Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -154.877922 |
| Energy at 298.15K | -154.883545 |
| Nuclear repulsion energy | 103.704736 |
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 HF/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3438 |
3093 |
0.00 |
|
|
|
| 2 |
Ag |
3357 |
3021 |
0.00 |
|
|
|
| 3 |
Ag |
3333 |
2999 |
0.00 |
|
|
|
| 4 |
Ag |
1865 |
1679 |
0.00 |
|
|
|
| 5 |
Ag |
1619 |
1457 |
0.00 |
|
|
|
| 6 |
Ag |
1435 |
1291 |
0.00 |
|
|
|
| 7 |
Ag |
1338 |
1204 |
0.00 |
|
|
|
| 8 |
Ag |
964 |
868 |
0.00 |
|
|
|
| 9 |
Ag |
558 |
502 |
0.00 |
|
|
|
| 10 |
Au |
1161 |
1044 |
16.92 |
|
|
|
| 11 |
Au |
1116 |
1004 |
195.90 |
|
|
|
| 12 |
Au |
592 |
532 |
19.42 |
|
|
|
| 13 |
Au |
171 |
154 |
0.34 |
|
|
|
| 14 |
Bg |
1141 |
1027 |
0.00 |
|
|
|
| 15 |
Bg |
1093 |
984 |
0.00 |
|
|
|
| 16 |
Bg |
856 |
771 |
0.00 |
|
|
|
| 17 |
Bu |
3439 |
3095 |
69.13 |
|
|
|
| 18 |
Bu |
3363 |
3026 |
26.80 |
|
|
|
| 19 |
Bu |
3335 |
3001 |
29.50 |
|
|
|
| 20 |
Bu |
1781 |
1603 |
35.24 |
|
|
|
| 21 |
Bu |
1550 |
1395 |
4.72 |
|
|
|
| 22 |
Bu |
1449 |
1304 |
2.21 |
|
|
|
| 23 |
Bu |
1106 |
995 |
7.01 |
|
|
|
| 24 |
Bu |
323 |
291 |
2.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20191.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 18169.9 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 HF/LANL2DZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.736 |
0.000 |
| C2 |
0.000 |
-0.736 |
0.000 |
| C3 |
1.107 |
1.486 |
0.000 |
| C4 |
-1.107 |
-1.486 |
0.000 |
| H5 |
-0.965 |
1.213 |
0.000 |
| H6 |
0.965 |
-1.213 |
0.000 |
| H7 |
1.059 |
2.559 |
0.000 |
| H8 |
2.089 |
1.049 |
0.000 |
| H9 |
-1.059 |
-2.559 |
0.000 |
| H10 |
-2.089 |
-1.049 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4721 | 1.3374 | 2.4830 | 1.0764 | 2.1751 | 2.1080 | 2.1128 | 3.4607 | 2.7483 |
C2 | 1.4721 | | 2.4830 | 1.3374 | 2.1751 | 1.0764 | 3.4607 | 2.7483 | 2.1080 | 2.1128 | C3 | 1.3374 | 2.4830 | | 3.7069 | 2.0898 | 2.7036 | 1.0734 | 1.0753 | 4.5886 | 4.0802 | C4 | 2.4830 | 1.3374 | 3.7069 | | 2.7036 | 2.0898 | 4.5886 | 4.0802 | 1.0734 | 1.0753 | H5 | 1.0764 | 2.1751 | 2.0898 | 2.7036 | | 3.1003 | 2.4301 | 3.0587 | 3.7733 | 2.5267 | H6 | 2.1751 | 1.0764 | 2.7036 | 2.0898 | 3.1003 | | 3.7733 | 2.5267 | 2.4301 | 3.0587 | H7 | 2.1080 | 3.4607 | 1.0734 | 4.5886 | 2.4301 | 3.7733 | | 1.8278 | 5.5384 | 4.7885 | H8 | 2.1128 | 2.7483 | 1.0753 | 4.0802 | 3.0587 | 2.5267 | 1.8278 | | 4.7885 | 4.6763 | H9 | 3.4607 | 2.1080 | 4.5886 | 1.0734 | 3.7733 | 2.4301 | 5.5384 | 4.7885 | | 1.8278 | H10 | 2.7483 | 2.1128 | 4.0802 | 1.0753 | 2.5267 | 3.0587 | 4.7885 | 4.6763 | 1.8278 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
124.133 |
|
C1 |
C2 |
H6 |
116.322 |
| C1 |
C3 |
H7 |
121.557 |
|
C1 |
C3 |
H8 |
121.876 |
| C2 |
C1 |
C3 |
124.133 |
|
C2 |
C1 |
H5 |
116.322 |
| C2 |
C4 |
H9 |
121.557 |
|
C2 |
C4 |
H10 |
121.876 |
| C3 |
C1 |
H5 |
119.546 |
|
C4 |
C2 |
H6 |
119.546 |
| H7 |
C3 |
H8 |
116.567 |
|
H9 |
C4 |
H10 |
116.567 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.057 |
|
|
|
| 2 |
C |
-0.057 |
|
|
|
| 3 |
C |
-0.501 |
|
|
|
| 4 |
C |
-0.501 |
|
|
|
| 5 |
H |
0.185 |
|
|
|
| 6 |
H |
0.185 |
|
|
|
| 7 |
H |
0.192 |
|
|
|
| 8 |
H |
0.181 |
|
|
|
| 9 |
H |
0.192 |
|
|
|
| 10 |
H |
0.181 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.804 |
-0.148 |
0.000 |
| y |
-0.148 |
-23.380 |
0.000 |
| z |
0.000 |
0.000 |
-30.025 |
|
| Traceless |
| | x | y | z |
| x |
3.898 |
-0.148 |
0.000 |
| y |
-0.148 |
3.035 |
0.000 |
| z |
0.000 |
0.000 |
-6.933 |
|
| Polar |
| 3z2-r2 | -13.866 |
| x2-y2 | 0.575 |
| xy | -0.148 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.822 |
3.677 |
0.000 |
| y |
3.677 |
8.445 |
0.000 |
| z |
0.000 |
0.000 |
2.552 |
<r2> (average value of r
2) Å
2
| <r2> |
94.666 |
| (<r2>)1/2 |
9.730 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -154.872734 |
| Energy at 298.15K | -154.878317 |
| HF Energy | -154.872734 |
| Nuclear repulsion energy | 104.722519 |
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 HF/LANL2DZ
| 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 |
3442 |
3098 |
18.24 |
|
|
|
| 2 |
A |
3367 |
3030 |
20.27 |
|
|
|
| 3 |
A |
3338 |
3003 |
26.66 |
|
|
|
| 4 |
A |
1829 |
1646 |
1.55 |
|
|
|
| 5 |
A |
1607 |
1447 |
16.86 |
|
|
|
| 6 |
A |
1465 |
1319 |
0.01 |
|
|
|
| 7 |
A |
1176 |
1058 |
0.30 |
|
|
|
| 8 |
A |
1140 |
1026 |
0.27 |
|
|
|
| 9 |
A |
1103 |
993 |
14.53 |
|
|
|
| 10 |
A |
946 |
851 |
0.35 |
|
|
|
| 11 |
A |
833 |
750 |
4.97 |
|
|
|
| 12 |
A |
299 |
269 |
0.01 |
|
|
|
| 13 |
A |
157 |
141 |
0.13 |
|
|
|
| 14 |
B |
3439 |
3094 |
44.13 |
|
|
|
| 15 |
B |
3349 |
3014 |
27.11 |
|
|
|
| 16 |
B |
3334 |
3000 |
3.50 |
|
|
|
| 17 |
B |
1822 |
1639 |
7.92 |
|
|
|
| 18 |
B |
1579 |
1421 |
3.32 |
|
|
|
| 19 |
B |
1431 |
1288 |
0.01 |
|
|
|
| 20 |
B |
1214 |
1092 |
13.31 |
|
|
|
| 21 |
B |
1147 |
1032 |
5.15 |
|
|
|
| 22 |
B |
1113 |
1002 |
177.01 |
|
|
|
| 23 |
B |
676 |
608 |
13.94 |
|
|
|
| 24 |
B |
524 |
471 |
22.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20164.4 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 18145.9 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 HF/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.100 |
0.734 |
0.549 |
| C2 |
-0.100 |
-0.734 |
0.549 |
| C3 |
-0.100 |
1.551 |
-0.490 |
| C4 |
0.100 |
-1.551 |
-0.490 |
| H5 |
0.421 |
1.156 |
1.486 |
| H6 |
-0.421 |
-1.156 |
1.486 |
| H7 |
0.081 |
2.607 |
-0.409 |
| H8 |
-0.464 |
1.195 |
-1.435 |
| H9 |
-0.081 |
-2.607 |
-0.409 |
| H10 |
0.464 |
-1.195 |
-1.435 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4810 | 1.3373 | 2.5102 | 1.0764 | 2.1727 | 2.1042 | 2.1143 | 3.4800 | 2.7911 |
C2 | 1.4810 | | 2.5102 | 1.3373 | 2.1727 | 1.0764 | 3.4800 | 2.7911 | 2.1042 | 2.1143 | C3 | 1.3373 | 2.5102 | | 3.1094 | 2.0812 | 3.3670 | 1.0737 | 1.0743 | 4.1590 | 2.9589 | C4 | 2.5102 | 1.3373 | 3.1094 | | 3.3670 | 2.0812 | 4.1590 | 2.9589 | 1.0737 | 1.0743 | H5 | 1.0764 | 2.1727 | 2.0812 | 3.3670 | | 2.4609 | 2.4109 | 3.0529 | 4.2430 | 3.7500 | H6 | 2.1727 | 1.0764 | 3.3670 | 2.0812 | 2.4609 | | 4.2430 | 3.7500 | 2.4109 | 3.0529 | H7 | 2.1042 | 3.4800 | 1.0737 | 4.1590 | 2.4109 | 4.2430 | | 1.8286 | 5.2160 | 3.9561 | H8 | 2.1143 | 2.7911 | 1.0743 | 2.9589 | 3.0529 | 3.7500 | 1.8286 | | 3.9561 | 2.5635 | H9 | 3.4800 | 2.1042 | 4.1590 | 1.0737 | 4.2430 | 2.4109 | 5.2160 | 3.9561 | | 1.8286 | H10 | 2.7911 | 2.1143 | 2.9589 | 1.0743 | 3.7500 | 3.0529 | 3.9561 | 2.5635 | 1.8286 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
125.840 |
|
C1 |
C2 |
H6 |
115.416 |
| C1 |
C3 |
H7 |
121.168 |
|
C1 |
C3 |
H8 |
122.123 |
| C2 |
C1 |
C3 |
125.840 |
|
C2 |
C1 |
H5 |
115.416 |
| C2 |
C4 |
H9 |
121.168 |
|
C2 |
C4 |
H10 |
122.123 |
| C3 |
C1 |
H5 |
118.737 |
|
C4 |
C2 |
H6 |
118.737 |
| H7 |
C3 |
H8 |
116.702 |
|
H9 |
C4 |
H10 |
116.702 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.090 |
|
|
|
| 2 |
C |
-0.090 |
|
|
|
| 3 |
C |
-0.473 |
|
|
|
| 4 |
C |
-0.473 |
|
|
|
| 5 |
H |
0.183 |
|
|
|
| 6 |
H |
0.183 |
|
|
|
| 7 |
H |
0.190 |
|
|
|
| 8 |
H |
0.189 |
|
|
|
| 9 |
H |
0.190 |
|
|
|
| 10 |
H |
0.189 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.109 |
0.109 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.237 |
0.836 |
0.000 |
| y |
0.836 |
-23.520 |
0.000 |
| z |
0.000 |
0.000 |
-23.121 |
|
| Traceless |
| | x | y | z |
| x |
-5.917 |
0.836 |
0.000 |
| y |
0.836 |
2.659 |
0.000 |
| z |
0.000 |
0.000 |
3.257 |
|
| Polar |
| 3z2-r2 | 6.514 |
| x2-y2 | -5.717 |
| xy | 0.836 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.002 |
-0.185 |
0.000 |
| y |
-0.185 |
8.556 |
0.000 |
| z |
0.000 |
0.000 |
6.686 |
<r2> (average value of r
2) Å
2
| <r2> |
86.670 |
| (<r2>)1/2 |
9.310 |