Jump to
S1C2
S1C3
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.045897 |
| Energy at 298.15K | -208.052028 |
| HF Energy | -208.045897 |
| Nuclear repulsion energy | 120.673409 |
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 HF/daug-cc-pVTZ
| 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' |
3841 |
3474 |
41.30 |
|
|
|
| 2 |
A' |
3251 |
2941 |
27.58 |
|
|
|
| 3 |
A' |
3169 |
2866 |
66.54 |
|
|
|
| 4 |
A' |
3142 |
2842 |
56.66 |
|
|
|
| 5 |
A' |
1936 |
1752 |
689.50 |
|
|
|
| 6 |
A' |
1659 |
1501 |
24.51 |
|
|
|
| 7 |
A' |
1621 |
1466 |
7.25 |
|
|
|
| 8 |
A' |
1600 |
1447 |
7.22 |
|
|
|
| 9 |
A' |
1522 |
1377 |
9.40 |
|
|
|
| 10 |
A' |
1398 |
1265 |
193.32 |
|
|
|
| 11 |
A' |
1257 |
1137 |
51.70 |
|
|
|
| 12 |
A' |
1085 |
981 |
46.54 |
|
|
|
| 13 |
A' |
658 |
595 |
16.53 |
|
|
|
| 14 |
A' |
374 |
338 |
9.62 |
|
|
|
| 15 |
A" |
3215 |
2909 |
37.51 |
|
|
|
| 16 |
A" |
1604 |
1451 |
5.63 |
|
|
|
| 17 |
A" |
1250 |
1131 |
1.66 |
|
|
|
| 18 |
A" |
1173 |
1061 |
0.02 |
|
|
|
| 19 |
A" |
641 |
580 |
139.26 |
|
|
|
| 20 |
A" |
195 |
177 |
0.14 |
|
|
|
| 21 |
A" |
77 |
70 |
0.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17333.3 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 15679.7 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 HF/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.291 |
-0.750 |
0.000 |
| O2 |
1.391 |
-1.205 |
0.000 |
| N3 |
0.000 |
0.561 |
0.000 |
| C4 |
-1.332 |
1.112 |
0.000 |
| H5 |
-0.596 |
-1.385 |
0.000 |
| H6 |
0.779 |
1.177 |
0.000 |
| H7 |
-2.052 |
0.306 |
0.000 |
| H8 |
-1.507 |
1.719 |
0.880 |
| H9 |
-1.507 |
1.719 |
-0.880 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1904 | 1.3428 | 2.4698 | 1.0915 | 1.9878 | 2.5697 | 3.1782 | 3.1782 |
O2 | 1.1904 | | 2.2485 | 3.5754 | 1.9951 | 2.4602 | 3.7597 | 4.2100 | 4.2100 | N3 | 1.3428 | 2.2485 | | 1.4411 | 2.0358 | 0.9930 | 2.0674 | 2.0942 | 2.0942 | C4 | 2.4698 | 3.5754 | 1.4411 | | 2.6036 | 2.1114 | 1.0807 | 1.0829 | 1.0829 | H5 | 1.0915 | 1.9951 | 2.0358 | 2.6036 | | 2.9083 | 2.2316 | 3.3526 | 3.3526 | H6 | 1.9878 | 2.4602 | 0.9930 | 2.1114 | 2.9083 | | 2.9613 | 2.5085 | 2.5085 | H7 | 2.5697 | 3.7597 | 2.0674 | 1.0807 | 2.2316 | 2.9613 | | 1.7508 | 1.7508 | H8 | 3.1782 | 4.2100 | 2.0942 | 1.0829 | 3.3526 | 2.5085 | 1.7508 | | 1.7593 | H9 | 3.1782 | 4.2100 | 2.0942 | 1.0829 | 3.3526 | 2.5085 | 1.7508 | 1.7593 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.000 |
|
C1 |
N3 |
H6 |
115.831 |
| O2 |
C1 |
N3 |
125.035 |
|
O2 |
C1 |
H5 |
121.864 |
| N3 |
C1 |
H5 |
113.101 |
|
N3 |
C4 |
H7 |
109.297 |
| N3 |
C4 |
H8 |
111.347 |
|
N3 |
C4 |
H9 |
111.347 |
| C4 |
N3 |
H6 |
119.169 |
|
H7 |
C4 |
H8 |
108.043 |
| H7 |
C4 |
H9 |
108.043 |
|
H8 |
C4 |
H9 |
108.652 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.298 |
|
|
|
| 2 |
O |
-1.296 |
|
|
|
| 3 |
N |
-0.558 |
|
|
|
| 4 |
C |
-1.621 |
|
|
|
| 5 |
H |
1.434 |
|
|
|
| 6 |
H |
0.377 |
|
|
|
| 7 |
H |
0.663 |
|
|
|
| 8 |
H |
0.649 |
|
|
|
| 9 |
H |
0.649 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.471 |
2.753 |
0.000 |
4.430 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.332 |
4.646 |
0.000 |
| y |
4.646 |
-24.501 |
0.000 |
| z |
0.000 |
0.000 |
-24.811 |
|
| Traceless |
| | x | y | z |
| x |
-2.676 |
4.646 |
0.000 |
| y |
4.646 |
1.570 |
0.000 |
| z |
0.000 |
0.000 |
1.106 |
|
| Polar |
| 3z2-r2 | 2.212 |
| x2-y2 | -2.831 |
| xy | 4.646 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.990 |
-0.967 |
0.000 |
| y |
-0.967 |
5.838 |
0.000 |
| z |
0.000 |
0.000 |
4.065 |
<r2> (average value of r
2) Å
2
| <r2> |
87.774 |
| (<r2>)1/2 |
9.369 |
Jump to
S1C1
S1C3
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.045897 |
| Energy at 298.15K | -208.052028 |
| HF Energy | -208.045897 |
| Nuclear repulsion energy | 120.673409 |
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 HF/daug-cc-pVTZ
Geometric Data calculated at HF/daug-cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -208.047830 |
| Energy at 298.15K | -208.053853 |
| HF Energy | -208.047830 |
| Nuclear repulsion energy | 122.928363 |
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 HF/daug-cc-pVTZ
| 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 |
3892 |
3520 |
47.90 |
|
|
|
| 2 |
A |
3259 |
2948 |
26.03 |
|
|
|
| 3 |
A |
3241 |
2931 |
28.20 |
|
|
|
| 4 |
A |
3182 |
2879 |
34.03 |
|
|
|
| 5 |
A |
3146 |
2846 |
97.37 |
|
|
|
| 6 |
A |
1928 |
1744 |
459.01 |
|
|
|
| 7 |
A |
1674 |
1514 |
207.02 |
|
|
|
| 8 |
A |
1630 |
1474 |
9.10 |
|
|
|
| 9 |
A |
1599 |
1447 |
7.91 |
|
|
|
| 10 |
A |
1585 |
1434 |
16.16 |
|
|
|
| 11 |
A |
1542 |
1395 |
12.15 |
|
|
|
| 12 |
A |
1332 |
1205 |
95.32 |
|
|
|
| 13 |
A |
1272 |
1150 |
11.58 |
|
|
|
| 14 |
A |
1255 |
1135 |
0.13 |
|
|
|
| 15 |
A |
1169 |
1058 |
1.37 |
|
|
|
| 16 |
A |
1018 |
921 |
19.81 |
|
|
|
| 17 |
A |
833 |
754 |
9.45 |
|
|
|
| 18 |
A |
498 |
450 |
16.99 |
|
|
|
| 19 |
A |
289 |
262 |
12.73 |
|
|
|
| 20 |
A |
247 |
224 |
96.66 |
|
|
|
| 21 |
A |
50 |
45 |
10.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17319.8 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 15667.5 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 HF/daug-cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.864 |
0.418 |
0.000 |
| O2 |
1.368 |
-0.661 |
-0.000 |
| N3 |
-0.458 |
0.646 |
0.000 |
| C4 |
-1.427 |
-0.428 |
-0.000 |
| H5 |
1.455 |
1.335 |
-0.000 |
| H6 |
-0.770 |
1.585 |
-0.000 |
| H7 |
-2.418 |
0.001 |
0.001 |
| H8 |
-1.314 |
-1.050 |
-0.877 |
| H9 |
-1.312 |
-1.051 |
0.876 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.1912 | 1.3411 | 2.4418 | 1.0912 | 2.0073 | 3.3084 | 2.7685 | 2.7680 |
O2 | 1.1912 | | 2.2457 | 2.8050 | 1.9982 | 3.1007 | 3.8440 | 2.8481 | 2.8470 | N3 | 1.3411 | 2.2457 | | 1.4464 | 2.0330 | 0.9890 | 2.0638 | 2.0924 | 2.0925 | C4 | 2.4418 | 2.8050 | 1.4464 | | 3.3783 | 2.1169 | 1.0801 | 1.0813 | 1.0813 | H5 | 1.0912 | 1.9982 | 2.0330 | 3.3783 | | 2.2386 | 4.0964 | 3.7579 | 3.7578 | H6 | 2.0073 | 3.1007 | 0.9890 | 2.1169 | 2.2386 | | 2.2858 | 2.8294 | 2.8303 | H7 | 3.3084 | 3.8440 | 2.0638 | 1.0801 | 4.0964 | 2.2858 | | 1.7597 | 1.7597 | H8 | 2.7685 | 2.8481 | 2.0924 | 1.0813 | 3.7579 | 2.8294 | 1.7597 | | 1.7527 | H9 | 2.7680 | 2.8470 | 2.0925 | 1.0813 | 3.7578 | 2.8303 | 1.7597 | 1.7527 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
122.278 |
|
C1 |
N3 |
H6 |
118.178 |
| O2 |
C1 |
N3 |
124.849 |
|
O2 |
C1 |
H5 |
122.141 |
| N3 |
C1 |
H5 |
113.010 |
|
N3 |
C4 |
H7 |
108.674 |
| N3 |
C4 |
H8 |
110.918 |
|
N3 |
C4 |
H9 |
110.923 |
| C4 |
N3 |
H6 |
119.544 |
|
H7 |
C4 |
H8 |
109.001 |
| H7 |
C4 |
H9 |
109.003 |
|
H8 |
C4 |
H9 |
108.283 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.289 |
|
|
|
| 2 |
O |
-1.184 |
|
|
|
| 3 |
N |
-0.402 |
|
|
|
| 4 |
C |
-1.667 |
|
|
|
| 5 |
H |
1.352 |
|
|
|
| 6 |
H |
0.353 |
|
|
|
| 7 |
H |
0.603 |
|
|
|
| 8 |
H |
0.617 |
|
|
|
| 9 |
H |
0.617 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.916 |
2.965 |
-0.001 |
4.159 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.525 |
3.219 |
0.000 |
| y |
3.219 |
-22.616 |
-0.002 |
| z |
0.000 |
-0.002 |
-24.890 |
|
| Traceless |
| | x | y | z |
| x |
-1.772 |
3.219 |
0.000 |
| y |
3.219 |
2.592 |
-0.002 |
| z |
0.000 |
-0.002 |
-0.820 |
|
| Polar |
| 3z2-r2 | -1.640 |
| x2-y2 | -2.909 |
| xy | 3.219 |
| xz | 0.000 |
| yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.134 |
-0.105 |
0.000 |
| y |
-0.105 |
5.498 |
0.000 |
| z |
0.000 |
0.000 |
4.106 |
<r2> (average value of r
2) Å
2
| <r2> |
76.950 |
| (<r2>)1/2 |
8.772 |