Jump to
S1C2
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -169.831601 |
| Energy at 298.15K | -169.835612 |
| HF Energy | -169.831601 |
| Nuclear repulsion energy | 71.145103 |
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 B1B95/6-311G*
| 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' |
3877 |
3717 |
51.53 |
|
|
|
| 2 |
A' |
3568 |
3420 |
2.87 |
|
|
|
| 3 |
A' |
3046 |
2919 |
81.37 |
|
|
|
| 4 |
A' |
1804 |
1729 |
204.30 |
|
|
|
| 5 |
A' |
1458 |
1397 |
15.23 |
|
|
|
| 6 |
A' |
1357 |
1301 |
180.35 |
|
|
|
| 7 |
A' |
1213 |
1163 |
59.44 |
|
|
|
| 8 |
A' |
1082 |
1037 |
215.20 |
|
|
|
| 9 |
A' |
626 |
600 |
1.05 |
|
|
|
| 10 |
A" |
1056 |
1012 |
7.13 |
|
|
|
| 11 |
A" |
842 |
807 |
71.13 |
|
|
|
| 12 |
A" |
401 |
384 |
83.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10164.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 9743.2 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.371 |
0.000 |
| O2 |
-0.998 |
-0.533 |
0.000 |
| N3 |
1.193 |
-0.012 |
0.000 |
| H4 |
-0.344 |
1.413 |
0.000 |
| H5 |
-1.843 |
-0.083 |
0.000 |
| H6 |
1.814 |
0.789 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3462 | 1.2534 | 1.0967 | 1.8985 | 1.8615 |
O2 | 1.3462 | | 2.2521 | 2.0522 | 0.9581 | 3.1068 | N3 | 1.2534 | 2.2521 | | 2.0957 | 3.0377 | 1.0134 | H4 | 1.0967 | 2.0522 | 2.0957 | | 2.1177 | 2.2459 | H5 | 1.8985 | 0.9581 | 3.0377 | 2.1177 | | 3.7599 | H6 | 1.8615 | 3.1068 | 1.0134 | 2.2459 | 3.7599 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
109.807 |
|
C1 |
N3 |
H6 |
109.958 |
| O2 |
C1 |
N3 |
120.028 |
|
O2 |
C1 |
H4 |
113.910 |
| N3 |
C1 |
H4 |
126.062 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.102 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
N |
-0.491 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
| 5 |
H |
0.402 |
|
|
|
| 6 |
H |
0.285 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.132 |
3.342 |
0.000 |
3.964 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.563 |
1.260 |
0.000 |
| y |
1.260 |
-17.818 |
0.000 |
| z |
0.000 |
0.000 |
-18.681 |
|
| Traceless |
| | x | y | z |
| x |
4.687 |
1.260 |
0.000 |
| y |
1.260 |
-1.696 |
0.000 |
| z |
0.000 |
0.000 |
-2.990 |
|
| Polar |
| 3z2-r2 | -5.981 |
| x2-y2 | 4.255 |
| xy | 1.260 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.807 |
-0.009 |
0.000 |
| y |
-0.009 |
2.904 |
0.000 |
| z |
0.000 |
0.000 |
1.707 |
<r2> (average value of r
2) Å
2
| <r2> |
40.884 |
| (<r2>)1/2 |
6.394 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -169.842680 |
| Energy at 298.15K | -169.846864 |
| HF Energy | -169.842680 |
| Nuclear repulsion energy | 71.530478 |
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 B1B95/6-311G*
| 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' |
3766 |
3610 |
32.63 |
|
|
|
| 2 |
A' |
3572 |
3424 |
2.80 |
|
|
|
| 3 |
A' |
3137 |
3007 |
42.70 |
|
|
|
| 4 |
A' |
1775 |
1701 |
282.54 |
|
|
|
| 5 |
A' |
1425 |
1366 |
26.35 |
|
|
|
| 6 |
A' |
1392 |
1334 |
2.05 |
|
|
|
| 7 |
A' |
1221 |
1170 |
125.45 |
|
|
|
| 8 |
A' |
1091 |
1046 |
174.29 |
|
|
|
| 9 |
A' |
591 |
566 |
56.69 |
|
|
|
| 10 |
A" |
1066 |
1022 |
0.08 |
|
|
|
| 11 |
A" |
845 |
810 |
28.01 |
|
|
|
| 12 |
A" |
666 |
638 |
219.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10272.9 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 9847.6 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.415 |
0.000 |
| O2 |
-1.105 |
-0.335 |
0.000 |
| N3 |
1.151 |
-0.093 |
0.000 |
| H4 |
-0.267 |
1.472 |
0.000 |
| H5 |
-0.816 |
-1.257 |
0.000 |
| H6 |
1.868 |
0.623 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3358 | 1.2578 | 1.0904 | 1.8604 | 1.8797 |
O2 | 1.3358 | | 2.2688 | 1.9922 | 0.9659 | 3.1238 | N3 | 1.2578 | 2.2688 | | 2.1120 | 2.2852 | 1.0130 | H4 | 1.0904 | 1.9922 | 2.1120 | | 2.7836 | 2.2986 | H5 | 1.8604 | 0.9659 | 2.2852 | 2.7836 | | 3.2765 | H6 | 1.8797 | 3.1238 | 1.0130 | 2.2986 | 3.2765 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
106.750 |
|
C1 |
N3 |
H6 |
111.283 |
| O2 |
C1 |
N3 |
122.003 |
|
O2 |
C1 |
H4 |
109.985 |
| N3 |
C1 |
H4 |
128.013 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.132 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.547 |
|
|
|
| 4 |
H |
0.204 |
|
|
|
| 5 |
H |
0.402 |
|
|
|
| 6 |
H |
0.294 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.157 |
0.989 |
0.000 |
1.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.445 |
3.433 |
0.000 |
| y |
3.433 |
-13.846 |
0.000 |
| z |
0.000 |
0.000 |
-18.673 |
|
| Traceless |
| | x | y | z |
| x |
-3.186 |
3.433 |
0.000 |
| y |
3.433 |
5.213 |
0.000 |
| z |
0.000 |
0.000 |
-2.027 |
|
| Polar |
| 3z2-r2 | -4.055 |
| x2-y2 | -5.600 |
| xy | 3.433 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.305 |
0.068 |
0.000 |
| y |
0.068 |
3.307 |
0.000 |
| z |
0.000 |
0.000 |
1.693 |
<r2> (average value of r
2) Å
2
| <r2> |
40.213 |
| (<r2>)1/2 |
6.341 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -169.836611 |
| Energy at 298.15K | -169.840728 |
| HF Energy | -169.836611 |
| Nuclear repulsion energy | 71.068344 |
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 B1B95/6-311G*
| 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' |
3799 |
3642 |
18.92 |
|
|
|
| 2 |
A' |
3477 |
3333 |
9.42 |
|
|
|
| 3 |
A' |
3201 |
3068 |
16.71 |
|
|
|
| 4 |
A' |
1771 |
1698 |
291.22 |
|
|
|
| 5 |
A' |
1428 |
1369 |
0.75 |
|
|
|
| 6 |
A' |
1365 |
1309 |
27.11 |
|
|
|
| 7 |
A' |
1142 |
1095 |
296.58 |
|
|
|
| 8 |
A' |
1102 |
1056 |
29.18 |
|
|
|
| 9 |
A' |
595 |
571 |
39.18 |
|
|
|
| 10 |
A" |
1089 |
1044 |
78.97 |
|
|
|
| 11 |
A" |
862 |
826 |
60.25 |
|
|
|
| 12 |
A" |
546 |
523 |
90.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10188.1 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 9766.3 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.435 |
0.000 |
| O2 |
-1.095 |
-0.352 |
0.000 |
| N3 |
1.219 |
0.127 |
0.000 |
| H4 |
-0.305 |
1.477 |
0.000 |
| H5 |
-0.837 |
-1.280 |
0.000 |
| H6 |
1.373 |
-0.881 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3482 | 1.2568 | 1.0859 | 1.9078 | 1.9016 |
O2 | 1.3482 | | 2.3627 | 1.9920 | 0.9630 | 2.5239 | N3 | 1.2568 | 2.3627 | | 2.0355 | 2.4909 | 1.0201 | H4 | 1.0859 | 1.9920 | 2.0355 | | 2.8074 | 2.8941 | H5 | 1.9078 | 0.9630 | 2.4909 | 2.8074 | | 2.2453 | H6 | 1.9016 | 2.5239 | 1.0201 | 2.8941 | 2.2453 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
110.151 |
|
C1 |
N3 |
H6 |
112.853 |
| O2 |
C1 |
N3 |
130.145 |
|
O2 |
C1 |
H4 |
109.377 |
| N3 |
C1 |
H4 |
120.478 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.120 |
|
|
|
| 2 |
O |
-0.486 |
|
|
|
| 3 |
N |
-0.513 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
| 5 |
H |
0.386 |
|
|
|
| 6 |
H |
0.260 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.933 |
-2.037 |
0.000 |
2.241 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.051 |
-1.926 |
0.000 |
| y |
-1.926 |
-12.776 |
0.000 |
| z |
0.000 |
0.000 |
-18.657 |
|
| Traceless |
| | x | y | z |
| x |
-7.334 |
-1.926 |
0.000 |
| y |
-1.926 |
8.078 |
0.000 |
| z |
0.000 |
0.000 |
-0.744 |
|
| Polar |
| 3z2-r2 | -1.487 |
| x2-y2 | -10.275 |
| xy | -1.926 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.121 |
-0.152 |
0.000 |
| y |
-0.152 |
3.473 |
0.000 |
| z |
0.000 |
0.000 |
1.715 |
<r2> (average value of r
2) Å
2
| <r2> |
40.841 |
| (<r2>)1/2 |
6.391 |