Jump to
S1C2
Energy calculated at HSEh1PBE/3-21G
| hartrees |
Energy at 0K | -3097.424050 |
Energy at 298.15K | |
HF Energy | -3097.424050 |
Nuclear repulsion energy | 284.121633 |
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 HSEh1PBE/3-21G
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' |
3169 |
3053 |
3.48 |
2.49 |
0.15 |
0.27 |
2 |
A' |
3160 |
3044 |
0.09 |
148.00 |
0.08 |
0.14 |
3 |
A' |
1532 |
1475 |
4.52 |
15.27 |
0.74 |
0.85 |
4 |
A' |
1528 |
1472 |
15.67 |
6.44 |
0.75 |
0.86 |
5 |
A' |
1329 |
1280 |
0.12 |
35.00 |
0.51 |
0.68 |
6 |
A' |
1268 |
1221 |
31.76 |
0.20 |
0.33 |
0.50 |
7 |
A' |
1084 |
1044 |
1.29 |
22.32 |
0.66 |
0.80 |
8 |
A' |
694 |
669 |
8.15 |
88.40 |
0.31 |
0.48 |
9 |
A' |
647 |
624 |
85.35 |
0.30 |
0.68 |
0.81 |
10 |
A' |
244 |
235 |
1.09 |
7.04 |
0.40 |
0.57 |
11 |
A' |
193 |
185 |
9.52 |
0.07 |
0.58 |
0.73 |
12 |
A" |
3254 |
3135 |
0.25 |
1.76 |
0.75 |
0.86 |
13 |
A" |
3228 |
3109 |
0.00 |
94.70 |
0.75 |
0.86 |
14 |
A" |
1337 |
1288 |
0.02 |
11.19 |
0.75 |
0.86 |
15 |
A" |
1154 |
1112 |
1.47 |
0.04 |
0.75 |
0.86 |
16 |
A" |
965 |
929 |
0.11 |
15.89 |
0.75 |
0.86 |
17 |
A" |
788 |
759 |
8.71 |
0.08 |
0.75 |
0.86 |
18 |
A" |
113 |
108 |
6.93 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12842.2 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 12370.9 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 HSEh1PBE/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.644 |
0.000 |
C2 |
1.218 |
-0.239 |
0.000 |
Br3 |
-1.605 |
-0.530 |
0.000 |
Cl4 |
2.728 |
0.900 |
0.000 |
H5 |
-0.056 |
1.259 |
0.896 |
H6 |
-0.056 |
1.259 |
-0.896 |
H7 |
1.303 |
-0.844 |
0.900 |
H8 |
1.303 |
-0.844 |
-0.900 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5039 | 1.9885 | 2.7397 | 1.0886 | 1.0886 | 2.1730 | 2.1730 |
C2 | 1.5039 | | 2.8378 | 1.8908 | 2.1609 | 2.1609 | 1.0882 | 1.0882 | Br3 | 1.9885 | 2.8378 | | 4.5625 | 2.5306 | 2.5306 | 3.0606 | 3.0606 | Cl4 | 2.7397 | 1.8908 | 4.5625 | | 2.9466 | 2.9466 | 2.4246 | 2.4246 | H5 | 1.0886 | 2.1609 | 2.5306 | 2.9466 | | 1.7926 | 2.5039 | 3.0819 | H6 | 1.0886 | 2.1609 | 2.5306 | 2.9466 | 1.7926 | | 3.0819 | 2.5039 | H7 | 2.1730 | 1.0882 | 3.0606 | 2.4246 | 2.5039 | 3.0819 | | 1.8009 | H8 | 2.1730 | 1.0882 | 3.0606 | 2.4246 | 3.0819 | 2.5039 | 1.8009 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
107.063 |
|
C1 |
C2 |
H7 |
112.945 |
C1 |
C2 |
H8 |
112.945 |
|
C2 |
C1 |
Br3 |
107.890 |
C2 |
C1 |
Cl4 |
41.284 |
|
C2 |
C1 |
H6 |
111.926 |
Br3 |
C1 |
H5 |
106.981 |
|
Br3 |
C1 |
H6 |
106.981 |
Cl4 |
C2 |
H7 |
105.779 |
|
Cl4 |
C2 |
H8 |
105.779 |
H5 |
C1 |
H6 |
110.839 |
|
H7 |
C2 |
H8 |
111.682 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.660 |
|
|
|
2 |
C |
-0.576 |
|
|
|
3 |
Br |
0.074 |
|
|
|
4 |
Cl |
-0.034 |
|
|
|
5 |
H |
0.301 |
|
|
|
6 |
H |
0.301 |
|
|
|
7 |
H |
0.298 |
|
|
|
8 |
H |
0.298 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.705 |
-0.404 |
0.000 |
0.813 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-52.284 |
-3.461 |
0.000 |
y |
-3.461 |
-43.652 |
0.000 |
z |
0.000 |
0.000 |
-43.365 |
|
Traceless |
| x | y | z |
x |
-8.775 |
-3.461 |
0.000 |
y |
-3.461 |
4.172 |
0.000 |
z |
0.000 |
0.000 |
4.603 |
|
Polar |
3z2-r2 | 9.206 |
x2-y2 | -8.631 |
xy | -3.461 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.495 |
2.784 |
0.000 |
y |
2.784 |
5.325 |
0.000 |
z |
0.000 |
0.000 |
3.544 |
<r2> (average value of r
2) Å
2
<r2> |
292.196 |
(<r2>)1/2 |
17.094 |
Jump to
S1C1
Energy calculated at HSEh1PBE/3-21G
| hartrees |
Energy at 0K | -3097.420321 |
Energy at 298.15K | |
HF Energy | -3097.420321 |
Nuclear repulsion energy | 301.433838 |
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 HSEh1PBE/3-21G
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 |
3224 |
3106 |
0.44 |
33.36 |
0.75 |
0.85 |
2 |
A |
3206 |
3088 |
0.05 |
95.06 |
0.75 |
0.86 |
3 |
A |
3141 |
3025 |
6.82 |
183.60 |
0.03 |
0.06 |
4 |
A |
3131 |
3016 |
2.14 |
70.73 |
0.45 |
0.62 |
5 |
A |
1514 |
1458 |
16.32 |
17.34 |
0.74 |
0.85 |
6 |
A |
1506 |
1451 |
9.67 |
12.87 |
0.73 |
0.84 |
7 |
A |
1358 |
1308 |
16.62 |
5.90 |
0.67 |
0.80 |
8 |
A |
1330 |
1281 |
37.74 |
1.49 |
0.74 |
0.85 |
9 |
A |
1234 |
1188 |
1.12 |
28.11 |
0.75 |
0.86 |
10 |
A |
1179 |
1136 |
1.42 |
10.70 |
0.75 |
0.86 |
11 |
A |
1062 |
1023 |
3.88 |
4.25 |
0.65 |
0.79 |
12 |
A |
934 |
900 |
10.72 |
12.98 |
0.53 |
0.69 |
13 |
A |
868 |
836 |
29.08 |
2.77 |
0.64 |
0.78 |
14 |
A |
634 |
611 |
25.24 |
16.44 |
0.54 |
0.70 |
15 |
A |
589 |
567 |
10.00 |
16.34 |
0.18 |
0.31 |
16 |
A |
388 |
373 |
8.50 |
4.15 |
0.75 |
0.86 |
17 |
A |
249 |
239 |
1.55 |
1.77 |
0.45 |
0.62 |
18 |
A |
97 |
94 |
0.77 |
2.43 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12820.9 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 12350.4 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 HSEh1PBE/3-21G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.010 |
1.130 |
-0.401 |
C2 |
1.262 |
0.964 |
0.415 |
Br3 |
-1.354 |
-0.234 |
0.037 |
Cl4 |
2.176 |
-0.598 |
-0.085 |
H5 |
-0.449 |
2.097 |
-0.179 |
H6 |
0.212 |
1.046 |
-1.468 |
H7 |
1.965 |
1.777 |
0.222 |
H8 |
1.061 |
0.862 |
1.480 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5034 | 1.9780 | 2.7887 | 1.0927 | 1.0895 | 2.1510 | 2.1710 |
C2 | 1.5034 | | 2.9021 | 1.8774 | 2.1364 | 2.1572 | 1.0917 | 1.0888 | Br3 | 1.9780 | 2.9021 | | 3.5509 | 2.5092 | 2.5214 | 3.8849 | 3.0194 | Cl4 | 2.7887 | 1.8774 | 3.5509 | | 3.7631 | 2.9109 | 2.4039 | 2.4133 | H5 | 1.0927 | 2.1364 | 2.5092 | 3.7631 | | 1.7889 | 2.4679 | 2.5609 | H6 | 1.0895 | 2.1572 | 2.5214 | 2.9109 | 1.7889 | | 2.5416 | 3.0733 | H7 | 2.1510 | 1.0917 | 3.8849 | 2.4039 | 2.4679 | 2.5416 | | 1.7991 | H8 | 2.1710 | 1.0888 | 3.0194 | 2.4133 | 2.5609 | 3.0733 | 1.7991 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
110.663 |
|
C1 |
C2 |
H7 |
110.972 |
C1 |
C2 |
H8 |
112.787 |
|
C2 |
C1 |
Br3 |
112.225 |
C2 |
C1 |
Cl4 |
39.045 |
|
C2 |
C1 |
H6 |
111.612 |
Br3 |
C1 |
H5 |
105.977 |
|
Br3 |
C1 |
H6 |
106.976 |
Cl4 |
C2 |
H7 |
105.013 |
|
Cl4 |
C2 |
H8 |
105.811 |
H5 |
C1 |
H6 |
110.127 |
|
H7 |
C2 |
H8 |
111.193 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.670 |
|
|
|
2 |
C |
-0.584 |
|
|
|
3 |
Br |
0.089 |
|
|
|
4 |
Cl |
-0.017 |
|
|
|
5 |
H |
0.291 |
|
|
|
6 |
H |
0.301 |
|
|
|
7 |
H |
0.291 |
|
|
|
8 |
H |
0.298 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.102 |
3.149 |
0.204 |
3.157 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.284 |
3.441 |
0.616 |
y |
3.441 |
-40.607 |
-0.105 |
z |
0.616 |
-0.105 |
-42.945 |
|
Traceless |
| x | y | z |
x |
-6.508 |
3.441 |
0.616 |
y |
3.441 |
5.007 |
-0.105 |
z |
0.616 |
-0.105 |
1.501 |
|
Polar |
3z2-r2 | 3.002 |
x2-y2 | -7.677 |
xy | 3.441 |
xz | 0.616 |
yz | -0.105 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.907 |
0.311 |
-0.508 |
y |
0.311 |
6.393 |
0.051 |
z |
-0.508 |
0.051 |
3.837 |
<r2> (average value of r
2) Å
2
<r2> |
224.121 |
(<r2>)1/2 |
14.971 |