Jump to
S1C2
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -192.155414 |
| Energy at 298.15K | |
| HF Energy | -192.155414 |
| Nuclear repulsion energy | 128.950096 |
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/cc-pVTZ
| 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 |
3020 |
2987 |
19.17 |
|
|
|
| 2 |
A1 |
2940 |
2908 |
0.14 |
|
|
|
| 3 |
A1 |
1471 |
1455 |
0.01 |
|
|
|
| 4 |
A1 |
1416 |
1401 |
6.46 |
|
|
|
| 5 |
A1 |
1322 |
1307 |
0.25 |
|
|
|
| 6 |
A1 |
1068 |
1057 |
6.57 |
|
|
|
| 7 |
A1 |
940 |
930 |
27.37 |
|
|
|
| 8 |
A1 |
795 |
786 |
5.19 |
|
|
|
| 9 |
A2 |
2973 |
2941 |
0.00 |
|
|
|
| 10 |
A2 |
1188 |
1175 |
0.00 |
|
|
|
| 11 |
A2 |
1126 |
1114 |
0.00 |
|
|
|
| 12 |
A2 |
807 |
799 |
0.00 |
|
|
|
| 13 |
B1 |
3077 |
3043 |
12.80 |
|
|
|
| 14 |
B1 |
2972 |
2939 |
68.78 |
|
|
|
| 15 |
B1 |
1145 |
1133 |
0.37 |
|
|
|
| 16 |
B1 |
1106 |
1093 |
1.09 |
|
|
|
| 17 |
B1 |
739 |
731 |
0.62 |
|
|
|
| 18 |
B1 |
71i |
70i |
2.10 |
|
|
|
| 19 |
B2 |
2930 |
2898 |
149.17 |
|
|
|
| 20 |
B2 |
1440 |
1424 |
0.13 |
|
|
|
| 21 |
B2 |
1258 |
1244 |
0.01 |
|
|
|
| 22 |
B2 |
1211 |
1197 |
15.72 |
|
|
|
| 23 |
B2 |
1066 |
1054 |
100.90 |
|
|
|
| 24 |
B2 |
952 |
942 |
4.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18445.5 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 18244.4 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 LSDA/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.062 |
| C2 |
0.000 |
0.000 |
-1.064 |
| C3 |
0.000 |
1.024 |
0.064 |
| C4 |
0.000 |
-1.024 |
0.064 |
| H5 |
0.893 |
0.000 |
-1.699 |
| H6 |
-0.893 |
0.000 |
-1.699 |
| H7 |
0.896 |
1.665 |
0.130 |
| H8 |
-0.896 |
1.665 |
0.130 |
| H9 |
-0.896 |
-1.665 |
0.130 |
| H10 |
0.896 |
-1.665 |
0.130 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1251 | 1.4296 | 1.4296 | 2.9017 | 2.9017 | 2.1081 | 2.1081 | 2.1081 | 2.1081 |
C2 | 2.1251 | | 1.5232 | 1.5232 | 1.0961 | 1.0961 | 2.2360 | 2.2360 | 2.2360 | 2.2360 | C3 | 1.4296 | 1.5232 | | 2.0481 | 2.2260 | 2.2260 | 1.1039 | 1.1039 | 2.8353 | 2.8353 | C4 | 1.4296 | 1.5232 | 2.0481 | | 2.2260 | 2.2260 | 2.8353 | 2.8353 | 1.1039 | 1.1039 | H5 | 2.9017 | 1.0961 | 2.2260 | 2.2260 | | 1.7856 | 2.4735 | 3.0528 | 3.0528 | 2.4735 | H6 | 2.9017 | 1.0961 | 2.2260 | 2.2260 | 1.7856 | | 3.0528 | 2.4735 | 2.4735 | 3.0528 | H7 | 2.1081 | 2.2360 | 1.1039 | 2.8353 | 2.4735 | 3.0528 | | 1.7928 | 3.7819 | 3.3300 | H8 | 2.1081 | 2.2360 | 1.1039 | 2.8353 | 3.0528 | 2.4735 | 1.7928 | | 3.3300 | 3.7819 | H9 | 2.1081 | 2.2360 | 2.8353 | 1.1039 | 3.0528 | 2.4735 | 3.7819 | 3.3300 | | 1.7928 | H10 | 2.1081 | 2.2360 | 2.8353 | 1.1039 | 2.4735 | 3.0528 | 3.3300 | 3.7819 | 1.7928 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.002 |
|
O1 |
C3 |
H7 |
111.982 |
| O1 |
C3 |
H8 |
111.982 |
|
O1 |
C4 |
C2 |
92.002 |
| O1 |
C4 |
H9 |
111.982 |
|
O1 |
C4 |
H10 |
111.982 |
| C2 |
C3 |
H7 |
115.751 |
|
C2 |
C3 |
H8 |
115.751 |
| C2 |
C4 |
H9 |
115.751 |
|
C2 |
C4 |
H10 |
115.751 |
| C3 |
O1 |
C4 |
91.504 |
|
C3 |
C2 |
C4 |
84.493 |
| C3 |
C2 |
H5 |
115.431 |
|
C3 |
C2 |
H6 |
115.431 |
| C4 |
C2 |
H5 |
115.431 |
|
C4 |
C2 |
H6 |
115.431 |
| H5 |
C2 |
H6 |
109.086 |
|
H7 |
C3 |
H8 |
108.586 |
| H9 |
C4 |
H10 |
108.586 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.254 |
|
|
|
| 2 |
C |
-0.296 |
|
|
|
| 3 |
C |
-0.003 |
|
|
|
| 4 |
C |
-0.003 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.120 |
|
|
|
| 7 |
H |
0.079 |
|
|
|
| 8 |
H |
0.079 |
|
|
|
| 9 |
H |
0.079 |
|
|
|
| 10 |
H |
0.079 |
|
|
|
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 |
-1.813 |
1.813 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.340 |
0.000 |
0.000 |
| y |
0.000 |
-23.413 |
0.000 |
| z |
0.000 |
0.000 |
-27.854 |
|
| Traceless |
| | x | y | z |
| x |
1.294 |
0.000 |
0.000 |
| y |
0.000 |
2.684 |
0.000 |
| z |
0.000 |
0.000 |
-3.978 |
|
| Polar |
| 3z2-r2 | -7.956 |
| x2-y2 | -0.927 |
| 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 |
5.367 |
0.000 |
0.000 |
| y |
0.000 |
6.517 |
0.000 |
| z |
0.000 |
0.000 |
5.430 |
<r2> (average value of r
2) Å
2
| <r2> |
65.916 |
| (<r2>)1/2 |
8.119 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -192.155479 |
| Energy at 298.15K | -192.162725 |
| HF Energy | -192.155479 |
| Nuclear repulsion energy | 129.118120 |
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/cc-pVTZ
| 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' |
3076 |
3042 |
14.40 |
|
|
|
| 2 |
A' |
3017 |
2984 |
20.94 |
|
|
|
| 3 |
A' |
2987 |
2955 |
34.37 |
|
|
|
| 4 |
A' |
2926 |
2894 |
38.80 |
|
|
|
| 5 |
A' |
1468 |
1452 |
0.27 |
|
|
|
| 6 |
A' |
1413 |
1398 |
6.39 |
|
|
|
| 7 |
A' |
1318 |
1304 |
0.18 |
|
|
|
| 8 |
A' |
1155 |
1143 |
0.15 |
|
|
|
| 9 |
A' |
1113 |
1100 |
2.36 |
|
|
|
| 10 |
A' |
1070 |
1058 |
7.90 |
|
|
|
| 11 |
A' |
935 |
925 |
25.04 |
|
|
|
| 12 |
A' |
834 |
825 |
8.66 |
|
|
|
| 13 |
A' |
696 |
689 |
1.08 |
|
|
|
| 14 |
A' |
107 |
106 |
2.51 |
|
|
|
| 15 |
A" |
2988 |
2956 |
27.84 |
|
|
|
| 16 |
A" |
2917 |
2885 |
110.71 |
|
|
|
| 17 |
A" |
1436 |
1420 |
0.03 |
|
|
|
| 18 |
A" |
1255 |
1241 |
0.02 |
|
|
|
| 19 |
A" |
1215 |
1202 |
12.13 |
|
|
|
| 20 |
A" |
1178 |
1165 |
4.40 |
|
|
|
| 21 |
A" |
1121 |
1109 |
0.34 |
|
|
|
| 22 |
A" |
1055 |
1043 |
94.47 |
|
|
|
| 23 |
A" |
950 |
940 |
2.71 |
|
|
|
| 24 |
A" |
807 |
798 |
0.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18518.3 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 18316.5 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.201 |
-1.041 |
0.000 |
| C2 |
-0.054 |
1.061 |
0.000 |
| C3 |
-0.054 |
-0.070 |
1.018 |
| C4 |
-0.054 |
-0.070 |
-1.018 |
| H5 |
0.872 |
1.650 |
0.000 |
| H6 |
-0.916 |
1.738 |
0.000 |
| H7 |
0.732 |
-0.058 |
1.790 |
| H8 |
-1.032 |
-0.238 |
1.507 |
| H9 |
0.732 |
-0.058 |
-1.790 |
| H10 |
-1.032 |
-0.238 |
-1.507 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1176 | 1.4302 | 1.4302 | 2.7730 | 2.9948 | 2.1101 | 2.1067 | 2.1101 | 2.1067 |
C2 | 2.1176 | | 1.5218 | 1.5218 | 1.0967 | 1.0961 | 2.2530 | 2.2171 | 2.2530 | 2.2171 | C3 | 1.4302 | 1.5218 | | 2.0368 | 2.2023 | 2.2466 | 1.1017 | 1.1063 | 2.9166 | 2.7137 | C4 | 1.4302 | 1.5218 | 2.0368 | | 2.2023 | 2.2466 | 2.9166 | 2.7137 | 1.1017 | 1.1063 | H5 | 2.7730 | 1.0967 | 2.2023 | 2.2023 | | 1.7901 | 2.4783 | 3.0754 | 2.4783 | 3.0754 | H6 | 2.9948 | 1.0961 | 2.2466 | 2.2466 | 1.7901 | | 3.0245 | 2.4873 | 3.0245 | 2.4873 | H7 | 2.1101 | 2.2530 | 1.1017 | 2.9166 | 2.4783 | 3.0245 | | 1.7957 | 3.5806 | 3.7441 | H8 | 2.1067 | 2.2171 | 1.1063 | 2.7137 | 3.0754 | 2.4873 | 1.7957 | | 3.7441 | 3.0146 | H9 | 2.1101 | 2.2530 | 2.9166 | 1.1017 | 2.4783 | 3.0245 | 3.5806 | 3.7441 | | 1.7957 | H10 | 2.1067 | 2.2171 | 2.7137 | 1.1063 | 3.0754 | 2.4873 | 3.7441 | 3.0146 | 1.7957 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.613 |
|
O1 |
C3 |
H7 |
112.250 |
| O1 |
C3 |
H8 |
111.669 |
|
O1 |
C4 |
C2 |
91.613 |
| O1 |
C4 |
H9 |
112.250 |
|
O1 |
C4 |
H10 |
111.669 |
| C2 |
C3 |
H7 |
117.462 |
|
C2 |
C3 |
H8 |
114.115 |
| C2 |
C4 |
H9 |
117.462 |
|
C2 |
C4 |
H10 |
114.115 |
| C3 |
O1 |
C4 |
90.804 |
|
C3 |
C2 |
C4 |
84.008 |
| C3 |
C2 |
H5 |
113.505 |
|
C3 |
C2 |
H6 |
117.291 |
| C4 |
C2 |
H5 |
113.505 |
|
C4 |
C2 |
H6 |
117.291 |
| H5 |
C2 |
H6 |
109.441 |
|
H7 |
C3 |
H8 |
108.827 |
| H9 |
C4 |
H10 |
108.827 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.251 |
|
|
|
| 2 |
C |
-0.284 |
|
|
|
| 3 |
C |
-0.011 |
|
|
|
| 4 |
C |
-0.011 |
|
|
|
| 5 |
H |
0.117 |
|
|
|
| 6 |
H |
0.118 |
|
|
|
| 7 |
H |
0.087 |
|
|
|
| 8 |
H |
0.074 |
|
|
|
| 9 |
H |
0.087 |
|
|
|
| 10 |
H |
0.074 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.345 |
1.757 |
0.000 |
1.790 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.544 |
0.615 |
0.000 |
| y |
0.615 |
-27.747 |
0.000 |
| z |
0.000 |
0.000 |
-23.339 |
|
| Traceless |
| | x | y | z |
| x |
0.999 |
0.615 |
0.000 |
| y |
0.615 |
-3.805 |
0.000 |
| z |
0.000 |
0.000 |
2.807 |
|
| Polar |
| 3z2-r2 | 5.613 |
| x2-y2 | 3.203 |
| xy | 0.615 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.423 |
-0.002 |
0.000 |
| y |
-0.002 |
5.453 |
0.000 |
| z |
0.000 |
0.000 |
6.500 |
<r2> (average value of r
2) Å
2
| <r2> |
65.667 |
| (<r2>)1/2 |
8.104 |