Jump to
S1C2
Energy calculated at B3LYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -193.120770 |
Energy at 298.15K | -193.128001 |
HF Energy | -193.120770 |
Nuclear repulsion energy | 128.030090 |
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 B3LYP/6-31G(2df,p)
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 |
3082 |
2975 |
27.17 |
|
|
|
2 |
A1 |
3017 |
2912 |
1.59 |
|
|
|
3 |
A1 |
1545 |
1491 |
0.01 |
|
|
|
4 |
A1 |
1491 |
1439 |
1.31 |
|
|
|
5 |
A1 |
1384 |
1335 |
4.35 |
|
|
|
6 |
A1 |
1052 |
1015 |
6.48 |
|
|
|
7 |
A1 |
932 |
899 |
24.42 |
|
|
|
8 |
A1 |
819 |
790 |
4.31 |
|
|
|
9 |
A2 |
3050 |
2943 |
0.00 |
|
|
|
10 |
A2 |
1233 |
1190 |
0.00 |
|
|
|
11 |
A2 |
1164 |
1123 |
0.00 |
|
|
|
12 |
A2 |
834 |
805 |
0.00 |
|
|
|
13 |
B1 |
3136 |
3027 |
31.00 |
|
|
|
14 |
B1 |
3049 |
2942 |
84.60 |
|
|
|
15 |
B1 |
1193 |
1152 |
0.50 |
|
|
|
16 |
B1 |
1149 |
1109 |
2.12 |
|
|
|
17 |
B1 |
762 |
735 |
0.17 |
|
|
|
18 |
B1 |
71 |
69 |
2.55 |
|
|
|
19 |
B2 |
3006 |
2901 |
158.22 |
|
|
|
20 |
B2 |
1515 |
1462 |
4.14 |
|
|
|
21 |
B2 |
1313 |
1267 |
0.02 |
|
|
|
22 |
B2 |
1260 |
1216 |
4.81 |
|
|
|
23 |
B2 |
1043 |
1007 |
98.28 |
|
|
|
24 |
B2 |
944 |
911 |
5.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19022.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 18356.8 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 B3LYP/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.069 |
C2 |
0.000 |
0.000 |
-1.077 |
C3 |
0.000 |
1.037 |
0.066 |
C4 |
0.000 |
-1.037 |
0.066 |
H5 |
0.889 |
0.000 |
-1.710 |
H6 |
-0.889 |
0.000 |
-1.710 |
H7 |
0.892 |
1.673 |
0.134 |
H8 |
-0.892 |
1.673 |
0.134 |
H9 |
-0.892 |
-1.673 |
0.134 |
H10 |
0.892 |
-1.673 |
0.134 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1461 | 1.4426 | 1.4426 | 2.9174 | 2.9174 | 2.1135 | 2.1135 | 2.1135 | 2.1135 |
C2 | 2.1461 | | 1.5432 | 1.5432 | 1.0910 | 1.0910 | 2.2495 | 2.2495 | 2.2495 | 2.2495 | C3 | 1.4426 | 1.5432 | | 2.0736 | 2.2400 | 2.2400 | 1.0973 | 1.0973 | 2.8533 | 2.8533 | C4 | 1.4426 | 1.5432 | 2.0736 | | 2.2400 | 2.2400 | 2.8533 | 2.8533 | 1.0973 | 1.0973 | H5 | 2.9174 | 1.0910 | 2.2400 | 2.2400 | | 1.7779 | 2.4895 | 3.0607 | 3.0607 | 2.4895 | H6 | 2.9174 | 1.0910 | 2.2400 | 2.2400 | 1.7779 | | 3.0607 | 2.4895 | 2.4895 | 3.0607 | H7 | 2.1135 | 2.2495 | 1.0973 | 2.8533 | 2.4895 | 3.0607 | | 1.7832 | 3.7911 | 3.3455 | H8 | 2.1135 | 2.2495 | 1.0973 | 2.8533 | 3.0607 | 2.4895 | 1.7832 | | 3.3455 | 3.7911 | H9 | 2.1135 | 2.2495 | 2.8533 | 1.0973 | 3.0607 | 2.4895 | 3.7911 | 3.3455 | | 1.7832 | H10 | 2.1135 | 2.2495 | 2.8533 | 1.0973 | 2.4895 | 3.0607 | 3.3455 | 3.7911 | 1.7832 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.843 |
|
O1 |
C3 |
H7 |
111.919 |
O1 |
C3 |
H8 |
111.919 |
|
O1 |
C4 |
C2 |
91.843 |
O1 |
C4 |
H9 |
111.919 |
|
O1 |
C4 |
H10 |
111.919 |
C2 |
C3 |
H7 |
115.814 |
|
C2 |
C3 |
H8 |
115.814 |
C2 |
C4 |
H9 |
115.814 |
|
C2 |
C4 |
H10 |
115.814 |
C3 |
O1 |
C4 |
91.895 |
|
C3 |
C2 |
C4 |
84.418 |
C3 |
C2 |
H5 |
115.429 |
|
C3 |
C2 |
H6 |
115.429 |
C4 |
C2 |
H5 |
115.429 |
|
C4 |
C2 |
H6 |
115.429 |
H5 |
C2 |
H6 |
109.138 |
|
H7 |
C3 |
H8 |
108.691 |
H9 |
C4 |
H10 |
108.691 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.270 |
|
|
|
2 |
C |
-0.258 |
|
|
|
3 |
C |
-0.051 |
|
|
|
4 |
C |
-0.051 |
|
|
|
5 |
H |
0.113 |
|
|
|
6 |
H |
0.113 |
|
|
|
7 |
H |
0.101 |
|
|
|
8 |
H |
0.101 |
|
|
|
9 |
H |
0.101 |
|
|
|
10 |
H |
0.101 |
|
|
|
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 |
-1.797 |
1.797 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.941 |
0.000 |
0.000 |
y |
0.000 |
-22.938 |
0.000 |
z |
0.000 |
0.000 |
-27.264 |
|
Traceless |
| x | y | z |
x |
1.160 |
0.000 |
0.000 |
y |
0.000 |
2.665 |
0.000 |
z |
0.000 |
0.000 |
-3.825 |
|
Polar |
3z2-r2 | -7.650 |
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 |
5.812 |
0.000 |
z |
0.000 |
0.000 |
4.732 |
<r2> (average value of r
2) Å
2
<r2> |
66.362 |
(<r2>)1/2 |
8.146 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -193.120770 |
Energy at 298.15K | -193.128002 |
HF Energy | -193.120770 |
Nuclear repulsion energy | 128.031414 |
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 B3LYP/6-31G(2df,p)
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' |
3136 |
3026 |
31.18 |
|
|
|
2 |
A' |
3082 |
2974 |
27.22 |
|
|
|
3 |
A' |
3049 |
2942 |
84.47 |
|
|
|
4 |
A' |
3017 |
2912 |
1.60 |
|
|
|
5 |
A' |
1545 |
1491 |
0.01 |
|
|
|
6 |
A' |
1491 |
1439 |
1.31 |
|
|
|
7 |
A' |
1384 |
1335 |
4.35 |
|
|
|
8 |
A' |
1193 |
1151 |
0.51 |
|
|
|
9 |
A' |
1149 |
1109 |
2.12 |
|
|
|
10 |
A' |
1052 |
1015 |
6.49 |
|
|
|
11 |
A' |
932 |
899 |
24.40 |
|
|
|
12 |
A' |
819 |
791 |
4.30 |
|
|
|
13 |
A' |
762 |
735 |
0.17 |
|
|
|
14 |
A' |
72 |
69 |
2.55 |
|
|
|
15 |
A" |
3050 |
2943 |
0.00 |
|
|
|
16 |
A" |
3007 |
2901 |
158.21 |
|
|
|
17 |
A" |
1515 |
1462 |
4.14 |
|
|
|
18 |
A" |
1313 |
1267 |
0.03 |
|
|
|
19 |
A" |
1261 |
1216 |
4.78 |
|
|
|
20 |
A" |
1233 |
1190 |
0.00 |
|
|
|
21 |
A" |
1164 |
1123 |
0.00 |
|
|
|
22 |
A" |
1044 |
1007 |
98.33 |
|
|
|
23 |
A" |
944 |
911 |
5.35 |
|
|
|
24 |
A" |
834 |
805 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19022.7 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 18356.9 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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.002 |
-1.069 |
0.000 |
C2 |
-0.000 |
1.077 |
0.000 |
C3 |
-0.000 |
-0.066 |
1.037 |
C4 |
-0.000 |
-0.066 |
-1.037 |
H5 |
0.888 |
1.710 |
0.000 |
H6 |
-0.889 |
1.709 |
0.000 |
H7 |
0.890 |
-0.134 |
1.674 |
H8 |
-0.893 |
-0.135 |
1.672 |
H9 |
0.890 |
-0.134 |
-1.674 |
H10 |
-0.893 |
-0.135 |
-1.672 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1458 | 1.4425 | 1.4425 | 2.9171 | 2.9175 | 2.1136 | 2.1137 | 2.1136 | 2.1137 |
C2 | 2.1458 | | 1.5432 | 1.5432 | 1.0910 | 1.0911 | 2.2498 | 2.2491 | 2.2498 | 2.2491 | C3 | 1.4425 | 1.5432 | | 2.0738 | 2.2404 | 2.2400 | 1.0973 | 1.0973 | 2.8544 | 2.8527 | C4 | 1.4425 | 1.5432 | 2.0738 | | 2.2404 | 2.2400 | 2.8544 | 2.8527 | 1.0973 | 1.0973 | H5 | 2.9171 | 1.0910 | 2.2404 | 2.2404 | | 1.7775 | 2.4906 | 3.0609 | 2.4906 | 3.0609 | H6 | 2.9175 | 1.0911 | 2.2400 | 2.2400 | 1.7775 | | 3.0606 | 2.4888 | 3.0606 | 2.4888 | H7 | 2.1136 | 2.2498 | 1.0973 | 2.8544 | 2.4906 | 3.0606 | | 1.7831 | 3.3481 | 3.7913 | H8 | 2.1137 | 2.2491 | 1.0973 | 2.8527 | 3.0609 | 2.4888 | 1.7831 | | 3.7913 | 3.3436 | H9 | 2.1136 | 2.2498 | 2.8544 | 1.0973 | 2.4906 | 3.0606 | 3.3481 | 3.7913 | | 1.7831 | H10 | 2.1137 | 2.2491 | 2.8527 | 1.0973 | 3.0609 | 2.4888 | 3.7913 | 3.3436 | 1.7831 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.829 |
|
O1 |
C3 |
H7 |
111.928 |
O1 |
C3 |
H8 |
111.936 |
|
O1 |
C4 |
C2 |
91.829 |
O1 |
C4 |
H9 |
111.928 |
|
O1 |
C4 |
H10 |
111.936 |
C2 |
C3 |
H7 |
115.841 |
|
C2 |
C3 |
H8 |
115.782 |
C2 |
C4 |
H9 |
115.841 |
|
C2 |
C4 |
H10 |
115.782 |
C3 |
O1 |
C4 |
91.913 |
|
C3 |
C2 |
C4 |
84.430 |
C3 |
C2 |
H5 |
115.464 |
|
C3 |
C2 |
H6 |
115.419 |
C4 |
C2 |
H5 |
115.464 |
|
C4 |
C2 |
H6 |
115.419 |
H5 |
C2 |
H6 |
109.095 |
|
H7 |
C3 |
H8 |
108.686 |
H9 |
C4 |
H10 |
108.686 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.269 |
|
|
|
2 |
C |
-0.258 |
|
|
|
3 |
C |
-0.051 |
|
|
|
4 |
C |
-0.051 |
|
|
|
5 |
H |
0.113 |
|
|
|
6 |
H |
0.112 |
|
|
|
7 |
H |
0.101 |
|
|
|
8 |
H |
0.101 |
|
|
|
9 |
H |
0.101 |
|
|
|
10 |
H |
0.101 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.003 |
1.797 |
0.000 |
1.797 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.943 |
0.004 |
0.000 |
y |
0.004 |
-27.263 |
0.000 |
z |
0.000 |
0.000 |
-22.936 |
|
Traceless |
| x | y | z |
x |
1.157 |
0.004 |
0.000 |
y |
0.004 |
-3.824 |
0.000 |
z |
0.000 |
0.000 |
2.667 |
|
Polar |
3z2-r2 | 5.334 |
x2-y2 | 3.321 |
xy | 0.004 |
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 |
4.732 |
0.000 |
z |
0.000 |
0.000 |
5.812 |
<r2> (average value of r
2) Å
2
<r2> |
66.362 |
(<r2>)1/2 |
8.146 |