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S1C2
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -135.101825 |
| Energy at 298.15K | -135.109903 |
| Nuclear repulsion energy | 81.921442 |
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 BLYP/6-31G(2df,p)
| 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' |
3348 |
3330 |
3.92 |
|
|
|
| 2 |
A' |
3010 |
2994 |
48.91 |
|
|
|
| 3 |
A' |
2949 |
2933 |
39.03 |
|
|
|
| 4 |
A' |
2945 |
2929 |
23.15 |
|
|
|
| 5 |
A' |
1626 |
1617 |
12.86 |
|
|
|
| 6 |
A' |
1468 |
1460 |
0.56 |
|
|
|
| 7 |
A' |
1447 |
1439 |
0.00 |
|
|
|
| 8 |
A' |
1368 |
1360 |
1.51 |
|
|
|
| 9 |
A' |
1344 |
1337 |
18.97 |
|
|
|
| 10 |
A' |
1125 |
1119 |
10.33 |
|
|
|
| 11 |
A' |
1013 |
1008 |
16.66 |
|
|
|
| 12 |
A' |
892 |
887 |
103.64 |
|
|
|
| 13 |
A' |
831 |
827 |
51.64 |
|
|
|
| 14 |
A' |
387 |
385 |
4.73 |
|
|
|
| 15 |
A" |
3420 |
3401 |
1.88 |
|
|
|
| 16 |
A" |
3016 |
2999 |
59.04 |
|
|
|
| 17 |
A" |
2976 |
2960 |
9.54 |
|
|
|
| 18 |
A" |
1459 |
1451 |
4.61 |
|
|
|
| 19 |
A" |
1360 |
1353 |
0.01 |
|
|
|
| 20 |
A" |
1240 |
1233 |
0.08 |
|
|
|
| 21 |
A" |
986 |
980 |
0.99 |
|
|
|
| 22 |
A" |
760 |
756 |
1.03 |
|
|
|
| 23 |
A" |
290 |
289 |
33.00 |
|
|
|
| 24 |
A" |
248 |
247 |
8.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19753.5 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 19644.8 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 BLYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.327 |
-0.079 |
0.000 |
| C2 |
0.000 |
0.578 |
0.000 |
| C3 |
1.226 |
-0.362 |
0.000 |
| H4 |
2.172 |
0.207 |
0.000 |
| H5 |
1.225 |
-1.013 |
0.891 |
| H6 |
1.225 |
-1.013 |
-0.891 |
| H7 |
0.041 |
1.240 |
-0.882 |
| H8 |
0.041 |
1.240 |
0.882 |
| H9 |
-1.387 |
-0.703 |
0.813 |
| H10 |
-1.387 |
-0.703 |
-0.813 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4807 | 2.5690 | 3.5104 | 2.8599 | 2.8599 | 2.0955 | 2.0955 | 1.0266 | 1.0266 |
C2 | 1.4807 | | 1.5452 | 2.2032 | 2.1967 | 2.1967 | 1.1040 | 1.1040 | 2.0555 | 2.0555 | C3 | 2.5690 | 1.5452 | | 1.1033 | 1.1032 | 1.1032 | 2.1794 | 2.1794 | 2.7580 | 2.7580 | H4 | 3.5104 | 2.2032 | 1.1033 | | 1.7824 | 1.7824 | 2.5268 | 2.5268 | 3.7620 | 3.7620 | H5 | 2.8599 | 2.1967 | 1.1032 | 1.7824 | | 1.7814 | 3.1018 | 2.5450 | 2.6315 | 3.1341 | H6 | 2.8599 | 2.1967 | 1.1032 | 1.7824 | 1.7814 | | 2.5450 | 3.1018 | 3.1341 | 2.6315 | H7 | 2.0955 | 1.1040 | 2.1794 | 2.5268 | 3.1018 | 2.5450 | | 1.7650 | 2.9479 | 2.4124 | H8 | 2.0955 | 1.1040 | 2.1794 | 2.5268 | 2.5450 | 3.1018 | 1.7650 | | 2.4124 | 2.9479 | H9 | 1.0266 | 2.0555 | 2.7580 | 3.7620 | 2.6315 | 3.1341 | 2.9479 | 2.4124 | | 1.6264 | H10 | 1.0266 | 2.0555 | 2.7580 | 3.7620 | 3.1341 | 2.6315 | 2.4124 | 2.9479 | 1.6264 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.188 |
|
N1 |
C2 |
H7 |
107.439 |
| N1 |
C2 |
H8 |
107.439 |
|
C2 |
N1 |
H9 |
108.778 |
| C2 |
N1 |
H10 |
108.778 |
|
C2 |
C3 |
H4 |
111.492 |
| C2 |
C3 |
H5 |
110.981 |
|
C2 |
C3 |
H6 |
110.981 |
| C3 |
C2 |
H7 |
109.576 |
|
C3 |
C2 |
H8 |
109.576 |
| H4 |
C3 |
H5 |
107.767 |
|
H4 |
C3 |
H6 |
107.767 |
| H5 |
C3 |
H6 |
107.685 |
|
H7 |
C2 |
H8 |
106.137 |
| H9 |
N1 |
H10 |
104.768 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.441 |
|
|
|
| 2 |
C |
-0.096 |
|
|
|
| 3 |
C |
-0.327 |
|
|
|
| 4 |
H |
0.095 |
|
|
|
| 5 |
H |
0.094 |
|
|
|
| 6 |
H |
0.094 |
|
|
|
| 7 |
H |
0.089 |
|
|
|
| 8 |
H |
0.089 |
|
|
|
| 9 |
H |
0.201 |
|
|
|
| 10 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.823 |
-0.915 |
0.000 |
1.231 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.627 |
2.325 |
0.000 |
| y |
2.325 |
-20.178 |
0.000 |
| z |
0.000 |
0.000 |
-19.190 |
|
| Traceless |
| | x | y | z |
| x |
-3.942 |
2.325 |
0.000 |
| y |
2.325 |
1.231 |
0.000 |
| z |
0.000 |
0.000 |
2.712 |
|
| Polar |
| 3z2-r2 | 5.424 |
| x2-y2 | -3.449 |
| xy | 2.325 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.182 |
0.219 |
0.000 |
| y |
0.219 |
4.612 |
0.000 |
| z |
0.000 |
0.000 |
4.575 |
<r2> (average value of r
2) Å
2
| <r2> |
59.494 |
| (<r2>)1/2 |
7.713 |
Jump to
S1C1
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -135.100869 |
| 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 BLYP/6-31G(2df,p)
Geometric Data calculated at BLYP/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability