Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -207.831596 |
Energy at 298.15K | -207.837743 |
Nuclear repulsion energy | 117.020672 |
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 |
4084 |
3675 |
100.32 |
|
|
|
2 |
A |
3348 |
3013 |
26.12 |
|
|
|
3 |
A |
3328 |
2995 |
9.72 |
|
|
|
4 |
A |
3208 |
2887 |
33.70 |
|
|
|
5 |
A |
1905 |
1714 |
11.74 |
|
|
|
6 |
A |
1634 |
1471 |
15.55 |
|
|
|
7 |
A |
1580 |
1422 |
1.78 |
|
|
|
8 |
A |
1537 |
1383 |
38.80 |
|
|
|
9 |
A |
1388 |
1249 |
71.34 |
|
|
|
10 |
A |
1262 |
1135 |
9.00 |
|
|
|
11 |
A |
1105 |
994 |
119.09 |
|
|
|
12 |
A |
977 |
879 |
21.96 |
|
|
|
13 |
A |
594 |
535 |
18.92 |
|
|
|
14 |
A |
341 |
307 |
2.56 |
|
|
|
15 |
A |
3280 |
2951 |
38.91 |
|
|
|
16 |
A |
1634 |
1470 |
16.38 |
|
|
|
17 |
A |
1224 |
1102 |
2.40 |
|
|
|
18 |
A |
1027 |
924 |
20.81 |
|
|
|
19 |
A |
387 |
348 |
248.08 |
|
|
|
20 |
A |
315 |
284 |
2.48 |
|
|
|
21 |
A |
200 |
180 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17178.1 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15458.5 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 |
-1.282 |
1.338 |
0.000 |
C2 |
0.000 |
0.559 |
0.000 |
N3 |
-0.011 |
-0.710 |
0.000 |
O4 |
1.302 |
-1.242 |
0.000 |
H5 |
1.216 |
-2.191 |
0.000 |
H6 |
-2.134 |
0.674 |
0.000 |
H7 |
-1.334 |
1.977 |
0.875 |
H8 |
-1.334 |
1.977 |
-0.875 |
H9 |
0.936 |
1.093 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5001 | 2.4109 | 3.6514 | 4.3229 | 1.0803 | 1.0846 | 1.0846 | 2.2313 |
C2 | 1.5001 | | 1.2692 | 2.2221 | 3.0060 | 2.1375 | 2.1342 | 2.1342 | 1.0778 | N3 | 2.4109 | 1.2692 | | 1.4160 | 1.9220 | 2.5355 | 3.1203 | 3.1203 | 2.0369 | O4 | 3.6514 | 2.2221 | 1.4160 | | 0.9523 | 3.9346 | 4.2511 | 4.2511 | 2.3638 | H5 | 4.3229 | 3.0060 | 1.9220 | 0.9523 | | 4.4080 | 4.9628 | 4.9628 | 3.2956 | H6 | 1.0803 | 2.1375 | 2.5355 | 3.9346 | 4.4080 | | 1.7614 | 1.7614 | 3.0988 | H7 | 1.0846 | 2.1342 | 3.1203 | 4.2511 | 4.9628 | 1.7614 | | 1.7503 | 2.5879 | H8 | 1.0846 | 2.1342 | 3.1203 | 4.2511 | 4.9628 | 1.7614 | 1.7503 | | 2.5879 | H9 | 2.2313 | 1.0778 | 2.0369 | 2.3638 | 3.2956 | 3.0988 | 2.5879 | 2.5879 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
120.821 |
|
C1 |
C2 |
H9 |
118.977 |
C2 |
C1 |
H6 |
110.811 |
|
C2 |
C1 |
H7 |
110.281 |
C2 |
C1 |
H8 |
110.281 |
|
C2 |
N3 |
O4 |
111.580 |
N3 |
C2 |
H9 |
120.201 |
|
N3 |
O4 |
H5 |
106.860 |
H6 |
C1 |
H7 |
108.903 |
|
H6 |
C1 |
H8 |
108.903 |
H7 |
C1 |
H8 |
107.585 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.572 |
|
|
|
2 |
C |
-0.009 |
|
|
|
3 |
N |
-0.054 |
|
|
|
4 |
O |
-0.575 |
|
|
|
5 |
H |
0.414 |
|
|
|
6 |
H |
0.211 |
|
|
|
7 |
H |
0.190 |
|
|
|
8 |
H |
0.190 |
|
|
|
9 |
H |
0.205 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.614 |
1.058 |
0.000 |
1.223 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.508 |
-2.162 |
0.000 |
y |
-2.162 |
-18.257 |
0.000 |
z |
0.000 |
0.000 |
-25.431 |
|
Traceless |
| x | y | z |
x |
-4.664 |
-2.162 |
0.000 |
y |
-2.162 |
7.713 |
0.000 |
z |
0.000 |
0.000 |
-3.049 |
|
Polar |
3z2-r2 | -6.098 |
x2-y2 | -8.251 |
xy | -2.162 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.517 |
-1.266 |
0.000 |
y |
-1.266 |
6.616 |
0.000 |
z |
0.000 |
0.000 |
2.715 |
<r2> (average value of r
2) Å
2
<r2> |
92.783 |
(<r2>)1/2 |
9.632 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -207.831618 |
Energy at 298.15K | -207.837772 |
HF Energy | -207.831618 |
Nuclear repulsion energy | 119.550990 |
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' |
4086 |
3677 |
103.40 |
|
|
|
2 |
A' |
3389 |
3050 |
26.23 |
|
|
|
3 |
A' |
3361 |
3025 |
1.92 |
|
|
|
4 |
A' |
3211 |
2890 |
28.14 |
|
|
|
5 |
A' |
1915 |
1723 |
17.99 |
|
|
|
6 |
A' |
1630 |
1467 |
19.44 |
|
|
|
7 |
A' |
1571 |
1414 |
15.88 |
|
|
|
8 |
A' |
1492 |
1343 |
1.96 |
|
|
|
9 |
A' |
1449 |
1304 |
101.79 |
|
|
|
10 |
A' |
1251 |
1126 |
17.72 |
|
|
|
11 |
A' |
1028 |
925 |
111.33 |
|
|
|
12 |
A' |
973 |
875 |
25.68 |
|
|
|
13 |
A' |
719 |
647 |
16.38 |
|
|
|
14 |
A' |
325 |
293 |
2.53 |
|
|
|
15 |
A" |
3278 |
2950 |
35.72 |
|
|
|
16 |
A" |
1645 |
1480 |
19.33 |
|
|
|
17 |
A" |
1212 |
1090 |
1.12 |
|
|
|
18 |
A" |
983 |
885 |
9.52 |
|
|
|
19 |
A" |
526 |
473 |
19.19 |
|
|
|
20 |
A" |
407 |
366 |
217.91 |
|
|
|
21 |
A" |
59 |
53 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17254.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15527.1 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 |
-1.456 |
0.492 |
0.000 |
C2 |
0.000 |
0.865 |
0.000 |
N3 |
1.012 |
0.095 |
0.000 |
O4 |
0.672 |
-1.277 |
0.000 |
H5 |
1.494 |
-1.758 |
0.000 |
H6 |
-1.597 |
-0.576 |
0.000 |
H7 |
-1.940 |
0.914 |
0.875 |
H8 |
-1.940 |
0.914 |
-0.875 |
H9 |
0.255 |
1.908 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5033 | 2.5004 | 2.7678 | 3.7105 | 1.0772 | 1.0848 | 1.0848 | 2.2210 |
C2 | 1.5033 | | 1.2716 | 2.2444 | 3.0183 | 2.1506 | 2.1284 | 2.1284 | 1.0742 | N3 | 2.5004 | 1.2716 | | 1.4133 | 1.9146 | 2.6940 | 3.1859 | 3.1859 | 1.9650 | O4 | 2.7678 | 2.2444 | 1.4133 | | 0.9522 | 2.3750 | 3.5196 | 3.5196 | 3.2122 | H5 | 3.7105 | 3.0183 | 1.9146 | 0.9522 | | 3.3092 | 4.4379 | 4.4379 | 3.8699 | H6 | 1.0772 | 2.1506 | 2.6940 | 2.3750 | 3.3092 | | 1.7614 | 1.7614 | 3.0982 | H7 | 1.0848 | 2.1284 | 3.1859 | 3.5196 | 4.4379 | 1.7614 | | 1.7494 | 2.5630 | H8 | 1.0848 | 2.1284 | 3.1859 | 3.5196 | 4.4379 | 1.7614 | 1.7494 | | 2.5630 | H9 | 2.2210 | 1.0742 | 1.9650 | 3.2122 | 3.8699 | 3.0982 | 2.5630 | 2.5630 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
128.409 |
|
C1 |
C2 |
H9 |
118.062 |
C2 |
C1 |
H6 |
111.840 |
|
C2 |
C1 |
H7 |
109.589 |
C2 |
C1 |
H8 |
109.589 |
|
C2 |
N3 |
O4 |
113.326 |
N3 |
C2 |
H9 |
113.528 |
|
N3 |
O4 |
H5 |
106.436 |
H6 |
C1 |
H7 |
109.120 |
|
H6 |
C1 |
H8 |
109.120 |
H7 |
C1 |
H8 |
107.480 |
|
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 |
-0.593 |
|
|
|
2 |
C |
-0.047 |
|
|
|
3 |
N |
-0.031 |
|
|
|
4 |
O |
-0.588 |
|
|
|
5 |
H |
0.419 |
|
|
|
6 |
H |
0.248 |
|
|
|
7 |
H |
0.192 |
|
|
|
8 |
H |
0.192 |
|
|
|
9 |
H |
0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.871 |
0.634 |
0.000 |
1.077 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.426 |
-4.545 |
0.000 |
y |
-4.545 |
-21.315 |
0.000 |
z |
0.000 |
0.000 |
-25.516 |
|
Traceless |
| x | y | z |
x |
-0.011 |
-4.545 |
0.000 |
y |
-4.545 |
3.156 |
0.000 |
z |
0.000 |
0.000 |
-3.145 |
|
Polar |
3z2-r2 | -6.290 |
x2-y2 | -2.111 |
xy | -4.545 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.175 |
-1.409 |
0.000 |
y |
-1.409 |
5.710 |
0.000 |
z |
0.000 |
0.000 |
2.790 |
<r2> (average value of r
2) Å
2
<r2> |
79.822 |
(<r2>)1/2 |
8.934 |