Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| hartrees |
Energy at 0K | -959.101835 |
Energy at 298.15K | |
HF Energy | -959.101835 |
Nuclear repulsion energy | 126.107576 |
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 B1B95/6-31+G**
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 |
3305 |
3161 |
0.42 |
|
|
|
2 |
A1 |
775 |
742 |
8.83 |
|
|
|
3 |
A1 |
319 |
305 |
0.30 |
|
|
|
4 |
B1 |
320i |
306i |
59.93 |
|
|
|
5 |
B2 |
1264 |
1209 |
54.11 |
|
|
|
6 |
B2 |
953 |
912 |
170.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3147.8 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3011.2 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 B1B95/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.666 |
H2 |
0.000 |
0.000 |
1.743 |
Cl3 |
0.000 |
1.473 |
-0.169 |
Cl4 |
0.000 |
-1.473 |
-0.169 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0775 | 1.6926 | 1.6926 |
H2 | 1.0775 | | 2.4133 | 2.4133 | Cl3 | 1.6926 | 2.4133 | | 2.9452 | Cl4 | 1.6926 | 2.4133 | 2.9452 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.538 |
|
Cl3 |
C1 |
Cl4 |
120.923 |
Cl4 |
C1 |
H2 |
119.538 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.383 |
|
|
|
2 |
H |
0.232 |
|
|
|
3 |
Cl |
0.075 |
|
|
|
4 |
Cl |
0.075 |
|
|
|
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 |
0.956 |
0.956 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.012 |
0.000 |
0.000 |
y |
0.000 |
-31.078 |
0.000 |
z |
0.000 |
0.000 |
-29.003 |
|
Traceless |
| x | y | z |
x |
-1.971 |
0.000 |
0.000 |
y |
0.000 |
-0.571 |
0.000 |
z |
0.000 |
0.000 |
2.542 |
|
Polar |
3z2-r2 | 5.084 |
x2-y2 | -0.933 |
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 |
3.281 |
0.000 |
0.000 |
y |
0.000 |
7.163 |
0.000 |
z |
0.000 |
0.000 |
4.321 |
<r2> (average value of r
2) Å
2
<r2> |
99.569 |
(<r2>)1/2 |
9.978 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| hartrees |
Energy at 0K | -959.102326 |
Energy at 298.15K | -959.103097 |
HF Energy | -959.102326 |
Nuclear repulsion energy | 125.976613 |
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 B1B95/6-31+G**
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' |
3269 |
3127 |
0.83 |
|
|
|
2 |
A' |
778 |
744 |
13.14 |
|
|
|
3 |
A' |
434 |
415 |
33.22 |
|
|
|
4 |
A' |
311 |
297 |
1.52 |
|
|
|
5 |
A" |
1269 |
1213 |
47.00 |
|
|
|
6 |
A" |
928 |
887 |
192.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3494.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3342.5 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.011 |
0.685 |
0.000 |
H2 |
-0.434 |
1.669 |
0.000 |
Cl3 |
0.011 |
-0.170 |
1.470 |
Cl4 |
0.011 |
-0.170 |
-1.470 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0801 | 1.7001 | 1.7001 |
H2 | 1.0801 | | 2.3958 | 2.3958 | Cl3 | 1.7001 | 2.3958 | | 2.9393 | Cl4 | 1.7001 | 2.3958 | 2.9393 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
117.268 |
|
Cl3 |
C1 |
Cl4 |
119.638 |
Cl4 |
C1 |
H2 |
117.268 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.361 |
|
|
|
2 |
H |
0.226 |
|
|
|
3 |
Cl |
0.068 |
|
|
|
4 |
Cl |
0.068 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.484 |
0.884 |
0.000 |
1.008 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.767 |
-0.907 |
0.000 |
y |
-0.907 |
-29.380 |
0.000 |
z |
0.000 |
0.000 |
-31.206 |
|
Traceless |
| x | y | z |
x |
-1.474 |
-0.907 |
0.000 |
y |
-0.907 |
2.107 |
0.000 |
z |
0.000 |
0.000 |
-0.633 |
|
Polar |
3z2-r2 | -1.266 |
x2-y2 | -2.387 |
xy | -0.907 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.342 |
-0.079 |
0.000 |
y |
-0.079 |
4.352 |
0.000 |
z |
0.000 |
0.000 |
7.230 |
<r2> (average value of r
2) Å
2
<r2> |
99.437 |
(<r2>)1/2 |
9.972 |