Jump to
S1C2
S1C3
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -224.135757 |
| Energy at 298.15K | -224.141717 |
| HF Energy | -224.135757 |
| Nuclear repulsion energy | 123.650550 |
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 LSDA/6-31+G**
| 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 |
3644 |
3589 |
53.83 |
|
|
|
| 2 |
A |
3517 |
3464 |
4.01 |
|
|
|
| 3 |
A |
1791 |
1764 |
458.55 |
|
|
|
| 4 |
A |
1553 |
1529 |
2.31 |
|
|
|
| 5 |
A |
1120 |
1103 |
0.32 |
|
|
|
| 6 |
A |
967 |
953 |
7.74 |
|
|
|
| 7 |
A |
489 |
482 |
44.18 |
|
|
|
| 8 |
A |
457 |
450 |
1.72 |
|
|
|
| 9 |
A |
341 |
336 |
67.61 |
|
|
|
| 10 |
B |
3643 |
3589 |
53.21 |
|
|
|
| 11 |
B |
3509 |
3457 |
60.18 |
|
|
|
| 12 |
B |
1567 |
1544 |
353.27 |
|
|
|
| 13 |
B |
1411 |
1390 |
130.66 |
|
|
|
| 14 |
B |
989 |
975 |
10.58 |
|
|
|
| 15 |
B |
751 |
740 |
33.96 |
|
|
|
| 16 |
B |
559 |
551 |
55.48 |
|
|
|
| 17 |
B |
526 |
518 |
93.99 |
|
|
|
| 18 |
B |
421 |
415 |
304.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13627.6 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 13423.2 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 LSDA/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.135 |
| O2 |
0.000 |
0.000 |
1.361 |
| N3 |
0.000 |
1.156 |
-0.606 |
| N4 |
0.000 |
-1.156 |
-0.606 |
| H5 |
0.159 |
1.997 |
-0.054 |
| H6 |
0.386 |
1.158 |
-1.549 |
| H7 |
-0.159 |
-1.997 |
-0.054 |
| H8 |
-0.386 |
-1.158 |
-1.549 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2262 | 1.3737 | 1.3737 | 2.0122 | 2.0795 | 2.0122 | 2.0795 |
O2 | 1.2262 | | 2.2822 | 2.2822 | 2.4527 | 3.1555 | 2.4527 | 3.1555 | N3 | 1.3737 | 2.2822 | | 2.3130 | 1.0184 | 1.0186 | 3.2055 | 2.5283 | N4 | 1.3737 | 2.2822 | 2.3130 | | 3.2055 | 2.5283 | 1.0184 | 1.0186 | H5 | 2.0122 | 2.4527 | 1.0184 | 3.2055 | | 1.7296 | 4.0067 | 3.5332 | H6 | 2.0795 | 3.1555 | 1.0186 | 2.5283 | 1.7296 | | 3.5332 | 2.4403 | H7 | 2.0122 | 2.4527 | 3.2055 | 1.0184 | 4.0067 | 3.5332 | | 1.7296 | H8 | 2.0795 | 3.1555 | 2.5283 | 1.0186 | 3.5332 | 2.4403 | 1.7296 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.712 |
|
C1 |
N3 |
H6 |
120.018 |
| C1 |
N4 |
H7 |
113.712 |
|
C1 |
N4 |
H8 |
120.018 |
| O2 |
C1 |
N3 |
122.659 |
|
O2 |
C1 |
N4 |
122.659 |
| N3 |
C1 |
N4 |
114.682 |
|
H5 |
N3 |
H6 |
116.230 |
| H7 |
N4 |
H8 |
116.230 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.400 |
|
|
|
| 2 |
O |
-0.510 |
|
|
|
| 3 |
N |
-0.588 |
|
|
|
| 4 |
N |
-0.588 |
|
|
|
| 5 |
H |
0.335 |
|
|
|
| 6 |
H |
0.307 |
|
|
|
| 7 |
H |
0.335 |
|
|
|
| 8 |
H |
0.307 |
|
|
|
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 |
-4.086 |
4.086 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.153 |
2.934 |
0.000 |
| y |
2.934 |
-17.584 |
0.000 |
| z |
0.000 |
0.000 |
-25.440 |
|
| Traceless |
| | x | y | z |
| x |
-4.642 |
2.934 |
0.000 |
| y |
2.934 |
8.212 |
0.000 |
| z |
0.000 |
0.000 |
-3.571 |
|
| Polar |
| 3z2-r2 | -7.141 |
| x2-y2 | -8.569 |
| xy | 2.934 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.714 |
0.058 |
0.000 |
| y |
0.058 |
5.745 |
0.000 |
| z |
0.000 |
0.000 |
6.027 |
<r2> (average value of r
2) Å
2
| <r2> |
69.012 |
| (<r2>)1/2 |
8.307 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -224.134846 |
| Energy at 298.15K | |
| HF Energy | -224.134846 |
| Nuclear repulsion energy | 123.691452 |
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 LSDA/6-31+G**
| 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' |
3678 |
3622 |
60.74 |
|
|
|
| 2 |
A' |
3542 |
3489 |
6.97 |
|
|
|
| 3 |
A' |
1782 |
1756 |
492.82 |
|
|
|
| 4 |
A' |
1551 |
1528 |
8.28 |
|
|
|
| 5 |
A' |
1106 |
1089 |
0.17 |
|
|
|
| 6 |
A' |
971 |
957 |
5.84 |
|
|
|
| 7 |
A' |
746 |
735 |
5.47 |
|
|
|
| 8 |
A' |
549 |
541 |
17.50 |
|
|
|
| 9 |
A' |
459 |
452 |
4.59 |
|
|
|
| 10 |
A' |
171 |
168 |
467.47 |
|
|
|
| 11 |
A" |
3675 |
3620 |
63.95 |
|
|
|
| 12 |
A" |
3531 |
3478 |
66.82 |
|
|
|
| 13 |
A" |
1566 |
1543 |
427.59 |
|
|
|
| 14 |
A" |
1411 |
1390 |
99.45 |
|
|
|
| 15 |
A" |
950 |
936 |
6.42 |
|
|
|
| 16 |
A" |
545 |
537 |
14.64 |
|
|
|
| 17 |
A" |
355 |
350 |
8.27 |
|
|
|
| 18 |
A" |
239i |
235i |
16.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13175.2 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 12977.6 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 LSDA/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.003 |
0.133 |
0.000 |
| O2 |
0.017 |
1.360 |
0.000 |
| N3 |
0.017 |
-0.596 |
1.158 |
| N4 |
0.017 |
-0.596 |
-1.158 |
| H5 |
-0.073 |
-0.061 |
2.017 |
| H6 |
-0.122 |
-1.602 |
1.194 |
| H7 |
-0.073 |
-0.061 |
-2.017 |
| H8 |
-0.122 |
-1.602 |
-1.194 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2277 | 1.3683 | 1.3683 | 2.0274 | 2.1100 | 2.0274 | 2.1100 |
O2 | 1.2277 | | 2.2735 | 2.2735 | 2.4687 | 3.1972 | 2.4687 | 3.1972 | N3 | 1.3683 | 2.2735 | | 2.3157 | 1.0162 | 1.0161 | 3.2207 | 2.5621 | N4 | 1.3683 | 2.2735 | 2.3157 | | 3.2207 | 2.5621 | 1.0162 | 1.0161 | H5 | 2.0274 | 2.4687 | 1.0162 | 3.2207 | | 1.7479 | 4.0335 | 3.5624 | H6 | 2.1100 | 3.1972 | 1.0161 | 2.5621 | 1.7479 | | 3.5624 | 2.3889 | H7 | 2.0274 | 2.4687 | 3.2207 | 1.0162 | 4.0335 | 3.5624 | | 1.7479 | H8 | 2.1100 | 3.1972 | 2.5621 | 1.0161 | 3.5624 | 2.3889 | 1.7479 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
115.688 |
|
C1 |
N3 |
H6 |
123.811 |
| C1 |
N4 |
H7 |
115.688 |
|
C1 |
N4 |
H8 |
123.811 |
| O2 |
C1 |
N3 |
122.180 |
|
O2 |
C1 |
N4 |
122.180 |
| N3 |
C1 |
N4 |
115.604 |
|
H5 |
N3 |
H6 |
118.641 |
| H7 |
N4 |
H8 |
118.641 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.456 |
|
|
|
| 2 |
O |
-0.534 |
|
|
|
| 3 |
N |
-0.603 |
|
|
|
| 4 |
N |
-0.603 |
|
|
|
| 5 |
H |
0.339 |
|
|
|
| 6 |
H |
0.302 |
|
|
|
| 7 |
H |
0.339 |
|
|
|
| 8 |
H |
0.302 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.769 |
-4.490 |
0.000 |
4.556 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.861 |
0.840 |
0.000 |
| y |
0.840 |
-24.674 |
0.000 |
| z |
0.000 |
0.000 |
-16.887 |
|
| Traceless |
| | x | y | z |
| x |
-6.080 |
0.840 |
0.000 |
| y |
0.840 |
-2.800 |
0.000 |
| z |
0.000 |
0.000 |
8.881 |
|
| Polar |
| 3z2-r2 | 17.762 |
| x2-y2 | -2.187 |
| xy | 0.840 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.670 |
0.022 |
0.000 |
| y |
0.022 |
5.914 |
0.000 |
| z |
0.000 |
0.000 |
5.739 |
<r2> (average value of r
2) Å
2
| <r2> |
69.076 |
| (<r2>)1/2 |
8.311 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -224.134825 |
| Energy at 298.15K | |
| HF Energy | -224.134825 |
| Nuclear repulsion energy | 123.706164 |
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 LSDA/6-31+G**
| 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 |
3685 |
3630 |
64.09 |
|
|
|
| 2 |
A1 |
3548 |
3495 |
6.09 |
|
|
|
| 3 |
A1 |
1782 |
1755 |
503.08 |
|
|
|
| 4 |
A1 |
1549 |
1526 |
5.49 |
|
|
|
| 5 |
A1 |
1101 |
1084 |
0.20 |
|
|
|
| 6 |
A1 |
972 |
957 |
5.18 |
|
|
|
| 7 |
A1 |
459 |
452 |
3.94 |
|
|
|
| 8 |
A2 |
350 |
345 |
0.00 |
|
|
|
| 9 |
A2 |
299i |
295i |
0.00 |
|
|
|
| 10 |
B1 |
747 |
735 |
3.43 |
|
|
|
| 11 |
B1 |
555 |
547 |
11.80 |
|
|
|
| 12 |
B1 |
119i |
117i |
489.15 |
|
|
|
| 13 |
B2 |
3683 |
3628 |
66.40 |
|
|
|
| 14 |
B2 |
3537 |
3484 |
71.66 |
|
|
|
| 15 |
B2 |
1567 |
1543 |
447.75 |
|
|
|
| 16 |
B2 |
1411 |
1390 |
95.35 |
|
|
|
| 17 |
B2 |
944 |
930 |
5.25 |
|
|
|
| 18 |
B2 |
543 |
535 |
13.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13006.8 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 12811.7 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 LSDA/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.133 |
| O2 |
0.000 |
0.000 |
1.361 |
| N3 |
0.000 |
1.157 |
-0.595 |
| N4 |
0.000 |
-1.157 |
-0.595 |
| H5 |
0.000 |
2.022 |
-0.064 |
| H6 |
0.000 |
1.198 |
-1.610 |
| H7 |
0.000 |
-2.022 |
-0.064 |
| H8 |
0.000 |
-1.198 |
-1.610 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2279 | 1.3671 | 1.3671 | 2.0318 | 2.1150 | 2.0318 | 2.1150 |
O2 | 1.2279 | | 2.2728 | 2.2728 | 2.4736 | 3.2034 | 2.4736 | 3.2034 | N3 | 1.3671 | 2.2728 | | 2.3138 | 1.0157 | 1.0156 | 3.2233 | 2.5641 | N4 | 1.3671 | 2.2728 | 2.3138 | | 3.2233 | 2.5641 | 1.0157 | 1.0156 | H5 | 2.0318 | 2.4736 | 1.0157 | 3.2233 | | 1.7526 | 4.0445 | 3.5722 | H6 | 2.1150 | 3.2034 | 1.0156 | 2.5641 | 1.7526 | | 3.5722 | 2.3957 | H7 | 2.0318 | 2.4736 | 3.2233 | 1.0157 | 4.0445 | 3.5722 | | 1.7526 | H8 | 2.1150 | 3.2034 | 2.5641 | 1.0156 | 3.5722 | 2.3957 | 1.7526 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.231 |
|
C1 |
N3 |
H6 |
124.502 |
| C1 |
N4 |
H7 |
116.231 |
|
C1 |
N4 |
H8 |
124.502 |
| O2 |
C1 |
N3 |
122.193 |
|
O2 |
C1 |
N4 |
122.193 |
| N3 |
C1 |
N4 |
115.614 |
|
H5 |
N3 |
H6 |
119.267 |
| H7 |
N4 |
H8 |
119.267 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.477 |
|
|
|
| 2 |
O |
-0.541 |
|
|
|
| 3 |
N |
-0.615 |
|
|
|
| 4 |
N |
-0.615 |
|
|
|
| 5 |
H |
0.341 |
|
|
|
| 6 |
H |
0.306 |
|
|
|
| 7 |
H |
0.341 |
|
|
|
| 8 |
H |
0.306 |
|
|
|
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 |
-4.563 |
4.563 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.961 |
0.000 |
0.000 |
| y |
0.000 |
-16.733 |
0.000 |
| z |
0.000 |
0.000 |
-24.557 |
|
| Traceless |
| | x | y | z |
| x |
-6.316 |
0.000 |
0.000 |
| y |
0.000 |
9.026 |
0.000 |
| z |
0.000 |
0.000 |
-2.710 |
|
| Polar |
| 3z2-r2 | -5.420 |
| x2-y2 | -10.228 |
| 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 |
3.652 |
0.000 |
0.000 |
| y |
0.000 |
5.724 |
0.000 |
| z |
0.000 |
0.000 |
5.882 |
<r2> (average value of r
2) Å
2
| <r2> |
69.075 |
| (<r2>)1/2 |
8.311 |