Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -225.108632 |
| Energy at 298.15K | -225.114620 |
| HF Energy | -225.108632 |
| Nuclear repulsion energy | 123.109716 |
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 B1B95/6-31G
| 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 |
3805 |
3629 |
39.07 |
|
|
|
| 2 |
A |
3665 |
3496 |
6.06 |
|
|
|
| 3 |
A |
1770 |
1688 |
400.72 |
|
|
|
| 4 |
A |
1684 |
1606 |
2.28 |
|
|
|
| 5 |
A |
1164 |
1110 |
1.35 |
|
|
|
| 6 |
A |
991 |
945 |
4.33 |
|
|
|
| 7 |
A |
521 |
496 |
0.00 |
|
|
|
| 8 |
A |
482 |
459 |
3.54 |
|
|
|
| 9 |
A |
212 |
202 |
0.00 |
|
|
|
| 10 |
B |
3802 |
3626 |
39.09 |
|
|
|
| 11 |
B |
3657 |
3488 |
60.25 |
|
|
|
| 12 |
B |
1671 |
1594 |
265.65 |
|
|
|
| 13 |
B |
1491 |
1422 |
259.90 |
|
|
|
| 14 |
B |
1029 |
981 |
8.38 |
|
|
|
| 15 |
B |
784 |
747 |
172.85 |
|
|
|
| 16 |
B |
584 |
556 |
185.04 |
|
|
|
| 17 |
B |
560 |
534 |
14.67 |
|
|
|
| 18 |
B |
515 |
491 |
522.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14192.7 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 13535.6 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 B1B95/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.131 |
| O2 |
0.000 |
0.000 |
1.378 |
| N3 |
0.000 |
1.161 |
-0.602 |
| N4 |
0.000 |
-1.161 |
-0.602 |
| H5 |
0.002 |
2.023 |
-0.089 |
| H6 |
-0.002 |
1.194 |
-1.605 |
| H7 |
-0.002 |
-2.023 |
-0.089 |
| H8 |
0.002 |
-1.194 |
-1.605 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2470 | 1.3730 | 1.3730 | 2.0353 | 2.1069 | 2.0353 | 2.1069 |
O2 | 1.2470 | | 2.2953 | 2.2953 | 2.4992 | 3.2130 | 2.4992 | 3.2130 | N3 | 1.3730 | 2.2953 | | 2.3219 | 1.0035 | 1.0035 | 3.2254 | 2.5594 | N4 | 1.3730 | 2.2953 | 2.3219 | | 3.2254 | 2.5594 | 1.0035 | 1.0035 | H5 | 2.0353 | 2.4992 | 1.0035 | 3.2254 | | 1.7281 | 4.0467 | 3.5564 | H6 | 2.1069 | 3.2130 | 1.0035 | 2.5594 | 1.7281 | | 3.5564 | 2.3875 | H7 | 2.0353 | 2.4992 | 3.2254 | 1.0035 | 4.0467 | 3.5564 | | 1.7281 | H8 | 2.1069 | 3.2130 | 2.5594 | 1.0035 | 3.5564 | 2.3875 | 1.7281 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.983 |
|
C1 |
N3 |
H6 |
124.144 |
| C1 |
N4 |
H7 |
116.983 |
|
C1 |
N4 |
H8 |
124.144 |
| O2 |
C1 |
N3 |
122.270 |
|
O2 |
C1 |
N4 |
122.270 |
| N3 |
C1 |
N4 |
115.460 |
|
H5 |
N3 |
H6 |
118.873 |
| H7 |
N4 |
H8 |
118.873 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.671 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.774 |
|
|
|
| 4 |
N |
-0.774 |
|
|
|
| 5 |
H |
0.354 |
|
|
|
| 6 |
H |
0.327 |
|
|
|
| 7 |
H |
0.354 |
|
|
|
| 8 |
H |
0.327 |
|
|
|
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 |
-4.670 |
4.670 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.681 |
0.010 |
0.000 |
| y |
0.010 |
-15.944 |
0.000 |
| z |
0.000 |
0.000 |
-24.071 |
|
| Traceless |
| | x | y | z |
| x |
-5.673 |
0.010 |
0.000 |
| y |
0.010 |
8.932 |
0.000 |
| z |
0.000 |
0.000 |
-3.259 |
|
| Polar |
| 3z2-r2 | -6.517 |
| x2-y2 | -9.736 |
| xy | 0.010 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.458 |
0.001 |
0.000 |
| y |
0.001 |
4.415 |
0.000 |
| z |
0.000 |
0.000 |
4.766 |
<r2> (average value of r
2) Å
2
| <r2> |
69.121 |
| (<r2>)1/2 |
8.314 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -225.104054 |
| Energy at 298.15K | -225.110071 |
| HF Energy | -225.104054 |
| Nuclear repulsion energy | 123.251407 |
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 B1B95/6-31G
| 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' |
3819 |
3642 |
41.97 |
|
|
|
| 2 |
A' |
3679 |
3509 |
6.63 |
|
|
|
| 3 |
A' |
1778 |
1695 |
409.50 |
|
|
|
| 4 |
A' |
1691 |
1612 |
2.08 |
|
|
|
| 5 |
A' |
1169 |
1115 |
1.45 |
|
|
|
| 6 |
A' |
997 |
951 |
4.36 |
|
|
|
| 7 |
A' |
789 |
753 |
183.72 |
|
|
|
| 8 |
A' |
587 |
559 |
201.06 |
|
|
|
| 9 |
A' |
521 |
497 |
506.02 |
|
|
|
| 10 |
A' |
484 |
461 |
3.52 |
|
|
|
| 11 |
A" |
3816 |
3639 |
39.27 |
|
|
|
| 12 |
A" |
3671 |
3501 |
63.49 |
|
|
|
| 13 |
A" |
1678 |
1601 |
271.17 |
|
|
|
| 14 |
A" |
1500 |
1430 |
260.31 |
|
|
|
| 15 |
A" |
1035 |
987 |
7.97 |
|
|
|
| 16 |
A" |
563 |
537 |
14.94 |
|
|
|
| 17 |
A" |
527 |
503 |
0.00 |
|
|
|
| 18 |
A" |
219 |
208 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14259.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 13599.7 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 B1B95/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.131 |
0.000 |
| O2 |
-0.000 |
1.377 |
0.000 |
| N3 |
0.000 |
-0.601 |
1.160 |
| N4 |
0.000 |
-0.601 |
-1.160 |
| H5 |
0.000 |
-0.088 |
2.021 |
| H6 |
0.001 |
-1.603 |
1.192 |
| H7 |
0.000 |
-0.088 |
-2.021 |
| H8 |
0.001 |
-1.603 |
-1.192 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2457 | 1.3713 | 1.3713 | 2.0331 | 2.1042 | 2.0331 | 2.1042 |
O2 | 1.2457 | | 2.2925 | 2.2925 | 2.4962 | 3.2092 | 2.4962 | 3.2092 | N3 | 1.3713 | 2.2925 | | 2.3194 | 1.0025 | 1.0025 | 3.2219 | 2.5565 | N4 | 1.3713 | 2.2925 | 2.3194 | | 3.2219 | 2.5565 | 1.0025 | 1.0025 | H5 | 2.0331 | 2.4962 | 1.0025 | 3.2219 | | 1.7265 | 4.0424 | 3.5525 | H6 | 2.1042 | 3.2092 | 1.0025 | 2.5565 | 1.7265 | | 3.5525 | 2.3846 | H7 | 2.0331 | 2.4962 | 3.2219 | 1.0025 | 4.0424 | 3.5525 | | 1.7265 | H8 | 2.1042 | 3.2092 | 2.5565 | 1.0025 | 3.5525 | 2.3846 | 1.7265 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.991 |
|
C1 |
N3 |
H6 |
124.120 |
| C1 |
N4 |
H7 |
116.991 |
|
C1 |
N4 |
H8 |
124.120 |
| O2 |
C1 |
N3 |
122.256 |
|
O2 |
C1 |
N4 |
122.256 |
| N3 |
C1 |
N4 |
115.488 |
|
H5 |
N3 |
H6 |
118.889 |
| H7 |
N4 |
H8 |
118.889 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.682 |
|
|
|
| 2 |
O |
-0.490 |
|
|
|
| 3 |
N |
-0.783 |
|
|
|
| 4 |
N |
-0.783 |
|
|
|
| 5 |
H |
0.356 |
|
|
|
| 6 |
H |
0.330 |
|
|
|
| 7 |
H |
0.356 |
|
|
|
| 8 |
H |
0.330 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.007 |
-4.692 |
0.000 |
4.692 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.681 |
-0.008 |
0.000 |
| y |
-0.008 |
-24.097 |
0.000 |
| z |
0.000 |
0.000 |
-15.945 |
|
| Traceless |
| | x | y | z |
| x |
-5.660 |
-0.008 |
0.000 |
| y |
-0.008 |
-3.284 |
0.000 |
| z |
0.000 |
0.000 |
8.944 |
|
| Polar |
| 3z2-r2 | 17.888 |
| x2-y2 | -1.584 |
| xy | -0.008 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.455 |
-0.002 |
0.000 |
| y |
-0.002 |
4.735 |
0.000 |
| z |
0.000 |
0.000 |
4.371 |
<r2> (average value of r
2) Å
2
| <r2> |
68.998 |
| (<r2>)1/2 |
8.306 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -225.104054 |
| Energy at 298.15K | -225.110068 |
| HF Energy | -225.104054 |
| Nuclear repulsion energy | 123.247826 |
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 B1B95/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3819 |
3642 |
41.92 |
|
|
|
| 2 |
A1 |
3680 |
3509 |
6.64 |
|
|
|
| 3 |
A1 |
1778 |
1696 |
410.02 |
|
|
|
| 4 |
A1 |
1691 |
1612 |
1.81 |
|
|
|
| 5 |
A1 |
1169 |
1115 |
1.42 |
|
|
|
| 6 |
A1 |
996 |
950 |
4.40 |
|
|
|
| 7 |
A1 |
484 |
461 |
3.51 |
|
|
|
| 8 |
A2 |
526 |
502 |
0.00 |
|
|
|
| 9 |
A2 |
218 |
208 |
0.00 |
|
|
|
| 10 |
B1 |
789 |
753 |
183.26 |
|
|
|
| 11 |
B1 |
586 |
559 |
199.80 |
|
|
|
| 12 |
B1 |
520 |
496 |
507.91 |
|
|
|
| 13 |
B2 |
3816 |
3640 |
39.38 |
|
|
|
| 14 |
B2 |
3672 |
3502 |
63.44 |
|
|
|
| 15 |
B2 |
1678 |
1600 |
270.37 |
|
|
|
| 16 |
B2 |
1499 |
1429 |
260.90 |
|
|
|
| 17 |
B2 |
1034 |
986 |
8.03 |
|
|
|
| 18 |
B2 |
562 |
536 |
14.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14258.6 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 13598.5 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 B1B95/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.131 |
| O2 |
0.000 |
0.000 |
1.376 |
| N3 |
0.000 |
1.160 |
-0.601 |
| N4 |
0.000 |
-1.160 |
-0.601 |
| H5 |
0.000 |
2.021 |
-0.089 |
| H6 |
0.000 |
1.192 |
-1.603 |
| H7 |
0.000 |
-2.021 |
-0.089 |
| H8 |
0.000 |
-1.192 |
-1.603 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2455 | 1.3715 | 1.3715 | 2.0334 | 2.1041 | 2.0334 | 2.1041 |
O2 | 1.2455 | | 2.2925 | 2.2925 | 2.4966 | 3.2090 | 2.4966 | 3.2090 | N3 | 1.3715 | 2.2925 | | 2.3196 | 1.0025 | 1.0024 | 3.2223 | 2.5564 | N4 | 1.3715 | 2.2925 | 2.3196 | | 3.2223 | 2.5564 | 1.0025 | 1.0024 | H5 | 2.0334 | 2.4966 | 1.0025 | 3.2223 | | 1.7265 | 4.0430 | 3.5524 | H6 | 2.1041 | 3.2090 | 1.0024 | 2.5564 | 1.7265 | | 3.5524 | 2.3840 | H7 | 2.0334 | 2.4966 | 3.2223 | 1.0025 | 4.0430 | 3.5524 | | 1.7265 | H8 | 2.1041 | 3.2090 | 2.5564 | 1.0024 | 3.5524 | 2.3840 | 1.7265 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
117.008 |
|
C1 |
N3 |
H6 |
124.098 |
| C1 |
N4 |
H7 |
117.008 |
|
C1 |
N4 |
H8 |
124.098 |
| O2 |
C1 |
N3 |
122.258 |
|
O2 |
C1 |
N4 |
122.258 |
| N3 |
C1 |
N4 |
115.484 |
|
H5 |
N3 |
H6 |
118.894 |
| H7 |
N4 |
H8 |
118.894 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.682 |
|
|
|
| 2 |
O |
-0.490 |
|
|
|
| 3 |
N |
-0.783 |
|
|
|
| 4 |
N |
-0.783 |
|
|
|
| 5 |
H |
0.356 |
|
|
|
| 6 |
H |
0.330 |
|
|
|
| 7 |
H |
0.356 |
|
|
|
| 8 |
H |
0.330 |
|
|
|
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 |
-4.690 |
4.690 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.681 |
0.000 |
0.000 |
| y |
0.000 |
-15.945 |
0.000 |
| z |
0.000 |
0.000 |
-24.097 |
|
| Traceless |
| | x | y | z |
| x |
-5.660 |
0.000 |
0.000 |
| y |
0.000 |
8.944 |
0.000 |
| z |
0.000 |
0.000 |
-3.283 |
|
| Polar |
| 3z2-r2 | -6.566 |
| x2-y2 | -9.736 |
| 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 |
1.455 |
0.000 |
0.000 |
| y |
0.000 |
4.371 |
0.000 |
| z |
0.000 |
0.000 |
4.734 |
<r2> (average value of r
2) Å
2
| <r2> |
69.002 |
| (<r2>)1/2 |
8.307 |