Jump to
S1C2
S1C3
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -222.180283 |
| Energy at 298.15K | -222.186010 |
| HF Energy | -222.180283 |
| Nuclear repulsion energy | 119.120620 |
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/STO-3G
| 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 |
3807 |
3362 |
0.25 |
|
|
|
| 2 |
A |
3602 |
3181 |
1.29 |
|
|
|
| 3 |
A |
1946 |
1718 |
96.19 |
|
|
|
| 4 |
A |
1774 |
1567 |
0.45 |
|
|
|
| 5 |
A |
1262 |
1115 |
0.37 |
|
|
|
| 6 |
A |
946 |
835 |
1.73 |
|
|
|
| 7 |
A |
714 |
631 |
126.18 |
|
|
|
| 8 |
A |
433 |
382 |
2.26 |
|
|
|
| 9 |
A |
368 |
325 |
72.68 |
|
|
|
| 10 |
B |
3805 |
3360 |
0.24 |
|
|
|
| 11 |
B |
3606 |
3184 |
5.82 |
|
|
|
| 12 |
B |
1775 |
1567 |
33.07 |
|
|
|
| 13 |
B |
1416 |
1250 |
132.95 |
|
|
|
| 14 |
B |
1135 |
1003 |
19.52 |
|
|
|
| 15 |
B |
729 |
644 |
240.18 |
|
|
|
| 16 |
B |
572 |
505 |
172.74 |
|
|
|
| 17 |
B |
509 |
449 |
16.45 |
|
|
|
| 18 |
B |
344 |
304 |
0.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14371.5 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 12690.1 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 B1B95/STO-3G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.176 |
| O2 |
0.000 |
0.000 |
1.422 |
| N3 |
0.000 |
1.198 |
-0.660 |
| N4 |
0.000 |
-1.198 |
-0.660 |
| H5 |
0.375 |
2.003 |
-0.105 |
| H6 |
0.619 |
1.063 |
-1.495 |
| H7 |
-0.375 |
-2.003 |
-0.105 |
| H8 |
-0.619 |
-1.063 |
-1.495 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2459 | 1.4605 | 1.4605 | 2.0575 | 2.0750 | 2.0575 | 2.0750 |
O2 | 1.2459 | | 2.4018 | 2.4018 | 2.5467 | 3.1659 | 2.5467 | 3.1659 | N3 | 1.4605 | 2.4018 | | 2.3952 | 1.0477 | 1.0485 | 3.2703 | 2.4879 | N4 | 1.4605 | 2.4018 | 2.3952 | | 3.2703 | 2.4879 | 1.0477 | 1.0485 | H5 | 2.0575 | 2.5467 | 1.0477 | 3.2703 | | 1.6964 | 4.0764 | 3.5102 | H6 | 2.0750 | 3.1659 | 1.0485 | 2.4879 | 1.6964 | | 3.5102 | 2.4596 | H7 | 2.0575 | 2.5467 | 3.2703 | 1.0477 | 4.0764 | 3.5102 | | 1.6964 | H8 | 2.0750 | 3.1659 | 2.4879 | 1.0485 | 3.5102 | 2.4596 | 1.6964 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
109.119 |
|
C1 |
N3 |
H6 |
110.517 |
| C1 |
N4 |
H7 |
109.119 |
|
C1 |
N4 |
H8 |
110.517 |
| O2 |
C1 |
N3 |
124.916 |
|
O2 |
C1 |
N4 |
124.916 |
| N3 |
C1 |
N4 |
110.169 |
|
H5 |
N3 |
H6 |
108.045 |
| H7 |
N4 |
H8 |
108.045 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.263 |
|
|
|
| 2 |
O |
-0.236 |
|
|
|
| 3 |
N |
-0.390 |
|
|
|
| 4 |
N |
-0.390 |
|
|
|
| 5 |
H |
0.190 |
|
|
|
| 6 |
H |
0.187 |
|
|
|
| 7 |
H |
0.190 |
|
|
|
| 8 |
H |
0.187 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.874 |
1.874 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.164 |
4.332 |
0.000 |
| y |
4.332 |
-18.455 |
0.000 |
| z |
0.000 |
0.000 |
-22.976 |
|
| Traceless |
| | x | y | z |
| x |
-0.449 |
4.332 |
0.000 |
| y |
4.332 |
3.615 |
0.000 |
| z |
0.000 |
0.000 |
-3.166 |
|
| Polar |
| 3z2-r2 | -6.332 |
| x2-y2 | -2.709 |
| xy | 4.332 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.832 |
0.335 |
0.000 |
| y |
0.335 |
3.112 |
0.000 |
| z |
0.000 |
0.000 |
3.297 |
<r2> (average value of r
2) Å
2
| <r2> |
71.397 |
| (<r2>)1/2 |
8.450 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -222.175870 |
| Energy at 298.15K | -222.181398 |
| HF Energy | -222.175870 |
| Nuclear repulsion energy | 119.271650 |
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/STO-3G
| 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' |
3844 |
3394 |
0.09 |
|
|
|
| 2 |
A' |
3641 |
3215 |
1.39 |
|
|
|
| 3 |
A' |
1945 |
1718 |
100.39 |
|
|
|
| 4 |
A' |
1794 |
1584 |
15.39 |
|
|
|
| 5 |
A' |
1262 |
1115 |
2.14 |
|
|
|
| 6 |
A' |
955 |
843 |
17.53 |
|
|
|
| 7 |
A' |
707 |
624 |
154.74 |
|
|
|
| 8 |
A' |
592 |
523 |
104.63 |
|
|
|
| 9 |
A' |
465 |
411 |
11.65 |
|
|
|
| 10 |
A' |
377 |
332 |
65.46 |
|
|
|
| 11 |
A" |
3840 |
3391 |
1.29 |
|
|
|
| 12 |
A" |
3634 |
3208 |
8.98 |
|
|
|
| 13 |
A" |
1767 |
1561 |
21.67 |
|
|
|
| 14 |
A" |
1423 |
1256 |
131.08 |
|
|
|
| 15 |
A" |
1115 |
985 |
16.94 |
|
|
|
| 16 |
A" |
580 |
513 |
237.07 |
|
|
|
| 17 |
A" |
497 |
439 |
37.16 |
|
|
|
| 18 |
A" |
216 |
191 |
0.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14326.7 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 12650.4 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 B1B95/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.006 |
0.169 |
0.000 |
| O2 |
0.068 |
1.413 |
0.000 |
| N3 |
0.068 |
-0.650 |
1.201 |
| N4 |
0.068 |
-0.650 |
-1.201 |
| H5 |
-0.248 |
-0.093 |
2.027 |
| H6 |
-0.515 |
-1.515 |
1.135 |
| H7 |
-0.248 |
-0.093 |
-2.027 |
| H8 |
-0.515 |
-1.515 |
-1.135 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2455 | 1.4551 | 1.4551 | 2.0591 | 2.0968 | 2.0591 | 2.0968 |
O2 | 1.2455 | | 2.3871 | 2.3871 | 2.5443 | 3.1941 | 2.5443 | 3.1941 | N3 | 1.4551 | 2.3871 | | 2.4022 | 1.0449 | 1.0454 | 3.2907 | 2.5584 | N4 | 1.4551 | 2.3871 | 2.4022 | | 3.2907 | 2.5584 | 1.0449 | 1.0454 | H5 | 2.0591 | 2.5443 | 1.0449 | 3.2907 | | 1.7002 | 4.0533 | 3.4773 | H6 | 2.0968 | 3.1941 | 1.0454 | 2.5584 | 1.7002 | | 3.4773 | 2.2699 | H7 | 2.0591 | 2.5443 | 3.2907 | 1.0449 | 4.0533 | 3.4773 | | 1.7002 | H8 | 2.0968 | 3.1941 | 2.5584 | 1.0454 | 3.4773 | 2.2699 | 1.7002 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
109.820 |
|
C1 |
N3 |
H6 |
112.950 |
| C1 |
N4 |
H7 |
109.820 |
|
C1 |
N4 |
H8 |
112.950 |
| O2 |
C1 |
N3 |
124.060 |
|
O2 |
C1 |
N4 |
124.060 |
| N3 |
C1 |
N4 |
111.270 |
|
H5 |
N3 |
H6 |
108.855 |
| H7 |
N4 |
H8 |
108.855 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.268 |
|
|
|
| 2 |
O |
-0.242 |
|
|
|
| 3 |
N |
-0.385 |
|
|
|
| 4 |
N |
-0.385 |
|
|
|
| 5 |
H |
0.192 |
|
|
|
| 6 |
H |
0.180 |
|
|
|
| 7 |
H |
0.192 |
|
|
|
| 8 |
H |
0.180 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.815 |
-1.987 |
0.000 |
3.446 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.832 |
2.668 |
0.000 |
| y |
2.668 |
-22.823 |
0.000 |
| z |
0.000 |
0.000 |
-17.674 |
|
| Traceless |
| | x | y | z |
| x |
-1.583 |
2.668 |
0.000 |
| y |
2.668 |
-3.070 |
0.000 |
| z |
0.000 |
0.000 |
4.654 |
|
| Polar |
| 3z2-r2 | 9.307 |
| x2-y2 | 0.992 |
| xy | 2.668 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.729 |
0.358 |
0.000 |
| y |
0.358 |
3.307 |
0.000 |
| z |
0.000 |
0.000 |
3.181 |
<r2> (average value of r
2) Å
2
| <r2> |
71.385 |
| (<r2>)1/2 |
8.449 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -222.170105 |
| Energy at 298.15K | |
| HF Energy | -222.170105 |
| Nuclear repulsion energy | 120.187479 |
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/STO-3G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3997 |
3530 |
9.98 |
|
|
|
| 2 |
A1 |
3776 |
3334 |
11.47 |
|
|
|
| 3 |
A1 |
1949 |
1721 |
160.45 |
|
|
|
| 4 |
A1 |
1722 |
1521 |
5.03 |
|
|
|
| 5 |
A1 |
1147 |
1013 |
2.34 |
|
|
|
| 6 |
A1 |
978 |
863 |
2.98 |
|
|
|
| 7 |
A1 |
446 |
394 |
3.03 |
|
|
|
| 8 |
A2 |
361 |
319 |
0.00 |
|
|
|
| 9 |
A2 |
529i |
468i |
0.00 |
|
|
|
| 10 |
B1 |
678 |
599 |
9.11 |
|
|
|
| 11 |
B1 |
498 |
440 |
10.36 |
|
|
|
| 12 |
B1 |
454i |
401i |
580.19 |
|
|
|
| 13 |
B2 |
3995 |
3527 |
12.27 |
|
|
|
| 14 |
B2 |
3768 |
3327 |
47.13 |
|
|
|
| 15 |
B2 |
1709 |
1509 |
94.15 |
|
|
|
| 16 |
B2 |
1435 |
1267 |
233.50 |
|
|
|
| 17 |
B2 |
1000 |
883 |
3.54 |
|
|
|
| 18 |
B2 |
515 |
455 |
5.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13495.4 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 11916.4 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 B1B95/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.174 |
| O2 |
0.000 |
0.000 |
1.421 |
| N3 |
0.000 |
1.177 |
-0.627 |
| N4 |
0.000 |
-1.177 |
-0.627 |
| H5 |
0.000 |
2.094 |
-0.161 |
| H6 |
0.000 |
1.164 |
-1.657 |
| H7 |
0.000 |
-2.094 |
-0.161 |
| H8 |
0.000 |
-1.164 |
-1.657 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2477 | 1.4235 | 1.4235 | 2.1207 | 2.1693 | 2.1207 | 2.1693 |
O2 | 1.2477 | | 2.3626 | 2.3626 | 2.6245 | 3.2910 | 2.6245 | 3.2910 | N3 | 1.4235 | 2.3626 | | 2.3537 | 1.0291 | 1.0298 | 3.3041 | 2.5573 | N4 | 1.4235 | 2.3626 | 2.3537 | | 3.3041 | 2.5573 | 1.0291 | 1.0298 | H5 | 2.1207 | 2.6245 | 1.0291 | 3.3041 | | 1.7619 | 4.1883 | 3.5853 | H6 | 2.1693 | 3.2910 | 1.0298 | 2.5573 | 1.7619 | | 3.5853 | 2.3279 | H7 | 2.1207 | 2.6245 | 3.3041 | 1.0291 | 4.1883 | 3.5853 | | 1.7619 | H8 | 2.1693 | 3.2910 | 2.5573 | 1.0298 | 3.5853 | 2.3279 | 1.7619 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
118.801 |
|
C1 |
N3 |
H6 |
123.519 |
| C1 |
N4 |
H7 |
118.801 |
|
C1 |
N4 |
H8 |
123.519 |
| O2 |
C1 |
N3 |
124.237 |
|
O2 |
C1 |
N4 |
124.237 |
| N3 |
C1 |
N4 |
111.527 |
|
H5 |
N3 |
H6 |
117.680 |
| H7 |
N4 |
H8 |
117.680 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.295 |
|
|
|
| 2 |
O |
-0.268 |
|
|
|
| 3 |
N |
-0.414 |
|
|
|
| 4 |
N |
-0.414 |
|
|
|
| 5 |
H |
0.206 |
|
|
|
| 6 |
H |
0.194 |
|
|
|
| 7 |
H |
0.206 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.147 |
3.147 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.732 |
0.000 |
0.000 |
| y |
0.000 |
-15.489 |
0.000 |
| z |
0.000 |
0.000 |
-21.008 |
|
| Traceless |
| | x | y | z |
| x |
-4.483 |
0.000 |
0.000 |
| y |
0.000 |
6.381 |
0.000 |
| z |
0.000 |
0.000 |
-1.897 |
|
| Polar |
| 3z2-r2 | -3.795 |
| x2-y2 | -7.243 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.415 |
0.000 |
0.000 |
| y |
0.000 |
3.133 |
0.000 |
| z |
0.000 |
0.000 |
3.362 |
<r2> (average value of r
2) Å
2
| <r2> |
70.596 |
| (<r2>)1/2 |
8.402 |