Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -191.838880 |
| Energy at 298.15K | |
| HF Energy | -191.838880 |
| Nuclear repulsion energy | 103.199868 |
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 B1B95/6-31+G**
| 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' |
3276 |
3134 |
4.66 |
70.89 |
0.53 |
0.70 |
| 2 |
A' |
3225 |
3085 |
1.27 |
101.18 |
0.31 |
0.48 |
| 3 |
A' |
3176 |
3038 |
4.87 |
78.51 |
0.13 |
0.23 |
| 4 |
A' |
2938 |
2811 |
89.84 |
104.31 |
0.32 |
0.48 |
| 5 |
A' |
1822 |
1743 |
278.24 |
91.61 |
0.37 |
0.54 |
| 6 |
A' |
1708 |
1634 |
2.10 |
48.89 |
0.11 |
0.20 |
| 7 |
A' |
1461 |
1398 |
13.08 |
6.53 |
0.52 |
0.69 |
| 8 |
A' |
1395 |
1334 |
5.54 |
22.64 |
0.36 |
0.53 |
| 9 |
A' |
1300 |
1243 |
3.42 |
9.24 |
0.19 |
0.31 |
| 10 |
A' |
1183 |
1132 |
38.32 |
12.66 |
0.65 |
0.78 |
| 11 |
A' |
929 |
888 |
20.50 |
1.34 |
0.01 |
0.01 |
| 12 |
A' |
574 |
549 |
5.80 |
5.65 |
0.24 |
0.38 |
| 13 |
A' |
318 |
304 |
10.53 |
1.02 |
0.34 |
0.50 |
| 14 |
A" |
1037 |
992 |
12.08 |
1.71 |
0.75 |
0.86 |
| 15 |
A" |
1028 |
983 |
5.54 |
3.49 |
0.75 |
0.86 |
| 16 |
A" |
1002 |
959 |
51.27 |
2.09 |
0.75 |
0.86 |
| 17 |
A" |
611 |
585 |
12.09 |
1.35 |
0.75 |
0.86 |
| 18 |
A" |
170 |
162 |
4.64 |
0.68 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13575.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 12986.2 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.150 |
-0.741 |
0.000 |
| C2 |
0.000 |
0.720 |
0.000 |
| C3 |
1.213 |
1.277 |
0.000 |
| O4 |
-1.216 |
-1.317 |
0.000 |
| H5 |
0.802 |
-1.310 |
0.000 |
| H6 |
-0.912 |
1.308 |
0.000 |
| H7 |
1.356 |
2.350 |
0.000 |
| H8 |
2.108 |
0.660 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4689 | 2.4355 | 1.2115 | 1.1098 | 2.1858 | 3.4392 | 2.6580 |
C2 | 1.4689 | | 1.3349 | 2.3726 | 2.1831 | 1.0849 | 2.1207 | 2.1087 | C3 | 2.4355 | 1.3349 | | 3.5540 | 2.6195 | 2.1253 | 1.0832 | 1.0863 | O4 | 1.2115 | 2.3726 | 3.5540 | | 2.0186 | 2.6425 | 4.4798 | 3.8680 | H5 | 1.1098 | 2.1831 | 2.6195 | 2.0186 | | 3.1293 | 3.7024 | 2.3641 | H6 | 2.1858 | 1.0849 | 2.1253 | 2.6425 | 3.1293 | | 2.4962 | 3.0883 | H7 | 3.4392 | 2.1207 | 1.0832 | 4.4798 | 3.7024 | 2.4962 | | 1.8495 | H8 | 2.6580 | 2.1087 | 1.0863 | 3.8680 | 2.3641 | 3.0883 | 1.8495 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.527 |
|
C1 |
C2 |
H6 |
116.923 |
| C2 |
C1 |
O4 |
124.264 |
|
C2 |
C1 |
H5 |
114.975 |
| C2 |
C3 |
H7 |
122.231 |
|
C2 |
C3 |
H8 |
120.796 |
| C3 |
C2 |
H6 |
122.549 |
|
O4 |
C1 |
H5 |
120.761 |
| H7 |
C3 |
H8 |
116.974 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.017 |
|
|
|
| 2 |
C |
0.123 |
|
|
|
| 3 |
C |
-0.376 |
|
|
|
| 4 |
O |
-0.390 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.175 |
|
|
|
| 7 |
H |
0.169 |
|
|
|
| 8 |
H |
0.161 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.665 |
2.203 |
0.000 |
3.458 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.759 |
-2.880 |
0.000 |
| y |
-2.880 |
-24.087 |
0.000 |
| z |
0.000 |
0.000 |
-25.105 |
|
| Traceless |
| | x | y | z |
| x |
-0.163 |
-2.880 |
0.000 |
| y |
-2.880 |
0.845 |
0.000 |
| z |
0.000 |
0.000 |
-0.682 |
|
| Polar |
| 3z2-r2 | -1.365 |
| x2-y2 | -0.672 |
| xy | -2.880 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.514 |
1.902 |
0.000 |
| y |
1.902 |
6.768 |
0.000 |
| z |
0.000 |
0.000 |
3.453 |
<r2> (average value of r
2) Å
2
| <r2> |
83.411 |
| (<r2>)1/2 |
9.133 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -191.835642 |
| Energy at 298.15K | |
| HF Energy | -191.835642 |
| Nuclear repulsion energy | 104.774127 |
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 B1B95/6-31+G**
| 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' |
3286 |
3144 |
1.65 |
57.77 |
0.62 |
0.77 |
| 2 |
A' |
3211 |
3072 |
10.40 |
128.81 |
0.25 |
0.40 |
| 3 |
A' |
3184 |
3046 |
4.41 |
59.75 |
0.16 |
0.27 |
| 4 |
A' |
2968 |
2840 |
130.66 |
171.60 |
0.32 |
0.49 |
| 5 |
A' |
1821 |
1742 |
139.28 |
22.31 |
0.61 |
0.76 |
| 6 |
A' |
1699 |
1626 |
72.10 |
66.74 |
0.13 |
0.24 |
| 7 |
A' |
1441 |
1379 |
39.19 |
7.45 |
0.75 |
0.86 |
| 8 |
A' |
1429 |
1367 |
6.35 |
9.74 |
0.17 |
0.29 |
| 9 |
A' |
1315 |
1258 |
2.19 |
19.16 |
0.29 |
0.45 |
| 10 |
A' |
1071 |
1024 |
4.64 |
4.05 |
0.73 |
0.84 |
| 11 |
A' |
949 |
908 |
63.48 |
6.32 |
0.13 |
0.23 |
| 12 |
A' |
685 |
655 |
12.20 |
1.02 |
0.75 |
0.86 |
| 13 |
A' |
285 |
273 |
7.22 |
3.74 |
0.40 |
0.57 |
| 14 |
A" |
1041 |
996 |
3.13 |
7.03 |
0.75 |
0.86 |
| 15 |
A" |
1027 |
982 |
49.63 |
0.76 |
0.75 |
0.86 |
| 16 |
A" |
1015 |
971 |
7.41 |
0.61 |
0.75 |
0.86 |
| 17 |
A" |
560 |
536 |
11.96 |
2.05 |
0.75 |
0.86 |
| 18 |
A" |
159 |
152 |
7.59 |
0.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13573.3 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 12984.2 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.887 |
-0.287 |
0.000 |
| C2 |
0.000 |
0.897 |
0.000 |
| C3 |
1.328 |
0.767 |
0.000 |
| O4 |
-0.495 |
-1.434 |
0.000 |
| H5 |
-1.973 |
-0.073 |
0.000 |
| H6 |
-0.476 |
1.872 |
0.000 |
| H7 |
1.987 |
1.627 |
0.000 |
| H8 |
1.775 |
-0.222 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4790 | 2.4535 | 1.2126 | 1.1068 | 2.1977 | 3.4530 | 2.6629 |
C2 | 1.4790 | | 1.3345 | 2.3822 | 2.1985 | 1.0856 | 2.1167 | 2.0976 | C3 | 2.4535 | 1.3345 | | 2.8577 | 3.4067 | 2.1158 | 1.0832 | 1.0849 | O4 | 1.2126 | 2.3822 | 2.8577 | | 2.0098 | 3.3060 | 3.9403 | 2.5727 | H5 | 1.1068 | 2.1985 | 3.4067 | 2.0098 | | 2.4545 | 4.3094 | 3.7510 | H6 | 2.1977 | 1.0856 | 2.1158 | 3.3060 | 2.4545 | | 2.4748 | 3.0741 | H7 | 3.4530 | 2.1167 | 1.0832 | 3.9403 | 4.3094 | 2.4748 | | 1.8610 | H8 | 2.6629 | 2.0976 | 1.0849 | 2.5727 | 3.7510 | 3.0741 | 1.8610 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.307 |
|
C1 |
C2 |
H6 |
117.118 |
| C2 |
C1 |
O4 |
124.222 |
|
C2 |
C1 |
H5 |
115.727 |
| C2 |
C3 |
H7 |
121.865 |
|
C2 |
C3 |
H8 |
119.866 |
| C3 |
C2 |
H6 |
121.575 |
|
O4 |
C1 |
H5 |
120.050 |
| H7 |
C3 |
H8 |
118.269 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.070 |
|
|
|
| 2 |
C |
0.052 |
|
|
|
| 3 |
C |
-0.355 |
|
|
|
| 4 |
O |
-0.395 |
|
|
|
| 5 |
H |
0.121 |
|
|
|
| 6 |
H |
0.156 |
|
|
|
| 7 |
H |
0.163 |
|
|
|
| 8 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.254 |
2.853 |
0.000 |
2.864 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.086 |
-0.700 |
0.000 |
| y |
-0.700 |
-26.556 |
0.000 |
| z |
0.000 |
0.000 |
-25.069 |
|
| Traceless |
| | x | y | z |
| x |
5.726 |
-0.700 |
0.000 |
| y |
-0.700 |
-3.978 |
0.000 |
| z |
0.000 |
0.000 |
-1.749 |
|
| Polar |
| 3z2-r2 | -3.497 |
| x2-y2 | 6.469 |
| xy | -0.700 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.446 |
0.505 |
0.000 |
| y |
0.505 |
6.189 |
0.000 |
| z |
0.000 |
0.000 |
3.437 |
<r2> (average value of r
2) Å
2
| <r2> |
74.913 |
| (<r2>)1/2 |
8.655 |