Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -191.768696 |
| Energy at 298.15K | |
| HF Energy | -191.768696 |
| Nuclear repulsion energy | 102.695689 |
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 B1B95/6-31G
| 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' |
3293 |
3141 |
8.57 |
67.14 |
0.51 |
0.67 |
| 2 |
A' |
3239 |
3089 |
1.76 |
90.30 |
0.33 |
0.49 |
| 3 |
A' |
3190 |
3042 |
4.99 |
69.49 |
0.10 |
0.19 |
| 4 |
A' |
2990 |
2851 |
89.89 |
88.23 |
0.28 |
0.43 |
| 5 |
A' |
1755 |
1674 |
158.66 |
88.19 |
0.33 |
0.50 |
| 6 |
A' |
1710 |
1631 |
28.86 |
3.81 |
0.12 |
0.22 |
| 7 |
A' |
1493 |
1424 |
8.58 |
10.02 |
0.48 |
0.65 |
| 8 |
A' |
1427 |
1361 |
7.76 |
18.28 |
0.46 |
0.63 |
| 9 |
A' |
1331 |
1270 |
2.26 |
10.57 |
0.34 |
0.51 |
| 10 |
A' |
1212 |
1156 |
31.44 |
11.95 |
0.64 |
0.78 |
| 11 |
A' |
955 |
911 |
22.13 |
1.14 |
0.11 |
0.20 |
| 12 |
A' |
581 |
554 |
8.01 |
6.89 |
0.38 |
0.55 |
| 13 |
A' |
320 |
305 |
10.00 |
0.64 |
0.29 |
0.45 |
| 14 |
A" |
1060 |
1011 |
2.37 |
1.59 |
0.75 |
0.86 |
| 15 |
A" |
1051 |
1003 |
26.85 |
5.21 |
0.75 |
0.86 |
| 16 |
A" |
1027 |
979 |
46.93 |
1.93 |
0.75 |
0.86 |
| 17 |
A" |
626 |
597 |
12.55 |
5.75 |
0.75 |
0.86 |
| 18 |
A" |
183 |
175 |
5.09 |
1.30 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13721.1 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 13085.8 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 B1B95/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.136 |
-0.741 |
0.000 |
| C2 |
0.000 |
0.715 |
0.000 |
| C3 |
1.206 |
1.295 |
0.000 |
| O4 |
-1.220 |
-1.334 |
0.000 |
| H5 |
0.813 |
-1.304 |
0.000 |
| H6 |
-0.919 |
1.291 |
0.000 |
| H7 |
1.333 |
2.370 |
0.000 |
| H8 |
2.114 |
0.700 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4629 | 2.4384 | 1.2352 | 1.1035 | 2.1775 | 3.4402 | 2.6725 |
C2 | 1.4629 | | 1.3377 | 2.3850 | 2.1769 | 1.0840 | 2.1244 | 2.1144 | C3 | 2.4384 | 1.3377 | | 3.5769 | 2.6284 | 2.1242 | 1.0823 | 1.0859 | O4 | 1.2352 | 2.3850 | 3.5769 | | 2.0329 | 2.6424 | 4.4982 | 3.9057 | H5 | 1.1035 | 2.1769 | 2.6284 | 2.0329 | | 3.1197 | 3.7102 | 2.3897 | H6 | 2.1775 | 1.0840 | 2.1242 | 2.6424 | 3.1197 | | 2.4964 | 3.0898 | H7 | 3.4402 | 2.1244 | 1.0823 | 4.4982 | 3.7102 | 2.4964 | | 1.8432 | H8 | 2.6725 | 2.1144 | 1.0859 | 3.9057 | 2.3897 | 3.0898 | 1.8432 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.014 |
|
C1 |
C2 |
H6 |
116.733 |
| C2 |
C1 |
O4 |
124.038 |
|
C2 |
C1 |
H5 |
115.325 |
| C2 |
C3 |
H7 |
122.422 |
|
C2 |
C3 |
H8 |
121.129 |
| C3 |
C2 |
H6 |
122.254 |
|
O4 |
C1 |
H5 |
120.637 |
| H7 |
C3 |
H8 |
116.449 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.181 |
|
|
|
| 2 |
C |
-0.124 |
|
|
|
| 3 |
C |
-0.321 |
|
|
|
| 4 |
O |
-0.406 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
| 6 |
H |
0.189 |
|
|
|
| 7 |
H |
0.177 |
|
|
|
| 8 |
H |
0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.689 |
2.273 |
0.000 |
3.521 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.484 |
-3.007 |
0.000 |
| y |
-3.007 |
-23.971 |
0.000 |
| z |
0.000 |
0.000 |
-24.527 |
|
| Traceless |
| | x | y | z |
| x |
-0.235 |
-3.007 |
0.000 |
| y |
-3.007 |
0.534 |
0.000 |
| z |
0.000 |
0.000 |
-0.299 |
|
| Polar |
| 3z2-r2 | -0.598 |
| x2-y2 | -0.513 |
| xy | -3.007 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.684 |
1.860 |
0.000 |
| y |
1.860 |
6.000 |
0.000 |
| z |
0.000 |
0.000 |
1.827 |
<r2> (average value of r
2) Å
2
| <r2> |
83.820 |
| (<r2>)1/2 |
9.155 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -191.766682 |
| Energy at 298.15K | |
| HF Energy | -191.766682 |
| Nuclear repulsion energy | 104.345198 |
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 B1B95/6-31G
| 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' |
3302 |
3149 |
3.82 |
54.74 |
0.58 |
0.74 |
| 2 |
A' |
3229 |
3080 |
10.68 |
109.55 |
0.25 |
0.40 |
| 3 |
A' |
3198 |
3050 |
3.75 |
53.87 |
0.12 |
0.21 |
| 4 |
A' |
3026 |
2886 |
124.48 |
141.16 |
0.32 |
0.48 |
| 5 |
A' |
1755 |
1674 |
33.09 |
3.95 |
0.66 |
0.80 |
| 6 |
A' |
1693 |
1615 |
113.35 |
59.77 |
0.28 |
0.43 |
| 7 |
A' |
1477 |
1409 |
40.63 |
9.23 |
0.39 |
0.56 |
| 8 |
A' |
1455 |
1388 |
5.22 |
10.91 |
0.50 |
0.67 |
| 9 |
A' |
1353 |
1290 |
2.24 |
15.73 |
0.44 |
0.61 |
| 10 |
A' |
1103 |
1052 |
6.22 |
4.80 |
0.75 |
0.86 |
| 11 |
A' |
976 |
931 |
57.45 |
5.77 |
0.24 |
0.39 |
| 12 |
A' |
700 |
668 |
10.77 |
1.10 |
0.74 |
0.85 |
| 13 |
A' |
294 |
280 |
8.61 |
3.75 |
0.50 |
0.67 |
| 14 |
A" |
1068 |
1019 |
0.58 |
9.56 |
0.75 |
0.86 |
| 15 |
A" |
1053 |
1004 |
64.55 |
0.11 |
0.75 |
0.86 |
| 16 |
A" |
1037 |
989 |
0.68 |
2.17 |
0.75 |
0.86 |
| 17 |
A" |
586 |
559 |
12.34 |
7.05 |
0.75 |
0.86 |
| 18 |
A" |
197 |
188 |
9.29 |
0.84 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13750.0 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 13113.4 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 B1B95/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.891 |
-0.271 |
0.000 |
| C2 |
0.000 |
0.899 |
0.000 |
| C3 |
1.331 |
0.761 |
0.000 |
| O4 |
-0.496 |
-1.443 |
0.000 |
| H5 |
-1.970 |
-0.054 |
0.000 |
| H6 |
-0.471 |
1.876 |
0.000 |
| H7 |
2.001 |
1.611 |
0.000 |
| H8 |
1.772 |
-0.229 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4708 | 2.4499 | 1.2372 | 1.1001 | 2.1875 | 3.4506 | 2.6636 |
C2 | 1.4708 | | 1.3378 | 2.3943 | 2.1886 | 1.0844 | 2.1239 | 2.1010 | C3 | 2.4499 | 1.3378 | | 2.8629 | 3.3998 | 2.1186 | 1.0824 | 1.0847 | O4 | 1.2372 | 2.3943 | 2.8629 | | 2.0249 | 3.3192 | 3.9451 | 2.5724 | H5 | 1.1001 | 2.1886 | 3.3998 | 2.0249 | | 2.4440 | 4.3060 | 3.7460 | H6 | 2.1875 | 1.0844 | 2.1186 | 3.3192 | 2.4440 | | 2.4861 | 3.0764 | H7 | 3.4506 | 2.1239 | 1.0824 | 3.9451 | 4.3060 | 2.4861 | | 1.8548 | H8 | 2.6636 | 2.1010 | 1.0847 | 2.5724 | 3.7460 | 3.0764 | 1.8548 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.379 |
|
C1 |
C2 |
H6 |
116.961 |
| C2 |
C1 |
O4 |
124.076 |
|
C2 |
C1 |
H5 |
115.958 |
| C2 |
C3 |
H7 |
122.348 |
|
C2 |
C3 |
H8 |
119.930 |
| C3 |
C2 |
H6 |
121.660 |
|
O4 |
C1 |
H5 |
119.966 |
| H7 |
C3 |
H8 |
117.721 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.177 |
|
|
|
| 2 |
C |
-0.155 |
|
|
|
| 3 |
C |
-0.291 |
|
|
|
| 4 |
O |
-0.403 |
|
|
|
| 5 |
H |
0.136 |
|
|
|
| 6 |
H |
0.168 |
|
|
|
| 7 |
H |
0.170 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.266 |
2.952 |
0.000 |
2.964 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.723 |
-0.709 |
0.000 |
| y |
-0.709 |
-26.447 |
0.000 |
| z |
0.000 |
0.000 |
-24.500 |
|
| Traceless |
| | x | y | z |
| x |
5.750 |
-0.709 |
0.000 |
| y |
-0.709 |
-4.335 |
0.000 |
| z |
0.000 |
0.000 |
-1.415 |
|
| Polar |
| 3z2-r2 | -2.830 |
| x2-y2 | 6.724 |
| xy | -0.709 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.667 |
0.483 |
0.000 |
| y |
0.483 |
5.489 |
0.000 |
| z |
0.000 |
0.000 |
1.826 |
<r2> (average value of r
2) Å
2
| <r2> |
74.917 |
| (<r2>)1/2 |
8.655 |