Nagasaki 852, Japan. (Na+, Li+) cations can pass through the Ca channels to generate action potentials. performed using single glass micro-electrodes.

Size: px
Start display at page:

Download "Nagasaki 852, Japan. (Na+, Li+) cations can pass through the Ca channels to generate action potentials. performed using single glass micro-electrodes."

Transcription

1 J. Physiol. (1983), 339, pp With 8 text-figures Printed in G0reat Britain PERMEATION OF DIVALENT AND MONOVALENT CATIONS THROUGH THE OVARIAN OOCYTE MEMBRANE OF THE MOUSE BY SHIGERU YOSHIDA From the Department of Physiology, Nagasaki University School of Medicine, Nagasaki 852, Japan (Received 14 September 1982) SUMMARY 1. Ovarian oocytes were isolated from adult mice and intracellular recording was performed using single glass micro-electrodes. 2. The resting potential was mv in standard solution, and the oocyte showed a regenerative response at the cessation of hyperpolarizing current pulse. 3. Ca spikes were observed under Na+-free conditions. The overshoot of the spike increased 28 mv for a 10-fold increase in [Ca2+]0 and showed saturation as [Ca2+]0 was elevated. The spike was insensitive to tetrodotoxin (TTX) and was blocked by polyvalent cations such as Co2+, Cd2+, Mn2+ and La3+. Sr2+ or Ba2+ substituted for Ca2+ in generating action potentials. 4. Na spikes were observed under Ca2+-free conditions. The overshoot of the spike showed the slope of 39 mv for a 10-fold increase in [Na+]o and a saturation was detected when [Na+]0 was raised. The spike was resistant to TTX and was blocked by Ca antagonists such as Co2+, Cd2+, Mn2+ or La3+. Li+ substituted for Na+ in producing spikes, while Rb+ did not. The overshoot and maximum rate of rise of the Na spike became smaller when Ca2+ was present in the bathing solution, indicating a competition between Na+ and Ca Mn2+ acted not only as a Ca blocker but also as a charge carrier during excitation. Mn spikes were detected in Na+-, Ca2+-free solutions and were blocked by Ca antagonists. 6. The resting membrane is permeable to not only Na+ but also to some extent to K+. 7. It is suggested that the ovarian oocyte membrane of the mouse has voltagedependent Ca channels, and both divalent (Ca2+, Sr2+, Ba2+, Mn2+) and monovalent (Na+, Li+) cations can pass through the Ca channels to generate action potentials. INTRODUCTION Electrical properties of the egg cell membrane have been studied in marine animals, amphibians, insects and mammals (see reviews: Hagiwara & Miyazaki, 1977; Hagiwara & Jaffe, 1979; Hagiwara & Byerly, 1981). Since Takahashi and his colleagues showed that the tunicate eggs were excitable (Takahashi, Miyazaki & Kidokoro, 1971), action potentials have been reported in various kinds of eggs and

2 632 such action potentials were found to be produced by divalent cations passing through Ca channels. In contrast, Na channels were described only in tunicate eggs (Miyazaki, Takahashi & Tsuda, 1974) and in Xenopus oocytes (Baud, Kado & Marcher, 1982). Thus, it has been generally considered that the Ca channels but not Na channels are widely distributed in eggs. As for mammalian preparations, electrophysiological study has been performed in oocytes of the mouse (Powers & Tupper, 1974; Okamoto, Takahashi & Yamashita, 1977; Yamashita, 1982; Powers, 1982). It was shown that the unfertilized oocytes could generate Ca-dependent action potentials as off-responses at the cessation of hyperpolarization, and the excitability was retained by substituting Sr2+ or Ba2+ for Ca2+ (Okamoto et al. 1977). They concluded that the inward current is attributable to Ca current through Ca channels and the contribution of Na ions to the current was negligible. In the present study, electrophysiological experiments were carried out on isolated ovarian oocytes of the mouse. A preliminary report has been published (Yoshida, 1982). TABLE 1. S. YOSHIDA Ionic compositions of solutions (mm) NaCl KCl CaCl2 MnCl2 MgCl2 TMA-Cl PIPES (1) Standard (2)0Na,OCa (3)0Na,80Ca (4)ONa, 320Ca (5) 0 Na, 0Ca,80Mn (6) XNa, 0Ca X All solutions contained1 mg/ml. glucose and were adjusted to ph 7*4 using 5 mm-pipes. Solutions of desired ionic concentration were obtained by mixing these media in an appropriate ratio. X indictes that X mm (between 150 and 750 mm) NaCl is present in the solution (6). In solutions lacking Ca2+, 2 mm-egta was added to chelate residual CA2+. TMA-Cl is tetramethylammonium chloride. For other solutions see text. METHODS Material&. Ovaries were dissected from sexually mature (older than 8 weeks) female mice of ICR strain. The ovaries were cleared of the adipose and the connective tissues covering the surface of them with surgical knives and the large follicles were broken with shap hypodermal needles under a dissecting microscope in the standard solution containing 0-2 % hyaluronidase (Type I-S, Sigma) at room temperature (20-23 C). The follicular cells surrounding the oocytes were dispersed by hyaluronidase in a few minutes and the isolated ovarian oocytes were collected and rinsed with standard solution (Iwamatsu & Chung, 1972). The diameter of the isolated oocytes was between 40 and 60 #m. Solutions. Table 1 lists the compositions of the solutions used in the present study. All solutions contained 1 mg/ml. glucose and the ph was adjusted to 7-4 using piperazine-n-n'-bis(2- ethanesulphonic acid) (PIPES) as a buffer. In the standard solution, PIPES was titrated with NaOH to adjust the ph. In Na+-free solutions, NaCl was replaced with tetramethylammonium chloride (TMA-Cl; Nakarai Chemicals, Japan) and the PIPES was titrated with tetramethylammonium hydroxide (TMA-OH). Sr2+ or Ba21 solution was prepared by substituting SrCl2 or BaCl2 for CaCl2. Similarly, Li+ or Rb+ solution was made by substituting LiCl or RbCl for NaCl, and the PIPES was titrated with NaOH in Na+ solutions and with TMA-OH in Li+ and Rb+ solutions to adjust the ph. 2 mm-ethylene glycol bis (fl-aminoethylether)-n,n'-tetraacetic acid (EGTA) was added to these Ca2+-free, monovalent-cation solutions to chelate residual Ca2+. A medium having a desired concentration of ions was obtained by mixing these solutions in an appropriate ratio. Tetrodotoxin (TTX; Sankyo, Japan), CoC12, CdCl2 and LaCl3 were applied to test solutions when necessary.

3 EXCITABILITY OF OVARIAN OOCYTES Recordings. Intracellular recordings were performing by penetrating the isolated ovarian oocytes with a single glass micro-electrode filled with 3 M-KCl (30-60 MO resistance). The penetration was performed by applying an oscillating current through the electrode by transiently increasing the negative capacitance of the pre-amplifier. A bridge circuit was used for simultaneous current injection and membrane potential recording. The measurement of the membrane potential was performed by recording the potential difference between an intracellular electrode and a reference electrode. The intensity of the current injected through the electrode was monitored by the potential drop across a 109 Q resistor. Differentiation of the membrane potential was carried out using an electrical differentiator. All experiments were performed at room temperature (20-23 TC). A mV - 2nA 05 sec Fig. 1. Intracellular recordings of potential responses obtained from the isolated ovarian oocyte of the mouse in standard solution. A, regenerative response elicited at the cessation of hyperpolarizing current pulse. B, action potentials revealed by two-step current stimulation. Dashed line: reference potential level. Voltage, current and time scales apply to both records. (Part of action potentials is retouched.) RESULTS Action potentials in standard solution The resting potential of the isolated mouse ovarian oocytes was mv (mean + S.D.) (n = 8) in standard solution. The membrane resistance was between 11-4 and MQ (average, 39-0 Me). The present study shows for the first time that the mammalian oocyte membrane is excitable even before ovulation. Fig. 1 illustrates responses of the ovarian oocyte having the resting potential of -7 mv in standard solution. The dashed line indicates the reference or zero potential level. The membrane showed only a passive electrotonic response when hyperpolarized with a small current. However, a regenerative response was elicited at the cessation of the current pulse when the membrane was hyperpolarized approximately below -70 mv (Fig. 1 A). The spike reached a voltage of +4 mv. Two-step current stimulation was applied to the oocyte to reveal action potentials more clearly (Fig. 1 B). A hyperpolarizing pre-pulse was used to remove inactivation of the ionic channels, and a test pulse, triggered on the end of the pre-pulse, evoked the action potentials. The time course and the threshold membrane potential of the spike can be clearly seen using this technique. The action potentials are slow in time course, and the duration of the spike is 0-22 sec at the critical level in this case.

4 634 S. YOSHIDA In order to check the ionic mechanisms underlying the generation of action potentials, excitability of the oocyte membrane was examined both under Na+-free and Ca2+-free conditions. Action potentials dependent on divalent cations For checking responses of the ovarian oocyte under Na+-free conditions, external Ca2+ concentration ([Ca2+]0) of the bathing medium was chosen to be 10, 20, 40, 80, 160 or 320 mm. Na+ was replaced with tetramethylammonium+ (TMA+) to compensate the osmolarity of the solution when [Ca2+]o was less than 80 mm (see Table 1.) A 0 Na, 20 mm-ca B 0 Na, 80 mm-ca C 0 Na, 320 mm-ca - - -N mv v...j... L10 V/sec IlnA 0-5sec Fig. 2. Effects ofexternal Ca2+ concentration on the overshoot of the action potential under Na+-free conditions. Dashed line: zero potential level. Top traces: membrane potential. Middle traces: differentiated record of the membrane potential. Bottom traces: current pulses used for stimulation. Spikes in A and B are generated by hyperpolarizing current pulse in the form of off-responses, while the spike in C is produced by a depolarizing current pulse because the resting potential is large in Na+-free, 320 mm-ca2+ solution. Voltage, differential, current and time calibrations apply to all records. The resting potential increased with log [Ca2+]O approximately in a linear fashion (Fig. 3A, Er). The ovarian oocytes generated action potentials as off-responses when the external Ca2+ concentration was below 160 mm. However, at 320 mm-ca2+, action potentials were elicited by a short depolarizing pulse as displayed in Fig. 2C because the resting potential was large enough to produce spikes in such a way. The overshoot of the spike increased directly with [Ca2+]o (Fig. 2). The values of the peak potential are plotted against log [Ca2+]o (Fig. 3A, E.). The peak value became larger in amplitude and saturated as the magnitude of the membrane hyperpolarization was increased. Thus, the saturated peak values are plotted. The overshoot increased by 28 mv per 10-fold change in [Ca2+]o when [Ca2+]o was changed between 10 and 80 mm. The dashed line in Fig. 3A shows the expected Nernstian slope of 29 mv for a 10-fold increase in [Ca2+]O. A saturation phenomenon was found when [Ca2+]o was greater than 80 mm (Hagiwara, 1973). Fig. 3B shows that the maximum rate of rise (m.r.r.) of the spike, indicating the amount of inward Ca current, was approximately 1 V/sec at 10 mm-ca2+, and it

5 EXCITABILITY OF OVARIAN OOCYTES 635 increased in a linear fashion up to 6 V/sec at 80 mm-ca2+. However, it showed a saturation when [Ca2+]. was more than 80 mm, and it was close to 7 V/sec at 320 mm-ca2. The critical level or the threshold membrane potential of the spike became more positive with the increase of [Ca2+]o (Fig. 3A, En). The critical membrane potential was obtained by examing the spike elicited by two-step current stimulation. This stabilizing action of Ca2+ has been thought to reflect the surface potential of the membrane (Hagiwara, 1973). 40 A - E _ 0' CL (U~~~~~~~~~~~~~E E -50 Er 8 M LB 5e Ca2+ concentration (mm) Fig. 3. A, effects of [Ca2+]0 on the overshoot potential (E8, O), the threshold or critical membrane potential (E,, A) and the resting potential (Er, El) of the spikes under Na+-free conditions. Bars indicate standard deviation. The dashed lines shows the Nernstian slope of 29 mv for a 10-fold increase in [Ca2+]0. B, effects of [Ca2+]o on the maximum rate of rise (m.r.r.) of the spikes. The concentration of Ca2+ is indicated in logarithmic scale (mm). Thus the action potential under Na+-free conditions appears to be dependent on Ca2+. The Ca spikes (Fig. 4A) were insensitive to high concentration of tetrodotoxin (10-5 g/ml. TTX) (Fig. 4B), and were totally blocked by 5 mm-cd2+ added to the bathing medium (Fig. 4C). Other 'Ca blockers' such as 5 mm-co2+, 10 mm-mn2+ and 1 mm-la3+ were also effective in suppressing the Ca spikes (not illustrated). The spikes persisted when external Ca2+ was replaced by Sr2+ (Fig. 4D) or by Ba2+ (Fig. 4E). This evidence indicates that the ovarian oocyte membrane of the mouse has voltage-dependent Ca channels. Action potentials dependent on monovalent cations Possibility that monovalent cations could maintain the action potential was examined in Ca2+-free solutions (2 mm-egta). The oocytes became very leaky under

6 636 S. YOSHIDA such conditions, and a large current was necessary to evoke action potentials. In addition, it was very difficult to obtain a stable recording from the oocytes in such solutions, for example, some oocytes showed regenerative responses immediately after the penetration of the micro-electrode and became inexcitable within a few minutes. On the contrary, when the penetration was performed very successfully, a stable recording was obtained for more than 30 min. When Mn2+ was used to substitute for Ca2+, as was done in the case of ovulated mouse oocytes by Okamoto and others (Okamoto et at. 1977), it was found that the Mn2+ prevented the oocyte 0 Na, 40 mm-ca O'Na, 40 mm-ca A 0 Na, 40 mm-ca B 10-5 g/ml. TTX C 10- g/ml. TTX, 5 mm-cd D ONa, 0Ca, 40mM-Sr E 0Na, OCa, 40mM-Ba 1S~~~~ X g S~~~~50mV _ f'rna 0-5 sec Fig. 4. Divalent cation-dependent action potentials recorded under Na+-free conditions. Ca spikes (A) are insensitive to a high concentration of tetrodotoxin (10-5 g/ml. TTX) (B), and were blocked by 5 mm-cd2+ (C). Sr21 (D) or Ba2+ (E) substitutes for Ca2+ in generating action potentials. Voltage, current and time calibrations are the same in all records. membrane from becoming leaky. However, Mn2+ was not used for substitution in the present study since it suppresses action potentials dependent on monovalent cations as will be stated below. The resting membrane potential decreased with a small slope when [Na+]o was increased. It was mv (n = 3) at 150 mm-na+, mv (n = 7) at 300 mm-na+, -68±+ 1-9 mv (n = 5) at 450 mm-na+, mv (n = 5) at 600 mm-na+ and mv (n = 5) at 750 mm-na+ (Fig. 6A, Er). Fig. 5A-C and Fig. 6A (ES)-B show that the overshoot and the maximum rate of rise (m.r.r.) of the spike varied with [Na+]O. The overshoot showed the slope of 39 mv for a 10-fold increase in [Na+]. (dashed line in Fig. 6A) (Yamamoto & Washio, 1979). It shows a saturation phenomenon when [Na+]o was raised more than 450 mm. The m.r.r. was 3-6 V/sec at 150 mm-na+, 16-3 V/sec at 300 mm-na+, 22-1 V/sec at

7 EXCITABILITY OF OVARIAN OOCYTES 637 A 150 mm-na, 0 Ca B 300 mm-na, 0 Ca C 450 mm-na, 0 Ca D 150 mm-na, 5 mm-ca E 300 mm-na, 5 mm-ca F 450 mm-na, 5 mm-ca I 50mV.>h V/sec 0-2 sec Fig. 5. A-C, effect of [Na+]o on the overshoot and the maximum rate of rise of the spikes under Ca2+-free conditions. D-F, competition phenomenon observed between Na+ and Ca2+. The concentration of Ca2+ was held constant at 5 mm while that of Na+ was changed. Dashed line: reference potential level. Voltage, differential and time scales apply to all records. 30 _, ne _ 0 5 _ 0 0 _ 0 CL (U~~~~~~~~~E E _ Na' concentration (mm) Fig. 6. A, effects of [Na+]o on the overshoot potential (E., 0), the critical membrane potential (Er, A) and the resting potential (Er, El) of the spikes under Ca2+-free conditions. The dashed line indicates the slope of 39 mv for a 10-fold increase in concentration. 0 show the spike overshoot when 5 mm-ca2+ was present in the bathing solution. B, effects of [Na+]o on the maximum rate of rise (m.r.r.) of the spikes. The m.r.r. remains constant when 5 mm-ca2+ was added to the solutions (0). The Na+ concentration is indicated in logarithmic scale (mm).

8 638 S. YOSHIDA 450 mm-na+, 23-7 V/sec at 600 mm-na+ and 25-2 V/sec at 750 mm-na+. A saturation is seen when [Na+]. is high (Fig. 6B). These values of m.r.r. are larger than those of Ca spikes (Fig. 3B). The critical membrane potential of the spike (Fig. 6A, Ej) did not substantially change with [Na+]O. Thus it can be said that the spikes are dependent on Na+, i.e. Na spikes. The Na spikes (Fig. 7A) were resistant to 10-5 g/ml. TTX (Fig. 7B) and were completely blocked by Ca antagonists such as 5 mm-co2+, 5 mm-cd2+, 10 mm-mn2+ and 1 mm-la3+ (Fig. 7 C). This kind of blocking suggests that the Na+ goes through 300 mm-na, 0 Ca 300 mm-na, 0 Ca A 300 mm-na, 0 Ca B 10-5 g/ml. TTX -C105 g/ml. TTX, 1 mm-la 1w1 _4cCl1-_ D 300mM-Li,ONa,OCa E 600mM-Rb,ONa,OCa i= ½1I50mV. 2 na II 05 sec Fig. 7. Monovalent cation-dependent spikes recorded under CaW+-free conditions. The Na spikes (A) are resistant to 10-5 g/ml. tetrodotoxin (TTX) and are blocked by 1 mm-la3+ (C) Li+ substituted for Na+ in producing an action potential (D) while Rb+ did not (E). Voltage, current and time scales apply to all records. the Ca channel instead of the separate Na channel during excitation. Li+ substituted for Na+ in generating action potentials (Fig. 7 D). In contrast, Rb+ did not maintain action potentials (Fig. 7E), indicating that the permeability of Rb+ is negligible in the ovarian oocyte membrane of the mouse. Competition between monovalent and divalent cations The other evidence that the Na+ enters through the Ca channel is the presence of competition between Na+ and Ca2+ revealed in the present work. Fig. 5D-F and Fig. 6A-B show the peak level and the m.r.r. of the spike examined in the solutions containing various concentrations of Na+ and a fixed value of 5 mm-ca2+. Both parameters were smaller than those obtained when only Na+ was present in the bathing medium. The values ofthe peak level and the m.r.r. of the spikes were + 1 mv and 3'7 V/sec at 150 mm-na+, 5 mm-ca2+; + 2 mv and 3.9 V/sec at 300 mm-na+,

9 EXCITABILITY OF OVARIAN OOCYTES mm-ca2+; -2 mv and 30 V/sec at 450 mm-na+, 5 mm-ca2 and -3 mv and 2-8 V/sec at 600 mm-na+, 5 mm-ca2+. The values almost remain constant even though [Na+]. was changed in the wide range of concentration. This competition suggests that the Na+ goes through the Ca channel rather the Na channel and both ions compete at the same binding site of the Ca channel. It is supposed that the affinity of Na+ to the site is much smaller than that of Ca2. Competition was also observed between Na+ and Mn2+. Generation of Na spikes was suppressed by Mn2+ which passes through the Ca channel and produces Mn spikes (see below). 0 Na, 0 Ca A 300 mm-na, 0 Ca mm-na, 0 Ca, 10 mm-mn C 10 mm-mn, 155 mm-k 0 Na, 0 Ca D 0 Na, 0 Ca, 80 mm-mn E 80 mm-mn, 10 mm-co A C X S~~~~~~~~50mV T 2nA 0_2 na 0-5 sec Fig. 8. The role ofmn2+ as a Ca blocker and a charge carrier during excitation in the ovarian oocyte membrane of the mouse. The Na spike (A) is blocked by 10 mm-mn2+ (B), but small action potentials (Mn spikes) are revealed when the outward K current is suppressed by elevating the external K+ concentration in Na+-, Ca2+-free solution (C). The Mn spike also appears when Mn2+ concentration was raised up to 80 mm (D). The spike is blocked by Ca antagonist, 10 mm-co2+ (E). Voltage and time scales are the same in all records. Current calibration is 2 na for A and 0-2 na for other records. Mn spikes As is displayed in Fig. 8, Na spikes (A) were completely blocked by 10 mm-mn2+ and the ovarian oocyte showed a passive change of the membrane potential (B). Thus Mn2+ acted as a Ca blocker because it was already verified that the spikes were generated by the Na current through the Ca channels. When appropriate conditions were chosen, action potentials dependent on Mn2+ were revealed. Fig. 8C shows that the ovarian oocyte of the mouse produced small regenerative responses when the outward K current was suppressed by raising the [K+]o from normal 5 mm to 155 mm. The oocyte had a resting potential of -14 mv and the peak level of spike was -4 mv. An alternative technique to reveal Mn spikes

10 640 S. YOSHIDA was to increase the external Mn2+ concentration under Na+-, Ca2+-free conditions (Fig. 8D). In such a solution, the ovarian oocyte showed a resting potential of -10 mv and an overshoot of 2 mv. The spikes disappeared either in the presence of Ca blockers, e.g. 10 mm-co2+ (Fig. 8E) or in the absence of Mn2+ (not illustrated). Thus the action potentials are considered to be dependent on Mn2+ which goes through the Ca channel. This observation corresponds to the report that Mn2+ carried small inward current under voltage-clamp technique in the ovulated mouse oocytes (Okamoto et al. 1977). It is concluded that the Mn2+ has two actions in the ovarian oocyte membrane of the mouse: (1) action of Mn2+ as a Ca blocker, and (2) action of Mn2+ as a charge carrier during excitation (Ochi, 1976). Resting potential of the ovarian oocyte membrane It is shown above that the resting membrane potential varied with [Ca2+]0 with a negative slope (Fig. 3A) and with [Na+]. with a positive slope (Fig. 6A). Further study of the resting membrane was carried out by varying the [K+]. in the presence of 10 mm-mn2+ under Na+-and Ca2+-free conditions (not displayed). The resting potential changed with a very small positive slope when [K+]. was increased mv (n = 3) at 5 mm-k+, mv (n = 3) at 55 mm-k+ and mv at 155 mm-k+ (n = 3). It is suggested that the resting membrane of the ovarian oocyte is permeable to not only Na+ but also to some extent to K+, and Ca2+ reduces the leakage due to stabilizing effect (Okamoto et al. 1977). DISCUSSION In the present study, it was shown for the first time that mammalian oocytes, even before ovulation, are electrically excitable. The Ca channels are present in the ovarian oocyte membrane of the mouse. Such voltage-dependent Ca channels have been identified in all eggs of vertebrate and invertebrate animals examined so far (Hagiwara & Miyazaki, 1977; Hagiwara & Jaffe, 1979; Hagiwara & Byerly, 1981). It is very characteristic that the ovarian oocytes revealed action potentials dependent on either Na+ or Li+ under Ca2+-free conditions. In eggs of the starfish Mediaster, a Na-dependent current was found but the study concluded that Na+ just played a facilitating role and an actual current was carried only by Ca2+ (Hagiwara, Ozawa & Sand, 1975). Eggs of the tunicate Halocynthia are known to have the Na channels in addition to the Ca channels (Okamoto, Takahashi & Yoshii, 1976). Xenopus oocytes have the Na channels which are induced by depolarization. These Na channels do not have an inactivation mechanism (Baud et al. 1982). Okamoto and his colleagues investigated ovulated and unfertilized oocytes of the mouse and concluded that the contribution of Na+ to the inward current was negligible (Okamoto et al. 1977). They compared the I-V relations taken in media containing Na+ and in media without Na+, and they were negative as to the passage of the Na+ through the membrane during excitation because no substantial change could be detected in the I- V curves. However, those workers replaced Ca2+ with Mn2+ in making Ca2+-free, Na+ solutions. This replacement is not appropriate for estimating

11 EXCITABILITY OF OVARIAN OOCYTES the permeation of Na+ through the oocyte membrane because it was found in the present study that Mn2+ suppresses the action potentials dependent on monovalent cations. In fact, further study revealed that the ovulated oocytes of the mouse produced Na or Li spikes under Ca2+-, MnS+-free conditions (S. Yoshida, in preparation). The inward current carried by monovalent cations was insensitive to TTX and was blocked by Ca antagonists such as Co2+, Cd2+, Mn2+ and La3+ in the ovarian oocytes, suggesting that monovalent cations enter through the Ca channels. Such rather unselective Ca channels permeable both to divalent and monovalent cations have been reported in insect muscles (Yamamoto & Washio, 1979), and cardiac preparations (Vitek & Trautwein, 1971; Goldman & Morak, 1977; Reuter & Scholz, 1977). The idea that monovalent cations pass through the Ca channels was further verified by the competition phenomenon observed between monovalent and divalent cations, both between Na+ and Ca2+ (Figs. 5 and 6), and Na+ and Mn2+ (Fig. 8). It is suggested that Ca2+ is more permeable than Na+ through the Ca channels in the mouse ovarian oocytes. Since the competition presumably takes place at the binding site connected with the Ca channel, the affinity of this site for divalent cations is probably larger than for monovalent cations. However, it should be taken into account that the concentration of monovalent cations cannot be raised so much as can be done in the case of divalent cations. Further study is necessary to conclude that monovalent cations surely pass through the Ca channels because the block of Na spikes by Co2+ etc. might be explained by an influence of a Ca-antagonist on a separate Na+-selective channel. Development of ion channels have been studied in many excitable cells including cleavage-arrested embryos of an ascidian (Takahashi & Yoshii, 1981). In general, inward current is carried in large part by Ca2+ at first, a Na+ current appears later, and in some instances the Ca2+ current disappears at late stages of development (Spitzer, 1979). Similar results were obtained in mouse dorsal root ganglion cells, and it was proposed that the number of Ca channels per unit area of the membrane decreases with time while that of Na channels increases (Matsuda, Yoshida & Yonezawa, 1978; Yoshida, Matsuda & Samejima, 1978). Present work shows that an unselective or immature Ca channel is present in the early stage of development, i.e. ovarian oocytes. This kind of Ca channel may be a prototype of Na channel which is observed in the later stages of development. I thank Drs W. J. Moody, Jr and Y. Matsuda for their comments on the manuscript and Mr M. Yogata and Mrs N. Momosaki for making figures. This work was supported by a research grant from the Japan Ministry of Education. REFERENCES BAUD, C., KADO, R. T. & MARCHER, K. (1982). Sodium channels induced by depolarization of the XenopuB laevis oocyte. Proc. natn. Acad. Sci. U.S.A. 79, GOLDMAN, Y. & MORAD, M. (1977). Ionic membrane conductance during the time course of the cardiac action potential. J. Physiol. 268, HAGIWARA, S. (1973). Ca spike. Adv. Biophya. 4, HAGIWARA, S. & BYERLY, L. (1981). Calcium channel. Ann. Rev. Neurowci. 4, HAGIWARA, S. & JAFFE, L. A. (1979). Electrical properties of egg cell membranes. Ann. Rev. Biophys. Bioeng. 8, PHY

12 642 S. YOSHIDA HAGIWARA, S. & MIYAZAKI, S. (1977). Ca and Na spikes in egg cell membrane. Prog. clin. biol. Re8. 15, HAGIWARA, S., OZAWA, S. & SAND, 0. (1975). Voltage clamp analysis of two inward current mechanisms in the egg cell membrane of a starfish. J. gen. Phy8iol. 65, IWAMATSU, T. & CHANG, M. C. (1972). Sperm penetration in vitro of mouse oocytes at various times during maturation. J. Reprod. Fert. 3, MATSUDA, Y., YOSHIDA, S. & YONEZAWA, T. (1978). Tetrodotoxin sensitivity and Ca component of action potentials of mouse dorsal root ganglion cells cultured in vitro. Brain Re8. 154, MIYAZAKI, S., TAKAHASHI, K. & TSUDA, K. (1974). Electrical excitability in the egg cell membrane of the tunicate. J. Physiol. 238, OCHI, R. (1976). Manganese-dependent propagated action potentials and their depression by electrical stimulation in guinea-pig myocardium perfused by sodium-free media. J. Physiol. 263, OKAMOTO, H., TAKAHASHI, K. & YAMASHITA, N. (1977). Ionic currents through the membrane of the mammalian oocyte and their comparison with those in the tunicate and sea urchin. J. Physiol. 267, OKAMOTO, H., TAKAHASHI, K. & YOSHII, M. (1976). Two components of the calcium current in the egg cell membrane of the tunicate. J. Physiol. 255, POWERS, R. D. (1982). Changes in mouse oocyte membrane potential and permeability during meiotic maturation. J. exp. Zool. 221, POWERS, R. D. & TUPPER, J. T. (1974). Some electrophysiological and permeability properties of the mouse egg. Dev1 Biol. 38, REUTER, H. & SCHOLZ, H. (1977). A study of the ion selectivity and the kinetic properties of the calcium-dependent slow inward current in mammalian cardiac muscle. J. Physiol. 264, SPITZER, N. C. (1979). Ion channels in development. Ann. Rev. Neuro8ci. 2, TAKAHASHI, K., MIYAZAKI, S. & KIDOKORO, Y. (1971). Development of excitability in embryonic muscle cell membranes in certain tunicates. Science, N. Y. 171, TAKAHASHI, K. & YOSHII, M. (1981). Development of sodium, calcium and potassium channels in the cleavage-arrested embryo of an ascidian. J. Physiol. 315, VITEK, M. & TRAUTWEIN, W. (1971). Slow inward current and action potential in cardiac Purkinje fibres. The effect of Mn2+-ions. Pfluger8 Arch. 323, YAMAMOTO, D. & WASHIO, H. (1979). Permeation of sodium through calcium channels of an insect muscle membrane. Can. J. Physiol. Pharmac. 57, YAMASHITA, N. (1982). Enhancement of ionic currents through voltage-gated channels in the mouse oocyte after fertilization. J. Physiol. 329, YOSHIDA, S. (1982). Na and Ca spikes produced by ions passing through Ca channels in mouse ovarian oocytes. Pflilger8 Arch. 395, YOSHIDA, S., MATSUDA, Y. & SAMEJIMA, A. (1978). Tetrodotoxin-resistant sodium and calcium components of action potentials in dorsal root ganglion cells of the adult mouse. J. Neurophysiol. 41,

EFFECTS OF VARIOUS IONS ON THE RESTING AND ACTIVE MEMBRANE OF THE SOMATIC MUSCLE OF THE EARTHWORM

EFFECTS OF VARIOUS IONS ON THE RESTING AND ACTIVE MEMBRANE OF THE SOMATIC MUSCLE OF THE EARTHWORM J. Exp. BioL (1969), 50, 405-41 s 405 With 8 text-figures Printed in Great Britain EFFECTS OF VARIOUS IONS ON THE RESTING AND ACTIVE MEMBRANE OF THE SOMATIC MUSCLE OF THE EARTHWORM BY T. HIDAKA, Y. ITO,

More information

U.C.L.A., Los Angeles, California 90024, U.S.A. (Received 28 September 1978)

U.C.L.A., Los Angeles, California 90024, U.S.A. (Received 28 September 1978) J. Phyeiol. (1979), 292, pp. 25 1-265 251 With 7 text-ftgurem Printed in Great Britain EFFECTS OF II[ERNAL POTASSIUM AND SODIUM ON THE ANOMALOUS RECTIFICATION OF THE STARFISH EGG AS EXAMINED BY INTERNAL

More information

Three Components of Calcium Currents in Crayfish Skeletal Muscle Fibres

Three Components of Calcium Currents in Crayfish Skeletal Muscle Fibres Gen. Physiol. Biophys. (1991), 10, 599 605 599 Short communication Three Components of Calcium Currents in Crayfish Skeletal Muscle Fibres M. HENČEK and D. ZACHAROVÁ Institute of Molecular Physiology and

More information

6.3.4 Action potential

6.3.4 Action potential I ion C m C m dφ dt Figure 6.8: Electrical circuit model of the cell membrane. Normally, cells are net negative inside the cell which results in a non-zero resting membrane potential. The membrane potential

More information

CALCIUM ACTION POTENTIALS IN THE SKELETAL MUSCLE FIBRES OF THE STICK INSECT CARAUSIUS MOROSUS

CALCIUM ACTION POTENTIALS IN THE SKELETAL MUSCLE FIBRES OF THE STICK INSECT CARAUSIUS MOROSUS 7. exp. BM. (1981), 93, 357-267 257 With 8 figures Printed m Great Britain CALCIUM ACTION POTENTIALS IN THE SKELETAL MUSCLE FIBRES OF THE STICK INSECT CARAUSIUS MOROSUS BY FRANCES M. ASHCROFT* Department

More information

BRIEF COMMUNICATION OF ASYMMETRY CURRENT SQUID AXON MEMBRANE FREQUENCY DOMAIN ANALYSIS

BRIEF COMMUNICATION OF ASYMMETRY CURRENT SQUID AXON MEMBRANE FREQUENCY DOMAIN ANALYSIS FREQUENCY DOMAIN ANALYSIS OF ASYMMETRY CURRENT IN SQUID AXON MEMBRANE SHIRo TAKASHIMA, Department ofbioengineering D2, University of Pennsylvania, Philadelphia, Pennsylvania 19104 U.S.A. ABSTRACT The change

More information

Voltage-clamp and Hodgkin-Huxley models

Voltage-clamp and Hodgkin-Huxley models Voltage-clamp and Hodgkin-Huxley models Read: Hille, Chapters 2-5 (best Koch, Chapters 6, 8, 9 See also Hodgkin and Huxley, J. Physiol. 117:500-544 (1952. (the source Clay, J. Neurophysiol. 80:903-913

More information

Potential, Structure, and Excitability of Giant Axon Membrane

Potential, Structure, and Excitability of Giant Axon Membrane Potential, Structure, and Excitability of Giant Axon Membrane T. NARAHASHI From the Laboratory of Applied Entomology, Faculty of Agriculture, University of Tokyo, Tokyo, Japan Intracellular perfusion of

More information

Membrane Potentials, Action Potentials, and Synaptic Transmission. Membrane Potential

Membrane Potentials, Action Potentials, and Synaptic Transmission. Membrane Potential Cl Cl - - + K + K+ K + K Cl - 2/2/15 Membrane Potentials, Action Potentials, and Synaptic Transmission Core Curriculum II Spring 2015 Membrane Potential Example 1: K +, Cl - equally permeant no charge

More information

Channels can be activated by ligand-binding (chemical), voltage change, or mechanical changes such as stretch.

Channels can be activated by ligand-binding (chemical), voltage change, or mechanical changes such as stretch. 1. Describe the basic structure of an ion channel. Name 3 ways a channel can be "activated," and describe what occurs upon activation. What are some ways a channel can decide what is allowed to pass through?

More information

Voltage-clamp and Hodgkin-Huxley models

Voltage-clamp and Hodgkin-Huxley models Voltage-clamp and Hodgkin-Huxley models Read: Hille, Chapters 2-5 (best) Koch, Chapters 6, 8, 9 See also Clay, J. Neurophysiol. 80:903-913 (1998) (for a recent version of the HH squid axon model) Rothman

More information

Mn 2+ IONS PASS THROUGH Ca 2+ CHANNELS IN MYOEPITHELIAL CELLS

Mn 2+ IONS PASS THROUGH Ca 2+ CHANNELS IN MYOEPITHELIAL CELLS J. exp. Biol. (1979), 8a, 287-238 227 With 6 figures Wrinted in Great Britain Mn 2+ IONS PASS THROUGH Ca 2+ CHANNELS IN MYOEPITHELIAL CELLS BY M. ANDERSON Department of Biological Sciences, Smith College,

More information

Inactivation of Calcium Current in the Somatic Membrane of Snail Neurons

Inactivation of Calcium Current in the Somatic Membrane of Snail Neurons \ Gen. Physiol. Biophys. (1984), 3, 1 17 1 Inactivation of Calcium Current in the Somatic Membrane of Snail Neurons P. A. DOROSHENKO, P. G. KOSTYUK and A. E. MARTYNYUK A. A. Bogomoletz Institute of Physiology,

More information

SENSORY MECHANISMS IN PARAMECIUM

SENSORY MECHANISMS IN PARAMECIUM J. Exp. Biol. (1972), 56, 683-694 683 With 8 text-figures in Great Britain SENSORY MECHANISMS IN PARAMECIUM I. TWO COMPONENTS OF THE ELECTRIC RESPONSE TO MECHANICAL STIMULATION OF THE ANTERIOR SURFACE

More information

Membrane Currents in Mammalian Ventricular Heart Muscle Fibers Using a Voltage-Clamp Technique

Membrane Currents in Mammalian Ventricular Heart Muscle Fibers Using a Voltage-Clamp Technique Membrane Currents in Mammalian Ventricular Heart Muscle Fibers Using a Voltage-Clamp Technique GERHARD GIEBISCH and SILVIO WEIDMANN From the Department of Physiology, University of Berne, Berne, Switzerland.

More information

Structure and Measurement of the brain lecture notes

Structure and Measurement of the brain lecture notes Structure and Measurement of the brain lecture notes Marty Sereno 2009/2010!"#$%&'(&#)*%$#&+,'-&.)"/*"&.*)*-'(0&1223 Neurons and Models Lecture 1 Topics Membrane (Nernst) Potential Action potential/voltage-gated

More information

EK), closer to EC,. Farmington, CT 06032, U.S.A. [K]i = 121 mm and [Cl]i = 44 mm. The natural external medium is pond water

EK), closer to EC,. Farmington, CT 06032, U.S.A. [K]i = 121 mm and [Cl]i = 44 mm. The natural external medium is pond water J. Phy8iol. (1985), 358, pp. 299-319 299 With 7 text-figures Printed in Great Britain FERTILIZATION-INDUCED IONIC CONDUCTANCES IN EGGS OF THE FROG, RANA PIPIENS BY LAURINDA A. JAFFE AND LYANNE C. SCHLICHTER*

More information

POTASSIUM PERMEABILITY IN

POTASSIUM PERMEABILITY IN SLOW CHANGES OF POTASSIUM PERMEABILITY IN THE SQUID GIANT AXON GERALD EHRENSTEIN and DANIEL L. GILBERT From the National Institutes of Health, Bethesda, Maryland, and the Marine Biological Laboratory,

More information

Biomedical Instrumentation

Biomedical Instrumentation ELEC ENG 4BD4: Biomedical Instrumentation Lecture 5 Bioelectricity 1. INTRODUCTION TO BIOELECTRICITY AND EXCITABLE CELLS Historical perspective: Bioelectricity first discovered by Luigi Galvani in 1780s

More information

Resting Membrane Potential

Resting Membrane Potential Resting Membrane Potential Fig. 12.09a,b Recording of Resting and It is recorded by cathode ray oscilloscope action potentials -70 0 mv + it is negative in polarized (resting, the membrane can be excited)

More information

MINIATURE EXCITATORY JUNCTION POTENTIALS IN THE SOMATIC MUSCLE OF THE EARTHWORM, PHERETIMA COMMUNISSIMA, IN SODIUM FREE SOLUTION

MINIATURE EXCITATORY JUNCTION POTENTIALS IN THE SOMATIC MUSCLE OF THE EARTHWORM, PHERETIMA COMMUNISSIMA, IN SODIUM FREE SOLUTION J. Exp. Biol. (1969), 50, 107118 With 11 textfigures Printed in Great Britain MINIATURE EXCITATORY JUNCTION POTENTIALS IN THE SOMATIC MUSCLE OF THE EARTHWORM, PHERETIMA COMMUNISSIMA, IN SODIUM FREE SOLUTION

More information

DIVALENT CATIONS AS CHARGE CARRIERS DURING TWO FUNCTIONALLY DIFFERENT MEMBRANE CURRENTS IN THE CILIATE STYLONYCHIA

DIVALENT CATIONS AS CHARGE CARRIERS DURING TWO FUNCTIONALLY DIFFERENT MEMBRANE CURRENTS IN THE CILIATE STYLONYCHIA J. exp. Biol. (1980), 88, 73-89 73 With 11 figures Printed in Great Britain DIVALENT CATIONS AS CHARGE CARRIERS DURING TWO FUNCTIONALLY DIFFERENT MEMBRANE CURRENTS IN THE CILIATE STYLONYCHIA BY JACQUES

More information

ACTION POTENTIAL. Dr. Ayisha Qureshi Professor MBBS, MPhil

ACTION POTENTIAL. Dr. Ayisha Qureshi Professor MBBS, MPhil ACTION POTENTIAL Dr. Ayisha Qureshi Professor MBBS, MPhil DEFINITIONS: Stimulus: A stimulus is an external force or event which when applied to an excitable tissue produces a characteristic response. Subthreshold

More information

Neurophysiology. Danil Hammoudi.MD

Neurophysiology. Danil Hammoudi.MD Neurophysiology Danil Hammoudi.MD ACTION POTENTIAL An action potential is a wave of electrical discharge that travels along the membrane of a cell. Action potentials are an essential feature of animal

More information

Ca-INDUCED K + -OUTWARD CURRENT IN PARAMECIUM TETRAURELIA

Ca-INDUCED K + -OUTWARD CURRENT IN PARAMECIUM TETRAURELIA J. exp. Biol. (1980), 88, 293-303 293 With 6 figures Printed in Great Britain Ca-INDUCED K + -OUTWARD CURRENT IN PARAMECIUM TETRAURELIA BY YOUKO SATOW AND CHING KUNG Laboratory of Molecular Biology and

More information

Rahaf Nasser mohammad khatatbeh

Rahaf Nasser mohammad khatatbeh 7 7... Hiba Abu Hayyeh... Rahaf Nasser mohammad khatatbeh Mohammad khatatbeh Brief introduction about membrane potential The term membrane potential refers to a separation of opposite charges across the

More information

Quantitative Electrophysiology

Quantitative Electrophysiology ECE 795: Quantitative Electrophysiology Notes for Lecture #1 Wednesday, September 13, 2006 1. INTRODUCTION TO EXCITABLE CELLS Historical perspective: Bioelectricity first discovered by Luigi Galvani in

More information

BRIEF COMMUNICATION 3,4-DIAMINOPYRIDINE A POTENT NEW POTASSIUM CHANNEL BLOCKER

BRIEF COMMUNICATION 3,4-DIAMINOPYRIDINE A POTENT NEW POTASSIUM CHANNEL BLOCKER BRIEF COMMUNICATION 3,4-DIAMINOPYRIDINE A POTENT NEW POTASSIUM CHANNEL BLOCKER GLENN E. KIRSCH AND ToSHIo NARAHASHI, Department ofpharmacology, Northwestem University Medical School, Chicago, Illinois

More information

Modeling of Action Potential Generation in NG cells

Modeling of Action Potential Generation in NG cells Modeling of Action Potential Generation in NG108-15 cells NanoScience Technology Center University of Central Florida 144 Research Parkway, Suite 400 Orlando, FL 386 * Corresponding author Email: pmolnar@mail.ucf.edu

More information

Clasificador 198, Correo Central, Santiago, Chile

Clasificador 198, Correo Central, Santiago, Chile J. Physiol. (197), 211, pp. 753-765 753 With 6 text-figurem Printed in Great Britain TIME COURSE OF THE SODIUM PERMEABILITY CHANGE DURING A SINGLE MEMBRANE ACTION POTENTIAL BY ILLANI ATWATER, FRANCISCO

More information

Quantitative Electrophysiology

Quantitative Electrophysiology ECE 795: Quantitative Electrophysiology Notes for Lecture #1 Tuesday, September 18, 2012 1. INTRODUCTION TO EXCITABLE CELLS Historical perspective: Bioelectricity first discovered by Luigi Galvani in 1780s

More information

Lecture 2. Excitability and ionic transport

Lecture 2. Excitability and ionic transport Lecture 2 Excitability and ionic transport Selective membrane permeability: The lipid barrier of the cell membrane and cell membrane transport proteins Chemical compositions of extracellular and intracellular

More information

Introduction to electrophysiology. Dr. Tóth András

Introduction to electrophysiology. Dr. Tóth András Introduction to electrophysiology Dr. Tóth András Topics Transmembran transport Donnan equilibrium Resting potential Ion channels Local and action potentials Intra- and extracellular propagation of the

More information

ELECTROPHYSIOLOGY OF THE HEART OF AN ISOPOD CRUSTACEAN: PORCELLIO DILATATUS

ELECTROPHYSIOLOGY OF THE HEART OF AN ISOPOD CRUSTACEAN: PORCELLIO DILATATUS J. Exp.Biol. (1972). 57. 609-631 609 " s text-figures TPrmted in Great Britain ELECTROPHYSIOLOGY OF THE HEART OF AN ISOPOD CRUSTACEAN: PORCELLIO DILATATUS II. EFFECTS OF IONS AND MEMBRANE PERMEABILITY

More information

V m = the Value of the Na Battery Plus the Voltage Drop Across g Na. I Na is Isolated By Blocking I K. and g K

V m = the Value of the Na Battery Plus the Voltage Drop Across g Na. I Na is Isolated By Blocking I K. and g K VoltageGated Ion Channels and the Action Potential VoltageGated Ion Channels and the Action Potential jdk3 Principles of Neural Science, chaps 8&9 The Action Potential Generation Conduction VoltageGated

More information

Editorial. What is the true resting potential of small cells? Jean-Marc Dubois

Editorial. What is the true resting potential of small cells? Jean-Marc Dubois Gen. Physiol. Biophys. (2000), 19, 3 7 3 Editorial What is the true resting potential of small cells? Jean-Marc Dubois In order to understand almost anything, it is necessary to first obtain a measurement

More information

THE NEGATIVE INOTROPIC EFFECT OF RAISED EXTRACELLULAR POTASSIUM AND CAESIUM IONS ON ISOLATED FROG ATRIAL TRABECULAE

THE NEGATIVE INOTROPIC EFFECT OF RAISED EXTRACELLULAR POTASSIUM AND CAESIUM IONS ON ISOLATED FROG ATRIAL TRABECULAE Quarterly Journal of Experimental Physiology (1987), 72, 561-570 Printed in Great Britain THE NEGATIVE INOTROPIC EFFECT OF RAISED EXTRACELLULAR POTASSIUM AND CAESIUM IONS ON ISOLATED FROG ATRIAL TRABECULAE

More information

Membrane Physiology. Dr. Hiwa Shafiq Oct-18 1

Membrane Physiology. Dr. Hiwa Shafiq Oct-18 1 Membrane Physiology Dr. Hiwa Shafiq 22-10-2018 29-Oct-18 1 Chemical compositions of extracellular and intracellular fluids. 29-Oct-18 2 Transport through the cell membrane occurs by one of two basic processes:

More information

COGNITIVE SCIENCE 107A

COGNITIVE SCIENCE 107A COGNITIVE SCIENCE 107A Electrophysiology: Electrotonic Properties 2 Jaime A. Pineda, Ph.D. The Model Neuron Lab Your PC/CSB115 http://cogsci.ucsd.edu/~pineda/cogs107a/index.html Labs - Electrophysiology

More information

A 'TEA + -INSENSITIVE' MUTANT WITH INCREASED POTASSIUM CONDUCTANCE IN PARAMECIUM AURELIA

A 'TEA + -INSENSITIVE' MUTANT WITH INCREASED POTASSIUM CONDUCTANCE IN PARAMECIUM AURELIA J. txp. Biol. (1976), 65, 51-63 With 9 figures Printed in Great Britain A 'TEA + -INSENSITIVE' MUTANT WITH INCREASED POTASSIUM CONDUCTANCE IN PARAMECIUM AURELIA BY YOUKO SATOW AND CHING RUNG Laboratory

More information

Ion Channel Structure and Function (part 1)

Ion Channel Structure and Function (part 1) Ion Channel Structure and Function (part 1) The most important properties of an ion channel Intrinsic properties of the channel (Selectivity and Mode of Gating) + Location Physiological Function Types

More information

Lecture Notes 8C120 Inleiding Meten en Modelleren. Cellular electrophysiology: modeling and simulation. Nico Kuijpers

Lecture Notes 8C120 Inleiding Meten en Modelleren. Cellular electrophysiology: modeling and simulation. Nico Kuijpers Lecture Notes 8C2 Inleiding Meten en Modelleren Cellular electrophysiology: modeling and simulation Nico Kuijpers nico.kuijpers@bf.unimaas.nl February 9, 2 2 8C2 Inleiding Meten en Modelleren Extracellular

More information

Resting membrane potential,

Resting membrane potential, Resting membrane potential Inside of each cell is negative as compared with outer surface: negative resting membrane potential (between -30 and -90 mv) Examination with microelectrode (Filled with KCl

More information

Action Potential Propagation

Action Potential Propagation Action Potential Propagation 2 Action Potential is a transient alteration of transmembrane voltage (or membrane potential) across an excitable membrane generated by the activity of voltage-gated ion channels.

More information

Peripheral Nerve II. Amelyn Ramos Rafael, MD. Anatomical considerations

Peripheral Nerve II. Amelyn Ramos Rafael, MD. Anatomical considerations Peripheral Nerve II Amelyn Ramos Rafael, MD Anatomical considerations 1 Physiologic properties of the nerve Irritability of the nerve A stimulus applied on the nerve causes the production of a nerve impulse,

More information

Modeling action potential generation and propagation in NRK fibroblasts

Modeling action potential generation and propagation in NRK fibroblasts Am J Physiol Cell Physiol 287: C851 C865, 2004. First published May 12, 2004; 10.1152/ajpcell.00220.2003. Modeling action potential generation and propagation in NRK fibroblasts J. J. Torres, 1,2 L. N.

More information

General Physics. Nerve Conduction. Newton s laws of Motion Work, Energy and Power. Fluids. Direct Current (DC)

General Physics. Nerve Conduction. Newton s laws of Motion Work, Energy and Power. Fluids. Direct Current (DC) Newton s laws of Motion Work, Energy and Power Fluids Direct Current (DC) Nerve Conduction Wave properties of light Ionizing Radiation General Physics Prepared by: Sujood Alazzam 2017/2018 CHAPTER OUTLINE

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Supplementary Figure S1. Pulses >3mJ reduce membrane resistance in HEK cells. Reversal potentials in a representative cell for IR-induced currents with laser pulses of 0.74 to

More information

Some Predictions Concerning the Calcium Channel Model with Different Conformational States

Some Predictions Concerning the Calcium Channel Model with Different Conformational States Gen. Physiol. Biophys. (1986), 6, 649 659 649 Short communication Some Predictions Concerning the Calcium Channel Model with Different Conformational States P. G. KOSTYUK and S. L. MIRONOV A. A. Bogomoletz

More information

Chapter 1 subtitles Ion gradients

Chapter 1 subtitles Ion gradients CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND Chapter 1 subtitles Ion gradients Introduction In this first chapter, I'll explain the basic knowledge required to understand the electrical signals generated

More information

Neuroscience 201A Exam Key, October 7, 2014

Neuroscience 201A Exam Key, October 7, 2014 Neuroscience 201A Exam Key, October 7, 2014 Question #1 7.5 pts Consider a spherical neuron with a diameter of 20 µm and a resting potential of -70 mv. If the net negativity on the inside of the cell (all

More information

Nakajima, 1966; Okamoto, Takahashi & Yoshi, 1976; Kostyuk & Krishtal, 1977a;

Nakajima, 1966; Okamoto, Takahashi & Yoshi, 1976; Kostyuk & Krishtal, 1977a; J. Physiol. (1984), 356, pp. 491-55 491 With 7 text-figures Printed in Great Britain TWO CLCIUM CURRENTS IN NENTHES REN CEODENT TUS EGG CELL MEMBRNES BY. P. FOX ND S. KRSNE From the Department of Physiology,

More information

Action potentials. Conductances channels

Action potentials. Conductances channels Action potentials Conductances channels Cole and Curtis AC Wheatstone bridge resistance decreased during action potential R1 & R2 divide one path, Rv (variable) and Ru divide the other Galvanometer between

More information

DYNAMICS OF POTASSIUM ION CURRENTS IN

DYNAMICS OF POTASSIUM ION CURRENTS IN DYNAMICS OF POTASSIUM ION CURRENTS IN SQUID AXON MEMBRANE A RE-EXAMINATION J. W. MOORE AND STEVEN H. YOUNG, Department ofphysiology, Duke University Medical Center, Durham, North Carolina 27710, and Marine

More information

(Received 25 August 1969)

(Received 25 August 1969) J. Physiol. (1970), 207, pp. 211-229 211 With 10 text-fgures Printed in Great Britain THE RELATION BETWEEN MEMBRANE POTENTIAL, MEMBRANE CURRENTS AND ACTIVATION OF CONTRACTION IN VENTRICULAR MYOCARDIAL

More information

Electrophysiology of the neuron

Electrophysiology of the neuron School of Mathematical Sciences G4TNS Theoretical Neuroscience Electrophysiology of the neuron Electrophysiology is the study of ionic currents and electrical activity in cells and tissues. The work of

More information

LESSON 2.2 WORKBOOK How do our axons transmit electrical signals?

LESSON 2.2 WORKBOOK How do our axons transmit electrical signals? LESSON 2.2 WORKBOOK How do our axons transmit electrical signals? This lesson introduces you to the action potential, which is the process by which axons signal electrically. In this lesson you will learn

More information

assumptions is that different ions move independently across the cell 7-2

assumptions is that different ions move independently across the cell 7-2 J. Phyeiol. (1977), 265, pp. 193-26 193 With 6 text-ftgure8 Printed in Great Britain REDUCTION OF POTASSIUM PERMEABILITY BY CHLORIDE SUBSTITUTION IN CARDIAC CELLS BY E. CARMELIET AND F. VERDONCK From the

More information

they give no information about the rate at which repolarization restores the

they give no information about the rate at which repolarization restores the 497 J. Physiol. (1952) ii6, 497-506 THE DUAL EFFECT OF MEMBRANE POTENTIAL ON SODIUM CONDUCTANCE IN THE GIANT AXON OF LOLIGO BY A. L. HODGKIN AND A. F. HUXLEY From the Laboratory of the Marine Biological

More information

9.01 Introduction to Neuroscience Fall 2007

9.01 Introduction to Neuroscience Fall 2007 MIT OpenCourseWare http://ocw.mit.edu 9.01 Introduction to Neuroscience Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 9.01 Recitation (R02)

More information

All-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model

All-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model All-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model S. A. Sadegh Zadeh, C. Kambhampati International Science Index, Mathematical and Computational Sciences waset.org/publication/10008281

More information

Sugashima Marine Biological Laboratory, School of Science, Nagoya University, Sugashima, Toba, Mie 517, Japan

Sugashima Marine Biological Laboratory, School of Science, Nagoya University, Sugashima, Toba, Mie 517, Japan CELL STRUCTURE AND FUNCTION 14, 697-706 (1989) c by Japan Society for Cell Biology Membrane Potential Change in a Sea Urchin Egg Induced by Calcium Ionophore A23187 Has The Same Component that is Involved

More information

CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND

CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND Chapter 1 Zoom in on Patch configurations In the jargon of electrophysiologists, a patch is a piece of neuronal membrane. Researchers invented a technique known

More information

Overview Organization: Central Nervous System (CNS) Peripheral Nervous System (PNS) innervate Divisions: a. Afferent

Overview Organization: Central Nervous System (CNS) Peripheral Nervous System (PNS) innervate Divisions: a. Afferent Overview Organization: Central Nervous System (CNS) Brain and spinal cord receives and processes information. Peripheral Nervous System (PNS) Nerve cells that link CNS with organs throughout the body.

More information

Ch. 5. Membrane Potentials and Action Potentials

Ch. 5. Membrane Potentials and Action Potentials Ch. 5. Membrane Potentials and Action Potentials Basic Physics of Membrane Potentials Nerve and muscle cells: Excitable Capable of generating rapidly changing electrochemical impulses at their membranes

More information

Parameters for Minimal Model of Cardiac Cell from Two Different Methods: Voltage-Clamp and MSE Method

Parameters for Minimal Model of Cardiac Cell from Two Different Methods: Voltage-Clamp and MSE Method Parameters for Minimal Model of Cardiac Cell from Two Different Methods: oltage-clamp and MSE Method Soheila Esmaeili 1, * and Bahareh beheshti 1 Department of Biomedical engineering, ran University of

More information

MEMBRANE POTENTIALS AND ACTION POTENTIALS:

MEMBRANE POTENTIALS AND ACTION POTENTIALS: University of Jordan Faculty of Medicine Department of Physiology & Biochemistry Medical students, 2017/2018 +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ Review: Membrane physiology

More information

Neural Modeling and Computational Neuroscience. Claudio Gallicchio

Neural Modeling and Computational Neuroscience. Claudio Gallicchio Neural Modeling and Computational Neuroscience Claudio Gallicchio 1 Neuroscience modeling 2 Introduction to basic aspects of brain computation Introduction to neurophysiology Neural modeling: Elements

More information

Equivalent Circuit of the Membrane Connected to the Voltage Clamp. I mon. For Large Depolarizations, Both I Na and I K Are Activated

Equivalent Circuit of the Membrane Connected to the Voltage Clamp. I mon. For Large Depolarizations, Both I Na and I K Are Activated VoltageGated Ion Channels and the Action Potential jdk3 Principles of Neural Science, chaps 8&9 VoltageGated Ion Channels and the Action Potential The Action Potential Generation Conduction VoltageGated

More information

Transport of ions across plasma membranes

Transport of ions across plasma membranes Transport of ions across plasma membranes Plasma Membranes of Excitable tissues Ref: Guyton, 13 th ed: pp: 61-71. 12 th ed: pp: 57-69. 11th ed: p57-71, Electrical properties of plasma membranes Part A:

More information

Surface Density of Calcium Ions and Calcium Spikes in the Barnacle Muscle Fiber Membrane

Surface Density of Calcium Ions and Calcium Spikes in the Barnacle Muscle Fiber Membrane Published Online: 1 January, 1967 Supp Info: http://doi.org/10.1085/jgp.50.3.583 Downloaded from jgp.rupress.org on September 25, 2018 Surface Density of Calcium Ions and Calcium Spikes in the Barnacle

More information

Decoding. How well can we learn what the stimulus is by looking at the neural responses?

Decoding. How well can we learn what the stimulus is by looking at the neural responses? Decoding How well can we learn what the stimulus is by looking at the neural responses? Two approaches: devise explicit algorithms for extracting a stimulus estimate directly quantify the relationship

More information

Basic elements of neuroelectronics -- membranes -- ion channels -- wiring. Elementary neuron models -- conductance based -- modelers alternatives

Basic elements of neuroelectronics -- membranes -- ion channels -- wiring. Elementary neuron models -- conductance based -- modelers alternatives Computing in carbon Basic elements of neuroelectronics -- membranes -- ion channels -- wiring Elementary neuron models -- conductance based -- modelers alternatives Wiring neurons together -- synapses

More information

STUDIES OF CHANGING MEMBRANE POTENTIAL * : 1. BASIC ELECTRICAL THEORY, 2. GRADED AND ACTION POTENTIALS 3. THE VOLTAGE CLAMP AND MEMBRANE POTENTIALS

STUDIES OF CHANGING MEMBRANE POTENTIAL * : 1. BASIC ELECTRICAL THEORY, 2. GRADED AND ACTION POTENTIALS 3. THE VOLTAGE CLAMP AND MEMBRANE POTENTIALS STUDIES OF CHANGING MEMBRANE POTENTIAL * : 1. BASIC ELECTRICAL THEORY, 2. GRADED AND ACTION POTENTIALS 3. THE VOLTAGE CLAMP AND MEMBRANE POTENTIALS I. INTRODUCTION A. So far we have only considered the

More information

J. Physiol. ('959) I48,

J. Physiol. ('959) I48, 665 J. Physiol. ('959) I48, 665-670 ON INCREASING THE VELOCITY OF A NERVE IMPULSE BY J. DEL CASTILLO* AND J. W. MOORE From the National Institute of Neurological Diseases and Blindness, National Institutes

More information

Introduction to electrophysiology 1. Dr. Tóth András

Introduction to electrophysiology 1. Dr. Tóth András Introduction to electrophysiology 1. Dr. Tóth András Topics Transmembran transport Donnan equilibrium Resting potential Ion channels Local and action potentials Intra- and extracellular propagation of

More information

Potassium Uptake Mechanisms of Cultured Oligodendrocytes Studied with lon-sensitive Electrodes

Potassium Uptake Mechanisms of Cultured Oligodendrocytes Studied with lon-sensitive Electrodes Potassium Uptake Mechanisms of Cultured Oligodendrocytes Studied with lon-sensitive Electrodes H. Kettenmann, R. K. Orkand, and M. Schachner Introduction Physiological studies over the past two decades

More information

5.4 Modelling ensembles of voltage-gated ion channels

5.4 Modelling ensembles of voltage-gated ion channels 5.4 MODELLING ENSEMBLES 05 to as I g (Hille, 200). Gating currents tend to be much smaller than the ionic currents flowing through the membrane. In order to measure gating current, the ionic current is

More information

University of Tokyo, Tokyo, Japan

University of Tokyo, Tokyo, Japan J. Phy~iol. (1976), 255, pp. 527-561 527 With 14 text -ftgurea8 Printed in Great Britain TWO COMPONENTS OF THE CALCIUM CURRENT IN THE EGG CELL MEMBRANE OF THE TUNICATE By HARUMASA OKAMOTO,* KUNITARO TAKAHASHI

More information

Simulation of Cardiac Action Potentials Background Information

Simulation of Cardiac Action Potentials Background Information Simulation of Cardiac Action Potentials Background Information Rob MacLeod and Quan Ni February 7, 2 Introduction The goal of assignments related to this document is to experiment with a numerical simulation

More information

Neural Conduction. biologyaspoetry.com

Neural Conduction. biologyaspoetry.com Neural Conduction biologyaspoetry.com Resting Membrane Potential -70mV A cell s membrane potential is the difference in the electrical potential ( charge) between the inside and outside of the cell. The

More information

BME 5742 Biosystems Modeling and Control

BME 5742 Biosystems Modeling and Control BME 5742 Biosystems Modeling and Control Hodgkin-Huxley Model for Nerve Cell Action Potential Part 1 Dr. Zvi Roth (FAU) 1 References Hoppensteadt-Peskin Ch. 3 for all the mathematics. Cooper s The Cell

More information

(Received 18 September 1964)

(Received 18 September 1964) J. Physiol. (1965), 177, pp. 453-462 453 With 6 text-ftgurem Printed in Great Britain POTASSIUM AND RUBIDIUM EXCHANGE ACROSS THE SURFACE MEMBRANE OF CARDIAC PURKINJE FIBRES BY P. MULLER From the Department

More information

Relevance to Block by Dihydropyridines

Relevance to Block by Dihydropyridines Published Online: 1 April, 1987 Supp Info: http://doi.org/10.1085/jgp.89.4.629 Downloaded from jgp.rupress.org on January 6, 2019 Negative Surface Charge Density Near Heart Calcium Channels Relevance to

More information

BRIEF COMMUNICATION SQUID AXONS IN REDUCED EXTERNAL CA++ FAIL THE STANDARD HODGKIN-HUXLEY MODEL AND TO ACCOMMODATE TO SLOWLY RISING CURRENTS

BRIEF COMMUNICATION SQUID AXONS IN REDUCED EXTERNAL CA++ FAIL THE STANDARD HODGKIN-HUXLEY MODEL AND TO ACCOMMODATE TO SLOWLY RISING CURRENTS BRIEF COMMUNICATION THE STANDARD HODGKIN-HUXLEY MODEL AND SQUID AXONS IN REDUCED EXTERNAL CA++ FAIL TO ACCOMMODATE TO SLOWLY RISING CURRENTS ERIC JAKOBSSON, Department of Physiology and Biophysics and

More information

OSMOTIC TOLERANCE OF Ca-DEPENDENT EXCITABILITY IN THE MARINE CILIATE PARAMECIUM CALKINS J

OSMOTIC TOLERANCE OF Ca-DEPENDENT EXCITABILITY IN THE MARINE CILIATE PARAMECIUM CALKINS J J. exp. Biol. (1982), 97, 311-324 311 With 10 figures Wrinted in Great Britain OSMOTIC TOLERANCE OF Ca-DEPENDENT EXCITABILITY IN THE MARINE CILIATE PARAMECIUM CALKINS J BY JOACHIM W. DEITMER AND HANS MACHEMER

More information

potential cannot be considered to be constant. (Received 25 August 1969) potential of calcium current was estimated to be about + 60 mv in normal

potential cannot be considered to be constant. (Received 25 August 1969) potential of calcium current was estimated to be about + 60 mv in normal J. Physiol. (1970), 207, pp. 191-209 191 With 10 text gurem Printed in Great Britain MEMBRANE CALCIUM CURRENT IN VENTRICULAR MYOCARDIAL FIBRES BY G. W. BEELER JR. AND H. REUTER* From the Section of Physiology

More information

dependence similar to that of the zero-time extrapolated estimates of the K inward Medicine, University of Tokyo, Tokyo, Japan

dependence similar to that of the zero-time extrapolated estimates of the K inward Medicine, University of Tokyo, Tokyo, Japan J. Phy"io. (1981), 311, pp. 289-35 289 With 8 text-figurem Printed in Great Britain UNTARY CURRENT THROUGH SODUM CHANNEL AND ANOMALOUS RECTFER CHANNEL ESTMATED FROM TRANSENT CURRENT NOSE N THE TUNCATE

More information

Supporting Information

Supporting Information Supporting Information Mullins et al. 10.1073/pnas.0906781106 SI Text Detection of Calcium Binding by 45 Ca 2 Overlay. The 45 CaCl 2 (1 mci, 37 MBq) was obtained from NEN. The general method of 45 Ca 2

More information

Membrane Protein Channels

Membrane Protein Channels Membrane Protein Channels Potassium ions queuing up in the potassium channel Pumps: 1000 s -1 Channels: 1000000 s -1 Pumps & Channels The lipid bilayer of biological membranes is intrinsically impermeable

More information

Conductance Change Associated with Receptor Potentials of Gustatory Cells in Rat

Conductance Change Associated with Receptor Potentials of Gustatory Cells in Rat Published Online: 1 December, 1971 Supp Info: http://doi.org/10.1085/jgp.58.6.688 Downloaded from jgp.rupress.org on January 22, 2019 Conductance Change Associated with Receptor Potentials of Gustatory

More information

7 Membrane Potential. The Resting Membrane Potential Results From the Separation of Charges Across the Cell Membrane. Back.

7 Membrane Potential. The Resting Membrane Potential Results From the Separation of Charges Across the Cell Membrane. Back. Back 7 Membrane Potential John Koester Steven A. Siegelbaum INFORMATION IS CARRIED WITHIN and between neurons by electrical and chemical signals. Transient electrical signals are particularly important

More information

A note on discontinuous rate functions for the gate variables in mathematical models of cardiac cells

A note on discontinuous rate functions for the gate variables in mathematical models of cardiac cells Procedia Computer Science (2) (22) 6 945 95 Procedia Computer Science www.elsevier.com/locate/procedia International Conference on Computational Science ICCS 2 A note on discontinuous rate functions for

More information

Supplementary Figure 1

Supplementary Figure 1 Supplementary Figure 1 Activation of P2X2 receptor channels in symmetric Na + solutions only modestly alters the intracellular ion concentration. a,b) ATP (30 µm) activated P2X2 receptor channel currents

More information

Ionic Blockage of Sodium Channels in Nerve

Ionic Blockage of Sodium Channels in Nerve Ionic Blockage of Sodium Channels in Nerve ANN M. WOODHULL From the Department of Physiology and Biophysics, University of Washington School of Medicine, Seattle, Washington 98195. Dr. Woodhull's present

More information

PNS Chapter 7. Membrane Potential / Neural Signal Processing Spring 2017 Prof. Byron Yu

PNS Chapter 7. Membrane Potential / Neural Signal Processing Spring 2017 Prof. Byron Yu PNS Chapter 7 Membrane Potential 18-698 / 42-632 Neural Signal Processing Spring 2017 Prof. Byron Yu Roadmap Introduction to neuroscience Chapter 1 The brain and behavior Chapter 2 Nerve cells and behavior

More information

Action Potential (AP) NEUROEXCITABILITY II-III. Na + and K + Voltage-Gated Channels. Voltage-Gated Channels. Voltage-Gated Channels

Action Potential (AP) NEUROEXCITABILITY II-III. Na + and K + Voltage-Gated Channels. Voltage-Gated Channels. Voltage-Gated Channels NEUROEXCITABILITY IIIII Action Potential (AP) enables longdistance signaling woohoo! shows threshold activation allornone in amplitude conducted without decrement caused by increase in conductance PNS

More information

Voltage-Dependent Membrane Capacitance in Rat Pituitary Nerve Terminals Due to Gating Currents

Voltage-Dependent Membrane Capacitance in Rat Pituitary Nerve Terminals Due to Gating Currents 1220 Biophysical Journal Volume 80 March 2001 1220 1229 Voltage-Dependent Membrane Capacitance in Rat Pituitary Nerve Terminals Due to Gating Currents Gordan Kilic* and Manfred Lindau *University of Colorado

More information

Influence of permeating ions on potassium channel block by external tetraethylammonium

Influence of permeating ions on potassium channel block by external tetraethylammonium 4414 Journal of Physiology (1995), 486.2, pp.267-272 267 Influence of permeating ions on potassium channel block by external tetraethylammonium Stephen R. Ikeda* and Stephen J. Korn t *Department of Pharmacology

More information

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES Physiology Unit 2 MEMBRANE POTENTIALS and SYNAPSES Neuron Communication Neurons are stimulated by receptors on dendrites and cell bodies (soma) Ligand gated ion channels GPCR s Neurons stimulate cells

More information