Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -154.333770 |
Energy at 298.15K | |
HF Energy | -154.333770 |
Nuclear repulsion energy | 74.334701 |
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 B97D3/6-311+G(3df,2p)
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' |
3733 |
3684 |
6.96 |
|
|
|
2 |
A' |
3091 |
3051 |
11.05 |
|
|
|
3 |
A' |
2917 |
2880 |
65.53 |
|
|
|
4 |
A' |
1487 |
1468 |
0.11 |
|
|
|
5 |
A' |
1441 |
1423 |
3.15 |
|
|
|
6 |
A' |
1385 |
1367 |
7.13 |
|
|
|
7 |
A' |
1199 |
1183 |
35.09 |
|
|
|
8 |
A' |
1019 |
1006 |
38.30 |
|
|
|
9 |
A' |
908 |
896 |
91.28 |
|
|
|
10 |
A' |
614 |
606 |
14.47 |
|
|
|
11 |
A' |
378 |
373 |
24.71 |
|
|
|
12 |
A" |
3196 |
3154 |
13.53 |
|
|
|
13 |
A" |
2950 |
2912 |
47.31 |
|
|
|
14 |
A" |
1248 |
1232 |
0.17 |
|
|
|
15 |
A" |
1139 |
1125 |
0.22 |
|
|
|
16 |
A" |
797 |
787 |
0.10 |
|
|
|
17 |
A" |
198 |
195 |
102.27 |
|
|
|
18 |
A" |
172i |
170i |
3.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13763.1 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 13584.2 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 B97D3/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-1.118 |
-0.393 |
0.000 |
C2 |
0.000 |
0.538 |
0.000 |
C3 |
1.265 |
-0.233 |
0.000 |
H4 |
-1.930 |
0.130 |
0.000 |
H5 |
-0.057 |
1.180 |
0.892 |
H6 |
-0.057 |
1.180 |
-0.892 |
H7 |
1.698 |
-0.584 |
-0.931 |
H8 |
1.698 |
-0.584 |
0.931 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
O1 | | 1.4548 | 2.3885 | 0.9663 | 2.0970 | 2.0970 | 2.9722 | 2.9722 |
C2 | 1.4548 | | 1.4816 | 1.9728 | 1.1010 | 1.1010 | 2.2381 | 2.2381 | C3 | 2.3885 | 1.4816 | | 3.2160 | 2.1316 | 2.1316 | 1.0850 | 1.0850 | H4 | 0.9663 | 1.9728 | 3.2160 | | 2.3252 | 2.3252 | 3.8134 | 3.8134 | H5 | 2.0970 | 1.1010 | 2.1316 | 2.3252 | | 1.7840 | 3.0853 | 2.4895 | H6 | 2.0970 | 1.1010 | 2.1316 | 2.3252 | 1.7840 | | 2.4895 | 3.0853 | H7 | 2.9722 | 2.2381 | 1.0850 | 3.8134 | 3.0853 | 2.4895 | | 1.8617 | H8 | 2.9722 | 2.2381 | 1.0850 | 3.8134 | 2.4895 | 3.0853 | 1.8617 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C3 |
108.833 |
|
O1 |
C2 |
H5 |
110.559 |
O1 |
C2 |
H6 |
110.559 |
|
C2 |
O1 |
H4 |
108.858 |
C2 |
C3 |
H7 |
120.358 |
|
C2 |
C3 |
H8 |
120.358 |
C3 |
C2 |
H5 |
109.583 |
|
C3 |
C2 |
H6 |
109.583 |
H5 |
C2 |
H6 |
107.710 |
|
H7 |
C3 |
H8 |
118.238 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.549 |
|
|
|
2 |
C |
0.243 |
|
|
|
3 |
C |
-0.418 |
|
|
|
4 |
H |
0.205 |
|
|
|
5 |
H |
0.114 |
|
|
|
6 |
H |
0.114 |
|
|
|
7 |
H |
0.146 |
|
|
|
8 |
H |
0.146 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.030 |
1.521 |
0.000 |
1.522 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.215 |
-2.864 |
0.000 |
y |
-2.864 |
-20.603 |
0.000 |
z |
0.000 |
0.000 |
-19.200 |
|
Traceless |
| x | y | z |
x |
2.687 |
-2.864 |
0.000 |
y |
-2.864 |
-2.395 |
0.000 |
z |
0.000 |
0.000 |
-0.292 |
|
Polar |
3z2-r2 | -0.583 |
x2-y2 | 3.388 |
xy | -2.864 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.938 |
-0.183 |
0.000 |
y |
-0.183 |
4.716 |
0.000 |
z |
0.000 |
0.000 |
4.473 |
<r2> (average value of r
2) Å
2
<r2> |
51.083 |
(<r2>)1/2 |
7.147 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -154.335427 |
Energy at 298.15K | -154.339945 |
HF Energy | -154.335427 |
Nuclear repulsion energy | 74.752335 |
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 B97D3/6-311+G(3df,2p)
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 |
3774 |
3725 |
19.66 |
|
|
|
2 |
A |
3214 |
3172 |
7.43 |
|
|
|
3 |
A |
3104 |
3063 |
6.59 |
|
|
|
4 |
A |
2876 |
2838 |
61.12 |
|
|
|
5 |
A |
2809 |
2773 |
63.27 |
|
|
|
6 |
A |
1451 |
1432 |
7.30 |
|
|
|
7 |
A |
1425 |
1407 |
4.36 |
|
|
|
8 |
A |
1384 |
1366 |
1.54 |
|
|
|
9 |
A |
1244 |
1228 |
45.30 |
|
|
|
10 |
A |
1186 |
1171 |
4.48 |
|
|
|
11 |
A |
1073 |
1059 |
51.18 |
|
|
|
12 |
A |
1044 |
1030 |
30.79 |
|
|
|
13 |
A |
927 |
915 |
16.36 |
|
|
|
14 |
A |
837 |
826 |
21.61 |
|
|
|
15 |
A |
461 |
455 |
35.53 |
|
|
|
16 |
A |
405 |
399 |
24.03 |
|
|
|
17 |
A |
249 |
246 |
82.48 |
|
|
|
18 |
A |
107 |
106 |
22.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13784.6 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 13605.4 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 B97D3/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-1.119 |
-0.376 |
-0.059 |
C2 |
-0.003 |
0.517 |
0.033 |
C3 |
1.256 |
-0.254 |
-0.013 |
H4 |
-1.922 |
0.127 |
0.119 |
H5 |
-0.065 |
1.099 |
0.978 |
H6 |
-0.026 |
1.262 |
-0.784 |
H7 |
2.193 |
0.246 |
-0.227 |
H8 |
1.259 |
-1.302 |
0.265 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
O1 | | 1.4331 | 2.3786 | 0.9638 | 2.0892 | 2.0987 | 3.3745 | 2.5725 |
C2 | 1.4331 | | 1.4766 | 1.9606 | 1.1111 | 1.1059 | 2.2275 | 2.2257 | C3 | 2.3786 | 1.4766 | | 3.2031 | 2.1343 | 2.1298 | 1.0840 | 1.0838 | H4 | 0.9638 | 1.9606 | 3.2031 | | 2.2657 | 2.3876 | 4.1313 | 3.4899 | H5 | 2.0892 | 1.1111 | 2.1343 | 2.2657 | | 1.7696 | 2.6972 | 2.8329 | H6 | 2.0987 | 1.1059 | 2.1298 | 2.3876 | 1.7696 | | 2.5030 | 3.0534 | H7 | 3.3745 | 2.2275 | 1.0840 | 4.1313 | 2.6972 | 2.5030 | | 1.8739 | H8 | 2.5725 | 2.2257 | 1.0838 | 3.4899 | 2.8329 | 3.0534 | 1.8739 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C3 |
109.660 |
|
O1 |
C2 |
H5 |
109.818 |
O1 |
C2 |
H6 |
110.935 |
|
C2 |
O1 |
H4 |
108.576 |
C2 |
C3 |
H7 |
120.387 |
|
C2 |
C3 |
H8 |
119.551 |
C3 |
C2 |
H5 |
110.199 |
|
C3 |
C2 |
H6 |
110.127 |
H5 |
C2 |
H6 |
106.050 |
|
H7 |
C3 |
H8 |
119.576 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.562 |
|
|
|
2 |
C |
0.307 |
|
|
|
3 |
C |
-0.486 |
|
|
|
4 |
H |
0.208 |
|
|
|
5 |
H |
0.116 |
|
|
|
6 |
H |
0.111 |
|
|
|
7 |
H |
0.153 |
|
|
|
8 |
H |
0.152 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.207 |
1.663 |
0.432 |
1.730 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.699 |
-1.891 |
-0.799 |
y |
-1.891 |
-19.584 |
-0.407 |
z |
-0.799 |
-0.407 |
-20.708 |
|
Traceless |
| x | y | z |
x |
3.447 |
-1.891 |
-0.799 |
y |
-1.891 |
-0.881 |
-0.407 |
z |
-0.799 |
-0.407 |
-2.566 |
|
Polar |
3z2-r2 | -5.132 |
x2-y2 | 2.885 |
xy | -1.891 |
xz | -0.799 |
yz | -0.407 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.778 |
-0.232 |
-0.086 |
y |
-0.232 |
4.896 |
0.043 |
z |
-0.086 |
0.043 |
4.416 |
<r2> (average value of r
2) Å
2
<r2> |
50.881 |
(<r2>)1/2 |
7.133 |