Jump to
S1C2
Energy calculated at B3LYP/6-311G**
| | hartrees |
| Energy at 0K | -194.412430 |
| Energy at 298.15K | -194.421337 |
| Nuclear repulsion energy | 130.213566 |
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/6-311G**
| 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' |
3842 |
3714 |
22.29 |
|
|
|
| 2 |
A' |
3093 |
2990 |
38.50 |
|
|
|
| 3 |
A' |
3032 |
2931 |
35.71 |
|
|
|
| 4 |
A' |
3021 |
2921 |
25.30 |
|
|
|
| 5 |
A' |
2955 |
2857 |
63.39 |
|
|
|
| 6 |
A' |
1529 |
1479 |
3.96 |
|
|
|
| 7 |
A' |
1510 |
1460 |
4.52 |
|
|
|
| 8 |
A' |
1497 |
1447 |
1.05 |
|
|
|
| 9 |
A' |
1462 |
1413 |
2.44 |
|
|
|
| 10 |
A' |
1415 |
1368 |
1.76 |
|
|
|
| 11 |
A' |
1354 |
1309 |
6.85 |
|
|
|
| 12 |
A' |
1265 |
1223 |
55.61 |
|
|
|
| 13 |
A' |
1099 |
1062 |
1.90 |
|
|
|
| 14 |
A' |
1064 |
1029 |
79.77 |
|
|
|
| 15 |
A' |
1035 |
1001 |
22.78 |
|
|
|
| 16 |
A' |
888 |
858 |
6.29 |
|
|
|
| 17 |
A' |
457 |
442 |
10.63 |
|
|
|
| 18 |
A' |
273 |
264 |
4.03 |
|
|
|
| 19 |
A" |
3085 |
2983 |
80.87 |
|
|
|
| 20 |
A" |
3059 |
2958 |
1.95 |
|
|
|
| 21 |
A" |
2980 |
2881 |
57.42 |
|
|
|
| 22 |
A" |
1502 |
1452 |
7.90 |
|
|
|
| 23 |
A" |
1322 |
1278 |
0.09 |
|
|
|
| 24 |
A" |
1268 |
1226 |
0.03 |
|
|
|
| 25 |
A" |
1186 |
1147 |
1.33 |
|
|
|
| 26 |
A" |
906 |
876 |
2.78 |
|
|
|
| 27 |
A" |
775 |
749 |
0.92 |
|
|
|
| 28 |
A" |
273 |
264 |
115.59 |
|
|
|
| 29 |
A" |
230 |
222 |
3.49 |
|
|
|
| 30 |
A" |
125 |
121 |
4.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 23749.7 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 22961.2 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 B3LYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.445 |
1.242 |
0.000 |
| C2 |
0.000 |
0.738 |
0.000 |
| C3 |
0.094 |
-0.780 |
0.000 |
| O4 |
1.474 |
-1.137 |
0.000 |
| H5 |
-1.480 |
2.334 |
0.000 |
| H6 |
-1.990 |
0.895 |
0.883 |
| H7 |
-1.990 |
0.895 |
-0.883 |
| H8 |
0.535 |
1.114 |
0.878 |
| H9 |
0.535 |
1.114 |
-0.878 |
| H10 |
-0.417 |
-1.182 |
0.888 |
| H11 |
-0.417 |
-1.182 |
-0.888 |
| H12 |
1.536 |
-2.096 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5305 | 2.5415 | 3.7659 | 1.0925 | 1.0946 | 1.0946 | 2.1693 | 2.1693 | 2.7794 | 2.7794 | 4.4758 |
C2 | 1.5305 | | 1.5208 | 2.3847 | 2.1769 | 2.1828 | 2.1828 | 1.0947 | 1.0947 | 2.1564 | 2.1564 | 3.2234 | C3 | 2.5415 | 1.5208 | | 1.4255 | 3.4896 | 2.8159 | 2.8159 | 2.1340 | 2.1340 | 1.1008 | 1.1008 | 1.9523 | O4 | 3.7659 | 2.3847 | 1.4255 | | 4.5579 | 4.1120 | 4.1120 | 2.5924 | 2.5924 | 2.0900 | 2.0900 | 0.9612 | H5 | 1.0925 | 2.1769 | 3.4896 | 4.5579 | | 1.7642 | 1.7642 | 2.5134 | 2.5134 | 3.7797 | 3.7797 | 5.3596 | H6 | 1.0946 | 2.1828 | 2.8159 | 4.1120 | 1.7642 | | 1.7668 | 2.5341 | 3.0860 | 2.6057 | 3.1507 | 4.7075 | H7 | 1.0946 | 2.1828 | 2.8159 | 4.1120 | 1.7642 | 1.7668 | | 3.0860 | 2.5341 | 3.1507 | 2.6057 | 4.7075 | H8 | 2.1693 | 1.0947 | 2.1340 | 2.5924 | 2.5134 | 2.5341 | 3.0860 | | 1.7557 | 2.4863 | 3.0495 | 3.4755 | H9 | 2.1693 | 1.0947 | 2.1340 | 2.5924 | 2.5134 | 3.0860 | 2.5341 | 1.7557 | | 3.0495 | 2.4863 | 3.4755 | H10 | 2.7794 | 2.1564 | 1.1008 | 2.0900 | 3.7797 | 2.6057 | 3.1507 | 2.4863 | 3.0495 | | 1.7760 | 2.3323 | H11 | 2.7794 | 2.1564 | 1.1008 | 2.0900 | 3.7797 | 3.1507 | 2.6057 | 3.0495 | 2.4863 | 1.7760 | | 2.3323 | H12 | 4.4758 | 3.2234 | 1.9523 | 0.9612 | 5.3596 | 4.7075 | 4.7075 | 3.4755 | 3.4755 | 2.3323 | 2.3323 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.798 |
|
C1 |
C2 |
H8 |
110.346 |
| C1 |
C2 |
H9 |
110.346 |
|
C2 |
C1 |
H5 |
111.082 |
| C2 |
C1 |
H6 |
111.432 |
|
C2 |
C1 |
H7 |
111.432 |
| C2 |
C3 |
O4 |
108.029 |
|
C2 |
C3 |
H10 |
109.638 |
| C2 |
C3 |
H11 |
109.638 |
|
C3 |
C2 |
H8 |
108.248 |
| C3 |
C2 |
H9 |
108.248 |
|
C3 |
O4 |
H12 |
108.195 |
| O4 |
C3 |
H10 |
110.993 |
|
O4 |
C3 |
H11 |
110.993 |
| H5 |
C1 |
H6 |
107.539 |
|
H5 |
C1 |
H7 |
107.539 |
| H6 |
C1 |
H7 |
107.620 |
|
H8 |
C2 |
H9 |
106.631 |
| H10 |
C3 |
H11 |
107.545 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.309 |
|
|
|
| 2 |
C |
-0.243 |
|
|
|
| 3 |
C |
0.006 |
|
|
|
| 4 |
O |
-0.403 |
|
|
|
| 5 |
H |
0.113 |
|
|
|
| 6 |
H |
0.102 |
|
|
|
| 7 |
H |
0.102 |
|
|
|
| 8 |
H |
0.115 |
|
|
|
| 9 |
H |
0.115 |
|
|
|
| 10 |
H |
0.084 |
|
|
|
| 11 |
H |
0.084 |
|
|
|
| 12 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.105 |
-1.019 |
0.000 |
1.503 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.659 |
-1.016 |
0.000 |
| y |
-1.016 |
-22.062 |
0.000 |
| z |
0.000 |
0.000 |
-26.778 |
|
| Traceless |
| | x | y | z |
| x |
-5.239 |
-1.016 |
0.000 |
| y |
-1.016 |
6.157 |
0.000 |
| z |
0.000 |
0.000 |
-0.917 |
|
| Polar |
| 3z2-r2 | -1.835 |
| x2-y2 | -7.597 |
| xy | -1.016 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.191 |
-0.561 |
0.000 |
| y |
-0.561 |
6.399 |
0.000 |
| z |
0.000 |
0.000 |
5.308 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G**
| | hartrees |
| Energy at 0K | -194.412802 |
| Energy at 298.15K | |
| HF Energy | -194.412802 |
| Nuclear repulsion energy | 132.463446 |
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/6-311G**
| 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 |
3844 |
3717 |
25.06 |
110.73 |
0.31 |
0.47 |
| 2 |
A |
3111 |
3008 |
28.33 |
41.77 |
0.74 |
0.85 |
| 3 |
A |
3084 |
2982 |
56.50 |
63.74 |
0.55 |
0.71 |
| 4 |
A |
3054 |
2953 |
26.08 |
93.22 |
0.71 |
0.83 |
| 5 |
A |
3024 |
2924 |
13.01 |
202.78 |
0.02 |
0.04 |
| 6 |
A |
3023 |
2923 |
65.25 |
56.88 |
0.25 |
0.40 |
| 7 |
A |
2988 |
2889 |
54.48 |
98.57 |
0.75 |
0.86 |
| 8 |
A |
2959 |
2861 |
67.15 |
117.67 |
0.12 |
0.21 |
| 9 |
A |
1523 |
1473 |
2.57 |
5.82 |
0.69 |
0.81 |
| 10 |
A |
1512 |
1462 |
7.57 |
6.01 |
0.75 |
0.86 |
| 11 |
A |
1496 |
1447 |
8.02 |
14.36 |
0.75 |
0.86 |
| 12 |
A |
1479 |
1429 |
3.00 |
12.68 |
0.74 |
0.85 |
| 13 |
A |
1454 |
1406 |
2.90 |
2.02 |
0.21 |
0.34 |
| 14 |
A |
1411 |
1364 |
4.54 |
1.14 |
0.74 |
0.85 |
| 15 |
A |
1383 |
1337 |
0.93 |
1.19 |
0.73 |
0.84 |
| 16 |
A |
1327 |
1283 |
20.78 |
11.18 |
0.74 |
0.85 |
| 17 |
A |
1272 |
1230 |
0.53 |
7.35 |
0.75 |
0.85 |
| 18 |
A |
1252 |
1210 |
39.09 |
3.57 |
0.55 |
0.71 |
| 19 |
A |
1160 |
1121 |
5.66 |
0.77 |
0.23 |
0.38 |
| 20 |
A |
1117 |
1080 |
6.13 |
3.67 |
0.63 |
0.77 |
| 21 |
A |
1064 |
1029 |
46.04 |
2.59 |
0.67 |
0.81 |
| 22 |
A |
985 |
952 |
47.72 |
4.16 |
0.75 |
0.86 |
| 23 |
A |
929 |
898 |
2.68 |
0.50 |
0.74 |
0.85 |
| 24 |
A |
864 |
835 |
2.09 |
9.52 |
0.16 |
0.27 |
| 25 |
A |
777 |
751 |
0.90 |
0.56 |
0.54 |
0.70 |
| 26 |
A |
479 |
463 |
8.46 |
0.24 |
0.45 |
0.62 |
| 27 |
A |
328 |
317 |
6.99 |
0.31 |
0.40 |
0.57 |
| 28 |
A |
253 |
244 |
110.61 |
3.91 |
0.74 |
0.85 |
| 29 |
A |
224 |
217 |
1.97 |
0.07 |
0.58 |
0.73 |
| 30 |
A |
149 |
144 |
7.31 |
0.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 23761.1 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 22972.2 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 B3LYP/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.543 |
-0.516 |
0.129 |
| C2 |
-0.633 |
0.642 |
-0.289 |
| C3 |
0.770 |
0.546 |
0.293 |
| O4 |
1.384 |
-0.637 |
-0.219 |
| H5 |
-2.526 |
-0.436 |
-0.342 |
| H6 |
-1.693 |
-0.527 |
1.214 |
| H7 |
-1.101 |
-1.471 |
-0.159 |
| H8 |
-0.547 |
0.675 |
-1.380 |
| H9 |
-1.069 |
1.599 |
0.023 |
| H10 |
0.714 |
0.514 |
1.392 |
| H11 |
1.349 |
1.438 |
0.012 |
| H12 |
2.244 |
-0.734 |
0.197 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5308 | 2.5503 | 2.9499 | 1.0931 | 1.0950 | 1.0913 | 2.1649 | 2.1694 | 2.7834 | 3.4917 | 3.7942 |
C2 | 1.5308 | | 1.5222 | 2.3896 | 2.1792 | 2.1789 | 2.1684 | 1.0953 | 1.0960 | 2.1579 | 2.1570 | 3.2268 | C3 | 2.5503 | 1.5222 | | 1.4279 | 3.4975 | 2.8396 | 2.7881 | 2.1334 | 2.1360 | 1.1008 | 1.0994 | 1.9550 | O4 | 2.9499 | 2.3896 | 1.4279 | | 3.9171 | 3.3955 | 2.6217 | 2.6073 | 3.3276 | 2.0900 | 2.0876 | 0.9610 | H5 | 1.0931 | 2.1792 | 3.4975 | 3.9171 | | 1.7673 | 1.7709 | 2.4957 | 2.5291 | 3.7955 | 4.3189 | 4.8102 | H6 | 1.0950 | 2.1789 | 2.8396 | 3.3955 | 1.7673 | | 1.7676 | 3.0798 | 2.5152 | 2.6278 | 3.8151 | 4.0711 | H7 | 1.0913 | 2.1684 | 2.7881 | 2.6217 | 1.7709 | 1.7676 | | 2.5304 | 3.0752 | 3.1043 | 3.8067 | 3.4439 | H8 | 2.1649 | 1.0953 | 2.1334 | 2.6073 | 2.4957 | 3.0798 | 2.5304 | | 1.7590 | 3.0499 | 2.4733 | 3.5026 | H9 | 2.1694 | 1.0960 | 2.1360 | 3.3276 | 2.5291 | 2.5152 | 3.0752 | 1.7590 | | 2.4962 | 2.4234 | 4.0559 | H10 | 2.7834 | 2.1579 | 1.1008 | 2.0900 | 3.7955 | 2.6278 | 3.1043 | 3.0499 | 2.4962 | | 1.7778 | 2.3077 | H11 | 3.4917 | 2.1570 | 1.0994 | 2.0876 | 4.3189 | 3.8151 | 3.8067 | 2.4733 | 2.4234 | 1.7778 | | 2.3563 | H12 | 3.7942 | 3.2268 | 1.9550 | 0.9610 | 4.8102 | 4.0711 | 3.4439 | 3.5026 | 4.0559 | 2.3077 | 2.3563 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
113.305 |
|
C1 |
C2 |
H8 |
109.941 |
| C1 |
C2 |
H9 |
110.256 |
|
C2 |
C1 |
H5 |
111.209 |
| C2 |
C1 |
H6 |
111.072 |
|
C2 |
C1 |
H7 |
110.463 |
| C2 |
C3 |
O4 |
108.158 |
|
C2 |
C3 |
H10 |
109.665 |
| C2 |
C3 |
H11 |
109.675 |
|
C3 |
C2 |
H8 |
108.082 |
| C3 |
C2 |
H9 |
108.240 |
|
C3 |
O4 |
H12 |
108.257 |
| O4 |
C3 |
H10 |
110.819 |
|
O4 |
C3 |
H11 |
110.714 |
| H5 |
C1 |
H6 |
107.738 |
|
H5 |
C1 |
H7 |
108.332 |
| H6 |
C1 |
H7 |
107.901 |
|
H8 |
C2 |
H9 |
106.779 |
| H10 |
C3 |
H11 |
107.805 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.298 |
|
|
|
| 2 |
C |
-0.243 |
|
|
|
| 3 |
C |
-0.010 |
|
|
|
| 4 |
O |
-0.403 |
|
|
|
| 5 |
H |
0.105 |
|
|
|
| 6 |
H |
0.095 |
|
|
|
| 7 |
H |
0.122 |
|
|
|
| 8 |
H |
0.115 |
|
|
|
| 9 |
H |
0.102 |
|
|
|
| 10 |
H |
0.085 |
|
|
|
| 11 |
H |
0.093 |
|
|
|
| 12 |
H |
0.237 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.774 |
0.890 |
1.014 |
1.555 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.069 |
-0.252 |
2.022 |
| y |
-0.252 |
-27.310 |
-0.594 |
| z |
2.022 |
-0.594 |
-26.997 |
|
| Traceless |
| | x | y | z |
| x |
4.084 |
-0.252 |
2.022 |
| y |
-0.252 |
-2.277 |
-0.594 |
| z |
2.022 |
-0.594 |
-1.807 |
|
| Polar |
| 3z2-r2 | -3.613 |
| x2-y2 | 4.241 |
| xy | -0.252 |
| xz | 2.022 |
| yz | -0.594 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.550 |
0.058 |
0.154 |
| y |
0.058 |
5.817 |
-0.004 |
| z |
0.154 |
-0.004 |
5.498 |
<r2> (average value of r
2) Å
2
| <r2> |
95.560 |
| (<r2>)1/2 |
9.775 |