Jump to
S1C2
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -148.720028 |
Energy at 298.15K | -148.722310 |
Nuclear repulsion energy | 59.304845 |
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*
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' |
3589 |
3407 |
42.65 |
|
|
|
2 |
A' |
2405 |
2283 |
98.76 |
|
|
|
3 |
A' |
1667 |
1582 |
49.35 |
|
|
|
4 |
A' |
1120 |
1063 |
6.77 |
|
|
|
5 |
A' |
604 |
573 |
238.62 |
|
|
|
6 |
A' |
492 |
467 |
57.43 |
|
|
|
7 |
A" |
3688 |
3501 |
59.04 |
|
|
|
8 |
A" |
1211 |
1150 |
0.52 |
|
|
|
9 |
A" |
416 |
394 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7595.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 7210.4 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*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.218 |
0.000 |
N2 |
-0.039 |
1.380 |
0.000 |
N3 |
0.104 |
-1.119 |
0.000 |
H4 |
-0.228 |
-1.569 |
0.841 |
H5 |
-0.228 |
-1.569 |
-0.841 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1623 | 1.3412 | 1.9886 | 1.9886 |
N2 | 1.1623 | | 2.5029 | 3.0724 | 3.0724 | N3 | 1.3412 | 2.5029 | | 1.0105 | 1.0105 | H4 | 1.9886 | 3.0724 | 1.0105 | | 1.6829 | H5 | 1.9886 | 3.0724 | 1.0105 | 1.6829 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
114.747 |
|
C1 |
N3 |
H5 |
114.747 |
N2 |
C1 |
N3 |
177.473 |
|
H4 |
N3 |
H5 |
112.768 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.467 |
|
|
|
2 |
N |
-0.438 |
|
|
|
3 |
N |
-0.787 |
|
|
|
4 |
H |
0.379 |
|
|
|
5 |
H |
0.379 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.082 |
-4.385 |
0.000 |
4.517 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.062 |
2.110 |
0.000 |
y |
2.110 |
-17.961 |
0.000 |
z |
0.000 |
0.000 |
-14.672 |
|
Traceless |
| x | y | z |
x |
-1.746 |
2.110 |
0.000 |
y |
2.110 |
-1.594 |
0.000 |
z |
0.000 |
0.000 |
3.339 |
|
Polar |
3z2-r2 | 6.679 |
x2-y2 | -0.101 |
xy | 2.110 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.589 |
-0.028 |
0.000 |
y |
-0.028 |
4.762 |
0.000 |
z |
0.000 |
0.000 |
2.074 |
<r2> (average value of r
2) Å
2
<r2> |
39.462 |
(<r2>)1/2 |
6.282 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -148.718621 |
Energy at 298.15K | |
HF Energy | -148.718621 |
Nuclear repulsion energy | 59.446241 |
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*
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 |
3661 |
3476 |
72.37 |
|
|
|
2 |
A1 |
2404 |
2282 |
126.84 |
|
|
|
3 |
A1 |
1644 |
1561 |
59.05 |
|
|
|
4 |
A1 |
1157 |
1098 |
10.06 |
|
|
|
5 |
B1 |
533 |
506 |
1.28 |
|
|
|
6 |
B1 |
435i |
413i |
341.71 |
|
|
|
7 |
B2 |
3777 |
3586 |
94.33 |
|
|
|
8 |
B2 |
1146 |
1088 |
5.40 |
|
|
|
9 |
B2 |
413 |
392 |
0.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7149.8 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 6787.3 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*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.219 |
N2 |
0.000 |
0.000 |
1.383 |
N3 |
0.000 |
0.000 |
-1.107 |
H4 |
0.000 |
0.865 |
-1.619 |
H5 |
0.000 |
-0.865 |
-1.619 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1640 | 1.3261 | 2.0308 | 2.0308 |
N2 | 1.1640 | | 2.4901 | 3.1235 | 3.1235 | N3 | 1.3261 | 2.4901 | | 1.0047 | 1.0047 | H4 | 2.0308 | 3.1235 | 1.0047 | | 1.7297 | H5 | 2.0308 | 3.1235 | 1.0047 | 1.7297 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.592 |
|
C1 |
N3 |
H5 |
120.592 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
118.817 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.494 |
|
|
|
2 |
N |
-0.440 |
|
|
|
3 |
N |
-0.829 |
|
|
|
4 |
H |
0.387 |
|
|
|
5 |
H |
0.387 |
|
|
|
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 |
-4.771 |
4.771 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.271 |
0.000 |
0.000 |
y |
0.000 |
-14.382 |
0.000 |
z |
0.000 |
0.000 |
-17.162 |
|
Traceless |
| x | y | z |
x |
-2.499 |
0.000 |
0.000 |
y |
0.000 |
3.335 |
0.000 |
z |
0.000 |
0.000 |
-0.836 |
|
Polar |
3z2-r2 | -1.672 |
x2-y2 | -3.890 |
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 |
1.495 |
0.000 |
0.000 |
y |
0.000 |
2.018 |
0.000 |
z |
0.000 |
0.000 |
4.787 |
<r2> (average value of r
2) Å
2
<r2> |
39.361 |
(<r2>)1/2 |
6.274 |