<i>I</i> <sub>A</sub> in Kenyon Cells of the Mushroom Body of Honeybees Resembles Shaker Currents: Kinetics, Modulation by K<sup>+</sup>, and Simulation

  • Corinna Pelz
    Institut für Neurobiologie, Freie Universität Berlin, D-14195 Berlin, Germany
  • Johannes Jander
    Institut für Neurobiologie, Freie Universität Berlin, D-14195 Berlin, Germany
  • Hendrik Rosenboom
    Institut für Neurobiologie, Freie Universität Berlin, D-14195 Berlin, Germany
  • Martin Hammer
    Institut für Neurobiologie, Freie Universität Berlin, D-14195 Berlin, Germany
  • Randolf Menzel
    Institut für Neurobiologie, Freie Universität Berlin, D-14195 Berlin, Germany

抄録

<jats:p> I <jats:sub>A</jats:sub> in Kenyon cells of the mushroom body of honeybees resembles shaker currents: kinetics, modulation by K<jats:sup>+</jats:sup>, and simulation. Cultured Kenyon cells from the mushroom body of the honeybee, Apis mellifera, show a voltage-gated, fast transient K<jats:sup>+</jats:sup> current that is sensitive to 4-aminopyridine, an A current. The kinetic properties of this A current and its modulation by extracellular K<jats:sup>+</jats:sup> ions were investigated in vitro with the whole cell patch-clamp technique. The A current was isolated from other voltage-gated currents either pharmacologically or with suitable voltage-clamp protocols. Hodgkin- and Huxley-style mathematical equations were used for the description of this current and for the simulation of action potentials in a Kenyon cell model. Activation and inactivation of the A current are fast and voltage dependent with time constants of 0.4 ± 0.1 ms (means ± SE) at +45 mV and 3.0 ± 1.6 ms at +45 mV, respectively. The pronounced voltage dependence of the inactivation kinetics indicates that at least a part of this current of the honeybee Kenyon cells is a shaker-like current. Deactivation and recovery from inactivation also show voltage dependency. The time constant of deactivation has a value of 0.4 ± 0.1 ms at −75 mV. Recovery from inactivation needs a double-exponential function to be fitted adequately; the resulting time constants are 18 ± 3.1 ms for the fast and 745 ± 107 ms for the slow process at −75 mV. Half-maximal activation of the A current occurs at −0.7 ± 2.9 mV, and half-maximal inactivation occurs at −54.7 ± 2.4 mV. An increase in the extracellular K<jats:sup>+</jats:sup>concentration increases the conductance and accelerates the recovery from inactivation of the A current, affecting the slow but not the fast time constant. With respect to these modulations the current under investigation resembles some of the shaker-like currents. The data of the A current were incorporated into a reduced computational model of the voltage-gated currents of Kenyon cells. In addition, the model contained a delayed rectifier K<jats:sup>+</jats:sup> current, a Na<jats:sup>+</jats:sup>current, and a leakage current. The model is able to generate an action potential on current injection. The model predicts that the A current causes repolarization of the action potential but not a delay in the initiation of the action potential. It further predicts that the activation of the delayed rectifier K<jats:sup>+</jats:sup> current is too slow to contribute markedly to repolarization during a single action potential. Because of its fast activation, the A current reduces the amplitude of the net depolarizing current and thus reduces the peak amplitude and the duration of the action potential. </jats:p>

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