Jump to
S1C2
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -154.277052 |
Energy at 298.15K | |
HF Energy | -154.277052 |
Nuclear repulsion energy | 74.915610 |
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' |
3791 |
3599 |
8.48 |
|
|
|
2 |
A' |
3196 |
3034 |
9.66 |
|
|
|
3 |
A' |
3018 |
2865 |
66.76 |
|
|
|
4 |
A' |
1552 |
1474 |
1.19 |
|
|
|
5 |
A' |
1505 |
1429 |
4.85 |
|
|
|
6 |
A' |
1453 |
1379 |
7.76 |
|
|
|
7 |
A' |
1250 |
1187 |
59.26 |
|
|
|
8 |
A' |
1078 |
1023 |
96.74 |
|
|
|
9 |
A' |
1025 |
973 |
26.01 |
|
|
|
10 |
A' |
610 |
579 |
18.26 |
|
|
|
11 |
A' |
371 |
352 |
32.71 |
|
|
|
12 |
A" |
3303 |
3136 |
13.54 |
|
|
|
13 |
A" |
3053 |
2898 |
65.96 |
|
|
|
14 |
A" |
1300 |
1234 |
0.21 |
|
|
|
15 |
A" |
1183 |
1123 |
1.30 |
|
|
|
16 |
A" |
815 |
773 |
0.20 |
|
|
|
17 |
A" |
267 |
253 |
133.26 |
|
|
|
18 |
A" |
133i |
126i |
1.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14318.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 13592.5 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) |
O1 |
-1.110 |
-0.364 |
0.000 |
C2 |
0.000 |
0.532 |
0.000 |
C3 |
1.256 |
-0.254 |
0.000 |
H4 |
-1.911 |
0.175 |
0.000 |
H5 |
-0.031 |
1.182 |
0.886 |
H6 |
-0.031 |
1.182 |
-0.886 |
H7 |
1.657 |
-0.646 |
-0.927 |
H8 |
1.657 |
-0.646 |
0.927 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
O1 | | 1.4265 | 2.3682 | 0.9659 | 2.0831 | 2.0831 | 2.9308 | 2.9308 |
C2 | 1.4265 | | 1.4820 | 1.9440 | 1.0992 | 1.0992 | 2.2342 | 2.2342 | C3 | 2.3682 | 1.4820 | | 3.1959 | 2.1225 | 2.1225 | 1.0832 | 1.0832 | H4 | 0.9659 | 1.9440 | 3.1959 | | 2.3094 | 2.3094 | 3.7762 | 3.7762 | H5 | 2.0831 | 1.0992 | 2.1225 | 2.3094 | | 1.7719 | 3.0784 | 2.4882 | H6 | 2.0831 | 1.0992 | 2.1225 | 2.3094 | 1.7719 | | 2.4882 | 3.0784 | H7 | 2.9308 | 2.2342 | 1.0832 | 3.7762 | 3.0784 | 2.4882 | | 1.8543 | H8 | 2.9308 | 2.2342 | 1.0832 | 3.7762 | 2.4882 | 3.0784 | 1.8543 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C3 |
109.007 |
|
O1 |
C2 |
H5 |
110.463 |
O1 |
C2 |
H6 |
110.463 |
|
C2 |
O1 |
H4 |
107.126 |
C2 |
C3 |
H7 |
120.344 |
|
C2 |
C3 |
H8 |
120.344 |
C3 |
C2 |
H5 |
109.738 |
|
C3 |
C2 |
H6 |
109.738 |
H5 |
C2 |
H6 |
107.415 |
|
H7 |
C3 |
H8 |
117.730 |
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 |
O |
-0.624 |
|
|
|
2 |
C |
-0.086 |
|
|
|
3 |
C |
-0.319 |
|
|
|
4 |
H |
0.399 |
|
|
|
5 |
H |
0.143 |
|
|
|
6 |
H |
0.143 |
|
|
|
7 |
H |
0.172 |
|
|
|
8 |
H |
0.172 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.187 |
1.514 |
0.000 |
1.526 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.319 |
-2.846 |
0.000 |
y |
-2.846 |
-19.722 |
0.000 |
z |
0.000 |
0.000 |
-18.565 |
|
Traceless |
| x | y | z |
x |
2.825 |
-2.846 |
0.000 |
y |
-2.846 |
-2.280 |
0.000 |
z |
0.000 |
0.000 |
-0.545 |
|
Polar |
3z2-r2 | -1.090 |
x2-y2 | 3.403 |
xy | -2.846 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.192 |
-0.540 |
0.000 |
y |
-0.540 |
3.175 |
0.000 |
z |
0.000 |
0.000 |
3.381 |
<r2> (average value of r
2) Å
2
<r2> |
49.923 |
(<r2>)1/2 |
7.066 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -154.278910 |
Energy at 298.15K | -154.283530 |
HF Energy | -154.278910 |
Nuclear repulsion energy | 75.277192 |
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 |
3828 |
3634 |
17.76 |
|
|
|
2 |
A |
3321 |
3153 |
7.14 |
|
|
|
3 |
A |
3208 |
3046 |
5.51 |
|
|
|
4 |
A |
2981 |
2830 |
69.74 |
|
|
|
5 |
A |
2916 |
2768 |
72.45 |
|
|
|
6 |
A |
1528 |
1450 |
7.07 |
|
|
|
7 |
A |
1492 |
1417 |
6.28 |
|
|
|
8 |
A |
1441 |
1368 |
1.81 |
|
|
|
9 |
A |
1290 |
1225 |
77.04 |
|
|
|
10 |
A |
1235 |
1172 |
7.15 |
|
|
|
11 |
A |
1157 |
1098 |
48.77 |
|
|
|
12 |
A |
1085 |
1030 |
23.85 |
|
|
|
13 |
A |
979 |
930 |
11.25 |
|
|
|
14 |
A |
880 |
835 |
14.25 |
|
|
|
15 |
A |
447 |
424 |
21.08 |
|
|
|
16 |
A |
389 |
369 |
51.81 |
|
|
|
17 |
A |
287 |
272 |
98.04 |
|
|
|
18 |
A |
138 |
131 |
24.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14300.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 13575.4 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 C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-1.099 |
-0.381 |
-0.058 |
C2 |
-0.012 |
0.520 |
0.034 |
C3 |
1.242 |
-0.252 |
-0.018 |
H4 |
-1.901 |
0.126 |
0.109 |
H5 |
-0.070 |
1.097 |
0.977 |
H6 |
-0.035 |
1.262 |
-0.780 |
H7 |
2.182 |
0.245 |
-0.217 |
H8 |
1.240 |
-1.293 |
0.278 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
O1 | | 1.4147 | 2.3452 | 0.9637 | 2.0772 | 2.0863 | 3.3440 | 2.5329 |
C2 | 1.4147 | | 1.4742 | 1.9312 | 1.1066 | 1.1019 | 2.2256 | 2.2166 | C3 | 2.3452 | 1.4742 | | 3.1688 | 2.1287 | 2.1227 | 1.0819 | 1.0816 | H4 | 0.9637 | 1.9312 | 3.1688 | | 2.2470 | 2.3590 | 4.0981 | 3.4509 | H5 | 2.0772 | 1.1066 | 2.1287 | 2.2470 | | 1.7650 | 2.6875 | 2.8129 | H6 | 2.0863 | 1.1019 | 2.1227 | 2.3590 | 1.7650 | | 2.5030 | 3.0450 | H7 | 3.3440 | 2.2256 | 1.0819 | 4.0981 | 2.6875 | 2.5030 | | 1.8703 | H8 | 2.5329 | 2.2166 | 1.0816 | 3.4509 | 2.8129 | 3.0450 | 1.8703 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C3 |
108.525 |
|
O1 |
C2 |
H5 |
110.345 |
O1 |
C2 |
H6 |
111.389 |
|
C2 |
O1 |
H4 |
107.043 |
C2 |
C3 |
H7 |
120.309 |
|
C2 |
C3 |
H8 |
119.504 |
C3 |
C2 |
H5 |
110.330 |
|
C3 |
C2 |
H6 |
110.143 |
H5 |
C2 |
H6 |
106.108 |
|
H7 |
C3 |
H8 |
119.652 |
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 |
O |
-0.627 |
|
|
|
2 |
C |
-0.074 |
|
|
|
3 |
C |
-0.340 |
|
|
|
4 |
H |
0.404 |
|
|
|
5 |
H |
0.147 |
|
|
|
6 |
H |
0.148 |
|
|
|
7 |
H |
0.160 |
|
|
|
8 |
H |
0.181 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.323 |
1.680 |
0.472 |
1.774 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-15.559 |
-1.853 |
-0.551 |
y |
-1.853 |
-18.928 |
-0.414 |
z |
-0.551 |
-0.414 |
-20.015 |
|
Traceless |
| x | y | z |
x |
3.913 |
-1.853 |
-0.551 |
y |
-1.853 |
-1.141 |
-0.414 |
z |
-0.551 |
-0.414 |
-2.772 |
|
Polar |
3z2-r2 | -5.544 |
x2-y2 | 3.370 |
xy | -1.853 |
xz | -0.551 |
yz | -0.414 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.367 |
-0.215 |
-0.178 |
y |
-0.215 |
3.729 |
-0.123 |
z |
-0.178 |
-0.123 |
2.662 |
<r2> (average value of r
2) Å
2
<r2> |
49.752 |
(<r2>)1/2 |
7.053 |