Kinetics of Extracellular ATP from Goldfish Hepatocytes: A Lesson from Mathematical Modeling

被引:5
作者
Chara, Osvaldo [2 ,3 ]
Pafundo, Diego E. [1 ]
Schwarzbaum, Pablo J. [1 ]
机构
[1] Univ Buenos Aires, Fac Farm & Bioquim, IQUIFIB, RA-1113 Buenos Aires, DF, Argentina
[2] Univ Buenos Aires, Fac Med, Dept Fisiol & Biofis, RA-1121 Buenos Aires, DF, Argentina
[3] Natl Univ La Plata, Consejo Nacl Invest Cient & Tecn, Inst Fis Liquidos & Sistemas Biol, Comis Invest Cient Prov Buenos Aires, RA-1900 La Plata, Argentina
关键词
Extracellular ATP; Mathematical modeling; Simulations; Release of ATP; RELEASE; MECHANISMS; MEMBRANE;
D O I
10.1007/s11538-008-9392-4
中图分类号
Q [生物科学];
学科分类号
090105 [作物生产系统与生态工程];
摘要
In goldfish hepatocytes, hypotonic exposure leads to cell swelling, followed by a compensatory shrinkage termed RVD. It has been previously shown that ATP is accumulated in the extracellular medium of swollen cells in a non-linear fashion, and that extracellular ATP (ATPe) is an essential intermediate to trigger RVD. Thus, to understand how RVD proceeds in goldfish hepatocytes, we developed two mathematical models accounting for the experimental ATPe kinetics reported recently by Pafundo et al. in Am. J. Physiol. 294, R220-R233, 2008. Four different equations for ATPe fluxes were built to account for the release of ATP by lytic (J (L) ) and nonlytic mechanisms (J (NL) ), ATPe diffusion (J (D) ), and ATPe consumption by ectonucleotidases (J (V) ). Particular focus was given to J (NL) , defined as the product of a time function (J (R) ) and a positive feedback mechanism whereby ATPe amplifies J (NL) . Several J (R) functions (Constant, Step, Impulse, Gaussian, and Lognormal) were studied. Models were tested without (model 1) or with (model 2) diffusion of ATPe. Mathematical analysis allowed us to get a general expression for each of the models. Subsequently, by using model dependent fit (simulations) as well as model analysis at infinite time, we observed that: use of J (D) does not lead to improvements of the models. Constant and Step time functions are only applicable when J (R) =0 (and thus, J (NL) =0), so that the only source of ATPe would be J (L) , a result incompatible with experimental data. use of impulse, Gaussian, and lognormal J (R) s in the models led to reasonable good fits to experimental data, with the lognormal function in model 1 providing the best option.
引用
收藏
页码:1025 / 1047
页数:23
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