Jump to
S1C2
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -191.823798 |
| Energy at 298.15K | |
| HF Energy | -191.823798 |
| Nuclear repulsion energy | 103.258814 |
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 B1B95/6-31G**
| 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' |
3282 |
3133 |
6.30 |
65.10 |
0.53 |
0.69 |
| 2 |
A' |
3232 |
3086 |
1.82 |
94.13 |
0.32 |
0.49 |
| 3 |
A' |
3186 |
3042 |
5.53 |
67.73 |
0.11 |
0.19 |
| 4 |
A' |
2933 |
2800 |
102.29 |
84.17 |
0.29 |
0.45 |
| 5 |
A' |
1846 |
1763 |
222.36 |
59.21 |
0.38 |
0.55 |
| 6 |
A' |
1724 |
1646 |
2.54 |
26.50 |
0.20 |
0.33 |
| 7 |
A' |
1476 |
1409 |
11.55 |
6.81 |
0.53 |
0.69 |
| 8 |
A' |
1412 |
1348 |
5.89 |
21.28 |
0.45 |
0.62 |
| 9 |
A' |
1309 |
1250 |
3.43 |
6.77 |
0.35 |
0.51 |
| 10 |
A' |
1187 |
1133 |
36.05 |
11.97 |
0.63 |
0.77 |
| 11 |
A' |
933 |
891 |
19.74 |
1.17 |
0.11 |
0.20 |
| 12 |
A' |
575 |
549 |
6.29 |
5.12 |
0.35 |
0.52 |
| 13 |
A' |
316 |
302 |
9.54 |
0.86 |
0.35 |
0.52 |
| 14 |
A" |
1047 |
1000 |
8.69 |
2.40 |
0.75 |
0.86 |
| 15 |
A" |
1030 |
983 |
7.82 |
4.33 |
0.75 |
0.86 |
| 16 |
A" |
1000 |
955 |
41.08 |
0.40 |
0.75 |
0.86 |
| 17 |
A" |
613 |
585 |
8.82 |
4.53 |
0.75 |
0.86 |
| 18 |
A" |
173 |
165 |
4.00 |
1.58 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13636.3 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 13019.9 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 B1B95/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.151 |
-0.742 |
0.000 |
| C2 |
0.000 |
0.720 |
0.000 |
| C3 |
1.211 |
1.277 |
0.000 |
| O4 |
-1.215 |
-1.318 |
0.000 |
| H5 |
0.807 |
-1.305 |
0.000 |
| H6 |
-0.913 |
1.307 |
0.000 |
| H7 |
1.357 |
2.351 |
0.000 |
| H8 |
2.107 |
0.662 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4694 | 2.4352 | 1.2094 | 1.1113 | 2.1855 | 3.4406 | 2.6588 |
C2 | 1.4694 | | 1.3329 | 2.3722 | 2.1793 | 1.0851 | 2.1215 | 2.1078 | C3 | 2.4352 | 1.3329 | | 3.5518 | 2.6126 | 2.1239 | 1.0837 | 1.0868 | O4 | 1.2094 | 2.3722 | 3.5518 | | 2.0218 | 2.6418 | 4.4800 | 3.8667 | H5 | 1.1113 | 2.1793 | 2.6126 | 2.0218 | | 3.1267 | 3.6962 | 2.3570 | H6 | 2.1855 | 1.0851 | 2.1239 | 2.6418 | 3.1267 | | 2.4983 | 3.0878 | H7 | 3.4406 | 2.1215 | 1.0837 | 4.4800 | 3.6962 | 2.4983 | | 1.8480 | H8 | 2.6588 | 2.1078 | 1.0868 | 3.8667 | 2.3570 | 3.0878 | 1.8480 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.604 |
|
C1 |
C2 |
H6 |
116.836 |
| C2 |
C1 |
O4 |
124.348 |
|
C2 |
C1 |
H5 |
114.512 |
| C2 |
C3 |
H7 |
122.439 |
|
C2 |
C3 |
H8 |
120.833 |
| C3 |
C2 |
H6 |
122.560 |
|
O4 |
C1 |
H5 |
121.140 |
| H7 |
C3 |
H8 |
116.728 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.225 |
|
|
|
| 2 |
C |
-0.138 |
|
|
|
| 3 |
C |
-0.354 |
|
|
|
| 4 |
O |
-0.406 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.185 |
|
|
|
| 7 |
H |
0.188 |
|
|
|
| 8 |
H |
0.180 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.392 |
2.061 |
0.000 |
3.157 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.851 |
-2.497 |
0.000 |
| y |
-2.497 |
-23.457 |
0.000 |
| z |
0.000 |
0.000 |
-24.300 |
|
| Traceless |
| | x | y | z |
| x |
0.028 |
-2.497 |
0.000 |
| y |
-2.497 |
0.618 |
0.000 |
| z |
0.000 |
0.000 |
-0.646 |
|
| Polar |
| 3z2-r2 | -1.293 |
| x2-y2 | -0.393 |
| xy | -2.497 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.624 |
1.655 |
0.000 |
| y |
1.655 |
6.064 |
0.000 |
| z |
0.000 |
0.000 |
2.069 |
<r2> (average value of r
2) Å
2
| <r2> |
82.868 |
| (<r2>)1/2 |
9.103 |
Jump to
S1C1
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -191.821274 |
| Energy at 298.15K | |
| HF Energy | -191.821274 |
| Nuclear repulsion energy | 104.930587 |
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 B1B95/6-31G**
| 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' |
3294 |
3145 |
2.52 |
52.86 |
0.64 |
0.78 |
| 2 |
A' |
3218 |
3072 |
10.63 |
120.11 |
0.23 |
0.37 |
| 3 |
A' |
3196 |
3052 |
5.16 |
46.66 |
0.16 |
0.28 |
| 4 |
A' |
2967 |
2833 |
146.55 |
142.45 |
0.32 |
0.49 |
| 5 |
A' |
1843 |
1760 |
107.36 |
12.96 |
0.49 |
0.66 |
| 6 |
A' |
1713 |
1636 |
65.20 |
42.85 |
0.22 |
0.37 |
| 7 |
A' |
1457 |
1391 |
32.63 |
9.68 |
0.75 |
0.85 |
| 8 |
A' |
1445 |
1379 |
11.23 |
8.68 |
0.25 |
0.40 |
| 9 |
A' |
1327 |
1267 |
1.97 |
15.24 |
0.44 |
0.61 |
| 10 |
A' |
1076 |
1027 |
4.95 |
4.94 |
0.73 |
0.84 |
| 11 |
A' |
956 |
912 |
60.21 |
4.66 |
0.21 |
0.35 |
| 12 |
A' |
687 |
656 |
11.56 |
0.72 |
0.74 |
0.85 |
| 13 |
A' |
292 |
279 |
7.12 |
2.98 |
0.47 |
0.64 |
| 14 |
A" |
1045 |
998 |
8.55 |
9.23 |
0.75 |
0.86 |
| 15 |
A" |
1036 |
989 |
25.32 |
0.98 |
0.75 |
0.86 |
| 16 |
A" |
1010 |
964 |
15.96 |
0.15 |
0.75 |
0.86 |
| 17 |
A" |
566 |
540 |
7.79 |
6.61 |
0.75 |
0.86 |
| 18 |
A" |
182 |
174 |
7.48 |
0.91 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13653.8 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 13036.7 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 B1B95/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.887 |
-0.284 |
0.000 |
| C2 |
0.000 |
0.899 |
0.000 |
| C3 |
1.325 |
0.758 |
0.000 |
| O4 |
-0.492 |
-1.428 |
0.000 |
| H5 |
-1.974 |
-0.066 |
0.000 |
| H6 |
-0.471 |
1.878 |
0.000 |
| H7 |
1.997 |
1.608 |
0.000 |
| H8 |
1.759 |
-0.237 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4787 | 2.4454 | 1.2108 | 1.1081 | 2.2014 | 3.4495 | 2.6468 |
C2 | 1.4787 | | 1.3327 | 2.3791 | 2.1972 | 1.0859 | 2.1194 | 2.0940 | C3 | 2.4454 | 1.3327 | | 2.8431 | 3.4004 | 2.1164 | 1.0837 | 1.0851 | O4 | 1.2108 | 2.3791 | 2.8431 | | 2.0125 | 3.3063 | 3.9266 | 2.5475 | H5 | 1.1081 | 2.1972 | 3.4004 | 2.0125 | | 2.4575 | 4.3096 | 3.7368 | H6 | 2.2014 | 1.0859 | 2.1164 | 3.3063 | 2.4575 | | 2.4826 | 3.0729 | H7 | 3.4495 | 2.1194 | 1.0837 | 3.9266 | 4.3096 | 2.4826 | | 1.8599 | H8 | 2.6468 | 2.0940 | 1.0851 | 2.5475 | 3.7368 | 3.0729 | 1.8599 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.783 |
|
C1 |
C2 |
H6 |
117.452 |
| C2 |
C1 |
O4 |
124.098 |
|
C2 |
C1 |
H5 |
115.550 |
| C2 |
C3 |
H7 |
122.245 |
|
C2 |
C3 |
H8 |
119.661 |
| C3 |
C2 |
H6 |
121.766 |
|
O4 |
C1 |
H5 |
120.352 |
| H7 |
C3 |
H8 |
118.095 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.216 |
|
|
|
| 2 |
C |
-0.169 |
|
|
|
| 3 |
C |
-0.323 |
|
|
|
| 4 |
O |
-0.399 |
|
|
|
| 5 |
H |
0.124 |
|
|
|
| 6 |
H |
0.167 |
|
|
|
| 7 |
H |
0.180 |
|
|
|
| 8 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.261 |
2.617 |
0.000 |
2.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.810 |
-0.647 |
0.000 |
| y |
-0.647 |
-25.502 |
0.000 |
| z |
0.000 |
0.000 |
-24.277 |
|
| Traceless |
| | x | y | z |
| x |
5.080 |
-0.647 |
0.000 |
| y |
-0.647 |
-3.459 |
0.000 |
| z |
0.000 |
0.000 |
-1.621 |
|
| Polar |
| 3z2-r2 | -3.241 |
| x2-y2 | 5.692 |
| xy | -0.647 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.780 |
0.494 |
0.000 |
| y |
0.494 |
5.455 |
0.000 |
| z |
0.000 |
0.000 |
2.066 |
<r2> (average value of r
2) Å
2
| <r2> |
74.164 |
| (<r2>)1/2 |
8.612 |