Jump to
S1C2
Energy calculated at B2PLYP=FULL/aug-cc-pVTZ
| hartrees |
Energy at 0K | -193.040422 |
Energy at 298.15K | |
HF Energy | -192.773114 |
Nuclear repulsion energy | 128.278932 |
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 B2PLYP=FULL/aug-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 |
3105 |
2979 |
26.17 |
|
|
|
2 |
A1 |
3058 |
2934 |
0.14 |
|
|
|
3 |
A1 |
1559 |
1496 |
0.02 |
|
|
|
4 |
A1 |
1511 |
1449 |
3.53 |
|
|
|
5 |
A1 |
1382 |
1326 |
1.42 |
|
|
|
6 |
A1 |
1049 |
1006 |
4.92 |
|
|
|
7 |
A1 |
924 |
886 |
34.68 |
|
|
|
8 |
A1 |
810 |
777 |
6.43 |
|
|
|
9 |
A2 |
3094 |
2969 |
0.00 |
|
|
|
10 |
A2 |
1251 |
1200 |
0.00 |
|
|
|
11 |
A2 |
1172 |
1124 |
0.00 |
|
|
|
12 |
A2 |
843 |
809 |
0.00 |
|
|
|
13 |
B1 |
3158 |
3030 |
31.25 |
|
|
|
14 |
B1 |
3092 |
2967 |
58.47 |
|
|
|
15 |
B1 |
1211 |
1162 |
0.12 |
|
|
|
16 |
B1 |
1154 |
1108 |
2.23 |
|
|
|
17 |
B1 |
772 |
741 |
0.21 |
|
|
|
18 |
B1 |
50i |
47i |
4.24 |
|
|
|
19 |
B2 |
3050 |
2926 |
145.93 |
|
|
|
20 |
B2 |
1531 |
1469 |
0.74 |
|
|
|
21 |
B2 |
1324 |
1270 |
0.10 |
|
|
|
22 |
B2 |
1270 |
1219 |
7.84 |
|
|
|
23 |
B2 |
1030 |
988 |
92.45 |
|
|
|
24 |
B2 |
952 |
913 |
7.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19126.2 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 18349.6 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 B2PLYP=FULL/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.071 |
C2 |
0.000 |
0.000 |
-1.072 |
C3 |
0.000 |
1.037 |
0.061 |
C4 |
0.000 |
-1.037 |
0.061 |
H5 |
0.886 |
0.000 |
-1.698 |
H6 |
-0.886 |
0.000 |
-1.698 |
H7 |
0.889 |
1.662 |
0.132 |
H8 |
-0.889 |
1.662 |
0.132 |
H9 |
-0.889 |
-1.662 |
0.132 |
H10 |
0.889 |
-1.662 |
0.132 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1431 | 1.4479 | 1.4479 | 2.9075 | 2.9075 | 2.1063 | 2.1063 | 2.1063 | 2.1063 |
C2 | 2.1431 | | 1.5361 | 1.5361 | 1.0850 | 1.0850 | 2.2370 | 2.2370 | 2.2370 | 2.2370 | C3 | 1.4479 | 1.5361 | | 2.0746 | 2.2261 | 2.2261 | 1.0894 | 1.0894 | 2.8433 | 2.8433 | C4 | 1.4479 | 1.5361 | 2.0746 | | 2.2261 | 2.2261 | 2.8433 | 2.8433 | 1.0894 | 1.0894 | H5 | 2.9075 | 1.0850 | 2.2261 | 2.2261 | | 1.7723 | 2.4724 | 3.0439 | 3.0439 | 2.4724 | H6 | 2.9075 | 1.0850 | 2.2261 | 2.2261 | 1.7723 | | 3.0439 | 2.4724 | 2.4724 | 3.0439 | H7 | 2.1063 | 2.2370 | 1.0894 | 2.8433 | 2.4724 | 3.0439 | | 1.7789 | 3.7707 | 3.3247 | H8 | 2.1063 | 2.2370 | 1.0894 | 2.8433 | 3.0439 | 2.4724 | 1.7789 | | 3.3247 | 3.7707 | H9 | 2.1063 | 2.2370 | 2.8433 | 1.0894 | 3.0439 | 2.4724 | 3.7707 | 3.3247 | | 1.7789 | H10 | 2.1063 | 2.2370 | 2.8433 | 1.0894 | 2.4724 | 3.0439 | 3.3247 | 3.7707 | 1.7789 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.763 |
|
O1 |
C3 |
H7 |
111.438 |
O1 |
C3 |
H8 |
111.438 |
|
O1 |
C4 |
C2 |
91.763 |
O1 |
C4 |
H9 |
111.438 |
|
O1 |
C4 |
H10 |
111.438 |
C2 |
C3 |
H7 |
115.822 |
|
C2 |
C3 |
H8 |
115.822 |
C2 |
C4 |
H9 |
115.822 |
|
C2 |
C4 |
H10 |
115.822 |
C3 |
O1 |
C4 |
91.519 |
|
C3 |
C2 |
C4 |
84.955 |
C3 |
C2 |
H5 |
115.187 |
|
C3 |
C2 |
H6 |
115.187 |
C4 |
C2 |
H5 |
115.187 |
|
C4 |
C2 |
H6 |
115.187 |
H5 |
C2 |
H6 |
109.517 |
|
H7 |
C3 |
H8 |
109.460 |
H9 |
C4 |
H10 |
109.460 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/aug-cc-pVTZ
| hartrees |
Energy at 0K | -193.040438 |
Energy at 298.15K | -193.047688 |
HF Energy | -192.773042 |
Nuclear repulsion energy | 128.345938 |
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 B2PLYP=FULL/aug-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' |
3158 |
3029 |
32.01 |
|
|
|
2 |
A' |
3105 |
2979 |
29.70 |
|
|
|
3 |
A' |
3095 |
2970 |
42.62 |
|
|
|
4 |
A' |
3054 |
2930 |
14.75 |
|
|
|
5 |
A' |
1558 |
1495 |
0.05 |
|
|
|
6 |
A' |
1510 |
1449 |
3.51 |
|
|
|
7 |
A' |
1381 |
1325 |
1.37 |
|
|
|
8 |
A' |
1214 |
1165 |
0.10 |
|
|
|
9 |
A' |
1158 |
1111 |
2.58 |
|
|
|
10 |
A' |
1050 |
1007 |
5.34 |
|
|
|
11 |
A' |
923 |
886 |
32.94 |
|
|
|
12 |
A' |
834 |
801 |
7.83 |
|
|
|
13 |
A' |
747 |
716 |
0.96 |
|
|
|
14 |
A' |
71 |
68 |
4.31 |
|
|
|
15 |
A" |
3098 |
2972 |
12.03 |
|
|
|
16 |
A" |
3047 |
2923 |
130.69 |
|
|
|
17 |
A" |
1530 |
1468 |
0.70 |
|
|
|
18 |
A" |
1323 |
1269 |
0.12 |
|
|
|
19 |
A" |
1275 |
1224 |
5.94 |
|
|
|
20 |
A" |
1244 |
1194 |
2.13 |
|
|
|
21 |
A" |
1170 |
1122 |
0.21 |
|
|
|
22 |
A" |
1026 |
984 |
90.71 |
|
|
|
23 |
A" |
953 |
915 |
6.07 |
|
|
|
24 |
A" |
842 |
808 |
0.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19183.1 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 18404.3 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 B2PLYP=FULL/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.127 |
-1.063 |
0.000 |
C2 |
-0.034 |
1.071 |
0.000 |
C3 |
-0.034 |
-0.063 |
1.035 |
C4 |
-0.034 |
-0.063 |
-1.035 |
H5 |
0.870 |
1.670 |
0.000 |
H6 |
-0.902 |
1.722 |
0.000 |
H7 |
0.792 |
-0.081 |
1.743 |
H8 |
-0.975 |
-0.196 |
1.570 |
H9 |
0.792 |
-0.081 |
-1.743 |
H10 |
-0.975 |
-0.196 |
-1.570 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1399 | 1.4482 | 1.4482 | 2.8324 | 2.9692 | 2.1081 | 2.1053 | 2.1081 | 2.1053 |
C2 | 2.1399 | | 1.5353 | 1.5353 | 1.0853 | 1.0850 | 2.2470 | 2.2262 | 2.2470 | 2.2262 | C3 | 1.4482 | 1.5353 | | 2.0703 | 2.2123 | 2.2387 | 1.0885 | 1.0905 | 2.8985 | 2.7732 | C4 | 1.4482 | 1.5353 | 2.0703 | | 2.2123 | 2.2387 | 2.8985 | 2.7732 | 1.0885 | 1.0905 | H5 | 2.8324 | 1.0853 | 2.2123 | 2.2123 | | 1.7733 | 2.4723 | 3.0586 | 2.4723 | 3.0586 | H6 | 2.9692 | 1.0850 | 2.2387 | 2.2387 | 1.7733 | | 3.0268 | 2.4800 | 3.0268 | 2.4800 | H7 | 2.1081 | 2.2470 | 1.0885 | 2.8985 | 2.4723 | 3.0268 | | 1.7796 | 3.4859 | 3.7570 | H8 | 2.1053 | 2.2262 | 1.0905 | 2.7732 | 3.0586 | 2.4800 | 1.7796 | | 3.7570 | 3.1405 | H9 | 2.1081 | 2.2470 | 2.8985 | 1.0885 | 2.4723 | 3.0268 | 3.4859 | 3.7570 | | 1.7796 | H10 | 2.1053 | 2.2262 | 2.7732 | 1.0905 | 3.0586 | 2.4800 | 3.7570 | 3.1405 | 1.7796 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.605 |
|
O1 |
C3 |
H7 |
111.627 |
O1 |
C3 |
H8 |
111.269 |
|
O1 |
C4 |
C2 |
91.605 |
O1 |
C4 |
H9 |
111.627 |
|
O1 |
C4 |
H10 |
111.269 |
C2 |
C3 |
H7 |
116.797 |
|
C2 |
C3 |
H8 |
114.894 |
C2 |
C4 |
H9 |
116.797 |
|
C2 |
C4 |
H10 |
114.894 |
C3 |
O1 |
C4 |
91.249 |
|
C3 |
C2 |
C4 |
84.784 |
C3 |
C2 |
H5 |
114.074 |
|
C3 |
C2 |
H6 |
116.314 |
C4 |
C2 |
H5 |
114.074 |
|
C4 |
C2 |
H6 |
116.314 |
H5 |
C2 |
H6 |
109.589 |
|
H7 |
C3 |
H8 |
109.515 |
H9 |
C4 |
H10 |
109.515 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability