Bisphosphonates conjugated to fluoroquinolone antibacterials through an intermediate carbon had better activity than conjugates lacking the carbon. Virtually all molar-based activity of these esterified bisphosphonate derivatives was identical to that of its parent. De-esterified free-acid forms retained good activity against most Gram-negative bacteria, but not against Gram-positives. A free-acid derivative remained bound to washed bone and completely inhibited Staphylococcus aureus growth. The more potent parent, ciprofloxacin, failed to bind significantly, and bacterial growth occurred.
Ab initio calculations with large basis sets and
electron correlation were applied to the study of geometry
of
the 2-propyl cation in ion pairs with trihydro fluoroborate
(A) or dihydrolithiate (B) as anion. The
goal was
to model the ion pair formed by ionization in a solvent with good
anion-stabilizing properties, but of low
dielectric constant, like trifluoroacetic acid (TFA). The effect
of the anion, seen already at long distances,
was that the preferred cation conformation changed from C1,C3
staggered as in the isolated carbocation
(chiral 2-propyl cation, 1) to C1,C3 eclipsed
(C
s
symmetry, 2). The
optimized cation geometry was essentially
the same at the MP2(FC)/6-31G*, MP2(FC)/6-31++G*, and
MP2(FU)/6-311G** levels, but the position of
the anion above the cation was somewhat more sensitive to the basis
set. The preferred anion position was
in the plane bisecting the C1−C2−C3 angle of 2 and in
the region “inside” that angle. This “inside”
displacement became more pronounced as the interionic distance,
d, was made shorter; at the same time, the
anion moved slightly off the bisecting plane. Elimination within
the ion pair to form propene occurred at d
< 2.5 Å. When the anion was allowed to “fall” freely, the
reaction pathway was determined by the initial
position of the anion: elimination for a position “inside” the
C1−C2−C3 angle and recombination to
2-fluoropropane (occurring at d = 1.5−1.7 Å) for a
position “outside” the C1−C2−C3 angle. The
equilibrium
cation geometry did not change significantly in 2.B relative
to 2.A, but the distortions toward elimination
occurred at longer distances for the more basic anion B and
elimination itself took place at d = 3.5 Å.
The
energy difference beween 1.A (optimized with the methyl
groups held staggered) and 2.A at d = 3.4 Å
was
2.39 and 3.25 kcal/mol at the MP2(FC)/6-31++G* and
MP2(FU)/6-311G** levels, respectively. The
equilibrium position of the anion paired with 1 was above
the C1−C2 bond, close to the syn hydrogen at C1.
Thus, methyl rotation along the lowest-energy pathway involves
also a movement of the anion relative to the
cation.
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