Jump to
S1C2
Energy calculated at SVWN/6-311G**
| hartrees |
Energy at 0K | -134.483976 |
Energy at 298.15K | -134.492081 |
Nuclear repulsion energy | 83.096533 |
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 SVWN/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' |
3412 |
3376 |
0.55 |
|
|
|
2 |
A' |
3034 |
3003 |
32.45 |
|
|
|
3 |
A' |
2958 |
2928 |
38.31 |
|
|
|
4 |
A' |
2951 |
2920 |
14.53 |
|
|
|
5 |
A' |
1592 |
1575 |
27.61 |
|
|
|
6 |
A' |
1430 |
1416 |
6.08 |
|
|
|
7 |
A' |
1410 |
1395 |
0.34 |
|
|
|
8 |
A' |
1339 |
1325 |
20.87 |
|
|
|
9 |
A' |
1317 |
1303 |
6.19 |
|
|
|
10 |
A' |
1145 |
1133 |
9.80 |
|
|
|
11 |
A' |
1071 |
1060 |
23.11 |
|
|
|
12 |
A' |
879 |
870 |
0.06 |
|
|
|
13 |
A' |
809 |
800 |
215.32 |
|
|
|
14 |
A' |
390 |
386 |
8.45 |
|
|
|
15 |
A" |
3494 |
3457 |
0.43 |
|
|
|
16 |
A" |
3036 |
3004 |
36.10 |
|
|
|
17 |
A" |
2991 |
2960 |
8.61 |
|
|
|
18 |
A" |
1419 |
1404 |
13.87 |
|
|
|
19 |
A" |
1337 |
1323 |
0.00 |
|
|
|
20 |
A" |
1220 |
1207 |
0.01 |
|
|
|
21 |
A" |
970 |
960 |
1.00 |
|
|
|
22 |
A" |
754 |
746 |
2.47 |
|
|
|
23 |
A" |
303 |
300 |
35.40 |
|
|
|
24 |
A" |
259 |
256 |
14.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19757.8 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 19552.3 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 SVWN/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-1.290 |
-0.080 |
0.000 |
C2 |
0.000 |
0.569 |
0.000 |
C3 |
1.197 |
-0.356 |
0.000 |
H4 |
2.153 |
0.194 |
0.000 |
H5 |
1.185 |
-1.009 |
0.889 |
H6 |
1.185 |
-1.009 |
-0.889 |
H7 |
0.045 |
1.239 |
-0.878 |
H8 |
0.045 |
1.239 |
0.878 |
H9 |
-1.381 |
-0.686 |
0.820 |
H10 |
-1.381 |
-0.686 |
-0.820 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
N1 | | 1.4444 | 2.5025 | 3.4539 | 2.7897 | 2.7897 | 2.0717 | 2.0717 | 1.0240 | 1.0240 |
C2 | 1.4444 | | 1.5130 | 2.1851 | 2.1649 | 2.1649 | 1.1047 | 1.1047 | 2.0389 | 2.0389 | C3 | 2.5025 | 1.5130 | | 1.1031 | 1.1032 | 1.1032 | 2.1541 | 2.1541 | 2.7258 | 2.7258 | H4 | 3.4539 | 2.1851 | 1.1031 | | 1.7819 | 1.7819 | 2.5105 | 2.5105 | 3.7334 | 3.7334 | H5 | 2.7897 | 2.1649 | 1.1032 | 1.7819 | | 1.7782 | 3.0780 | 2.5204 | 2.5879 | 3.1008 | H6 | 2.7897 | 2.1649 | 1.1032 | 1.7819 | 1.7782 | | 2.5204 | 3.0780 | 3.1008 | 2.5879 | H7 | 2.0717 | 1.1047 | 2.1541 | 2.5105 | 3.0780 | 2.5204 | | 1.7554 | 2.9363 | 2.3962 | H8 | 2.0717 | 1.1047 | 2.1541 | 2.5105 | 2.5204 | 3.0780 | 1.7554 | | 2.3962 | 2.9363 | H9 | 1.0240 | 2.0389 | 2.7258 | 3.7334 | 2.5879 | 3.1008 | 2.9363 | 2.3962 | | 1.6409 | H10 | 1.0240 | 2.0389 | 2.7258 | 3.7334 | 3.1008 | 2.5879 | 2.3962 | 2.9363 | 1.6409 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
C2 |
C3 |
115.581 |
|
N1 |
C2 |
H7 |
107.983 |
N1 |
C2 |
H8 |
107.983 |
|
C2 |
N1 |
H9 |
110.211 |
C2 |
N1 |
H10 |
110.211 |
|
C2 |
C3 |
H4 |
112.341 |
C2 |
C3 |
H5 |
110.714 |
|
C2 |
C3 |
H6 |
110.714 |
C3 |
C2 |
H7 |
109.775 |
|
C3 |
C2 |
H8 |
109.775 |
H4 |
C3 |
H5 |
107.737 |
|
H4 |
C3 |
H6 |
107.737 |
H5 |
C3 |
H6 |
107.400 |
|
H7 |
C2 |
H8 |
105.219 |
H9 |
N1 |
H10 |
106.492 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at SVWN/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.460 |
|
|
|
2 |
C |
-0.258 |
|
|
|
3 |
C |
-0.427 |
|
|
|
4 |
H |
0.142 |
|
|
|
5 |
H |
0.136 |
|
|
|
6 |
H |
0.136 |
|
|
|
7 |
H |
0.160 |
|
|
|
8 |
H |
0.160 |
|
|
|
9 |
H |
0.205 |
|
|
|
10 |
H |
0.205 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.804 |
-0.967 |
0.000 |
1.258 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.986 |
2.673 |
0.000 |
y |
2.673 |
-20.598 |
0.000 |
z |
0.000 |
0.000 |
-19.338 |
|
Traceless |
| x | y | z |
x |
-4.017 |
2.673 |
0.000 |
y |
2.673 |
1.064 |
0.000 |
z |
0.000 |
0.000 |
2.954 |
|
Polar |
3z2-r2 | 5.908 |
x2-y2 | -3.387 |
xy | 2.673 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.551 |
0.135 |
0.000 |
y |
0.135 |
4.970 |
0.000 |
z |
0.000 |
0.000 |
4.844 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at SVWN/6-311G**
| hartrees |
Energy at 0K | -134.483203 |
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 SVWN/6-311G**
Geometric Data calculated at SVWN/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability