Jump to
S1C2
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -151.165554 |
| Energy at 298.15K | -151.173534 |
| HF Energy | -151.165554 |
| Nuclear repulsion energy | 82.687006 |
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 B97D3/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3405 |
3357 |
7.86 |
|
|
|
| 2 |
A1 |
2994 |
2951 |
49.61 |
|
|
|
| 3 |
A1 |
1642 |
1619 |
40.10 |
|
|
|
| 4 |
A1 |
1459 |
1438 |
0.20 |
|
|
|
| 5 |
A1 |
1081 |
1066 |
30.80 |
|
|
|
| 6 |
A1 |
838 |
826 |
0.10 |
|
|
|
| 7 |
A1 |
447 |
441 |
5.35 |
|
|
|
| 8 |
A2 |
3491 |
3441 |
0.00 |
|
|
|
| 9 |
A2 |
1374 |
1354 |
0.00 |
|
|
|
| 10 |
A2 |
1066 |
1051 |
0.00 |
|
|
|
| 11 |
A2 |
267 |
263 |
0.00 |
|
|
|
| 12 |
B1 |
3489 |
3440 |
3.16 |
|
|
|
| 13 |
B1 |
3035 |
2992 |
36.29 |
|
|
|
| 14 |
B1 |
1351 |
1332 |
1.16 |
|
|
|
| 15 |
B1 |
839 |
827 |
0.59 |
|
|
|
| 16 |
B1 |
408 |
402 |
87.04 |
|
|
|
| 17 |
B2 |
3405 |
3357 |
0.08 |
|
|
|
| 18 |
B2 |
1632 |
1609 |
0.99 |
|
|
|
| 19 |
B2 |
1362 |
1343 |
19.45 |
|
|
|
| 20 |
B2 |
1024 |
1009 |
49.21 |
|
|
|
| 21 |
B2 |
784 |
773 |
455.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17696.8 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 17443.8 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 B97D3/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.554 |
| N2 |
0.000 |
1.271 |
-0.183 |
| N3 |
0.000 |
-1.271 |
-0.183 |
| H4 |
0.883 |
0.000 |
1.207 |
| H5 |
-0.883 |
0.000 |
1.207 |
| H6 |
0.816 |
1.316 |
-0.794 |
| H7 |
-0.816 |
1.316 |
-0.794 |
| H8 |
-0.816 |
-1.316 |
-0.794 |
| H9 |
0.816 |
-1.316 |
-0.794 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4699 | 1.4699 | 1.0975 | 1.0975 | 2.0528 | 2.0528 | 2.0528 | 2.0528 |
N2 | 1.4699 | | 2.5429 | 2.0802 | 2.0802 | 1.0199 | 1.0199 | 2.7807 | 2.7807 | N3 | 1.4699 | 2.5429 | | 2.0802 | 2.0802 | 2.7807 | 2.7807 | 1.0199 | 1.0199 | H4 | 1.0975 | 2.0802 | 2.0802 | | 1.7653 | 2.3951 | 2.9355 | 2.9355 | 2.3951 | H5 | 1.0975 | 2.0802 | 2.0802 | 1.7653 | | 2.9355 | 2.3951 | 2.3951 | 2.9355 | H6 | 2.0528 | 1.0199 | 2.7807 | 2.3951 | 2.9355 | | 1.6318 | 3.0966 | 2.6317 | H7 | 2.0528 | 1.0199 | 2.7807 | 2.9355 | 2.3951 | 1.6318 | | 2.6317 | 3.0966 | H8 | 2.0528 | 2.7807 | 1.0199 | 2.9355 | 2.3951 | 3.0966 | 2.6317 | | 1.6318 | H9 | 2.0528 | 2.7807 | 1.0199 | 2.3951 | 2.9355 | 2.6317 | 3.0966 | 1.6318 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H6 |
110.455 |
|
C1 |
N2 |
H7 |
110.455 |
| C1 |
N3 |
H8 |
110.455 |
|
C1 |
N3 |
H9 |
110.455 |
| N2 |
C1 |
N3 |
121.707 |
|
N2 |
C1 |
H4 |
106.663 |
| N2 |
C1 |
H5 |
106.663 |
|
N3 |
C1 |
H4 |
106.663 |
| N3 |
C1 |
H5 |
106.663 |
|
H4 |
C1 |
H5 |
107.863 |
| H6 |
N2 |
H7 |
107.856 |
|
H8 |
N3 |
H9 |
107.856 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.059 |
|
|
|
| 2 |
N |
-0.441 |
|
|
|
| 3 |
N |
-0.441 |
|
|
|
| 4 |
H |
0.123 |
|
|
|
| 5 |
H |
0.123 |
|
|
|
| 6 |
H |
0.174 |
|
|
|
| 7 |
H |
0.174 |
|
|
|
| 8 |
H |
0.174 |
|
|
|
| 9 |
H |
0.174 |
|
|
|
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 |
-1.854 |
1.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.934 |
0.000 |
0.000 |
| y |
0.000 |
-25.990 |
0.000 |
| z |
0.000 |
0.000 |
-18.190 |
|
| Traceless |
| | x | y | z |
| x |
5.156 |
0.000 |
0.000 |
| y |
0.000 |
-8.428 |
0.000 |
| z |
0.000 |
0.000 |
3.271 |
|
| Polar |
| 3z2-r2 | 6.543 |
| x2-y2 | 9.056 |
| 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 |
4.328 |
0.000 |
0.000 |
| y |
0.000 |
4.743 |
0.000 |
| z |
0.000 |
0.000 |
4.274 |
<r2> (average value of r
2) Å
2
| <r2> |
54.247 |
| (<r2>)1/2 |
7.365 |
Jump to
S1C1
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -151.161758 |
| Energy at 298.15K | -151.169694 |
| HF Energy | -151.161758 |
| Nuclear repulsion energy | 83.225506 |
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 B97D3/6-311G**
| 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 |
3511 |
3461 |
0.39 |
|
|
|
| 2 |
A |
3418 |
3369 |
0.18 |
|
|
|
| 3 |
A |
2864 |
2823 |
136.88 |
|
|
|
| 4 |
A |
1617 |
1593 |
0.67 |
|
|
|
| 5 |
A |
1507 |
1485 |
1.95 |
|
|
|
| 6 |
A |
1343 |
1324 |
1.70 |
|
|
|
| 7 |
A |
1187 |
1170 |
2.72 |
|
|
|
| 8 |
A |
945 |
932 |
1.21 |
|
|
|
| 9 |
A |
862 |
850 |
166.44 |
|
|
|
| 10 |
A |
477 |
471 |
0.45 |
|
|
|
| 11 |
A |
293 |
289 |
21.17 |
|
|
|
| 12 |
B |
3511 |
3461 |
0.23 |
|
|
|
| 13 |
B |
3418 |
3369 |
5.91 |
|
|
|
| 14 |
B |
2875 |
2834 |
123.37 |
|
|
|
| 15 |
B |
1614 |
1591 |
71.19 |
|
|
|
| 16 |
B |
1422 |
1402 |
31.81 |
|
|
|
| 17 |
B |
1232 |
1215 |
13.16 |
|
|
|
| 18 |
B |
1103 |
1087 |
20.76 |
|
|
|
| 19 |
B |
964 |
950 |
19.99 |
|
|
|
| 20 |
B |
825 |
813 |
151.23 |
|
|
|
| 21 |
B |
273 |
269 |
78.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17630.9 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 17378.7 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 B97D3/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.548 |
| N2 |
0.000 |
1.178 |
-0.320 |
| N3 |
0.000 |
-1.178 |
-0.320 |
| H4 |
0.886 |
-0.090 |
1.208 |
| H5 |
-0.886 |
0.090 |
1.208 |
| H6 |
-0.033 |
2.027 |
0.240 |
| H7 |
0.871 |
1.193 |
-0.850 |
| H8 |
0.033 |
-2.027 |
0.240 |
| H9 |
-0.871 |
-1.193 |
-0.850 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4635 | 1.4635 | 1.1082 | 1.1082 | 2.0510 | 2.0337 | 2.0510 | 2.0337 |
N2 | 1.4635 | | 2.3562 | 2.1744 | 2.0749 | 1.0182 | 1.0193 | 3.2544 | 2.5808 | N3 | 1.4635 | 2.3562 | | 2.0749 | 2.1744 | 3.2544 | 2.5808 | 1.0182 | 1.0193 | H4 | 1.1082 | 2.1744 | 2.0749 | | 1.7802 | 2.5026 | 2.4253 | 2.3280 | 2.9220 | H5 | 1.1082 | 2.0749 | 2.1744 | 1.7802 | | 2.3280 | 2.9220 | 2.5026 | 2.4253 | H6 | 2.0510 | 1.0182 | 3.2544 | 2.5026 | 2.3280 | | 1.6435 | 4.0555 | 3.5017 | H7 | 2.0337 | 1.0193 | 2.5808 | 2.4253 | 2.9220 | 1.6435 | | 3.5017 | 2.9537 | H8 | 2.0510 | 3.2544 | 1.0182 | 2.3280 | 2.5026 | 4.0555 | 3.5017 | | 1.6435 | H9 | 2.0337 | 2.5808 | 1.0193 | 2.9220 | 2.4253 | 3.5017 | 2.9537 | 1.6435 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H6 |
111.147 |
|
C1 |
N2 |
H7 |
109.193 |
| C1 |
N3 |
H8 |
111.147 |
|
C1 |
N3 |
H9 |
109.193 |
| N2 |
C1 |
N3 |
107.485 |
|
N2 |
C1 |
H4 |
114.606 |
| N2 |
C1 |
H5 |
106.815 |
|
N3 |
C1 |
H4 |
106.815 |
| N3 |
C1 |
H5 |
114.606 |
|
H4 |
C1 |
H5 |
106.750 |
| H6 |
N2 |
H7 |
108.318 |
|
H8 |
N3 |
H9 |
108.318 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.004 |
|
|
|
| 2 |
N |
-0.463 |
|
|
|
| 3 |
N |
-0.463 |
|
|
|
| 4 |
H |
0.088 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
| 6 |
H |
0.184 |
|
|
|
| 7 |
H |
0.192 |
|
|
|
| 8 |
H |
0.184 |
|
|
|
| 9 |
H |
0.192 |
|
|
|
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 |
1.438 |
1.438 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.743 |
2.887 |
0.000 |
| y |
2.887 |
-16.658 |
0.000 |
| z |
0.000 |
0.000 |
-20.521 |
|
| Traceless |
| | x | y | z |
| x |
-1.153 |
2.887 |
0.000 |
| y |
2.887 |
3.473 |
0.000 |
| z |
0.000 |
0.000 |
-2.320 |
|
| Polar |
| 3z2-r2 | -4.641 |
| x2-y2 | -3.084 |
| xy | 2.887 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.860 |
0.069 |
0.000 |
| y |
0.069 |
5.153 |
0.000 |
| z |
0.000 |
0.000 |
4.298 |
<r2> (average value of r
2) Å
2
| <r2> |
53.170 |
| (<r2>)1/2 |
7.292 |