Jump to
S1C2
Energy calculated at wB97X-D/3-21G*
| hartrees |
Energy at 0K | -3098.334612 |
Energy at 298.15K | |
HF Energy | -3098.334612 |
Nuclear repulsion energy | 288.000749 |
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 wB97X-D/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' |
3159 |
2994 |
4.94 |
2.46 |
0.11 |
0.19 |
2 |
A' |
3150 |
2986 |
0.12 |
133.61 |
0.08 |
0.16 |
3 |
A' |
1546 |
1465 |
10.09 |
11.08 |
0.75 |
0.86 |
4 |
A' |
1542 |
1461 |
8.09 |
12.42 |
0.75 |
0.86 |
5 |
A' |
1366 |
1294 |
1.23 |
12.17 |
0.53 |
0.69 |
6 |
A' |
1291 |
1224 |
25.47 |
1.50 |
0.42 |
0.60 |
7 |
A' |
1047 |
992 |
1.18 |
7.66 |
0.75 |
0.86 |
8 |
A' |
750 |
711 |
12.25 |
54.67 |
0.30 |
0.46 |
9 |
A' |
687 |
651 |
61.68 |
1.28 |
0.28 |
0.44 |
10 |
A' |
259 |
246 |
1.31 |
5.03 |
0.35 |
0.51 |
11 |
A' |
201 |
190 |
6.63 |
0.20 |
0.36 |
0.53 |
12 |
A" |
3235 |
3067 |
0.21 |
1.56 |
0.75 |
0.86 |
13 |
A" |
3212 |
3044 |
0.05 |
92.06 |
0.75 |
0.86 |
14 |
A" |
1346 |
1276 |
0.06 |
13.32 |
0.75 |
0.86 |
15 |
A" |
1184 |
1123 |
2.27 |
0.11 |
0.75 |
0.86 |
16 |
A" |
997 |
945 |
0.07 |
9.59 |
0.75 |
0.86 |
17 |
A" |
797 |
755 |
7.76 |
0.03 |
0.75 |
0.86 |
18 |
A" |
111 |
106 |
5.99 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12939.6 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 12264.2 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 wB97X-D/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.657 |
0.000 |
C2 |
1.218 |
-0.258 |
0.000 |
Br3 |
-1.601 |
-0.459 |
0.000 |
Cl4 |
2.724 |
0.757 |
0.000 |
H5 |
-0.032 |
1.276 |
0.895 |
H6 |
-0.032 |
1.276 |
-0.895 |
H7 |
1.245 |
-0.880 |
0.893 |
H8 |
1.245 |
-0.880 |
-0.893 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5236 | 1.9517 | 2.7255 | 1.0889 | 1.0889 | 2.1701 | 2.1701 |
C2 | 1.5236 | | 2.8266 | 1.8157 | 2.1721 | 2.1721 | 1.0890 | 1.0890 | Br3 | 1.9517 | 2.8266 | | 4.4926 | 2.5048 | 2.5048 | 3.0121 | 3.0121 | Cl4 | 2.7255 | 1.8157 | 4.4926 | | 2.9436 | 2.9436 | 2.3805 | 2.3805 | H5 | 1.0889 | 2.1721 | 2.5048 | 2.9436 | | 1.7904 | 2.5057 | 3.0786 | H6 | 1.0889 | 2.1721 | 2.5048 | 2.9436 | 1.7904 | | 3.0786 | 2.5057 | H7 | 2.1701 | 1.0890 | 3.0121 | 2.3805 | 2.5057 | 3.0786 | | 1.7867 | H8 | 2.1701 | 1.0890 | 3.0121 | 2.3805 | 3.0786 | 2.5057 | 1.7867 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
109.101 |
|
C1 |
C2 |
H7 |
111.244 |
C1 |
C2 |
H8 |
111.244 |
|
C2 |
C1 |
Br3 |
108.216 |
C2 |
C1 |
Cl4 |
39.014 |
|
C2 |
C1 |
H6 |
111.406 |
Br3 |
C1 |
H5 |
107.514 |
|
Br3 |
C1 |
H6 |
107.514 |
Cl4 |
C2 |
H7 |
107.425 |
|
Cl4 |
C2 |
H8 |
107.425 |
H5 |
C1 |
H6 |
110.595 |
|
H7 |
C2 |
H8 |
110.244 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.481 |
|
|
|
2 |
C |
-0.526 |
|
|
|
3 |
Br |
-0.060 |
|
|
|
4 |
Cl |
-0.056 |
|
|
|
5 |
H |
0.279 |
|
|
|
6 |
H |
0.279 |
|
|
|
7 |
H |
0.283 |
|
|
|
8 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.462 |
-0.182 |
0.000 |
0.496 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.415 |
-2.143 |
0.000 |
y |
-2.143 |
-42.719 |
0.000 |
z |
0.000 |
0.000 |
-43.123 |
|
Traceless |
| x | y | z |
x |
-7.494 |
-2.143 |
0.000 |
y |
-2.143 |
4.050 |
0.000 |
z |
0.000 |
0.000 |
3.444 |
|
Polar |
3z2-r2 | 6.888 |
x2-y2 | -7.696 |
xy | -2.143 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.335 |
1.934 |
0.000 |
y |
1.934 |
5.754 |
0.000 |
z |
0.000 |
0.000 |
4.641 |
<r2> (average value of r
2) Å
2
<r2> |
284.329 |
(<r2>)1/2 |
16.862 |
Jump to
S1C1
Energy calculated at wB97X-D/3-21G*
| hartrees |
Energy at 0K | -3098.331959 |
Energy at 298.15K | |
HF Energy | -3098.331959 |
Nuclear repulsion energy | 305.698054 |
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 wB97X-D/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 |
3212 |
3045 |
0.41 |
31.03 |
0.75 |
0.86 |
2 |
A |
3197 |
3030 |
0.20 |
92.64 |
0.75 |
0.85 |
3 |
A |
3140 |
2976 |
8.46 |
152.31 |
0.03 |
0.06 |
4 |
A |
3130 |
2966 |
3.18 |
62.03 |
0.42 |
0.59 |
5 |
A |
1534 |
1454 |
19.98 |
19.33 |
0.74 |
0.85 |
6 |
A |
1526 |
1446 |
4.76 |
9.85 |
0.73 |
0.85 |
7 |
A |
1380 |
1308 |
15.65 |
3.98 |
0.75 |
0.86 |
8 |
A |
1355 |
1284 |
26.25 |
2.38 |
0.68 |
0.81 |
9 |
A |
1256 |
1191 |
1.84 |
19.39 |
0.74 |
0.85 |
10 |
A |
1204 |
1141 |
1.64 |
7.53 |
0.74 |
0.85 |
11 |
A |
1038 |
984 |
1.98 |
3.24 |
0.74 |
0.85 |
12 |
A |
960 |
910 |
11.81 |
6.88 |
0.50 |
0.66 |
13 |
A |
895 |
848 |
24.06 |
1.62 |
0.71 |
0.83 |
14 |
A |
684 |
648 |
17.14 |
11.25 |
0.48 |
0.65 |
15 |
A |
619 |
587 |
8.02 |
15.35 |
0.18 |
0.30 |
16 |
A |
404 |
383 |
6.68 |
2.84 |
0.74 |
0.85 |
17 |
A |
248 |
235 |
1.28 |
0.97 |
0.35 |
0.52 |
18 |
A |
100 |
95 |
0.61 |
1.30 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12940.3 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 12264.8 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 wB97X-D/3-21G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.006 |
1.129 |
-0.387 |
C2 |
1.278 |
0.923 |
0.405 |
Br3 |
-1.334 |
-0.230 |
0.037 |
Cl4 |
2.135 |
-0.589 |
-0.088 |
H5 |
-0.446 |
2.092 |
-0.126 |
H6 |
0.180 |
1.077 |
-1.459 |
H7 |
1.964 |
1.751 |
0.216 |
H8 |
1.072 |
0.847 |
1.472 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5221 | 1.9468 | 2.7609 | 1.0914 | 1.0894 | 2.1514 | 2.1672 |
C2 | 1.5221 | | 2.8786 | 1.8068 | 2.1500 | 2.1693 | 1.0918 | 1.0895 | Br3 | 1.9468 | 2.8786 | | 3.4899 | 2.4918 | 2.4977 | 3.8511 | 3.0013 | Cl4 | 2.7609 | 1.8068 | 3.4899 | | 3.7224 | 2.9122 | 2.3657 | 2.3724 | H5 | 1.0914 | 2.1500 | 2.4918 | 3.7224 | | 1.7888 | 2.4579 | 2.5319 | H6 | 1.0894 | 2.1693 | 2.4977 | 2.9122 | 1.7888 | | 2.5379 | 3.0729 | H7 | 2.1514 | 1.0918 | 3.8511 | 2.3657 | 2.4579 | 2.5379 | | 1.7869 | H8 | 2.1672 | 1.0895 | 3.0013 | 2.3724 | 2.5319 | 3.0729 | 1.7869 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
111.785 |
|
C1 |
C2 |
H7 |
109.684 |
C1 |
C2 |
H8 |
111.077 |
|
C2 |
C1 |
Br3 |
111.577 |
C2 |
C1 |
Cl4 |
37.423 |
|
C2 |
C1 |
H6 |
111.253 |
Br3 |
C1 |
H5 |
106.791 |
|
Br3 |
C1 |
H6 |
107.301 |
Cl4 |
C2 |
H7 |
106.794 |
|
Cl4 |
C2 |
H8 |
107.386 |
H5 |
C1 |
H6 |
110.209 |
|
H7 |
C2 |
H8 |
110.002 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.485 |
|
|
|
2 |
C |
-0.527 |
|
|
|
3 |
Br |
-0.049 |
|
|
|
4 |
Cl |
-0.042 |
|
|
|
5 |
H |
0.270 |
|
|
|
6 |
H |
0.278 |
|
|
|
7 |
H |
0.273 |
|
|
|
8 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.110 |
2.812 |
0.163 |
2.819 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-47.169 |
3.114 |
0.436 |
y |
3.114 |
-39.935 |
-0.133 |
z |
0.436 |
-0.133 |
-42.698 |
|
Traceless |
| x | y | z |
x |
-5.853 |
3.114 |
0.436 |
y |
3.114 |
4.999 |
-0.133 |
z |
0.436 |
-0.133 |
0.854 |
|
Polar |
3z2-r2 | 1.708 |
x2-y2 | -7.234 |
xy | 3.114 |
xz | 0.436 |
yz | -0.133 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.341 |
0.211 |
-0.353 |
y |
0.211 |
6.766 |
0.075 |
z |
-0.353 |
0.075 |
4.819 |
<r2> (average value of r
2) Å
2
<r2> |
218.091 |
(<r2>)1/2 |
14.768 |