Jump to
S1C2
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -112.407355 |
Energy at 298.15K | -112.412633 |
HF Energy | -112.407355 |
Counterpoise corrected energy | |
CP Energy at 298.15K | |
Counterpoise optimized geometry corrected energy | |
CP opt. Energy at 298.15K | |
Nuclear repulsion energy | 40.107703 |
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 HF/6-311G*
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
Ag |
3828 |
3462 |
0.00 |
|
|
|
2 |
Ag |
3708 |
3354 |
0.00 |
|
|
|
3 |
Ag |
1880 |
1701 |
0.00 |
|
|
|
4 |
Ag |
1254 |
1134 |
0.00 |
|
|
|
5 |
Ag |
450 |
407 |
0.00 |
|
|
|
6 |
Ag |
125 |
113 |
0.00 |
|
|
|
7 |
Au |
3826 |
3460 |
0.02 |
|
|
|
8 |
Au |
1895 |
1714 |
56.91 |
|
|
|
9 |
Au |
233 |
211 |
128.47 |
|
|
|
10 |
Au |
90 |
81 |
25.11 |
|
|
|
11 |
Bg |
3825 |
3460 |
0.00 |
|
|
|
12 |
Bg |
1882 |
1702 |
0.00 |
|
|
|
13 |
Bg |
110 |
99 |
0.00 |
|
|
|
14 |
Bu |
3827 |
3461 |
10.40 |
|
|
|
15 |
Bu |
3709 |
3354 |
6.92 |
|
|
|
16 |
Bu |
1863 |
1685 |
42.99 |
|
|
|
17 |
Bu |
1233 |
1115 |
488.09 |
|
|
|
18 |
Bu |
71 |
65 |
267.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16903.7 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15287.7 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 HF/6-311G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
H1 |
0.668 |
0.890 |
0.000 |
N2 |
0.000 |
1.633 |
0.000 |
N3 |
0.000 |
-1.633 |
0.000 |
H4 |
0.176 |
2.199 |
0.805 |
H5 |
0.176 |
2.199 |
-0.805 |
H6 |
-0.668 |
-0.890 |
0.000 |
H7 |
-0.176 |
-2.199 |
-0.805 |
H8 |
-0.176 |
-2.199 |
0.805 |
Atom - Atom Distances (Å)
|
H1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H1 | | 0.9998 | 2.6105 | 1.6135 | 1.6135 | 2.2261 | 3.3015 | 3.3015 |
N2 | 0.9998 | | 3.2669 | 0.9992 | 0.9992 | 2.6105 | 3.9196 | 3.9196 | N3 | 2.6105 | 3.2669 | | 3.9196 | 3.9196 | 0.9998 | 0.9992 | 0.9992 | H4 | 1.6135 | 0.9992 | 3.9196 | | 1.6102 | 3.3015 | 4.6958 | 4.4111 | H5 | 1.6135 | 0.9992 | 3.9196 | 1.6102 | | 3.3015 | 4.4111 | 4.6958 | H6 | 2.2261 | 2.6105 | 0.9998 | 3.3015 | 3.3015 | | 1.6135 | 1.6135 | H7 | 3.3015 | 3.9196 | 0.9992 | 4.6958 | 4.4111 | 1.6135 | | 1.6102 | H8 | 3.3015 | 3.9196 | 0.9992 | 4.4111 | 4.6958 | 1.6135 | 1.6102 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
H1 |
N2 |
H4 |
107.634 |
|
H1 |
N2 |
H5 |
107.634 |
H1 |
H3 |
N6 |
56.798 |
|
H1 |
H3 |
H7 |
126.280 |
H1 |
H3 |
H8 |
126.280 |
|
N2 |
H1 |
H3 |
123.202 |
H4 |
N2 |
H5 |
107.364 |
|
N6 |
H3 |
H7 |
107.634 |
N6 |
H3 |
H8 |
107.634 |
|
H7 |
H3 |
H8 |
107.364 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
H |
0.370 |
|
|
|
2 |
N |
-1.047 |
|
|
|
3 |
N |
-1.047 |
|
|
|
4 |
H |
0.339 |
|
|
|
5 |
H |
0.339 |
|
|
|
6 |
H |
0.370 |
|
|
|
7 |
H |
0.339 |
|
|
|
8 |
H |
0.339 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.689 |
4.065 |
0.000 |
y |
4.065 |
-8.693 |
0.000 |
z |
0.000 |
0.000 |
-12.154 |
|
Traceless |
| x | y | z |
x |
-6.265 |
4.065 |
0.000 |
y |
4.065 |
5.728 |
0.000 |
z |
0.000 |
0.000 |
0.537 |
|
Polar |
3z2-r2 | 1.073 |
x2-y2 | -7.995 |
xy | 4.065 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.071 |
-0.075 |
0.000 |
y |
-0.075 |
3.044 |
0.000 |
z |
0.000 |
0.000 |
2.671 |
<r2> (average value of r
2) Å
2
<r2> |
69.697 |
(<r2>)1/2 |
8.348 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -112.407355 |
Energy at 298.15K | -112.412622 |
HF Energy | -112.407355 |
Counterpoise corrected energy | |
CP Energy at 298.15K | |
Counterpoise optimized geometry corrected energy | |
CP opt. Energy at 298.15K | |
Nuclear repulsion energy | 40.105996 |
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 HF/6-311G*
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' |
3828 |
3462 |
0.00 |
|
|
|
2 |
A' |
3827 |
3461 |
10.37 |
|
|
|
3 |
A' |
3709 |
3355 |
6.93 |
|
|
|
4 |
A' |
3708 |
3354 |
0.00 |
|
|
|
5 |
A' |
1880 |
1701 |
0.00 |
|
|
|
6 |
A' |
1863 |
1685 |
43.00 |
|
|
|
7 |
A' |
1254 |
1134 |
0.00 |
|
|
|
8 |
A' |
1232 |
1114 |
488.19 |
|
|
|
9 |
A' |
449 |
406 |
0.00 |
|
|
|
10 |
A' |
125 |
113 |
0.00 |
|
|
|
11 |
A' |
69 |
63 |
267.86 |
|
|
|
12 |
A" |
3826 |
3460 |
0.02 |
|
|
|
13 |
A" |
3826 |
3460 |
0.00 |
|
|
|
14 |
A" |
1895 |
1714 |
56.93 |
|
|
|
15 |
A" |
1882 |
1702 |
0.00 |
|
|
|
16 |
A" |
232 |
210 |
128.25 |
|
|
|
17 |
A" |
108 |
98 |
0.00 |
|
|
|
18 |
A" |
88 |
79 |
25.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16900.9 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15285.2 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
H1 |
0.167 |
0.708 |
0.000 |
N2 |
-0.026 |
1.683 |
0.000 |
N3 |
-0.026 |
-1.591 |
0.000 |
H4 |
0.344 |
2.115 |
0.809 |
H5 |
0.344 |
2.115 |
-0.809 |
H6 |
-1.008 |
-1.450 |
0.000 |
H7 |
0.262 |
-2.066 |
-0.820 |
H8 |
0.262 |
-2.066 |
0.820 |
Atom - Atom Distances (Å)
|
H1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H1 | | 0.9934 | 2.3074 | 1.6321 | 1.6321 | 2.4575 | 2.8949 | 2.8949 |
N2 | 0.9934 | | 3.2737 | 0.9890 | 0.9890 | 3.2830 | 3.8486 | 3.8486 | N3 | 2.3074 | 3.2737 | | 3.8111 | 3.8111 | 0.9915 | 0.9907 | 0.9907 | H4 | 1.6321 | 0.9890 | 3.8111 | | 1.6179 | 3.8975 | 4.4880 | 4.1820 | H5 | 1.6321 | 0.9890 | 3.8111 | 1.6179 | | 3.8975 | 4.1820 | 4.4880 | H6 | 2.4575 | 3.2830 | 0.9915 | 3.8975 | 3.8975 | | 1.6326 | 1.6326 | H7 | 2.8949 | 3.8486 | 0.9907 | 4.4880 | 4.1820 | 1.6326 | | 1.6396 | H8 | 2.8949 | 3.8486 | 0.9907 | 4.1820 | 4.4880 | 1.6326 | 1.6396 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
H1 |
N2 |
H4 |
110.829 |
|
H1 |
N2 |
H5 |
110.829 |
H1 |
H3 |
N6 |
86.645 |
|
H1 |
H3 |
H7 |
116.985 |
H1 |
H3 |
H8 |
116.985 |
|
N2 |
H1 |
H3 |
163.955 |
H4 |
N2 |
H5 |
109.757 |
|
N6 |
H3 |
H7 |
110.895 |
N6 |
H3 |
H8 |
110.895 |
|
H7 |
H3 |
H8 |
111.687 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
H |
0.370 |
|
|
|
2 |
N |
-1.047 |
|
|
|
3 |
N |
-1.047 |
|
|
|
4 |
H |
0.339 |
|
|
|
5 |
H |
0.339 |
|
|
|
6 |
H |
0.370 |
|
|
|
7 |
H |
0.339 |
|
|
|
8 |
H |
0.339 |
|
|
|
Electric dipole moments
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.688 |
4.064 |
0.000 |
y |
4.064 |
-8.692 |
0.000 |
z |
0.000 |
0.000 |
-12.154 |
|
Traceless |
| x | y | z |
x |
-6.265 |
4.064 |
0.000 |
y |
4.064 |
5.729 |
0.000 |
z |
0.000 |
0.000 |
0.536 |
|
Polar |
3z2-r2 | 1.073 |
x2-y2 | -7.996 |
xy | 4.064 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.071 |
-0.075 |
0.000 |
y |
-0.075 |
3.044 |
0.000 |
z |
0.000 |
0.000 |
2.671 |
<r2> (average value of r
2) Å
2
<r2> |
69.711 |
(<r2>)1/2 |
8.349 |