Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -3113.434667 |
Energy at 298.15K | |
HF Energy | -3113.434667 |
Nuclear repulsion energy | 290.271412 |
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/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' |
3136 |
3001 |
7.26 |
31.87 |
0.04 |
0.09 |
2 |
A' |
3122 |
2989 |
2.48 |
142.18 |
0.04 |
0.08 |
3 |
A' |
1491 |
1427 |
3.21 |
5.92 |
0.75 |
0.86 |
4 |
A' |
1486 |
1422 |
4.74 |
4.14 |
0.75 |
0.86 |
5 |
A' |
1310 |
1254 |
1.26 |
14.79 |
0.56 |
0.72 |
6 |
A' |
1222 |
1170 |
37.40 |
2.53 |
0.38 |
0.55 |
7 |
A' |
1086 |
1040 |
1.15 |
6.11 |
0.75 |
0.85 |
8 |
A' |
754 |
722 |
29.55 |
45.28 |
0.27 |
0.43 |
9 |
A' |
659 |
631 |
54.34 |
15.28 |
0.24 |
0.38 |
10 |
A' |
248 |
238 |
0.81 |
4.07 |
0.30 |
0.47 |
11 |
A' |
188 |
180 |
7.18 |
0.14 |
0.33 |
0.50 |
12 |
A" |
3208 |
3071 |
0.79 |
7.63 |
0.75 |
0.86 |
13 |
A" |
3181 |
3044 |
0.43 |
79.45 |
0.75 |
0.86 |
14 |
A" |
1291 |
1236 |
0.02 |
3.10 |
0.75 |
0.86 |
15 |
A" |
1124 |
1076 |
2.05 |
0.06 |
0.75 |
0.86 |
16 |
A" |
973 |
932 |
0.23 |
3.34 |
0.75 |
0.86 |
17 |
A" |
765 |
732 |
3.45 |
0.02 |
0.75 |
0.86 |
18 |
A" |
110 |
105 |
5.54 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12677.7 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 12133.8 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.641 |
0.000 |
C2 |
1.225 |
-0.226 |
0.000 |
Br3 |
-1.580 |
-0.493 |
0.000 |
Cl4 |
2.677 |
0.820 |
0.000 |
H5 |
-0.059 |
1.259 |
0.887 |
H6 |
-0.059 |
1.259 |
-0.887 |
H7 |
1.276 |
-0.849 |
0.885 |
H8 |
1.276 |
-0.849 |
-0.885 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5013 | 1.9445 | 2.6832 | 1.0828 | 1.0828 | 2.1523 | 2.1523 |
C2 | 1.5013 | | 2.8179 | 1.7894 | 2.1548 | 2.1548 | 1.0836 | 1.0836 | Br3 | 1.9445 | 2.8179 | | 4.4548 | 2.4834 | 2.4834 | 3.0111 | 3.0111 | Cl4 | 2.6832 | 1.7894 | 4.4548 | | 2.9099 | 2.9099 | 2.3521 | 2.3521 | H5 | 1.0828 | 2.1548 | 2.4834 | 2.9099 | | 1.7743 | 2.4952 | 3.0607 | H6 | 1.0828 | 2.1548 | 2.4834 | 2.9099 | 1.7743 | | 3.0607 | 2.4952 | H7 | 2.1523 | 1.0836 | 3.0111 | 2.3521 | 2.4952 | 3.0607 | | 1.7708 | H8 | 2.1523 | 1.0836 | 3.0111 | 2.3521 | 3.0607 | 2.4952 | 1.7708 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.935 |
|
C1 |
C2 |
H7 |
111.719 |
C1 |
C2 |
H8 |
111.719 |
|
C2 |
C1 |
Br3 |
109.051 |
C2 |
C1 |
Cl4 |
39.110 |
|
C2 |
C1 |
H6 |
111.981 |
Br3 |
C1 |
H5 |
106.756 |
|
Br3 |
C1 |
H6 |
106.756 |
Cl4 |
C2 |
H7 |
107.345 |
|
Cl4 |
C2 |
H8 |
107.345 |
H5 |
C1 |
H6 |
110.037 |
|
H7 |
C2 |
H8 |
109.581 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.203 |
|
|
|
2 |
C |
-0.164 |
|
|
|
3 |
Br |
-0.122 |
|
|
|
4 |
Cl |
-0.156 |
|
|
|
5 |
H |
0.160 |
|
|
|
6 |
H |
0.160 |
|
|
|
7 |
H |
0.162 |
|
|
|
8 |
H |
0.162 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.050 |
-0.017 |
0.000 |
0.053 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.775 |
-2.215 |
0.000 |
y |
-2.215 |
-43.176 |
0.000 |
z |
0.000 |
0.000 |
-43.283 |
|
Traceless |
| x | y | z |
x |
-6.546 |
-2.215 |
0.000 |
y |
-2.215 |
3.353 |
0.000 |
z |
0.000 |
0.000 |
3.193 |
|
Polar |
3z2-r2 | 6.386 |
x2-y2 | -6.599 |
xy | -2.215 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
11.277 |
1.958 |
0.000 |
y |
1.958 |
7.317 |
0.000 |
z |
0.000 |
0.000 |
5.936 |
<r2> (average value of r
2) Å
2
<r2> |
280.292 |
(<r2>)1/2 |
16.742 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -3113.431903 |
Energy at 298.15K | |
HF Energy | -3113.431903 |
Nuclear repulsion energy | 306.861168 |
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/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 |
3185 |
3048 |
1.39 |
38.82 |
0.75 |
0.86 |
2 |
A |
3162 |
3026 |
1.26 |
80.60 |
0.75 |
0.86 |
3 |
A |
3115 |
2981 |
11.72 |
169.95 |
0.03 |
0.07 |
4 |
A |
3096 |
2963 |
9.13 |
115.22 |
0.17 |
0.30 |
5 |
A |
1470 |
1407 |
4.46 |
5.89 |
0.75 |
0.86 |
6 |
A |
1462 |
1399 |
9.06 |
8.06 |
0.74 |
0.85 |
7 |
A |
1330 |
1273 |
17.79 |
1.80 |
0.73 |
0.84 |
8 |
A |
1290 |
1235 |
45.01 |
2.51 |
0.45 |
0.62 |
9 |
A |
1212 |
1160 |
2.03 |
8.24 |
0.72 |
0.84 |
10 |
A |
1146 |
1096 |
1.09 |
3.18 |
0.72 |
0.84 |
11 |
A |
1053 |
1008 |
2.14 |
1.78 |
0.72 |
0.83 |
12 |
A |
938 |
897 |
8.79 |
4.43 |
0.36 |
0.53 |
13 |
A |
872 |
835 |
20.46 |
1.54 |
0.75 |
0.86 |
14 |
A |
692 |
662 |
18.48 |
8.26 |
0.35 |
0.52 |
15 |
A |
592 |
567 |
10.82 |
15.50 |
0.16 |
0.28 |
16 |
A |
383 |
367 |
6.95 |
1.99 |
0.71 |
0.83 |
17 |
A |
238 |
228 |
1.17 |
1.24 |
0.47 |
0.64 |
18 |
A |
97 |
93 |
0.51 |
1.36 |
0.71 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 12665.9 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 12122.6 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 B1B95/cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.010 |
1.101 |
-0.380 |
C2 |
1.276 |
0.899 |
0.399 |
Br3 |
-1.342 |
-0.224 |
0.036 |
Cl4 |
2.145 |
-0.577 |
-0.086 |
H5 |
-0.427 |
2.064 |
-0.132 |
H6 |
0.182 |
1.041 |
-1.448 |
H7 |
1.949 |
1.732 |
0.215 |
H8 |
1.083 |
0.823 |
1.463 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5007 | 1.9385 | 2.7319 | 1.0854 | 1.0834 | 2.1243 | 2.1511 |
C2 | 1.5007 | | 2.8717 | 1.7801 | 2.1307 | 2.1518 | 1.0872 | 1.0843 | Br3 | 1.9385 | 2.8717 | | 3.5068 | 2.4698 | 2.4750 | 3.8329 | 3.0022 | Cl4 | 2.7319 | 1.7801 | 3.5068 | | 3.6866 | 2.8858 | 2.3373 | 2.3432 | H5 | 1.0854 | 2.1307 | 2.4698 | 3.6866 | | 1.7743 | 2.4240 | 2.5226 | H6 | 1.0834 | 2.1518 | 2.4750 | 2.8858 | 1.7743 | | 2.5231 | 3.0556 | H7 | 2.1243 | 1.0872 | 3.8329 | 2.3373 | 2.4240 | 2.5231 | | 1.7711 | H8 | 2.1511 | 1.0843 | 3.0022 | 2.3432 | 2.5226 | 3.0556 | 1.7711 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
112.472 |
|
C1 |
C2 |
H7 |
109.305 |
C1 |
C2 |
H8 |
111.634 |
|
C2 |
C1 |
Br3 |
112.612 |
C2 |
C1 |
Cl4 |
37.023 |
|
C2 |
C1 |
H6 |
111.745 |
Br3 |
C1 |
H5 |
106.056 |
|
Br3 |
C1 |
H6 |
106.517 |
Cl4 |
C2 |
H7 |
106.700 |
|
Cl4 |
C2 |
H8 |
107.271 |
H5 |
C1 |
H6 |
109.785 |
|
H7 |
C2 |
H8 |
109.294 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.208 |
|
|
|
2 |
C |
-0.172 |
|
|
|
3 |
Br |
-0.104 |
|
|
|
4 |
Cl |
-0.137 |
|
|
|
5 |
H |
0.150 |
|
|
|
6 |
H |
0.158 |
|
|
|
7 |
H |
0.152 |
|
|
|
8 |
H |
0.160 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.383 |
2.651 |
0.102 |
2.680 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.279 |
2.646 |
0.431 |
y |
2.646 |
-40.346 |
-0.097 |
z |
0.431 |
-0.097 |
-42.953 |
|
Traceless |
| x | y | z |
x |
-5.629 |
2.646 |
0.431 |
y |
2.646 |
4.770 |
-0.097 |
z |
0.431 |
-0.097 |
0.859 |
|
Polar |
3z2-r2 | 1.719 |
x2-y2 | -6.933 |
xy | 2.646 |
xz | 0.431 |
yz | -0.097 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.299 |
0.289 |
-0.199 |
y |
0.289 |
8.077 |
0.038 |
z |
-0.199 |
0.038 |
6.234 |
<r2> (average value of r
2) Å
2
<r2> |
218.247 |
(<r2>)1/2 |
14.773 |