Jump to
S1C2
Energy calculated at HF/3-21G
| hartrees |
Energy at 0K | -111.753551 |
Energy at 298.15K | -111.759242 |
HF Energy | -111.753551 |
Counterpoise corrected energy | -55.872165 |
CP Energy at 298.15K | -55.877569 |
Counterpoise optimized geometry corrected energy | |
CP opt. Energy at 298.15K | |
Nuclear repulsion energy | 40.993042 |
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/3-21G
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 |
3789 |
3431 |
0.00 |
|
|
|
2 |
Ag |
3628 |
3285 |
0.00 |
|
|
|
3 |
Ag |
1863 |
1687 |
0.00 |
|
|
|
4 |
Ag |
1007 |
912 |
0.00 |
|
|
|
5 |
Ag |
564 |
511 |
0.00 |
|
|
|
6 |
Ag |
187 |
170 |
0.00 |
|
|
|
7 |
Au |
3786 |
3429 |
0.83 |
|
|
|
8 |
Au |
1890 |
1712 |
47.79 |
|
|
|
9 |
Au |
304 |
275 |
107.49 |
|
|
|
10 |
Au |
139 |
126 |
33.15 |
|
|
|
11 |
Bg |
3785 |
3428 |
0.00 |
|
|
|
12 |
Bg |
1874 |
1697 |
0.00 |
|
|
|
13 |
Bg |
203 |
184 |
0.00 |
|
|
|
14 |
Bu |
3791 |
3433 |
50.60 |
|
|
|
15 |
Bu |
3633 |
3290 |
22.06 |
|
|
|
16 |
Bu |
1846 |
1672 |
34.52 |
|
|
|
17 |
Bu |
926 |
838 |
801.09 |
|
|
|
18 |
Bu |
57 |
52 |
333.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16635.9 cm
-1
Scaled (by 0.9056) Zero Point Vibrational Energy (zpe) 15065.4 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 HF/3-21G
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
H1 |
0.636 |
0.761 |
0.000 |
N2 |
0.000 |
1.539 |
0.000 |
N3 |
0.000 |
-1.539 |
0.000 |
H4 |
0.073 |
2.096 |
0.831 |
H5 |
0.073 |
2.096 |
-0.831 |
H6 |
-0.636 |
-0.761 |
0.000 |
H7 |
-0.073 |
-2.096 |
-0.831 |
H8 |
-0.073 |
-2.096 |
0.831 |
Atom - Atom Distances (Å)
|
H1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H1 | | 1.0043 | 2.3865 | 1.6701 | 1.6701 | 1.9842 | 3.0597 | 3.0597 |
N2 | 1.0043 | | 3.0775 | 1.0036 | 1.0036 | 2.3865 | 3.7297 | 3.7297 | N3 | 2.3865 | 3.0775 | | 3.7297 | 3.7297 | 1.0043 | 1.0036 | 1.0036 | H4 | 1.6701 | 1.0036 | 3.7297 | | 1.6622 | 3.0597 | 4.5128 | 4.1955 | H5 | 1.6701 | 1.0036 | 3.7297 | 1.6622 | | 3.0597 | 4.1955 | 4.5128 | H6 | 1.9842 | 2.3865 | 1.0043 | 3.0597 | 3.0597 | | 1.6701 | 1.6701 | H7 | 3.0597 | 3.7297 | 1.0036 | 4.5128 | 4.1955 | 1.6701 | | 1.6622 | H8 | 3.0597 | 3.7297 | 1.0036 | 4.1955 | 4.5128 | 1.6701 | 1.6622 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
H1 |
N2 |
H4 |
112.566 |
|
H1 |
N2 |
H5 |
112.566 |
H1 |
H3 |
N6 |
54.742 |
|
H1 |
H3 |
H7 |
123.720 |
H1 |
H3 |
H8 |
123.720 |
|
N2 |
H1 |
H3 |
125.258 |
H4 |
N2 |
H5 |
111.817 |
|
N6 |
H3 |
H7 |
112.566 |
N6 |
H3 |
H8 |
112.566 |
|
H7 |
H3 |
H8 |
111.817 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
H |
0.327 |
|
|
|
2 |
N |
-0.905 |
|
|
|
3 |
N |
-0.905 |
|
|
|
4 |
H |
0.289 |
|
|
|
5 |
H |
0.289 |
|
|
|
6 |
H |
0.327 |
|
|
|
7 |
H |
0.289 |
|
|
|
8 |
H |
0.289 |
|
|
|
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 |
-15.964 |
3.161 |
0.000 |
y |
3.161 |
-8.264 |
0.000 |
z |
0.000 |
0.000 |
-11.553 |
|
Traceless |
| x | y | z |
x |
-6.055 |
3.161 |
0.000 |
y |
3.161 |
5.494 |
0.000 |
z |
0.000 |
0.000 |
0.561 |
|
Polar |
3z2-r2 | 1.122 |
x2-y2 | -7.700 |
xy | 3.161 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.969 |
-0.397 |
0.000 |
y |
-0.397 |
2.563 |
0.000 |
z |
0.000 |
0.000 |
2.322 |
<r2> (average value of r
2) Å
2
<r2> |
62.932 |
(<r2>)1/2 |
7.933 |
Jump to
S1C1
Energy calculated at HF/3-21G
| hartrees |
Energy at 0K | -111.753766 |
Energy at 298.15K | -111.759257 |
HF Energy | -111.753766 |
Counterpoise corrected energy | -55.872165 |
CP Energy at 298.15K | -55.877569 |
Counterpoise optimized geometry corrected energy | |
CP opt. Energy at 298.15K | |
Nuclear repulsion energy | 40.145858 |
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/3-21G
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' |
3791 |
3433 |
6.16 |
|
|
|
2 |
A' |
3743 |
3390 |
54.02 |
|
|
|
3 |
A' |
3639 |
3295 |
0.68 |
|
|
|
4 |
A' |
3589 |
3251 |
96.85 |
|
|
|
5 |
A' |
1868 |
1692 |
16.06 |
|
|
|
6 |
A' |
1854 |
1679 |
25.58 |
|
|
|
7 |
A' |
1009 |
914 |
355.50 |
|
|
|
8 |
A' |
949 |
860 |
382.52 |
|
|
|
9 |
A' |
446 |
404 |
61.73 |
|
|
|
10 |
A' |
164 |
149 |
32.09 |
|
|
|
11 |
A' |
115 |
105 |
71.39 |
|
|
|
12 |
A" |
3790 |
3432 |
4.02 |
|
|
|
13 |
A" |
3771 |
3415 |
1.24 |
|
|
|
14 |
A" |
1907 |
1727 |
24.43 |
|
|
|
15 |
A" |
1860 |
1684 |
24.52 |
|
|
|
16 |
A" |
347 |
314 |
57.48 |
|
|
|
17 |
A" |
157 |
142 |
46.51 |
|
|
|
18 |
A" |
47 |
43 |
27.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16523.2 cm
-1
Scaled (by 0.9056) Zero Point Vibrational Energy (zpe) 14963.4 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 HF/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
H1 |
0.166 |
0.681 |
0.000 |
N2 |
-0.023 |
1.665 |
0.000 |
N3 |
-0.023 |
-1.587 |
0.000 |
H4 |
0.288 |
2.128 |
0.828 |
H5 |
0.288 |
2.128 |
-0.828 |
H6 |
-1.008 |
-1.413 |
0.000 |
H7 |
0.294 |
-2.036 |
-0.835 |
H8 |
0.294 |
-2.036 |
0.835 |
Atom - Atom Distances (Å)
|
H1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H1 | | 1.0018 | 2.2761 | 1.6715 | 1.6715 | 2.4009 | 2.8458 | 2.8458 |
N2 | 1.0018 | | 3.2520 | 0.9985 | 0.9985 | 3.2317 | 3.8075 | 3.8075 | N3 | 2.2761 | 3.2520 | | 3.8189 | 3.8189 | 1.0003 | 1.0001 | 1.0001 | H4 | 1.6715 | 0.9985 | 3.8189 | | 1.6561 | 3.8606 | 4.4842 | 4.1643 | H5 | 1.6715 | 0.9985 | 3.8189 | 1.6561 | | 3.8606 | 4.1643 | 4.4842 | H6 | 2.4009 | 3.2317 | 1.0003 | 3.8606 | 3.8606 | | 1.6677 | 1.6677 | H7 | 2.8458 | 3.8075 | 1.0001 | 4.4842 | 4.1643 | 1.6677 | | 1.6709 | H8 | 2.8458 | 3.8075 | 1.0001 | 4.1643 | 4.4842 | 1.6677 | 1.6709 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
H1 |
N2 |
H4 |
113.361 |
|
H1 |
N2 |
H5 |
113.361 |
H1 |
H3 |
N6 |
84.747 |
|
H1 |
H3 |
H7 |
114.913 |
H1 |
H3 |
H8 |
114.913 |
|
N2 |
H1 |
H3 |
164.335 |
H4 |
N2 |
H5 |
112.057 |
|
N6 |
H3 |
H7 |
112.960 |
N6 |
H3 |
H8 |
112.960 |
|
H7 |
H3 |
H8 |
113.321 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
H |
0.331 |
|
|
|
2 |
N |
-0.918 |
|
|
|
3 |
N |
-0.872 |
|
|
|
4 |
H |
0.271 |
|
|
|
5 |
H |
0.271 |
|
|
|
6 |
H |
0.311 |
|
|
|
7 |
H |
0.303 |
|
|
|
8 |
H |
0.303 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.146 |
-2.807 |
0.000 |
3.032 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.256 |
3.607 |
0.000 |
y |
3.607 |
-10.410 |
0.000 |
z |
0.000 |
0.000 |
-11.589 |
|
Traceless |
| x | y | z |
x |
-3.257 |
3.607 |
0.000 |
y |
3.607 |
2.513 |
0.000 |
z |
0.000 |
0.000 |
0.744 |
|
Polar |
3z2-r2 | 1.489 |
x2-y2 | -3.847 |
xy | 3.607 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.485 |
0.005 |
0.000 |
y |
0.005 |
2.051 |
0.000 |
z |
0.000 |
0.000 |
2.339 |
<r2> (average value of r
2) Å
2
<r2> |
67.637 |
(<r2>)1/2 |
8.224 |