Jump to
S1C2
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.089476 |
| Energy at 298.15K | -209.095523 |
| Nuclear repulsion energy | 117.317215 |
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 B3PW91/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 |
3842 |
3706 |
92.35 |
|
|
|
| 2 |
A |
3153 |
3042 |
11.29 |
|
|
|
| 3 |
A |
3106 |
2996 |
14.24 |
|
|
|
| 4 |
A |
3036 |
2929 |
18.90 |
|
|
|
| 5 |
A |
1744 |
1682 |
0.47 |
|
|
|
| 6 |
A |
1455 |
1403 |
13.76 |
|
|
|
| 7 |
A |
1434 |
1383 |
8.37 |
|
|
|
| 8 |
A |
1373 |
1324 |
22.78 |
|
|
|
| 9 |
A |
1281 |
1236 |
48.26 |
|
|
|
| 10 |
A |
1149 |
1108 |
3.74 |
|
|
|
| 11 |
A |
1027 |
991 |
159.21 |
|
|
|
| 12 |
A |
910 |
878 |
10.28 |
|
|
|
| 13 |
A |
569 |
549 |
14.05 |
|
|
|
| 14 |
A |
323 |
312 |
3.45 |
|
|
|
| 15 |
A |
3100 |
2990 |
12.79 |
|
|
|
| 16 |
A |
1443 |
1392 |
9.04 |
|
|
|
| 17 |
A |
1060 |
1023 |
1.52 |
|
|
|
| 18 |
A |
902 |
870 |
9.10 |
|
|
|
| 19 |
A |
426 |
411 |
128.56 |
|
|
|
| 20 |
A |
289 |
279 |
0.12 |
|
|
|
| 21 |
A |
204 |
196 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15912.6 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 15349.3 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 B3PW91/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.295 |
1.303 |
0.000 |
| C2 |
0.000 |
0.565 |
0.000 |
| N3 |
0.007 |
-0.710 |
0.000 |
| O4 |
1.310 |
-1.212 |
0.000 |
| H5 |
1.174 |
-2.166 |
0.000 |
| H6 |
-2.136 |
0.599 |
0.000 |
| H7 |
-1.370 |
1.953 |
0.885 |
| H8 |
-1.370 |
1.953 |
-0.885 |
| H9 |
0.948 |
1.121 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4905 | 2.3973 | 3.6207 | 4.2579 | 1.0963 | 1.1006 | 1.1006 | 2.2503 |
C2 | 1.4905 | | 1.2754 | 2.2076 | 2.9730 | 2.1366 | 2.1414 | 2.1414 | 1.0987 | N3 | 2.3973 | 1.2754 | | 1.3962 | 1.8660 | 2.5117 | 3.1257 | 3.1257 | 2.0588 | O4 | 3.6207 | 2.2076 | 1.3962 | | 0.9640 | 3.8932 | 4.2403 | 4.2403 | 2.3609 | H5 | 4.2579 | 2.9730 | 1.8660 | 0.9640 | | 4.3136 | 4.9215 | 4.9215 | 3.2951 | H6 | 1.0963 | 2.1366 | 2.5117 | 3.8932 | 4.3136 | | 1.7893 | 1.7893 | 3.1279 | H7 | 1.1006 | 2.1414 | 3.1257 | 4.2403 | 4.9215 | 1.7893 | | 1.7699 | 2.6167 | H8 | 1.1006 | 2.1414 | 3.1257 | 4.2403 | 4.9215 | 1.7893 | 1.7699 | | 2.6167 | H9 | 2.2503 | 1.0987 | 2.0588 | 2.3609 | 3.2951 | 3.1279 | 2.6167 | 2.6167 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
119.963 |
|
C1 |
C2 |
H9 |
119.949 |
| C2 |
C1 |
H6 |
110.451 |
|
C2 |
C1 |
H7 |
110.569 |
| C2 |
C1 |
H8 |
110.569 |
|
C2 |
N3 |
O4 |
111.368 |
| N3 |
C2 |
H9 |
120.088 |
|
N3 |
O4 |
H5 |
102.952 |
| H6 |
C1 |
H7 |
109.067 |
|
H6 |
C1 |
H8 |
109.067 |
| H7 |
C1 |
H8 |
107.036 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.236 |
|
|
|
| 2 |
C |
0.771 |
|
|
|
| 3 |
N |
-0.212 |
|
|
|
| 4 |
O |
-0.395 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
-0.118 |
|
|
|
| 7 |
H |
-0.052 |
|
|
|
| 8 |
H |
-0.052 |
|
|
|
| 9 |
H |
-0.304 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.378 |
0.709 |
0.000 |
0.803 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.452 |
-2.101 |
0.000 |
| y |
-2.101 |
-19.049 |
0.000 |
| z |
0.000 |
0.000 |
-25.378 |
|
| Traceless |
| | x | y | z |
| x |
-3.238 |
-2.101 |
0.000 |
| y |
-2.101 |
6.366 |
0.000 |
| z |
0.000 |
0.000 |
-3.127 |
|
| Polar |
| 3z2-r2 | -6.254 |
| x2-y2 | -6.403 |
| xy | -2.101 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.463 |
-1.453 |
0.000 |
| y |
-1.453 |
7.777 |
0.000 |
| z |
0.000 |
0.000 |
4.492 |
<r2> (average value of r
2) Å
2
| <r2> |
91.813 |
| (<r2>)1/2 |
9.582 |
Jump to
S1C1
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -209.088749 |
| Energy at 298.15K | |
| HF Energy | -209.088749 |
| Nuclear repulsion energy | 119.768346 |
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 B3PW91/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' |
3847 |
3710 |
92.86 |
|
|
|
| 2 |
A' |
3183 |
3070 |
7.54 |
|
|
|
| 3 |
A' |
3163 |
3052 |
4.10 |
|
|
|
| 4 |
A' |
3043 |
2936 |
12.90 |
|
|
|
| 5 |
A' |
1750 |
1688 |
8.97 |
|
|
|
| 6 |
A' |
1448 |
1397 |
21.06 |
|
|
|
| 7 |
A' |
1383 |
1334 |
33.12 |
|
|
|
| 8 |
A' |
1368 |
1319 |
25.67 |
|
|
|
| 9 |
A' |
1331 |
1284 |
28.81 |
|
|
|
| 10 |
A' |
1138 |
1098 |
8.21 |
|
|
|
| 11 |
A' |
950 |
916 |
152.59 |
|
|
|
| 12 |
A' |
922 |
889 |
0.57 |
|
|
|
| 13 |
A' |
677 |
653 |
12.06 |
|
|
|
| 14 |
A' |
307 |
296 |
1.48 |
|
|
|
| 15 |
A" |
3105 |
2995 |
10.42 |
|
|
|
| 16 |
A" |
1450 |
1399 |
9.41 |
|
|
|
| 17 |
A" |
1044 |
1007 |
0.72 |
|
|
|
| 18 |
A" |
857 |
827 |
15.70 |
|
|
|
| 19 |
A" |
512 |
494 |
45.34 |
|
|
|
| 20 |
A" |
408 |
393 |
69.80 |
|
|
|
| 21 |
A" |
21i |
20i |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15931.3 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 15367.4 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 B3PW91/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.448 |
0.494 |
0.000 |
| C2 |
0.000 |
0.858 |
0.000 |
| N3 |
1.016 |
0.082 |
0.000 |
| O4 |
0.658 |
-1.269 |
0.000 |
| H5 |
1.515 |
-1.710 |
0.000 |
| H6 |
-1.592 |
-0.590 |
0.000 |
| H7 |
-1.942 |
0.924 |
0.884 |
| H8 |
-1.942 |
0.924 |
-0.884 |
| H9 |
0.279 |
1.916 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4933 | 2.4978 | 2.7460 | 3.6922 | 1.0935 | 1.1003 | 1.1003 | 2.2374 |
C2 | 1.4933 | | 1.2782 | 2.2263 | 2.9814 | 2.1527 | 2.1350 | 2.1350 | 1.0939 | N3 | 2.4978 | 1.2782 | | 1.3972 | 1.8600 | 2.6932 | 3.1999 | 3.1999 | 1.9763 | O4 | 2.7460 | 2.2263 | 1.3972 | | 0.9636 | 2.3502 | 3.5143 | 3.5143 | 3.2070 | H5 | 3.6922 | 2.9814 | 1.8600 | 0.9636 | | 3.3025 | 4.4349 | 4.4349 | 3.8305 | H6 | 1.0935 | 2.1527 | 2.6932 | 2.3502 | 3.3025 | | 1.7880 | 1.7880 | 3.1279 | H7 | 1.1003 | 2.1350 | 3.1999 | 3.5143 | 4.4349 | 1.7880 | | 1.7677 | 2.5884 | H8 | 1.1003 | 2.1350 | 3.1999 | 3.5143 | 4.4349 | 1.7880 | 1.7677 | | 2.5884 | H9 | 2.2374 | 1.0939 | 1.9763 | 3.2070 | 3.8305 | 3.1279 | 2.5884 | 2.5884 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.477 |
|
C1 |
C2 |
H9 |
118.910 |
| C2 |
C1 |
H6 |
111.715 |
|
C2 |
C1 |
H7 |
109.882 |
| C2 |
C1 |
H8 |
109.882 |
|
C2 |
N3 |
O4 |
112.557 |
| N3 |
C2 |
H9 |
112.613 |
|
N3 |
O4 |
H5 |
102.412 |
| H6 |
C1 |
H7 |
109.176 |
|
H6 |
C1 |
H8 |
109.176 |
| H7 |
C1 |
H8 |
106.884 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.384 |
|
|
|
| 2 |
C |
0.595 |
|
|
|
| 3 |
N |
-0.123 |
|
|
|
| 4 |
O |
-0.432 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
| 6 |
H |
-0.124 |
|
|
|
| 7 |
H |
-0.062 |
|
|
|
| 8 |
H |
-0.062 |
|
|
|
| 9 |
H |
-0.311 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.851 |
0.237 |
0.000 |
0.883 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.326 |
-3.853 |
0.000 |
| y |
-3.853 |
-21.344 |
0.000 |
| z |
0.000 |
0.000 |
-25.405 |
|
| Traceless |
| | x | y | z |
| x |
0.048 |
-3.853 |
0.000 |
| y |
-3.853 |
3.022 |
0.000 |
| z |
0.000 |
0.000 |
-3.070 |
|
| Polar |
| 3z2-r2 | -6.140 |
| x2-y2 | -1.983 |
| xy | -3.853 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.901 |
-1.139 |
0.000 |
| y |
-1.139 |
6.869 |
0.000 |
| z |
0.000 |
0.000 |
4.490 |
<r2> (average value of r
2) Å
2
| <r2> |
79.322 |
| (<r2>)1/2 |
8.906 |