Jump to
S1C2
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -2608.721119 |
| Energy at 298.15K | -2608.724804 |
| HF Energy | -2608.721119 |
| Nuclear repulsion energy | 78.610123 |
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 ROHF/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' |
3361 |
3009 |
5.62 |
|
|
|
| 2 |
A' |
1481 |
1326 |
51.50 |
|
|
|
| 3 |
A' |
642 |
575 |
23.42 |
|
|
|
| 4 |
A' |
198 |
177 |
94.07 |
|
|
|
| 5 |
A" |
3537 |
3167 |
0.00 |
|
|
|
| 6 |
A" |
982 |
879 |
0.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5100.0 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 4566.1 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 ROHF/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.004 |
1.537 |
0.000 |
| Br2 |
-0.004 |
-0.379 |
0.000 |
| H3 |
0.080 |
2.019 |
0.948 |
| H4 |
0.080 |
2.019 |
-0.948 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.9154 | 1.0668 | 1.0668 |
Br2 | 1.9154 | | 2.5796 | 2.5796 | H3 | 1.0668 | 2.5796 | | 1.8955 | H4 | 1.0668 | 2.5796 | 1.8955 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
116.884 |
|
Br2 |
C1 |
H4 |
116.884 |
| H3 |
C1 |
H4 |
125.356 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.486 |
|
|
|
| 2 |
Br |
0.043 |
|
|
|
| 3 |
H |
0.221 |
|
|
|
| 4 |
H |
0.221 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.176 |
1.759 |
0.000 |
1.768 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.503 |
0.347 |
0.000 |
| y |
0.347 |
-21.677 |
0.000 |
| z |
0.000 |
0.000 |
-24.476 |
|
| Traceless |
| | x | y | z |
| x |
-3.427 |
0.347 |
0.000 |
| y |
0.347 |
3.812 |
0.000 |
| z |
0.000 |
0.000 |
-0.385 |
|
| Polar |
| 3z2-r2 | -0.771 |
| x2-y2 | -4.826 |
| xy | 0.347 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
44.277 |
| (<r2>)1/2 |
6.654 |
Jump to
S1C1
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -2608.716996 |
| Energy at 298.15K | |
| HF Energy | -2608.716996 |
| Nuclear repulsion energy | 78.826758 |
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 ROHF/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 |
A1 |
3383 |
3028 |
5.14 |
|
|
|
| 2 |
A1 |
1491 |
1335 |
52.64 |
|
|
|
| 3 |
A1 |
658 |
589 |
25.10 |
|
|
|
| 4 |
B1 |
422i |
378i |
109.51 |
|
|
|
| 5 |
B2 |
3565 |
3191 |
0.12 |
|
|
|
| 6 |
B2 |
989 |
885 |
0.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4831.2 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 4325.4 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 ROHF/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.531 |
| Br2 |
0.000 |
0.000 |
0.378 |
| H3 |
0.000 |
0.948 |
-2.017 |
| H4 |
0.000 |
-0.948 |
-2.017 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
H4 |
| C1 | | 1.9093 | 1.0652 | 1.0652 |
Br2 | 1.9093 | | 2.5755 | 2.5755 | H3 | 1.0652 | 2.5755 | | 1.8965 | H4 | 1.0652 | 2.5755 | 1.8965 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.104 |
|
Br2 |
C1 |
H4 |
117.104 |
| H3 |
C1 |
H4 |
125.792 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.503 |
|
|
|
| 2 |
Br |
0.048 |
|
|
|
| 3 |
H |
0.227 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
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 |
-1.766 |
1.766 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.541 |
0.000 |
0.000 |
| y |
0.000 |
-24.427 |
-0.001 |
| z |
0.000 |
-0.001 |
-21.632 |
|
| Traceless |
| | x | y | z |
| x |
-3.512 |
0.000 |
0.000 |
| y |
0.000 |
-0.340 |
-0.001 |
| z |
0.000 |
-0.001 |
3.852 |
|
| Polar |
| 3z2-r2 | 7.704 |
| x2-y2 | -2.115 |
| xy | 0.000 |
| xz | 0.000 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
44.116 |
| (<r2>)1/2 |
6.642 |