Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -133.174551 |
Energy at 298.15K | -133.178734 |
HF Energy | -133.174551 |
Nuclear repulsion energy | 65.032824 |
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 HSEh1PBE/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' |
3489 |
3348 |
1.30 |
|
|
|
2 |
A' |
3285 |
3152 |
6.75 |
|
|
|
3 |
A' |
3173 |
3045 |
5.10 |
|
|
|
4 |
A' |
3063 |
2939 |
58.18 |
|
|
|
5 |
A' |
1530 |
1468 |
10.56 |
|
|
|
6 |
A' |
1469 |
1410 |
4.09 |
|
|
|
7 |
A' |
1375 |
1320 |
39.49 |
|
|
|
8 |
A' |
1266 |
1215 |
6.79 |
|
|
|
9 |
A' |
1127 |
1081 |
22.39 |
|
|
|
10 |
A' |
1003 |
962 |
9.47 |
|
|
|
11 |
A' |
491 |
471 |
12.34 |
|
|
|
12 |
A" |
1056 |
1013 |
0.01 |
|
|
|
13 |
A" |
807 |
774 |
10.37 |
|
|
|
14 |
A" |
685 |
657 |
122.34 |
|
|
|
15 |
A" |
532 |
510 |
7.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12174.7 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 11682.9 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.416 |
0.000 |
C2 |
1.149 |
-0.376 |
0.000 |
N3 |
-1.188 |
-0.134 |
0.000 |
H4 |
0.141 |
1.504 |
0.000 |
H5 |
2.141 |
0.058 |
0.000 |
H6 |
1.046 |
-1.456 |
0.000 |
H7 |
-1.904 |
0.593 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
C1 | | 1.3956 | 1.3091 | 1.0971 | 2.1707 | 2.1441 | 1.9122 |
C2 | 1.3956 | | 2.3493 | 2.1337 | 1.0833 | 1.0841 | 3.2029 | N3 | 1.3091 | 2.3493 | | 2.1090 | 3.3346 | 2.5956 | 1.0200 | H4 | 1.0971 | 2.1337 | 2.1090 | | 2.4682 | 3.0951 | 2.2386 | H5 | 2.1707 | 1.0833 | 3.3346 | 2.4682 | | 1.8686 | 4.0802 | H6 | 2.1441 | 1.0841 | 2.5956 | 3.0951 | 1.8686 | | 3.5913 | H7 | 1.9122 | 3.2029 | 1.0200 | 2.2386 | 4.0802 | 3.5913 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H5 |
121.740 |
|
C1 |
C2 |
H6 |
119.153 |
C1 |
N3 |
H7 |
109.747 |
|
C2 |
C1 |
N3 |
120.561 |
C2 |
C1 |
H4 |
117.238 |
|
N3 |
C1 |
H4 |
122.201 |
H5 |
C2 |
H6 |
119.107 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.075 |
|
|
|
2 |
C |
-0.410 |
|
|
|
3 |
N |
-0.463 |
|
|
|
4 |
H |
0.191 |
|
|
|
5 |
H |
0.229 |
|
|
|
6 |
H |
0.240 |
|
|
|
7 |
H |
0.287 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.011 |
1.656 |
0.000 |
1.940 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.711 |
-2.872 |
0.000 |
y |
-2.872 |
-17.614 |
0.000 |
z |
0.000 |
0.000 |
-20.297 |
|
Traceless |
| x | y | z |
x |
2.244 |
-2.872 |
0.000 |
y |
-2.872 |
0.890 |
0.000 |
z |
0.000 |
0.000 |
-3.135 |
|
Polar |
3z2-r2 | -6.269 |
x2-y2 | 0.903 |
xy | -2.872 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.493 |
-0.420 |
0.000 |
y |
-0.420 |
4.237 |
0.000 |
z |
0.000 |
0.000 |
2.231 |
<r2> (average value of r
2) Å
2
<r2> |
45.243 |
(<r2>)1/2 |
6.726 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -133.173762 |
Energy at 298.15K | -133.177927 |
HF Energy | -133.173762 |
Nuclear repulsion energy | 65.017816 |
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 HSEh1PBE/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' |
3430 |
3291 |
11.84 |
|
|
|
2 |
A' |
3264 |
3132 |
12.05 |
|
|
|
3 |
A' |
3156 |
3029 |
6.06 |
|
|
|
4 |
A' |
3129 |
3002 |
26.75 |
|
|
|
5 |
A' |
1510 |
1449 |
6.61 |
|
|
|
6 |
A' |
1466 |
1407 |
4.35 |
|
|
|
7 |
A' |
1396 |
1340 |
14.33 |
|
|
|
8 |
A' |
1257 |
1206 |
37.16 |
|
|
|
9 |
A' |
1153 |
1107 |
29.53 |
|
|
|
10 |
A' |
993 |
952 |
0.85 |
|
|
|
11 |
A' |
496 |
476 |
8.68 |
|
|
|
12 |
A" |
1084 |
1040 |
59.74 |
|
|
|
13 |
A" |
818 |
785 |
76.09 |
|
|
|
14 |
A" |
684 |
656 |
4.14 |
|
|
|
15 |
A" |
491 |
472 |
0.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12162.7 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 11671.3 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.447 |
0.000 |
C2 |
1.125 |
-0.381 |
0.000 |
N3 |
-1.253 |
0.068 |
0.000 |
H4 |
0.164 |
1.526 |
0.000 |
H5 |
2.129 |
0.027 |
0.000 |
H6 |
1.020 |
-1.463 |
0.000 |
H7 |
-1.296 |
-0.956 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
C1 | | 1.3971 | 1.3090 | 1.0924 | 2.1704 | 2.1649 | 1.9093 |
C2 | 1.3971 | | 2.4204 | 2.1362 | 1.0839 | 1.0866 | 2.4883 | N3 | 1.3090 | 2.4204 | | 2.0339 | 3.3827 | 2.7406 | 1.0245 | H4 | 1.0924 | 2.1362 | 2.0339 | | 2.4719 | 3.1094 | 2.8799 | H5 | 2.1704 | 1.0839 | 3.3827 | 2.4719 | | 1.8573 | 3.5634 | H6 | 2.1649 | 1.0866 | 2.7406 | 3.1094 | 1.8573 | | 2.3709 | H7 | 1.9093 | 2.4883 | 1.0245 | 2.8799 | 3.5634 | 2.3709 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H5 |
121.531 |
|
C1 |
C2 |
H6 |
120.792 |
C1 |
N3 |
H7 |
109.207 |
|
C2 |
C1 |
N3 |
126.842 |
C2 |
C1 |
H4 |
117.684 |
|
N3 |
C1 |
H4 |
115.474 |
H5 |
C2 |
H6 |
117.677 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.053 |
|
|
|
2 |
C |
-0.453 |
|
|
|
3 |
N |
-0.456 |
|
|
|
4 |
H |
0.221 |
|
|
|
5 |
H |
0.232 |
|
|
|
6 |
H |
0.232 |
|
|
|
7 |
H |
0.276 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.134 |
-1.121 |
0.000 |
2.410 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.797 |
2.209 |
0.000 |
y |
2.209 |
-16.137 |
0.000 |
z |
0.000 |
0.000 |
-20.298 |
|
Traceless |
| x | y | z |
x |
-2.579 |
2.209 |
0.000 |
y |
2.209 |
4.410 |
0.000 |
z |
0.000 |
0.000 |
-1.831 |
|
Polar |
3z2-r2 | -3.662 |
x2-y2 | -4.660 |
xy | 2.209 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.236 |
-0.155 |
0.000 |
y |
-0.155 |
4.351 |
0.000 |
z |
0.000 |
0.000 |
2.246 |
<r2> (average value of r
2) Å
2
<r2> |
45.272 |
(<r2>)1/2 |
6.728 |