.55 |
0.75 |
0.86 |
| 17 |
A" |
563 |
540 |
11.51 |
4.18 |
0.75 |
0.86 |
| 18 |
A" |
181 |
174 |
7.53 |
0.49 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13566.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 13004.4 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.884 |
-0.289 |
0.000 |
| C2 |
0.000 |
0.897 |
0.000 |
| C3 |
1.322 |
0.763 |
0.000 |
| O4 |
-0.492 |
-1.427 |
0.000 |
| H5 |
-1.971 |
-0.074 |
0.000 |
| H6 |
-0.474 |
1.873 |
0.000 |
| H7 |
1.989 |
1.616 |
0.000 |
| H8 |
1.764 |
-0.226 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4791 | 2.4443 | 1.2037 | 1.1079 | 2.2002 | 3.4470 | 2.6488 |
C2 | 1.4791 | | 1.3288 | 2.3753 | 2.1970 | 1.0847 | 2.1148 | 2.0910 | C3 | 2.4443 | 1.3288 | | 2.8440 | 3.3978 | 2.1107 | 1.0822 | 1.0836 | O4 | 1.2037 | 2.3753 | 2.8440 | | 2.0045 | 3.2997 | 3.9260 | 2.5557 | H5 | 1.1079 | 2.1970 | 3.3978 | 2.0045 | | 2.4558 | 4.3052 | 3.7380 | H6 | 2.2002 | 1.0847 | 2.1107 | 3.2997 | 2.4558 | | 2.4759 | 3.0678 | H7 | 3.4470 | 2.1148 | 1.0822 | 3.9260 | 4.3052 | 2.4759 | | 1.8556 | H8 | 2.6488 | 2.0910 | 1.0836 | 2.5557 | 3.7380 | 3.0678 | 1.8556 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.945 |
|
C1 |
C2 |
H6 |
117.398 |
| C2 |
C1 |
O4 |
124.278 |
|
C2 |
C1 |
H5 |
115.517 |
| C2 |
C3 |
H7 |
122.268 |
|
C2 |
C3 |
H8 |
119.828 |
| C3 |
C2 |
H6 |
121.657 |
|
O4 |
C1 |
H5 |
120.204 |
| H7 |
C3 |
H8 |
117.904 |
|
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 |
0.098 |
|
|
|
| 2 |
C |
-0.292 |
|
|
|
| 3 |
C |
-0.369 |
|
|
|
| 4 |
O |
-0.293 |
|
|
|
| 5 |
H |
0.167 |
|
|
|
| 6 |
H |
0.212 |
|
|
|
| 7 |
H |
0.231 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.225 |
2.631 |
0.000 |
2.641 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.993 |
-0.617 |
0.000 |
| y |
-0.617 |
-25.816 |
0.000 |
| z |
0.000 |
0.000 |
-24.807 |
|
| Traceless |
| | x | y | z |
| x |
5.319 |
-0.617 |
0.000 |
| y |
-0.617 |
-3.416 |
0.000 |
| z |
0.000 |
0.000 |
-1.903 |
|
| Polar |
| 3z2-r2 | -3.806 |
| x2-y2 | 5.823 |
| xy | -0.617 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.065 |
0.441 |
0.000 |
| y |
0.441 |
5.611 |
0.000 |
| z |
0.000 |
0.000 |
2.519 |
<r2> (average value of r
2) Å
2
| <r2> |
74.279 |
| (<r2>)1/2 |
8.619 |