Jump to
S1C2
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -192.093771 |
| Energy at 298.15K | |
| HF Energy | -192.093771 |
| Nuclear repulsion energy | 128.536202 |
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 LSDA/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 |
A1 |
3032 |
2987 |
20.21 |
|
|
|
| 2 |
A1 |
2957 |
2913 |
0.02 |
|
|
|
| 3 |
A1 |
1481 |
1459 |
0.12 |
|
|
|
| 4 |
A1 |
1426 |
1404 |
6.86 |
|
|
|
| 5 |
A1 |
1325 |
1305 |
0.70 |
|
|
|
| 6 |
A1 |
1068 |
1052 |
8.19 |
|
|
|
| 7 |
A1 |
944 |
930 |
31.94 |
|
|
|
| 8 |
A1 |
790 |
778 |
3.79 |
|
|
|
| 9 |
A2 |
2995 |
2950 |
0.00 |
|
|
|
| 10 |
A2 |
1185 |
1167 |
0.00 |
|
|
|
| 11 |
A2 |
1126 |
1109 |
0.00 |
|
|
|
| 12 |
A2 |
811 |
799 |
0.00 |
|
|
|
| 13 |
B1 |
3094 |
3047 |
13.91 |
|
|
|
| 14 |
B1 |
2994 |
2949 |
71.87 |
|
|
|
| 15 |
B1 |
1143 |
1126 |
0.63 |
|
|
|
| 16 |
B1 |
1107 |
1090 |
1.27 |
|
|
|
| 17 |
B1 |
745 |
734 |
0.92 |
|
|
|
| 18 |
B1 |
83i |
82i |
2.84 |
|
|
|
| 19 |
B2 |
2947 |
2903 |
156.92 |
|
|
|
| 20 |
B2 |
1448 |
1427 |
0.41 |
|
|
|
| 21 |
B2 |
1263 |
1244 |
0.24 |
|
|
|
| 22 |
B2 |
1211 |
1193 |
19.46 |
|
|
|
| 23 |
B2 |
1074 |
1058 |
105.67 |
|
|
|
| 24 |
B2 |
957 |
942 |
4.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18519.6 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 18241.8 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 LSDA/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.065 |
| C2 |
0.000 |
0.000 |
-1.069 |
| C3 |
0.000 |
1.026 |
0.064 |
| C4 |
0.000 |
-1.026 |
0.064 |
| H5 |
0.897 |
0.000 |
-1.707 |
| H6 |
-0.897 |
0.000 |
-1.707 |
| H7 |
0.900 |
1.668 |
0.134 |
| H8 |
-0.900 |
1.668 |
0.134 |
| H9 |
-0.900 |
-1.668 |
0.134 |
| H10 |
0.900 |
-1.668 |
0.134 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1342 | 1.4339 | 1.4339 | 2.9136 | 2.9136 | 2.1118 | 2.1118 | 2.1118 | 2.1118 |
C2 | 2.1342 | | 1.5284 | 1.5284 | 1.1005 | 1.1005 | 2.2446 | 2.2446 | 2.2446 | 2.2446 | C3 | 1.4339 | 1.5284 | | 2.0525 | 2.2344 | 2.2344 | 1.1074 | 1.1074 | 2.8414 | 2.8414 | C4 | 1.4339 | 1.5284 | 2.0525 | | 2.2344 | 2.2344 | 2.8414 | 2.8414 | 1.1074 | 1.1074 | H5 | 2.9136 | 1.1005 | 2.2344 | 2.2344 | | 1.7932 | 2.4840 | 3.0655 | 3.0655 | 2.4840 | H6 | 2.9136 | 1.1005 | 2.2344 | 2.2344 | 1.7932 | | 3.0655 | 2.4840 | 2.4840 | 3.0655 | H7 | 2.1118 | 2.2446 | 1.1074 | 2.8414 | 2.4840 | 3.0655 | | 1.7997 | 3.7904 | 3.3359 | H8 | 2.1118 | 2.2446 | 1.1074 | 2.8414 | 3.0655 | 2.4840 | 1.7997 | | 3.3359 | 3.7904 | H9 | 2.1118 | 2.2446 | 2.8414 | 1.1074 | 3.0655 | 2.4840 | 3.7904 | 3.3359 | | 1.7997 | H10 | 2.1118 | 2.2446 | 2.8414 | 1.1074 | 2.4840 | 3.0655 | 3.3359 | 3.7904 | 1.7997 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.122 |
|
O1 |
C3 |
H7 |
111.753 |
| O1 |
C3 |
H8 |
111.753 |
|
O1 |
C4 |
C2 |
92.122 |
| O1 |
C4 |
H9 |
111.753 |
|
O1 |
C4 |
H10 |
111.753 |
| C2 |
C3 |
H7 |
115.840 |
|
C2 |
C3 |
H8 |
115.840 |
| C2 |
C4 |
H9 |
115.840 |
|
C2 |
C4 |
H10 |
115.840 |
| C3 |
O1 |
C4 |
91.399 |
|
C3 |
C2 |
C4 |
84.356 |
| C3 |
C2 |
H5 |
115.447 |
|
C3 |
C2 |
H6 |
115.447 |
| C4 |
C2 |
H5 |
115.447 |
|
C4 |
C2 |
H6 |
115.447 |
| H5 |
C2 |
H6 |
109.126 |
|
H7 |
C3 |
H8 |
108.692 |
| H9 |
C4 |
H10 |
108.692 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.342 |
|
|
|
| 2 |
C |
-0.365 |
|
|
|
| 3 |
C |
-0.172 |
|
|
|
| 4 |
C |
-0.172 |
|
|
|
| 5 |
H |
0.190 |
|
|
|
| 6 |
H |
0.190 |
|
|
|
| 7 |
H |
0.168 |
|
|
|
| 8 |
H |
0.168 |
|
|
|
| 9 |
H |
0.168 |
|
|
|
| 10 |
H |
0.168 |
|
|
|
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 |
-2.115 |
2.115 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.495 |
0.000 |
0.000 |
| y |
0.000 |
-23.361 |
0.000 |
| z |
0.000 |
0.000 |
-28.438 |
|
| Traceless |
| | x | y | z |
| x |
1.405 |
0.000 |
0.000 |
| y |
0.000 |
3.105 |
0.000 |
| z |
0.000 |
0.000 |
-4.510 |
|
| Polar |
| 3z2-r2 | -9.019 |
| x2-y2 | -1.134 |
| 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 |
5.311 |
0.000 |
0.000 |
| y |
0.000 |
6.337 |
0.000 |
| z |
0.000 |
0.000 |
5.399 |
<r2> (average value of r
2) Å
2
| <r2> |
66.379 |
| (<r2>)1/2 |
8.147 |
Jump to
S1C1
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -192.093901 |
| Energy at 298.15K | -192.101157 |
| HF Energy | -192.093901 |
| Nuclear repulsion energy | 128.746710 |
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 LSDA/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' |
3093 |
3046 |
16.05 |
|
|
|
| 2 |
A' |
3029 |
2984 |
23.43 |
|
|
|
| 3 |
A' |
3009 |
2964 |
34.03 |
|
|
|
| 4 |
A' |
2942 |
2898 |
43.63 |
|
|
|
| 5 |
A' |
1477 |
1455 |
0.32 |
|
|
|
| 6 |
A' |
1423 |
1402 |
6.70 |
|
|
|
| 7 |
A' |
1320 |
1301 |
0.61 |
|
|
|
| 8 |
A' |
1156 |
1139 |
0.15 |
|
|
|
| 9 |
A' |
1116 |
1099 |
3.07 |
|
|
|
| 10 |
A' |
1070 |
1054 |
10.13 |
|
|
|
| 11 |
A' |
937 |
923 |
28.84 |
|
|
|
| 12 |
A' |
838 |
825 |
8.81 |
|
|
|
| 13 |
A' |
693 |
683 |
1.12 |
|
|
|
| 14 |
A' |
120 |
118 |
3.56 |
|
|
|
| 15 |
A" |
3011 |
2966 |
28.86 |
|
|
|
| 16 |
A" |
2933 |
2889 |
114.12 |
|
|
|
| 17 |
A" |
1444 |
1422 |
0.15 |
|
|
|
| 18 |
A" |
1260 |
1241 |
0.70 |
|
|
|
| 19 |
A" |
1215 |
1197 |
14.46 |
|
|
|
| 20 |
A" |
1175 |
1157 |
5.78 |
|
|
|
| 21 |
A" |
1119 |
1102 |
0.66 |
|
|
|
| 22 |
A" |
1060 |
1044 |
96.30 |
|
|
|
| 23 |
A" |
953 |
938 |
1.76 |
|
|
|
| 24 |
A" |
811 |
799 |
1.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18601.0 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 18322.0 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 LSDA/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.227 |
-1.039 |
0.000 |
| C2 |
-0.061 |
1.066 |
0.000 |
| C3 |
-0.061 |
-0.071 |
1.019 |
| C4 |
-0.061 |
-0.071 |
-1.019 |
| H5 |
0.871 |
1.652 |
0.000 |
| H6 |
-0.925 |
1.747 |
0.000 |
| H7 |
0.713 |
-0.057 |
1.809 |
| H8 |
-1.050 |
-0.257 |
1.486 |
| H9 |
0.713 |
-0.057 |
-1.809 |
| H10 |
-1.050 |
-0.257 |
-1.486 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1242 | 1.4347 | 1.4347 | 2.7670 | 3.0151 | 2.1143 | 2.1100 | 2.1143 | 2.1100 |
C2 | 2.1242 | | 1.5269 | 1.5269 | 1.1011 | 1.1006 | 2.2653 | 2.2223 | 2.2653 | 2.2223 | C3 | 1.4347 | 1.5269 | | 2.0385 | 2.2084 | 2.2566 | 1.1053 | 1.1100 | 2.9319 | 2.7002 | C4 | 1.4347 | 1.5269 | 2.0385 | | 2.2084 | 2.2566 | 2.9319 | 2.7002 | 1.1053 | 1.1100 | H5 | 2.7670 | 1.1011 | 2.2084 | 2.2084 | | 1.7986 | 2.4940 | 3.0899 | 2.4940 | 3.0899 | H6 | 3.0151 | 1.1006 | 2.2566 | 2.2566 | 1.7986 | | 3.0349 | 2.4986 | 3.0349 | 2.4986 | H7 | 2.1143 | 2.2653 | 1.1053 | 2.9319 | 2.4940 | 3.0349 | | 1.8033 | 3.6177 | 3.7423 | H8 | 2.1100 | 2.2223 | 1.1100 | 2.7002 | 3.0899 | 2.4986 | 1.8033 | | 3.7423 | 2.9722 | H9 | 2.1143 | 2.2653 | 2.9319 | 1.1053 | 2.4940 | 3.0349 | 3.6177 | 3.7423 | | 1.8033 | H10 | 2.1100 | 2.2223 | 2.7002 | 1.1100 | 3.0899 | 2.4986 | 3.7423 | 2.9722 | 1.8033 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.605 |
|
O1 |
C3 |
H7 |
112.050 |
| O1 |
C3 |
H8 |
111.388 |
|
O1 |
C4 |
C2 |
91.605 |
| O1 |
C4 |
H9 |
112.050 |
|
O1 |
C4 |
H10 |
111.388 |
| C2 |
C3 |
H7 |
117.884 |
|
C2 |
C3 |
H8 |
113.935 |
| C2 |
C4 |
H9 |
117.884 |
|
C2 |
C4 |
H10 |
113.935 |
| C3 |
O1 |
C4 |
90.539 |
|
C3 |
C2 |
C4 |
83.752 |
| C3 |
C2 |
H5 |
113.365 |
|
C3 |
C2 |
H6 |
117.457 |
| C4 |
C2 |
H5 |
113.365 |
|
C4 |
C2 |
H6 |
117.457 |
| H5 |
C2 |
H6 |
109.557 |
|
H7 |
C3 |
H8 |
108.985 |
| H9 |
C4 |
H10 |
108.985 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.333 |
|
|
|
| 2 |
C |
-0.357 |
|
|
|
| 3 |
C |
-0.182 |
|
|
|
| 4 |
C |
-0.182 |
|
|
|
| 5 |
H |
0.191 |
|
|
|
| 6 |
H |
0.187 |
|
|
|
| 7 |
H |
0.172 |
|
|
|
| 8 |
H |
0.167 |
|
|
|
| 9 |
H |
0.172 |
|
|
|
| 10 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.453 |
2.032 |
0.000 |
2.082 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.781 |
0.782 |
0.000 |
| y |
0.782 |
-28.275 |
0.000 |
| z |
0.000 |
0.000 |
-23.265 |
|
| Traceless |
| | x | y | z |
| x |
0.989 |
0.782 |
0.000 |
| y |
0.782 |
-4.252 |
0.000 |
| z |
0.000 |
0.000 |
3.263 |
|
| Polar |
| 3z2-r2 | 6.527 |
| x2-y2 | 3.494 |
| xy | 0.782 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.429 |
-0.040 |
0.000 |
| y |
-0.040 |
5.446 |
0.000 |
| z |
0.000 |
0.000 |
6.342 |
<r2> (average value of r
2) Å
2
| <r2> |
66.064 |
| (<r2>)1/2 |
8.128 |