Jump to
S1C2
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -194.226915 |
| Energy at 298.15K | -194.235762 |
| HF Energy | -194.226915 |
| Nuclear repulsion energy | |
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 B97D3/6-31G*
| 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' |
3674 |
3602 |
5.79 |
|
|
|
| 2 |
A' |
3066 |
3006 |
41.92 |
|
|
|
| 3 |
A' |
2995 |
2936 |
40.33 |
|
|
|
| 4 |
A' |
2985 |
2927 |
28.74 |
|
|
|
| 5 |
A' |
2901 |
2844 |
75.50 |
|
|
|
| 6 |
A' |
1529 |
1499 |
4.72 |
|
|
|
| 7 |
A' |
1510 |
1480 |
3.79 |
|
|
|
| 8 |
A' |
1495 |
1466 |
0.78 |
|
|
|
| 9 |
A' |
1451 |
1423 |
6.16 |
|
|
|
| 10 |
A' |
1410 |
1382 |
0.68 |
|
|
|
| 11 |
A' |
1339 |
1313 |
7.02 |
|
|
|
| 12 |
A' |
1256 |
1231 |
54.41 |
|
|
|
| 13 |
A' |
1087 |
1066 |
2.34 |
|
|
|
| 14 |
A' |
1044 |
1024 |
73.52 |
|
|
|
| 15 |
A' |
1023 |
1003 |
27.84 |
|
|
|
| 16 |
A' |
878 |
861 |
5.80 |
|
|
|
| 17 |
A' |
451 |
442 |
10.40 |
|
|
|
| 18 |
A' |
272 |
267 |
3.95 |
|
|
|
| 19 |
A" |
3058 |
2998 |
84.22 |
|
|
|
| 20 |
A" |
3031 |
2971 |
4.84 |
|
|
|
| 21 |
A" |
2926 |
2868 |
79.66 |
|
|
|
| 22 |
A" |
1504 |
1474 |
6.22 |
|
|
|
| 23 |
A" |
1308 |
1283 |
0.35 |
|
|
|
| 24 |
A" |
1256 |
1231 |
0.01 |
|
|
|
| 25 |
A" |
1174 |
1151 |
1.13 |
|
|
|
| 26 |
A" |
896 |
878 |
2.98 |
|
|
|
| 27 |
A" |
762 |
748 |
0.79 |
|
|
|
| 28 |
A" |
280 |
275 |
118.40 |
|
|
|
| 29 |
A" |
232 |
227 |
2.09 |
|
|
|
| 30 |
A" |
122 |
120 |
4.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 23456.6 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 22996.8 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 B97D3/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.453 |
1.236 |
0.000 |
| C2 |
0.000 |
0.745 |
0.000 |
| C3 |
0.099 |
-0.779 |
0.000 |
| O4 |
1.483 |
-1.136 |
0.000 |
| H5 |
-1.499 |
2.334 |
0.000 |
| H6 |
-1.996 |
0.878 |
0.889 |
| H7 |
-1.996 |
0.878 |
-0.889 |
| H8 |
0.534 |
1.128 |
0.884 |
| H9 |
0.534 |
1.128 |
-0.884 |
| H10 |
-0.422 |
-1.183 |
0.892 |
| H11 |
-0.422 |
-1.183 |
-0.892 |
| H12 |
1.530 |
-2.107 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5340 | 2.5430 | 3.7745 | 1.0993 | 1.1012 | 1.1012 | 2.1776 | 2.1776 | 2.7769 | 2.7769 | 4.4804 |
C2 | 1.5340 | | 1.5264 | 2.3948 | 2.1852 | 2.1893 | 2.1893 | 1.1013 | 1.1013 | 2.1657 | 2.1657 | 3.2360 | C3 | 2.5430 | 1.5264 | | 1.4299 | 3.4991 | 2.8150 | 2.8150 | 2.1461 | 2.1461 | 1.1091 | 1.1091 | 1.9526 | O4 | 3.7745 | 2.3948 | 1.4299 | | 4.5755 | 4.1174 | 4.1174 | 2.6086 | 2.6086 | 2.1042 | 2.1042 | 0.9725 | H5 | 1.0993 | 2.1852 | 3.4991 | 4.5755 | | 1.7767 | 1.7767 | 2.5240 | 2.5240 | 3.7854 | 3.7854 | 5.3759 | H6 | 1.1012 | 2.1893 | 2.8150 | 4.1174 | 1.7767 | | 1.7774 | 2.5428 | 3.0995 | 2.5939 | 3.1462 | 4.7048 | H7 | 1.1012 | 2.1893 | 2.8150 | 4.1174 | 1.7767 | 1.7774 | | 3.0995 | 2.5428 | 3.1462 | 2.5939 | 4.7048 | H8 | 2.1776 | 1.1013 | 2.1461 | 2.6086 | 2.5240 | 2.5428 | 3.0995 | | 1.7670 | 2.5013 | 3.0672 | 3.4981 | H9 | 2.1776 | 1.1013 | 2.1461 | 2.6086 | 2.5240 | 3.0995 | 2.5428 | 1.7670 | | 3.0672 | 2.5013 | 3.4981 | H10 | 2.7769 | 2.1657 | 1.1091 | 2.1042 | 3.7854 | 2.5939 | 3.1462 | 2.5013 | 3.0672 | | 1.7836 | 2.3363 | H11 | 2.7769 | 2.1657 | 1.1091 | 2.1042 | 3.7854 | 3.1462 | 2.5939 | 3.0672 | 2.5013 | 1.7836 | | 2.3363 | H12 | 4.4804 | 3.2360 | 1.9526 | 0.9725 | 5.3759 | 4.7048 | 4.7048 | 3.4981 | 3.4981 | 2.3363 | 2.3363 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.386 |
|
C1 |
C2 |
H8 |
110.363 |
| C1 |
C2 |
H9 |
110.363 |
|
C2 |
C1 |
H5 |
111.081 |
| C2 |
C1 |
H6 |
111.296 |
|
C2 |
C1 |
H7 |
111.296 |
| C2 |
C3 |
O4 |
108.160 |
|
C2 |
C3 |
H10 |
109.494 |
| C2 |
C3 |
H11 |
109.494 |
|
C3 |
C2 |
H8 |
108.424 |
| C3 |
C2 |
H9 |
108.424 |
|
C3 |
O4 |
H12 |
107.199 |
| O4 |
C3 |
H10 |
111.319 |
|
O4 |
C3 |
H11 |
111.319 |
| H5 |
C1 |
H6 |
107.688 |
|
H5 |
C1 |
H7 |
107.688 |
| H6 |
C1 |
H7 |
107.611 |
|
H8 |
C2 |
H9 |
106.686 |
| H10 |
C3 |
H11 |
107.038 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.464 |
|
|
|
| 2 |
C |
-0.265 |
|
|
|
| 3 |
C |
-0.039 |
|
|
|
| 4 |
O |
-0.603 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
| 6 |
H |
0.147 |
|
|
|
| 7 |
H |
0.147 |
|
|
|
| 8 |
H |
0.152 |
|
|
|
| 9 |
H |
0.152 |
|
|
|
| 10 |
H |
0.117 |
|
|
|
| 11 |
H |
0.117 |
|
|
|
| 12 |
H |
0.385 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.069 |
-0.980 |
0.000 |
1.450 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.972 |
-1.063 |
0.000 |
| y |
-1.063 |
-21.477 |
0.000 |
| z |
0.000 |
0.000 |
-26.345 |
|
| Traceless |
| | x | y | z |
| x |
-5.061 |
-1.063 |
0.000 |
| y |
-1.063 |
6.182 |
0.000 |
| z |
0.000 |
0.000 |
-1.121 |
|
| Polar |
| 3z2-r2 | -2.242 |
| x2-y2 | -7.495 |
| xy | -1.063 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.802 |
-0.552 |
0.000 |
| y |
-0.552 |
6.013 |
0.000 |
| z |
0.000 |
0.000 |
4.988 |
<r2> (average value of r
2) Å
2
| <r2> |
107.757 |
| (<r2>)1/2 |
10.381 |
Jump to
S1C1
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -194.227158 |
| Energy at 298.15K | |
| HF Energy | -194.227158 |
| Nuclear repulsion energy | 131.903281 |
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 B97D3/6-31G*
| 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 |
3676 |
3604 |
7.44 |
125.55 |
0.31 |
0.47 |
| 2 |
A |
3090 |
3029 |
32.25 |
40.39 |
0.74 |
0.85 |
| 3 |
A |
3059 |
2999 |
59.61 |
59.75 |
0.60 |
0.75 |
| 4 |
A |
3027 |
2967 |
28.65 |
88.17 |
0.73 |
0.85 |
| 5 |
A |
2992 |
2933 |
27.69 |
127.14 |
0.03 |
0.06 |
| 6 |
A |
2988 |
2929 |
53.27 |
91.75 |
0.12 |
0.21 |
| 7 |
A |
2934 |
2876 |
80.98 |
92.11 |
0.74 |
0.85 |
| 8 |
A |
2906 |
2849 |
81.29 |
105.81 |
0.12 |
0.21 |
| 9 |
A |
1523 |
1493 |
3.42 |
6.67 |
0.62 |
0.76 |
| 10 |
A |
1513 |
1483 |
5.89 |
10.21 |
0.75 |
0.85 |
| 11 |
A |
1498 |
1469 |
6.98 |
23.59 |
0.75 |
0.86 |
| 12 |
A |
1480 |
1451 |
1.98 |
19.05 |
0.75 |
0.86 |
| 13 |
A |
1445 |
1417 |
7.30 |
3.08 |
0.61 |
0.76 |
| 14 |
A |
1406 |
1379 |
2.14 |
4.59 |
0.73 |
0.84 |
| 15 |
A |
1368 |
1341 |
3.66 |
1.70 |
0.75 |
0.86 |
| 16 |
A |
1319 |
1293 |
22.36 |
17.40 |
0.74 |
0.85 |
| 17 |
A |
1255 |
1230 |
0.62 |
10.06 |
0.75 |
0.86 |
| 18 |
A |
1245 |
1221 |
37.33 |
8.49 |
0.67 |
0.81 |
| 19 |
A |
1149 |
1127 |
4.45 |
1.85 |
0.48 |
0.65 |
| 20 |
A |
1106 |
1085 |
5.35 |
2.77 |
0.57 |
0.73 |
| 21 |
A |
1050 |
1029 |
42.35 |
2.69 |
0.70 |
0.82 |
| 22 |
A |
972 |
953 |
52.96 |
4.09 |
0.74 |
0.85 |
| 23 |
A |
920 |
902 |
3.15 |
0.63 |
0.74 |
0.85 |
| 24 |
A |
855 |
838 |
1.65 |
9.21 |
0.20 |
0.33 |
| 25 |
A |
768 |
753 |
0.85 |
0.66 |
0.55 |
0.71 |
| 26 |
A |
474 |
465 |
7.74 |
0.29 |
0.47 |
0.64 |
| 27 |
A |
329 |
323 |
9.82 |
0.49 |
0.55 |
0.71 |
| 28 |
A |
256 |
251 |
108.02 |
4.98 |
0.74 |
0.85 |
| 29 |
A |
226 |
222 |
2.23 |
0.10 |
0.65 |
0.79 |
| 30 |
A |
146 |
143 |
7.86 |
0.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 23487.3 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 23026.9 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 B97D3/6-31G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.549 |
-0.517 |
0.130 |
| C2 |
-0.637 |
0.642 |
-0.292 |
| C3 |
0.771 |
0.545 |
0.293 |
| O4 |
1.391 |
-0.638 |
-0.222 |
| H5 |
-2.548 |
-0.420 |
-0.319 |
| H6 |
-1.671 |
-0.542 |
1.224 |
| H7 |
-1.120 |
-1.478 |
-0.183 |
| H8 |
-0.553 |
0.676 |
-1.390 |
| H9 |
-1.071 |
1.605 |
0.025 |
| H10 |
0.709 |
0.512 |
1.400 |
| H11 |
1.351 |
1.449 |
0.021 |
| H12 |
2.257 |
-0.722 |
0.213 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5341 | 2.5563 | 2.9636 | 1.0998 | 1.1015 | 1.0977 | 2.1740 | 2.1774 | 2.7871 | 3.5051 | 3.8118 |
C2 | 1.5341 | | 1.5275 | 2.3994 | 2.1867 | 2.1844 | 2.1775 | 1.1018 | 1.1026 | 2.1658 | 2.1682 | 3.2386 | C3 | 2.5563 | 1.5275 | | 1.4321 | 3.5101 | 2.8307 | 2.8101 | 2.1454 | 2.1419 | 1.1089 | 1.1080 | 1.9545 | O4 | 2.9636 | 2.3994 | 1.4321 | | 3.9465 | 3.3887 | 2.6489 | 2.6211 | 3.3400 | 2.1025 | 2.1012 | 0.9722 | H5 | 1.0998 | 2.1867 | 3.5101 | 3.9465 | | 1.7792 | 1.7821 | 2.5157 | 2.5296 | 3.7987 | 4.3373 | 4.8434 | H6 | 1.1015 | 2.1844 | 2.8307 | 3.3887 | 1.7792 | | 1.7777 | 3.0935 | 2.5311 | 2.6090 | 3.8141 | 4.0604 | H7 | 1.0977 | 2.1775 | 2.8101 | 2.6489 | 1.7821 | 1.7777 | | 2.5339 | 3.0902 | 3.1323 | 3.8363 | 3.4833 | H8 | 2.1740 | 1.1018 | 2.1454 | 2.6211 | 2.5157 | 3.0935 | 2.5339 | | 1.7701 | 3.0664 | 2.4927 | 3.5238 | H9 | 2.1774 | 1.1026 | 2.1419 | 3.3400 | 2.5296 | 2.5311 | 3.0902 | 1.7701 | | 2.5007 | 2.4276 | 4.0650 | H10 | 2.7871 | 2.1658 | 1.1089 | 2.1025 | 3.7987 | 2.6090 | 3.1323 | 3.0664 | 2.5007 | | 1.7867 | 2.3083 | H11 | 3.5051 | 2.1682 | 1.1080 | 2.1012 | 4.3373 | 3.8141 | 3.8363 | 2.4927 | 2.4276 | 1.7867 | | 2.3598 | H12 | 3.8118 | 3.2386 | 1.9545 | 0.9722 | 4.8434 | 4.0604 | 3.4833 | 3.5238 | 4.0650 | 2.3083 | 2.3598 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
113.222 |
|
C1 |
C2 |
H8 |
110.047 |
| C1 |
C2 |
H9 |
110.265 |
|
C2 |
C1 |
H5 |
111.166 |
| C2 |
C1 |
H6 |
110.888 |
|
C2 |
C1 |
H7 |
110.566 |
| C2 |
C3 |
O4 |
108.287 |
|
C2 |
C3 |
H10 |
109.443 |
| C2 |
C3 |
H11 |
109.681 |
|
C3 |
C2 |
H8 |
108.279 |
| C3 |
C2 |
H9 |
107.959 |
|
C3 |
O4 |
H12 |
107.212 |
| O4 |
C3 |
H10 |
111.032 |
|
O4 |
C3 |
H11 |
110.983 |
| H5 |
C1 |
H6 |
107.845 |
|
H5 |
C1 |
H7 |
108.379 |
| H6 |
C1 |
H7 |
107.876 |
|
H8 |
C2 |
H9 |
106.837 |
| H10 |
C3 |
H11 |
107.403 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.454 |
|
|
|
| 2 |
C |
-0.268 |
|
|
|
| 3 |
C |
-0.044 |
|
|
|
| 4 |
O |
-0.600 |
|
|
|
| 5 |
H |
0.144 |
|
|
|
| 6 |
H |
0.139 |
|
|
|
| 7 |
H |
0.173 |
|
|
|
| 8 |
H |
0.151 |
|
|
|
| 9 |
H |
0.135 |
|
|
|
| 10 |
H |
0.117 |
|
|
|
| 11 |
H |
0.120 |
|
|
|
| 12 |
H |
0.386 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.733 |
0.810 |
0.986 |
1.472 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.490 |
-0.273 |
2.063 |
| y |
-0.273 |
-26.759 |
-0.591 |
| z |
2.063 |
-0.591 |
-26.466 |
|
| Traceless |
| | x | y | z |
| x |
4.122 |
-0.273 |
2.063 |
| y |
-0.273 |
-2.281 |
-0.591 |
| z |
2.063 |
-0.591 |
-1.841 |
|
| Polar |
| 3z2-r2 | -3.682 |
| x2-y2 | 4.269 |
| xy | -0.273 |
| xz | 2.063 |
| yz | -0.591 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.183 |
-0.013 |
0.145 |
| y |
-0.013 |
5.444 |
0.032 |
| z |
0.145 |
0.032 |
5.147 |
<r2> (average value of r
2) Å
2
| <r2> |
95.839 |
| (<r2>)1/2 |
9.790 |