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Vol. 283, Issue 1, 293-304, 1997

Kinetic Evidence for Active Efflux Transport across the Blood-Brain Barrier of Quinolone Antibiotics1

Tsuyoshi Ooie2, Tetsuya Terasaki3, Hiroshi Suzuki and Yuichi Sugiyama

Department of Pharmaceutics, Faculty of Pharmaceutical Sciences, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan


    Abstract
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

A distributed model has been used to clarify the mechanism of the restricted and differential distribution of the quinolone antibiotics in the rat central nervous system (CNS). The symmetrical permeability clearances across the blood-brain barrier (BBB), PSBBB, and across the blood-cerebrospinal fluid barrier (BCSFB), PSCSF, and the active efflux clearances across the BBB, PSBBB,eff, were obtained from a nonlinear least squares regression analysis combined with the fast inverse Laplace transforming program for in vivo data. The values of PSBBB,eff were 10- to 260-fold greater than those of PSBBB, providing kinetic evidence to support the hypothesis that a significant efflux transport across the BBB is responsible for the limited distribution of quinolones in brain tissue. Moreover, by simulation studies, we could demonstrate the concentration profiles in the brain as a function of the distance from the ependymal surface. However, active efflux transport across the BCSFB has been suggested to have only a slight effect on the apparent elimination from the cerebrospinal fluid. Comparing the apparent brain tissue-to-unbound serum concentration ratio at steady state, it has been suggested that the net flux across the BBB, i.e., the ratio of PSBBB to the sum of PSBBB and PSBBB,eff, is a determinant for the differential distribution of these quinolones in brain tissue. Such a putative active efflux transport system would play a significant role in decreasing the brain interstitial fluid concentration of quinolones.


    Introduction
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

The side effect of quinolone antimicrobial agents (quinolones) on the CNS such as confusion, hallucinations, anxiety, agitation, depression and convulsive seizures is one of the most serious problems associated with their use as chemotherapeutic agents (Christ, 1990). Because the interaction of quinolones with the receptor of GABA in the brain is responsible for CNS side effects (Akahane et al., 1989), it is important to understand the mechanism for the distribution of quinolones in brain tissue and the CSF in quantitative terms. Several investigators have reported that quinolone concentrations in brain tissue and CSF are lower than in serum after systemic administration (Ichikawa et al., 1992; Sato et al., 1988). In addition, we previously demonstrated the presence of such an active transport from the CSF to blood across the BCSFB by examining the efflux of quinolones from the CSF after intracerebroventricular administration (Ooie et al., 1996b) and by examining the uptake of quinolones by the isolated choroid plexus (Ooie et al., 1996a). We have also demonstrated that brain-to-plasma and CSF-to-plasma unbound concentration of quinolones are less than unity at steady state (Ooie et al., 1996c). However, no report has appeared in which the efflux transport for quinolones across the BBB has been characterized. To clarify the mechanism for the restricted distribution in the brain tissue and the CSF, one of the best ways is to apply pharmacokinetic model analysis as reported previously (Dykstra et al., 1993; Ogawa et al., 1994; Sato et al., 1988; Wang and Sawchuk, 1995). Considering the anatomical features of the brain tissue and the CSF, the distributed model (Collins and Dedrick, 1983; Suzuki et al., 1997) will provide much more information about the kinetics of drug diffusion through the brain tissue.

The present study investigated the process governing the restricted distribution of quinolones in the CNS based on the distributed model. In this study, we determined the initial CNS uptake of quinolones in rats. Moreover, these data, along with previously published data [brain-to-plasma and CSF-to-plasma concentration at steady state (Ooie et al., 1996c) and CSF concentration profiles after intracerebroventricular administration (Ooie et al., 1996b)] were kinetically analyzed to establish the presence of active transport for the efflux of quinolones from the brain to blood across the BBB. To clarify the mechanism of the differential distribution of quinolones in the CNS, a comparative kinetic analysis was also performed for six quinolone analogs: NFLX, AM-1155, OFLX, FLRX, SPFX and PFLX.

    Materials and Methods
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

Materials. All the quinolones, NFLX, AM-1155, FLRX, OFLX, SPFX and PFLX were synthesized in the Central Research Laboratories of Kyorin Pharmaceutical Co., Ltd. (Tochigi, Japan). All other chemicals were commercial products of analytical grade. Male Wistar rats weighing 250 to 300 g (Japan Laboratory Animals, Inc., Tokyo, Japan) were used throughout the experiments, which were conducted according to the guidelines provided by the Institutional Animal Care Committee (Faculty of Pharmaceutical Sciences, The University of Tokyo).

In vivo distribution of quinolones. Rats were anesthetized with an i.p. dose of 1.5 g/kg ethylcarbamate, and cannulation with polyethylene tubing (PE-50) was performed into the femoral artery and vein. An i.v. bolus dose of quinolone (10 mg/kg) was administered through the femoral vein cannula. At fixed times after injection of each quinolone, arterial blood specimens were withdrawn and centrifuged to obtain serum. At 1, 3, 5 and 10 min after i.v. administration, crystal-clear CSF specimens were obtained from individual rats by cisternal puncture with a 24-gauge needle (Matsushita et al., 1991). Immediately after collection of the CSF, each rat was decapitated and the cerebral cortex removed.

Determination of drug concentrations. Brain tissues were homogenized with 4 volumes of 0.067 M phosphate buffer (pH 7.0). After centrifugation of tissue homogenates, supernatants were used to measure drug concentrations. The concentration of quinolones in serum, tissue homogenates and CSF was determined by the HPLC as described previously (Ooie et al., 1997).

Kinetic analysis of serum concentration-time profiles. With the previously reported values for the serum unbound fraction (Ooie et al., 1996c), the unbound serum concentration of each quinolone (Cp,u) was obtained from the in vivo study after i.v. administration. The area under the unbound serum concentration-time curve for time t (AUCu,0-t) of each quinolone was estimated by the linear trapezoidal rule. The apparent influx clearance across the BBB and BCSFB (PSBBB,app and PSCSF,app) were obtained from in vivo data by dividing the brain or the CSF concentration at 1 min by the corresponding AUCu,0-1 min after i.v. administration; these were used as initial estimates for the distributed model analysis described as follows. Mean Cp,u values obtained from 6 to 12 rats after i.v. administration of each quinolone versus time profiles were examined by nonlinear least squares regression analysis (Yamaoka et al., 1981) by the following equation:
C<SUB>p,u</SUB>(<IT>t</IT>)<IT>=A · e</IT><SUP>(−<IT>&agr; · t</IT>)</SUP><IT>+B · e</IT><SUP>(−<IT>&bgr; · t</IT>)</SUP> (1)

Distributed model analysis. A distributed model (Collins and Dedrick, 1983; Suzuki et al., 1997) has been used to analyze quinolone distribution in the CNS. The analysis was performed according to the method described previously (Suzuki et al., 1997) with some modifications. A diagrammatic representation of an anatomical compartment in the brain tissue and the CSF is presented in figure 1. In estimating the brain tissue concentration-time or the CSF concentration-time profiles the following assumptions were made: 1) The brain tissue and the CSF are described by a one-dimensional slab of tissue. 2) Drug permeates through the BBB and the BCSFB in both directions, i.e., influx and efflux. 3) There is a constant bulk flow of the CSF. 4) Drug concentration in brain ISF at the ependymal surface is the same as that in the CSF. 5) Drug diffuses through the brain tissue according to Fick's law of diffusion. 6) Drug distributes into the intracellular fluid space in the brain. Based on this model (fig. 1), the Laplace transformed equations of total brain (Cbr) and CSF concentration (CCSF) after i.v. or intracerebroventricular administration were obtained.


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Fig. 1.   Distributed model for the kinetic analysis of quinolone distribution between brain tissue, CSF and blood.

Equation 2 represents a mass balance equation describing the drug concentration in the brain tissue:
<FR><NU>∂C<SUB>br</SUB>(<IT>x,t</IT>)</NU><DE><IT>∂t</IT></DE></FR><IT>=</IT><IT>D</IT><SUB>t</SUB><IT> · </IT><FR><NU><IT>∂<SUP>2</SUP>C</IT><SUB>br</SUB>(<IT>x,t</IT>)</NU><DE><IT>∂x</IT><SUP><IT>2</IT></SUP></DE></FR><IT>+</IT>PS<SUB>BBB</SUB><IT> · C</IT><SUB>p,u</SUB>(<IT>t</IT>) (2)
−<FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</NU><DE><IT>V</IT><SUB>br</SUB></DE></FR><IT> · C</IT><SUB>br</SUB>(<IT>x,t</IT>)
where Cbr(x,t) is the drug concentration in the brain tissue at a distance, x, from the ependymal surface at time t. Dt, PSBBB and PSBBB,eff represent the apparent diffusion coefficient through the brain tissue, the permeability clearance of symmetrical transport across the BBB and the permeability clearance of the active efflux process from the brain ISF to circulating blood across the BBB, respectively. Cp,u(t) is the unbound drug concentration in the serum at time t, Vbr is the distribution volume in the brain tissue defined as the concentration ratio of total brain-to-ISF.

Equation 3 represents a mass balance equation describing the drug concentration in the CSF:
  V<SUB>CSF</SUB><IT> · </IT><FR><NU>d<IT>C</IT><SUB>CSF</SUB>(<IT>t</IT>)</NU><DE>d<IT>t</IT></DE></FR><IT>=</IT>PS<SUB>CSF</SUB><IT> · C</IT><SUB>p,u</SUB>(<IT>t</IT>)<IT>−</IT>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>) (3)
 · C<SUB>CSF</SUB>(<IT>t</IT>)<IT>+D</IT><SUB>t</SUB><IT> · </IT>Ar<IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂x</IT></DE></FR>
where CCSF(t) is the drug concentration in the CSF at time t, VCSF is volume of the CSF, PSCSF is the symmetrical permeability clearance across the BCSFB, PSCSF,eff is the active efflux clearance across the BCSFB, Q is the bulk flow rate of the CSF and Ar is the surface area of the cerebroventricular ependyma. Assuming that the ISF concentration (CISF) at the ependymal surface is the same as the CSF concentration, i.e., CCSF(t) = CISF(0,t) = Cbr(0,t)/Vbr, equation 3 can be converted to equation 4 as a boundary condition of equation 2, at x = 0. 
 V<SUB>CSF</SUB><IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂t</IT></DE></FR><IT>=</IT><IT>V</IT><SUB>br</SUB><IT> · </IT>PS<SUB>CSF</SUB><IT> · C</IT><SUB>p,u</SUB>(<IT>t</IT>)<IT>−</IT>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>) (4)
 · C<SUB>br</SUB>(<IT>0,t</IT>)<IT>+</IT>(<IT>D</IT><SUB>t</SUB><IT> · </IT>Ar<IT> · V</IT><SUB>br</SUB>)<IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂x</IT></DE></FR>
At some distance (x*) from the ependymal surface, CSF events no longer create a driving force for diffusion flux, so that other boundary conditions of equation 2 can be defined, at x >= x*:
<FR><NU>∂C<SUB>br</SUB>(<IT>x*,t</IT>)</NU><DE><IT>∂t</IT></DE></FR><IT>=</IT>PS<SUB>BBB</SUB><IT> · C</IT><SUB>p,u</SUB>(<IT>t</IT>)<IT>−</IT><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</NU><DE><IT>V</IT><SUB>br</SUB></DE></FR><IT> · C</IT><SUB>br</SUB>(<IT>x*,t</IT>) (5)
Moreover, there is no drug in brain tissue and the CSF at time t = 0. Thus, we have used the following relationship as an initial condition of equations 2 to 5:
C<SUB>br</SUB>(<IT>x,0</IT>)<IT>=0</IT> (6)
Taking the Laplace transform of equations 2 to 5, equations 7 and 8 can be obtained for the drug concentration in brain and brain ISF, respectively, at a distance x:
  C<SUP>iv</SUP><SUB>br</SUB>(<IT>x,s</IT>)<IT>=</IT><FR><NU><AR><R><C><FR><NU><IT>V</IT><SUB>br</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT>PS<SUB>CSF</SUB><IT> · </IT><FENCE><FR><NU><IT>A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU><IT>B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></FENCE></C></R><R><C><IT>   −</IT><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE></C></R><R><C><IT>        · </IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></DE></FR></C></R></AR></NU><DE><AR><R><C><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU><IT>D</IT><SUB>t</SUB><IT> · </IT>Ar</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></C></R><R><C><IT>    · V</IT><SUB>br</SUB><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></C></R></AR></DE></FR> (7)
 · exp<FENCE><IT>−x · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></FENCE>
+<FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></DE></FR>
and
C<SUP>iv</SUP><SUB>ISF</SUB>(<IT>x,s</IT>)<IT>=</IT><FR><NU><IT>C</IT><SUP>iv</SUP><SUB>br</SUB>(<IT>x,s</IT>)</NU><DE><IT>V</IT><SUB>br</SUB></DE></FR> (8)
where s is the operator of time t. In this calculation, we assumed that Cp,u(t) is given by equation 1 and x* right-arrow infinity . Defining the thickness of cerebral cortex surrounding the CSF as L, the following equation can be derived for the average drug concentration in the brain,
<OVL>C</OVL><SUB>br</SUB>(<IT>s</IT>)<IT>=</IT><FR><NU><AR><R><C><IT>−</IT><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT> · </IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></DE></FR></C></R><R><C><IT>           +</IT><FR><NU><IT>V</IT><SUB>br</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT>PS<SUB>CSF</SUB><IT> · </IT><FENCE><FR><NU><IT>A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU><IT>B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></FENCE></C></R></AR></NU><DE><AR><R><C><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU><IT>D</IT><SUB>t</SUB><IT> · </IT>Ar</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></C></R><R><C><IT>   · V</IT><SUB>br</SUB><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></C></R></AR></DE></FR> (9)
 · <FR><NU><FENCE>1−exp<FENCE><IT>−L · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></FENCE></FENCE></NU><DE><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V<SUB>br</SUB>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></DE></FR>
 · <FR><NU>1</NU><DE>L</DE></FR>+<FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></DE></FR>
Moreover, considering the condition that x is zero, i.e., the CSF concentration at time t, the following equation can be obtained from equations 7 and 8;
C<SUP>iv</SUP><SUB>CSF</SUB>(<IT>s</IT>)
=<FR><NU><FENCE><FR><NU><AR><R><C>−<FENCE>s+<FR><NU>Q+PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE></C></R><R><C><IT> · </IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></DE></FR></C></R><R><C><IT>+</IT><FR><NU><IT>V</IT><SUB>br</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT>PS<SUB>CSF</SUB><IT> · </IT><FENCE><FR><NU><IT>A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU><IT>B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></FENCE></C></R></AR></NU><DE><AR><R><C><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU><IT>D</IT><SUB>t</SUB><IT> · </IT>Ar</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></C></R><R><C><IT>   · V</IT><SUB>br</SUB><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></C></R></AR></DE></FR><IT>+</IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>s+&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>s+&bgr;</IT></DE></FR></NU><DE><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</NU><DE><IT>V</IT><SUB>br</SUB></DE></FR><IT>+s</IT></DE></FR>}</FENCE></NU><DE><IT>V</IT><SUB>br</SUB></DE></FR> (10)
With equations 9 and 10, the area under concentration-time curve of average brain tissue and the CSF, i.e., AUCbriv and AUCCSFiv, respectively, can be obtained as:
AUC<SUP>iv</SUP><SUB>br</SUB><IT>=</IT><LIM><OP><UP>lim</UP></OP><LL><IT>s→0</IT></LL></LIM><OVL><IT>C</IT></OVL><SUB>br</SUB>(<IT>s</IT>) (11)
=<FR><NU><AR><R><C>−<FENCE><FR><NU>Q+PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT> · </IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></DE></FR></C></R><R><C><IT>              +</IT><FR><NU><IT>V</IT><SUB>br</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT>PS<SUB>CSF</SUB><IT> · </IT><FENCE><FR><NU><IT>A</IT></NU><DE><IT>&agr;</IT></DE></FR><IT>+</IT><FR><NU><IT>B</IT></NU><DE><IT>&bgr;</IT></DE></FR></FENCE></C></R></AR></NU><DE><AR><R><C><FENCE><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU>Ar</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></C></R><R><C><IT> · </IT><RAD><RCD>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · V</IT><SUB>br</SUB><IT> · D</IT><SUB>t</SUB></RCD></RAD></C></R></AR></DE></FR>
 · <FR><NU><FENCE>1−exp<FENCE><IT>−L · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></FENCE></FENCE></NU><DE><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></DE></FR><IT> · </IT><FR><NU><IT>1</IT></NU><DE><IT>L</IT></DE></FR><IT>+</IT><FR><NU><AR><R><C><FENCE><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>&agr;</IT></DE></FR></FENCE></C></R><R><C><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>&bgr;</IT></DE></FR></C></R></AR></NU><DE><FR><NU><AR><R><C>PS<SUB>BBB</SUB></C></R><R><C><IT>+</IT>PS<SUB>BBB,eff</SUB>)</C></R></AR></NU><DE><IT>V</IT><SUB>br</SUB></DE></FR></DE></FR>
and
AUC<SUP>iv</SUP><SUB>CSF</SUB><IT>=</IT><LIM><OP><UP>lim</UP></OP><LL><IT>s→0</IT></LL></LIM><IT>C</IT><SUP>iv</SUP><SUB>CSF</SUB>(<IT>s</IT>) (12)
=<FENCE><FR><NU><AR><R><C>−<FENCE><FR><NU>Q+PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE></C></R><R><C><IT> · </IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></DE></FR></C></R><R><C><IT>+</IT><FR><NU><IT>V</IT><SUB>br</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT>PS<SUB>CSF</SUB><IT> · </IT><FENCE><FR><NU><IT>A</IT></NU><DE><IT>&agr;</IT></DE></FR><IT>+</IT><FR><NU><IT>B</IT></NU><DE><IT>&bgr;</IT></DE></FR></FENCE></C></R></AR></NU><DE><AR><R><C><FENCE><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU>Ar</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></C></R><R><C><IT> · </IT><RAD><RCD>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · D</IT><SUB>t</SUB><IT> · V</IT><SUB>br</SUB></RCD></RAD></C></R></AR></DE></FR><IT>+</IT><FR><NU><FR><NU>PS<SUB>BBB</SUB><IT> · A</IT></NU><DE><IT>&agr;</IT></DE></FR><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · B</IT></NU><DE><IT>&bgr;</IT></DE></FR></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></DE></FR></FENCE><IT>/V</IT><SUB>br</SUB>
With use of equations 11 and 12, the brain-to-unbound serum concentration ratio (Kp,u,br) at steady state and the CSF-to-unbound serum concentration ratio (Kp,u,CSF) at steady state can be obtained as the ratio of AUCbriv to the area under the unbound serum concentration-time curve (AUCu) and that of AUCCSFiv to AUCu by the following equations:
K<SUB>p,u,br</SUB>(at steady state)<IT>=</IT><FR><NU>AUC<SUP>iv</SUP><SUB>br</SUB></NU><DE>AUC<SUB>u</SUB></DE></FR> (13)
 =<FR><NU>V<SUB>br</SUB><IT> · </IT><FENCE>PS<SUB>CSF</SUB><IT>−</IT><FR><NU>PS<SUB>BBB</SUB><IT> · </IT>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)</NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</DE></FR></FENCE></NU><DE><AR><R><C><IT>L</IT>{(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)</C></R><R><C><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD><IT>+</IT>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · </IT>Ar}</C></R></AR></DE></FR>
 · <FENCE>1−exp<FENCE><IT>−L · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></FENCE></FENCE><IT>+</IT><FR><NU>PS<SUB>BBB</SUB><IT> · V</IT><SUB>br</SUB></NU><DE>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</DE></FR>
and
K<SUB>p,u,CSF</SUB>(at steady state)<IT>=</IT><FR><NU>AUC<SUP>iv</SUP><SUB>CSF</SUB></NU><DE>AUC<SUB>u</SUB></DE></FR> (14)
 =<FR><NU>PS<SUB>CSF</SUB><IT>−</IT><FR><NU>PS<SUB>BBB</SUB><IT> · </IT>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)</NU><DE>PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB></DE></FR></NU><DE>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)<IT>+</IT>Ar<IT> · </IT><RAD><RCD>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · D</IT><SUB>t</SUB><IT> · V</IT><SUB>br</SUB></RCD></RAD></DE></FR>
+<FR><NU>PS<SUB>BBB</SUB></NU><DE>PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB></DE></FR>
For an intracerebroventricular administration, mass balance equations describing the drug concentration in the brain tissue and the CSF can be obtained as equations 15 and 16, respectively.
<FR><NU>∂C<SUB>br</SUB>(<IT>x,t</IT>)</NU><DE><IT>∂t</IT></DE></FR><IT>=D</IT><SUB>t</SUB><IT> · </IT><FR><NU><IT>∂<SUP>2</SUP>C</IT><SUB>br</SUB>(<IT>x,t</IT>)</NU><DE><IT>∂x</IT><SUP><IT>2</IT></SUP></DE></FR><IT>−</IT><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)</NU><DE><IT>V</IT><SUB>br</SUB></DE></FR><IT> · C</IT><SUB>br</SUB>(<IT>x,t</IT>) (15)
   V<SUB>CSF</SUB><IT> · </IT><FR><NU>d<IT>C</IT><SUB>CSF</SUB>(<IT>t</IT>)</NU><DE>d<IT>t</IT></DE></FR><IT>=</IT><IT>D</IT><SUB>t</SUB><IT> · </IT>Ar<IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂x</IT></DE></FR> (16)
−(Q+PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)<IT> · </IT>C<SUB>CSF</SUB>(<IT>t</IT>)
Assuming that CCSF(t) = CISF(0,t) = Cbr(0,t)/Vbr, the following equa tion can be obtained as a boundary condition of equation 15, at x =0:
   V<SUB>CSF</SUB><IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂t</IT></DE></FR><IT>=</IT><IT>D</IT><SUB>t</SUB><IT> · </IT>Ar<IT> · V</IT><SUB>br</SUB><IT> · </IT><FR><NU><IT>∂C</IT><SUB>br</SUB>(<IT>0,t</IT>)</NU><DE><IT>∂x</IT></DE></FR> (17)
−(Q+PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)<IT> · C</IT><SUB>br</SUB>(<IT>0,t</IT>)
With the boundary condition that a distance x is significantly greater than x*, the following relation is obtained, at x >=  x*.
C<SUB>br</SUB>(<IT>x*,t</IT>)<IT>=0</IT> (18)

As an initial condition of equation 15, the following relationship is obtained for the CSF concentration at time zero:
C<SUB>CSF</SUB>(<IT>0</IT>)<IT>=</IT><FR><NU>DOSE</NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR> (19)
Taking the Laplace transform of equations 15 to 17, the following equations can be obtained.
C<SUP>icv</SUP><SUB>ISF</SUB>(<IT>x,s</IT>) (20)
<IT>=</IT><FR><NU><IT>DOSE/V</IT><SUB>CSF</SUB></NU><DE><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU>Ar<IT> · V</IT><SUB>br</SUB><IT> · D</IT><SUB>t</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></DE></FR>
<IT> · exp</IT><FENCE><IT>−x · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></FENCE>
and
C<SUP>icv</SUP><SUB>CSF</SUB>(<IT>s</IT>) (21)
<IT>=</IT><FR><NU><IT>DOSE/V</IT><SUB>CSF</SUB></NU><DE><FENCE><IT>s+</IT><FR><NU><IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR></FENCE><IT>+</IT><FR><NU>Ar<IT> · V</IT><SUB>br</SUB><IT> · D</IT><SUB>t</SUB></NU><DE><IT>V</IT><SUB>CSF</SUB></DE></FR><IT> · </IT><RAD><RCD><FR><NU>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT>/V</IT><SUB>br</SUB><IT>+s</IT></NU><DE><IT>D</IT><SUB>t</SUB></DE></FR></RCD></RAD></DE></FR>
With use of equation 21, the area under concentration-time curve of the CSF after an intracerebroventricular administration (AUCCSFicv) was obtained as:
AUC<SUP>icv</SUP><SUB>CSF</SUB><IT>=</IT><LIM><OP>lim</OP><LL><IT>s→0</IT></LL></LIM><IT>C</IT><SUP>icv</SUP><SUB>CSF</SUB>(<IT>s</IT>) (22)
<IT>=</IT><FR><NU><IT>DOSE</IT></NU><DE>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>)<IT>+</IT><RAD><RCD>Ar<SUP><IT>2</IT></SUP><IT> · V</IT><SUB>br</SUB><IT> · </IT>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · D</IT><SUB>t</SUB></RCD></RAD></DE></FR>
Accordingly, the efflux clearance from the CSF after an intracerebroventricular bolus administration (CLCSF) is described by the following equation.
CL<SUB>CSF</SUB><IT>=</IT>(<IT>Q+</IT>PS<SUB>CSF</SUB><IT>+</IT>PS<SUB>CSF,eff</SUB>) (23)
<IT>+</IT><RAD><RCD><IT>Ar<SUP>2</SUP> · V</IT><SUB>br</SUB><IT> · </IT>(PS<SUB>BBB</SUB><IT>+</IT>PS<SUB>BBB,eff</SUB>)<IT> · D</IT><SUB>t</SUB></RCD></RAD>

Estimation of BBB and BCSFB permeability. For the model analysis, the fixed parameters were obtained in the following way. Regarding Dt of quinolones, the diffusion coefficient of quinolones in agar (Dw), was estimated from a previous report based on the molecular weight (Fenstermacher and Kaye, 1988). Based on the previously reported relationship (Fenstermacher and Kaye, 1988) between the ratio of Dt to Dw and Vbr, defined as the ratio of the Cbr and CISF, the Dt value of each quinolone was estimated and is listed in table 1. The Vbr values of NFLX, OFLX, FLRX and PFLX were taken from a previous report which was determined by using a brain microdialysis (Ooie et al., 1997). For AM-1155 and SPFX, the Vbr value was estimated from the mean Vbr value of NFLX, OFLX, FLRX and PFLX, i.e., 1.94 ± 0.36 ml/g brain (mean ± S.E.). PSCSF,eff was obtained from the uptake study using the isolated choroid plexus reported previously (Ooie et al., 1996c). The serum unbound fraction (fu) of quinolones, Q, VCSF, Ar, and L were taken from previous reports (Cserr and Dyke 1971; Ogawa et al., 1994; Ooie et al., 1996c; Suzuki et al., 1985) and are listed in tables 1 and 2. The total brain concentration-to-unbound serum concentration ratio (Kp,u,br) at steady state and the CSF-to-unbound serum concentration ratio (Kp,u,CSF) at steady state after i.v. constant infusion, and CLCSF were taken from previous reports (Ooie et al., 1996b,c) and are listed in table 1.


                              
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TABLE 1
Physicochemical and pharmacokinetic parameters of quinolone antibiotics


                              
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TABLE 2
Physiological and anatomical parameters used for the distributed model analysis

By use of equations 9, 10 and 21, PSBBB, PSBBB,eff and PSCSF were determined simultaneously by a nonlinear least squares regression analysis program combined with the fast inverse Laplace transform algorithm (MULTI(FILT)) developed previously (Yano et al., 1989). For the model fitting, the following in vivo data were used simultaneously: 1) Cbr-time profile after i.v. bolus administration (data shown in fig. 2B as an integration plot); 2) CCSF-time profile after i.v. bolus administration (data shown in fig. 2C as an integration plot); 3) The value of Kp,u,br at steady state after a constant i.v. infusion (table 1); 4) The value of Kp,u,CSF at steady state after constant i.v. infusion (table 1); 5) CCSF-time profile after intracerebroventricular bolus administration (taken from a previous study; Ooie et al., 1996b). Cp,u-time profiles of quinolones descried above were substituted for A, B, alpha  and beta  in equations 9 and 10. The initial values of PSBBB and PSCSF were set as the apparent influx clearance obtained in in vivo experiment, PSBBB,app and PSCSF,app, respectively. The initial value of PSBBB,eff was assumed to be zero. The PSBBB and PSCSF were allowed to vary within a range of ±50% of its initial value.


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Fig. 2.   Unbound serum concentration-time profile (A), total brain-to-unbound serum concentration ratio (Kp,u,br; B) versus the ratio of the area under the unbound serum concentration time curve (AUCu) to the unbound serum concentration (Cp,u), and CSF-to-unbound serum concentration ratio (Kp,u,CSF; C) versus the ratio of the area under the unbound serum concentration time curve (AUCu) to the unbound serum concentration (Cp,u) of quinolones in rats. Six different quinolones (10 mg/kg) were administered intravenously and blood samples were collected. At 1, 3, 5 and 10 min after dosing, CSF was obtained from individual rats by cisternal puncture. Immediately after the collection of CSF, the cerebrum was removed. Each point represents the mean ± S.E. of 4 to 12 animals. Where error bars are not shown, the S.E. is contained within the symbol. square , NFLX; open circle , AM-1155; black-triangle, FLRX; black-square, OFLX; triangle , SPFX; bullet , PFLX.

The concentration of quinolone in brain tissue was determined by subtracting the quinolone concentration in the brain vascular space from the observed total brain concentration. The blood vascular volume was assumed to be 0.020 ml/g from the reported plasma vascular volume (0.011 ml/g; Pardridge et al., 1991) using a hematocrit of 0.45. This value has been reported as the distribution space of mouse immunoglobulin G in rat brain (Pardridge et al., 1991). Reed and Woodbury (1963) obtained a value of 0.01 ml/g for the distribution of [14C]inulin (5,000 Da) in rat brain, whereas they obtained value of 0.005 ml/g for [131I]serum albumin (69,000 Da). With use of sucrose, Smith et al. (1988) also reported that the vascular space in rat brain is approximately 0.007 ml/g brain. Because we did not measure the cerebral vascular space in each rat, variations in this value may affect the analysis, in particular for quinolones (such as NFLX) whose brain distribution is limited.

Simulation of drug concentration in the CNS. The equations for Kp,u,br (equation 13) and Kp,u,CSF (equation 14) at steady state after i.v. administration and for CLCSF after intracerebroventricular administration (equation 23) were used in the simulation study. To predict the CISF in various regions of the CNS, equations 8 and 20 were used. Unbound serum concentration versus time profiles of three different quinolones (NFLX, FLRX and PFLX) were taken from previous reports (Ichikawa et al., 1992; Jaehde et al., 1992; Kusajima et al., 1986) and were used for the estimation of CISF after i.v. bolus administration at a dose of 10 mg/kg. Furthermore, CISF after intracerebroventricular administration at a dose of 10 µg/animal was predicted with equation 20. For the simulation study, Laplace transformed equations (equations 8 and 20) were analyzed using the fast inverse Laplace transform program (FILT; Yano et al., 1989).

Data analysis. Model calculation and fitting were carried out on an IBM RISC System/6000 work station using AIX XL FORTRAN Compiler/6000. The results of kinetic analysis are expressed as means ± calculated S.D. except when noted otherwise. Statistical analysis was performed by Student's t-test. Correlation was tested by Pearson's product moment correlation coefficient (r).

    Results
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Abstract
Introduction
Materials & Methods
Results
Discussion
References

CNS distribution of quinolones after i.v. bolus administration. The concentrations in the serum, brain tissue and the CSF were determined after i.v. administration of 10 mg/kg of each quinolone. By using the previously reported fu for each quinolone (table 1; Ooie et al., 1996c), the Cp,u-time profiles were obtained and are shown in figure 2A. The pharmacokinetic parameters to describe the curve were obtained by nonlinear least squares regression analysis and are listed in table 1. Figure 2B illustrates initial uptake of quinolones into the CNS after i.v. administration as an integration plot (Kp,u,br vs. AUCu/Cp,u; Patlak et al., 1983). In principle, extrapolation of the Kp,u,br versus AUCu/Cp,u line yields the cerebral vascular volume as the y-intercept. As shown in figure 2B, however, the values of the y-intercept for some quinolones are much higher than the vascular space; e.g., 0.13 and 0.14 ml/g brain for SPFX and PFLX, respectively. These results may be accounted for by considering the rapid passage of these two quinolones across the BBB. To quantify this rapid passage by model analysis, the PSBBB,app value was determined with the early time point (1 min after i.v. administration) data, rather than the slope of the integration plot, assuming no adsorption of quinolone to the luminal surface of brain capillaries and no back flux from the brain into the circulating blood. The PSBBB,app values for six kinds of quinolone antibiotics (table 1) were further used as the initial value for PSBBB in the kinetic analysis. Comparing the values of PSBBB,app, NFLX and PFLX were the smallest and greatest, respectively, and a 35-fold difference was observed between them. Figure 2C illustrates the Kp,u,CSF versus AUC u /Cp,u plot. Similarly, PSCSF,app values were determined and are listed in table 1. Comparing the values of PSCSF,app, NFLX and SPFX were the smallest and greatest, respectively, and a 27-fold difference was observed between them.

Distributed model analysis. By use of equations 9, 10 and 21, PSBBB, PSBBB,eff and PSCSF were obtained by nonlinear least squares regression analysis. Figure 3 represents the comparison between observed and fitted values for the six quinolones. As shown in figure 3, A, C, D and E, a fairly good coincidence was observed between observed and model-fitted values for the brain concentration after i.v. bolus administration, the steady state Kp,u,br and Kp,u,CSF after i.v. constant infusion and the CSF concentration after intracerebroventricular bolus administration. For the CSF concentration after i.v. bolus administration, the model values were relatively smaller than the observed values (fig. 3B).


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Fig. 3.   Comparison of fitted and observed values for quinolone distribution in the CNS. (A) total brain concentration after i.v. bolus administration; (B) CSF concentration after i.v. bolus administration; (C) brain-to-unbound serum concentration ratio (Kp,u,br) at steady state, the observed values were taken from a previous report (Ooie et al., 1996c); (D) CSF-to-unbound serum concentration ratio (Kp,u,CSF) at steady state, the observed values were taken from a previous report (Ooie et al., 1996c); (E) CSF concentration after intracerebroventricular administration, the observed values were taken from a previous report (Ooie et al., 1996b). square , NFLX; open circle , AM-1155; black-triangle, FLRX; black-square, OFLX; triangle , SPFX; bullet , PFLX.

The fitted parameters for the quinolones (PSBBB, PSBBB,eff and PSCSF) are summarized in table 3. The PSBBB values of SPFX and PFLX were about 80-fold greater than the PSBBB value of NFLX. Moreover, the PSBBB,eff value was 11- to 260-fold greater than the PSBBB value (table 3). With use of the fitted parameters obtained, the net flux across the BBB [PSBBB/(PSBBB + PSBBB,eff)] was also calculated. A good correlation was observed (r = 0.93, P < .01) between net flux (table 3) and steady state Kp,br values (table 1). PSCSF of NFLX was smaller than Q, whereas the PSCSF of SPFX was 5-fold greater than Q (table 3). Assuming that PSBBB,eff equals zero, the Kp,u,br values were simulated to be approximately 5- to 10-fold greater than the observed values (data not shown).


                              
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TABLE 3
Permeability clearance of quinolones obtained by nonlinear least squares regression analysis combined with a fast inverse Laplace transform algorithm (MULTI(FILT))

As shown in figure 4A, a fairly good correlation was observed between the PSBBB and the octanol-water partition coefficient (Ooie et al., 1996c) for the quinolones examined (r = 0.90, P < .01). There was also a good correlation between the PSCSF and the octanol-water partition coefficient (r = 0.88, P < .01), but not for the PSBBB,eff (r = 0.52, not significant).


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Fig. 4.   Relationship between the octanol-water partition coefficient (log Papp) and symmetrical permeability clearance across the BBB (PSBBB; A), symmetrical permeability clearance across the BCSFB (PSCSF; B) and asymmetric clearance across the BBB (PSBBB,eff; C). The straight line represents the result of linear regression analysis. square , NFLX; open circle , AM-1155; black-triangle, FLRX; black-square, OFLX; triangle , SPFX; bullet , PFLX.

Because the penetration of ligands across the erythrocyte membrane is rapid enough (Simanjuntak et al., 1991), the unbound plasma concentration equals the unbound blood concentration by their definition. The kinetic parameters defined for the plasma unbound concentration, therefore, can be used if these values are defined for the unbound blood concentration.

Prediction of brain ISF concentration as a function of the distances from the ependymal surface. Figure 5 represents the CISF-time profiles as a function of the distance from the ependymal surface after i.v. bolus administration of NFLX, FLRX and PFLX at a dose of 10 mg/kg to rats. A significant gradient of CISF was observed as a function of the distance from the surface. No significant difference in CISF was observed at cerebral regions more than 1 mm distant from the ependymal surface (fig. 5).


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Fig. 5.   Prediction of concentration-time profile of quinolone distribution in various regions of the CNS and serum after i.v. bolus administration of quinolones, 10 mg/kg, to rats. (A) NFLX; (B) FLRX; (C) PFLX. Values close to the line represent the distance from the ependymal surface.

Figure 6 represents the CISF-time profiles as a function of the distance from the ependymal surface after intracerebroventricular bolus administration of NFLX, FLRX and PFLX at a dose of 10 µg/animal to rats. During the terminal phase, an approximately 10- and 1000-fold difference was observed between the CSF and ISF concentrations at a distance of 0.5 mm and 1 mm from the surface of ependymal cell layer, respectively (fig. 6).


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Fig. 6.   Prediction of brain ISF concentration-time profiles in various regions of the CNS after intracerebroventricular administration of quinolones, 10 µg/animal, to rats. (A) NFLX; (B) FLRX; (C) PFLX. Values close to the line represent the distance from the ependymal surface.

Effect of diffusion through brain tissue and active efflux clearance across the BCSFB on Kp,u,br and Kp,u,CSF at steady state. The equation representing Kp,u,br and Kp,u,CSF at steady state were obtained as equations 13 and 14, respectively. Assuming that the diffusion coefficient through the brain tissue is zero, the Kp,u,br and the Kp,u,CSF values were estimated and compared with the fitted values in figure 7, A and B, respectively. The simulated Kp,u,br value was lower than that of the fitted value, whereas the simulated Kp,u,CSF value was greater than the fitted value for all quinolones studied. Figures 8, A and B, represent the effect of the active efflux clearance across the BCSFB on the Kp,u,br and the Kp,u,CSF values, respectively. Only a slight difference was observed between the fitted and simulated values even if PSCSF,eff was assumed to be zero.


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Fig. 7.   Comparison between fitted (solid bars) and simulated (open bars) Kp,u,br and Kp,u,CSF values assuming no diffusion through brain parenchyma tissue. (A) brain-to-unbound serum concentration ratio at steady state; (B) CSF-to-unbound serum concentration ratio at steady state.


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Fig. 8.   Comparison between fitted (solid bars) and simulated (open bars) Kp,u,br and Kp,u,CSF values assuming no active efflux via a BCSFB (PSCSF,eff = 0). (A) brain-to-unbound serum concentration ratio at steady state; (B) CSF-to-unbound serum concentration ratio at steady state.

Analysis of the efflux clearance from the CSF after an intracerebroventricular bolus administration. The CLCSF is given as a function of Q, PSCSF, PSCSF,eff, Dt and PSBBB,eff (equation 23). By substituting the fitted parameter values to equation 23, CLCSF was calculated. As shown in figure 9, a fairly good agreement between observed and fitted values was obtained for CLCSF. Figure 9 also indicates that the diffusion through the brain tissue and the subsequent efflux across the BBB plays an important role in the elimination of quinolones from the CSF after intracerebroventricular administration.


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Fig. 9.   Contribution of the CSF bulk flow rate (striped bars), active efflux clearance across the BCSFB (cross-hatched bars), symmetrical permeability clearance across the BCSFB (open bars) and diffusion through the brain tissues and the resultant efflux across the BBB (hatched bars) to apparent CSF efflux clearance after intracerebroventricular bolus administration. Observed values of the apparent CSF efflux clearance were taken from a previous report (Ooie et al., 1996b) and represented as closed bars.

    Discussion
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Abstract
Introduction
Materials & Methods
Results
Discussion
References

The drug concentration in the brain ISF is a determinant for in vivo CNS effects, although several processes needed to be considered for the precise analysis. Because there is free ligand exchange between CSF and ISF, the distributed model should be suitable for the kinetic analysis of drug distribution in the brain tissue and CSF (Collins and Dedrick, 1983; Suzuki et al., 1997). The major assumptions of this model are that there is free ligand exchange between CSF and ISF, and that the ligand molecules diffuse through the brain parenchyma according to Fick's law. Both these assumptions have been confirmed as being justified by previous reports in which the ligand concentration in the brain parenchyma was determined as a function of the distance from the ependymal surface in the ventriculocisternal perfusion experiments. The kinetic analysis of the experimental data revealed that the CNS profiles can be described by the assumptions described previously (Patlak and Fenstermacher, 1975; Blasberg et al., 1975; Fenstermacher and Davson, 1982). In addition, Dykstra and his collaborators (1993) confirmed this hypothesis by examining the brain concentration profiles after ligand administration through a microdialysis probe implanted into the cerebral cortex. Fenstermacher and Kaye (1988) summarized the Dt values determined by the method described previously and found a good relationship between Dt and Dw. Based on this relationship, we estimate the Dt values for quinolone antibiotics.

The efflux clearance across the BBB (the sum of PSBBB and PSBBB,eff) was 12- to 260-fold greater than PSBBB. Moreover, after i.v. bolus administration, the concentration gradient was observed from CSF to brain ISF; the brain acts as a sink (fig. 5). These results provide kinetic evidence to support the hypothesis that a significant efflux transport from the brain ISF to the capillary lumen across the BBB is the predominant factor involved in the restricted distribution of quinolones in brain ISF after systemic administration (Ooie et al., 1997). Furthermore, the good correlation between PSBBB/(PSBBB + PSBBB,eff) and the Kp,u,br at the steady state indicated that the transport across the BBB is a determinant for the different distribution of these quinolones in the brain tissue.

To evaluate the effect of drug diffusion through the brain tissue on the apparent distribution in brain tissue and the CSF, simulation studies were performed for the prediction of Kp,u,br and Kp,u,CSF at steady state assuming no drug diffusion through brain tissue. As shown in figure 7, 16% to 52% reduction was observed in Kp,u,br whereas 170% to 45% increase was demonstrated in Kp,u,CSF. These results suggest that the CSF acts as a pool to supply quinolone molecules to the brain ISF by diffusion, whereas brain ISF acts as a sink to eliminate quinolone molecules from the CSF at steady state following i.v. administration.

Regarding the efflux across the BCSFB, we have previously demonstrated that the in vitro uptake clearance of beta -lactam antibiotics by the isolated choroid plexus is similar to the in vivo efflux clearance across the BCSFB determined by intracerebroventricular administration (Ogawa et al., 1994). We have also found that quinolone is transported by the isolated choroid plexus via an organic anion transport system which is also responsible for the efflux of beta -lactam antibiotics across the BCSFB (Ooie et al., 1996a). Therefore, in the present study, we have assumed that PSCSF,eff of quinolones is the same as the uptake clearance determined by the isolated choroid plexus reported previously (Ooie et al., 1996c). Assuming that the PSCSF,eff is zero, the participation of active efflux transport across the BCSFB was studied by examining the apparent distribution in the brain tissue and the CSF. As shown in figure 8, active efflux transport across the BCSFB plays only a minor role in the distribution of quinolones both in brain tissue and the CSF. These results are in good agreement with the results shown in figure 9 that less than 20% of the apparent efflux clearance from the CSF is caused by active efflux transport across the BCSFB. Unlike beta -lactam antibiotics reported previously (Ogawa et al., 1994), these simulation results also agree well with our previous finding that probenecid has no significant inhibitory effect on the apparent elimination of FLRX from the CSF after intracerebroventricular administration and that the elimination of FLRX was not saturable (Ooie et al., 1996b).

As a barrier function of brain capillary endothelial cells, it has been reported that P-glycoprotein acts as a primary active efflux transport system to pump vincristine (Tsuji et al., 1992), cyclosporin A (Tatsuta et al., 1992) and vinblastine (Schinkel et al., 1994) out of the brain into the circulating blood. Moreover, several reports have provided kinetic evidence that an efflux transport system for beta -lactam antibiotics (Matsushita et al., 1991), azidodeoxythymidine (Dykstra et al., 1993; Takasawa et al., 1997) and valproic acid (Adkison et al., 1994) is located on the BBB. Although this transport system has not been characterized yet, the transporter may be different from P-glycoprotein (mdr1).

Regarding the CNS toxicity of quinolone antibiotics, drug concentrations in the brain ISF would be a determinant for their duration and severity. The present study suggests that the affinity of quinolones to a putative carrier-mediated efflux transport system may be important in reducing brain ISF concentrations and consequent CNS effect. Although a 10-fold difference was observed between SPFX and OFLX for PSBBB,eff (table 3), comparison with the physicochemical nature of quinolones revealed that there is no significant relationship between the lipophilicity and PSBBB,eff (fig. 4C). Because it has not been possible to demonstrate the efflux transport of quinolones in the primary cultured bovine brain capillary endothelial cells (Jaehde et al., 1993), presumably because of the down-regulation of the expression of the transporter, it would be important to use an in vivo method to characterize the transport property across the BBB. One of the rational ways to characterize the efflux transport system at the BBB is to examine the elimination of ligand from the brain after microinjection into the cerebral cortex (Leininger et al., 1991; Banks et al., 1994; Kakee et al., 1996).

In conclusion, it has been demonstrated that the significantly limited distribution of quinolones in the brain tissue is caused by the presence of an active efflux transport system located on the BBB. Depending on the distance from the ependymal surface, there is a significant concentration gradient from the CSF to the brain ISF after systemic administration. One of the most important factors regulating brain ISF concentrations of quinolones may be an affinity for the putative efflux transport system on the BBB.

    GLOSSARY

Cp,u = unbound serum concentration
fu = serum unbound fraction
AUCu = area under the unbound serum concentration-time curve
PSBBB,app = apparent influx clearance across the BBB
PSCSF,app = apparent influx clearance across the BCSFB
PSBBB = symmetrical permeability clearance across the BBB
PSBBB,eff = efflux clearance across the BBB
PSCSF = symmetrical permeability clearance across the BCSFB
PSCSF,eff = efflux clearance across the BCSFB
Cbr = total brain concentration
CISF = ISF concentration
CCSF = CSF concentration
Kp,u,br = total brain-to-unbound serum concentration ratio (Cbr/Cp,u)
Kp,u,CSF = CSF-to-unbound serum concentration ratio (CCSF/Cp,u)
CLCSF = apparent efflux clearance from the CSF
Dt = diffusion coefficient in the brain tissue
Dw = diffusion coefficient in the agar
Mw = molecular weight
Vbr = distribution volume in brain tissue (Cbr/CISF)
VCSF = volume of the CSF
Ar = surface area of the ependyma
Q = bulk flow rate of the CSF
L = thickness of the brain cortex

    Footnotes

Accepted for publication June 10, 1997.

Received for publication January 6, 1997.

1   This research was supported in part by a Grant-in-Aid for Scientific Research from the Ministry of Education, Science and Culture, Japan and the Research Fund from the Human Science Foundation.

2   Present address: Central Research Laboratories, Kyorin Pharmaceutical Co., Ltd., Nogi-machi, Shimotsuga-gun, Tochigi 329-01, Japan.

3   Present address: Department of Pharmaceutics, Faculty of Pharmaceutical Sciences, Tohoku University, Aoba-ku, Sendai 980-77, Japan.

Send reprint requests to: Yuichi Sugiyama, Ph.D., Professor, Department of Pharmaceutics, Faculty of Pharmaceutical Sciences, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113, Japan.

    Abbreviations

CNS, central nervous system; GABA, gamma -aminobutyric acid; CSF, cerebrospinal fluid; ISF, interstitial fluid; BBB, blood-brain barrier; BCSFB, blood-CSF barrier; NFLX, norfloxacin; OFLX, ofloxacin; FLRX, fleroxacin; PFLX, pefloxacin; AM-1155, (±)-1-cyclopropyl-6-fluoro-1,4-dihydro-8-methoxy-7-(3-methyl-1-piperazinyl)-4-oxo-3-quinolinecarboxylic acid ; SPFX, sparfloxacin; HPLC, high-performance liquid chromatography.

    References
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Abstract
Introduction
Materials & Methods
Results
Discussion
References


0022-3565/97/2831-0293$03.00/0
THE JOURNAL OF PHARMACOLOGY AND EXPERIMENTAL THERAPEUTICS
Copyright © 1997 by The American Society for Pharmacology and Experimental Therapeutics



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