Jump to
S1C2
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -356.544857 |
| Energy at 298.15K | -356.550122 |
| HF Energy | -356.544857 |
| Nuclear repulsion energy | 235.094608 |
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/6-31G*
| 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' |
4050 |
3639 |
135.94 |
|
|
|
| 2 |
A' |
3976 |
3572 |
103.32 |
|
|
|
| 3 |
A' |
3843 |
3453 |
89.00 |
|
|
|
| 4 |
A' |
2047 |
1839 |
7.90 |
|
|
|
| 5 |
A' |
2008 |
1804 |
852.23 |
|
|
|
| 6 |
A' |
1786 |
1605 |
133.95 |
|
|
|
| 7 |
A' |
1589 |
1428 |
20.08 |
|
|
|
| 8 |
A' |
1445 |
1298 |
101.54 |
|
|
|
| 9 |
A' |
1332 |
1197 |
373.57 |
|
|
|
| 10 |
A' |
1212 |
1089 |
6.03 |
|
|
|
| 11 |
A' |
861 |
774 |
11.27 |
|
|
|
| 12 |
A' |
671 |
603 |
99.92 |
|
|
|
| 13 |
A' |
580 |
521 |
0.10 |
|
|
|
| 14 |
A' |
453 |
407 |
3.21 |
|
|
|
| 15 |
A' |
297 |
267 |
16.31 |
|
|
|
| 16 |
A" |
918 |
825 |
4.24 |
|
|
|
| 17 |
A" |
714 |
642 |
208.90 |
|
|
|
| 18 |
A" |
654 |
588 |
29.43 |
|
|
|
| 19 |
A" |
479 |
430 |
13.95 |
|
|
|
| 20 |
A" |
333 |
299 |
306.60 |
|
|
|
| 21 |
A" |
53 |
48 |
1.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14650.0 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13163.0 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 HF/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.753 |
0.000 |
| C2 |
-0.055 |
-0.783 |
0.000 |
| O3 |
-1.087 |
-1.376 |
0.000 |
| O4 |
1.024 |
1.356 |
0.000 |
| O5 |
-1.189 |
1.303 |
0.000 |
| N6 |
1.171 |
-1.324 |
0.000 |
| H7 |
1.259 |
-2.315 |
0.000 |
| H8 |
1.983 |
-0.752 |
0.000 |
| H9 |
-1.086 |
2.251 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
O4 |
O5 |
N6 |
H7 |
H8 |
H9 |
| C1 | | 1.5372 | 2.3909 | 1.1881 | 1.3104 | 2.3848 | 3.3164 | 2.4894 | 1.8497 |
C2 | 1.5372 | | 1.1907 | 2.3953 | 2.3747 | 1.3399 | 2.0182 | 2.0382 | 3.2039 | O3 | 2.3909 | 1.1907 | | 3.4525 | 2.6813 | 2.2587 | 2.5270 | 3.1332 | 3.6265 | O4 | 1.1881 | 2.3953 | 3.4525 | | 2.2140 | 2.6840 | 3.6782 | 2.3153 | 2.2920 | O5 | 1.3104 | 2.3747 | 2.6813 | 2.2140 | | 3.5320 | 4.3687 | 3.7798 | 0.9528 | N6 | 2.3848 | 1.3399 | 2.2587 | 2.6840 | 3.5320 | | 0.9945 | 0.9938 | 4.2277 | H7 | 3.3164 | 2.0182 | 2.5270 | 3.6782 | 4.3687 | 0.9945 | | 1.7229 | 5.1325 | H8 | 2.4894 | 2.0382 | 3.1332 | 2.3153 | 3.7798 | 0.9938 | 1.7229 | | 4.2934 | H9 | 1.8497 | 3.2039 | 3.6265 | 2.2920 | 0.9528 | 4.2277 | 5.1325 | 4.2934 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O3 |
121.923 |
|
C1 |
C2 |
N6 |
111.788 |
| C1 |
O5 |
H9 |
108.601 |
|
C2 |
C1 |
O4 |
122.513 |
| C2 |
C1 |
O5 |
112.773 |
|
C2 |
N6 |
H7 |
118.912 |
| C2 |
N6 |
H8 |
120.981 |
|
O3 |
C2 |
N6 |
126.289 |
| O4 |
C1 |
O5 |
124.714 |
|
H7 |
N6 |
H8 |
120.107 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.694 |
|
|
|
| 2 |
C |
0.682 |
|
|
|
| 3 |
O |
-0.557 |
|
|
|
| 4 |
O |
-0.556 |
|
|
|
| 5 |
O |
-0.658 |
|
|
|
| 6 |
N |
-0.914 |
|
|
|
| 7 |
H |
0.407 |
|
|
|
| 8 |
H |
0.427 |
|
|
|
| 9 |
H |
0.475 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.222 |
0.752 |
0.000 |
2.346 |
| CHELPG |
0.217 |
2.334 |
0.002 |
2.345 |
| AIM |
|
|
|
|
| ESP |
2.230 |
0.737 |
0.000 |
2.348 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.781 |
-10.419 |
0.000 |
| y |
-10.419 |
-28.325 |
0.004 |
| z |
0.000 |
0.004 |
-33.092 |
|
| Traceless |
| | x | y | z |
| x |
-5.072 |
-10.419 |
0.000 |
| y |
-10.419 |
6.111 |
0.004 |
| z |
0.000 |
0.004 |
-1.039 |
|
| Polar |
| 3z2-r2 | -2.078 |
| x2-y2 | -7.456 |
| xy | -10.419 |
| xz | 0.000 |
| yz | 0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.892 |
0.091 |
0.001 |
| y |
0.091 |
5.058 |
0.000 |
| z |
0.001 |
0.000 |
2.388 |
<r2> (average value of r
2) Å
2
| <r2> |
139.497 |
| (<r2>)1/2 |
11.811 |
Jump to
S1C1
Energy calculated at HF/6-31G*
| | hartrees |
| Energy at 0K | -356.549331 |
| Energy at 298.15K | -356.554852 |
| HF Energy | -356.549331 |
| Nuclear repulsion energy | 236.343580 |
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/6-31G*
| 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' |
3981 |
3577 |
192.68 |
|
|
|
| 2 |
A' |
3965 |
3562 |
99.02 |
|
|
|
| 3 |
A' |
3833 |
3444 |
97.97 |
|
|
|
| 4 |
A' |
2081 |
1870 |
247.67 |
|
|
|
| 5 |
A' |
1982 |
1781 |
564.58 |
|
|
|
| 6 |
A' |
1789 |
1607 |
93.54 |
|
|
|
| 7 |
A' |
1608 |
1445 |
172.37 |
|
|
|
| 8 |
A' |
1468 |
1319 |
551.69 |
|
|
|
| 9 |
A' |
1335 |
1200 |
12.18 |
|
|
|
| 10 |
A' |
1216 |
1093 |
0.76 |
|
|
|
| 11 |
A' |
890 |
800 |
9.93 |
|
|
|
| 12 |
A' |
688 |
618 |
25.93 |
|
|
|
| 13 |
A' |
595 |
535 |
3.47 |
|
|
|
| 14 |
A' |
449 |
404 |
6.67 |
|
|
|
| 15 |
A' |
304 |
273 |
40.13 |
|
|
|
| 16 |
A" |
903 |
812 |
0.03 |
|
|
|
| 17 |
A" |
726 |
653 |
165.12 |
|
|
|
| 18 |
A" |
693 |
623 |
12.21 |
|
|
|
| 19 |
A" |
518 |
465 |
171.97 |
|
|
|
| 20 |
A" |
404 |
363 |
200.83 |
|
|
|
| 21 |
A" |
107 |
96 |
6.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14767.8 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 13268.9 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/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.004 |
-0.791 |
0.000 |
| C2 |
0.000 |
0.746 |
0.000 |
| O3 |
-1.052 |
1.326 |
0.000 |
| O4 |
1.004 |
-1.422 |
0.000 |
| O5 |
-1.203 |
-1.298 |
0.000 |
| N6 |
1.213 |
1.289 |
0.000 |
| H7 |
1.309 |
2.280 |
0.000 |
| H8 |
2.021 |
0.709 |
0.000 |
| H9 |
-1.841 |
-0.586 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
O4 |
O5 |
N6 |
H7 |
H8 |
H9 |
| C1 | | 1.5371 | 2.3654 | 1.1828 | 1.3085 | 2.4064 | 3.3367 | 2.5137 | 1.8558 |
C2 | 1.5371 | | 1.2008 | 2.3895 | 2.3715 | 1.3291 | 2.0164 | 2.0213 | 2.2718 | O3 | 2.3654 | 1.2008 | | 3.4319 | 2.6281 | 2.2648 | 2.5459 | 3.1339 | 2.0679 | O4 | 1.1828 | 2.3895 | 3.4319 | | 2.2101 | 2.7198 | 3.7147 | 2.3613 | 2.9651 | O5 | 1.3085 | 2.3715 | 2.6281 | 2.2101 | | 3.5396 | 4.3712 | 3.7971 | 0.9563 | N6 | 2.4064 | 1.3291 | 2.2648 | 2.7198 | 3.5396 | | 0.9950 | 0.9951 | 3.5833 | H7 | 3.3367 | 2.0164 | 2.5459 | 3.7147 | 4.3712 | 0.9950 | | 1.7249 | 4.2580 | H8 | 2.5137 | 2.0213 | 3.1339 | 2.3613 | 3.7971 | 0.9951 | 1.7249 | | 4.0728 | H9 | 1.8558 | 2.2718 | 2.0679 | 2.9651 | 0.9563 | 3.5833 | 4.2580 | 4.0728 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O3 |
119.014 |
|
C1 |
C2 |
N6 |
113.993 |
| C1 |
O5 |
H9 |
109.063 |
|
C2 |
C1 |
O4 |
122.396 |
| C2 |
C1 |
O5 |
112.649 |
|
C2 |
N6 |
H7 |
119.668 |
| C2 |
N6 |
H8 |
120.166 |
|
O3 |
C2 |
N6 |
126.993 |
| O4 |
C1 |
O5 |
124.955 |
|
H7 |
N6 |
H8 |
120.166 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.729 |
|
|
|
| 2 |
C |
0.661 |
|
|
|
| 3 |
O |
-0.612 |
|
|
|
| 4 |
O |
-0.536 |
|
|
|
| 5 |
O |
-0.691 |
|
|
|
| 6 |
N |
-0.904 |
|
|
|
| 7 |
H |
0.412 |
|
|
|
| 8 |
H |
0.434 |
|
|
|
| 9 |
H |
0.505 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.355 |
2.565 |
0.000 |
2.901 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.388 |
7.536 |
0.000 |
| y |
7.536 |
-38.165 |
0.000 |
| z |
0.000 |
0.000 |
-33.057 |
|
| Traceless |
| | x | y | z |
| x |
5.223 |
7.536 |
0.000 |
| y |
7.536 |
-6.443 |
0.000 |
| z |
0.000 |
0.000 |
1.220 |
|
| Polar |
| 3z2-r2 | 2.439 |
| x2-y2 | 7.777 |
| xy | 7.536 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.148 |
-0.225 |
0.000 |
| y |
-0.225 |
4.704 |
0.000 |
| z |
0.000 |
0.000 |
2.380 |
<r2> (average value of r
2) Å
2
| <r2> |
137.617 |
| (<r2>)1/2 |
11.731 |