Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -133.028734 |
Energy at 298.15K | -133.034311 |
HF Energy | -133.028734 |
Nuclear repulsion energy | 70.892184 |
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 HF/LANL2DZ
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' |
3718 |
3346 |
4.25 |
|
|
|
2 |
A' |
3335 |
3001 |
28.57 |
|
|
|
3 |
A' |
3249 |
2924 |
68.27 |
|
|
|
4 |
A' |
3199 |
2878 |
29.30 |
|
|
|
5 |
A' |
1863 |
1676 |
72.53 |
|
|
|
6 |
A' |
1626 |
1463 |
16.87 |
|
|
|
7 |
A' |
1569 |
1412 |
15.34 |
|
|
|
8 |
A' |
1537 |
1383 |
38.66 |
|
|
|
9 |
A' |
1373 |
1235 |
44.46 |
|
|
|
10 |
A' |
1162 |
1046 |
37.16 |
|
|
|
11 |
A' |
1003 |
902 |
8.99 |
|
|
|
12 |
A' |
521 |
469 |
24.07 |
|
|
|
13 |
A" |
3268 |
2941 |
46.03 |
|
|
|
14 |
A" |
1631 |
1468 |
16.21 |
|
|
|
15 |
A" |
1256 |
1131 |
5.23 |
|
|
|
16 |
A" |
1195 |
1075 |
23.41 |
|
|
|
17 |
A" |
762 |
686 |
102.96 |
|
|
|
18 |
A" |
184 |
165 |
3.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16224.2 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 14600.1 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.045 |
-0.628 |
0.000 |
C2 |
0.000 |
0.452 |
0.000 |
N3 |
1.246 |
0.184 |
0.000 |
H4 |
-0.576 |
-1.601 |
0.000 |
H5 |
-1.681 |
-0.539 |
0.875 |
H6 |
-1.681 |
-0.539 |
-0.875 |
H7 |
-0.376 |
1.469 |
0.000 |
H8 |
1.864 |
0.981 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5024 | 2.4301 | 1.0798 | 1.0857 | 1.0857 | 2.2018 | 3.3243 |
C2 | 1.5024 | | 1.2739 | 2.1319 | 2.1388 | 2.1388 | 1.0852 | 1.9377 | N3 | 2.4301 | 1.2739 | | 2.5506 | 3.1395 | 3.1395 | 2.0691 | 1.0087 | H4 | 1.0798 | 2.1319 | 2.5506 | | 1.7647 | 1.7647 | 3.0770 | 3.5527 | H5 | 1.0857 | 2.1388 | 3.1395 | 1.7647 | | 1.7498 | 2.5505 | 3.9557 | H6 | 1.0857 | 2.1388 | 3.1395 | 1.7647 | 1.7498 | | 2.5505 | 3.9557 | H7 | 2.2018 | 1.0852 | 2.0691 | 3.0770 | 2.5505 | 2.5505 | | 2.2925 | H8 | 3.3243 | 1.9377 | 1.0087 | 3.5527 | 3.9557 | 3.9557 | 2.2925 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
121.945 |
|
C1 |
C2 |
H7 |
115.673 |
C2 |
C1 |
H4 |
110.224 |
|
C2 |
C1 |
H5 |
110.424 |
C2 |
C1 |
H6 |
110.424 |
|
C2 |
N3 |
H8 |
115.700 |
N3 |
C2 |
H7 |
122.382 |
|
H4 |
C1 |
H5 |
109.161 |
H4 |
C1 |
H6 |
109.161 |
|
H5 |
C1 |
H6 |
107.385 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.559 |
|
|
|
2 |
C |
-0.030 |
|
|
|
3 |
N |
-0.409 |
|
|
|
4 |
H |
0.217 |
|
|
|
5 |
H |
0.182 |
|
|
|
6 |
H |
0.182 |
|
|
|
7 |
H |
0.158 |
|
|
|
8 |
H |
0.258 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.695 |
1.919 |
0.000 |
2.560 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.023 |
3.106 |
0.000 |
y |
3.106 |
-17.734 |
0.000 |
z |
0.000 |
0.000 |
-20.212 |
|
Traceless |
| x | y | z |
x |
-1.050 |
3.106 |
0.000 |
y |
3.106 |
2.383 |
0.000 |
z |
0.000 |
0.000 |
-1.333 |
|
Polar |
3z2-r2 | -2.666 |
x2-y2 | -2.289 |
xy | 3.106 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.666 |
0.127 |
0.000 |
y |
0.127 |
3.570 |
0.000 |
z |
0.000 |
0.000 |
2.628 |
<r2> (average value of r
2) Å
2
<r2> |
50.707 |
(<r2>)1/2 |
7.121 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -133.028048 |
Energy at 298.15K | -133.033612 |
HF Energy | -133.028048 |
Nuclear repulsion energy | 70.823149 |
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 HF/LANL2DZ
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' |
3692 |
3322 |
4.74 |
|
|
|
2 |
A' |
3348 |
3013 |
56.98 |
|
|
|
3 |
A' |
3295 |
2966 |
22.51 |
|
|
|
4 |
A' |
3199 |
2879 |
22.08 |
|
|
|
5 |
A' |
1849 |
1664 |
75.30 |
|
|
|
6 |
A' |
1632 |
1469 |
32.36 |
|
|
|
7 |
A' |
1569 |
1412 |
16.86 |
|
|
|
8 |
A' |
1536 |
1382 |
4.03 |
|
|
|
9 |
A' |
1377 |
1239 |
91.11 |
|
|
|
10 |
A' |
1162 |
1045 |
40.94 |
|
|
|
11 |
A' |
989 |
890 |
0.59 |
|
|
|
12 |
A' |
519 |
467 |
11.24 |
|
|
|
13 |
A" |
3280 |
2951 |
35.58 |
|
|
|
14 |
A" |
1626 |
1463 |
14.95 |
|
|
|
15 |
A" |
1261 |
1135 |
57.83 |
|
|
|
16 |
A" |
1201 |
1080 |
27.72 |
|
|
|
17 |
A" |
779 |
701 |
18.41 |
|
|
|
18 |
A" |
174 |
157 |
0.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16243.2 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 14617.3 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.032 |
-0.616 |
0.000 |
C2 |
0.000 |
0.487 |
0.000 |
N3 |
1.267 |
0.362 |
0.000 |
H4 |
-0.571 |
-1.597 |
0.000 |
H5 |
-1.668 |
-0.532 |
0.875 |
H6 |
-1.668 |
-0.532 |
-0.875 |
H7 |
-0.384 |
1.493 |
0.000 |
H8 |
1.612 |
-0.588 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5105 | 2.4989 | 1.0835 | 1.0849 | 1.0849 | 2.2069 | 2.6440 |
C2 | 1.5105 | | 1.2735 | 2.1606 | 2.1417 | 2.1417 | 1.0772 | 1.9372 | N3 | 2.4989 | 1.2735 | | 2.6868 | 3.1912 | 3.1912 | 2.0015 | 1.0104 | H4 | 1.0835 | 2.1606 | 2.6868 | | 1.7611 | 1.7611 | 3.0959 | 2.4051 | H5 | 1.0849 | 2.1417 | 3.1912 | 1.7611 | | 1.7494 | 2.5532 | 3.3952 | H6 | 1.0849 | 2.1417 | 3.1912 | 1.7611 | 1.7494 | | 2.5532 | 3.3952 | H7 | 2.2069 | 1.0772 | 2.0015 | 3.0959 | 2.5532 | 2.5532 | | 2.8833 | H8 | 2.6440 | 1.9372 | 1.0104 | 2.4051 | 3.3952 | 3.3952 | 2.8833 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
127.478 |
|
C1 |
C2 |
H7 |
116.033 |
C2 |
C1 |
H4 |
111.743 |
|
C2 |
C1 |
H5 |
110.139 |
C2 |
C1 |
H6 |
110.139 |
|
C2 |
N3 |
H8 |
115.547 |
N3 |
C2 |
H7 |
116.489 |
|
H4 |
C1 |
H5 |
108.619 |
H4 |
C1 |
H6 |
108.619 |
|
H5 |
C1 |
H6 |
107.465 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.579 |
|
|
|
2 |
C |
-0.032 |
|
|
|
3 |
N |
-0.396 |
|
|
|
4 |
H |
0.182 |
|
|
|
5 |
H |
0.198 |
|
|
|
6 |
H |
0.198 |
|
|
|
7 |
H |
0.184 |
|
|
|
8 |
H |
0.244 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.457 |
-1.799 |
0.000 |
3.046 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.073 |
-4.164 |
0.000 |
y |
-4.164 |
-19.343 |
0.000 |
z |
0.000 |
0.000 |
-20.165 |
|
Traceless |
| x | y | z |
x |
-2.320 |
-4.164 |
0.000 |
y |
-4.164 |
1.777 |
0.000 |
z |
0.000 |
0.000 |
0.543 |
|
Polar |
3z2-r2 | 1.086 |
x2-y2 | -2.731 |
xy | -4.164 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.460 |
-0.261 |
0.000 |
y |
-0.261 |
3.668 |
0.000 |
z |
0.000 |
0.000 |
2.638 |
<r2> (average value of r
2) Å
2
<r2> |
50.934 |
(<r2>)1/2 |
7.137 |