Jump to
S1C2
Energy calculated at B3PW91/3-21G
| hartrees |
Energy at 0K | -207.897018 |
Energy at 298.15K | -207.902969 |
Nuclear repulsion energy | 115.369657 |
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 B3PW91/3-21G
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 |
3533 |
3396 |
27.95 |
|
|
|
2 |
A |
3161 |
3038 |
11.31 |
|
|
|
3 |
A |
3140 |
3018 |
3.08 |
|
|
|
4 |
A |
3052 |
2933 |
12.30 |
|
|
|
5 |
A |
1682 |
1617 |
2.42 |
|
|
|
6 |
A |
1534 |
1474 |
11.59 |
|
|
|
7 |
A |
1452 |
1395 |
8.97 |
|
|
|
8 |
A |
1415 |
1360 |
30.50 |
|
|
|
9 |
A |
1280 |
1230 |
49.13 |
|
|
|
10 |
A |
1158 |
1113 |
10.23 |
|
|
|
11 |
A |
1003 |
964 |
90.32 |
|
|
|
12 |
A |
907 |
872 |
14.52 |
|
|
|
13 |
A |
544 |
523 |
15.48 |
|
|
|
14 |
A |
310 |
298 |
2.54 |
|
|
|
15 |
A |
3107 |
2986 |
11.06 |
|
|
|
16 |
A |
1542 |
1482 |
14.28 |
|
|
|
17 |
A |
1107 |
1064 |
0.00 |
|
|
|
18 |
A |
931 |
895 |
26.60 |
|
|
|
19 |
A |
374 |
359 |
160.46 |
|
|
|
20 |
A |
276 |
266 |
5.18 |
|
|
|
21 |
A |
205 |
197 |
0.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15855.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15240.2 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.273 |
1.354 |
0.000 |
C2 |
0.000 |
0.563 |
0.000 |
N3 |
-0.046 |
-0.720 |
0.000 |
O4 |
1.331 |
-1.250 |
0.000 |
H5 |
1.149 |
-2.227 |
0.000 |
H6 |
-2.132 |
0.677 |
0.000 |
H7 |
-1.325 |
2.000 |
0.887 |
H8 |
-1.325 |
2.000 |
-0.887 |
H9 |
0.952 |
1.093 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4991 | 2.4102 | 3.6829 | 4.3231 | 1.0936 | 1.0978 | 1.0978 | 2.2407 |
C2 | 1.4991 | | 1.2840 | 2.2491 | 3.0169 | 2.1349 | 2.1462 | 2.1462 | 1.0897 | N3 | 2.4102 | 1.2840 | | 1.4754 | 1.9229 | 2.5103 | 3.1336 | 3.1336 | 2.0700 | O4 | 3.6829 | 2.2491 | 1.4754 | | 0.9931 | 3.9626 | 4.2897 | 4.2897 | 2.3738 | H5 | 4.3231 | 3.0169 | 1.9229 | 0.9931 | | 4.3810 | 4.9767 | 4.9767 | 3.3255 | H6 | 1.0936 | 2.1349 | 2.5103 | 3.9626 | 4.3810 | | 1.7851 | 1.7851 | 3.1119 | H7 | 1.0978 | 2.1462 | 3.1336 | 4.2897 | 4.9767 | 1.7851 | | 1.7732 | 2.6065 | H8 | 1.0978 | 2.1462 | 3.1336 | 4.2897 | 4.9767 | 1.7851 | 1.7732 | | 2.6065 | H9 | 2.2407 | 1.0897 | 2.0700 | 2.3738 | 3.3255 | 3.1119 | 2.6065 | 2.6065 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
119.795 |
|
C1 |
C2 |
H9 |
119.033 |
C2 |
C1 |
H6 |
109.866 |
|
C2 |
C1 |
H7 |
110.513 |
C2 |
C1 |
H8 |
110.513 |
|
C2 |
N3 |
O4 |
108.993 |
N3 |
C2 |
H9 |
121.171 |
|
N3 |
O4 |
H5 |
100.510 |
H6 |
C1 |
H7 |
109.090 |
|
H6 |
C1 |
H8 |
109.090 |
H7 |
C1 |
H8 |
107.721 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.453 |
|
|
|
2 |
H |
0.376 |
|
|
|
3 |
N |
-0.254 |
|
|
|
4 |
C |
0.068 |
|
|
|
5 |
H |
0.232 |
|
|
|
6 |
C |
-0.683 |
|
|
|
7 |
H |
0.245 |
|
|
|
8 |
H |
0.234 |
|
|
|
9 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.475 |
0.516 |
0.000 |
0.701 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.074 |
-2.173 |
0.000 |
y |
-2.173 |
-17.835 |
0.000 |
z |
0.000 |
0.000 |
-24.812 |
|
Traceless |
| x | y | z |
x |
-3.751 |
-2.173 |
0.000 |
y |
-2.173 |
7.108 |
0.000 |
z |
0.000 |
0.000 |
-3.357 |
|
Polar |
3z2-r2 | -6.714 |
x2-y2 | -7.239 |
xy | -2.173 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
93.511 |
(<r2>)1/2 |
9.670 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G
| hartrees |
Energy at 0K | -207.898325 |
Energy at 298.15K | -207.904236 |
HF Energy | -207.898325 |
Nuclear repulsion energy | 118.220285 |
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 B3PW91/3-21G
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' |
3542 |
3405 |
27.85 |
|
|
|
2 |
A' |
3198 |
3074 |
2.80 |
|
|
|
3 |
A' |
3166 |
3043 |
10.96 |
|
|
|
4 |
A' |
3057 |
2938 |
8.78 |
|
|
|
5 |
A' |
1692 |
1626 |
2.95 |
|
|
|
6 |
A' |
1530 |
1471 |
17.65 |
|
|
|
7 |
A' |
1442 |
1386 |
28.13 |
|
|
|
8 |
A' |
1378 |
1325 |
1.28 |
|
|
|
9 |
A' |
1339 |
1287 |
72.12 |
|
|
|
10 |
A' |
1155 |
1110 |
16.87 |
|
|
|
11 |
A' |
934 |
898 |
73.66 |
|
|
|
12 |
A' |
901 |
866 |
34.51 |
|
|
|
13 |
A' |
667 |
642 |
12.80 |
|
|
|
14 |
A' |
308 |
296 |
2.38 |
|
|
|
15 |
A" |
3107 |
2987 |
9.78 |
|
|
|
16 |
A" |
1554 |
1493 |
17.14 |
|
|
|
17 |
A" |
1103 |
1060 |
|
|
|
|
18 |
A" |
878 |
844 |
19.22 |
|
|
|
19 |
A" |
489 |
470 |
24.51 |
|
|
|
20 |
A" |
355 |
341 |
128.46 |
|
|
|
21 |
A" |
41 |
39 |
0.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15916.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15299.3 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 B3PW91/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.442 |
0.478 |
0.000 |
C2 |
0.000 |
0.883 |
0.000 |
N3 |
1.035 |
0.121 |
0.000 |
O4 |
0.633 |
-1.298 |
0.000 |
H5 |
1.524 |
-1.733 |
0.000 |
H6 |
-1.521 |
-0.609 |
0.000 |
H7 |
-1.949 |
0.883 |
0.886 |
H8 |
-1.949 |
0.883 |
-0.886 |
H9 |
0.238 |
1.945 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4979 | 2.5031 | 2.7309 | 3.7000 | 1.0902 | 1.0979 | 1.0979 | 2.2304 |
C2 | 1.4979 | | 1.2858 | 2.2710 | 3.0283 | 2.1310 | 2.1410 | 2.1410 | 1.0883 | N3 | 2.5031 | 1.2858 | | 1.4749 | 1.9177 | 2.6587 | 3.2053 | 3.2053 | 1.9910 | O4 | 2.7309 | 2.2710 | 1.4749 | | 0.9925 | 2.2610 | 3.4938 | 3.4938 | 3.2670 | H5 | 3.7000 | 3.0283 | 1.9177 | 0.9925 | | 3.2462 | 4.4381 | 4.4381 | 3.8971 | H6 | 1.0902 | 2.1310 | 2.6587 | 2.2610 | 3.2462 | | 1.7873 | 1.7873 | 3.1015 | H7 | 1.0979 | 2.1410 | 3.2053 | 3.4938 | 4.4381 | 1.7873 | | 1.7711 | 2.5878 | H8 | 1.0979 | 2.1410 | 3.2053 | 3.4938 | 4.4381 | 1.7873 | 1.7711 | | 2.5878 | H9 | 2.2304 | 1.0883 | 1.9910 | 3.2670 | 3.8971 | 3.1015 | 2.5878 | 2.5878 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
127.943 |
|
C1 |
C2 |
H9 |
118.325 |
C2 |
C1 |
H6 |
109.849 |
|
C2 |
C1 |
H7 |
110.183 |
C2 |
C1 |
H8 |
110.183 |
|
C2 |
N3 |
O4 |
110.508 |
N3 |
C2 |
H9 |
113.732 |
|
N3 |
O4 |
H5 |
100.175 |
H6 |
C1 |
H7 |
109.535 |
|
H6 |
C1 |
H8 |
109.535 |
H7 |
C1 |
H8 |
107.518 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.700 |
|
|
|
2 |
C |
0.056 |
|
|
|
3 |
N |
-0.253 |
|
|
|
4 |
O |
-0.456 |
|
|
|
5 |
H |
0.380 |
|
|
|
6 |
H |
0.266 |
|
|
|
7 |
H |
0.233 |
|
|
|
8 |
H |
0.233 |
|
|
|
9 |
H |
0.240 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.507 |
0.240 |
0.000 |
0.561 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.372 |
-4.030 |
0.000 |
y |
-4.030 |
-20.569 |
0.000 |
z |
0.000 |
0.000 |
-24.839 |
|
Traceless |
| x | y | z |
x |
0.333 |
-4.030 |
0.000 |
y |
-4.030 |
3.036 |
0.000 |
z |
0.000 |
0.000 |
-3.369 |
|
Polar |
3z2-r2 | -6.738 |
x2-y2 | -1.802 |
xy | -4.030 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.197 |
-1.360 |
0.000 |
y |
-1.360 |
5.625 |
0.000 |
z |
0.000 |
0.000 |
2.445 |
<r2> (average value of r
2) Å
2
<r2> |
79.507 |
(<r2>)1/2 |
8.917 |