Jump to
S1C2
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -223.932266 |
| Energy at 298.15K | -223.938565 |
| HF Energy | -223.932266 |
| Nuclear repulsion energy | 123.836087 |
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 |
4023 |
3620 |
90.04 |
|
|
|
| 2 |
A |
3871 |
3483 |
11.85 |
|
|
|
| 3 |
A |
1850 |
1665 |
455.53 |
|
|
|
| 4 |
A |
1794 |
1614 |
188.89 |
|
|
|
| 5 |
A |
1250 |
1125 |
14.49 |
|
|
|
| 6 |
A |
1037 |
933 |
7.11 |
|
|
|
| 7 |
A |
584 |
526 |
0.00 |
|
|
|
| 8 |
A |
514 |
462 |
3.48 |
|
|
|
| 9 |
A |
301 |
271 |
0.00 |
|
|
|
| 10 |
B |
4020 |
3617 |
35.09 |
|
|
|
| 11 |
B |
3865 |
3478 |
108.07 |
|
|
|
| 12 |
B |
1797 |
1617 |
250.47 |
|
|
|
| 13 |
B |
1576 |
1418 |
363.11 |
|
|
|
| 14 |
B |
1131 |
1018 |
10.14 |
|
|
|
| 15 |
B |
859 |
773 |
242.35 |
|
|
|
| 16 |
B |
620 |
558 |
422.16 |
|
|
|
| 17 |
B |
594 |
535 |
22.53 |
|
|
|
| 18 |
B |
558 |
502 |
353.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15121.4 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 13607.8 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 |
0.000 |
0.000 |
0.129 |
| O2 |
0.000 |
0.000 |
1.366 |
| N3 |
0.000 |
1.161 |
-0.596 |
| N4 |
0.000 |
-1.161 |
-0.596 |
| H5 |
-0.000 |
2.016 |
-0.091 |
| H6 |
-0.001 |
1.184 |
-1.587 |
| H7 |
0.000 |
-2.016 |
-0.091 |
| H8 |
0.001 |
-1.184 |
-1.587 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2368 | 1.3689 | 1.3689 | 2.0276 | 2.0852 | 2.0276 | 2.0852 |
O2 | 1.2368 | | 2.2800 | 2.2800 | 2.4872 | 3.1818 | 2.4872 | 3.1818 | N3 | 1.3689 | 2.2800 | | 2.3218 | 0.9927 | 0.9914 | 3.2163 | 2.5457 | N4 | 1.3689 | 2.2800 | 2.3218 | | 3.2163 | 2.5457 | 0.9927 | 0.9914 | H5 | 2.0276 | 2.4872 | 0.9927 | 3.2163 | | 1.7116 | 4.0311 | 3.5320 | H6 | 2.0852 | 3.1818 | 0.9914 | 2.5457 | 1.7116 | | 3.5320 | 2.3679 | H7 | 2.0276 | 2.4872 | 3.2163 | 0.9927 | 4.0311 | 3.5320 | | 1.7116 | H8 | 2.0852 | 3.1818 | 2.5457 | 0.9914 | 3.5320 | 2.3679 | 1.7116 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.423 |
|
C1 |
N3 |
H6 |
123.333 |
| C1 |
N4 |
H7 |
117.423 |
|
C1 |
N4 |
H8 |
123.333 |
| O2 |
C1 |
N3 |
122.001 |
|
O2 |
C1 |
N4 |
122.001 |
| N3 |
C1 |
N4 |
115.998 |
|
H5 |
N3 |
H6 |
119.245 |
| H7 |
N4 |
H8 |
119.245 |
|
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 |
0.595 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.808 |
|
|
|
| 4 |
N |
-0.808 |
|
|
|
| 5 |
H |
0.394 |
|
|
|
| 6 |
H |
0.359 |
|
|
|
| 7 |
H |
0.394 |
|
|
|
| 8 |
H |
0.359 |
|
|
|
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 |
-5.279 |
5.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.458 |
-0.005 |
0.000 |
| y |
-0.005 |
-16.418 |
0.000 |
| z |
0.000 |
0.000 |
-25.799 |
|
| Traceless |
| | x | y | z |
| x |
-5.349 |
-0.005 |
0.000 |
| y |
-0.005 |
9.710 |
0.000 |
| z |
0.000 |
0.000 |
-4.361 |
|
| Polar |
| 3z2-r2 | -8.723 |
| x2-y2 | -10.040 |
| xy | -0.005 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.889 |
-0.000 |
0.000 |
| y |
-0.000 |
3.827 |
0.000 |
| z |
0.000 |
0.000 |
4.504 |
<r2> (average value of r
2) Å
2
| <r2> |
69.155 |
| (<r2>)1/2 |
8.316 |
Jump to
S1C1
S1C3
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -223.932266 |
| Energy at 298.15K | -223.938565 |
| HF Energy | -223.932266 |
| Nuclear repulsion energy | 123.836754 |
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' |
4023 |
3620 |
90.03 |
|
|
|
| 2 |
A' |
3871 |
3483 |
11.88 |
|
|
|
| 3 |
A' |
1850 |
1665 |
452.87 |
|
|
|
| 4 |
A' |
1793 |
1614 |
191.37 |
|
|
|
| 5 |
A' |
1250 |
1125 |
14.57 |
|
|
|
| 6 |
A' |
1037 |
933 |
7.07 |
|
|
|
| 7 |
A' |
860 |
774 |
242.49 |
|
|
|
| 8 |
A' |
620 |
558 |
423.31 |
|
|
|
| 9 |
A' |
558 |
503 |
351.91 |
|
|
|
| 10 |
A' |
514 |
462 |
3.48 |
|
|
|
| 11 |
A" |
4019 |
3617 |
35.10 |
|
|
|
| 12 |
A" |
3865 |
3478 |
108.06 |
|
|
|
| 13 |
A" |
1797 |
1617 |
250.72 |
|
|
|
| 14 |
A" |
1576 |
1419 |
363.00 |
|
|
|
| 15 |
A" |
1131 |
1018 |
10.10 |
|
|
|
| 16 |
A" |
594 |
535 |
22.53 |
|
|
|
| 17 |
A" |
584 |
526 |
0.00 |
|
|
|
| 18 |
A" |
301 |
271 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15121.8 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 13608.1 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 |
0.129 |
0.000 |
| O2 |
0.000 |
1.366 |
0.000 |
| N3 |
0.000 |
-0.596 |
1.161 |
| N4 |
0.000 |
-0.596 |
-1.161 |
| H5 |
0.000 |
-0.091 |
2.015 |
| H6 |
-0.001 |
-1.587 |
1.184 |
| H7 |
0.000 |
-0.091 |
-2.015 |
| H8 |
-0.001 |
-1.587 |
-1.184 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2369 | 1.3688 | 1.3688 | 2.0275 | 2.0852 | 2.0275 | 2.0852 |
O2 | 1.2369 | | 2.2800 | 2.2800 | 2.4872 | 3.1819 | 2.4872 | 3.1819 | N3 | 1.3688 | 2.2800 | | 2.3217 | 0.9927 | 0.9914 | 3.2162 | 2.5457 | N4 | 1.3688 | 2.2800 | 2.3217 | | 3.2162 | 2.5457 | 0.9927 | 0.9914 | H5 | 2.0275 | 2.4872 | 0.9927 | 3.2162 | | 1.7116 | 4.0309 | 3.5319 | H6 | 2.0852 | 3.1819 | 0.9914 | 2.5457 | 1.7116 | | 3.5319 | 2.3680 | H7 | 2.0275 | 2.4872 | 3.2162 | 0.9927 | 4.0309 | 3.5319 | | 1.7116 | H8 | 2.0852 | 3.1819 | 2.5457 | 0.9914 | 3.5319 | 2.3680 | 1.7116 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.421 |
|
C1 |
N3 |
H6 |
123.340 |
| C1 |
N4 |
H7 |
117.421 |
|
C1 |
N4 |
H8 |
123.340 |
| O2 |
C1 |
N3 |
122.002 |
|
O2 |
C1 |
N4 |
122.002 |
| N3 |
C1 |
N4 |
115.997 |
|
H5 |
N3 |
H6 |
119.239 |
| H7 |
N4 |
H8 |
119.239 |
|
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 |
0.595 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.807 |
|
|
|
| 4 |
N |
-0.807 |
|
|
|
| 5 |
H |
0.394 |
|
|
|
| 6 |
H |
0.359 |
|
|
|
| 7 |
H |
0.394 |
|
|
|
| 8 |
H |
0.359 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.003 |
-5.280 |
0.000 |
5.280 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.458 |
0.004 |
0.000 |
| y |
0.004 |
-25.800 |
0.000 |
| z |
0.000 |
0.000 |
-16.418 |
|
| Traceless |
| | x | y | z |
| x |
-5.349 |
0.004 |
0.000 |
| y |
0.004 |
-4.363 |
0.000 |
| z |
0.000 |
0.000 |
9.711 |
|
| Polar |
| 3z2-r2 | 19.423 |
| x2-y2 | -0.657 |
| xy | 0.004 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.889 |
0.000 |
0.000 |
| y |
0.000 |
4.504 |
0.000 |
| z |
0.000 |
0.000 |
3.827 |
<r2> (average value of r
2) Å
2
| <r2> |
69.154 |
| (<r2>)1/2 |
8.316 |
Jump to
S1C1
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -223.932266 |
| Energy at 298.15K | -223.938563 |
| HF Energy | -223.932266 |
| Nuclear repulsion energy | 123.831353 |
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 |
A1 |
4023 |
3620 |
90.06 |
|
|
|
| 2 |
A1 |
3871 |
3483 |
11.78 |
|
|
|
| 3 |
A1 |
1850 |
1665 |
455.56 |
|
|
|
| 4 |
A1 |
1794 |
1614 |
188.72 |
|
|
|
| 5 |
A1 |
1250 |
1125 |
14.47 |
|
|
|
| 6 |
A1 |
1036 |
933 |
7.14 |
|
|
|
| 7 |
A1 |
514 |
462 |
3.48 |
|
|
|
| 8 |
A2 |
584 |
525 |
0.00 |
|
|
|
| 9 |
A2 |
301 |
271 |
0.00 |
|
|
|
| 10 |
B1 |
859 |
773 |
241.97 |
|
|
|
| 11 |
B1 |
620 |
558 |
421.84 |
|
|
|
| 12 |
B1 |
558 |
502 |
354.05 |
|
|
|
| 13 |
B2 |
4020 |
3617 |
35.06 |
|
|
|
| 14 |
B2 |
3865 |
3478 |
108.19 |
|
|
|
| 15 |
B2 |
1797 |
1617 |
250.22 |
|
|
|
| 16 |
B2 |
1576 |
1418 |
363.26 |
|
|
|
| 17 |
B2 |
1131 |
1018 |
10.16 |
|
|
|
| 18 |
B2 |
594 |
535 |
22.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15120.5 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 13606.9 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 C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.129 |
| O2 |
0.000 |
0.000 |
1.366 |
| N3 |
0.000 |
1.161 |
-0.596 |
| N4 |
0.000 |
-1.161 |
-0.596 |
| H5 |
0.000 |
2.016 |
-0.091 |
| H6 |
0.000 |
1.184 |
-1.587 |
| H7 |
0.000 |
-2.016 |
-0.091 |
| H8 |
0.000 |
-1.184 |
-1.587 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2368 | 1.3690 | 1.3690 | 2.0277 | 2.0852 | 2.0277 | 2.0852 |
O2 | 1.2368 | | 2.2799 | 2.2799 | 2.4872 | 3.1818 | 2.4872 | 3.1818 | N3 | 1.3690 | 2.2799 | | 2.3223 | 0.9927 | 0.9913 | 3.2167 | 2.5461 | N4 | 1.3690 | 2.2799 | 2.3223 | | 3.2167 | 2.5461 | 0.9927 | 0.9913 | H5 | 2.0277 | 2.4872 | 0.9927 | 3.2167 | | 1.7116 | 4.0314 | 3.5324 | H6 | 2.0852 | 3.1818 | 0.9913 | 2.5461 | 1.7116 | | 3.5324 | 2.3684 | H7 | 2.0277 | 2.4872 | 3.2167 | 0.9927 | 4.0314 | 3.5324 | | 1.7116 | H8 | 2.0852 | 3.1818 | 2.5461 | 0.9913 | 3.5324 | 2.3684 | 1.7116 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.429 |
|
C1 |
N3 |
H6 |
123.324 |
| C1 |
N4 |
H7 |
117.429 |
|
C1 |
N4 |
H8 |
123.324 |
| O2 |
C1 |
N3 |
121.990 |
|
O2 |
C1 |
N4 |
121.990 |
| N3 |
C1 |
N4 |
116.021 |
|
H5 |
N3 |
H6 |
119.247 |
| H7 |
N4 |
H8 |
119.247 |
|
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 |
0.595 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.808 |
|
|
|
| 4 |
N |
-0.808 |
|
|
|
| 5 |
H |
0.394 |
|
|
|
| 6 |
H |
0.359 |
|
|
|
| 7 |
H |
0.394 |
|
|
|
| 8 |
H |
0.359 |
|
|
|
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 |
-5.279 |
5.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.458 |
0.000 |
0.000 |
| y |
0.000 |
-16.417 |
0.000 |
| z |
0.000 |
0.000 |
-25.799 |
|
| Traceless |
| | x | y | z |
| x |
-5.350 |
0.000 |
0.000 |
| y |
0.000 |
9.712 |
0.000 |
| z |
0.000 |
0.000 |
-4.362 |
|
| Polar |
| 3z2-r2 | -8.724 |
| x2-y2 | -10.042 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.889 |
0.000 |
0.000 |
| y |
0.000 |
3.828 |
0.000 |
| z |
0.000 |
0.000 |
4.503 |
<r2> (average value of r
2) Å
2
| <r2> |
69.161 |
| (<r2>)1/2 |
8.316 |