Jump to
S1C2
S1C3
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -168.034597 |
| Energy at 298.15K | -168.038526 |
| HF Energy | -168.034597 |
| Nuclear repulsion energy | 70.043431 |
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/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' |
3436 |
3374 |
13.69 |
|
|
|
| 2 |
A' |
3359 |
3299 |
6.34 |
|
|
|
| 3 |
A' |
2879 |
2827 |
91.70 |
|
|
|
| 4 |
A' |
1772 |
1741 |
129.97 |
|
|
|
| 5 |
A' |
1389 |
1364 |
4.88 |
|
|
|
| 6 |
A' |
1237 |
1214 |
151.53 |
|
|
|
| 7 |
A' |
1157 |
1136 |
18.63 |
|
|
|
| 8 |
A' |
951 |
934 |
327.71 |
|
|
|
| 9 |
A' |
619 |
607 |
4.02 |
|
|
|
| 10 |
A" |
1038 |
1019 |
1.06 |
|
|
|
| 11 |
A" |
800 |
785 |
94.21 |
|
|
|
| 12 |
A" |
383 |
376 |
71.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9508.9 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 9337.7 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 LSDA/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.387 |
0.000 |
| O2 |
-1.004 |
-0.548 |
0.000 |
| N3 |
1.198 |
-0.007 |
0.000 |
| H4 |
-0.369 |
1.436 |
0.000 |
| H5 |
-1.891 |
-0.084 |
0.000 |
| H6 |
1.904 |
0.752 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3715 | 1.2612 | 1.1123 | 1.9487 | 1.9384 |
O2 | 1.3715 | | 2.2676 | 2.0826 | 1.0010 | 3.1847 | N3 | 1.2612 | 2.2676 | | 2.1304 | 3.0902 | 1.0357 | H4 | 1.1123 | 2.0826 | 2.1304 | | 2.1506 | 2.3741 | H5 | 1.9487 | 1.0010 | 3.0902 | 2.1506 | | 3.8857 | H6 | 1.9384 | 3.1847 | 1.0357 | 2.3741 | 3.8857 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
109.450 |
|
C1 |
N3 |
H6 |
114.765 |
| O2 |
C1 |
N3 |
118.873 |
|
O2 |
C1 |
H4 |
113.550 |
| N3 |
C1 |
H4 |
127.577 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.211 |
|
|
|
| 2 |
O |
-0.487 |
|
|
|
| 3 |
N |
-0.528 |
|
|
|
| 4 |
H |
0.164 |
|
|
|
| 5 |
H |
0.366 |
|
|
|
| 6 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.851 |
3.246 |
0.000 |
3.736 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.397 |
1.474 |
0.000 |
| y |
1.474 |
-18.090 |
0.000 |
| z |
0.000 |
0.000 |
-18.419 |
|
| Traceless |
| | x | y | z |
| x |
5.857 |
1.474 |
0.000 |
| y |
1.474 |
-2.682 |
0.000 |
| z |
0.000 |
0.000 |
-3.175 |
|
| Polar |
| 3z2-r2 | -6.350 |
| x2-y2 | 5.693 |
| xy | 1.474 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.886 |
0.052 |
0.000 |
| y |
0.052 |
2.577 |
0.000 |
| z |
0.000 |
0.000 |
0.964 |
<r2> (average value of r
2) Å
2
| <r2> |
41.563 |
| (<r2>)1/2 |
6.447 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -168.048910 |
| Energy at 298.15K | -168.053038 |
| HF Energy | -168.048910 |
| Nuclear repulsion energy | 70.432576 |
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/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' |
3358 |
3298 |
4.12 |
|
|
|
| 2 |
A' |
3315 |
3256 |
4.78 |
|
|
|
| 3 |
A' |
3025 |
2971 |
39.73 |
|
|
|
| 4 |
A' |
1714 |
1683 |
148.43 |
|
|
|
| 5 |
A' |
1360 |
1335 |
6.33 |
|
|
|
| 6 |
A' |
1343 |
1319 |
34.57 |
|
|
|
| 7 |
A' |
1124 |
1104 |
110.88 |
|
|
|
| 8 |
A' |
994 |
976 |
183.45 |
|
|
|
| 9 |
A' |
559 |
549 |
60.47 |
|
|
|
| 10 |
A" |
1042 |
1024 |
6.10 |
|
|
|
| 11 |
A" |
800 |
786 |
21.60 |
|
|
|
| 12 |
A" |
702 |
689 |
243.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9668.6 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 9494.6 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 LSDA/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.433 |
0.000 |
| O2 |
-1.118 |
-0.343 |
0.000 |
| N3 |
1.155 |
-0.088 |
0.000 |
| H4 |
-0.301 |
1.492 |
0.000 |
| H5 |
-0.784 |
-1.299 |
0.000 |
| H6 |
1.950 |
0.575 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3611 | 1.2668 | 1.1017 | 1.9009 | 1.9550 |
O2 | 1.3611 | | 2.2874 | 2.0091 | 1.0129 | 3.2027 | N3 | 1.2668 | 2.2874 | | 2.1491 | 2.2856 | 1.0354 | H4 | 1.1017 | 2.0091 | 2.1491 | | 2.8329 | 2.4310 | H5 | 1.9009 | 1.0129 | 2.2856 | 2.8329 | | 3.3144 | H6 | 1.9550 | 3.2027 | 1.0354 | 2.4310 | 3.3144 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
105.458 |
|
C1 |
N3 |
H6 |
115.890 |
| O2 |
C1 |
N3 |
120.971 |
|
O2 |
C1 |
H4 |
108.869 |
| N3 |
C1 |
H4 |
130.160 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.205 |
|
|
|
| 2 |
O |
-0.494 |
|
|
|
| 3 |
N |
-0.569 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
| 5 |
H |
0.361 |
|
|
|
| 6 |
H |
0.278 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.552 |
0.809 |
0.000 |
0.979 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.608 |
3.327 |
0.000 |
| y |
3.327 |
-13.924 |
0.000 |
| z |
0.000 |
0.000 |
-18.422 |
|
| Traceless |
| | x | y | z |
| x |
-2.434 |
3.327 |
0.000 |
| y |
3.327 |
4.591 |
0.000 |
| z |
0.000 |
0.000 |
-2.156 |
|
| Polar |
| 3z2-r2 | -4.312 |
| x2-y2 | -4.683 |
| xy | 3.327 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.078 |
0.226 |
0.000 |
| y |
0.226 |
3.168 |
0.000 |
| z |
0.000 |
0.000 |
0.971 |
<r2> (average value of r
2) Å
2
| <r2> |
40.821 |
| (<r2>)1/2 |
6.389 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -168.043841 |
| Energy at 298.15K | -168.047902 |
| HF Energy | -168.043841 |
| Nuclear repulsion energy | 69.752192 |
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/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' |
3356 |
3295 |
1.92 |
|
|
|
| 2 |
A' |
3251 |
3193 |
10.15 |
|
|
|
| 3 |
A' |
3106 |
3050 |
8.70 |
|
|
|
| 4 |
A' |
1710 |
1679 |
152.67 |
|
|
|
| 5 |
A' |
1379 |
1355 |
0.05 |
|
|
|
| 6 |
A' |
1293 |
1270 |
10.91 |
|
|
|
| 7 |
A' |
1045 |
1026 |
328.76 |
|
|
|
| 8 |
A' |
1026 |
1007 |
46.86 |
|
|
|
| 9 |
A' |
562 |
552 |
35.75 |
|
|
|
| 10 |
A" |
1052 |
1033 |
90.40 |
|
|
|
| 11 |
A" |
829 |
814 |
51.12 |
|
|
|
| 12 |
A" |
568 |
558 |
102.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9588.7 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 9416.1 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.435 |
0.000 |
| O2 |
-1.117 |
-0.368 |
0.000 |
| N3 |
1.234 |
0.151 |
0.000 |
| H4 |
-0.331 |
1.480 |
0.000 |
| H5 |
-0.841 |
-1.337 |
0.000 |
| H6 |
1.471 |
-0.867 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3757 | 1.2665 | 1.0961 | 1.9615 | 1.9640 |
O2 | 1.3757 | | 2.4081 | 2.0077 | 1.0082 | 2.6357 | N3 | 1.2665 | 2.4081 | | 2.0534 | 2.5536 | 1.0449 | H4 | 1.0961 | 2.0077 | 2.0534 | | 2.8627 | 2.9586 | H5 | 1.9615 | 1.0082 | 2.5536 | 2.8627 | | 2.3589 | H6 | 1.9640 | 2.6357 | 1.0449 | 2.9586 | 2.3589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
109.775 |
|
C1 |
N3 |
H6 |
116.028 |
| O2 |
C1 |
N3 |
131.358 |
|
O2 |
C1 |
H4 |
108.098 |
| N3 |
C1 |
H4 |
120.543 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.157 |
|
|
|
| 2 |
O |
-0.483 |
|
|
|
| 3 |
N |
-0.525 |
|
|
|
| 4 |
H |
0.252 |
|
|
|
| 5 |
H |
0.348 |
|
|
|
| 6 |
H |
0.251 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.655 |
-2.344 |
0.000 |
2.434 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.394 |
-2.112 |
0.000 |
| y |
-2.112 |
-12.809 |
0.000 |
| z |
0.000 |
0.000 |
-18.467 |
|
| Traceless |
| | x | y | z |
| x |
-6.756 |
-2.112 |
0.000 |
| y |
-2.112 |
7.621 |
0.000 |
| z |
0.000 |
0.000 |
-0.866 |
|
| Polar |
| 3z2-r2 | -1.731 |
| x2-y2 | -9.585 |
| xy | -2.112 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.799 |
-0.135 |
0.000 |
| y |
-0.135 |
3.416 |
0.000 |
| z |
0.000 |
0.000 |
1.037 |
<r2> (average value of r
2) Å
2
| <r2> |
41.909 |
| (<r2>)1/2 |
6.474 |