Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| hartrees |
Energy at 0K | -148.738678 |
Energy at 298.15K | -148.740991 |
Nuclear repulsion energy | 59.190710 |
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/cc-pVDZ
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' |
3548 |
3410 |
36.82 |
|
|
|
2 |
A' |
2389 |
2296 |
95.20 |
|
|
|
3 |
A' |
1604 |
1542 |
35.41 |
|
|
|
4 |
A' |
1107 |
1064 |
6.44 |
|
|
|
5 |
A' |
648 |
622 |
192.41 |
|
|
|
6 |
A' |
492 |
473 |
30.04 |
|
|
|
7 |
A" |
3643 |
3502 |
57.43 |
|
|
|
8 |
A" |
1199 |
1152 |
0.01 |
|
|
|
9 |
A" |
413 |
397 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7520.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 7228.7 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 B1B95/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.217 |
0.000 |
N2 |
-0.031 |
1.381 |
0.000 |
N3 |
0.108 |
-1.123 |
0.000 |
H4 |
-0.271 |
-1.555 |
0.838 |
H5 |
-0.271 |
-1.555 |
-0.838 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1641 | 1.3448 | 1.9792 | 1.9792 |
N2 | 1.1641 | | 2.5080 | 3.0628 | 3.0628 | N3 | 1.3448 | 2.5080 | | 1.0163 | 1.0163 | H4 | 1.9792 | 3.0628 | 1.0163 | | 1.6761 | H5 | 1.9792 | 3.0628 | 1.0163 | 1.6761 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
113.176 |
|
C1 |
N3 |
H5 |
113.176 |
N2 |
C1 |
N3 |
176.895 |
|
H4 |
N3 |
H5 |
111.105 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.004 |
|
|
|
2 |
N |
-0.153 |
|
|
|
3 |
N |
-0.135 |
|
|
|
4 |
H |
0.142 |
|
|
|
5 |
H |
0.142 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.071 |
-4.271 |
0.000 |
4.404 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.842 |
2.058 |
0.000 |
y |
2.058 |
-17.956 |
0.000 |
z |
0.000 |
0.000 |
-14.894 |
|
Traceless |
| x | y | z |
x |
-1.417 |
2.058 |
0.000 |
y |
2.058 |
-1.588 |
0.000 |
z |
0.000 |
0.000 |
3.005 |
|
Polar |
3z2-r2 | 6.010 |
x2-y2 | 0.114 |
xy | 2.058 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.775 |
0.025 |
0.000 |
y |
0.025 |
4.744 |
0.000 |
z |
0.000 |
0.000 |
2.184 |
<r2> (average value of r
2) Å
2
<r2> |
39.495 |
(<r2>)1/2 |
6.284 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| hartrees |
Energy at 0K | -148.733778 |
Energy at 298.15K | |
HF Energy | -148.733778 |
Nuclear repulsion energy | 59.427151 |
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/cc-pVDZ
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 |
3643 |
3502 |
70.57 |
|
|
|
2 |
A1 |
2401 |
2308 |
129.62 |
|
|
|
3 |
A1 |
1576 |
1515 |
46.15 |
|
|
|
4 |
A1 |
1153 |
1108 |
9.67 |
|
|
|
5 |
B1 |
532 |
511 |
0.15 |
|
|
|
6 |
B1 |
473i |
455i |
257.69 |
|
|
|
7 |
B2 |
3774 |
3628 |
105.33 |
|
|
|
8 |
B2 |
1120 |
1077 |
2.19 |
|
|
|
9 |
B2 |
408 |
392 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7066.8 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 6792.6 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 B1B95/cc-pVDZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.218 |
N2 |
0.000 |
0.000 |
1.382 |
N3 |
0.000 |
0.000 |
-1.108 |
H4 |
0.000 |
0.869 |
-1.616 |
H5 |
0.000 |
-0.869 |
-1.616 |
Atom - Atom Distances (Å)
|
C1 |
N2 |
N3 |
H4 |
H5 |
C1 | | 1.1643 | 1.3258 | 2.0299 | 2.0299 |
N2 | 1.1643 | | 2.4901 | 3.1221 | 3.1221 | N3 | 1.3258 | 2.4901 | | 1.0072 | 1.0072 | H4 | 2.0299 | 3.1221 | 1.0072 | | 1.7388 | H5 | 2.0299 | 3.1221 | 1.0072 | 1.7388 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H4 |
120.322 |
|
C1 |
N3 |
H5 |
120.322 |
N2 |
C1 |
N3 |
180.000 |
|
H4 |
N3 |
H5 |
119.356 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.026 |
|
|
|
2 |
N |
-0.164 |
|
|
|
3 |
N |
-0.149 |
|
|
|
4 |
H |
0.144 |
|
|
|
5 |
H |
0.144 |
|
|
|
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 |
-4.711 |
4.711 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.122 |
0.000 |
0.000 |
y |
0.000 |
-14.562 |
0.000 |
z |
0.000 |
0.000 |
-17.087 |
|
Traceless |
| x | y | z |
x |
-2.297 |
0.000 |
0.000 |
y |
0.000 |
3.042 |
0.000 |
z |
0.000 |
0.000 |
-0.745 |
|
Polar |
3z2-r2 | -1.491 |
x2-y2 | -3.559 |
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 |
1.659 |
0.000 |
0.000 |
y |
0.000 |
2.131 |
0.000 |
z |
0.000 |
0.000 |
4.745 |
<r2> (average value of r
2) Å
2
<r2> |
39.350 |
(<r2>)1/2 |
6.273 |