Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -209.090137 |
| Energy at 298.15K | -209.096200 |
| Nuclear repulsion energy | 117.891709 |
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 B1B95/6-311G*
| 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 |
3843 |
3684 |
66.12 |
|
|
|
| 2 |
A |
3156 |
3026 |
16.85 |
|
|
|
| 3 |
A |
3110 |
2981 |
17.65 |
|
|
|
| 4 |
A |
3048 |
2922 |
22.11 |
|
|
|
| 5 |
A |
1765 |
1692 |
1.66 |
|
|
|
| 6 |
A |
1499 |
1437 |
15.94 |
|
|
|
| 7 |
A |
1468 |
1407 |
15.55 |
|
|
|
| 8 |
A |
1409 |
1351 |
30.87 |
|
|
|
| 9 |
A |
1307 |
1253 |
50.45 |
|
|
|
| 10 |
A |
1160 |
1112 |
3.17 |
|
|
|
| 11 |
A |
1042 |
998 |
157.26 |
|
|
|
| 12 |
A |
922 |
884 |
9.21 |
|
|
|
| 13 |
A |
571 |
547 |
14.40 |
|
|
|
| 14 |
A |
323 |
310 |
2.74 |
|
|
|
| 15 |
A |
3104 |
2976 |
19.74 |
|
|
|
| 16 |
A |
1491 |
1429 |
11.03 |
|
|
|
| 17 |
A |
1080 |
1035 |
0.58 |
|
|
|
| 18 |
A |
914 |
876 |
10.15 |
|
|
|
| 19 |
A |
434 |
416 |
162.71 |
|
|
|
| 20 |
A |
291 |
279 |
0.70 |
|
|
|
| 21 |
A |
207 |
199 |
0.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16071.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15405.9 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.290 |
1.298 |
0.000 |
| C2 |
0.000 |
0.560 |
0.000 |
| N3 |
0.007 |
-0.707 |
0.000 |
| O4 |
1.304 |
-1.205 |
0.000 |
| H5 |
1.176 |
-2.156 |
0.000 |
| H6 |
-2.126 |
0.600 |
0.000 |
| H7 |
-1.370 |
1.944 |
0.878 |
| H8 |
-1.370 |
1.944 |
-0.878 |
| H9 |
0.944 |
1.109 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4862 | 2.3883 | 3.6054 | 4.2447 | 1.0888 | 1.0931 | 1.0931 | 2.2417 |
C2 | 1.4862 | | 1.2672 | 2.1951 | 2.9604 | 2.1259 | 2.1364 | 2.1364 | 1.0916 | N3 | 2.3883 | 1.2672 | | 1.3897 | 1.8622 | 2.5015 | 3.1139 | 3.1139 | 2.0431 | O4 | 3.6054 | 2.1951 | 1.3897 | | 0.9599 | 3.8762 | 4.2241 | 4.2241 | 2.3420 | H5 | 4.2447 | 2.9604 | 1.8622 | 0.9599 | | 4.3013 | 4.9061 | 4.9061 | 3.2735 | H6 | 1.0888 | 2.1259 | 2.5015 | 3.8762 | 4.3013 | | 1.7739 | 1.7739 | 3.1110 | H7 | 1.0931 | 2.1364 | 3.1139 | 4.2241 | 4.9061 | 1.7739 | | 1.7570 | 2.6123 | H8 | 1.0931 | 2.1364 | 3.1139 | 4.2241 | 4.9061 | 1.7739 | 1.7570 | | 2.6123 | H9 | 2.2417 | 1.0916 | 2.0431 | 2.3420 | 3.2735 | 3.1110 | 2.6123 | 2.6123 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.104 |
|
C1 |
C2 |
H9 |
120.049 |
| C2 |
C1 |
H6 |
110.345 |
|
C2 |
C1 |
H7 |
110.929 |
| C2 |
C1 |
H8 |
110.929 |
|
C2 |
N3 |
O4 |
111.333 |
| N3 |
C2 |
H9 |
119.847 |
|
N3 |
O4 |
H5 |
103.331 |
| H6 |
C1 |
H7 |
108.785 |
|
H6 |
C1 |
H8 |
108.785 |
| H7 |
C1 |
H8 |
106.967 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.696 |
|
|
|
| 2 |
C |
-0.008 |
|
|
|
| 3 |
N |
-0.115 |
|
|
|
| 4 |
O |
-0.489 |
|
|
|
| 5 |
H |
0.410 |
|
|
|
| 6 |
H |
0.240 |
|
|
|
| 7 |
H |
0.231 |
|
|
|
| 8 |
H |
0.231 |
|
|
|
| 9 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.372 |
0.371 |
0.000 |
0.525 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.408 |
-2.213 |
0.000 |
| y |
-2.213 |
-18.310 |
0.000 |
| z |
0.000 |
0.000 |
-25.077 |
|
| Traceless |
| | x | y | z |
| x |
-3.715 |
-2.213 |
0.000 |
| y |
-2.213 |
6.932 |
0.000 |
| z |
0.000 |
0.000 |
-3.217 |
|
| Polar |
| 3z2-r2 | -6.435 |
| x2-y2 | -7.098 |
| xy | -2.213 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.323 |
-1.355 |
0.000 |
| y |
-1.355 |
6.905 |
0.000 |
| z |
0.000 |
0.000 |
3.250 |
<r2> (average value of r
2) Å
2
| <r2> |
90.858 |
| (<r2>)1/2 |
9.532 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -209.086139 |
| Energy at 298.15K | -209.092134 |
| HF Energy | -209.086139 |
| Nuclear repulsion energy | 120.623086 |
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 B1B95/6-311G*
| 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' |
3870 |
3710 |
69.29 |
|
|
|
| 2 |
A' |
3203 |
3071 |
8.36 |
|
|
|
| 3 |
A' |
3179 |
3047 |
9.73 |
|
|
|
| 4 |
A' |
3066 |
2939 |
14.82 |
|
|
|
| 5 |
A' |
1783 |
1709 |
9.35 |
|
|
|
| 6 |
A' |
1500 |
1438 |
24.93 |
|
|
|
| 7 |
A' |
1425 |
1366 |
36.27 |
|
|
|
| 8 |
A' |
1407 |
1349 |
32.20 |
|
|
|
| 9 |
A' |
1361 |
1305 |
32.48 |
|
|
|
| 10 |
A' |
1158 |
1111 |
8.66 |
|
|
|
| 11 |
A' |
973 |
933 |
149.09 |
|
|
|
| 12 |
A' |
934 |
896 |
2.36 |
|
|
|
| 13 |
A' |
686 |
658 |
12.89 |
|
|
|
| 14 |
A' |
316 |
303 |
1.56 |
|
|
|
| 15 |
A" |
3120 |
2990 |
16.62 |
|
|
|
| 16 |
A" |
1505 |
1443 |
12.63 |
|
|
|
| 17 |
A" |
1071 |
1027 |
0.40 |
|
|
|
| 18 |
A" |
871 |
835 |
15.09 |
|
|
|
| 19 |
A" |
519 |
497 |
54.95 |
|
|
|
| 20 |
A" |
408 |
391 |
98.36 |
|
|
|
| 21 |
A" |
31 |
30 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16194.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15523.8 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.438 |
0.478 |
0.000 |
| C2 |
0.000 |
0.858 |
0.000 |
| N3 |
1.009 |
0.089 |
0.000 |
| O4 |
0.655 |
-1.253 |
0.000 |
| H5 |
1.502 |
-1.700 |
0.000 |
| H6 |
-1.561 |
-0.601 |
0.000 |
| H7 |
-1.940 |
0.892 |
0.877 |
| H8 |
-1.940 |
0.892 |
-0.877 |
| H9 |
0.269 |
1.909 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4878 | 2.4783 | 2.7158 | 3.6590 | 1.0852 | 1.0920 | 1.0920 | 2.2288 |
C2 | 1.4878 | | 1.2686 | 2.2098 | 2.9663 | 2.1363 | 2.1293 | 2.1293 | 1.0859 | N3 | 2.4783 | 1.2686 | | 1.3880 | 1.8558 | 2.6612 | 3.1799 | 3.1799 | 1.9652 | O4 | 2.7158 | 2.2098 | 1.3880 | | 0.9581 | 2.3096 | 3.4787 | 3.4787 | 3.1859 | H5 | 3.6590 | 2.9663 | 1.8558 | 0.9581 | | 3.2543 | 4.3972 | 4.3972 | 3.8144 | H6 | 1.0852 | 2.1363 | 2.6612 | 2.3096 | 3.2543 | | 1.7721 | 1.7721 | 3.1068 | H7 | 1.0920 | 2.1293 | 3.1799 | 3.4787 | 4.3972 | 1.7721 | | 1.7540 | 2.5859 | H8 | 1.0920 | 2.1293 | 3.1799 | 3.4787 | 4.3972 | 1.7721 | 1.7540 | | 2.5859 | H9 | 2.2288 | 1.0859 | 1.9652 | 3.1859 | 3.8144 | 3.1068 | 2.5859 | 2.5859 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
127.901 |
|
C1 |
C2 |
H9 |
119.171 |
| C2 |
C1 |
H6 |
111.290 |
|
C2 |
C1 |
H7 |
110.314 |
| C2 |
C1 |
H8 |
110.314 |
|
C2 |
N3 |
O4 |
112.493 |
| N3 |
C2 |
H9 |
112.928 |
|
N3 |
O4 |
H5 |
103.034 |
| H6 |
C1 |
H7 |
108.972 |
|
H6 |
C1 |
H8 |
108.972 |
| H7 |
C1 |
H8 |
106.862 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.720 |
|
|
|
| 2 |
C |
-0.039 |
|
|
|
| 3 |
N |
-0.107 |
|
|
|
| 4 |
O |
-0.506 |
|
|
|
| 5 |
H |
0.417 |
|
|
|
| 6 |
H |
0.267 |
|
|
|
| 7 |
H |
0.235 |
|
|
|
| 8 |
H |
0.235 |
|
|
|
| 9 |
H |
0.217 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.501 |
0.124 |
0.000 |
0.516 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.728 |
-4.085 |
0.000 |
| y |
-4.085 |
-20.924 |
0.000 |
| z |
0.000 |
0.000 |
-25.078 |
|
| Traceless |
| | x | y | z |
| x |
0.273 |
-4.085 |
0.000 |
| y |
-4.085 |
2.978 |
0.000 |
| z |
0.000 |
0.000 |
-3.252 |
|
| Polar |
| 3z2-r2 | -6.504 |
| x2-y2 | -1.803 |
| xy | -4.085 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.747 |
-1.241 |
0.000 |
| y |
-1.241 |
5.863 |
0.000 |
| z |
0.000 |
0.000 |
3.247 |
<r2> (average value of r
2) Å
2
| <r2> |
77.998 |
| (<r2>)1/2 |
8.832 |