Jump to
S1C2
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -192.077097 |
| Energy at 298.15K | |
| HF Energy | -192.077097 |
| Nuclear repulsion energy | 128.718987 |
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/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3040 |
2983 |
18.33 |
|
|
|
| 2 |
A1 |
2956 |
2901 |
0.64 |
|
|
|
| 3 |
A1 |
1514 |
1486 |
0.04 |
|
|
|
| 4 |
A1 |
1450 |
1423 |
4.28 |
|
|
|
| 5 |
A1 |
1349 |
1324 |
1.59 |
|
|
|
| 6 |
A1 |
1082 |
1062 |
7.21 |
|
|
|
| 7 |
A1 |
954 |
936 |
24.08 |
|
|
|
| 8 |
A1 |
796 |
781 |
2.96 |
|
|
|
| 9 |
A2 |
2987 |
2931 |
0.00 |
|
|
|
| 10 |
A2 |
1200 |
1178 |
0.00 |
|
|
|
| 11 |
A2 |
1141 |
1120 |
0.00 |
|
|
|
| 12 |
A2 |
820 |
805 |
0.00 |
|
|
|
| 13 |
B1 |
3099 |
3041 |
15.00 |
|
|
|
| 14 |
B1 |
2987 |
2931 |
90.76 |
|
|
|
| 15 |
B1 |
1155 |
1134 |
1.56 |
|
|
|
| 16 |
B1 |
1119 |
1098 |
0.48 |
|
|
|
| 17 |
B1 |
749 |
735 |
0.68 |
|
|
|
| 18 |
B1 |
63i |
62i |
1.53 |
|
|
|
| 19 |
B2 |
2943 |
2888 |
160.31 |
|
|
|
| 20 |
B2 |
1479 |
1451 |
2.44 |
|
|
|
| 21 |
B2 |
1273 |
1249 |
0.15 |
|
|
|
| 22 |
B2 |
1222 |
1200 |
16.38 |
|
|
|
| 23 |
B2 |
1091 |
1070 |
108.25 |
|
|
|
| 24 |
B2 |
964 |
946 |
3.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18653.0 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 18304.2 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 LSDA/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.064 |
| C2 |
0.000 |
0.000 |
-1.068 |
| C3 |
0.000 |
1.023 |
0.066 |
| C4 |
0.000 |
-1.023 |
0.066 |
| H5 |
0.897 |
0.000 |
-1.707 |
| H6 |
-0.897 |
0.000 |
-1.707 |
| H7 |
0.899 |
1.669 |
0.129 |
| H8 |
-0.899 |
1.669 |
0.129 |
| H9 |
-0.899 |
-1.669 |
0.129 |
| H10 |
0.899 |
-1.669 |
0.129 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1324 | 1.4286 | 1.4286 | 2.9120 | 2.9120 | 2.1135 | 2.1135 | 2.1135 | 2.1135 |
C2 | 2.1324 | | 1.5275 | 1.5275 | 1.1007 | 1.1007 | 2.2423 | 2.2423 | 2.2423 | 2.2423 | C3 | 1.4286 | 1.5275 | | 2.0451 | 2.2345 | 2.2345 | 1.1088 | 1.1088 | 2.8384 | 2.8384 | C4 | 1.4286 | 1.5275 | 2.0451 | | 2.2345 | 2.2345 | 2.8384 | 2.8384 | 1.1088 | 1.1088 | H5 | 2.9120 | 1.1007 | 2.2345 | 2.2345 | | 1.7937 | 2.4812 | 3.0627 | 3.0627 | 2.4812 | H6 | 2.9120 | 1.1007 | 2.2345 | 2.2345 | 1.7937 | | 3.0627 | 2.4812 | 2.4812 | 3.0627 | H7 | 2.1135 | 2.2423 | 1.1088 | 2.8384 | 2.4812 | 3.0627 | | 1.7972 | 3.7913 | 3.3383 | H8 | 2.1135 | 2.2423 | 1.1088 | 2.8384 | 3.0627 | 2.4812 | 1.7972 | | 3.3383 | 3.7913 | H9 | 2.1135 | 2.2423 | 2.8384 | 1.1088 | 3.0627 | 2.4812 | 3.7913 | 3.3383 | | 1.7972 | H10 | 2.1135 | 2.2423 | 2.8384 | 1.1088 | 2.4812 | 3.0627 | 3.3383 | 3.7913 | 1.7972 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.269 |
|
O1 |
C3 |
H7 |
112.190 |
| O1 |
C3 |
H8 |
112.190 |
|
O1 |
C4 |
C2 |
92.269 |
| O1 |
C4 |
H9 |
112.190 |
|
O1 |
C4 |
H10 |
112.190 |
| C2 |
C3 |
H7 |
115.632 |
|
C2 |
C3 |
H8 |
115.632 |
| C2 |
C4 |
H9 |
115.632 |
|
C2 |
C4 |
H10 |
115.632 |
| C3 |
O1 |
C4 |
91.415 |
|
C3 |
C2 |
C4 |
84.047 |
| C3 |
C2 |
H5 |
115.510 |
|
C3 |
C2 |
H6 |
115.510 |
| C4 |
C2 |
H5 |
115.510 |
|
C4 |
C2 |
H6 |
115.510 |
| H5 |
C2 |
H6 |
109.135 |
|
H7 |
C3 |
H8 |
108.270 |
| H9 |
C4 |
H10 |
108.270 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.419 |
|
|
|
| 2 |
C |
-0.414 |
|
|
|
| 3 |
C |
-0.092 |
|
|
|
| 4 |
C |
-0.092 |
|
|
|
| 5 |
H |
0.183 |
|
|
|
| 6 |
H |
0.183 |
|
|
|
| 7 |
H |
0.163 |
|
|
|
| 8 |
H |
0.163 |
|
|
|
| 9 |
H |
0.163 |
|
|
|
| 10 |
H |
0.163 |
|
|
|
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 |
-1.883 |
1.883 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.997 |
0.000 |
0.000 |
| y |
0.000 |
-22.994 |
0.000 |
| z |
0.000 |
0.000 |
-27.282 |
|
| Traceless |
| | x | y | z |
| x |
1.141 |
0.000 |
0.000 |
| y |
0.000 |
2.645 |
0.000 |
| z |
0.000 |
0.000 |
-3.786 |
|
| Polar |
| 3z2-r2 | -7.572 |
| x2-y2 | -1.003 |
| 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 |
4.821 |
0.000 |
0.000 |
| y |
0.000 |
5.741 |
0.000 |
| z |
0.000 |
0.000 |
4.494 |
<r2> (average value of r
2) Å
2
| <r2> |
65.843 |
| (<r2>)1/2 |
8.114 |
Jump to
S1C1
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -192.077135 |
| Energy at 298.15K | -192.084366 |
| HF Energy | -192.077135 |
| Nuclear repulsion energy | 128.867669 |
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/6-31G*
| 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' |
3098 |
3040 |
16.50 |
|
|
|
| 2 |
A' |
3037 |
2981 |
20.15 |
|
|
|
| 3 |
A' |
3001 |
2945 |
50.23 |
|
|
|
| 4 |
A' |
2943 |
2888 |
42.06 |
|
|
|
| 5 |
A' |
1510 |
1482 |
0.30 |
|
|
|
| 6 |
A' |
1448 |
1421 |
4.21 |
|
|
|
| 7 |
A' |
1346 |
1321 |
1.55 |
|
|
|
| 8 |
A' |
1165 |
1143 |
0.98 |
|
|
|
| 9 |
A' |
1127 |
1106 |
1.66 |
|
|
|
| 10 |
A' |
1083 |
1063 |
8.32 |
|
|
|
| 11 |
A' |
948 |
930 |
22.93 |
|
|
|
| 12 |
A' |
835 |
820 |
5.81 |
|
|
|
| 13 |
A' |
705 |
692 |
1.01 |
|
|
|
| 14 |
A' |
98 |
97 |
2.19 |
|
|
|
| 15 |
A" |
3002 |
2945 |
29.65 |
|
|
|
| 16 |
A" |
2932 |
2877 |
119.70 |
|
|
|
| 17 |
A" |
1475 |
1447 |
1.84 |
|
|
|
| 18 |
A" |
1272 |
1248 |
0.01 |
|
|
|
| 19 |
A" |
1227 |
1204 |
12.88 |
|
|
|
| 20 |
A" |
1192 |
1170 |
4.08 |
|
|
|
| 21 |
A" |
1136 |
1114 |
0.44 |
|
|
|
| 22 |
A" |
1079 |
1059 |
101.08 |
|
|
|
| 23 |
A" |
961 |
943 |
2.10 |
|
|
|
| 24 |
A" |
820 |
804 |
1.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18720.2 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 18370.1 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/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.195 |
-1.045 |
0.000 |
| C2 |
-0.052 |
1.066 |
0.000 |
| C3 |
-0.052 |
-0.071 |
1.018 |
| C4 |
-0.052 |
-0.071 |
-1.018 |
| H5 |
0.876 |
1.659 |
0.000 |
| H6 |
-0.919 |
1.744 |
0.000 |
| H7 |
0.740 |
-0.063 |
1.791 |
| H8 |
-1.031 |
-0.230 |
1.517 |
| H9 |
0.740 |
-0.063 |
-1.791 |
| H10 |
-1.031 |
-0.230 |
-1.517 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1251 | 1.4294 | 1.4294 | 2.7881 | 3.0028 | 2.1137 | 2.1137 | 2.1137 | 2.1137 |
C2 | 2.1251 | | 1.5263 | 1.5263 | 1.1011 | 1.1008 | 2.2608 | 2.2228 | 2.2608 | 2.2228 | C3 | 1.4294 | 1.5263 | | 2.0351 | 2.2115 | 2.2545 | 1.1068 | 1.1109 | 2.9182 | 2.7217 | C4 | 1.4294 | 1.5263 | 2.0351 | | 2.2115 | 2.2545 | 2.9182 | 2.7217 | 1.1068 | 1.1109 | H5 | 2.7881 | 1.1011 | 2.2115 | 2.2115 | | 1.7974 | 2.4889 | 3.0835 | 2.4889 | 3.0835 | H6 | 3.0028 | 1.1008 | 2.2545 | 2.2545 | 1.7974 | | 3.0376 | 2.4919 | 3.0376 | 2.4919 | H7 | 2.1137 | 2.2608 | 1.1068 | 2.9182 | 2.4889 | 3.0376 | | 1.7999 | 3.5826 | 3.7560 | H8 | 2.1137 | 2.2228 | 1.1109 | 2.7217 | 3.0835 | 2.4919 | 1.7999 | | 3.7560 | 3.0335 | H9 | 2.1137 | 2.2608 | 2.9182 | 1.1068 | 2.4889 | 3.0376 | 3.5826 | 3.7560 | | 1.7999 | H10 | 2.1137 | 2.2228 | 2.7217 | 1.1109 | 3.0835 | 2.4919 | 3.7560 | 3.0335 | 1.7999 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.882 |
|
O1 |
C3 |
H7 |
112.277 |
| O1 |
C3 |
H8 |
112.013 |
|
O1 |
C4 |
C2 |
91.882 |
| O1 |
C4 |
H9 |
112.277 |
|
O1 |
C4 |
H10 |
112.013 |
| C2 |
C3 |
H7 |
117.436 |
|
C2 |
C3 |
H8 |
113.961 |
| C2 |
C4 |
H9 |
117.436 |
|
C2 |
C4 |
H10 |
113.961 |
| C3 |
O1 |
C4 |
90.770 |
|
C3 |
C2 |
C4 |
83.623 |
| C3 |
C2 |
H5 |
113.660 |
|
C3 |
C2 |
H6 |
117.309 |
| C4 |
C2 |
H5 |
113.660 |
|
C4 |
C2 |
H6 |
117.309 |
| H5 |
C2 |
H6 |
109.433 |
|
H7 |
C3 |
H8 |
108.504 |
| H9 |
C4 |
H10 |
108.504 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.417 |
|
|
|
| 2 |
C |
-0.406 |
|
|
|
| 3 |
C |
-0.096 |
|
|
|
| 4 |
C |
-0.096 |
|
|
|
| 5 |
H |
0.184 |
|
|
|
| 6 |
H |
0.179 |
|
|
|
| 7 |
H |
0.168 |
|
|
|
| 8 |
H |
0.158 |
|
|
|
| 9 |
H |
0.168 |
|
|
|
| 10 |
H |
0.158 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.318 |
1.827 |
0.000 |
1.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.157 |
0.550 |
0.000 |
| y |
0.550 |
-27.199 |
0.000 |
| z |
0.000 |
0.000 |
-22.922 |
|
| Traceless |
| | x | y | z |
| x |
0.904 |
0.550 |
0.000 |
| y |
0.550 |
-3.660 |
0.000 |
| z |
0.000 |
0.000 |
2.756 |
|
| Polar |
| 3z2-r2 | 5.512 |
| x2-y2 | 3.042 |
| xy | 0.550 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.853 |
0.016 |
0.000 |
| y |
0.016 |
4.518 |
0.000 |
| z |
0.000 |
0.000 |
5.733 |
<r2> (average value of r
2) Å
2
| <r2> |
65.612 |
| (<r2>)1/2 |
8.100 |