Jump to
S1C2
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -192.149593 |
| Energy at 298.15K | |
| HF Energy | -192.149593 |
| Nuclear repulsion energy | 128.823925 |
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/TZVP
| 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 |
3026 |
2990 |
18.21 |
|
|
|
| 2 |
A1 |
2952 |
2918 |
0.19 |
|
|
|
| 3 |
A1 |
1478 |
1461 |
0.00 |
|
|
|
| 4 |
A1 |
1426 |
1409 |
7.88 |
|
|
|
| 5 |
A1 |
1340 |
1324 |
0.01 |
|
|
|
| 6 |
A1 |
1065 |
1052 |
7.06 |
|
|
|
| 7 |
A1 |
941 |
930 |
31.70 |
|
|
|
| 8 |
A1 |
796 |
787 |
2.98 |
|
|
|
| 9 |
A2 |
2987 |
2953 |
0.00 |
|
|
|
| 10 |
A2 |
1196 |
1182 |
0.00 |
|
|
|
| 11 |
A2 |
1137 |
1124 |
0.00 |
|
|
|
| 12 |
A2 |
819 |
809 |
0.00 |
|
|
|
| 13 |
B1 |
3085 |
3049 |
13.27 |
|
|
|
| 14 |
B1 |
2986 |
2952 |
68.14 |
|
|
|
| 15 |
B1 |
1154 |
1141 |
0.74 |
|
|
|
| 16 |
B1 |
1118 |
1105 |
1.07 |
|
|
|
| 17 |
B1 |
750 |
741 |
0.47 |
|
|
|
| 18 |
B1 |
39i |
39i |
2.25 |
|
|
|
| 19 |
B2 |
2941 |
2907 |
147.29 |
|
|
|
| 20 |
B2 |
1447 |
1430 |
0.07 |
|
|
|
| 21 |
B2 |
1286 |
1271 |
1.91 |
|
|
|
| 22 |
B2 |
1230 |
1216 |
26.57 |
|
|
|
| 23 |
B2 |
1059 |
1047 |
100.77 |
|
|
|
| 24 |
B2 |
961 |
950 |
5.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18569.0 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 18353.6 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/TZVP
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 |
-1.066 |
| C3 |
0.000 |
1.023 |
0.063 |
| C4 |
0.000 |
-1.023 |
0.063 |
| H5 |
0.895 |
0.000 |
-1.700 |
| H6 |
-0.895 |
0.000 |
-1.700 |
| H7 |
0.898 |
1.662 |
0.128 |
| H8 |
-0.898 |
1.662 |
0.128 |
| H9 |
-0.898 |
-1.662 |
0.128 |
| H10 |
0.898 |
-1.662 |
0.128 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1315 | 1.4324 | 1.4324 | 2.9065 | 2.9065 | 2.1090 | 2.1090 | 2.1090 | 2.1090 |
C2 | 2.1315 | | 1.5241 | 1.5241 | 1.0969 | 1.0969 | 2.2354 | 2.2354 | 2.2354 | 2.2354 | C3 | 1.4324 | 1.5241 | | 2.0470 | 2.2265 | 2.2265 | 1.1040 | 1.1040 | 2.8328 | 2.8328 | C4 | 1.4324 | 1.5241 | 2.0470 | | 2.2265 | 2.2265 | 2.8328 | 2.8328 | 1.1040 | 1.1040 | H5 | 2.9065 | 1.0969 | 2.2265 | 2.2265 | | 1.7908 | 2.4710 | 3.0532 | 3.0532 | 2.4710 | H6 | 2.9065 | 1.0969 | 2.2265 | 2.2265 | 1.7908 | | 3.0532 | 2.4710 | 2.4710 | 3.0532 | H7 | 2.1090 | 2.2354 | 1.1040 | 2.8328 | 2.4710 | 3.0532 | | 1.7960 | 3.7789 | 3.3249 | H8 | 2.1090 | 2.2354 | 1.1040 | 2.8328 | 3.0532 | 2.4710 | 1.7960 | | 3.3249 | 3.7789 | H9 | 2.1090 | 2.2354 | 2.8328 | 1.1040 | 3.0532 | 2.4710 | 3.7789 | 3.3249 | | 1.7960 | H10 | 2.1090 | 2.2354 | 2.8328 | 1.1040 | 2.4710 | 3.0532 | 3.3249 | 3.7789 | 1.7960 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.211 |
|
O1 |
C3 |
H7 |
111.853 |
| O1 |
C3 |
H8 |
111.853 |
|
O1 |
C4 |
C2 |
92.211 |
| O1 |
C4 |
H9 |
111.853 |
|
O1 |
C4 |
H10 |
111.853 |
| C2 |
C3 |
H7 |
115.618 |
|
C2 |
C3 |
H8 |
115.618 |
| C2 |
C4 |
H9 |
115.618 |
|
C2 |
C4 |
H10 |
115.618 |
| C3 |
O1 |
C4 |
91.210 |
|
C3 |
C2 |
C4 |
84.369 |
| C3 |
C2 |
H5 |
115.342 |
|
C3 |
C2 |
H6 |
115.342 |
| C4 |
C2 |
H5 |
115.342 |
|
C4 |
C2 |
H6 |
115.342 |
| H5 |
C2 |
H6 |
109.431 |
|
H7 |
C3 |
H8 |
108.854 |
| H9 |
C4 |
H10 |
108.854 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.180 |
|
|
|
| 2 |
C |
-0.365 |
|
|
|
| 3 |
C |
-0.217 |
|
|
|
| 4 |
C |
-0.217 |
|
|
|
| 5 |
H |
0.191 |
|
|
|
| 6 |
H |
0.191 |
|
|
|
| 7 |
H |
0.149 |
|
|
|
| 8 |
H |
0.149 |
|
|
|
| 9 |
H |
0.149 |
|
|
|
| 10 |
H |
0.149 |
|
|
|
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 |
-2.018 |
2.018 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.438 |
0.000 |
0.000 |
| y |
0.000 |
-23.427 |
0.000 |
| z |
0.000 |
0.000 |
-28.229 |
|
| Traceless |
| | x | y | z |
| x |
1.390 |
0.000 |
0.000 |
| y |
0.000 |
2.907 |
0.000 |
| z |
0.000 |
0.000 |
-4.297 |
|
| Polar |
| 3z2-r2 | -8.594 |
| x2-y2 | -1.011 |
| 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 |
5.395 |
0.000 |
0.000 |
| y |
0.000 |
6.426 |
0.000 |
| z |
0.000 |
0.000 |
5.348 |
<r2> (average value of r
2) Å
2
| <r2> |
66.089 |
| (<r2>)1/2 |
8.129 |
Jump to
S1C1
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -192.149600 |
| Energy at 298.15K | -192.156798 |
| HF Energy | -192.149600 |
| Nuclear repulsion energy | 128.890961 |
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/TZVP
| 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' |
3084 |
3048 |
13.98 |
|
|
|
| 2 |
A' |
3024 |
2989 |
19.16 |
|
|
|
| 3 |
A' |
2992 |
2958 |
48.74 |
|
|
|
| 4 |
A' |
2945 |
2911 |
21.31 |
|
|
|
| 5 |
A' |
1477 |
1460 |
0.10 |
|
|
|
| 6 |
A' |
1424 |
1407 |
7.73 |
|
|
|
| 7 |
A' |
1337 |
1322 |
0.04 |
|
|
|
| 8 |
A' |
1158 |
1145 |
0.51 |
|
|
|
| 9 |
A' |
1120 |
1107 |
1.54 |
|
|
|
| 10 |
A' |
1065 |
1053 |
7.67 |
|
|
|
| 11 |
A' |
938 |
927 |
30.83 |
|
|
|
| 12 |
A' |
816 |
807 |
4.66 |
|
|
|
| 13 |
A' |
726 |
717 |
0.61 |
|
|
|
| 14 |
A' |
70 |
69 |
2.48 |
|
|
|
| 15 |
A" |
2993 |
2959 |
15.70 |
|
|
|
| 16 |
A" |
2935 |
2901 |
126.81 |
|
|
|
| 17 |
A" |
1446 |
1429 |
0.04 |
|
|
|
| 18 |
A" |
1282 |
1268 |
1.30 |
|
|
|
| 19 |
A" |
1232 |
1217 |
23.22 |
|
|
|
| 20 |
A" |
1190 |
1176 |
3.21 |
|
|
|
| 21 |
A" |
1135 |
1122 |
0.51 |
|
|
|
| 22 |
A" |
1054 |
1042 |
98.30 |
|
|
|
| 23 |
A" |
960 |
949 |
4.45 |
|
|
|
| 24 |
A" |
819 |
810 |
0.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18611.1 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 18395.3 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/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.132 |
-1.056 |
0.000 |
| C2 |
-0.035 |
1.065 |
0.000 |
| C3 |
-0.035 |
-0.066 |
1.021 |
| C4 |
-0.035 |
-0.066 |
-1.021 |
| H5 |
0.879 |
1.672 |
0.000 |
| H6 |
-0.913 |
1.723 |
0.000 |
| H7 |
0.794 |
-0.079 |
1.748 |
| H8 |
-0.990 |
-0.194 |
1.564 |
| H9 |
0.794 |
-0.079 |
-1.748 |
| H10 |
-0.990 |
-0.194 |
-1.564 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1278 | 1.4327 | 1.4327 | 2.8288 | 2.9691 | 2.1096 | 2.1090 | 2.1096 | 2.1090 |
C2 | 2.1278 | | 1.5236 | 1.5236 | 1.0973 | 1.0969 | 2.2475 | 2.2230 | 2.2475 | 2.2230 | C3 | 1.4327 | 1.5236 | | 2.0427 | 2.2132 | 2.2388 | 1.1027 | 1.1055 | 2.8910 | 2.7588 | C4 | 1.4327 | 1.5236 | 2.0427 | | 2.2132 | 2.2388 | 2.8910 | 2.7588 | 1.1027 | 1.1055 | H5 | 2.8288 | 1.0973 | 2.2132 | 2.2132 | | 1.7924 | 2.4755 | 3.0691 | 2.4755 | 3.0691 | H6 | 2.9691 | 1.0969 | 2.2388 | 2.2388 | 1.7924 | | 3.0356 | 2.4750 | 3.0356 | 2.4750 | H7 | 2.1096 | 2.2475 | 1.1027 | 2.8910 | 2.4755 | 3.0356 | | 1.7971 | 3.4963 | 3.7636 | H8 | 2.1090 | 2.2230 | 1.1055 | 2.7588 | 3.0691 | 2.4750 | 1.7971 | | 3.7636 | 3.1277 | H9 | 2.1096 | 2.2475 | 2.8910 | 1.1027 | 2.4755 | 3.0356 | 3.4963 | 3.7636 | | 1.7971 | H10 | 2.1090 | 2.2230 | 2.7588 | 1.1055 | 3.0691 | 2.4750 | 3.7636 | 3.1277 | 1.7971 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.017 |
|
O1 |
C3 |
H7 |
111.967 |
| O1 |
C3 |
H8 |
111.740 |
|
O1 |
C4 |
C2 |
92.017 |
| O1 |
C4 |
H9 |
111.967 |
|
O1 |
C4 |
H10 |
111.740 |
| C2 |
C3 |
H7 |
116.773 |
|
C2 |
C3 |
H8 |
114.521 |
| C2 |
C4 |
H9 |
116.773 |
|
C2 |
C4 |
H10 |
114.521 |
| C3 |
O1 |
C4 |
90.946 |
|
C3 |
C2 |
C4 |
84.188 |
| C3 |
C2 |
H5 |
114.243 |
|
C3 |
C2 |
H6 |
116.428 |
| C4 |
C2 |
H5 |
114.243 |
|
C4 |
C2 |
H6 |
116.428 |
| H5 |
C2 |
H6 |
109.548 |
|
H7 |
C3 |
H8 |
108.943 |
| H9 |
C4 |
H10 |
108.943 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.183 |
|
|
|
| 2 |
C |
-0.362 |
|
|
|
| 3 |
C |
-0.219 |
|
|
|
| 4 |
C |
-0.219 |
|
|
|
| 5 |
H |
0.186 |
|
|
|
| 6 |
H |
0.194 |
|
|
|
| 7 |
H |
0.156 |
|
|
|
| 8 |
H |
0.145 |
|
|
|
| 9 |
H |
0.156 |
|
|
|
| 10 |
H |
0.145 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.243 |
1.994 |
0.000 |
2.008 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.534 |
0.449 |
0.000 |
| y |
0.449 |
-28.182 |
0.000 |
| z |
0.000 |
0.000 |
-23.384 |
|
| Traceless |
| | x | y | z |
| x |
1.249 |
0.449 |
0.000 |
| y |
0.449 |
-4.223 |
0.000 |
| z |
0.000 |
0.000 |
2.974 |
|
| Polar |
| 3z2-r2 | 5.948 |
| x2-y2 | 3.648 |
| xy | 0.449 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.427 |
-0.015 |
0.000 |
| y |
-0.015 |
5.359 |
0.000 |
| z |
0.000 |
0.000 |
6.426 |
<r2> (average value of r
2) Å
2
| <r2> |
65.987 |
| (<r2>)1/2 |
8.123 |