Jump to
S1C2
Energy calculated at wB97X-D/6-31+G**
| hartrees |
Energy at 0K | -148.741027 |
Energy at 298.15K | -148.743253 |
HF Energy | -148.741027 |
Nuclear repulsion energy | 59.256527 |
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 wB97X-D/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' |
3621 |
3448 |
54.50 |
|
|
|
2 |
A' |
2392 |
2278 |
134.26 |
|
|
|
3 |
A' |
1642 |
1564 |
55.95 |
|
|
|
4 |
A' |
1116 |
1063 |
10.55 |
|
|
|
5 |
A' |
545 |
519 |
131.41 |
|
|
|
6 |
A' |
471 |
449 |
154.38 |
|
|
|
7 |
A" |
3733 |
3555 |
80.74 |
|
|
|
8 |
A" |
1190 |
1134 |
0.57 |
|
|
|
9 |
A" |
408 |
388 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7558.8 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 7198.2 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 wB97X-D/6-31+G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.222 |
0.000 |
N2 |
-0.019 |
1.382 |
0.000 |
N3 |
0.085 |
-1.122 |
0.000 |
H4 |
-0.232 |
-1.576 |
0.847 |
H5 |
-0.232 |
-1.576 |
-0.847 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1606 | 1.3463 | 2.0004 | 2.0004 |
N2 | 1.1606 | | 2.5062 | 3.0841 | 3.0841 | N3 | 1.3463 | 2.5062 | | 1.0116 | 1.0116 | H4 | 2.0004 | 3.0841 | 1.0116 | | 1.6932 | H5 | 2.0004 | 3.0841 | 1.0116 | 1.6932 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
115.343 |
|
C1 |
N3 |
H5 |
115.343 |
N2 |
C1 |
N3 |
177.304 |
|
H4 |
N3 |
H5 |
113.634 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.421 |
|
|
|
2 |
N |
-0.424 |
|
|
|
3 |
N |
-0.681 |
|
|
|
4 |
H |
0.342 |
|
|
|
5 |
H |
0.342 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.974 |
-4.614 |
0.000 |
4.715 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.809 |
1.952 |
0.000 |
y |
1.952 |
-18.727 |
0.000 |
z |
0.000 |
0.000 |
-15.056 |
|
Traceless |
| x | y | z |
x |
-1.917 |
1.952 |
0.000 |
y |
1.952 |
-1.795 |
0.000 |
z |
0.000 |
0.000 |
3.712 |
|
Polar |
3z2-r2 | 7.424 |
x2-y2 | -0.082 |
xy | 1.952 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.385 |
-0.067 |
0.000 |
y |
-0.067 |
5.480 |
0.000 |
z |
0.000 |
0.000 |
2.484 |
<r2> (average value of r
2) Å
2
<r2> |
39.950 |
(<r2>)1/2 |
6.321 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31+G**
| hartrees |
Energy at 0K | -148.740236 |
Energy at 298.15K | |
HF Energy | -148.740236 |
Nuclear repulsion energy | 59.369663 |
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 wB97X-D/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 |
A1 |
3671 |
3496 |
79.81 |
|
|
|
2 |
A1 |
2391 |
2277 |
164.44 |
|
|
|
3 |
A1 |
1623 |
1546 |
61.64 |
|
|
|
4 |
A1 |
1144 |
1089 |
14.03 |
|
|
|
5 |
B1 |
524 |
499 |
0.37 |
|
|
|
6 |
B1 |
357i |
340i |
315.32 |
|
|
|
7 |
B2 |
3801 |
3619 |
112.74 |
|
|
|
8 |
B2 |
1139 |
1085 |
4.70 |
|
|
|
9 |
B2 |
404 |
385 |
0.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7169.8 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 6827.8 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 wB97X-D/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.221 |
N2 |
0.000 |
0.000 |
1.384 |
N3 |
0.000 |
0.000 |
-1.110 |
H4 |
0.000 |
0.868 |
-1.619 |
H5 |
0.000 |
-0.868 |
-1.619 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1628 | 1.3312 | 2.0341 | 2.0341 |
N2 | 1.1628 | | 2.4940 | 3.1254 | 3.1254 | N3 | 1.3312 | 2.4940 | | 1.0056 | 1.0056 | H4 | 2.0341 | 3.1254 | 1.0056 | | 1.7350 | H5 | 2.0341 | 3.1254 | 1.0056 | 1.7350 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.386 |
|
C1 |
N3 |
H5 |
120.386 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
119.229 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.444 |
|
|
|
2 |
N |
-0.428 |
|
|
|
3 |
N |
-0.718 |
|
|
|
4 |
H |
0.351 |
|
|
|
5 |
H |
0.351 |
|
|
|
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 |
-4.916 |
4.916 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.035 |
0.000 |
0.000 |
y |
0.000 |
-14.852 |
0.000 |
z |
0.000 |
0.000 |
-18.105 |
|
Traceless |
| x | y | z |
x |
-2.557 |
0.000 |
0.000 |
y |
0.000 |
3.718 |
0.000 |
z |
0.000 |
0.000 |
-1.161 |
|
Polar |
3z2-r2 | -2.323 |
x2-y2 | -4.184 |
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 |
2.353 |
0.000 |
0.000 |
y |
0.000 |
2.392 |
0.000 |
z |
0.000 |
0.000 |
5.532 |
<r2> (average value of r
2) Å
2
<r2> |
39.890 |
(<r2>)1/2 |
6.316 |