Jump to
S1C2
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -225.249157 |
| Energy at 298.15K | -225.255316 |
| HF Energy | -225.249157 |
| Nuclear repulsion energy | 124.118158 |
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 B1B95/6-311G*
| 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 |
3720 |
3566 |
32.53 |
|
|
|
| 2 |
A |
3606 |
3457 |
3.04 |
|
|
|
| 3 |
A |
1847 |
1771 |
415.82 |
|
|
|
| 4 |
A |
1628 |
1561 |
0.62 |
|
|
|
| 5 |
A |
1180 |
1131 |
3.01 |
|
|
|
| 6 |
A |
966 |
926 |
8.29 |
|
|
|
| 7 |
A |
578 |
554 |
76.48 |
|
|
|
| 8 |
A |
468 |
448 |
2.58 |
|
|
|
| 9 |
A |
383 |
367 |
72.19 |
|
|
|
| 10 |
B |
3720 |
3566 |
27.10 |
|
|
|
| 11 |
B |
3601 |
3452 |
44.06 |
|
|
|
| 12 |
B |
1634 |
1567 |
221.33 |
|
|
|
| 13 |
B |
1428 |
1369 |
199.42 |
|
|
|
| 14 |
B |
1047 |
1004 |
22.13 |
|
|
|
| 15 |
B |
792 |
759 |
77.10 |
|
|
|
| 16 |
B |
581 |
557 |
89.19 |
|
|
|
| 17 |
B |
543 |
520 |
168.52 |
|
|
|
| 18 |
B |
445 |
426 |
145.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14083.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 13500.3 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 B1B95/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.145 |
| O2 |
0.000 |
0.000 |
1.356 |
| N3 |
0.000 |
1.156 |
-0.611 |
| N4 |
0.000 |
-1.156 |
-0.611 |
| H5 |
0.207 |
1.978 |
-0.069 |
| H6 |
0.450 |
1.125 |
-1.511 |
| H7 |
-0.207 |
-1.978 |
-0.069 |
| H8 |
-0.450 |
-1.125 |
-1.511 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2104 | 1.3812 | 1.3812 | 1.9998 | 2.0524 | 1.9998 | 2.0524 |
O2 | 1.2104 | | 2.2812 | 2.2812 | 2.4458 | 3.1125 | 2.4458 | 3.1125 | N3 | 1.3812 | 2.2812 | | 2.3114 | 1.0062 | 1.0067 | 3.1865 | 2.4929 | N4 | 1.3812 | 2.2812 | 2.3114 | | 3.1865 | 2.4929 | 1.0062 | 1.0067 | H5 | 1.9998 | 2.4458 | 1.0062 | 3.1865 | | 1.6931 | 3.9766 | 3.4841 | H6 | 2.0524 | 3.1125 | 1.0067 | 2.4929 | 1.6931 | | 3.4841 | 2.4232 | H7 | 1.9998 | 2.4458 | 3.1865 | 1.0062 | 3.9766 | 3.4841 | | 1.6931 | H8 | 2.0524 | 3.1125 | 2.4929 | 1.0067 | 3.4841 | 2.4232 | 1.6931 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.839 |
|
C1 |
N3 |
H6 |
117.666 |
| C1 |
N4 |
H7 |
112.839 |
|
C1 |
N4 |
H8 |
117.666 |
| O2 |
C1 |
N3 |
123.205 |
|
O2 |
C1 |
N4 |
123.205 |
| N3 |
C1 |
N4 |
113.590 |
|
H5 |
N3 |
H6 |
114.519 |
| H7 |
N4 |
H8 |
114.519 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.428 |
|
|
|
| 2 |
O |
-0.386 |
|
|
|
| 3 |
N |
-0.480 |
|
|
|
| 4 |
N |
-0.480 |
|
|
|
| 5 |
H |
0.238 |
|
|
|
| 6 |
H |
0.221 |
|
|
|
| 7 |
H |
0.238 |
|
|
|
| 8 |
H |
0.221 |
|
|
|
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 |
-3.629 |
3.629 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.466 |
3.253 |
0.000 |
| y |
3.253 |
-17.591 |
0.000 |
| z |
0.000 |
0.000 |
-24.734 |
|
| Traceless |
| | x | y | z |
| x |
-3.304 |
3.253 |
0.000 |
| y |
3.253 |
7.009 |
0.000 |
| z |
0.000 |
0.000 |
-3.705 |
|
| Polar |
| 3z2-r2 | -7.410 |
| x2-y2 | -6.875 |
| xy | 3.253 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.521 |
0.173 |
0.000 |
| y |
0.173 |
4.821 |
0.000 |
| z |
0.000 |
0.000 |
4.954 |
<r2> (average value of r
2) Å
2
| <r2> |
68.082 |
| (<r2>)1/2 |
8.251 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -225.231404 |
| Energy at 298.15K | |
| HF Energy | -225.231404 |
| Nuclear repulsion energy | 124.283042 |
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 B1B95/6-311G*
| 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' |
3769 |
3613 |
25.71 |
|
|
|
| 2 |
A' |
3649 |
3498 |
7.60 |
|
|
|
| 3 |
A' |
1851 |
1775 |
457.71 |
|
|
|
| 4 |
A' |
1681 |
1612 |
13.92 |
|
|
|
| 5 |
A' |
1190 |
1141 |
2.71 |
|
|
|
| 6 |
A' |
980 |
939 |
9.30 |
|
|
|
| 7 |
A' |
786 |
754 |
29.62 |
|
|
|
| 8 |
A' |
559 |
535 |
37.57 |
|
|
|
| 9 |
A' |
477 |
457 |
14.34 |
|
|
|
| 10 |
A' |
368 |
353 |
434.82 |
|
|
|
| 11 |
A" |
3766 |
3610 |
28.55 |
|
|
|
| 12 |
A" |
3640 |
3489 |
36.00 |
|
|
|
| 13 |
A" |
1670 |
1601 |
243.18 |
|
|
|
| 14 |
A" |
1448 |
1388 |
218.22 |
|
|
|
| 15 |
A" |
1025 |
982 |
18.28 |
|
|
|
| 16 |
A" |
573 |
550 |
23.29 |
|
|
|
| 17 |
A" |
408 |
391 |
56.94 |
|
|
|
| 18 |
A" |
98i |
94i |
48.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13871.2 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 13297.0 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.008 |
0.142 |
0.000 |
| O2 |
0.034 |
1.352 |
0.000 |
| N3 |
0.034 |
-0.600 |
1.157 |
| N4 |
0.034 |
-0.600 |
-1.157 |
| H5 |
-0.146 |
-0.074 |
1.992 |
| H6 |
-0.252 |
-1.561 |
1.170 |
| H7 |
-0.146 |
-0.074 |
-1.992 |
| H8 |
-0.252 |
-1.561 |
-1.170 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2104 | 1.3746 | 1.3746 | 2.0099 | 2.0823 | 2.0099 | 2.0823 |
O2 | 1.2104 | | 2.2688 | 2.2688 | 2.4564 | 3.1520 | 2.4564 | 3.1520 | N3 | 1.3746 | 2.2688 | | 2.3149 | 1.0030 | 1.0031 | 3.1984 | 2.5347 | N4 | 1.3746 | 2.2688 | 2.3149 | | 3.1984 | 2.5347 | 1.0030 | 1.0031 | H5 | 2.0099 | 2.4564 | 1.0030 | 3.1984 | | 1.7026 | 3.9847 | 3.4965 | H6 | 2.0823 | 3.1520 | 1.0031 | 2.5347 | 1.7026 | | 3.4965 | 2.3407 | H7 | 2.0099 | 2.4564 | 3.1984 | 1.0030 | 3.9847 | 3.4965 | | 1.7026 | H8 | 2.0823 | 3.1520 | 2.5347 | 1.0031 | 3.4965 | 2.3407 | 1.7026 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
114.511 |
|
C1 |
N3 |
H6 |
121.483 |
| C1 |
N4 |
H7 |
114.511 |
|
C1 |
N4 |
H8 |
121.483 |
| O2 |
C1 |
N3 |
122.592 |
|
O2 |
C1 |
N4 |
122.592 |
| N3 |
C1 |
N4 |
114.700 |
|
H5 |
N3 |
H6 |
116.145 |
| H7 |
N4 |
H8 |
116.145 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.611 |
|
|
|
| 2 |
O |
-0.403 |
|
|
|
| 3 |
N |
-0.803 |
|
|
|
| 4 |
N |
-0.803 |
|
|
|
| 5 |
H |
0.363 |
|
|
|
| 6 |
H |
0.336 |
|
|
|
| 7 |
H |
0.363 |
|
|
|
| 8 |
H |
0.336 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.614 |
-4.049 |
0.000 |
4.358 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.304 |
1.683 |
0.000 |
| y |
1.683 |
-23.968 |
0.000 |
| z |
0.000 |
0.000 |
-16.815 |
|
| Traceless |
| | x | y | z |
| x |
-4.912 |
1.683 |
0.000 |
| y |
1.683 |
-2.909 |
0.000 |
| z |
0.000 |
0.000 |
7.821 |
|
| Polar |
| 3z2-r2 | 15.641 |
| x2-y2 | -1.336 |
| xy | 1.683 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.346 |
0.116 |
0.000 |
| y |
0.116 |
4.840 |
0.000 |
| z |
0.000 |
0.000 |
4.706 |
<r2> (average value of r
2) Å
2
| <r2> |
68.042 |
| (<r2>)1/2 |
8.249 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -225.230978 |
| Energy at 298.15K | |
| HF Energy | -225.230978 |
| Nuclear repulsion energy | 124.395642 |
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 B1B95/6-311G*
| 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 |
3805 |
3648 |
37.43 |
|
|
|
| 2 |
A1 |
3675 |
3523 |
4.83 |
|
|
|
| 3 |
A1 |
1844 |
1768 |
492.40 |
|
|
|
| 4 |
A1 |
1668 |
1598 |
1.33 |
|
|
|
| 5 |
A1 |
1165 |
1117 |
0.18 |
|
|
|
| 6 |
A1 |
988 |
947 |
7.95 |
|
|
|
| 7 |
A1 |
477 |
457 |
3.26 |
|
|
|
| 8 |
A2 |
375 |
359 |
0.00 |
|
|
|
| 9 |
A2 |
402i |
386i |
0.00 |
|
|
|
| 10 |
B1 |
790 |
757 |
11.55 |
|
|
|
| 11 |
B1 |
577 |
554 |
10.32 |
|
|
|
| 12 |
B1 |
255i |
244i |
558.13 |
|
|
|
| 13 |
B2 |
3803 |
3645 |
35.26 |
|
|
|
| 14 |
B2 |
3666 |
3514 |
53.63 |
|
|
|
| 15 |
B2 |
1662 |
1594 |
307.47 |
|
|
|
| 16 |
B2 |
1453 |
1393 |
224.29 |
|
|
|
| 17 |
B2 |
1000 |
958 |
11.14 |
|
|
|
| 18 |
B2 |
566 |
543 |
14.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13428.1 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12872.2 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 B1B95/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.142 |
| O2 |
0.000 |
0.000 |
1.354 |
| N3 |
0.000 |
1.153 |
-0.595 |
| N4 |
0.000 |
-1.153 |
-0.595 |
| H5 |
0.000 |
2.015 |
-0.086 |
| H6 |
0.000 |
1.185 |
-1.595 |
| H7 |
0.000 |
-2.015 |
-0.086 |
| H8 |
0.000 |
-1.185 |
-1.595 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2121 | 1.3682 | 1.3682 | 2.0277 | 2.1024 | 2.0277 | 2.1024 |
O2 | 1.2121 | | 2.2643 | 2.2643 | 2.4766 | 3.1781 | 2.4766 | 3.1781 | N3 | 1.3682 | 2.2643 | | 2.3059 | 1.0008 | 1.0007 | 3.2084 | 2.5426 | N4 | 1.3682 | 2.2643 | 2.3059 | | 3.2084 | 2.5426 | 1.0008 | 1.0007 | H5 | 2.0277 | 2.4766 | 1.0008 | 3.2084 | | 1.7221 | 4.0297 | 3.5374 | H6 | 2.1024 | 3.1781 | 1.0007 | 2.5426 | 1.7221 | | 3.5374 | 2.3694 | H7 | 2.0277 | 2.4766 | 3.2084 | 1.0008 | 4.0297 | 3.5374 | | 1.7221 | H8 | 2.1024 | 3.1781 | 2.5426 | 1.0007 | 3.5374 | 2.3694 | 1.7221 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.875 |
|
C1 |
N3 |
H6 |
124.393 |
| C1 |
N4 |
H7 |
116.875 |
|
C1 |
N4 |
H8 |
124.393 |
| O2 |
C1 |
N3 |
122.577 |
|
O2 |
C1 |
N4 |
122.577 |
| N3 |
C1 |
N4 |
114.846 |
|
H5 |
N3 |
H6 |
118.732 |
| H7 |
N4 |
H8 |
118.732 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.665 |
|
|
|
| 2 |
O |
-0.416 |
|
|
|
| 3 |
N |
-0.842 |
|
|
|
| 4 |
N |
-0.842 |
|
|
|
| 5 |
H |
0.371 |
|
|
|
| 6 |
H |
0.346 |
|
|
|
| 7 |
H |
0.371 |
|
|
|
| 8 |
H |
0.346 |
|
|
|
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 |
-4.372 |
4.372 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.664 |
0.000 |
0.000 |
| y |
0.000 |
-16.081 |
0.000 |
| z |
0.000 |
0.000 |
-23.464 |
|
| Traceless |
| | x | y | z |
| x |
-5.892 |
0.000 |
0.000 |
| y |
0.000 |
8.483 |
0.000 |
| z |
0.000 |
0.000 |
-2.591 |
|
| Polar |
| 3z2-r2 | -5.183 |
| x2-y2 | -9.584 |
| 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 |
2.266 |
0.000 |
0.000 |
| y |
0.000 |
4.684 |
0.000 |
| z |
0.000 |
0.000 |
4.781 |
<r2> (average value of r
2) Å
2
| <r2> |
67.956 |
| (<r2>)1/2 |
8.244 |