Jump to
S1C2
S1C3
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -207.948121 |
| Energy at 298.15K | -207.954331 |
| HF Energy | -207.948121 |
| Nuclear repulsion energy | 118.676993 |
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 B1B95/3-21G
| 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' |
3592 |
3436 |
23.74 |
|
|
|
| 2 |
A' |
3150 |
3014 |
15.38 |
|
|
|
| 3 |
A' |
3062 |
2930 |
41.67 |
|
|
|
| 4 |
A' |
2964 |
2836 |
93.97 |
|
|
|
| 5 |
A' |
1792 |
1714 |
336.02 |
|
|
|
| 6 |
A' |
1591 |
1522 |
16.45 |
|
|
|
| 7 |
A' |
1508 |
1443 |
3.25 |
|
|
|
| 8 |
A' |
1493 |
1428 |
4.75 |
|
|
|
| 9 |
A' |
1447 |
1384 |
16.50 |
|
|
|
| 10 |
A' |
1320 |
1263 |
85.81 |
|
|
|
| 11 |
A' |
1166 |
1115 |
44.48 |
|
|
|
| 12 |
A' |
1023 |
978 |
50.02 |
|
|
|
| 13 |
A' |
617 |
590 |
16.49 |
|
|
|
| 14 |
A' |
352 |
337 |
7.00 |
|
|
|
| 15 |
A" |
3121 |
2985 |
32.29 |
|
|
|
| 16 |
A" |
1553 |
1485 |
9.40 |
|
|
|
| 17 |
A" |
1165 |
1115 |
0.69 |
|
|
|
| 18 |
A" |
1089 |
1042 |
0.07 |
|
|
|
| 19 |
A" |
709 |
678 |
185.92 |
|
|
|
| 20 |
A" |
224 |
214 |
1.27 |
|
|
|
| 21 |
A" |
134 |
128 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16534.7 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15818.7 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.295 |
-0.745 |
0.000 |
| O2 |
1.425 |
-1.229 |
0.000 |
| N3 |
0.000 |
0.585 |
0.000 |
| C4 |
-1.359 |
1.107 |
0.000 |
| H5 |
-0.629 |
-1.348 |
0.000 |
| H6 |
0.780 |
1.232 |
0.000 |
| H7 |
-2.049 |
0.260 |
0.000 |
| H8 |
-1.559 |
1.711 |
0.889 |
| H9 |
-1.559 |
1.711 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2297 | 1.3616 | 2.4821 | 1.1030 | 2.0348 | 2.5495 | 3.2025 | 3.2025 |
O2 | 1.2297 | | 2.3065 | 3.6338 | 2.0574 | 2.5436 | 3.7792 | 4.2824 | 4.2824 | N3 | 1.3616 | 2.3065 | | 1.4556 | 2.0321 | 1.0133 | 2.0743 | 2.1190 | 2.1190 | C4 | 2.4821 | 3.6338 | 1.4556 | | 2.5604 | 2.1424 | 1.0924 | 1.0935 | 1.0935 | H5 | 1.1030 | 2.0574 | 2.0321 | 2.5604 | | 2.9388 | 2.1445 | 3.3180 | 3.3180 | H6 | 2.0348 | 2.5436 | 1.0133 | 2.1424 | 2.9388 | | 2.9910 | 2.5481 | 2.5481 | H7 | 2.5495 | 3.7792 | 2.0743 | 1.0924 | 2.1445 | 2.9910 | | 1.7706 | 1.7706 | H8 | 3.2025 | 4.2824 | 2.1190 | 1.0935 | 3.3180 | 2.5481 | 1.7706 | | 1.7783 | H9 | 3.2025 | 4.2824 | 2.1190 | 1.0935 | 3.3180 | 2.5481 | 1.7706 | 1.7783 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
123.513 |
|
C1 |
N3 |
H6 |
117.166 |
| O2 |
C1 |
N3 |
125.697 |
|
O2 |
C1 |
H5 |
123.666 |
| N3 |
C1 |
H5 |
110.637 |
|
N3 |
C4 |
H7 |
108.153 |
| N3 |
C4 |
H8 |
111.675 |
|
N3 |
C4 |
H9 |
111.675 |
| C4 |
N3 |
H6 |
119.321 |
|
H7 |
C4 |
H8 |
108.202 |
| H7 |
C4 |
H9 |
108.202 |
|
H8 |
C4 |
H9 |
108.813 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.444 |
|
|
|
| 2 |
O |
-0.494 |
|
|
|
| 3 |
N |
-0.710 |
|
|
|
| 4 |
C |
-0.422 |
|
|
|
| 5 |
H |
0.162 |
|
|
|
| 6 |
H |
0.338 |
|
|
|
| 7 |
H |
0.229 |
|
|
|
| 8 |
H |
0.227 |
|
|
|
| 9 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.943 |
2.763 |
0.000 |
4.036 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.742 |
3.818 |
0.000 |
| y |
3.818 |
-23.937 |
0.000 |
| z |
0.000 |
0.000 |
-24.511 |
|
| Traceless |
| | x | y | z |
| x |
-1.518 |
3.818 |
0.000 |
| y |
3.818 |
1.189 |
0.000 |
| z |
0.000 |
0.000 |
0.329 |
|
| Polar |
| 3z2-r2 | 0.657 |
| x2-y2 | -1.805 |
| xy | 3.818 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.967 |
-1.030 |
0.000 |
| y |
-1.030 |
5.013 |
0.000 |
| z |
0.000 |
0.000 |
2.444 |
<r2> (average value of r
2) Å
2
| <r2> |
89.339 |
| (<r2>)1/2 |
9.452 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -207.948121 |
| Energy at 298.15K | -207.954331 |
| HF Energy | -207.948121 |
| Nuclear repulsion energy | 118.676993 |
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 B1B95/3-21G
Geometric Data calculated at B1B95/3-21G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -207.950995 |
| Energy at 298.15K | -207.957368 |
| HF Energy | -207.950995 |
| Nuclear repulsion energy | 121.306413 |
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 B1B95/3-21G
| 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 |
3622 |
3466 |
28.71 |
|
|
|
| 2 |
A |
3180 |
3043 |
0.29 |
|
|
|
| 3 |
A |
3134 |
2999 |
32.65 |
|
|
|
| 4 |
A |
3072 |
2939 |
35.25 |
|
|
|
| 5 |
A |
3004 |
2874 |
113.82 |
|
|
|
| 6 |
A |
1762 |
1686 |
194.60 |
|
|
|
| 7 |
A |
1589 |
1520 |
45.04 |
|
|
|
| 8 |
A |
1574 |
1505 |
12.25 |
|
|
|
| 9 |
A |
1528 |
1461 |
85.31 |
|
|
|
| 10 |
A |
1469 |
1406 |
32.72 |
|
|
|
| 11 |
A |
1435 |
1373 |
5.01 |
|
|
|
| 12 |
A |
1225 |
1172 |
68.33 |
|
|
|
| 13 |
A |
1182 |
1131 |
52.46 |
|
|
|
| 14 |
A |
1168 |
1117 |
1.06 |
|
|
|
| 15 |
A |
1071 |
1024 |
1.62 |
|
|
|
| 16 |
A |
972 |
930 |
14.99 |
|
|
|
| 17 |
A |
795 |
760 |
0.00 |
|
|
|
| 18 |
A |
590 |
564 |
117.70 |
|
|
|
| 19 |
A |
356 |
341 |
61.57 |
|
|
|
| 20 |
A |
330 |
316 |
16.27 |
|
|
|
| 21 |
A |
148 |
142 |
0.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16602.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15883.6 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.859 |
0.447 |
0.001 |
| O2 |
1.364 |
-0.678 |
0.001 |
| N3 |
-0.479 |
0.675 |
-0.012 |
| C4 |
-1.402 |
-0.456 |
0.003 |
| H5 |
1.439 |
1.381 |
0.010 |
| H6 |
-0.833 |
1.620 |
0.047 |
| H7 |
-2.405 |
-0.104 |
-0.236 |
| H8 |
-1.088 |
-1.188 |
-0.743 |
| H9 |
-1.415 |
-0.952 |
0.977 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2334 | 1.3570 | 2.4344 | 1.1000 | 2.0591 | 3.3181 | 2.6487 | 2.8428 |
O2 | 1.2334 | | 2.2863 | 2.7750 | 2.0611 | 3.1796 | 3.8197 | 2.6124 | 2.9584 | N3 | 1.3570 | 2.2863 | | 1.4598 | 2.0439 | 1.0108 | 2.0893 | 2.0918 | 2.1216 | C4 | 2.4344 | 2.7750 | 1.4598 | | 3.3833 | 2.1528 | 1.0892 | 1.0910 | 1.0937 | H5 | 1.1000 | 2.0611 | 2.0439 | 3.3833 | | 2.2846 | 4.1279 | 3.6816 | 3.8112 | H6 | 2.0591 | 3.1796 | 1.0108 | 2.1528 | 2.2846 | | 2.3497 | 2.9279 | 2.7962 | H7 | 3.3181 | 3.8197 | 2.0893 | 1.0892 | 4.1279 | 2.3497 | | 1.7797 | 1.7806 | H8 | 2.6487 | 2.6124 | 2.0918 | 1.0910 | 3.6816 | 2.9279 | 1.7797 | | 1.7667 | H9 | 2.8428 | 2.9584 | 2.1216 | 1.0937 | 3.8112 | 2.7962 | 1.7806 | 1.7667 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
119.551 |
|
C1 |
N3 |
H6 |
120.115 |
| O2 |
C1 |
N3 |
123.849 |
|
O2 |
C1 |
H5 |
123.987 |
| N3 |
C1 |
H5 |
112.164 |
|
N3 |
C4 |
H7 |
109.240 |
| N3 |
C4 |
H8 |
109.330 |
|
N3 |
C4 |
H9 |
111.576 |
| C4 |
N3 |
H6 |
120.138 |
|
H7 |
C4 |
H8 |
109.424 |
| H7 |
C4 |
H9 |
109.313 |
|
H8 |
C4 |
H9 |
107.928 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.431 |
|
|
|
| 2 |
O |
-0.494 |
|
|
|
| 3 |
N |
-0.707 |
|
|
|
| 4 |
C |
-0.440 |
|
|
|
| 5 |
H |
0.180 |
|
|
|
| 6 |
H |
0.330 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.261 |
|
|
|
| 9 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.735 |
2.543 |
-0.001 |
3.734 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.945 |
2.551 |
0.001 |
| y |
2.551 |
-21.666 |
-0.001 |
| z |
0.001 |
-0.001 |
-24.520 |
|
| Traceless |
| | x | y | z |
| x |
-1.852 |
2.551 |
0.001 |
| y |
2.551 |
3.067 |
-0.001 |
| z |
0.001 |
-0.001 |
-1.215 |
|
| Polar |
| 3z2-r2 | -2.430 |
| x2-y2 | -3.280 |
| xy | 2.551 |
| xz | 0.001 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.361 |
-0.097 |
-0.000 |
| y |
-0.097 |
4.389 |
-0.000 |
| z |
-0.000 |
-0.000 |
2.441 |
<r2> (average value of r
2) Å
2
| <r2> |
77.438 |
| (<r2>)1/2 |
8.800 |