Jump to
S1C2
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -168.844454 |
| Energy at 298.15K | -168.848402 |
| HF Energy | -168.844454 |
| Nuclear repulsion energy | 70.545819 |
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' |
4097 |
3687 |
95.85 |
|
|
|
| 2 |
A' |
3784 |
3405 |
14.83 |
|
|
|
| 3 |
A' |
3280 |
2951 |
61.84 |
|
|
|
| 4 |
A' |
1893 |
1704 |
238.06 |
|
|
|
| 5 |
A' |
1542 |
1387 |
16.08 |
|
|
|
| 6 |
A' |
1366 |
1229 |
191.56 |
|
|
|
| 7 |
A' |
1238 |
1114 |
68.92 |
|
|
|
| 8 |
A' |
1085 |
976 |
306.08 |
|
|
|
| 9 |
A' |
642 |
578 |
2.44 |
|
|
|
| 10 |
A" |
1180 |
1062 |
9.49 |
|
|
|
| 11 |
A" |
907 |
816 |
98.68 |
|
|
|
| 12 |
A" |
304 |
274 |
155.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10658.0 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 9591.2 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.382 |
0.000 |
| O2 |
-1.009 |
-0.541 |
0.000 |
| N3 |
1.201 |
0.010 |
0.000 |
| H4 |
-0.339 |
1.410 |
0.000 |
| H5 |
-1.891 |
-0.187 |
0.000 |
| H6 |
1.889 |
0.742 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3675 | 1.2579 | 1.0824 | 1.9752 | 1.9233 |
O2 | 1.3675 | | 2.2777 | 2.0631 | 0.9510 | 3.1694 | N3 | 1.2579 | 2.2777 | | 2.0819 | 3.0991 | 1.0048 | H4 | 1.0824 | 2.0631 | 2.0819 | | 2.2275 | 2.3263 | H5 | 1.9752 | 0.9510 | 3.0991 | 2.2275 | | 3.8932 | H6 | 1.9233 | 3.1694 | 1.0048 | 2.3263 | 3.8932 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
115.678 |
|
C1 |
N3 |
H6 |
115.972 |
| O2 |
C1 |
N3 |
120.298 |
|
O2 |
C1 |
H4 |
114.226 |
| N3 |
C1 |
H4 |
125.476 |
|
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 |
0.104 |
|
|
|
| 2 |
O |
-0.563 |
|
|
|
| 3 |
N |
-0.389 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
| 5 |
H |
0.406 |
|
|
|
| 6 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.147 |
4.459 |
0.000 |
4.949 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.351 |
1.513 |
0.000 |
| y |
1.513 |
-18.747 |
0.000 |
| z |
0.000 |
0.000 |
-19.134 |
|
| Traceless |
| | x | y | z |
| x |
5.589 |
1.513 |
0.000 |
| y |
1.513 |
-2.504 |
0.000 |
| z |
0.000 |
0.000 |
-3.085 |
|
| Polar |
| 3z2-r2 | -6.170 |
| x2-y2 | 5.396 |
| xy | 1.513 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.797 |
-0.076 |
0.000 |
| y |
-0.076 |
2.415 |
0.000 |
| z |
0.000 |
0.000 |
1.307 |
<r2> (average value of r
2) Å
2
| <r2> |
41.967 |
| (<r2>)1/2 |
6.478 |
Jump to
S1C1
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -168.859021 |
| Energy at 298.15K | -168.863239 |
| HF Energy | -168.859021 |
| Nuclear repulsion energy | 70.901852 |
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' |
4040 |
3636 |
84.88 |
|
|
|
| 2 |
A' |
3801 |
3421 |
18.79 |
|
|
|
| 3 |
A' |
3389 |
3049 |
29.92 |
|
|
|
| 4 |
A' |
1852 |
1666 |
321.72 |
|
|
|
| 5 |
A' |
1513 |
1361 |
32.21 |
|
|
|
| 6 |
A' |
1457 |
1311 |
27.46 |
|
|
|
| 7 |
A' |
1253 |
1127 |
127.68 |
|
|
|
| 8 |
A' |
1106 |
995 |
263.94 |
|
|
|
| 9 |
A' |
606 |
545 |
64.98 |
|
|
|
| 10 |
A" |
1191 |
1071 |
1.08 |
|
|
|
| 11 |
A" |
916 |
825 |
82.39 |
|
|
|
| 12 |
A" |
642 |
578 |
341.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10882.0 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 9792.7 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.426 |
0.000 |
| O2 |
-1.110 |
-0.356 |
0.000 |
| N3 |
1.162 |
-0.066 |
0.000 |
| H4 |
-0.276 |
1.465 |
0.000 |
| H5 |
-0.913 |
-1.291 |
0.000 |
| H6 |
1.932 |
0.578 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3580 | 1.2624 | 1.0747 | 1.9448 | 1.9382 |
O2 | 1.3580 | | 2.2908 | 2.0029 | 0.9556 | 3.1823 | N3 | 1.2624 | 2.2908 | | 2.1008 | 2.4096 | 1.0036 | H4 | 1.0747 | 2.0029 | 2.1008 | | 2.8286 | 2.3798 | H5 | 1.9448 | 0.9556 | 2.4096 | 2.8286 | | 3.4037 | H6 | 1.9382 | 3.1823 | 1.0036 | 2.3798 | 3.4037 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
113.262 |
|
C1 |
N3 |
H6 |
117.133 |
| O2 |
C1 |
N3 |
121.857 |
|
O2 |
C1 |
H4 |
110.298 |
| N3 |
C1 |
H4 |
127.845 |
|
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 |
0.137 |
|
|
|
| 2 |
O |
-0.585 |
|
|
|
| 3 |
N |
-0.472 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
0.426 |
|
|
|
| 6 |
H |
0.287 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.544 |
1.477 |
0.000 |
1.574 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.610 |
4.083 |
0.000 |
| y |
4.083 |
-13.763 |
0.000 |
| z |
0.000 |
0.000 |
-19.140 |
|
| Traceless |
| | x | y | z |
| x |
-4.158 |
4.083 |
0.000 |
| y |
4.083 |
6.112 |
0.000 |
| z |
0.000 |
0.000 |
-1.954 |
|
| Polar |
| 3z2-r2 | -3.908 |
| x2-y2 | -6.847 |
| xy | 4.083 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.195 |
-0.104 |
0.000 |
| y |
-0.104 |
2.797 |
0.000 |
| z |
0.000 |
0.000 |
1.296 |
<r2> (average value of r
2) Å
2
| <r2> |
41.380 |
| (<r2>)1/2 |
6.433 |
Jump to
S1C1
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -168.851809 |
| Energy at 298.15K | -168.855915 |
| HF Energy | -168.851809 |
| Nuclear repulsion energy | 70.414081 |
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' |
4053 |
3647 |
57.94 |
|
|
|
| 2 |
A' |
3735 |
3361 |
12.84 |
|
|
|
| 3 |
A' |
3479 |
3130 |
13.95 |
|
|
|
| 4 |
A' |
1840 |
1656 |
316.41 |
|
|
|
| 5 |
A' |
1529 |
1376 |
0.38 |
|
|
|
| 6 |
A' |
1386 |
1248 |
40.33 |
|
|
|
| 7 |
A' |
1170 |
1053 |
376.77 |
|
|
|
| 8 |
A' |
1110 |
999 |
82.46 |
|
|
|
| 9 |
A' |
604 |
544 |
44.00 |
|
|
|
| 10 |
A" |
1199 |
1079 |
104.63 |
|
|
|
| 11 |
A" |
946 |
852 |
99.20 |
|
|
|
| 12 |
A" |
478 |
430 |
188.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10764.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 9686.6 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.451 |
0.000 |
| O2 |
-1.099 |
-0.374 |
0.000 |
| N3 |
1.223 |
0.138 |
0.000 |
| H4 |
-0.311 |
1.472 |
0.000 |
| H5 |
-0.934 |
-1.313 |
0.000 |
| H6 |
1.478 |
-0.838 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3738 | 1.2621 | 1.0678 | 1.9961 | 1.9609 |
O2 | 1.3738 | | 2.3772 | 2.0070 | 0.9540 | 2.6187 | N3 | 1.2621 | 2.3772 | | 2.0331 | 2.5994 | 1.0082 | H4 | 1.0678 | 2.0070 | 2.0331 | | 2.8544 | 2.9219 | H5 | 1.9961 | 0.9540 | 2.5994 | 2.8544 | | 2.4589 | H6 | 1.9609 | 2.6187 | 1.0082 | 2.9219 | 2.4589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
116.924 |
|
C1 |
N3 |
H6 |
119.056 |
| O2 |
C1 |
N3 |
128.759 |
|
O2 |
C1 |
H4 |
109.937 |
| N3 |
C1 |
H4 |
121.305 |
|
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 |
0.136 |
|
|
|
| 2 |
O |
-0.596 |
|
|
|
| 3 |
N |
-0.440 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
| 5 |
H |
0.411 |
|
|
|
| 6 |
H |
0.263 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.720 |
-2.332 |
0.000 |
2.440 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.905 |
-2.668 |
0.000 |
| y |
-2.668 |
-12.695 |
0.000 |
| z |
0.000 |
0.000 |
-19.135 |
|
| Traceless |
| | x | y | z |
| x |
-8.990 |
-2.668 |
0.000 |
| y |
-2.668 |
9.325 |
0.000 |
| z |
0.000 |
0.000 |
-0.335 |
|
| Polar |
| 3z2-r2 | -0.669 |
| x2-y2 | -12.210 |
| xy | -2.668 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.989 |
-0.307 |
0.000 |
| y |
-0.307 |
3.009 |
0.000 |
| z |
0.000 |
0.000 |
1.368 |
<r2> (average value of r
2) Å
2
| <r2> |
42.155 |
| (<r2>)1/2 |
6.493 |