Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31+G**
| hartrees |
Energy at 0K | -3109.827133 |
Energy at 298.15K | |
HF Energy | -3109.636407 |
Nuclear repulsion energy | 287.888602 |
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 B2PLYP=FULLultrafine/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' |
3159 |
3159 |
7.81 |
24.09 |
0.06 |
0.12 |
2 |
A' |
3148 |
3148 |
2.27 |
126.93 |
0.07 |
0.13 |
3 |
A' |
1519 |
1519 |
0.05 |
11.65 |
0.68 |
0.81 |
4 |
A' |
1516 |
1516 |
6.85 |
0.08 |
0.75 |
0.86 |
5 |
A' |
1359 |
1359 |
2.03 |
19.93 |
0.39 |
0.56 |
6 |
A' |
1264 |
1264 |
55.01 |
3.13 |
0.26 |
0.41 |
7 |
A' |
1086 |
1086 |
0.99 |
7.56 |
0.75 |
0.86 |
8 |
A' |
754 |
754 |
25.83 |
59.23 |
0.27 |
0.42 |
9 |
A' |
654 |
654 |
62.17 |
13.76 |
0.22 |
0.36 |
10 |
A' |
252 |
252 |
0.62 |
5.69 |
0.28 |
0.44 |
11 |
A' |
192 |
192 |
7.77 |
0.16 |
0.20 |
0.33 |
12 |
A" |
3237 |
3237 |
0.59 |
6.16 |
0.75 |
0.86 |
13 |
A" |
3213 |
3213 |
0.44 |
85.60 |
0.75 |
0.86 |
14 |
A" |
1316 |
1316 |
0.08 |
8.14 |
0.75 |
0.86 |
15 |
A" |
1153 |
1153 |
2.72 |
0.26 |
0.75 |
0.86 |
16 |
A" |
1006 |
1006 |
0.25 |
4.45 |
0.75 |
0.86 |
17 |
A" |
786 |
786 |
2.77 |
0.02 |
0.75 |
0.86 |
18 |
A" |
139 |
139 |
5.96 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12875.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12875.6 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 B2PLYP=FULLultrafine/6-31+G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.635 |
0.000 |
C2 |
1.245 |
-0.222 |
0.000 |
Br3 |
-1.591 |
-0.512 |
0.000 |
Cl4 |
2.690 |
0.859 |
0.000 |
H5 |
-0.065 |
1.254 |
0.890 |
H6 |
-0.065 |
1.254 |
-0.890 |
H7 |
1.303 |
-0.845 |
0.889 |
H8 |
1.303 |
-0.845 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5111 | 1.9607 | 2.6993 | 1.0863 | 1.0863 | 2.1627 | 2.1627 |
C2 | 1.5111 | | 2.8505 | 1.8046 | 2.1649 | 2.1649 | 1.0871 | 1.0871 | Br3 | 1.9607 | 2.8505 | | 4.4948 | 2.4970 | 2.4970 | 3.0452 | 3.0452 | Cl4 | 2.6993 | 1.8046 | 4.4948 | | 2.9225 | 2.9225 | 2.3704 | 2.3704 | H5 | 1.0863 | 2.1649 | 2.4970 | 2.9225 | | 1.7808 | 2.5054 | 3.0728 | H6 | 1.0863 | 2.1649 | 2.4970 | 2.9225 | 1.7808 | | 3.0728 | 2.5054 | H7 | 2.1627 | 1.0871 | 3.0452 | 2.3704 | 2.5054 | 3.0728 | | 1.7775 | H8 | 2.1627 | 1.0871 | 3.0452 | 2.3704 | 3.0728 | 2.5054 | 1.7775 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.675 |
|
C1 |
C2 |
H7 |
111.644 |
C1 |
C2 |
H8 |
111.644 |
|
C2 |
C1 |
Br3 |
109.694 |
C2 |
C1 |
Cl4 |
39.296 |
|
C2 |
C1 |
H6 |
111.873 |
Br3 |
C1 |
H5 |
106.509 |
|
Br3 |
C1 |
H6 |
106.509 |
Cl4 |
C2 |
H7 |
107.509 |
|
Cl4 |
C2 |
H8 |
107.509 |
H5 |
C1 |
H6 |
110.100 |
|
H7 |
C2 |
H8 |
109.679 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.301 |
|
|
|
2 |
C |
-0.315 |
|
|
|
3 |
Br |
-0.135 |
|
|
|
4 |
Cl |
-0.044 |
|
|
|
5 |
H |
0.194 |
|
|
|
6 |
H |
0.194 |
|
|
|
7 |
H |
0.203 |
|
|
|
8 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.051 |
-0.045 |
0.000 |
0.068 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-51.268 |
-2.509 |
-0.008 |
y |
-2.509 |
-44.225 |
-0.002 |
z |
-0.008 |
-0.002 |
-44.286 |
|
Traceless |
| x | y | z |
x |
-7.012 |
-2.509 |
-0.008 |
y |
-2.509 |
3.552 |
-0.002 |
z |
-0.008 |
-0.002 |
3.460 |
|
Polar |
3z2-r2 | 6.920 |
x2-y2 | -7.043 |
xy | -2.509 |
xz | -0.008 |
yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
11.005 |
1.916 |
-0.001 |
y |
1.916 |
7.452 |
-0.001 |
z |
-0.001 |
-0.001 |
6.272 |
<r2> (average value of r
2) Å
2
<r2> |
285.538 |
(<r2>)1/2 |
16.898 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31+G**
| hartrees |
Energy at 0K | -3109.823385 |
Energy at 298.15K | |
HF Energy | -3109.632489 |
Nuclear repulsion energy | 302.138178 |
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 B2PLYP=FULLultrafine/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 |
3213 |
3213 |
0.72 |
36.48 |
0.75 |
0.86 |
2 |
A |
3195 |
3195 |
1.01 |
80.78 |
0.75 |
0.86 |
3 |
A |
3137 |
3137 |
12.47 |
154.69 |
0.04 |
0.08 |
4 |
A |
3120 |
3120 |
9.18 |
100.06 |
0.21 |
0.34 |
5 |
A |
1501 |
1501 |
0.76 |
4.80 |
0.74 |
0.85 |
6 |
A |
1496 |
1496 |
12.72 |
13.02 |
0.73 |
0.84 |
7 |
A |
1368 |
1368 |
29.30 |
3.26 |
0.72 |
0.84 |
8 |
A |
1327 |
1327 |
61.06 |
2.97 |
0.24 |
0.38 |
9 |
A |
1240 |
1240 |
2.43 |
11.27 |
0.70 |
0.82 |
10 |
A |
1168 |
1168 |
2.12 |
3.14 |
0.72 |
0.84 |
11 |
A |
1070 |
1070 |
1.02 |
2.54 |
0.74 |
0.85 |
12 |
A |
950 |
950 |
9.01 |
6.98 |
0.22 |
0.36 |
13 |
A |
899 |
899 |
20.12 |
1.46 |
0.74 |
0.85 |
14 |
A |
685 |
685 |
23.69 |
10.57 |
0.39 |
0.56 |
15 |
A |
577 |
577 |
13.25 |
18.05 |
0.16 |
0.28 |
16 |
A |
396 |
396 |
7.13 |
2.16 |
0.70 |
0.83 |
17 |
A |
251 |
251 |
1.32 |
1.87 |
0.19 |
0.33 |
18 |
A |
92 |
92 |
0.72 |
1.11 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12842.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12842.1 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 B2PLYP=FULLultrafine/6-31+G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.022 |
1.073 |
-0.400 |
C2 |
1.277 |
0.882 |
0.419 |
Br3 |
-1.382 |
-0.222 |
0.036 |
Cl4 |
2.223 |
-0.560 |
-0.087 |
H5 |
-0.407 |
2.050 |
-0.183 |
H6 |
0.214 |
0.980 |
-1.465 |
H7 |
1.927 |
1.745 |
0.273 |
H8 |
1.053 |
0.775 |
1.478 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5109 | 1.9583 | 2.7587 | 1.0889 | 1.0869 | 2.1292 | 2.1627 |
C2 | 1.5109 | | 2.9041 | 1.7970 | 2.1361 | 2.1658 | 1.0905 | 1.0875 | Br3 | 1.9583 | 2.9041 | | 3.6229 | 2.4820 | 2.4992 | 3.8563 | 3.0000 | Cl4 | 2.7587 | 1.7970 | 3.6229 | | 3.7065 | 2.8827 | 2.3518 | 2.3662 | H5 | 1.0889 | 2.1361 | 2.4820 | 3.7065 | | 1.7817 | 2.3970 | 2.5526 | H6 | 1.0869 | 2.1658 | 2.4992 | 2.8827 | 1.7817 | | 2.5571 | 3.0674 | H7 | 2.1292 | 1.0905 | 3.8563 | 2.3518 | 2.3970 | 2.5571 | | 1.7771 | H8 | 2.1627 | 1.0875 | 3.0000 | 2.3662 | 2.5526 | 3.0674 | 1.7771 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.730 |
|
C1 |
C2 |
H7 |
108.791 |
C1 |
C2 |
H8 |
111.639 |
|
C2 |
C1 |
Br3 |
113.037 |
C2 |
C1 |
Cl4 |
36.929 |
|
C2 |
C1 |
H6 |
111.927 |
Br3 |
C1 |
H5 |
105.495 |
|
Br3 |
C1 |
H6 |
106.790 |
Cl4 |
C2 |
H7 |
106.486 |
|
Cl4 |
C2 |
H8 |
107.674 |
H5 |
C1 |
H6 |
109.939 |
|
H7 |
C2 |
H8 |
109.356 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.270 |
|
|
|
2 |
C |
-0.318 |
|
|
|
3 |
Br |
-0.147 |
|
|
|
4 |
Cl |
-0.033 |
|
|
|
5 |
H |
0.181 |
|
|
|
6 |
H |
0.194 |
|
|
|
7 |
H |
0.190 |
|
|
|
8 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.361 |
2.782 |
0.114 |
2.808 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.947 |
2.890 |
0.462 |
y |
2.890 |
-41.320 |
-0.129 |
z |
0.462 |
-0.129 |
-43.845 |
|
Traceless |
| x | y | z |
x |
-6.364 |
2.890 |
0.462 |
y |
2.890 |
5.075 |
-0.129 |
z |
0.462 |
-0.129 |
1.289 |
|
Polar |
3z2-r2 | 2.578 |
x2-y2 | -7.626 |
xy | 2.890 |
xz | 0.462 |
yz | -0.129 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.344 |
0.182 |
-0.292 |
y |
0.182 |
7.989 |
0.072 |
z |
-0.292 |
0.072 |
6.528 |
<r2> (average value of r
2) Å
2
<r2> |
227.644 |
(<r2>)1/2 |
15.088 |