Jump to
S1C2
Energy calculated at B1B95/3-21G
| hartrees |
Energy at 0K | -3098.662641 |
Energy at 298.15K | |
HF Energy | -3098.662641 |
Nuclear repulsion energy | 289.168229 |
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 B1B95/3-21G
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' |
3156 |
3020 |
5.69 |
5.59 |
0.08 |
0.15 |
2 |
A' |
3146 |
3010 |
0.32 |
133.75 |
0.08 |
0.14 |
3 |
A' |
1539 |
1473 |
10.84 |
7.80 |
0.75 |
0.86 |
4 |
A' |
1534 |
1468 |
4.86 |
14.93 |
0.75 |
0.86 |
5 |
A' |
1346 |
1288 |
1.82 |
12.44 |
0.55 |
0.71 |
6 |
A' |
1271 |
1216 |
27.48 |
1.81 |
0.44 |
0.61 |
7 |
A' |
1053 |
1008 |
1.29 |
8.04 |
0.75 |
0.86 |
8 |
A' |
730 |
698 |
15.36 |
61.79 |
0.30 |
0.46 |
9 |
A' |
676 |
647 |
68.76 |
1.31 |
0.29 |
0.45 |
10 |
A' |
256 |
244 |
1.26 |
4.90 |
0.35 |
0.52 |
11 |
A' |
193 |
184 |
7.15 |
0.13 |
0.39 |
0.56 |
12 |
A" |
3234 |
3094 |
0.51 |
2.78 |
0.75 |
0.86 |
13 |
A" |
3208 |
3069 |
0.08 |
90.44 |
0.75 |
0.86 |
14 |
A" |
1337 |
1280 |
0.08 |
12.29 |
0.75 |
0.86 |
15 |
A" |
1169 |
1119 |
2.65 |
0.12 |
0.75 |
0.86 |
16 |
A" |
988 |
945 |
0.06 |
9.86 |
0.75 |
0.86 |
17 |
A" |
791 |
757 |
7.42 |
0.03 |
0.75 |
0.86 |
18 |
A" |
113 |
108 |
5.65 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12869.7 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 12312.5 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.664 |
0.000 |
C2 |
1.206 |
-0.255 |
0.000 |
Br3 |
-1.592 |
-0.458 |
0.000 |
Cl4 |
2.711 |
0.752 |
0.000 |
H5 |
-0.032 |
1.281 |
0.895 |
H6 |
-0.032 |
1.281 |
-0.895 |
H7 |
1.227 |
-0.877 |
0.892 |
H8 |
1.227 |
-0.877 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5169 | 1.9480 | 2.7128 | 1.0873 | 1.0873 | 2.1624 | 2.1624 |
C2 | 1.5169 | | 2.8059 | 1.8107 | 2.1668 | 2.1668 | 1.0875 | 1.0875 | Br3 | 1.9480 | 2.8059 | | 4.4703 | 2.5022 | 2.5022 | 2.9859 | 2.9859 | Cl4 | 2.7128 | 1.8107 | 4.4703 | | 2.9337 | 2.9337 | 2.3777 | 2.3777 | H5 | 1.0873 | 2.1668 | 2.5022 | 2.9337 | | 1.7890 | 2.4988 | 3.0716 | H6 | 1.0873 | 2.1668 | 2.5022 | 2.9337 | 1.7890 | | 3.0716 | 2.4988 | H7 | 2.1624 | 1.0875 | 2.9859 | 2.3777 | 2.4988 | 3.0716 | | 1.7837 | H8 | 2.1624 | 1.0875 | 2.9859 | 2.3777 | 3.0716 | 2.4988 | 1.7837 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
108.909 |
|
C1 |
C2 |
H7 |
111.187 |
C1 |
C2 |
H8 |
111.187 |
|
C2 |
C1 |
Br3 |
107.505 |
C2 |
C1 |
Cl4 |
39.155 |
|
C2 |
C1 |
H6 |
111.555 |
Br3 |
C1 |
H5 |
107.651 |
|
Br3 |
C1 |
H6 |
107.651 |
Cl4 |
C2 |
H7 |
107.619 |
|
Cl4 |
C2 |
H8 |
107.619 |
H5 |
C1 |
H6 |
110.711 |
|
H7 |
C2 |
H8 |
110.178 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.485 |
|
|
|
2 |
C |
-0.533 |
|
|
|
3 |
Br |
-0.053 |
|
|
|
4 |
Cl |
-0.050 |
|
|
|
5 |
H |
0.278 |
|
|
|
6 |
H |
0.278 |
|
|
|
7 |
H |
0.282 |
|
|
|
8 |
H |
0.282 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.479 |
-0.167 |
0.000 |
0.507 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-50.020 |
-2.020 |
0.000 |
y |
-2.020 |
-42.575 |
0.000 |
z |
0.000 |
0.000 |
-43.023 |
|
Traceless |
| x | y | z |
x |
-7.221 |
-2.020 |
0.000 |
y |
-2.020 |
3.947 |
0.000 |
z |
0.000 |
0.000 |
3.274 |
|
Polar |
3z2-r2 | 6.548 |
x2-y2 | -7.445 |
xy | -2.020 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
9.517 |
1.934 |
0.000 |
y |
1.934 |
5.766 |
0.000 |
z |
0.000 |
0.000 |
4.638 |
<r2> (average value of r
2) Å
2
<r2> |
281.680 |
(<r2>)1/2 |
16.783 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| hartrees |
Energy at 0K | -3098.659998 |
Energy at 298.15K | |
HF Energy | -3098.659998 |
Nuclear repulsion energy | 308.183763 |
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 B1B95/3-21G
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 |
3208 |
3069 |
0.92 |
33.45 |
0.75 |
0.86 |
2 |
A |
3190 |
3051 |
0.40 |
90.97 |
0.75 |
0.86 |
3 |
A |
3133 |
2997 |
9.00 |
149.15 |
0.04 |
0.07 |
4 |
A |
3121 |
2986 |
4.74 |
81.20 |
0.31 |
0.48 |
5 |
A |
1524 |
1458 |
16.92 |
18.63 |
0.74 |
0.85 |
6 |
A |
1516 |
1451 |
4.56 |
10.18 |
0.73 |
0.84 |
7 |
A |
1368 |
1309 |
16.27 |
4.66 |
0.75 |
0.86 |
8 |
A |
1340 |
1282 |
27.39 |
2.43 |
0.70 |
0.82 |
9 |
A |
1239 |
1186 |
2.63 |
20.04 |
0.75 |
0.85 |
10 |
A |
1192 |
1140 |
1.74 |
7.71 |
0.74 |
0.85 |
11 |
A |
1036 |
991 |
2.17 |
3.35 |
0.75 |
0.86 |
12 |
A |
955 |
914 |
11.38 |
6.73 |
0.51 |
0.68 |
13 |
A |
884 |
846 |
23.72 |
1.39 |
0.72 |
0.84 |
14 |
A |
674 |
645 |
19.26 |
10.75 |
0.45 |
0.62 |
15 |
A |
614 |
587 |
8.67 |
14.74 |
0.18 |
0.30 |
16 |
A |
397 |
380 |
7.07 |
2.80 |
0.74 |
0.85 |
17 |
A |
242 |
232 |
1.18 |
0.85 |
0.40 |
0.57 |
18 |
A |
104 |
100 |
0.49 |
1.19 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12869.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 12312.0 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.005 |
1.142 |
-0.384 |
C2 |
1.273 |
0.927 |
0.403 |
Br3 |
-1.314 |
-0.231 |
0.037 |
Cl4 |
2.094 |
-0.596 |
-0.089 |
H5 |
-0.451 |
2.099 |
-0.115 |
H6 |
0.177 |
1.097 |
-1.456 |
H7 |
1.971 |
1.742 |
0.210 |
H8 |
1.067 |
0.858 |
1.469 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5163 | 1.9418 | 2.7417 | 1.0901 | 1.0880 | 2.1496 | 2.1594 |
C2 | 1.5163 | | 2.8570 | 1.7989 | 2.1482 | 2.1639 | 1.0909 | 1.0882 | Br3 | 1.9418 | 2.8570 | | 3.4298 | 2.4890 | 2.4924 | 3.8355 | 2.9832 | Cl4 | 2.7417 | 1.7989 | 3.4298 | | 3.7077 | 2.9001 | 2.3609 | 2.3658 | H5 | 1.0901 | 2.1482 | 2.4890 | 3.7077 | | 1.7880 | 2.4699 | 2.5206 | H6 | 1.0880 | 2.1639 | 2.4924 | 2.9001 | 1.7880 | | 2.5315 | 3.0660 | H7 | 2.1496 | 1.0909 | 3.8355 | 2.3609 | 2.4699 | 2.5315 | | 1.7850 | H8 | 2.1594 | 1.0882 | 2.9832 | 2.3658 | 2.5206 | 3.0660 | 1.7850 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Cl4 |
111.298 |
|
C1 |
C2 |
H7 |
110.004 |
C1 |
C2 |
H8 |
110.948 |
|
C2 |
C1 |
Br3 |
110.814 |
C2 |
C1 |
Cl4 |
37.686 |
|
C2 |
C1 |
H6 |
111.320 |
Br3 |
C1 |
H5 |
106.974 |
|
Br3 |
C1 |
H6 |
107.321 |
Cl4 |
C2 |
H7 |
107.002 |
|
Cl4 |
C2 |
H8 |
107.487 |
H5 |
C1 |
H6 |
110.352 |
|
H7 |
C2 |
H8 |
109.996 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.489 |
|
|
|
2 |
C |
-0.533 |
|
|
|
3 |
Br |
-0.043 |
|
|
|
4 |
Cl |
-0.035 |
|
|
|
5 |
H |
0.269 |
|
|
|
6 |
H |
0.278 |
|
|
|
7 |
H |
0.272 |
|
|
|
8 |
H |
0.282 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.126 |
2.753 |
0.159 |
2.761 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-46.772 |
3.040 |
0.417 |
y |
3.040 |
-39.798 |
-0.131 |
z |
0.417 |
-0.131 |
-42.616 |
|
Traceless |
| x | y | z |
x |
-5.565 |
3.040 |
0.417 |
y |
3.040 |
4.895 |
-0.131 |
z |
0.417 |
-0.131 |
0.669 |
|
Polar |
3z2-r2 | 1.339 |
x2-y2 | -6.973 |
xy | 3.040 |
xz | 0.417 |
yz | -0.131 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.360 |
0.217 |
-0.319 |
y |
0.217 |
6.814 |
0.076 |
z |
-0.319 |
0.076 |
4.827 |
<r2> (average value of r
2) Å
2
<r2> |
213.462 |
(<r2>)1/2 |
14.610 |