Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| hartrees |
Energy at 0K | -114.395228 |
Energy at 298.15K | -114.396618 |
HF Energy | -114.395228 |
Nuclear repulsion energy | 29.781948 |
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/LANL2DZ
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' |
3639 |
3497 |
44.28 |
|
|
|
2 |
A' |
2843 |
2733 |
164.89 |
|
|
|
3 |
A' |
1476 |
1419 |
39.16 |
|
|
|
4 |
A' |
1205 |
1158 |
22.88 |
|
|
|
5 |
A' |
1156 |
1111 |
224.19 |
|
|
|
6 |
A" |
1063 |
1022 |
184.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5690.8 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5470.0 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.774 |
0.000 |
O2 |
0.012 |
-0.588 |
0.000 |
H3 |
-1.091 |
1.005 |
0.000 |
H4 |
0.927 |
-0.947 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.3618 | 1.1268 | 1.9486 |
O2 | 1.3618 | | 1.9370 | 0.9827 | H3 | 1.1268 | 1.9370 | | 2.8068 | H4 | 1.9486 | 0.9827 | 2.8068 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
111.412 |
|
O2 |
C1 |
H3 |
101.805 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.139 |
|
|
|
2 |
O |
-0.398 |
|
|
|
3 |
H |
0.137 |
|
|
|
4 |
H |
0.400 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.265 |
-1.500 |
0.000 |
1.523 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.041 |
-4.404 |
0.000 |
y |
-4.404 |
-13.903 |
0.000 |
z |
0.000 |
0.000 |
-11.957 |
|
Traceless |
| x | y | z |
x |
1.889 |
-4.404 |
0.000 |
y |
-4.404 |
-2.404 |
0.000 |
z |
0.000 |
0.000 |
0.515 |
|
Polar |
3z2-r2 | 1.029 |
x2-y2 | 2.862 |
xy | -4.404 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.301 |
-0.586 |
0.000 |
y |
-0.586 |
2.606 |
0.000 |
z |
0.000 |
0.000 |
1.410 |
<r2> (average value of r
2) Å
2
<r2> |
17.997 |
(<r2>)1/2 |
4.242 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| hartrees |
Energy at 0K | -114.384752 |
Energy at 298.15K | -114.386127 |
HF Energy | -114.384752 |
Nuclear repulsion energy | 29.727641 |
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/LANL2DZ
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' |
3364 |
3234 |
39.53 |
|
|
|
2 |
A' |
2683 |
2579 |
259.42 |
|
|
|
3 |
A' |
1417 |
1362 |
88.36 |
|
|
|
4 |
A' |
1235 |
1187 |
33.60 |
|
|
|
5 |
A' |
1142 |
1097 |
71.77 |
|
|
|
6 |
A" |
983 |
945 |
46.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5412.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 5202.1 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.121 |
0.772 |
0.000 |
O2 |
0.121 |
-0.580 |
0.000 |
H3 |
-0.969 |
1.107 |
0.000 |
H4 |
-0.728 |
-1.099 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.3511 | 1.1410 | 2.0545 |
O2 | 1.3511 | | 2.0081 | 0.9955 | H3 | 1.1410 | 2.0081 | | 2.2191 | H4 | 2.0545 | 0.9955 | 2.2191 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
121.479 |
|
O2 |
C1 |
H3 |
107.076 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.054 |
|
|
|
2 |
O |
-0.393 |
|
|
|
3 |
H |
0.095 |
|
|
|
4 |
H |
0.352 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-3.590 |
-1.600 |
0.000 |
3.930 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.596 |
-0.083 |
0.000 |
y |
-0.083 |
-13.269 |
0.000 |
z |
0.000 |
0.000 |
-11.911 |
|
Traceless |
| x | y | z |
x |
-0.006 |
-0.083 |
0.000 |
y |
-0.083 |
-1.016 |
0.000 |
z |
0.000 |
0.000 |
1.022 |
|
Polar |
3z2-r2 | 2.043 |
x2-y2 | 0.673 |
xy | -0.083 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.219 |
0.126 |
0.000 |
y |
0.126 |
3.204 |
0.000 |
z |
0.000 |
0.000 |
1.460 |
<r2> (average value of r
2) Å
2
<r2> |
18.231 |
(<r2>)1/2 |
4.270 |