Jump to
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.144546 |
| Energy at 298.15K | -209.150569 |
| HF Energy | -209.144546 |
| Nuclear repulsion energy | 117.920413 |
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 wB97X-D/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' |
3903 |
3732 |
92.44 |
|
|
|
| 2 |
A' |
3163 |
3023 |
12.17 |
|
|
|
| 3 |
A' |
3123 |
2986 |
12.86 |
|
|
|
| 4 |
A' |
3054 |
2920 |
17.40 |
|
|
|
| 5 |
A' |
1772 |
1694 |
1.30 |
|
|
|
| 6 |
A' |
1481 |
1416 |
13.73 |
|
|
|
| 7 |
A' |
1456 |
1392 |
8.12 |
|
|
|
| 8 |
A' |
1409 |
1347 |
22.50 |
|
|
|
| 9 |
A' |
1305 |
1248 |
54.56 |
|
|
|
| 10 |
A' |
1160 |
1109 |
4.02 |
|
|
|
| 11 |
A' |
1049 |
1003 |
159.53 |
|
|
|
| 12 |
A' |
927 |
886 |
5.37 |
|
|
|
| 13 |
A' |
576 |
551 |
13.80 |
|
|
|
| 14 |
A' |
329 |
314 |
3.04 |
|
|
|
| 15 |
A" |
3114 |
2977 |
13.52 |
|
|
|
| 16 |
A" |
1487 |
1422 |
8.81 |
|
|
|
| 17 |
A" |
1090 |
1042 |
1.31 |
|
|
|
| 18 |
A" |
923 |
883 |
9.62 |
|
|
|
| 19 |
A" |
416 |
397 |
130.90 |
|
|
|
| 20 |
A" |
294 |
281 |
0.45 |
|
|
|
| 21 |
A" |
167 |
160 |
0.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16098.5 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 15390.1 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 wB97X-D/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.295 |
1.300 |
0.000 |
| C2 |
0.000 |
0.562 |
0.000 |
| N3 |
0.016 |
-0.702 |
0.000 |
| O4 |
1.303 |
-1.213 |
0.000 |
| H5 |
1.163 |
-2.159 |
0.000 |
| H6 |
-2.128 |
0.600 |
0.000 |
| H7 |
-1.367 |
1.942 |
0.879 |
| H8 |
-1.367 |
1.942 |
-0.879 |
| H9 |
0.934 |
1.123 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4904 | 2.3924 | 3.6140 | 4.2433 | 1.0876 | 1.0911 | 1.0911 | 2.2364 |
C2 | 1.4904 | | 1.2635 | 2.2015 | 2.9593 | 2.1282 | 2.1321 | 2.1321 | 1.0898 | N3 | 2.3924 | 1.2635 | | 1.3847 | 1.8549 | 2.5080 | 3.1100 | 3.1100 | 2.0424 | O4 | 3.6140 | 2.2015 | 1.3847 | | 0.9570 | 3.8803 | 4.2251 | 4.2251 | 2.3643 | H5 | 4.2433 | 2.9593 | 1.8549 | 0.9570 | | 4.2946 | 4.8981 | 4.8981 | 3.2900 | H6 | 1.0876 | 2.1282 | 2.5080 | 3.8803 | 4.2946 | | 1.7754 | 1.7754 | 3.1065 | H7 | 1.0911 | 2.1321 | 3.1100 | 4.2251 | 4.8981 | 1.7754 | | 1.7585 | 2.5962 | H8 | 1.0911 | 2.1321 | 3.1100 | 4.2251 | 4.8981 | 1.7754 | 1.7585 | | 2.5962 | H9 | 2.2364 | 1.0898 | 2.0424 | 2.3643 | 3.2900 | 3.1065 | 2.5962 | 2.5962 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.394 |
|
C1 |
C2 |
H9 |
119.356 |
| C2 |
C1 |
H6 |
110.301 |
|
C2 |
C1 |
H7 |
110.400 |
| C2 |
C1 |
H8 |
110.400 |
|
C2 |
N3 |
O4 |
112.386 |
| N3 |
C2 |
H9 |
120.250 |
|
N3 |
O4 |
H5 |
103.246 |
| H6 |
C1 |
H7 |
109.147 |
|
H6 |
C1 |
H8 |
109.147 |
| H7 |
C1 |
H8 |
107.384 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.214 |
|
|
|
| 2 |
C |
-0.049 |
|
|
|
| 3 |
N |
-0.052 |
|
|
|
| 4 |
O |
-0.243 |
|
|
|
| 5 |
H |
0.208 |
|
|
|
| 6 |
H |
0.094 |
|
|
|
| 7 |
H |
0.086 |
|
|
|
| 8 |
H |
0.086 |
|
|
|
| 9 |
H |
0.084 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.337 |
0.611 |
0.000 |
0.698 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.142 |
-2.089 |
0.000 |
| y |
-2.089 |
-18.666 |
0.000 |
| z |
0.000 |
0.000 |
-24.989 |
|
| Traceless |
| | x | y | z |
| x |
-3.314 |
-2.089 |
0.000 |
| y |
-2.089 |
6.400 |
0.000 |
| z |
0.000 |
0.000 |
-3.086 |
|
| Polar |
| 3z2-r2 | -6.171 |
| x2-y2 | -6.476 |
| xy | -2.089 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.742 |
-1.337 |
0.000 |
| y |
-1.337 |
7.175 |
0.000 |
| z |
0.000 |
0.000 |
3.821 |
<r2> (average value of r
2) Å
2
| <r2> |
90.953 |
| (<r2>)1/2 |
9.537 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.144081 |
| Energy at 298.15K | |
| HF Energy | -209.144081 |
| Nuclear repulsion energy | 120.422992 |
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 wB97X-D/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' |
3909 |
3737 |
93.96 |
|
|
|
| 2 |
A' |
3193 |
3052 |
7.29 |
|
|
|
| 3 |
A' |
3172 |
3033 |
5.73 |
|
|
|
| 4 |
A' |
3065 |
2930 |
12.38 |
|
|
|
| 5 |
A' |
1777 |
1698 |
8.39 |
|
|
|
| 6 |
A' |
1496 |
1430 |
17.52 |
|
|
|
| 7 |
A' |
1426 |
1363 |
16.77 |
|
|
|
| 8 |
A' |
1396 |
1334 |
39.83 |
|
|
|
| 9 |
A' |
1354 |
1294 |
37.17 |
|
|
|
| 10 |
A' |
1162 |
1110 |
11.18 |
|
|
|
| 11 |
A' |
976 |
933 |
145.94 |
|
|
|
| 12 |
A' |
929 |
888 |
0.61 |
|
|
|
| 13 |
A' |
693 |
662 |
13.07 |
|
|
|
| 14 |
A' |
329 |
315 |
1.30 |
|
|
|
| 15 |
A" |
3121 |
2984 |
11.77 |
|
|
|
| 16 |
A" |
1488 |
1422 |
9.48 |
|
|
|
| 17 |
A" |
1076 |
1029 |
0.44 |
|
|
|
| 18 |
A" |
867 |
829 |
14.03 |
|
|
|
| 19 |
A" |
514 |
491 |
30.71 |
|
|
|
| 20 |
A" |
395 |
378 |
88.25 |
|
|
|
| 21 |
A" |
67i |
64i |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16135.4 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 15425.4 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 wB97X-D/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.444 |
0.482 |
0.000 |
| C2 |
0.000 |
0.856 |
0.000 |
| N3 |
1.008 |
0.087 |
0.000 |
| O4 |
0.661 |
-1.259 |
0.000 |
| H5 |
1.514 |
-1.693 |
0.000 |
| H6 |
-1.581 |
-0.594 |
0.000 |
| H7 |
-1.935 |
0.906 |
0.878 |
| H8 |
-1.935 |
0.906 |
-0.878 |
| H9 |
0.266 |
1.907 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4920 | 2.4840 | 2.7322 | 3.6720 | 1.0849 | 1.0911 | 1.0911 | 2.2259 |
C2 | 1.4920 | | 1.2674 | 2.2160 | 2.9644 | 2.1452 | 2.1257 | 2.1257 | 1.0845 | N3 | 2.4840 | 1.2674 | | 1.3908 | 1.8506 | 2.6772 | 3.1786 | 3.1786 | 1.9655 | O4 | 2.7322 | 2.2160 | 1.3908 | | 0.9572 | 2.3383 | 3.4925 | 3.4925 | 3.1912 | H5 | 3.6720 | 2.9644 | 1.8506 | 0.9572 | | 3.2844 | 4.4071 | 4.4071 | 3.8104 | H6 | 1.0849 | 2.1452 | 2.6772 | 2.3383 | 3.2844 | | 1.7735 | 1.7735 | 3.1091 | H7 | 1.0911 | 2.1257 | 3.1786 | 3.4925 | 4.4071 | 1.7735 | | 1.7552 | 2.5724 | H8 | 1.0911 | 2.1257 | 3.1786 | 3.4925 | 4.4071 | 1.7735 | 1.7552 | | 2.5724 | H9 | 2.2259 | 1.0845 | 1.9655 | 3.1912 | 3.8104 | 3.1091 | 2.5724 | 2.5724 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.179 |
|
C1 |
C2 |
H9 |
118.672 |
| C2 |
C1 |
H6 |
111.732 |
|
C2 |
C1 |
H7 |
109.783 |
| C2 |
C1 |
H8 |
109.783 |
|
C2 |
N3 |
O4 |
112.860 |
| N3 |
C2 |
H9 |
113.149 |
|
N3 |
O4 |
H5 |
102.451 |
| H6 |
C1 |
H7 |
109.172 |
|
H6 |
C1 |
H8 |
109.172 |
| H7 |
C1 |
H8 |
107.081 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.238 |
|
|
|
| 2 |
C |
-0.092 |
|
|
|
| 3 |
N |
-0.057 |
|
|
|
| 4 |
O |
-0.243 |
|
|
|
| 5 |
H |
0.207 |
|
|
|
| 6 |
H |
0.109 |
|
|
|
| 7 |
H |
0.092 |
|
|
|
| 8 |
H |
0.092 |
|
|
|
| 9 |
H |
0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.736 |
0.192 |
0.000 |
0.761 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.905 |
-3.868 |
0.000 |
| y |
-3.868 |
-21.057 |
0.000 |
| z |
0.000 |
0.000 |
-25.008 |
|
| Traceless |
| | x | y | z |
| x |
0.128 |
-3.868 |
0.000 |
| y |
-3.868 |
2.900 |
0.000 |
| z |
0.000 |
0.000 |
-3.028 |
|
| Polar |
| 3z2-r2 | -6.055 |
| x2-y2 | -1.848 |
| xy | -3.868 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.193 |
-1.164 |
0.000 |
| y |
-1.164 |
6.279 |
0.000 |
| z |
0.000 |
0.000 |
3.817 |
<r2> (average value of r
2) Å
2
| <r2> |
78.405 |
| (<r2>)1/2 |
8.855 |