Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.392086 |
| Energy at 298.15K | -131.391376 |
| HF Energy | -131.392086 |
| Nuclear repulsion energy | 47.467854 |
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 mPW1PW91/6-31G(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' |
3427 |
3272 |
42.81 |
|
|
|
| 2 |
A' |
1802 |
1720 |
44.46 |
|
|
|
| 3 |
A' |
1246 |
1190 |
8.36 |
|
|
|
| 4 |
A' |
468 |
447 |
12.04 |
|
|
|
| 5 |
A' |
359 |
343 |
33.85 |
|
|
|
| 6 |
A" |
458 |
437 |
1.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3879.8 cm
-1
Scaled (by 0.9547) Zero Point Vibrational Energy (zpe) 3704.0 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 mPW1PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.090 |
-1.214 |
0.000 |
| C2 |
0.000 |
0.086 |
0.000 |
| N3 |
-0.165 |
1.273 |
0.000 |
| H4 |
0.617 |
-2.142 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3026 | 2.4994 | 1.0680 |
C2 | 1.3026 | | 1.1983 | 2.3120 | N3 | 2.4994 | 1.1983 | | 3.5034 | H4 | 1.0680 | 2.3120 | 3.5034 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.030 |
|
C2 |
C1 |
H4 |
154.341 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.391687 |
| Energy at 298.15K | |
| HF Energy | -131.391687 |
| Nuclear repulsion energy | 47.523962 |
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 mPW1PW91/6-31G(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 |
Σ |
3485 |
3327 |
70.69 |
|
|
|
| 2 |
Σ |
1745 |
1666 |
48.23 |
|
|
|
| 3 |
Σ |
1282 |
1224 |
5.51 |
|
|
|
| 4 |
Π |
459 |
438 |
0.60 |
|
|
|
| 4 |
Π |
459 |
438 |
0.60 |
|
|
|
| 5 |
Π |
259i |
247i |
46.28 |
|
|
|
| 5 |
Π |
259i |
247i |
46.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3455.6 cm
-1
Scaled (by 0.9547) Zero Point Vibrational Energy (zpe) 3299.0 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 mPW1PW91/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.205 |
| C2 |
0.000 |
0.000 |
0.081 |
| N3 |
0.000 |
0.000 |
1.288 |
| H4 |
0.000 |
0.000 |
-2.269 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2868 | 2.4930 | 1.0636 |
C2 | 1.2868 | | 1.2061 | 2.3505 | N3 | 2.4930 | 1.2061 | | 3.5566 | H4 | 1.0636 | 2.3505 | 3.5566 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.219 |
|
|
|
| 2 |
C |
0.306 |
|
|
|
| 3 |
N |
-0.346 |
|
|
|
| 4 |
H |
0.260 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.266 |
3.266 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.827 |
0.000 |
0.000 |
| y |
0.000 |
-16.827 |
0.000 |
| z |
0.000 |
0.000 |
-14.965 |
|
| Traceless |
| | x | y | z |
| x |
-0.931 |
0.000 |
0.000 |
| y |
0.000 |
-0.931 |
0.000 |
| z |
0.000 |
0.000 |
1.862 |
|
| Polar |
| 3z2-r2 | 3.723 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.031 |
0.000 |
0.000 |
| y |
0.000 |
2.031 |
0.000 |
| z |
0.000 |
0.000 |
6.172 |
<r2> (average value of r
2) Å
2
| <r2> |
35.633 |
| (<r2>)1/2 |
5.969 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.359981 |
| Energy at 298.15K | -131.359454 |
| HF Energy | -131.359981 |
| Nuclear repulsion energy | 47.130886 |
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 mPW1PW91/6-31G(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' |
3097 |
2957 |
7.29 |
|
|
|
| 2 |
A' |
2127 |
2031 |
23.42 |
|
|
|
| 3 |
A' |
1100 |
1050 |
39.36 |
|
|
|
| 4 |
A' |
946 |
903 |
43.49 |
|
|
|
| 5 |
A' |
467 |
446 |
24.34 |
|
|
|
| 6 |
A" |
327 |
313 |
12.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4031.7 cm
-1
Scaled (by 0.9547) Zero Point Vibrational Energy (zpe) 3849.1 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 mPW1PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.032 |
-1.280 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.180 |
1.254 |
0.000 |
| H4 |
1.069 |
-1.648 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3716 | 2.5429 | 1.1003 |
C2 | 1.3716 | | 1.1767 | 2.0412 | N3 | 2.5429 | 1.1767 | | 3.1592 | H4 | 1.1003 | 2.0412 | 3.1592 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.253 |
|
|
|
| 2 |
C |
0.332 |
|
|
|
| 3 |
N |
-0.292 |
|
|
|
| 4 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.622 |
-1.442 |
0.000 |
2.170 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.674 |
-2.373 |
0.000 |
| y |
-2.373 |
-20.365 |
0.000 |
| z |
0.000 |
0.000 |
-15.573 |
|
| Traceless |
| | x | y | z |
| x |
1.295 |
-2.373 |
0.000 |
| y |
-2.373 |
-4.242 |
0.000 |
| z |
0.000 |
0.000 |
2.947 |
|
| Polar |
| 3z2-r2 | 5.893 |
| x2-y2 | 3.691 |
| xy | -2.373 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.601 |
-0.595 |
0.000 |
| y |
-0.595 |
6.168 |
0.000 |
| z |
0.000 |
0.000 |
2.464 |
<r2> (average value of r
2) Å
2
| <r2> |
35.933 |
| (<r2>)1/2 |
5.994 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.359981 |
| Energy at 298.15K | -131.359454 |
| HF Energy | -131.359981 |
| Nuclear repulsion energy | 47.130886 |
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 mPW1PW91/6-31G(2df,p)
Geometric Data calculated at mPW1PW91/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability