Membrane potential measurements of unfertilized and fertilized Xenopus laevis eggs are affected by damage caused by the electrode

Iron oxide nanoparticles can cross plasma membranes

Iron deficiency is a major global public health problem despite decades of efforts with iron supplementation and fortification. The issue lies on the poor tolerability of the standard of care soluble iron salts, leading to non-compliance and ineffective correction of iron-deficiency anaemia. Iron nanoformulations have been proposed to fortify food and feed to address these issues. Since it was just postulated that some nanoparticles (NPs) might cross the plasma membrane also by a non-endocytotic pathway gaining direct access to the cytoplasm, we have studied iron NP uptake under this perspective. To this aim, we have used a recently tested protocol that has proven to be capable of following the cytoplasmic changes of iron concentration dynamics and we have demonstrated that iron oxide NPs, but not zerovalent iron NPs nor iron oxide NPs that were surrounded by a protein corona, can cross plasma membranes. By electrophysiology, we have also shown that a small and transient increase of membrane conductance parallels NP crossing of plasma membrane.

High-intensity electrostatic-field exposure system for cultured biological cells

We describe a new system for exposing cultured biological cells that have been plated on coverslips to strong electrostatic fields at magnitudes greater than 10(3) V/cm. Techniques are described that make use of mineral oil to render insignificant electrical conduction currents (total leakage current is less than 1.0 nA or less than 0.1 nA/coverslip), joule heating (less than 10(-6) W), or current-induced magnetic fields (less than 10(-13) T) in regions inhabited by cells. The mineral oil also eliminates a reduction in the strength of the applied field, which otherwise can occur from increased electrode-to-medium impedance at the site of application. Thus the applied field is reliably specified in the vicinity of a cell membrane. Control and electrostatic field chambers are housed in a grounded metal incubator. Cylindrical mu-metal shields can be used to reduce background magnetic fields in each chamber from 40 microT static and approximately 1 microT ac to, respectively, less than 3 microT static and approximately 100 nT ac. Contamination of cells by impurity atoms that may leach from electrodes was measured by atomic-absorption spectrophotometry and found to be negligible. Stray magnetic- and electric-field components within the incubator were measured, as were background fields around the laboratory.

Electrophysiological properties of Dictyostelium derived from membrane potential measurements with microelectrodes

Electrical membrane properties of the cellular slime mold Dictyostelium discoideum were investigated with the use of intracellular microelectrodes. The rapid potential transients (1 msec) upon microelectrode penetration of normal cells had a negative-going peak-shaped time course. This indicates that penetration of a cell with a microelectrode causes a rapid depolarization, which can just be recorded by the microelectrode itself. Therefore, the initial (negative) peak potential transient value Ep (-19mV) should be used as an indicator of the resting membrane potential Em of D. discoideum before impalement, rather than the subsequent semistationary depolarized value En (-5 mV). Using enlarged cells such as giant mutant cells (Ep = -39 mV) and electrofused normal cells (Ep = -30 mV) improved the reliability of Ep as an indicator of Em. From the data we concluded that Em of D. discoideum cells bathed in (mM) 40 NaCl, 5 KCl and 1 CaCl2 is at least -50 mV. This potential was shown to be dependent on extracellular potassium. The average input resistance Ri of the impaled cells was 56 M omega for normal D. discoideum. However, our analysis indicates that the membrane resistance of these cells before impalement is greater than 1 G omega. Specific membrane capacitance was 1-3 pF/cm2. Long-term recording of the membrane potential showed the existence of a transient hyperpolarization following the rapid impalement transient. This hyperpolarization was associated with an increase in Ri of the impaled cell. It was followed by a depolarization, which was associated with a decrease in Ri. The depolarization time was dependent on the filling of the microelectrode. The present characterization of the electrical membrane properties of Dictyostelium cells is a first step in a membrane electrophysiological analysis of signal transduction in cellular slime molds.

Calcium-dependent events at fertilization of the frog egg: injection of a calcium buffer blocks ion channel opening, exocytosis, and formation of pronuclei

Eggs of Xenopus laevis were injected with a calcium buffer before insemination, to examine the effect of preventing or suppressing the sperm-induced increase in intracellular calcium on the fertilization potential, exocytosis, and pronuclear formation. Microinjection of BAPTA [(1,2-bis(o-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid)] at concentrations between 0.2 and 0.7 mM usually suppressed the fertilization potential to a series of transient depolarizations. The fertilization potential was completely inhibited when the final concentration of BAPTA in the egg was greater than 0.7 mM. These observations support the hypothesis that activation of the chloride conductance responsible for the fertilization potential depends on an increase in intracellular calcium. Exocytosis of cortical granules and elevation of the fertilization envelope were prevented by injecting BAPTA at concentrations greater than 0.2 mM. Injection of BAPTA to suppress the rise in calcium did not inhibit sperm entry and BAPTA-injected eggs were highly polyspermic. Examination by light and electron microscopy revealed that sperm decondensation and pronuclear formation were prevented by injection of the calcium buffer before insemination.

Resting membrane potential and inward current properties of mouse ovarian oocytes and eggs

The electrical properties of the membrane of the ovarian oocyte at the germinal vesicle (GV) stage and of the ovulated egg of the mouse have been studied using a two-microelectrode voltage-clamp technique. The stable resting potential measured with a single electrode was -38.2 +/- 2.8 mV SE (18 oocytes, 5 animals) and -27.8 +/- 1.4 mV SE (28 eggs, 8 animals) in a solution containing 20 mM [Ca2+]0. The lower values appear to be strongly affected by damage due to electrode insertion. However, there was no evidence of the resting potential being more negative than -40 to -50 mV. Voltage-dependent inward current could not be activated from a holding potential (Vh) close to the resting potential. When Vh was set at -90 mV, depolarizing pulses activated a transient inward current in both oocytes and eggs. The threshold voltage, peak voltage and inactivation vs potential curve were very similar in oocytes and eggs. On the other hand, the current amplitude appeared reduced in ovulated eggs, whilst times to peak and inactivation time constants in eggs were significantly longer than in oocytes. In oocytes the inward current was blocked by 10 mM Co2+ and decreased by lowering [Ca2+]0 to 5 mM similarly to the results reported for eggs. It therefore appears that GV ovarian oocytes possess Ca2+ channels which differ from those present in eggs mainly with respect to their kinetic properties. The physiological role of this inward current remains obscure in both preparations since they are almost completely inactivated at the resting potential.