Jump to
S1C2
Energy calculated at BLYP/3-21G
| hartrees |
Energy at 0K | -229.836466 |
Energy at 298.15K | -229.842107 |
Nuclear repulsion energy | 155.746215 |
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 BLYP/3-21G
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 |
3202 |
3184 |
8.68 |
|
|
|
2 |
A1 |
3116 |
3099 |
0.24 |
|
|
|
3 |
A1 |
3070 |
3054 |
32.78 |
|
|
|
4 |
A1 |
1681 |
1672 |
5.55 |
|
|
|
5 |
A1 |
1447 |
1439 |
1.00 |
|
|
|
6 |
A1 |
1339 |
1332 |
2.05 |
|
|
|
7 |
A1 |
1137 |
1131 |
13.30 |
|
|
|
8 |
A1 |
807 |
803 |
2.01 |
|
|
|
9 |
A1 |
496 |
493 |
0.37 |
|
|
|
10 |
A1 |
216 |
215 |
0.03 |
|
|
|
11 |
A2 |
955 |
950 |
0.00 |
|
|
|
12 |
A2 |
842 |
837 |
0.00 |
|
|
|
13 |
A2 |
696 |
693 |
0.00 |
|
|
|
14 |
A2 |
119 |
118 |
0.00 |
|
|
|
15 |
B1 |
962 |
956 |
55.29 |
|
|
|
16 |
B1 |
845 |
841 |
126.57 |
|
|
|
17 |
B1 |
656 |
652 |
4.35 |
|
|
|
18 |
B1 |
88 |
88 |
2.02 |
|
|
|
19 |
B2 |
3202 |
3184 |
2.07 |
|
|
|
20 |
B2 |
3116 |
3099 |
0.64 |
|
|
|
21 |
B2 |
3065 |
3048 |
4.84 |
|
|
|
22 |
B2 |
1624 |
1615 |
323.09 |
|
|
|
23 |
B2 |
1426 |
1419 |
48.68 |
|
|
|
24 |
B2 |
1314 |
1306 |
0.41 |
|
|
|
25 |
B2 |
1132 |
1126 |
345.88 |
|
|
|
26 |
B2 |
1012 |
1006 |
53.19 |
|
|
|
27 |
B2 |
462 |
459 |
8.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19013.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 18908.5 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 BLYP/3-21G
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
0.347 |
C2 |
0.000 |
1.210 |
-0.385 |
C3 |
0.000 |
-1.210 |
-0.385 |
C4 |
0.000 |
2.397 |
0.236 |
C5 |
0.000 |
-2.397 |
0.236 |
H6 |
0.000 |
1.102 |
-1.475 |
H7 |
0.000 |
-1.102 |
-1.475 |
H8 |
0.000 |
3.320 |
-0.342 |
H9 |
0.000 |
2.461 |
1.323 |
H10 |
0.000 |
-3.320 |
-0.342 |
H11 |
0.000 |
-2.461 |
1.323 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
O1 | | 1.4147 | 1.4147 | 2.3997 | 2.3997 | 2.1292 | 2.1292 | 3.3907 | 2.6472 | 3.3907 | 2.6472 |
C2 | 1.4147 | | 2.4210 | 1.3392 | 3.6606 | 1.0952 | 2.5562 | 2.1100 | 2.1169 | 4.5307 | 4.0491 | C3 | 1.4147 | 2.4210 | | 3.6606 | 1.3392 | 2.5562 | 1.0952 | 4.5307 | 4.0491 | 2.1100 | 2.1169 | C4 | 2.3997 | 1.3392 | 3.6606 | | 4.7943 | 2.1456 | 3.8946 | 1.0887 | 1.0895 | 5.7462 | 4.9780 | C5 | 2.3997 | 3.6606 | 1.3392 | 4.7943 | | 3.8946 | 2.1456 | 5.7462 | 4.9780 | 1.0887 | 1.0895 | H6 | 2.1292 | 1.0952 | 2.5562 | 2.1456 | 3.8946 | | 2.2036 | 2.4908 | 3.1107 | 4.5646 | 4.5300 | H7 | 2.1292 | 2.5562 | 1.0952 | 3.8946 | 2.1456 | 2.2036 | | 4.5646 | 4.5300 | 2.4908 | 3.1107 | H8 | 3.3907 | 2.1100 | 4.5307 | 1.0887 | 5.7462 | 2.4908 | 4.5646 | | 1.8738 | 6.6400 | 6.0157 | H9 | 2.6472 | 2.1169 | 4.0491 | 1.0895 | 4.9780 | 3.1107 | 4.5300 | 1.8738 | | 6.0157 | 4.9213 | H10 | 3.3907 | 4.5307 | 2.1100 | 5.7462 | 1.0887 | 4.5646 | 2.4908 | 6.6400 | 6.0157 | | 1.8738 | H11 | 2.6472 | 4.0491 | 2.1169 | 4.9780 | 1.0895 | 4.5300 | 3.1107 | 6.0157 | 4.9213 | 1.8738 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C4 |
121.222 |
|
O1 |
C2 |
H6 |
115.470 |
O1 |
C3 |
C5 |
121.222 |
|
O1 |
C3 |
H7 |
115.470 |
C2 |
O1 |
C3 |
117.668 |
|
C2 |
C4 |
H8 |
120.351 |
C2 |
C4 |
H9 |
120.954 |
|
C3 |
C5 |
H10 |
120.351 |
C3 |
C5 |
H11 |
120.954 |
|
C4 |
C2 |
H6 |
123.307 |
C5 |
C3 |
H7 |
123.307 |
|
H8 |
C4 |
H9 |
118.695 |
H10 |
C5 |
H11 |
118.695 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.465 |
|
|
|
2 |
C |
0.100 |
|
|
|
3 |
C |
0.100 |
|
|
|
4 |
C |
-0.409 |
|
|
|
5 |
C |
-0.409 |
|
|
|
6 |
H |
0.177 |
|
|
|
7 |
H |
0.177 |
|
|
|
8 |
H |
0.177 |
|
|
|
9 |
H |
0.188 |
|
|
|
10 |
H |
0.177 |
|
|
|
11 |
H |
0.188 |
|
|
|
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 |
-1.358 |
1.358 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.702 |
0.000 |
0.000 |
y |
0.000 |
-26.788 |
0.000 |
z |
0.000 |
0.000 |
-27.629 |
|
Traceless |
| x | y | z |
x |
-6.493 |
0.000 |
0.000 |
y |
0.000 |
3.877 |
0.000 |
z |
0.000 |
0.000 |
2.616 |
|
Polar |
3z2-r2 | 5.232 |
x2-y2 | -6.914 |
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 |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
152.961 |
(<r2>)1/2 |
12.368 |
Jump to
S1C1
Energy calculated at BLYP/3-21G
| hartrees |
Energy at 0K | -229.838092 |
Energy at 298.15K | -229.843975 |
HF Energy | -229.838092 |
Nuclear repulsion energy | 158.073610 |
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 BLYP/3-21G
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 |
3197 |
3179 |
6.72 |
|
|
|
2 |
A |
3191 |
3174 |
11.07 |
|
|
|
3 |
A |
3135 |
3118 |
8.60 |
|
|
|
4 |
A |
3113 |
3096 |
1.12 |
|
|
|
5 |
A |
3110 |
3093 |
2.62 |
|
|
|
6 |
A |
3085 |
3068 |
11.08 |
|
|
|
7 |
A |
1651 |
1642 |
74.67 |
|
|
|
8 |
A |
1627 |
1618 |
126.33 |
|
|
|
9 |
A |
1451 |
1443 |
5.81 |
|
|
|
10 |
A |
1432 |
1424 |
16.62 |
|
|
|
11 |
A |
1348 |
1341 |
13.71 |
|
|
|
12 |
A |
1317 |
1309 |
2.90 |
|
|
|
13 |
A |
1172 |
1166 |
225.89 |
|
|
|
14 |
A |
1100 |
1094 |
11.64 |
|
|
|
15 |
A |
979 |
974 |
84.59 |
|
|
|
16 |
A |
975 |
969 |
14.34 |
|
|
|
17 |
A |
962 |
957 |
37.25 |
|
|
|
18 |
A |
863 |
858 |
60.79 |
|
|
|
19 |
A |
851 |
846 |
67.58 |
|
|
|
20 |
A |
806 |
801 |
7.50 |
|
|
|
21 |
A |
711 |
707 |
3.02 |
|
|
|
22 |
A |
687 |
683 |
2.59 |
|
|
|
23 |
A |
578 |
575 |
3.11 |
|
|
|
24 |
A |
428 |
426 |
2.05 |
|
|
|
25 |
A |
259 |
258 |
1.77 |
|
|
|
26 |
A |
197 |
196 |
8.59 |
|
|
|
27 |
A |
89 |
88 |
0.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19156.4 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 19051.1 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 BLYP/3-21G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-0.053 |
-0.800 |
0.045 |
C2 |
1.328 |
-0.499 |
0.014 |
C3 |
-0.968 |
0.259 |
0.282 |
C4 |
1.906 |
0.701 |
-0.147 |
C5 |
-2.221 |
0.205 |
-0.184 |
H6 |
1.894 |
-1.423 |
0.137 |
H7 |
-0.585 |
1.071 |
0.907 |
H8 |
2.993 |
0.778 |
-0.136 |
H9 |
1.340 |
1.616 |
-0.317 |
H10 |
-2.939 |
0.983 |
0.072 |
H11 |
-2.551 |
-0.621 |
-0.814 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
O1 | | 1.4143 | 1.4201 | 2.4756 | 2.4009 | 2.0463 | 2.1283 | 3.4354 | 2.8129 | 3.3929 | 2.6476 |
C2 | 1.4143 | | 2.4332 | 1.3416 | 3.6242 | 1.0903 | 2.6315 | 2.1035 | 2.1413 | 4.5181 | 3.9689 | C3 | 1.4201 | 2.4332 | | 2.9391 | 1.3383 | 3.3231 | 1.0937 | 4.0163 | 2.7435 | 2.1105 | 2.1173 | C4 | 2.4756 | 1.3416 | 2.9391 | | 4.1570 | 2.1430 | 2.7302 | 1.0895 | 1.0896 | 4.8585 | 4.6967 | C5 | 2.4009 | 3.6242 | 1.3383 | 4.1570 | | 4.4373 | 2.1490 | 5.2455 | 3.8328 | 1.0892 | 1.0898 | H6 | 2.0463 | 1.0903 | 3.3231 | 2.1430 | 4.4373 | | 3.6001 | 2.4756 | 3.1228 | 5.3995 | 4.6160 | H7 | 2.1283 | 2.6315 | 1.0937 | 2.7302 | 2.1490 | 3.6001 | | 3.7384 | 2.3458 | 2.4996 | 3.1130 | H8 | 3.4354 | 2.1035 | 4.0163 | 1.0895 | 5.2455 | 2.4756 | 3.7384 | | 1.8618 | 5.9392 | 5.7578 | H9 | 2.8129 | 2.1413 | 2.7435 | 1.0896 | 3.8328 | 3.1228 | 2.3458 | 1.8618 | | 4.3435 | 4.5160 | H10 | 3.3929 | 4.5181 | 2.1105 | 4.8585 | 1.0892 | 5.3995 | 2.4996 | 5.9392 | 4.3435 | | 1.8729 | H11 | 2.6476 | 3.9689 | 2.1173 | 4.6967 | 1.0898 | 4.6160 | 3.1130 | 5.7578 | 4.5160 | 1.8729 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C4 |
127.856 |
|
O1 |
C2 |
H6 |
108.892 |
O1 |
C3 |
C5 |
120.981 |
|
O1 |
C3 |
H7 |
115.084 |
C2 |
O1 |
C3 |
118.287 |
|
C2 |
C4 |
H8 |
119.464 |
C2 |
C4 |
H9 |
123.137 |
|
C3 |
C5 |
H10 |
120.429 |
C3 |
C5 |
H11 |
121.038 |
|
C4 |
C2 |
H6 |
123.250 |
C5 |
C3 |
H7 |
123.853 |
|
H8 |
C4 |
H9 |
117.379 |
H10 |
C5 |
H11 |
118.526 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.459 |
|
|
|
2 |
C |
0.067 |
|
|
|
3 |
C |
0.083 |
|
|
|
4 |
C |
-0.405 |
|
|
|
5 |
C |
-0.394 |
|
|
|
6 |
H |
0.197 |
|
|
|
7 |
H |
0.186 |
|
|
|
8 |
H |
0.179 |
|
|
|
9 |
H |
0.180 |
|
|
|
10 |
H |
0.178 |
|
|
|
11 |
H |
0.189 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.334 |
0.803 |
0.273 |
0.912 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.608 |
-1.659 |
0.611 |
y |
-1.659 |
-29.304 |
0.873 |
z |
0.611 |
0.873 |
-32.478 |
|
Traceless |
| x | y | z |
x |
4.283 |
-1.659 |
0.611 |
y |
-1.659 |
0.239 |
0.873 |
z |
0.611 |
0.873 |
-4.522 |
|
Polar |
3z2-r2 | -9.044 |
x2-y2 | 2.696 |
xy | -1.659 |
xz | 0.611 |
yz | 0.873 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.863 |
0.300 |
0.621 |
y |
0.300 |
5.897 |
0.339 |
z |
0.621 |
0.339 |
2.781 |
<r2> (average value of r
2) Å
2
<r2> |
136.285 |
(<r2>)1/2 |
11.674 |