Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -225.238962 |
Energy at 298.15K | -225.245163 |
HF Energy | -225.238962 |
Nuclear repulsion energy | 123.847164 |
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 B3PW91/6-311G*
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 |
3709 |
3571 |
20.92 |
|
|
|
2 |
A |
3598 |
3464 |
1.58 |
|
|
|
3 |
A |
1840 |
1771 |
413.62 |
|
|
|
4 |
A |
1673 |
1611 |
0.12 |
|
|
|
5 |
A |
1197 |
1152 |
3.59 |
|
|
|
6 |
A |
962 |
926 |
7.63 |
|
|
|
7 |
A |
597 |
575 |
89.67 |
|
|
|
8 |
A |
475 |
457 |
4.21 |
|
|
|
9 |
A |
387 |
372 |
76.23 |
|
|
|
10 |
B |
3709 |
3571 |
21.71 |
|
|
|
11 |
B |
3594 |
3460 |
31.86 |
|
|
|
12 |
B |
1675 |
1613 |
208.88 |
|
|
|
13 |
B |
1432 |
1379 |
212.52 |
|
|
|
14 |
B |
1062 |
1023 |
24.98 |
|
|
|
15 |
B |
796 |
767 |
94.82 |
|
|
|
16 |
B |
584 |
562 |
128.49 |
|
|
|
17 |
B |
552 |
532 |
184.76 |
|
|
|
18 |
B |
452 |
435 |
122.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14147.2 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 13619.5 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 B3PW91/6-311G*
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 |
1.358 |
N3 |
-0.117 |
1.152 |
-0.613 |
N4 |
0.117 |
-1.152 |
-0.613 |
H5 |
0.000 |
1.992 |
-0.069 |
H6 |
0.343 |
1.175 |
-1.510 |
H7 |
0.000 |
-1.992 |
-0.069 |
H8 |
-0.343 |
-1.175 |
-1.510 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2127 | 1.3846 | 1.3846 | 2.0039 | 2.0583 | 2.0039 | 2.0583 |
O2 | 1.2127 | | 2.2863 | 2.2863 | 2.4509 | 3.1179 | 2.4509 | 3.1179 | N3 | 1.3846 | 2.2863 | | 2.3169 | 1.0074 | 1.0082 | 3.1937 | 2.5041 | N4 | 1.3846 | 2.2863 | 2.3169 | | 3.1937 | 2.5041 | 1.0074 | 1.0082 | H5 | 2.0039 | 2.4509 | 1.0074 | 3.1937 | | 1.6914 | 3.9848 | 3.4961 | H6 | 2.0583 | 3.1179 | 1.0082 | 2.5041 | 1.6914 | | 3.4961 | 2.4475 | H7 | 2.0039 | 2.4509 | 3.1937 | 1.0074 | 3.9848 | 3.4961 | | 1.6914 | H8 | 2.0583 | 3.1179 | 2.5041 | 1.0082 | 3.4961 | 2.4475 | 1.6914 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
112.862 |
|
C1 |
N3 |
H6 |
117.822 |
C1 |
N4 |
H7 |
112.862 |
|
C1 |
N4 |
H8 |
117.822 |
O2 |
C1 |
N3 |
123.211 |
|
O2 |
C1 |
N4 |
123.211 |
N3 |
C1 |
N4 |
113.578 |
|
H5 |
N3 |
H6 |
114.110 |
H7 |
N4 |
H8 |
114.110 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.579 |
|
|
|
2 |
O |
-0.393 |
|
|
|
3 |
N |
-0.794 |
|
|
|
4 |
N |
-0.794 |
|
|
|
5 |
H |
0.359 |
|
|
|
6 |
H |
0.342 |
|
|
|
7 |
H |
0.359 |
|
|
|
8 |
H |
0.342 |
|
|
|
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 |
-3.638 |
3.638 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.309 |
2.686 |
0.000 |
y |
2.686 |
-16.859 |
0.000 |
z |
0.000 |
0.000 |
-24.783 |
|
Traceless |
| x | y | z |
x |
-4.487 |
2.686 |
0.000 |
y |
2.686 |
8.187 |
0.000 |
z |
0.000 |
0.000 |
-3.699 |
|
Polar |
3z2-r2 | -7.398 |
x2-y2 | -8.449 |
xy | 2.686 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.444 |
-0.079 |
0.000 |
y |
-0.079 |
4.750 |
0.000 |
z |
0.000 |
0.000 |
4.906 |
<r2> (average value of r
2) Å
2
<r2> |
68.370 |
(<r2>)1/2 |
8.269 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -225.237002 |
Energy at 298.15K | |
HF Energy | -225.237002 |
Nuclear repulsion energy | 123.898028 |
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 B3PW91/6-311G*
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' |
3744 |
3604 |
23.41 |
|
|
|
2 |
A' |
3625 |
3490 |
6.84 |
|
|
|
3 |
A' |
1830 |
1761 |
444.67 |
|
|
|
4 |
A' |
1677 |
1614 |
12.99 |
|
|
|
5 |
A' |
1186 |
1142 |
2.70 |
|
|
|
6 |
A' |
970 |
934 |
8.97 |
|
|
|
7 |
A' |
781 |
752 |
27.71 |
|
|
|
8 |
A' |
556 |
536 |
36.67 |
|
|
|
9 |
A' |
480 |
462 |
13.87 |
|
|
|
10 |
A' |
366 |
352 |
440.62 |
|
|
|
11 |
A" |
3741 |
3602 |
28.98 |
|
|
|
12 |
A" |
3616 |
3481 |
32.00 |
|
|
|
13 |
A" |
1663 |
1601 |
229.36 |
|
|
|
14 |
A" |
1437 |
1383 |
222.50 |
|
|
|
15 |
A" |
1020 |
982 |
20.34 |
|
|
|
16 |
A" |
572 |
551 |
22.00 |
|
|
|
17 |
A" |
404 |
389 |
55.41 |
|
|
|
18 |
A" |
93i |
89i |
48.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13788.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 13273.8 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.008 |
0.142 |
0.000 |
O2 |
0.034 |
1.356 |
0.000 |
N3 |
0.034 |
-0.601 |
1.161 |
N4 |
0.034 |
-0.601 |
-1.161 |
H5 |
-0.145 |
-0.074 |
1.999 |
H6 |
-0.249 |
-1.566 |
1.176 |
H7 |
-0.145 |
-0.074 |
-1.999 |
H8 |
-0.249 |
-1.566 |
-1.176 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2143 | 1.3789 | 1.3789 | 2.0163 | 2.0896 | 2.0163 | 2.0896 |
O2 | 1.2143 | | 2.2757 | 2.2757 | 2.4643 | 3.1625 | 2.4643 | 3.1625 | N3 | 1.3789 | 2.2757 | | 2.3226 | 1.0054 | 1.0057 | 3.2087 | 2.5444 | N4 | 1.3789 | 2.2757 | 2.3226 | | 3.2087 | 2.5444 | 1.0054 | 1.0057 | H5 | 2.0163 | 2.4643 | 1.0054 | 3.2087 | | 1.7069 | 3.9977 | 3.5094 | H6 | 2.0896 | 3.1625 | 1.0057 | 2.5444 | 1.7069 | | 3.5094 | 2.3520 | H7 | 2.0163 | 2.4643 | 3.2087 | 1.0054 | 3.9977 | 3.5094 | | 1.7069 | H8 | 2.0896 | 3.1625 | 2.5444 | 1.0057 | 3.5094 | 2.3520 | 1.7069 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
114.575 |
|
C1 |
N3 |
H6 |
121.605 |
C1 |
N4 |
H7 |
114.575 |
|
C1 |
N4 |
H8 |
121.605 |
O2 |
C1 |
N3 |
122.571 |
|
O2 |
C1 |
N4 |
122.571 |
N3 |
C1 |
N4 |
114.743 |
|
H5 |
N3 |
H6 |
116.151 |
H7 |
N4 |
H8 |
116.151 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.618 |
|
|
|
2 |
O |
-0.406 |
|
|
|
3 |
N |
-0.806 |
|
|
|
4 |
N |
-0.806 |
|
|
|
5 |
H |
0.364 |
|
|
|
6 |
H |
0.337 |
|
|
|
7 |
H |
0.364 |
|
|
|
8 |
H |
0.337 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.604 |
-4.064 |
0.000 |
4.369 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.383 |
1.678 |
0.000 |
y |
1.678 |
-23.990 |
0.000 |
z |
0.000 |
0.000 |
-16.791 |
|
Traceless |
| x | y | z |
x |
-4.993 |
1.678 |
0.000 |
y |
1.678 |
-2.903 |
0.000 |
z |
0.000 |
0.000 |
7.895 |
|
Polar |
3z2-r2 | 15.791 |
x2-y2 | -1.393 |
xy | 1.678 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.363 |
0.114 |
0.000 |
y |
0.114 |
4.887 |
0.000 |
z |
0.000 |
0.000 |
4.765 |
<r2> (average value of r
2) Å
2
<r2> |
68.409 |
(<r2>)1/2 |
8.271 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -225.236608 |
Energy at 298.15K | |
HF Energy | -225.236608 |
Nuclear repulsion energy | 124.011700 |
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 B3PW91/6-311G*
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 |
3779 |
3638 |
34.04 |
|
|
|
2 |
A1 |
3650 |
3514 |
4.01 |
|
|
|
3 |
A1 |
1823 |
1755 |
477.97 |
|
|
|
4 |
A1 |
1662 |
1600 |
0.57 |
|
|
|
5 |
A1 |
1160 |
1117 |
0.23 |
|
|
|
6 |
A1 |
978 |
942 |
7.73 |
|
|
|
7 |
A1 |
479 |
461 |
3.53 |
|
|
|
8 |
A2 |
372 |
358 |
0.00 |
|
|
|
9 |
A2 |
399i |
384i |
0.00 |
|
|
|
10 |
B1 |
785 |
756 |
11.11 |
|
|
|
11 |
B1 |
574 |
553 |
10.57 |
|
|
|
12 |
B1 |
251i |
241i |
561.23 |
|
|
|
13 |
B2 |
3777 |
3636 |
36.35 |
|
|
|
14 |
B2 |
3641 |
3505 |
47.52 |
|
|
|
15 |
B2 |
1654 |
1593 |
289.26 |
|
|
|
16 |
B2 |
1442 |
1388 |
231.54 |
|
|
|
17 |
B2 |
995 |
958 |
12.83 |
|
|
|
18 |
B2 |
565 |
544 |
14.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13343.4 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 12845.7 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 B3PW91/6-311G*
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 |
1.358 |
N3 |
0.000 |
1.157 |
-0.596 |
N4 |
0.000 |
-1.157 |
-0.596 |
H5 |
0.000 |
2.021 |
-0.086 |
H6 |
0.000 |
1.190 |
-1.599 |
H7 |
0.000 |
-2.021 |
-0.086 |
H8 |
0.000 |
-1.190 |
-1.599 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2159 | 1.3726 | 1.3726 | 2.0336 | 2.1092 | 2.0336 | 2.1092 |
O2 | 1.2159 | | 2.2713 | 2.2713 | 2.4839 | 3.1878 | 2.4839 | 3.1878 | N3 | 1.3726 | 2.2713 | | 2.3138 | 1.0032 | 1.0033 | 3.2183 | 2.5521 | N4 | 1.3726 | 2.2713 | 2.3138 | | 3.2183 | 2.5521 | 1.0032 | 1.0033 | H5 | 2.0336 | 2.4839 | 1.0032 | 3.2183 | | 1.7260 | 4.0415 | 3.5493 | H6 | 2.1092 | 3.1878 | 1.0033 | 2.5521 | 1.7260 | | 3.5493 | 2.3799 | H7 | 2.0336 | 2.4839 | 3.2183 | 1.0032 | 4.0415 | 3.5493 | | 1.7260 | H8 | 2.1092 | 3.1878 | 2.5521 | 1.0033 | 3.5493 | 2.3799 | 1.7260 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.880 |
|
C1 |
N3 |
H6 |
124.445 |
C1 |
N4 |
H7 |
116.880 |
|
C1 |
N4 |
H8 |
124.445 |
O2 |
C1 |
N3 |
122.556 |
|
O2 |
C1 |
N4 |
122.556 |
N3 |
C1 |
N4 |
114.887 |
|
H5 |
N3 |
H6 |
118.675 |
H7 |
N4 |
H8 |
118.675 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.671 |
|
|
|
2 |
O |
-0.419 |
|
|
|
3 |
N |
-0.845 |
|
|
|
4 |
N |
-0.845 |
|
|
|
5 |
H |
0.372 |
|
|
|
6 |
H |
0.347 |
|
|
|
7 |
H |
0.372 |
|
|
|
8 |
H |
0.347 |
|
|
|
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 |
-4.377 |
4.377 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.736 |
0.000 |
0.000 |
y |
0.000 |
-16.074 |
0.000 |
z |
0.000 |
0.000 |
-23.494 |
|
Traceless |
| x | y | z |
x |
-5.951 |
0.000 |
0.000 |
y |
0.000 |
8.541 |
0.000 |
z |
0.000 |
0.000 |
-2.589 |
|
Polar |
3z2-r2 | -5.179 |
x2-y2 | -9.661 |
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 |
2.284 |
0.000 |
0.000 |
y |
0.000 |
4.742 |
0.000 |
z |
0.000 |
0.000 |
4.829 |
<r2> (average value of r
2) Å
2
<r2> |
68.320 |
(<r2>)1/2 |
8.266 |