Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| hartrees |
Energy at 0K | -3113.121767 |
Energy at 298.15K | |
HF Energy | -3113.121767 |
Nuclear repulsion energy | 286.791366 |
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 B3LYP/cc-pVTZ
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' |
3113 |
3009 |
7.22 |
29.54 |
0.05 |
0.09 |
2 |
A' |
3100 |
2997 |
2.22 |
141.88 |
0.05 |
0.09 |
3 |
A' |
1495 |
1445 |
3.60 |
5.01 |
0.75 |
0.86 |
4 |
A' |
1490 |
1440 |
3.55 |
5.13 |
0.75 |
0.86 |
5 |
A' |
1309 |
1266 |
1.44 |
17.94 |
0.54 |
0.70 |
6 |
A' |
1226 |
1185 |
40.96 |
3.31 |
0.38 |
0.55 |
7 |
A' |
1060 |
1025 |
0.91 |
7.68 |
0.75 |
0.86 |
8 |
A' |
716 |
692 |
25.37 |
58.63 |
0.28 |
0.44 |
9 |
A' |
622 |
602 |
66.05 |
13.73 |
0.24 |
0.39 |
10 |
A' |
243 |
235 |
0.91 |
5.48 |
0.30 |
0.47 |
11 |
A' |
192 |
185 |
7.15 |
0.27 |
0.32 |
0.49 |
12 |
A" |
3182 |
3076 |
1.07 |
7.48 |
0.75 |
0.86 |
13 |
A" |
3155 |
3049 |
0.46 |
79.54 |
0.75 |
0.86 |
14 |
A" |
1292 |
1248 |
0.01 |
2.83 |
0.75 |
0.86 |
15 |
A" |
1121 |
1083 |
1.91 |
0.08 |
0.75 |
0.86 |
16 |
A" |
971 |
939 |
0.23 |
3.55 |
0.75 |
0.86 |
17 |
A" |
770 |
744 |
3.40 |
0.02 |
0.75 |
0.86 |
18 |
A" |
108 |
105 |
5.66 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12582.4 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 12162.1 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 B3LYP/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.645 |
0.000 |
C2 |
1.241 |
-0.212 |
0.000 |
Br3 |
-1.596 |
-0.519 |
0.000 |
Cl4 |
2.703 |
0.865 |
0.000 |
H5 |
-0.075 |
1.260 |
0.890 |
H6 |
-0.075 |
1.260 |
-0.890 |
H7 |
1.307 |
-0.832 |
0.888 |
H8 |
1.307 |
-0.832 |
-0.888 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5078 | 1.9751 | 2.7115 | 1.0840 | 1.0840 | 2.1631 | 2.1631 |
C2 | 1.5078 | | 2.8529 | 1.8158 | 2.1652 | 2.1652 | 1.0849 | 1.0849 | Br3 | 1.9751 | 2.8529 | | 4.5156 | 2.5039 | 2.5039 | 3.0519 | 3.0519 | Cl4 | 2.7115 | 1.8158 | 4.5156 | | 2.9429 | 2.9429 | 2.3695 | 2.3695 | H5 | 1.0840 | 2.1652 | 2.5039 | 2.9429 | | 1.7791 | 2.5073 | 3.0734 | H6 | 1.0840 | 2.1652 | 2.5039 | 2.9429 | 1.7791 | | 3.0734 | 2.5073 | H7 | 2.1631 | 1.0849 | 3.0519 | 2.3695 | 2.5073 | 3.0734 | | 1.7757 | H8 | 2.1631 | 1.0849 | 3.0519 | 2.3695 | 3.0734 | 2.5073 | 1.7757 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.986 |
|
C1 |
C2 |
H7 |
112.050 |
C1 |
C2 |
H8 |
112.050 |
|
C2 |
C1 |
Br3 |
109.257 |
C2 |
C1 |
Cl4 |
39.290 |
|
C2 |
C1 |
H6 |
112.280 |
Br3 |
C1 |
H5 |
106.181 |
|
Br3 |
C1 |
H6 |
106.181 |
Cl4 |
C2 |
H7 |
106.820 |
|
Cl4 |
C2 |
H8 |
106.820 |
H5 |
C1 |
H6 |
110.290 |
|
H7 |
C2 |
H8 |
109.839 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.156 |
|
|
|
2 |
C |
-0.109 |
|
|
|
3 |
Br |
-0.125 |
|
|
|
4 |
Cl |
-0.169 |
|
|
|
5 |
H |
0.139 |
|
|
|
6 |
H |
0.139 |
|
|
|
7 |
H |
0.141 |
|
|
|
8 |
H |
0.141 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.044 |
-0.020 |
0.000 |
0.048 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.424 |
-2.422 |
0.000 |
y |
-2.422 |
-43.715 |
0.000 |
z |
0.000 |
0.000 |
-43.723 |
|
Traceless |
| x | y | z |
x |
-6.705 |
-2.422 |
0.000 |
y |
-2.422 |
3.358 |
0.000 |
z |
0.000 |
0.000 |
3.347 |
|
Polar |
3z2-r2 | 6.694 |
x2-y2 | -6.709 |
xy | -2.422 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
11.631 |
2.131 |
0.000 |
y |
2.131 |
7.464 |
0.000 |
z |
0.000 |
0.000 |
5.986 |
<r2> (average value of r
2) Å
2
<r2> |
287.280 |
(<r2>)1/2 |
16.949 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| hartrees |
Energy at 0K | -3113.118578 |
Energy at 298.15K | |
HF Energy | -3113.118578 |
Nuclear repulsion energy | 302.092595 |
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 B3LYP/cc-pVTZ
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 |
3157 |
3051 |
1.62 |
36.76 |
0.75 |
0.86 |
2 |
A |
3133 |
3029 |
1.27 |
79.42 |
0.75 |
0.85 |
3 |
A |
3089 |
2986 |
12.06 |
172.98 |
0.04 |
0.07 |
4 |
A |
3069 |
2966 |
8.75 |
119.35 |
0.19 |
0.32 |
5 |
A |
1473 |
1423 |
4.75 |
6.44 |
0.75 |
0.86 |
6 |
A |
1466 |
1417 |
7.71 |
7.67 |
0.74 |
0.85 |
7 |
A |
1329 |
1284 |
19.93 |
1.99 |
0.71 |
0.83 |
8 |
A |
1290 |
1247 |
52.08 |
3.36 |
0.46 |
0.63 |
9 |
A |
1205 |
1165 |
2.28 |
8.55 |
0.73 |
0.85 |
10 |
A |
1142 |
1104 |
1.05 |
3.28 |
0.73 |
0.84 |
11 |
A |
1036 |
1002 |
2.06 |
1.61 |
0.72 |
0.84 |
12 |
A |
928 |
897 |
9.23 |
5.19 |
0.38 |
0.55 |
13 |
A |
869 |
840 |
19.94 |
1.39 |
0.75 |
0.86 |
14 |
A |
658 |
636 |
23.14 |
9.49 |
0.39 |
0.56 |
15 |
A |
561 |
542 |
12.38 |
16.83 |
0.16 |
0.28 |
16 |
A |
382 |
369 |
7.99 |
2.43 |
0.71 |
0.83 |
17 |
A |
240 |
232 |
1.36 |
1.58 |
0.41 |
0.58 |
18 |
A |
94 |
91 |
0.58 |
1.60 |
0.71 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 12559.3 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 12139.9 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 B3LYP/cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.020 |
1.097 |
-0.387 |
C2 |
1.287 |
0.900 |
0.406 |
Br3 |
-1.375 |
-0.225 |
0.036 |
Cl4 |
2.204 |
-0.574 |
-0.086 |
H5 |
-0.417 |
2.064 |
-0.148 |
H6 |
0.191 |
1.023 |
-1.455 |
H7 |
1.953 |
1.744 |
0.230 |
H8 |
1.091 |
0.811 |
1.470 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5074 | 1.9675 | 2.7670 | 1.0871 | 1.0847 | 2.1296 | 2.1622 |
C2 | 1.5074 | | 2.9132 | 1.8043 | 2.1365 | 2.1628 | 1.0890 | 1.0857 | Br3 | 1.9675 | 2.9132 | | 3.5980 | 2.4879 | 2.4964 | 3.8711 | 3.0348 | Cl4 | 2.7670 | 1.8043 | 3.5980 | | 3.7194 | 2.9119 | 2.3528 | 2.3616 | H5 | 1.0871 | 2.1365 | 2.4879 | 3.7194 | | 1.7780 | 2.4209 | 2.5417 | H6 | 1.0847 | 2.1628 | 2.4964 | 2.9119 | 1.7780 | | 2.5423 | 3.0674 | H7 | 2.1296 | 1.0890 | 3.8711 | 2.3528 | 2.4209 | 2.5423 | | 1.7743 | H8 | 2.1622 | 1.0857 | 3.0348 | 2.3616 | 2.5417 | 3.0674 | 1.7743 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
113.035 |
|
C1 |
C2 |
H7 |
109.147 |
C1 |
C2 |
H8 |
111.964 |
|
C2 |
C1 |
Br3 |
113.272 |
C2 |
C1 |
Cl4 |
36.877 |
|
C2 |
C1 |
H6 |
112.074 |
Br3 |
C1 |
H5 |
105.410 |
|
Br3 |
C1 |
H6 |
106.109 |
Cl4 |
C2 |
H7 |
106.169 |
|
Cl4 |
C2 |
H8 |
106.963 |
H5 |
C1 |
H6 |
109.902 |
|
H7 |
C2 |
H8 |
109.350 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.161 |
|
|
|
2 |
C |
-0.116 |
|
|
|
3 |
Br |
-0.110 |
|
|
|
4 |
Cl |
-0.153 |
|
|
|
5 |
H |
0.132 |
|
|
|
6 |
H |
0.135 |
|
|
|
7 |
H |
0.135 |
|
|
|
8 |
H |
0.137 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.379 |
2.683 |
0.105 |
2.711 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.993 |
2.697 |
0.448 |
y |
2.697 |
-40.815 |
-0.093 |
z |
0.448 |
-0.093 |
-43.372 |
|
Traceless |
| x | y | z |
x |
-5.899 |
2.697 |
0.448 |
y |
2.697 |
4.868 |
-0.093 |
z |
0.448 |
-0.093 |
1.032 |
|
Polar |
3z2-r2 | 2.064 |
x2-y2 | -7.178 |
xy | 2.697 |
xz | 0.448 |
yz | -0.093 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.569 |
0.294 |
-0.219 |
y |
0.294 |
8.169 |
0.039 |
z |
-0.219 |
0.039 |
6.302 |
<r2> (average value of r
2) Å
2
<r2> |
226.287 |
(<r2>)1/2 |
15.043 |