Jump to
S1C2
S1C3
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -208.123639 |
| Energy at 298.15K | -208.129729 |
| HF Energy | -208.123639 |
| Nuclear repulsion energy | 119.326018 |
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 LSDA/6-31+G**
| 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' |
3518 |
3465 |
30.55 |
|
|
|
| 2 |
A' |
3066 |
3020 |
7.31 |
|
|
|
| 3 |
A' |
2969 |
2924 |
47.16 |
|
|
|
| 4 |
A' |
2852 |
2810 |
89.28 |
|
|
|
| 5 |
A' |
1794 |
1767 |
514.28 |
|
|
|
| 6 |
A' |
1481 |
1459 |
33.31 |
|
|
|
| 7 |
A' |
1431 |
1410 |
11.77 |
|
|
|
| 8 |
A' |
1398 |
1377 |
6.61 |
|
|
|
| 9 |
A' |
1326 |
1306 |
17.69 |
|
|
|
| 10 |
A' |
1279 |
1260 |
46.32 |
|
|
|
| 11 |
A' |
1156 |
1138 |
14.55 |
|
|
|
| 12 |
A' |
994 |
979 |
45.70 |
|
|
|
| 13 |
A' |
608 |
599 |
15.49 |
|
|
|
| 14 |
A' |
336 |
331 |
8.36 |
|
|
|
| 15 |
A" |
3038 |
2993 |
14.15 |
|
|
|
| 16 |
A" |
1416 |
1395 |
10.51 |
|
|
|
| 17 |
A" |
1102 |
1085 |
0.00 |
|
|
|
| 18 |
A" |
981 |
966 |
3.61 |
|
|
|
| 19 |
A" |
629 |
619 |
122.52 |
|
|
|
| 20 |
A" |
224 |
220 |
0.58 |
|
|
|
| 21 |
A" |
134 |
132 |
0.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15865.1 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 15627.2 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 LSDA/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.276 |
-0.750 |
0.000 |
| O2 |
1.399 |
-1.231 |
0.000 |
| N3 |
0.000 |
0.573 |
0.000 |
| C4 |
-1.322 |
1.124 |
0.000 |
| H5 |
-0.656 |
-1.374 |
0.000 |
| H6 |
0.815 |
1.192 |
0.000 |
| H7 |
-2.045 |
0.291 |
0.000 |
| H8 |
-1.516 |
1.738 |
0.897 |
| H9 |
-1.516 |
1.738 |
-0.897 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2214 | 1.3514 | 2.4629 | 1.1222 | 2.0147 | 2.5443 | 3.1946 | 3.1946 |
O2 | 1.2214 | | 2.2830 | 3.5987 | 2.0602 | 2.4923 | 3.7657 | 4.2563 | 4.2563 | N3 | 1.3514 | 2.2830 | | 1.4323 | 2.0545 | 1.0229 | 2.0648 | 2.1117 | 2.1117 | C4 | 2.4629 | 3.5987 | 1.4323 | | 2.5850 | 2.1377 | 1.1033 | 1.1044 | 1.1044 | H5 | 1.1222 | 2.0602 | 2.0545 | 2.5850 | | 2.9572 | 2.1681 | 3.3507 | 3.3507 | H6 | 2.0147 | 2.4923 | 1.0229 | 2.1377 | 2.9572 | | 2.9985 | 2.5560 | 2.5560 | H7 | 2.5443 | 3.7657 | 2.0648 | 1.1033 | 2.1681 | 2.9985 | | 1.7834 | 1.7834 | H8 | 3.1946 | 4.2563 | 2.1117 | 1.1044 | 3.3507 | 2.5560 | 1.7834 | | 1.7947 | H9 | 3.1946 | 4.2563 | 2.1117 | 1.1044 | 3.3507 | 2.5560 | 1.7834 | 1.7947 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.423 |
|
C1 |
N3 |
H6 |
115.415 |
| O2 |
C1 |
N3 |
125.011 |
|
O2 |
C1 |
H5 |
123.006 |
| N3 |
C1 |
H5 |
111.983 |
|
N3 |
C4 |
H7 |
108.344 |
| N3 |
C4 |
H8 |
112.062 |
|
N3 |
C4 |
H9 |
112.062 |
| C4 |
N3 |
H6 |
120.162 |
|
H7 |
C4 |
H8 |
107.757 |
| H7 |
C4 |
H9 |
107.757 |
|
H8 |
C4 |
H9 |
108.678 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.180 |
|
|
|
| 2 |
O |
-0.462 |
|
|
|
| 3 |
N |
-0.263 |
|
|
|
| 4 |
C |
-0.483 |
|
|
|
| 5 |
H |
0.123 |
|
|
|
| 6 |
H |
0.330 |
|
|
|
| 7 |
H |
0.184 |
|
|
|
| 8 |
H |
0.196 |
|
|
|
| 9 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.189 |
3.031 |
0.000 |
4.400 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.133 |
4.228 |
0.000 |
| y |
4.228 |
-24.847 |
0.000 |
| z |
0.000 |
0.000 |
-25.377 |
|
| Traceless |
| | x | y | z |
| x |
-2.021 |
4.228 |
0.000 |
| y |
4.228 |
1.408 |
0.000 |
| z |
0.000 |
0.000 |
0.613 |
|
| Polar |
| 3z2-r2 | 1.226 |
| x2-y2 | -2.286 |
| xy | 4.228 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.657 |
-1.313 |
0.000 |
| y |
-1.313 |
6.602 |
0.000 |
| z |
0.000 |
0.000 |
3.971 |
<r2> (average value of r
2) Å
2
| <r2> |
89.001 |
| (<r2>)1/2 |
9.434 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -208.123639 |
| Energy at 298.15K | -208.129729 |
| HF Energy | -208.123639 |
| Nuclear repulsion energy | 119.326018 |
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 LSDA/6-31+G**
Geometric Data calculated at LSDA/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -208.125825 |
| Energy at 298.15K | -208.131927 |
| HF Energy | -208.125825 |
| Nuclear repulsion energy | 121.755124 |
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 LSDA/6-31+G**
| 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 |
3556 |
3503 |
28.93 |
|
|
|
| 2 |
A |
3082 |
3036 |
0.27 |
|
|
|
| 3 |
A |
3051 |
3005 |
14.30 |
|
|
|
| 4 |
A |
2976 |
2932 |
38.27 |
|
|
|
| 5 |
A |
2893 |
2850 |
104.02 |
|
|
|
| 6 |
A |
1779 |
1752 |
345.80 |
|
|
|
| 7 |
A |
1516 |
1493 |
98.77 |
|
|
|
| 8 |
A |
1435 |
1414 |
13.01 |
|
|
|
| 9 |
A |
1425 |
1404 |
17.37 |
|
|
|
| 10 |
A |
1367 |
1347 |
26.39 |
|
|
|
| 11 |
A |
1356 |
1336 |
4.65 |
|
|
|
| 12 |
A |
1208 |
1190 |
30.64 |
|
|
|
| 13 |
A |
1112 |
1095 |
23.98 |
|
|
|
| 14 |
A |
1103 |
1087 |
0.18 |
|
|
|
| 15 |
A |
986 |
971 |
29.53 |
|
|
|
| 16 |
A |
967 |
952 |
0.72 |
|
|
|
| 17 |
A |
752 |
741 |
0.12 |
|
|
|
| 18 |
A |
555 |
546 |
58.27 |
|
|
|
| 19 |
A |
308 |
303 |
64.42 |
|
|
|
| 20 |
A |
296 |
291 |
15.96 |
|
|
|
| 21 |
A |
99 |
97 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15910.2 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 15671.5 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 LSDA/6-31+G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.855 |
0.443 |
0.004 |
| O2 |
1.357 |
-0.674 |
-0.000 |
| N3 |
-0.476 |
0.660 |
-0.018 |
| C4 |
-1.399 |
-0.446 |
0.004 |
| H5 |
1.457 |
1.383 |
0.014 |
| H6 |
-0.817 |
1.618 |
0.053 |
| H7 |
-2.410 |
-0.080 |
-0.222 |
| H8 |
-1.096 |
-1.186 |
-0.754 |
| H9 |
-1.399 |
-0.946 |
0.988 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2247 | 1.3490 | 2.4230 | 1.1160 | 2.0446 | 3.3151 | 2.6524 | 2.8243 |
O2 | 1.2247 | | 2.2674 | 2.7655 | 2.0596 | 3.1599 | 3.8206 | 2.6169 | 2.9401 | N3 | 1.3490 | 2.2674 | | 1.4406 | 2.0637 | 1.0191 | 2.0813 | 2.0815 | 2.1079 | C4 | 2.4230 | 2.7655 | 1.4406 | | 3.3910 | 2.1443 | 1.0993 | 1.1016 | 1.1037 | H5 | 1.1160 | 2.0596 | 2.0637 | 3.3910 | | 2.2867 | 4.1414 | 3.7020 | 3.8112 | H6 | 2.0446 | 3.1599 | 1.0191 | 2.1443 | 2.2867 | | 2.3442 | 2.9305 | 2.7899 | H7 | 3.3151 | 3.8206 | 2.0813 | 1.0993 | 4.1414 | 2.3442 | | 1.7978 | 1.7997 | H8 | 2.6524 | 2.6169 | 2.0815 | 1.1016 | 3.7020 | 2.9305 | 1.7978 | | 1.7840 | H9 | 2.8243 | 2.9401 | 2.1079 | 1.1037 | 3.8112 | 2.7899 | 1.7997 | 1.7840 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
120.555 |
|
C1 |
N3 |
H6 |
118.740 |
| O2 |
C1 |
N3 |
123.447 |
|
O2 |
C1 |
H5 |
123.193 |
| N3 |
C1 |
H5 |
113.356 |
|
N3 |
C4 |
H7 |
109.324 |
| N3 |
C4 |
H8 |
109.201 |
|
N3 |
C4 |
H9 |
111.202 |
| C4 |
N3 |
H6 |
120.361 |
|
H7 |
C4 |
H8 |
109.540 |
| H7 |
C4 |
H9 |
109.564 |
|
H8 |
C4 |
H9 |
107.985 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.174 |
|
|
|
| 2 |
O |
-0.473 |
|
|
|
| 3 |
N |
-0.271 |
|
|
|
| 4 |
C |
-0.485 |
|
|
|
| 5 |
H |
0.129 |
|
|
|
| 6 |
H |
0.317 |
|
|
|
| 7 |
H |
0.190 |
|
|
|
| 8 |
H |
0.229 |
|
|
|
| 9 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.098 |
2.689 |
-0.002 |
4.103 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.104 |
2.664 |
0.001 |
| y |
2.664 |
-22.684 |
-0.003 |
| z |
0.001 |
-0.003 |
-25.465 |
|
| Traceless |
| | x | y | z |
| x |
-2.029 |
2.664 |
0.001 |
| y |
2.664 |
3.101 |
-0.003 |
| z |
0.001 |
-0.003 |
-1.072 |
|
| Polar |
| 3z2-r2 | -2.143 |
| x2-y2 | -3.420 |
| xy | 2.664 |
| xz | 0.001 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.114 |
-0.190 |
0.000 |
| y |
-0.190 |
5.896 |
0.000 |
| z |
0.000 |
0.000 |
4.043 |
<r2> (average value of r
2) Å
2
| <r2> |
77.891 |
| (<r2>)1/2 |
8.826 |