Jump to
S1C2
Energy calculated at BLYP/6-311G**
| hartrees |
Energy at 0K | -499.440027 |
Energy at 298.15K | |
HF Energy | -499.440027 |
Nuclear repulsion energy | 44.736933 |
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 BLYP/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' |
3095 |
3083 |
7.49 |
|
|
|
2 |
A' |
1371 |
1366 |
10.77 |
|
|
|
3 |
A' |
787 |
784 |
36.49 |
|
|
|
4 |
A' |
112 |
112 |
91.43 |
|
|
|
5 |
A" |
3251 |
3239 |
0.56 |
|
|
|
6 |
A" |
974 |
970 |
1.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4795.1 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 4776.4 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.000 |
1.137 |
0.000 |
Cl2 |
-0.000 |
-0.594 |
0.000 |
H3 |
0.001 |
1.634 |
0.963 |
H4 |
0.001 |
1.634 |
-0.963 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7307 | 1.0835 | 1.0835 |
Cl2 | 1.7307 | | 2.4266 | 2.4266 | H3 | 1.0835 | 2.4266 | | 1.9260 | H4 | 1.0835 | 2.4266 | 1.9260 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.281 |
|
Br2 |
C1 |
H4 |
117.281 |
H3 |
C1 |
H4 |
125.438 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.314 |
|
|
|
2 |
Cl |
-0.017 |
|
|
|
3 |
H |
0.166 |
|
|
|
4 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.002 |
1.111 |
0.000 |
1.111 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.869 |
0.004 |
0.000 |
y |
0.004 |
-17.725 |
0.000 |
z |
0.000 |
0.000 |
-18.836 |
|
Traceless |
| x | y | z |
x |
-2.589 |
0.004 |
0.000 |
y |
0.004 |
2.128 |
0.000 |
z |
0.000 |
0.000 |
0.461 |
|
Polar |
3z2-r2 | 0.922 |
x2-y2 | -3.144 |
xy | 0.004 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.754 |
0.000 |
0.000 |
y |
0.000 |
4.849 |
0.000 |
z |
0.000 |
0.000 |
2.371 |
<r2> (average value of r
2) Å
2
<r2> |
32.898 |
(<r2>)1/2 |
5.736 |
Jump to
S1C1
Energy calculated at BLYP/6-311G**
| hartrees |
Energy at 0K | -499.440033 |
Energy at 298.15K | -499.440716 |
HF Energy | -499.440033 |
Nuclear repulsion energy | 44.719460 |
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 BLYP/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 |
A1 |
3097 |
3085 |
7.43 |
|
|
|
2 |
A1 |
1371 |
1365 |
10.76 |
|
|
|
3 |
A1 |
783 |
780 |
36.62 |
|
|
|
4 |
B1 |
110 |
109 |
91.49 |
|
|
|
5 |
B2 |
3253 |
3241 |
0.53 |
|
|
|
6 |
B2 |
975 |
971 |
1.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4794.3 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 4775.6 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 BLYP/6-311G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.138 |
Cl2 |
0.000 |
0.000 |
0.594 |
H3 |
0.000 |
0.963 |
-1.634 |
H4 |
0.000 |
-0.963 |
-1.634 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7317 | 1.0835 | 1.0835 |
Cl2 | 1.7317 | | 2.4268 | 2.4268 | H3 | 1.0835 | 2.4268 | | 1.9270 | H4 | 1.0835 | 2.4268 | 1.9270 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
117.224 |
|
Br2 |
C1 |
H4 |
117.224 |
H3 |
C1 |
H4 |
125.551 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.314 |
|
|
|
2 |
Cl |
-0.017 |
|
|
|
3 |
H |
0.166 |
|
|
|
4 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-1.114 |
1.114 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.871 |
0.000 |
0.000 |
y |
0.000 |
-18.834 |
0.000 |
z |
0.000 |
0.000 |
-17.725 |
|
Traceless |
| x | y | z |
x |
-2.592 |
0.000 |
0.000 |
y |
0.000 |
0.464 |
0.000 |
z |
0.000 |
0.000 |
2.128 |
|
Polar |
3z2-r2 | 4.255 |
x2-y2 | -2.038 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.754 |
0.000 |
0.000 |
y |
0.000 |
2.372 |
0.000 |
z |
0.000 |
0.000 |
4.851 |
<r2> (average value of r
2) Å
2
<r2> |
32.912 |
(<r2>)1/2 |
5.737 |