Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.119728 |
| Energy at 298.15K | -209.125788 |
| Nuclear repulsion energy | 118.149712 |
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/cc-pVTZ
| 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 |
3885 |
3718 |
95.92 |
|
|
|
| 2 |
A |
3164 |
3028 |
11.50 |
|
|
|
| 3 |
A |
3117 |
2983 |
14.54 |
|
|
|
| 4 |
A |
3054 |
2923 |
17.56 |
|
|
|
| 5 |
A |
1768 |
1692 |
1.07 |
|
|
|
| 6 |
A |
1482 |
1418 |
11.75 |
|
|
|
| 7 |
A |
1449 |
1387 |
8.47 |
|
|
|
| 8 |
A |
1397 |
1337 |
22.84 |
|
|
|
| 9 |
A |
1294 |
1238 |
54.64 |
|
|
|
| 10 |
A |
1158 |
1108 |
3.57 |
|
|
|
| 11 |
A |
1041 |
996 |
159.14 |
|
|
|
| 12 |
A |
919 |
880 |
8.30 |
|
|
|
| 13 |
A |
570 |
546 |
13.41 |
|
|
|
| 14 |
A |
323 |
309 |
3.18 |
|
|
|
| 15 |
A |
3110 |
2976 |
13.46 |
|
|
|
| 16 |
A |
1476 |
1413 |
8.34 |
|
|
|
| 17 |
A |
1081 |
1035 |
1.25 |
|
|
|
| 18 |
A |
919 |
880 |
8.84 |
|
|
|
| 19 |
A |
413 |
395 |
128.35 |
|
|
|
| 20 |
A |
293 |
280 |
0.52 |
|
|
|
| 21 |
A |
206 |
198 |
0.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16058.6 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 15369.7 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.288 |
1.295 |
0.000 |
| C2 |
0.000 |
0.560 |
0.000 |
| N3 |
0.007 |
-0.704 |
0.000 |
| O4 |
1.302 |
-1.205 |
0.000 |
| H5 |
1.164 |
-2.152 |
0.000 |
| H6 |
-2.119 |
0.598 |
0.000 |
| H7 |
-1.364 |
1.939 |
0.876 |
| H8 |
-1.364 |
1.939 |
-0.876 |
| H9 |
0.939 |
1.108 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4829 | 2.3814 | 3.5996 | 4.2302 | 1.0854 | 1.0899 | 1.0899 | 2.2346 |
C2 | 1.4829 | | 1.2632 | 2.1929 | 2.9510 | 2.1198 | 2.1283 | 2.1283 | 1.0878 | N3 | 2.3814 | 1.2632 | | 1.3890 | 1.8539 | 2.4932 | 3.1031 | 3.1031 | 2.0376 | O4 | 3.5996 | 2.1929 | 1.3890 | | 0.9576 | 3.8677 | 4.2139 | 4.2139 | 2.3412 | H5 | 4.2302 | 2.9510 | 1.8539 | 0.9576 | | 4.2831 | 4.8881 | 4.8881 | 3.2681 | H6 | 1.0854 | 2.1198 | 2.4932 | 3.8677 | 4.2831 | | 1.7711 | 1.7711 | 3.1009 | H7 | 1.0899 | 2.1283 | 3.1031 | 4.2139 | 4.8881 | 1.7711 | | 1.7523 | 2.6001 | H8 | 1.0899 | 2.1283 | 3.1031 | 4.2139 | 4.8881 | 1.7711 | 1.7523 | | 2.6001 | H9 | 2.2346 | 1.0878 | 2.0376 | 2.3412 | 3.2681 | 3.1009 | 2.6001 | 2.6001 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.061 |
|
C1 |
C2 |
H9 |
119.963 |
| C2 |
C1 |
H6 |
110.291 |
|
C2 |
C1 |
H7 |
110.708 |
| C2 |
C1 |
H8 |
110.708 |
|
C2 |
N3 |
O4 |
111.458 |
| N3 |
C2 |
H9 |
119.977 |
|
N3 |
O4 |
H5 |
102.834 |
| H6 |
C1 |
H7 |
109.019 |
|
H6 |
C1 |
H8 |
109.019 |
| H7 |
C1 |
H8 |
107.015 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.316 |
|
|
|
| 2 |
C |
-0.044 |
|
|
|
| 3 |
N |
-0.061 |
|
|
|
| 4 |
O |
-0.255 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
| 6 |
H |
0.124 |
|
|
|
| 7 |
H |
0.117 |
|
|
|
| 8 |
H |
0.117 |
|
|
|
| 9 |
H |
0.094 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.340 |
0.556 |
0.000 |
0.652 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.146 |
-2.075 |
0.000 |
| y |
-2.075 |
-18.726 |
0.000 |
| z |
0.000 |
0.000 |
-24.982 |
|
| Traceless |
| | x | y | z |
| x |
-3.292 |
-2.075 |
0.000 |
| y |
-2.075 |
6.339 |
0.000 |
| z |
0.000 |
0.000 |
-3.047 |
|
| Polar |
| 3z2-r2 | -6.093 |
| x2-y2 | -6.421 |
| xy | -2.075 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.798 |
-1.384 |
0.000 |
| y |
-1.384 |
7.195 |
0.000 |
| z |
0.000 |
0.000 |
3.800 |
<r2> (average value of r
2) Å
2
| <r2> |
90.592 |
| (<r2>)1/2 |
9.518 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.119256 |
| Energy at 298.15K | -209.125242 |
| HF Energy | -209.119256 |
| Nuclear repulsion energy | 120.723594 |
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/cc-pVTZ
| 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' |
3888 |
3721 |
97.60 |
|
|
|
| 2 |
A' |
3194 |
3057 |
6.73 |
|
|
|
| 3 |
A' |
3172 |
3035 |
6.47 |
|
|
|
| 4 |
A' |
3061 |
2930 |
11.79 |
|
|
|
| 5 |
A' |
1771 |
1695 |
8.30 |
|
|
|
| 6 |
A' |
1476 |
1413 |
17.74 |
|
|
|
| 7 |
A' |
1402 |
1342 |
26.06 |
|
|
|
| 8 |
A' |
1383 |
1324 |
28.94 |
|
|
|
| 9 |
A' |
1346 |
1288 |
38.28 |
|
|
|
| 10 |
A' |
1146 |
1097 |
9.45 |
|
|
|
| 11 |
A' |
966 |
925 |
146.55 |
|
|
|
| 12 |
A' |
928 |
888 |
3.17 |
|
|
|
| 13 |
A' |
678 |
649 |
12.76 |
|
|
|
| 14 |
A' |
304 |
291 |
1.37 |
|
|
|
| 15 |
A" |
3114 |
2981 |
10.97 |
|
|
|
| 16 |
A" |
1485 |
1421 |
9.03 |
|
|
|
| 17 |
A" |
1065 |
1019 |
0.70 |
|
|
|
| 18 |
A" |
872 |
835 |
13.51 |
|
|
|
| 19 |
A" |
512 |
490 |
36.42 |
|
|
|
| 20 |
A" |
403 |
385 |
80.30 |
|
|
|
| 21 |
A" |
37 |
36 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16101.4 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 15410.6 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.437 |
0.480 |
0.000 |
| C2 |
0.000 |
0.856 |
0.000 |
| N3 |
1.007 |
0.088 |
0.000 |
| O4 |
0.654 |
-1.256 |
0.000 |
| H5 |
1.506 |
-1.692 |
0.000 |
| H6 |
-1.564 |
-0.596 |
0.000 |
| H7 |
-1.933 |
0.898 |
0.875 |
| H8 |
-1.933 |
0.898 |
-0.875 |
| H9 |
0.268 |
1.906 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4855 | 2.4750 | 2.7172 | 3.6575 | 1.0829 | 1.0897 | 1.0897 | 2.2227 |
C2 | 1.4855 | | 1.2664 | 2.2106 | 2.9599 | 2.1341 | 2.1225 | 2.1225 | 1.0832 | N3 | 2.4750 | 1.2664 | | 1.3891 | 1.8486 | 2.6602 | 3.1727 | 3.1727 | 1.9621 | O4 | 2.7172 | 2.2106 | 1.3891 | | 0.9574 | 2.3139 | 3.4782 | 3.4782 | 3.1846 | H5 | 3.6575 | 2.9599 | 1.8486 | 0.9574 | | 3.2598 | 4.3936 | 4.3936 | 3.8046 | H6 | 1.0829 | 2.1341 | 2.6602 | 2.3139 | 3.2598 | | 1.7705 | 1.7705 | 3.1005 | H7 | 1.0897 | 2.1225 | 3.1727 | 3.4782 | 4.3936 | 1.7705 | | 1.7504 | 2.5741 | H8 | 1.0897 | 2.1225 | 3.1727 | 3.4782 | 4.3936 | 1.7705 | 1.7504 | | 2.5741 | H9 | 2.2227 | 1.0832 | 1.9621 | 3.1846 | 3.8046 | 3.1005 | 2.5741 | 2.5741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
127.977 |
|
C1 |
C2 |
H9 |
119.006 |
| C2 |
C1 |
H6 |
111.413 |
|
C2 |
C1 |
H7 |
110.067 |
| C2 |
C1 |
H8 |
110.067 |
|
C2 |
N3 |
O4 |
112.624 |
| N3 |
C2 |
H9 |
113.018 |
|
N3 |
O4 |
H5 |
102.397 |
| H6 |
C1 |
H7 |
109.154 |
|
H6 |
C1 |
H8 |
109.154 |
| H7 |
C1 |
H8 |
106.870 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.339 |
|
|
|
| 2 |
C |
-0.092 |
|
|
|
| 3 |
N |
-0.066 |
|
|
|
| 4 |
O |
-0.255 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
| 6 |
H |
0.136 |
|
|
|
| 7 |
H |
0.123 |
|
|
|
| 8 |
H |
0.123 |
|
|
|
| 9 |
H |
0.144 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.695 |
0.156 |
0.000 |
0.712 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.904 |
-3.826 |
0.000 |
| y |
-3.826 |
-21.095 |
0.000 |
| z |
0.000 |
0.000 |
-25.003 |
|
| Traceless |
| | x | y | z |
| x |
0.145 |
-3.826 |
0.000 |
| y |
-3.826 |
2.859 |
0.000 |
| z |
0.000 |
0.000 |
-3.004 |
|
| Polar |
| 3z2-r2 | -6.008 |
| x2-y2 | -1.810 |
| xy | -3.826 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.209 |
-1.158 |
0.000 |
| y |
-1.158 |
6.269 |
0.000 |
| z |
0.000 |
0.000 |
3.795 |
<r2> (average value of r
2) Å
2
| <r2> |
77.972 |
| (<r2>)1/2 |
8.830 |