Jump to
S1C2
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -134.350846 |
| Energy at 298.15K | -134.359076 |
| HF Energy | -134.350846 |
| Nuclear repulsion energy | 82.173558 |
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 M06-2X/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' |
3411 |
3230 |
0.32 |
|
|
|
| 2 |
A' |
3151 |
2985 |
31.98 |
|
|
|
| 3 |
A' |
3118 |
2954 |
18.40 |
|
|
|
| 4 |
A' |
3083 |
2920 |
15.08 |
|
|
|
| 5 |
A' |
1717 |
1626 |
22.27 |
|
|
|
| 6 |
A' |
1573 |
1490 |
4.38 |
|
|
|
| 7 |
A' |
1558 |
1476 |
0.96 |
|
|
|
| 8 |
A' |
1466 |
1389 |
7.58 |
|
|
|
| 9 |
A' |
1417 |
1342 |
5.78 |
|
|
|
| 10 |
A' |
1173 |
1111 |
13.84 |
|
|
|
| 11 |
A' |
1059 |
1003 |
9.50 |
|
|
|
| 12 |
A' |
903 |
855 |
15.65 |
|
|
|
| 13 |
A' |
725 |
686 |
267.72 |
|
|
|
| 14 |
A' |
402 |
380 |
8.02 |
|
|
|
| 15 |
A" |
3513 |
3328 |
0.02 |
|
|
|
| 16 |
A" |
3177 |
3009 |
42.74 |
|
|
|
| 17 |
A" |
3148 |
2982 |
0.48 |
|
|
|
| 18 |
A" |
1572 |
1489 |
9.80 |
|
|
|
| 19 |
A" |
1413 |
1339 |
0.09 |
|
|
|
| 20 |
A" |
1307 |
1238 |
0.01 |
|
|
|
| 21 |
A" |
1032 |
977 |
1.89 |
|
|
|
| 22 |
A" |
811 |
768 |
1.97 |
|
|
|
| 23 |
A" |
344 |
326 |
55.93 |
|
|
|
| 24 |
A" |
289 |
274 |
8.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20680.1 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 19588.2 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 M06-2X/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.305 |
-0.107 |
0.000 |
| C2 |
0.000 |
0.588 |
0.000 |
| C3 |
1.226 |
-0.352 |
0.000 |
| H4 |
2.162 |
0.215 |
0.000 |
| H5 |
1.209 |
-0.994 |
0.888 |
| H6 |
1.209 |
-0.994 |
-0.888 |
| H7 |
0.032 |
1.237 |
-0.881 |
| H8 |
0.032 |
1.237 |
0.881 |
| H9 |
-1.434 |
-0.681 |
0.837 |
| H10 |
-1.434 |
-0.681 |
-0.837 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4783 | 2.5423 | 3.4814 | 2.8095 | 2.8095 | 2.0903 | 2.0903 | 1.0232 | 1.0232 |
C2 | 1.4783 | | 1.5450 | 2.1937 | 2.1800 | 2.1800 | 1.0943 | 1.0943 | 2.0897 | 2.0897 | C3 | 2.5423 | 1.5450 | | 1.0946 | 1.0955 | 1.0955 | 2.1739 | 2.1739 | 2.8077 | 2.8077 | H4 | 3.4814 | 2.1937 | 1.0946 | | 1.7769 | 1.7769 | 2.5208 | 2.5208 | 3.7990 | 3.7990 | H5 | 2.8095 | 2.1800 | 1.0955 | 1.7769 | | 1.7759 | 3.0803 | 2.5221 | 2.6620 | 3.1718 | H6 | 2.8095 | 2.1800 | 1.0955 | 1.7769 | 1.7759 | | 2.5221 | 3.0803 | 3.1718 | 2.6620 | H7 | 2.0903 | 1.0943 | 2.1739 | 2.5208 | 3.0803 | 2.5221 | | 1.7612 | 2.9628 | 2.4143 | H8 | 2.0903 | 1.0943 | 2.1739 | 2.5208 | 2.5221 | 3.0803 | 1.7612 | | 2.4143 | 2.9628 | H9 | 1.0232 | 2.0897 | 2.8077 | 3.7990 | 2.6620 | 3.1718 | 2.9628 | 2.4143 | | 1.6748 | H10 | 1.0232 | 2.0897 | 2.8077 | 3.7990 | 3.1718 | 2.6620 | 2.4143 | 2.9628 | 1.6748 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
114.455 |
|
N1 |
C2 |
H7 |
107.749 |
| N1 |
C2 |
H8 |
107.749 |
|
C2 |
N1 |
H9 |
112.030 |
| C2 |
N1 |
H10 |
112.030 |
|
C2 |
C3 |
H4 |
111.275 |
| C2 |
C3 |
H5 |
110.138 |
|
C2 |
C3 |
H6 |
110.138 |
| C3 |
C2 |
H7 |
109.727 |
|
C3 |
C2 |
H8 |
109.727 |
| H4 |
C3 |
H5 |
108.455 |
|
H4 |
C3 |
H6 |
108.455 |
| H5 |
C3 |
H6 |
108.302 |
|
H7 |
C2 |
H8 |
107.162 |
| H9 |
N1 |
H10 |
109.857 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.683 |
|
|
|
| 2 |
C |
-0.254 |
|
|
|
| 3 |
C |
-0.589 |
|
|
|
| 4 |
H |
0.191 |
|
|
|
| 5 |
H |
0.188 |
|
|
|
| 6 |
H |
0.188 |
|
|
|
| 7 |
H |
0.210 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
| 9 |
H |
0.269 |
|
|
|
| 10 |
H |
0.269 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.950 |
-1.078 |
0.000 |
1.437 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.777 |
2.833 |
0.000 |
| y |
2.833 |
-19.981 |
0.000 |
| z |
0.000 |
0.000 |
-18.905 |
|
| Traceless |
| | x | y | z |
| x |
-4.333 |
2.833 |
0.000 |
| y |
2.833 |
1.360 |
0.000 |
| z |
0.000 |
0.000 |
2.974 |
|
| Polar |
| 3z2-r2 | 5.947 |
| x2-y2 | -3.795 |
| xy | 2.833 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.207 |
0.354 |
0.000 |
| y |
0.354 |
3.778 |
0.000 |
| z |
0.000 |
0.000 |
4.008 |
<r2> (average value of r
2) Å
2
| <r2> |
59.126 |
| (<r2>)1/2 |
7.689 |
Jump to
S1C1
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -134.349865 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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 M06-2X/3-21G*
Geometric Data calculated at M06-2X/3-21G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability