Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -225.171894 |
| Energy at 298.15K | -225.178106 |
| HF Energy | -225.171894 |
| Nuclear repulsion energy | 123.925683 |
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 |
3725 |
3537 |
31.72 |
|
|
|
| 2 |
A |
3611 |
3428 |
2.48 |
|
|
|
| 3 |
A |
1880 |
1785 |
381.29 |
|
|
|
| 4 |
A |
1663 |
1579 |
0.29 |
|
|
|
| 5 |
A |
1198 |
1138 |
2.38 |
|
|
|
| 6 |
A |
976 |
927 |
7.11 |
|
|
|
| 7 |
A |
620 |
588 |
95.75 |
|
|
|
| 8 |
A |
468 |
444 |
3.67 |
|
|
|
| 9 |
A |
396 |
376 |
73.47 |
|
|
|
| 10 |
B |
3725 |
3537 |
29.47 |
|
|
|
| 11 |
B |
3608 |
3425 |
45.98 |
|
|
|
| 12 |
B |
1669 |
1584 |
214.82 |
|
|
|
| 13 |
B |
1451 |
1378 |
197.39 |
|
|
|
| 14 |
B |
1069 |
1014 |
18.73 |
|
|
|
| 15 |
B |
798 |
758 |
126.76 |
|
|
|
| 16 |
B |
587 |
557 |
201.80 |
|
|
|
| 17 |
B |
556 |
528 |
126.30 |
|
|
|
| 18 |
B |
456 |
433 |
85.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14228.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 13507.1 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 B1B95/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.144 |
| O2 |
0.000 |
0.000 |
1.358 |
| N3 |
0.000 |
1.157 |
-0.614 |
| N4 |
0.000 |
-1.157 |
-0.614 |
| H5 |
0.215 |
1.975 |
-0.065 |
| H6 |
0.474 |
1.126 |
-1.504 |
| H7 |
-0.215 |
-1.975 |
-0.065 |
| H8 |
-0.474 |
-1.126 |
-1.504 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2147 | 1.3824 | 1.3824 | 1.9978 | 2.0507 | 1.9978 | 2.0507 |
O2 | 1.2147 | | 2.2859 | 2.2859 | 2.4441 | 3.1117 | 2.4441 | 3.1117 | N3 | 1.3824 | 2.2859 | | 2.3133 | 1.0083 | 1.0089 | 3.1868 | 2.4955 | N4 | 1.3824 | 2.2859 | 2.3133 | | 3.1868 | 2.4955 | 1.0083 | 1.0089 | H5 | 1.9978 | 2.4441 | 1.0083 | 3.1868 | | 1.6904 | 3.9737 | 3.4872 | H6 | 2.0507 | 3.1117 | 1.0089 | 2.4955 | 1.6904 | | 3.4872 | 2.4435 | H7 | 1.9978 | 2.4441 | 3.1868 | 1.0083 | 3.9737 | 3.4872 | | 1.6904 | H8 | 2.0507 | 3.1117 | 2.4955 | 1.0089 | 3.4872 | 2.4435 | 1.6904 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.426 |
|
C1 |
N3 |
H6 |
117.238 |
| C1 |
N4 |
H7 |
112.426 |
|
C1 |
N4 |
H8 |
117.238 |
| O2 |
C1 |
N3 |
123.204 |
|
O2 |
C1 |
N4 |
123.204 |
| N3 |
C1 |
N4 |
113.592 |
|
H5 |
N3 |
H6 |
113.851 |
| H7 |
N4 |
H8 |
113.851 |
|
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 |
0.668 |
|
|
|
| 2 |
O |
-0.507 |
|
|
|
| 3 |
N |
-0.777 |
|
|
|
| 4 |
N |
-0.777 |
|
|
|
| 5 |
H |
0.356 |
|
|
|
| 6 |
H |
0.341 |
|
|
|
| 7 |
H |
0.356 |
|
|
|
| 8 |
H |
0.341 |
|
|
|
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 |
-3.533 |
3.533 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.212 |
3.594 |
0.000 |
| y |
3.594 |
-17.416 |
0.000 |
| z |
0.000 |
0.000 |
-24.510 |
|
| Traceless |
| | x | y | z |
| x |
-3.249 |
3.594 |
0.000 |
| y |
3.594 |
6.945 |
0.000 |
| z |
0.000 |
0.000 |
-3.697 |
|
| Polar |
| 3z2-r2 | -7.393 |
| x2-y2 | -6.796 |
| xy | 3.594 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.059 |
0.176 |
0.000 |
| y |
0.176 |
4.531 |
0.000 |
| z |
0.000 |
0.000 |
4.715 |
<r2> (average value of r
2) Å
2
| <r2> |
68.061 |
| (<r2>)1/2 |
8.250 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -225.169750 |
| Energy at 298.15K | -225.175400 |
| HF Energy | -225.169750 |
| Nuclear repulsion energy | 123.980469 |
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' |
3758 |
3567 |
34.22 |
|
|
|
| 2 |
A' |
3639 |
3454 |
10.63 |
|
|
|
| 3 |
A' |
1868 |
1773 |
404.63 |
|
|
|
| 4 |
A' |
1669 |
1584 |
16.99 |
|
|
|
| 5 |
A' |
1190 |
1130 |
2.65 |
|
|
|
| 6 |
A' |
985 |
935 |
8.19 |
|
|
|
| 7 |
A' |
778 |
739 |
43.68 |
|
|
|
| 8 |
A' |
557 |
528 |
44.96 |
|
|
|
| 9 |
A' |
477 |
453 |
37.37 |
|
|
|
| 10 |
A' |
407 |
386 |
401.86 |
|
|
|
| 11 |
A" |
3756 |
3565 |
37.73 |
|
|
|
| 12 |
A" |
3630 |
3446 |
42.86 |
|
|
|
| 13 |
A" |
1660 |
1575 |
240.60 |
|
|
|
| 14 |
A" |
1457 |
1384 |
194.84 |
|
|
|
| 15 |
A" |
1029 |
977 |
15.55 |
|
|
|
| 16 |
A" |
571 |
542 |
26.98 |
|
|
|
| 17 |
A" |
425 |
403 |
71.40 |
|
|
|
| 18 |
A" |
123 |
117 |
45.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13988.2 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 13279.0 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 |
0.008 |
0.139 |
0.000 |
| O2 |
0.037 |
1.356 |
0.000 |
| N3 |
0.037 |
-0.602 |
1.160 |
| N4 |
0.037 |
-0.602 |
-1.160 |
| H5 |
-0.156 |
-0.069 |
1.991 |
| H6 |
-0.276 |
-1.559 |
1.170 |
| H7 |
-0.156 |
-0.069 |
-1.991 |
| H8 |
-0.276 |
-1.559 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2167 | 1.3765 | 1.3765 | 2.0084 | 2.0815 | 2.0084 | 2.0815 |
O2 | 1.2167 | | 2.2753 | 2.2753 | 2.4555 | 3.1559 | 2.4555 | 3.1559 | N3 | 1.3765 | 2.2753 | | 2.3190 | 1.0063 | 1.0065 | 3.2009 | 2.5377 | N4 | 1.3765 | 2.2753 | 2.3190 | | 3.2009 | 2.5377 | 1.0063 | 1.0065 | H5 | 2.0084 | 2.4555 | 1.0063 | 3.2009 | | 1.7052 | 3.9816 | 3.4965 | H6 | 2.0815 | 3.1559 | 1.0065 | 2.5377 | 1.7052 | | 3.4965 | 2.3402 | H7 | 2.0084 | 2.4555 | 3.2009 | 1.0063 | 3.9816 | 3.4965 | | 1.7052 | H8 | 2.0815 | 3.1559 | 2.5377 | 1.0065 | 3.4965 | 2.3402 | 1.7052 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
113.983 |
|
C1 |
N3 |
H6 |
120.947 |
| C1 |
N4 |
H7 |
113.983 |
|
C1 |
N4 |
H8 |
120.947 |
| O2 |
C1 |
N3 |
122.540 |
|
O2 |
C1 |
N4 |
122.540 |
| N3 |
C1 |
N4 |
114.780 |
|
H5 |
N3 |
H6 |
115.814 |
| H7 |
N4 |
H8 |
115.814 |
|
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 |
0.694 |
|
|
|
| 2 |
O |
-0.520 |
|
|
|
| 3 |
N |
-0.779 |
|
|
|
| 4 |
N |
-0.779 |
|
|
|
| 5 |
H |
0.359 |
|
|
|
| 6 |
H |
0.333 |
|
|
|
| 7 |
H |
0.359 |
|
|
|
| 8 |
H |
0.333 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.776 |
-3.928 |
0.000 |
4.310 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.912 |
1.810 |
0.000 |
| y |
1.810 |
-23.788 |
0.000 |
| z |
0.000 |
0.000 |
-16.727 |
|
| Traceless |
| | x | y | z |
| x |
-4.654 |
1.810 |
0.000 |
| y |
1.810 |
-2.969 |
0.000 |
| z |
0.000 |
0.000 |
7.623 |
|
| Polar |
| 3z2-r2 | 15.246 |
| x2-y2 | -1.124 |
| xy | 1.810 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.934 |
0.155 |
0.000 |
| y |
0.155 |
4.736 |
0.000 |
| z |
0.000 |
0.000 |
4.565 |
<r2> (average value of r
2) Å
2
| <r2> |
68.101 |
| (<r2>)1/2 |
8.252 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -225.169005 |
| Energy at 298.15K | |
| HF Energy | -225.169005 |
| Nuclear repulsion energy | 124.108896 |
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 |
3799 |
3607 |
48.79 |
|
|
|
| 2 |
A1 |
3671 |
3485 |
7.35 |
|
|
|
| 3 |
A1 |
1863 |
1769 |
440.94 |
|
|
|
| 4 |
A1 |
1654 |
1570 |
4.35 |
|
|
|
| 5 |
A1 |
1160 |
1101 |
0.04 |
|
|
|
| 6 |
A1 |
994 |
944 |
6.60 |
|
|
|
| 7 |
A1 |
475 |
451 |
3.37 |
|
|
|
| 8 |
A2 |
379 |
360 |
0.00 |
|
|
|
| 9 |
A2 |
430i |
408i |
0.00 |
|
|
|
| 10 |
B1 |
778 |
739 |
15.25 |
|
|
|
| 11 |
B1 |
578 |
548 |
10.63 |
|
|
|
| 12 |
B1 |
306i |
291i |
579.15 |
|
|
|
| 13 |
B2 |
3797 |
3605 |
47.45 |
|
|
|
| 14 |
B2 |
3662 |
3477 |
66.08 |
|
|
|
| 15 |
B2 |
1653 |
1569 |
319.29 |
|
|
|
| 16 |
B2 |
1461 |
1387 |
195.03 |
|
|
|
| 17 |
B2 |
998 |
947 |
8.35 |
|
|
|
| 18 |
B2 |
561 |
533 |
15.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13374.6 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 12696.5 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 |
0.141 |
| O2 |
0.000 |
0.000 |
1.359 |
| N3 |
0.000 |
1.154 |
-0.596 |
| N4 |
0.000 |
-1.154 |
-0.596 |
| H5 |
0.000 |
2.018 |
-0.085 |
| H6 |
0.000 |
1.186 |
-1.600 |
| H7 |
0.000 |
-2.018 |
-0.085 |
| H8 |
0.000 |
-1.186 |
-1.600 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2180 | 1.3694 | 1.3694 | 2.0305 | 2.1060 | 2.0305 | 2.1060 |
O2 | 1.2180 | | 2.2704 | 2.2704 | 2.4814 | 3.1872 | 2.4814 | 3.1872 | N3 | 1.3694 | 2.2704 | | 2.3080 | 1.0037 | 1.0038 | 3.2128 | 2.5456 | N4 | 1.3694 | 2.2704 | 2.3080 | | 3.2128 | 2.5456 | 1.0037 | 1.0038 | H5 | 2.0305 | 2.4814 | 1.0037 | 3.2128 | | 1.7280 | 4.0357 | 3.5433 | H6 | 2.1060 | 3.1872 | 1.0038 | 2.5456 | 1.7280 | | 3.5433 | 2.3710 | H7 | 2.0305 | 2.4814 | 3.2128 | 1.0037 | 4.0357 | 3.5433 | | 1.7280 | H8 | 2.1060 | 3.1872 | 2.5456 | 1.0038 | 3.5433 | 2.3710 | 1.7280 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.819 |
|
C1 |
N3 |
H6 |
124.373 |
| C1 |
N4 |
H7 |
116.819 |
|
C1 |
N4 |
H8 |
124.373 |
| O2 |
C1 |
N3 |
122.573 |
|
O2 |
C1 |
N4 |
122.573 |
| N3 |
C1 |
N4 |
114.853 |
|
H5 |
N3 |
H6 |
118.808 |
| H7 |
N4 |
H8 |
118.808 |
|
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 |
0.738 |
|
|
|
| 2 |
O |
-0.534 |
|
|
|
| 3 |
N |
-0.805 |
|
|
|
| 4 |
N |
-0.805 |
|
|
|
| 5 |
H |
0.364 |
|
|
|
| 6 |
H |
0.339 |
|
|
|
| 7 |
H |
0.364 |
|
|
|
| 8 |
H |
0.339 |
|
|
|
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 |
-4.301 |
4.301 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.326 |
0.000 |
0.000 |
| y |
0.000 |
-15.885 |
0.000 |
| z |
0.000 |
0.000 |
-23.183 |
|
| Traceless |
| | x | y | z |
| x |
-5.791 |
0.000 |
0.000 |
| y |
0.000 |
8.370 |
0.000 |
| z |
0.000 |
0.000 |
-2.578 |
|
| Polar |
| 3z2-r2 | -5.156 |
| x2-y2 | -9.441 |
| 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 |
1.817 |
0.000 |
0.000 |
| y |
0.000 |
4.540 |
0.000 |
| z |
0.000 |
0.000 |
4.698 |
<r2> (average value of r
2) Å
2
| <r2> |
68.007 |
| (<r2>)1/2 |
8.247 |