Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -169.809683 |
| Energy at 298.15K | -169.813700 |
| HF Energy | -169.809683 |
| Nuclear repulsion energy | 71.174935 |
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 B1B95/6-31G(2df,p)
| 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' |
3910 |
3744 |
75.11 |
|
|
|
| 2 |
A' |
3578 |
3427 |
6.99 |
|
|
|
| 3 |
A' |
3052 |
2923 |
60.35 |
|
|
|
| 4 |
A' |
1808 |
1731 |
199.37 |
|
|
|
| 5 |
A' |
1432 |
1371 |
17.21 |
|
|
|
| 6 |
A' |
1344 |
1287 |
169.08 |
|
|
|
| 7 |
A' |
1204 |
1153 |
31.80 |
|
|
|
| 8 |
A' |
1077 |
1032 |
203.85 |
|
|
|
| 9 |
A' |
621 |
594 |
1.43 |
|
|
|
| 10 |
A" |
1054 |
1009 |
5.40 |
|
|
|
| 11 |
A" |
840 |
804 |
56.02 |
|
|
|
| 12 |
A" |
413 |
396 |
63.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10165.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 9735.8 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.371 |
0.000 |
| O2 |
-0.999 |
-0.527 |
0.000 |
| N3 |
1.193 |
-0.020 |
0.000 |
| H4 |
-0.338 |
1.414 |
0.000 |
| H5 |
-1.838 |
-0.066 |
0.000 |
| H6 |
1.817 |
0.779 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3435 | 1.2555 | 1.0966 | 1.8896 | 1.8627 |
O2 | 1.3435 | | 2.2503 | 2.0507 | 0.9575 | 3.1048 | N3 | 1.2555 | 2.2503 | | 2.0980 | 3.0319 | 1.0140 | H4 | 1.0966 | 2.0507 | 2.0980 | | 2.1075 | 2.2471 | H5 | 1.8896 | 0.9575 | 3.0319 | 2.1075 | | 3.7522 | H6 | 1.8627 | 3.1048 | 1.0140 | 2.2471 | 3.7522 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
109.264 |
|
C1 |
N3 |
H6 |
109.858 |
| O2 |
C1 |
N3 |
119.914 |
|
O2 |
C1 |
H4 |
113.987 |
| N3 |
C1 |
H4 |
126.099 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.135 |
|
|
|
| 2 |
O |
-0.362 |
|
|
|
| 3 |
N |
-0.433 |
|
|
|
| 4 |
H |
0.099 |
|
|
|
| 5 |
H |
0.318 |
|
|
|
| 6 |
H |
0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.066 |
2.956 |
0.000 |
3.607 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.652 |
1.122 |
0.000 |
| y |
1.122 |
-17.398 |
0.000 |
| z |
0.000 |
0.000 |
-18.295 |
|
| Traceless |
| | x | y | z |
| x |
4.195 |
1.122 |
0.000 |
| y |
1.122 |
-1.425 |
0.000 |
| z |
0.000 |
0.000 |
-2.770 |
|
| Polar |
| 3z2-r2 | -5.540 |
| x2-y2 | 3.746 |
| xy | 1.122 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.813 |
0.060 |
0.000 |
| y |
0.060 |
2.981 |
0.000 |
| z |
0.000 |
0.000 |
1.874 |
<r2> (average value of r
2) Å
2
| <r2> |
40.685 |
| (<r2>)1/2 |
6.379 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -169.818664 |
| Energy at 298.15K | -169.822832 |
| HF Energy | -169.818664 |
| Nuclear repulsion energy | 71.512902 |
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 B1B95/6-31G(2df,p)
| 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' |
3797 |
3636 |
47.96 |
|
|
|
| 2 |
A' |
3580 |
3428 |
6.58 |
|
|
|
| 3 |
A' |
3130 |
2998 |
34.36 |
|
|
|
| 4 |
A' |
1778 |
1703 |
255.26 |
|
|
|
| 5 |
A' |
1409 |
1349 |
29.71 |
|
|
|
| 6 |
A' |
1388 |
1330 |
0.96 |
|
|
|
| 7 |
A' |
1199 |
1148 |
118.04 |
|
|
|
| 8 |
A' |
1088 |
1042 |
150.33 |
|
|
|
| 9 |
A' |
587 |
562 |
49.99 |
|
|
|
| 10 |
A" |
1067 |
1022 |
0.00 |
|
|
|
| 11 |
A" |
844 |
808 |
24.40 |
|
|
|
| 12 |
A" |
643 |
616 |
168.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10254.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 9820.2 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.414 |
0.000 |
| O2 |
-1.107 |
-0.333 |
0.000 |
| N3 |
1.152 |
-0.095 |
0.000 |
| H4 |
-0.262 |
1.473 |
0.000 |
| H5 |
-0.810 |
-1.252 |
0.000 |
| H6 |
1.865 |
0.626 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3355 | 1.2593 | 1.0914 | 1.8519 | 1.8769 |
O2 | 1.3355 | | 2.2714 | 1.9942 | 0.9655 | 3.1227 | N3 | 1.2593 | 2.2714 | | 2.1117 | 2.2772 | 1.0138 | H4 | 1.0914 | 1.9942 | 2.1117 | | 2.7794 | 2.2899 | H5 | 1.8519 | 0.9655 | 2.2772 | 2.7794 | | 3.2677 | H6 | 1.8769 | 3.1227 | 1.0138 | 2.2899 | 3.2677 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
106.076 |
|
C1 |
N3 |
H6 |
110.860 |
| O2 |
C1 |
N3 |
122.152 |
|
O2 |
C1 |
H4 |
110.108 |
| N3 |
C1 |
H4 |
127.741 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.166 |
|
|
|
| 2 |
O |
-0.368 |
|
|
|
| 3 |
N |
-0.490 |
|
|
|
| 4 |
H |
0.127 |
|
|
|
| 5 |
H |
0.318 |
|
|
|
| 6 |
H |
0.246 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.054 |
0.877 |
0.000 |
0.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.887 |
3.061 |
0.000 |
| y |
3.061 |
-13.851 |
0.000 |
| z |
0.000 |
0.000 |
-18.279 |
|
| Traceless |
| | x | y | z |
| x |
-2.822 |
3.061 |
0.000 |
| y |
3.061 |
4.733 |
0.000 |
| z |
0.000 |
0.000 |
-1.911 |
|
| Polar |
| 3z2-r2 | -3.821 |
| x2-y2 | -5.037 |
| xy | 3.061 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.342 |
0.133 |
0.000 |
| y |
0.133 |
3.356 |
0.000 |
| z |
0.000 |
0.000 |
1.871 |
<r2> (average value of r
2) Å
2
| <r2> |
40.022 |
| (<r2>)1/2 |
6.326 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -169.813481 |
| Energy at 298.15K | -169.817590 |
| HF Energy | -169.813481 |
| Nuclear repulsion energy | 71.141835 |
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 B1B95/6-31G(2df,p)
| 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' |
3833 |
3671 |
31.00 |
|
|
|
| 2 |
A' |
3493 |
3345 |
4.06 |
|
|
|
| 3 |
A' |
3189 |
3054 |
14.32 |
|
|
|
| 4 |
A' |
1776 |
1700 |
257.55 |
|
|
|
| 5 |
A' |
1413 |
1353 |
1.58 |
|
|
|
| 6 |
A' |
1364 |
1307 |
25.97 |
|
|
|
| 7 |
A' |
1133 |
1085 |
237.59 |
|
|
|
| 8 |
A' |
1099 |
1053 |
52.45 |
|
|
|
| 9 |
A' |
590 |
565 |
34.97 |
|
|
|
| 10 |
A" |
1089 |
1043 |
52.45 |
|
|
|
| 11 |
A" |
863 |
827 |
53.66 |
|
|
|
| 12 |
A" |
540 |
517 |
72.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10190.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 9759.9 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.435 |
0.000 |
| O2 |
-1.095 |
-0.346 |
0.000 |
| N3 |
1.218 |
0.120 |
0.000 |
| H4 |
-0.299 |
1.481 |
0.000 |
| H5 |
-0.820 |
-1.269 |
0.000 |
| H6 |
1.353 |
-0.891 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3457 | 1.2585 | 1.0872 | 1.8915 | 1.8950 |
O2 | 1.3457 | | 2.3599 | 1.9932 | 0.9623 | 2.5080 | N3 | 1.2585 | 2.3599 | | 2.0383 | 2.4666 | 1.0201 | H4 | 1.0872 | 1.9932 | 2.0383 | | 2.7986 | 2.8907 | H5 | 1.8915 | 0.9623 | 2.4666 | 2.7986 | | 2.2059 | H6 | 1.8950 | 2.5080 | 1.0201 | 2.8907 | 2.2059 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
108.944 |
|
C1 |
N3 |
H6 |
112.118 |
| O2 |
C1 |
N3 |
129.941 |
|
O2 |
C1 |
H4 |
109.567 |
| N3 |
C1 |
H4 |
120.492 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.182 |
|
|
|
| 2 |
O |
-0.376 |
|
|
|
| 3 |
N |
-0.479 |
|
|
|
| 4 |
H |
0.148 |
|
|
|
| 5 |
H |
0.304 |
|
|
|
| 6 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.035 |
-1.773 |
0.000 |
2.053 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.161 |
-1.748 |
0.000 |
| y |
-1.748 |
-12.842 |
0.000 |
| z |
0.000 |
0.000 |
-18.260 |
|
| Traceless |
| | x | y | z |
| x |
-6.610 |
-1.748 |
0.000 |
| y |
-1.748 |
7.368 |
0.000 |
| z |
0.000 |
0.000 |
-0.758 |
|
| Polar |
| 3z2-r2 | -1.517 |
| x2-y2 | -9.319 |
| xy | -1.748 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.092 |
-0.174 |
0.000 |
| y |
-0.174 |
3.581 |
0.000 |
| z |
0.000 |
0.000 |
1.893 |
<r2> (average value of r
2) Å
2
| <r2> |
40.461 |
| (<r2>)1/2 |
6.361 |