Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| hartrees |
Energy at 0K | -3109.792006 |
Energy at 298.15K | |
HF Energy | -3109.611236 |
Nuclear repulsion energy | 287.678090 |
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/6-31G*
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' |
3166 |
3004 |
7.80 |
29.84 |
0.08 |
0.15 |
2 |
A' |
3154 |
2993 |
2.97 |
112.36 |
0.09 |
0.16 |
3 |
A' |
1538 |
1459 |
1.72 |
13.65 |
0.75 |
0.86 |
4 |
A' |
1534 |
1455 |
4.87 |
4.28 |
0.74 |
0.85 |
5 |
A' |
1363 |
1293 |
3.61 |
13.87 |
0.55 |
0.71 |
6 |
A' |
1261 |
1197 |
47.99 |
2.84 |
0.44 |
0.61 |
7 |
A' |
1087 |
1031 |
1.28 |
8.30 |
0.75 |
0.85 |
8 |
A' |
756 |
718 |
30.24 |
47.89 |
0.30 |
0.46 |
9 |
A' |
648 |
614 |
57.02 |
11.94 |
0.25 |
0.41 |
10 |
A' |
251 |
238 |
0.89 |
5.23 |
0.33 |
0.50 |
11 |
A' |
197 |
187 |
7.66 |
0.20 |
0.29 |
0.45 |
12 |
A" |
3243 |
3076 |
1.91 |
11.08 |
0.75 |
0.86 |
13 |
A" |
3217 |
3052 |
0.77 |
84.16 |
0.75 |
0.86 |
14 |
A" |
1326 |
1258 |
0.08 |
9.74 |
0.75 |
0.86 |
15 |
A" |
1158 |
1099 |
2.31 |
0.40 |
0.75 |
0.86 |
16 |
A" |
998 |
947 |
0.14 |
8.50 |
0.75 |
0.86 |
17 |
A" |
782 |
742 |
3.49 |
0.04 |
0.75 |
0.86 |
18 |
A" |
115 |
109 |
6.03 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12897.0 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 12235.4 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 B2PLYP=FULLultrafine/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.656 |
0.000 |
C2 |
1.232 |
-0.221 |
0.000 |
Br3 |
-1.594 |
-0.497 |
0.000 |
Cl4 |
2.705 |
0.821 |
0.000 |
H5 |
-0.063 |
1.274 |
0.892 |
H6 |
-0.063 |
1.274 |
-0.892 |
H7 |
1.274 |
-0.848 |
0.889 |
H8 |
1.274 |
-0.848 |
-0.889 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5128 | 1.9677 | 2.7101 | 1.0873 | 1.0873 | 2.1622 | 2.1622 |
C2 | 1.5128 | | 2.8402 | 1.8041 | 2.1704 | 2.1704 | 1.0885 | 1.0885 | Br3 | 1.9677 | 2.8402 | | 4.4969 | 2.5056 | 2.5056 | 3.0231 | 3.0231 | Cl4 | 2.7101 | 1.8041 | 4.4969 | | 2.9436 | 2.9436 | 2.3717 | 2.3717 | H5 | 1.0873 | 2.1704 | 2.5056 | 2.9436 | | 1.7849 | 2.5082 | 3.0764 | H6 | 1.0873 | 2.1704 | 2.5056 | 2.9436 | 1.7849 | | 3.0764 | 2.5082 | H7 | 2.1622 | 1.0885 | 3.0231 | 2.3717 | 2.5082 | 3.0764 | | 1.7777 | H8 | 2.1622 | 1.0885 | 3.0231 | 2.3717 | 3.0764 | 2.5082 | 1.7777 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.268 |
|
C1 |
C2 |
H7 |
111.402 |
C1 |
C2 |
H8 |
111.402 |
|
C2 |
C1 |
Br3 |
108.676 |
C2 |
C1 |
Cl4 |
38.933 |
|
C2 |
C1 |
H6 |
112.143 |
Br3 |
C1 |
H5 |
106.618 |
|
Br3 |
C1 |
H6 |
106.618 |
Cl4 |
C2 |
H7 |
107.565 |
|
Cl4 |
C2 |
H8 |
107.565 |
H5 |
C1 |
H6 |
110.322 |
|
H7 |
C2 |
H8 |
109.487 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.296 |
|
|
|
2 |
C |
-0.372 |
|
|
|
3 |
Br |
-0.133 |
|
|
|
4 |
Cl |
-0.072 |
|
|
|
5 |
H |
0.217 |
|
|
|
6 |
H |
0.217 |
|
|
|
7 |
H |
0.220 |
|
|
|
8 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.150 |
-0.036 |
0.000 |
0.154 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.457 |
-2.335 |
-0.007 |
y |
-2.335 |
-43.230 |
-0.002 |
z |
-0.007 |
-0.002 |
-43.433 |
|
Traceless |
| x | y | z |
x |
-7.126 |
-2.335 |
-0.007 |
y |
-2.335 |
3.715 |
-0.002 |
z |
-0.007 |
-0.002 |
3.411 |
|
Polar |
3z2-r2 | 6.822 |
x2-y2 | -7.227 |
xy | -2.335 |
xz | -0.007 |
yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.825 |
1.979 |
-0.000 |
y |
1.979 |
6.251 |
-0.000 |
z |
-0.000 |
-0.000 |
5.073 |
<r2> (average value of r
2) Å
2
<r2> |
285.121 |
(<r2>)1/2 |
16.886 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| hartrees |
Energy at 0K | -3109.789151 |
Energy at 298.15K | |
HF Energy | -3109.608133 |
Nuclear repulsion energy | 304.373910 |
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/6-31G*
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 |
3220 |
3055 |
1.94 |
42.38 |
0.75 |
0.86 |
2 |
A |
3197 |
3033 |
1.87 |
80.60 |
0.75 |
0.86 |
3 |
A |
3145 |
2984 |
11.24 |
131.34 |
0.06 |
0.11 |
4 |
A |
3126 |
2965 |
9.90 |
102.80 |
0.22 |
0.36 |
5 |
A |
1521 |
1443 |
1.72 |
8.17 |
0.70 |
0.83 |
6 |
A |
1513 |
1435 |
8.70 |
16.09 |
0.75 |
0.86 |
7 |
A |
1378 |
1308 |
28.84 |
3.92 |
0.75 |
0.86 |
8 |
A |
1330 |
1262 |
51.22 |
1.64 |
0.54 |
0.70 |
9 |
A |
1242 |
1178 |
4.04 |
17.18 |
0.75 |
0.85 |
10 |
A |
1174 |
1114 |
1.64 |
6.10 |
0.73 |
0.84 |
11 |
A |
1063 |
1008 |
1.53 |
3.90 |
0.75 |
0.86 |
12 |
A |
959 |
910 |
8.59 |
6.37 |
0.45 |
0.62 |
13 |
A |
890 |
844 |
19.19 |
1.52 |
0.71 |
0.83 |
14 |
A |
691 |
656 |
20.21 |
10.33 |
0.41 |
0.58 |
15 |
A |
580 |
550 |
12.50 |
15.76 |
0.21 |
0.34 |
16 |
A |
393 |
373 |
8.16 |
2.65 |
0.71 |
0.83 |
17 |
A |
245 |
233 |
1.24 |
1.06 |
0.32 |
0.48 |
18 |
A |
103 |
97 |
0.57 |
1.29 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 12884.0 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 12223.1 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/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
1.119 |
-0.383 |
C2 |
1.287 |
0.906 |
0.403 |
Br3 |
-1.351 |
-0.227 |
0.036 |
Cl4 |
2.159 |
-0.584 |
-0.087 |
H5 |
-0.426 |
2.082 |
-0.123 |
H6 |
0.181 |
1.064 |
-1.456 |
H7 |
1.964 |
1.744 |
0.222 |
H8 |
1.084 |
0.830 |
1.470 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5125 | 1.9610 | 2.7559 | 1.0899 | 1.0878 | 2.1371 | 2.1598 |
C2 | 1.5125 | | 2.8946 | 1.7947 | 2.1434 | 2.1688 | 1.0921 | 1.0890 | Br3 | 1.9610 | 2.8946 | | 3.5304 | 2.4927 | 2.4981 | 3.8613 | 3.0171 | Cl4 | 2.7559 | 1.7947 | 3.5304 | | 3.7137 | 2.9157 | 2.3563 | 2.3623 | H5 | 1.0899 | 2.1434 | 2.4927 | 3.7137 | | 1.7841 | 2.4386 | 2.5268 | H6 | 1.0878 | 2.1688 | 2.4981 | 2.9157 | 1.7841 | | 2.5416 | 3.0711 | H7 | 2.1371 | 1.0921 | 3.8613 | 2.3563 | 2.4386 | 2.5416 | | 1.7793 | H8 | 2.1598 | 1.0890 | 3.0171 | 2.3623 | 2.5268 | 3.0711 | 1.7793 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.605 |
|
C1 |
C2 |
H7 |
109.209 |
C1 |
C2 |
H8 |
111.196 |
|
C2 |
C1 |
Br3 |
112.246 |
C2 |
C1 |
Cl4 |
36.954 |
|
C2 |
C1 |
H6 |
112.001 |
Br3 |
C1 |
H5 |
106.029 |
|
Br3 |
C1 |
H6 |
106.500 |
Cl4 |
C2 |
H7 |
106.892 |
|
Cl4 |
C2 |
H8 |
107.475 |
H5 |
C1 |
H6 |
110.017 |
|
H7 |
C2 |
H8 |
109.330 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.301 |
|
|
|
2 |
C |
-0.369 |
|
|
|
3 |
Br |
-0.119 |
|
|
|
4 |
Cl |
-0.060 |
|
|
|
5 |
H |
0.206 |
|
|
|
6 |
H |
0.217 |
|
|
|
7 |
H |
0.207 |
|
|
|
8 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.341 |
2.790 |
0.118 |
2.813 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.584 |
2.893 |
0.450 |
y |
2.893 |
-40.352 |
-0.114 |
z |
0.450 |
-0.114 |
-43.039 |
|
Traceless |
| x | y | z |
x |
-5.889 |
2.893 |
0.450 |
y |
2.893 |
4.960 |
-0.114 |
z |
0.450 |
-0.114 |
0.929 |
|
Polar |
3z2-r2 | 1.857 |
x2-y2 | -7.232 |
xy | 2.893 |
xz | 0.450 |
yz | -0.114 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.938 |
0.212 |
-0.319 |
y |
0.212 |
7.120 |
0.083 |
z |
-0.319 |
0.083 |
5.252 |
<r2> (average value of r
2) Å
2
<r2> |
221.198 |
(<r2>)1/2 |
14.873 |