Jump to
S1C2
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.075609 |
| Energy at 298.15K | -209.081667 |
| 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 B1B95/aug-cc-pVDZ
| 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 |
3879 |
3716 |
97.37 |
|
|
|
| 2 |
A |
3177 |
3043 |
10.59 |
|
|
|
| 3 |
A |
3128 |
2996 |
13.64 |
|
|
|
| 4 |
A |
3060 |
2931 |
17.86 |
|
|
|
| 5 |
A |
1769 |
1695 |
0.69 |
|
|
|
| 6 |
A |
1459 |
1398 |
13.79 |
|
|
|
| 7 |
A |
1440 |
1380 |
7.60 |
|
|
|
| 8 |
A |
1375 |
1317 |
24.65 |
|
|
|
| 9 |
A |
1287 |
1233 |
49.25 |
|
|
|
| 10 |
A |
1154 |
1105 |
3.59 |
|
|
|
| 11 |
A |
1041 |
997 |
159.93 |
|
|
|
| 12 |
A |
914 |
875 |
8.08 |
|
|
|
| 13 |
A |
571 |
547 |
13.77 |
|
|
|
| 14 |
A |
321 |
308 |
3.34 |
|
|
|
| 15 |
A |
3126 |
2995 |
12.18 |
|
|
|
| 16 |
A |
1447 |
1386 |
8.91 |
|
|
|
| 17 |
A |
1064 |
1020 |
1.62 |
|
|
|
| 18 |
A |
905 |
867 |
8.68 |
|
|
|
| 19 |
A |
426 |
408 |
130.17 |
|
|
|
| 20 |
A |
291 |
279 |
0.14 |
|
|
|
| 21 |
A |
206 |
197 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16020.1 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15345.6 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.291 |
1.298 |
0.000 |
| C2 |
0.000 |
0.562 |
0.000 |
| N3 |
0.006 |
-0.709 |
0.000 |
| O4 |
1.305 |
-1.206 |
0.000 |
| H5 |
1.175 |
-2.158 |
0.000 |
| H6 |
-2.128 |
0.595 |
0.000 |
| H7 |
-1.366 |
1.946 |
0.883 |
| H8 |
-1.366 |
1.946 |
-0.883 |
| H9 |
0.948 |
1.112 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4860 | 2.3896 | 3.6067 | 4.2456 | 1.0931 | 1.0972 | 1.0972 | 2.2461 |
C2 | 1.4860 | | 1.2709 | 2.1975 | 2.9630 | 2.1280 | 2.1350 | 2.1350 | 1.0956 | N3 | 2.3896 | 1.2709 | | 1.3905 | 1.8617 | 2.5008 | 3.1156 | 3.1156 | 2.0498 | O4 | 3.6067 | 2.1975 | 1.3905 | | 0.9608 | 3.8764 | 4.2241 | 4.2241 | 2.3456 | H5 | 4.2456 | 2.9630 | 1.8617 | 0.9608 | | 4.2996 | 4.9065 | 4.9065 | 3.2781 | H6 | 1.0931 | 2.1280 | 2.5008 | 3.8764 | 4.2996 | | 1.7844 | 1.7844 | 3.1185 | H7 | 1.0972 | 2.1350 | 3.1156 | 4.2241 | 4.9065 | 1.7844 | | 1.7652 | 2.6124 | H8 | 1.0972 | 2.1350 | 3.1156 | 4.2241 | 4.9065 | 1.7844 | 1.7652 | | 2.6124 | H9 | 2.2461 | 1.0956 | 2.0498 | 2.3456 | 3.2781 | 3.1185 | 2.6124 | 2.6124 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
119.976 |
|
C1 |
C2 |
H9 |
120.171 |
| C2 |
C1 |
H6 |
110.270 |
|
C2 |
C1 |
H7 |
110.580 |
| C2 |
C1 |
H8 |
110.580 |
|
C2 |
N3 |
O4 |
111.239 |
| N3 |
C2 |
H9 |
119.853 |
|
N3 |
O4 |
H5 |
103.187 |
| H6 |
C1 |
H7 |
109.115 |
|
H6 |
C1 |
H8 |
109.115 |
| H7 |
C1 |
H8 |
107.108 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.367 |
|
|
|
| 2 |
C |
0.802 |
|
|
|
| 3 |
N |
-0.206 |
|
|
|
| 4 |
O |
-0.377 |
|
|
|
| 5 |
H |
0.113 |
|
|
|
| 6 |
H |
-0.159 |
|
|
|
| 7 |
H |
-0.089 |
|
|
|
| 8 |
H |
-0.089 |
|
|
|
| 9 |
H |
-0.362 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.380 |
0.695 |
0.000 |
0.792 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.474 |
-2.093 |
0.000 |
| y |
-2.093 |
-19.064 |
0.000 |
| z |
0.000 |
0.000 |
-25.361 |
|
| Traceless |
| | x | y | z |
| x |
-3.262 |
-2.093 |
0.000 |
| y |
-2.093 |
6.353 |
0.000 |
| z |
0.000 |
0.000 |
-3.092 |
|
| Polar |
| 3z2-r2 | -6.183 |
| x2-y2 | -6.410 |
| xy | -2.093 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.395 |
-1.421 |
0.000 |
| y |
-1.421 |
7.685 |
0.000 |
| z |
0.000 |
0.000 |
4.455 |
<r2> (average value of r
2) Å
2
| <r2> |
91.243 |
| (<r2>)1/2 |
9.552 |
Jump to
S1C1
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.075172 |
| Energy at 298.15K | -209.081110 |
| HF Energy | -209.075172 |
| Nuclear repulsion energy | 120.293141 |
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/aug-cc-pVDZ
| 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' |
3884 |
3720 |
98.40 |
|
|
|
| 2 |
A' |
3209 |
3074 |
6.15 |
|
|
|
| 3 |
A' |
3187 |
3053 |
5.19 |
|
|
|
| 4 |
A' |
3068 |
2938 |
12.24 |
|
|
|
| 5 |
A' |
1775 |
1700 |
9.58 |
|
|
|
| 6 |
A' |
1451 |
1390 |
20.81 |
|
|
|
| 7 |
A' |
1388 |
1330 |
35.74 |
|
|
|
| 8 |
A' |
1372 |
1314 |
26.65 |
|
|
|
| 9 |
A' |
1336 |
1280 |
26.58 |
|
|
|
| 10 |
A' |
1142 |
1094 |
7.79 |
|
|
|
| 11 |
A' |
964 |
924 |
147.47 |
|
|
|
| 12 |
A' |
930 |
890 |
4.26 |
|
|
|
| 13 |
A' |
677 |
649 |
12.12 |
|
|
|
| 14 |
A' |
306 |
293 |
1.49 |
|
|
|
| 15 |
A" |
3131 |
2999 |
9.87 |
|
|
|
| 16 |
A" |
1455 |
1394 |
9.28 |
|
|
|
| 17 |
A" |
1048 |
1004 |
0.81 |
|
|
|
| 18 |
A" |
863 |
826 |
14.70 |
|
|
|
| 19 |
A" |
513 |
491 |
46.27 |
|
|
|
| 20 |
A" |
411 |
394 |
70.85 |
|
|
|
| 21 |
A" |
12 |
11 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16059.6 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 15383.5 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 B1B95/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.441 |
0.484 |
0.000 |
| C2 |
0.000 |
0.858 |
0.000 |
| N3 |
1.013 |
0.085 |
0.000 |
| O4 |
0.653 |
-1.259 |
0.000 |
| H5 |
1.504 |
-1.704 |
0.000 |
| H6 |
-1.572 |
-0.599 |
0.000 |
| H7 |
-1.937 |
0.908 |
0.882 |
| H8 |
-1.937 |
0.908 |
-0.882 |
| H9 |
0.275 |
1.913 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4887 | 2.4857 | 2.7244 | 3.6689 | 1.0904 | 1.0969 | 1.0969 | 2.2332 |
C2 | 1.4887 | | 1.2738 | 2.2152 | 2.9709 | 2.1430 | 2.1285 | 2.1285 | 1.0907 | N3 | 2.4857 | 1.2738 | | 1.3911 | 1.8554 | 2.6733 | 3.1864 | 3.1864 | 1.9717 | O4 | 2.7244 | 2.2152 | 1.3911 | | 0.9605 | 2.3210 | 3.4902 | 3.4902 | 3.1948 | H5 | 3.6689 | 2.9709 | 1.8554 | 0.9605 | | 3.2688 | 4.4093 | 4.4093 | 3.8207 | H6 | 1.0904 | 2.1430 | 2.6733 | 2.3210 | 3.2688 | | 1.7836 | 1.7836 | 3.1178 | H7 | 1.0969 | 2.1285 | 3.1864 | 3.4902 | 4.4093 | 1.7836 | | 1.7631 | 2.5842 | H8 | 1.0969 | 2.1285 | 3.1864 | 3.4902 | 4.4093 | 1.7836 | 1.7631 | | 2.5842 | H9 | 2.2332 | 1.0907 | 1.9717 | 3.1948 | 3.8207 | 3.1178 | 2.5842 | 2.5842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.095 |
|
C1 |
C2 |
H9 |
119.139 |
| C2 |
C1 |
H6 |
111.451 |
|
C2 |
C1 |
H7 |
109.898 |
| C2 |
C1 |
H8 |
109.898 |
|
C2 |
N3 |
O4 |
112.382 |
| N3 |
C2 |
H9 |
112.766 |
|
N3 |
O4 |
H5 |
102.637 |
| H6 |
C1 |
H7 |
109.259 |
|
H6 |
C1 |
H8 |
109.259 |
| H7 |
C1 |
H8 |
106.967 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.523 |
|
|
|
| 2 |
C |
0.618 |
|
|
|
| 3 |
N |
-0.111 |
|
|
|
| 4 |
O |
-0.414 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
-0.178 |
|
|
|
| 7 |
H |
-0.101 |
|
|
|
| 8 |
H |
-0.101 |
|
|
|
| 9 |
H |
-0.355 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.828 |
0.227 |
0.000 |
0.858 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.345 |
-3.843 |
0.000 |
| y |
-3.843 |
-21.351 |
0.000 |
| z |
0.000 |
0.000 |
-25.388 |
|
| Traceless |
| | x | y | z |
| x |
0.024 |
-3.843 |
0.000 |
| y |
-3.843 |
3.016 |
0.000 |
| z |
0.000 |
0.000 |
-3.040 |
|
| Polar |
| 3z2-r2 | -6.080 |
| x2-y2 | -1.994 |
| xy | -3.843 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.821 |
-1.109 |
0.000 |
| y |
-1.109 |
6.785 |
0.000 |
| z |
0.000 |
0.000 |
4.451 |
<r2> (average value of r
2) Å
2
| <r2> |
78.626 |
| (<r2>)1/2 |
8.867 |