Table 3.
Root–mean–square vibrational amplitudes and vibrational corrections for 4-nitropyridine-N-oxide calculated from the molecular force field. Interatomic distances and vibrational amplitudes obtained from the GED refinements.a).
rh1b | l(GED)c | lcalc(B3LYP) | rh1-ra (B3LYP) | |
---|---|---|---|---|
C3–H4 | 1.092(8) | 0.078(3) l1d) | 0.075 | 0.0017 |
C2–H1 | 1.094(8) | 0.078(3) l1 | 0.075 | 0.0016 |
N2–O2 | 1.227(3) | 0.043(3) l1 | 0.040 | 0.0004 |
N1–O1 | 1.267(3) | 0.045(3) l1 | 0.042 | 0.0005 |
C2–C3 | 1.378(4) | 0.048(3) l1 | 0.045 | 0.0003 |
N1–C3 | 1.373(4) | 0.050(3) l1 | 0.047 | 0.0005 |
C1–C2 | 1.395(4) | 0.049(3) l1 | 0.046 | 0.0006 |
N2–C1 | 1.460(4) | 0.055(3) l1 | 0.052 | 0.0008 |
O2⋯O3 | 2.171(6) | 0.048(4) l2 | 0.049 | 0.0034 |
C3⋯O1 | 2.295(6) | 0.057(4) l2 | 0.058 | 0.0020 |
C1⋯O2 | 2.304(5) | 0.059(4) l2 | 0.060 | 0.0022 |
C3⋯C4 | 2.362(9) | 0.055(4) l2 | 0.057 | 0.0046 |
C1⋯C3 | 2.386(6) | 0.054(4) l2 | 0.055 | 0.0029 |
N1⋯C2 | 2.404(6) | 0.054(4) l2 | 0.055 | 0.0035 |
C2⋯C5 | 2.417(9) | 0.055(4) l2 | 0.056 | 0.0049 |
N2⋯C2 | 2.472(6) | 0.064(4) l2 | 0.065 | 0.0040 |
C2⋯O3 | 2.731(7) | 0.095(3) l3 | 0.096 | −0.0111 |
C2⋯C4 | 2.758(7) | 0.062(3) l3 | 0.063 | 0.0060 |
N1⋯C1 | 2.775(8) | 0.061(3) l3 | 0.062 | 0.0042 |
C2⋯O1 | 3.557(8) | 0.059(7) l4 | 0.061 | 0.0081 |
C2⋯O2 | 3.565(7) | 0.065(7) l4 | 0.066 | 0.0196 |
C3⋯N2 | 3.726(9) | 0.065(7) l4 | 0.066 | 0.0091 |
C1⋯O1 | 4.042(10) | 0.064(11) l5 | 0.064 | 0.0102 |
C3⋯O3 | 4.107(9) | 0.098(11) l5 | 0.098 | 0.0004 |
N1⋯N2 | 4.235(11) | 0.068(11) l5 | 0.068 | 0.0119 |
C3⋯O2 | 4.690(10) | 0.070(9) l6 | 0.072 | 0.0231 |
N1⋯O2 | 4.928(11) | 0.085(9) l6 | 0.087 | 0.0157 |
N2⋯O1 | 5.502(13) | 0.068(21) l7 | 0.071 | 0.0202 |
O1⋯O2 | 6.170(13) | 0.106(13) l8 | 0.093 | 0.0250 |
Values in Å, atom notifications are shown on Fig. 1.
Uncertainties in rh1 – distances are σ=(σsc2+(2.5σLS)2)1/2 (σsc = 0,002r, σLS–standard deviation in least–squares refinement).
Uncertainties for amplitudes are σ = 3σLS.
Group number of amplitude.