Jump to
S1C2
Energy calculated at B3PW91/3-21G
| hartrees |
Energy at 0K | -134.383785 |
Energy at 298.15K | -134.391913 |
Nuclear repulsion energy | 82.119923 |
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 B3PW91/3-21G
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' |
3422 |
3290 |
2.19 |
|
|
|
2 |
A' |
3118 |
2997 |
40.19 |
|
|
|
3 |
A' |
3061 |
2942 |
29.89 |
|
|
|
4 |
A' |
3042 |
2924 |
20.30 |
|
|
|
5 |
A' |
1723 |
1656 |
19.53 |
|
|
|
6 |
A' |
1558 |
1498 |
4.32 |
|
|
|
7 |
A' |
1539 |
1479 |
1.65 |
|
|
|
8 |
A' |
1446 |
1390 |
7.58 |
|
|
|
9 |
A' |
1397 |
1343 |
5.91 |
|
|
|
10 |
A' |
1162 |
1116 |
13.16 |
|
|
|
11 |
A' |
1042 |
1002 |
7.35 |
|
|
|
12 |
A' |
892 |
857 |
19.63 |
|
|
|
13 |
A' |
709 |
682 |
260.04 |
|
|
|
14 |
A' |
392 |
377 |
8.54 |
|
|
|
15 |
A" |
3523 |
3386 |
0.69 |
|
|
|
16 |
A" |
3126 |
3005 |
54.04 |
|
|
|
17 |
A" |
3094 |
2974 |
1.49 |
|
|
|
18 |
A" |
1559 |
1498 |
9.91 |
|
|
|
19 |
A" |
1409 |
1355 |
0.13 |
|
|
|
20 |
A" |
1299 |
1248 |
0.02 |
|
|
|
21 |
A" |
1026 |
986 |
1.75 |
|
|
|
22 |
A" |
790 |
759 |
3.17 |
|
|
|
23 |
A" |
311 |
299 |
55.23 |
|
|
|
24 |
A" |
257 |
247 |
10.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20448.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 19655.2 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-1.310 |
-0.100 |
0.000 |
C2 |
0.000 |
0.582 |
0.000 |
C3 |
1.228 |
-0.354 |
0.000 |
H4 |
2.165 |
0.217 |
0.000 |
H5 |
1.217 |
-0.998 |
0.889 |
H6 |
1.217 |
-0.998 |
-0.889 |
H7 |
0.036 |
1.234 |
-0.881 |
H8 |
0.036 |
1.234 |
0.881 |
H9 |
-1.434 |
-0.678 |
0.836 |
H10 |
-1.434 |
-0.678 |
-0.836 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
N1 | | 1.4768 | 2.5501 | 3.4887 | 2.8248 | 2.8248 | 2.0901 | 2.0901 | 1.0236 | 1.0236 |
C2 | 1.4768 | | 1.5441 | 2.1951 | 2.1833 | 2.1833 | 1.0968 | 1.0968 | 2.0839 | 2.0839 | C3 | 2.5501 | 1.5441 | | 1.0975 | 1.0976 | 1.0976 | 2.1725 | 2.1725 | 2.8084 | 2.8084 | H4 | 3.4887 | 2.1951 | 1.0975 | | 1.7789 | 1.7789 | 2.5181 | 2.5181 | 3.8012 | 3.8012 | H5 | 2.8248 | 2.1833 | 1.0976 | 1.7789 | | 1.7786 | 3.0837 | 2.5248 | 2.6704 | 3.1787 | H6 | 2.8248 | 2.1833 | 1.0976 | 1.7789 | 1.7786 | | 2.5248 | 3.0837 | 3.1787 | 2.6704 | H7 | 2.0901 | 1.0968 | 2.1725 | 2.5181 | 3.0837 | 2.5248 | | 1.7623 | 2.9608 | 2.4126 | H8 | 2.0901 | 1.0968 | 2.1725 | 2.5181 | 2.5248 | 3.0837 | 1.7623 | | 2.4126 | 2.9608 | H9 | 1.0236 | 2.0839 | 2.8084 | 3.8012 | 2.6704 | 3.1787 | 2.9608 | 2.4126 | | 1.6714 | H10 | 1.0236 | 2.0839 | 2.8084 | 3.8012 | 3.1787 | 2.6704 | 2.4126 | 2.9608 | 1.6714 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
C2 |
C3 |
115.143 |
|
N1 |
C2 |
H7 |
107.697 |
N1 |
C2 |
H8 |
107.697 |
|
C2 |
N1 |
H9 |
111.622 |
C2 |
N1 |
H10 |
111.622 |
|
C2 |
C3 |
H4 |
111.280 |
C2 |
C3 |
H5 |
110.337 |
|
C2 |
C3 |
H6 |
110.337 |
C3 |
C2 |
H7 |
109.535 |
|
C3 |
C2 |
H8 |
109.535 |
H4 |
C3 |
H5 |
108.276 |
|
H4 |
C3 |
H6 |
108.276 |
H5 |
C3 |
H6 |
108.242 |
|
H7 |
C2 |
H8 |
106.905 |
H9 |
N1 |
H10 |
109.455 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.680 |
|
|
|
2 |
C |
-0.287 |
|
|
|
3 |
C |
-0.633 |
|
|
|
4 |
H |
0.203 |
|
|
|
5 |
H |
0.202 |
|
|
|
6 |
H |
0.202 |
|
|
|
7 |
H |
0.223 |
|
|
|
8 |
H |
0.223 |
|
|
|
9 |
H |
0.274 |
|
|
|
10 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.900 |
-1.109 |
0.000 |
1.428 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
59.139 |
(<r2>)1/2 |
7.690 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| hartrees |
Energy at 0K | -134.382570 |
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 B3PW91/3-21G
Geometric Data calculated at B3PW91/3-21G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability