A 'TEA + -INSENSITIVE' MUTANT WITH INCREASED POTASSIUM CONDUCTANCE IN PARAMECIUM AURELIA
|
|
- Opal Long
- 5 years ago
- Views:
Transcription
1 J. txp. Biol. (1976), 65, 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 of Molecular Biology and Department of Genetics, University of Wisconsin, Madison, Wisconsin 53706, U.S.A. (Received 31 December 1975) SUMMARY A single-gene mutant of Paramecium aurelia is analysed electrophysiologically. (a) The regenerative Ca-response, triggered by small or moderate current, was smaller and slower in the mutant than in wild type, (b) Input resistance of the mutant membrane is about half of that of wild type bathed in various solutions. This is true for the zero-current input resistance and the chord resistance measured with high depolarizing current, (c) Membrane resistance of the mutant measured with hyperpolarizing currents is smaller than that of wild type only when K + is the major external cation, (d) Internally applied TEA + or externally applied Ba+ increases the membrane resistance of the mutant to that of wild type similarly treated. We conclude that the mutant has an increased K conductance. INTRODUCTION Despite intensive research the chemical identity of the ionic channels of excitable membranes and the molecular mechanism of ion permeation remain elusive. One approach to the problem is to identify these channels by genetic means. Mutants with defective channels can be used as the null control in physiological investigations and chemical identifications. Paramecium has been used in this approach to the study of membrane functions through mutations because information is available on both genetics (Sonneborn, 1970) and electrophysiology (Eckert, 1972; Naitoh & Eckert, 1974) of this genus. The rationale for genetic studies of the excitable membrane in Paramecium was given by Kung (1971^). Three hundred lines of mutants are now available in P. aurelia (Kung et al. 1975). Among them are ones with defects in their voltage-sensitive Ca channel which result in the loss of the Ca action potential (Kung & Eckert, 1972). There are conditional mutants which reveal their defects after growing at high temperatures (Satow, Chang & Kung, 1974; Satow & Kung, 19766). Since the ciliary motions of Paramecium are governed by the membrane potential and action potentials are coupled to reversal of the direction of ciliary beating (Eckert, 1972; Naitoh & Eckert, 1974), membrane defects are reflected as anomalies in the locomotor behaviour. Thus, mutants without action potentials are unable to reverse their ciliary beat and fail in the 'avoiding 4-3
2 52 YOUKO SATOW AND CHING KUNG reaction' (the 'pawn' mutants, Kung, 1971a), while those with prolonged depolarizations swim backward for long distances (the 'paranoiac' mutants, Kung, 1971a; Satow, Hansma & Kung, 1976). This paper reports our findings on a mutant which has a very low membrane resistance, a defect we have now traced to a K channel. The screening method used to isolate this mutant is based on one of its behavioural deficiencies, (i.e. its inability to generate spontaneous avoiding reactions in tetraethylammonium (TEA+) solutions). Details on mutagenesis, screening, behavioural phenotyping and genetic analyses of this 'TEA + -insensitive' mutant are given by Chang & Kung (1976). A preliminary report of this work has appeared elsewhere (Satow, 1975). MATERIALS AND METHODS Stocks and cultures We used the ' TEA+-insensitive' mutant (stock C14-152, genotype teaa/teaa) and wild type (stock 51s) from which the mutant was derived. Both stocks belong to species 4 of Paramecium aurelia. Cells were cultured in the Cerophyl medium bacterized with Aerobacter aerogenes 20 h before use (Sonnebom, 1970). Only robust cells in logphase growth were used. Solutions All solutions contained 1 mm-ca(oh) 2, 1 mm citric acid, buffered to ph with i-o-i-2mm Tris [tris (hydroxymethyl) aminomethane]. The K solution, containing in addition 4 mm-kcl, was the 'adaptation solution' in which the cells were penetrated by electrodes. In most experiments, the K solution was replaced by various test solutions in which K + was replaced by other cations. They were the Ca-, Mn-, Ba-, and TEA-solutions containing 2 mm of CaCl 2 or MnClj, 2 or 4 mm of BaCl a or 4 mm of NaCl or TEA-C1 (tetraethylammonium chloride, Aldrich Chemical Co.), respectively. In the series of experiments testing the effect of TEA+ in differentt concentrations, 1, 4 and 16 mm TEA-C1 were used. Recording The methods for intracellular recording were basically those of Naitoh & Ecker (1972). Modifications of the reference electrode and the use of continuous perfusion are described by Satow & Kung (1976a). To study the steady-state I-V relationship, 200 ms to 1 s pulses of current (less than io~ fl A) were delivered. Both the stimulating electrode and the recording electrode were filled with 500 mm-kcl with tip resistances of MD. Injection of TEA+ Microelectrodes filled with 100 mm TEA-C1 were used. A depolarizing io~ 9 d.c. current was applied through such an electrode for the ionophoretic injection of TEA+. Ten minutes of such a current is estimated to give 20 mm concentration of TEA+ in the cytoplasm, based on a transport number of 0*5 (Friedman & Eckert, 1973) and a cell volume of 1-5 x io~ 7 ml. The effect of injected TEA+ lasted over 30 min, during which time membrane properties were examined.
3 Wild type A mutant tvith increased G K TEA" mutant S3 11 / a > 50 ms Fig. I. Electrically triggered action potentials from wild type (left) and the ' TEA-insensitive' mutant (right) of P. aurelia bathed in K solution. The three traces in each frame from top to bottom are the first-derivative of potential (dvm/dt) (this trace also marks the reference level), potential (Vm) and injected current (7Xio" u A). Square pulses on the Vm traces are lorav, 10 ms calibration. Note that the peak potential, the maximal dvm\dt and the steady-state depolarization after spike are all smaller in the mutant. TEA Mn J TEA - mutant Fig. 2. Electrically triggered action potentials from two strains of P. aurelia. The responses of the mutant (bottom row) are weaker than those of wild type (top) and the mutant defect persists in five different bath solutions. The top bar in each frame marks the V = o reference. The bottom trace is the outward current injected (5 x io" 10 A). Square pulses on the Vm traces, when present, are 10 mv, 10 ms calibration. The major cations in the solutions used in each experiment are as marked. Complete compositions of these solutions are given in Materials and Methods. RESULTS Electrically evoked responses The most outstanding electrophysiological defect of the mutant is the diminution of its response to injected current. Fig. 1 shows the responses to a moderate outward current (7 x io~ 10 A) by wild type and the mutant bathed in the K solution. This is the 'adaptation solution' and there is no systematic difference in the resting level between the two strains in this solution (see Table 1). Wild type generates an action potential (the Ca regenerative response, Naitoh & Eckert, 1968 a; Satow & Kung, 19766) followed by a steady-state response. The action potential of the mutant evoked by a comparable current (right) is clearly smaller in amplitude. The maximal rate of rise, as seen from the peak of the dv/dt trace, and the steady-state depolarization by the constant current are also reduced. These defects of the mutant persist in different bath solutions. Fig. 2 shows the responses evoked by injected outward current from paramecia bathed in five solutions containing K+, Na+, TEA+, Ca^, or Mn as the major cation. Wild type generates
4 54 YOUKO SATOW AND CHING KUNG 5 10 x 10-' A Wild type B [Gi] 0 3 mn TEA" mutant Wild type j TEA" mutant- Fig. 3. I-V relationships of wild type and the mutant in (A) K solution; (B) Ca solution. Circles and bars are mean±s.d. (n = 5-14) from wild type. Triangles and bars are mean* ±S.D. (n = 3-10) from the mutant. Note the smaller slope resistance and chord resistance of the mutant throughout except in the region of strong hyperpolarization in A, where the external solution is devoid of K +.
5 A mutant with increased G K 55 Table 1. Membrane resistance (Rm) and resting potential (Vm) of ttoo strains of P. aurelia in three different solutions* K solution Ca solution TEA solution (A) (B) (A) (B) (A) (B) Wild type fim(mfl) Km(mV) 48-o±2i-i 56-0 ± ±290 7i-3±i8-o 8I-I± ± '2± ±3-4 -4O-Q±4-6 (A) (B) (A) (B) (A) (B) ttcr mutant Jta(Mfl) Fm(mV) ± ± ±5'6-2O-4± ± ± ±4-i 33'5±i6'2 Mean±8.D.,n = 7-16; chord resistance measured with io~ 10 A depolarizing (A) or hyperpolarizing (B) currents. See Materials and Methods for the compositions of solutions. action potentials when stimulated by injected current in allfivesolutions (Fig. 2, top). As in P. caudatum (Naitoh & Eckert, 1968 a), Mn 2 " 1 " does not inhibit this Ca response. In all five solutions, the Ca regenerative response of wild type evoked by small to moderate current (< 7 x io" 10 A) is faster and reaches higher peaks than that of the mutant. The regenerative responses of the mutant and wild type are graded to the stimuli. The steady-state depolarization of the mutant membrane after the spike is smaller than that of wild type in all solutions. At supramaximal currents (> io~ e A), the mutant can often give spikes equal to those of wild type in the peak potential and in the maximal rate of rise (see Fig. 5). This and other evidence presented below show that the Ca activation is not affected in this mutant unlike the case of 'pawn' mutants (Kung & Eckert, 1972; Satow & Kung, 19766; Schein, Katz & Bennett, 1976). I-V relations and membrane resistance Steady-state potential displacement by 200 msec injected current is plotted against the current strength. In paramecium, the I-V curves are sigmoidal (Naitoh & Eckert, 1968 a; Kung & Ecker, 1972). The resistance of the mutant membrane is smaller than that of the wild-type membrane at all points, when tested in the K solution (Fig. 3 A). In the Ca solution where no K + is added, both the mutant and the wildtype membrane appear more resistive than in the K solution (Fig. 3 B). The difference between the two strains remains clear for depolarizing currents, but ceases to be statistically significant for moderate or large hyperpolarizing currents. The zero-current input resistance of the resting membrane is estimated with small current injections. The results are summarized in Table 1. The resting membrane resistance is reduced to about half by the mutation. The comparison of the resistances of the two strains is valid since they are of the same size and rest at the same potential level. With the application of strong hyperpolarizing current, (e.g. io~ 9 A) the difference of the chord resistance between the two strains is not observed in the Ca solution (Fig. 3 B) and the TEA solution (Fig. 6), where [K] out = o, but it is seen in the K solution (Fig. 3 A). This result suggests that the mutant defect is on a K conductance.
6 56 YOUKO SATOW AND CHING KUNG Wad type III mm JIUUU1LJUilU TEA" mutant > TEA 25 sec 58S msec Fig. 4. Membrane potentials recorded intracellularly from two strains of Paramecium aurelia in TEA solution. Top: from wild type, showing action potentials generated spontaneously in 4 mm TEA+. Bottom: from the mutant, showing the complete lack of active response in the same solution. Cells were first adapted in the K solution. Arrows mark the time when the TEA solution begins to replace the K solution. Broken lines mark the reference level. See Materials and Methods for complete composition of the solutions. Effects of externally applied TEA+ When K solution is replaced with TEA solution (4 mm, see above for complete composition), wild-type animals respond with a train of action potentials as shown in Fig. 4 (top). The amplitude and frequency of the spikes vary. Both the up- and the downstrokes of the action potentials are steep, much like the response to Ba solution (Kung & Eckert, 1972; Satow et al. 1974; and Fig. 8) and unlike the response to the Na solution (Satow & Kung, 1974). Each spike corresponds to a transient period of ciliary reversal and so to an avoiding reaction in the free-swimming paramecium. Ciliary reversal is coupled to action potential through Ca*+ (Naitoh & Kaneko, 1972; Eckert, 1972). Thus, these spontaneously generated action potentials in the TEAsolutions are a form of Ca regenerative response. Fig. 4 (bottom) shows the response of the mutant to identical treatment. Excitation is conspicuously absent. Increasing the concentration of TEA+ in the solution up to 16 mm does not trigger any action potential. Corresponding behavioural tests have shown little or no avoiding reactions to TEA+, hence the name ' TEA-insensitive' when it was first described (Kung et al. 1975)- Friedman & Eckert (1973) showed that TEA + blocked K conductance and thus reduced the short-circuiting leakage and the repolarizing rate in P. caudatum. We have found a similar effect in the wild-type P. aurelia. Less than io~ w A is often sufficient to trigger an action potential in an animal bathed in 4 mm TEA+. The threshold cannot be accurately assessed because the membrane is spontaneously active in the TEA solution. Fig. 5 (top row) shows these triggered action potentials in wild type. The amplitude of the triggered action potential is sharply graded with the stimulus, approaching an all-or-none response. Increasing outward current strength increases the rate of rise, but not the peak potential. Although in the mutant there is no spontaneous response in the TEA solution we can evoke responses with outward currents (Fig. 5, bottom row). Unlike the wildtype response, the mutant response increases gradually with the injected current.
7 Wild type A mutant with increased G K 57 TEA" mutant 100 ms Fig. 5. Potential responses to injected currents in wild type (top row) and the mutant bathed in 4 DIM TEA solution (bottom row). The four traces in each frame from top to bottom are reference level, potential (Km), injected current (/) andfirst-derivativeof potential (dvmjdt). Square pulses on the Vm traces are 10 mv, 10 ms calibration. In wild type, the action potential is nearly all-or-none in amplitude in the presence of TEA" 1 ". The ma-rima! rate ofriseas seen in the dvmjdt increases with the current strength. In the mutant, the action potentials are small and graded gradually with the current strength. Close to normal spike amplitude and rate of rise are seen in the mutant only in response to strong depolarizing current (next to the last frame). Current strengths in the six frames from left to right are 1, a, 3, 5, 10 (outward) and 2 (inward current) x io" 10 A, respectively. The same specimen from each strain was used in all six experiments. [TEA] 0 4mM [Ca] 0 1 mil mv r -i >- 5 H- i i 10 xlo- )O A if Wild type L TEA" mutant Fig. 6. I-V relationships of wild type and the mutant in TEA solution. Circles and bars are means±8.d. (n 5-15) from wild type; triangles and bars (n =» 4-1 a), from the mutant Note that the externally applied TEA+ is unable to counteract the mutant defect. The difference between wild type and the mutant remains large except in the region of strong hyperpolarizations.
8 YOUKO SATOW AND CHING KUNG [K] u 4 mm [C;i] o 1 HIM mv i r / \ Wild type f \ o 1 ^^ 10 xl0-10 A TEA" mutant o f- \ Fig. 7. I-V relationships of wild type and the mutant after io min, io~* A ionophoretic injection of TEA" 1 ". The internally applied TEA+ increases the input resistance of both strains (see Fig. 3 A) and abolishes the difference between wild type (open symbols) and the mutant (closed symbols). Different symbols represent experiments with different specimens. Insert shows the membrane potentials of the two strains in response to +5 and sxio~ 18 A injected current where the downstrokes of the action potentials are no longer observed. Calibration". 20 mv, 150 ms. The peak potential and maximal rate of rise are smaller in the mutant for small moderate stimuli (1-5 x io~ 10 A), but approach those of wild type for very large currents (io~ 9 A). Fig. 5 also shows that the steady-state potential displacement by a given current is smaller in the mutant than in wild type. The I-V relation in 4 mm TEA solution is plotted for both strains (Fig. 6). Estimated zero-current input resistance of the mutant is clearly smaller than that of wild type (Table 1). Clear reduction in chord resistance in the mutant is seen for large depolarizing, but not for hyperpolarizing currents. This asymmetry is also observed in the Ca solution (Fig. 3 B), which like the TEA solution is devoid of K+. 16 mm TEA solution depolarizes both wild type and the mutant but the difference in resistance of the two strains remains clear. This difference persists when 1 mm TEA solution is used. Effects of internally applied TEA+ Externally applied TEA+ cannot eliminate the difference between wild type and the mutant. Therefore, we examined the effects of internally applied TEA+. Ionophoretically injected TEA+ blocks the downstroke of Ca response and increases the input resistance of the wild-type P. auretia bathed in the K solution. This is similar
9 A mutant with increased G R 59 Wild type TEA" mutant Fig. 8. Membrane potential* recorded intracellularly from the two strains in a 2 mm-ba solution. All-or-none action potentials are seen in both wild type (top) and the mutant (bottom). Records begin 3 min after the Ba solution begins to replace the K solution in which the cells were first adapted. See Materials and Methods for details on techniques and composition of solutions. to the finding of Friedman & Eckert (1973) in P. emulation. The effect is dependent on the amount of TEA+ injected. With io~ B A d.c. ionophoretic current, clear effects are first observed after 3 min. After 10 min of injection (about 20 mm TEA+ injected, see Materials and Methods) the steady-state potential displacements by test pulses increase to maximum (Fig. 7). The kinetics of the internal TEA+ effects cannot be accurately measured since the electrode characteristics are not uniform. Internal TEA + also reduces the resting potential and the rate of rise of the Ca action potential. The reasons for these changes are not clear. Injected TEA + has dramatic effects on the mutant. It increases the membrane resistance of the mutant to that of wild type, similarly treated. The distinct difference between the two strains before TEA+ injection in terms of the action potential and the after-spike steady-state response is no longer observed. Fig. 7 shows the I-V relation of the two strains of paramecia bathed in the K solution after a 10 min injection of TEA+: no significant difference remains between the two curves. Comparing Fig. 7 with Fig. 3 A we see that the input resistance of both strains is clearly increased by internal TEA+. The low-current (10-10 A) input resistances of two wild-type cells after this TEA+ injection were 115 and 90 MQ (de-) and 90 and no MO (hyperpolarizing direction). Those of two mutant cells were 112, 100 Mii and 82, 100 MQ, respectively. The effects of Ba*+ Naitoh & Eckert (19686) showed that Ba 2 * could carry the action current efficiently and block the K leakage in P. caudatum, resulting in all-or-none electrogenesis when the cell came into contact with Ba 2+. Such spikes were also recorded in wild-type P. aurelia (Kung & Eckert, 1972; Satow et al. 1974). Fig. 8 (top) shows this response of wild type when 2 mm-ba solution replaces the K solution in the bath. Fig. 8 (bottom) shows the response of the mutant. The down-stroke of the action potential is often steeper in the mutant than in wild type, although variations within each strain is
10 6o YOUKO SATOW AND CHING KUNG -10 xlo a 30 6 Wild type TEA" mutant ^ 40 Fig. 9. I-V relationships of wild type and the mutant in 4 mm-ba solution. Open circles and bars are means±s.d. (n = 4-12) from wild type; closed circles and bars (n >= 4-14) from the mutant. The difference between wild type and the mutant observed elsewhere is abolished by Ba*+. large. Each of the spikes is correlated with a rapid avoiding reaction. Neither the mutant nor wild type ever fails to respond to the Ba solution behaviourally or electrophysiologically. Fig. 9 shows the I~V relation with hyperpolarizing current of wild type and the mutant in 4 mm-ba solution. The depolarization half in this solution cannot be measured accurately, owing to spontaneous activity. The input resistances to small hyperpolarizing current (io~ w A) of wild type and the mutant are indistinguishable, being 93-3 ± 20-9 MQ and 92-1 ± 17-4 MO, respectively. DISCUSSION The physiological defects of the mutant are best explained by mutational increase of K conductance. The major evidence is as follows: (1) K + efflux limits the Ca response in Paramechun; larger K+ efflux in the mutant could explain the reduction of Ca action potentials (Figs. 1, 2 and 5). (2) The resting resistance of the mutant is half that of wild type. Membrane resistance of the mutant measured with large inward current is smaller than that of wild type only when K+ is the major external cation (Figs. 3 and 6). (3) Internally applied TEA+ counteracts the mutational effects, increasing the membrane resistance of the mutant to equal that of wild type (Fig. 7). Ca regenerative response In response to small or moderate currents the active depolarizations of the mutant are clearly smaller and slower than wild type (Figs. 1, 2 and 5). However, large outward current evokes Ca responses in the mutant which approach the peak potential and the maximal rate of rise of those of wild type (Fig. 5). This result suggests that the Ca activation mechanism of the mutant is not impaired. Other evidence showing that
11 A mutant with increased G K 61 fca activation is normal in the mutant is the observation of Ba spikes (Fig. 8). Apart trom a faster repolarization, the Ba spikes of the mutant are the same as those of wild type. Hagiwara et al. (1974) showed that Ba 2 " 1 " carries the action current through the Ca channel and blocks the early K + current in barnacle muscle. Since Ba I+ carries more current, the action potentials are all-or-none in character. Similar findings and interpretations have been made on P. caudatum (Naitoh & Eckert, 1968ft, 1972) and P. aurelia (Satow et al. 1974; Kung & Eckert, 1972). Since normal Ba spikes can be generated in the mutant (Fig. 8), there is no reason to believe that the Ca activation mechanism is defective as in the cases of the 'pawn' mutants (Kung & Eckert, 1972; Satow et al. 1974; Satow & Kung, 19766; Schein et al. 1976). In both crustacean muscle and paramecium, the regenerative Ca responses are graded to the strength of the stimuli. The graded Ca action potentials are often contrasted with the well-known all-or-none Na action potentials in nerve. The Ca response is graded because the Ca activation is considerably slower than the Na activation in nerves: the Ca action potential is determined by both inward Ca current and the counteracting outward K current (Hagiwara, Hayashi & Takashi, 1969; Naitoh & Eckert, 1968 a). The defective Ca action potentials of the mutant can therefore be the result of larger outward K counter current in the generation of action potential. The downstrokes of the action potentials of the mutant are often steeper than those of wild type and almost always undershoot the steady-state depolarization levels (Figs. 1, 2 and 5), suggesting increased K+ efflux during both depolarizing and repolarizing phases of the calcium action potential. I~V relations The sigmoidal nature of the I~V curves of Paramecium is not fully understood. Presumably there are voltage-insensitive ion channels as well as channels sensitive to depolarization and those sensitive to hyperpolarization. Paramecium membrane was found to be permeable to a large variety of cations based on their ability to depolarize the membrane (Naitoh & Eckert, 1968 a). Browning & Nelson (1976) show that the permeability to K + is higher than those to other ions in Paramecium. Comparing the parts of the I~V curves with, moderate to high hyperpolarizing currents, it is clear that the resistance of the mutant is nearly the same as that of wild type when tested in solutions devoid of K+, i.e. in the Ca solution (Fig. 3B) and the TEA solution (Fig. 6). Membrane resistance in this part of the I-V curve of the mutant is clearly smaller than that of wild type when K + is the major cation in the bath (Fig. 3 A). These observations are consistent with the view that the portion of the conductance increased by the mutation is K + specific, since for large hyperpolarizations the membrane current is carried by the cations in the external solution. The effects of TEA+ and Ba i+ Tetraethylammonium ion (TEA+) affects the K channels in excitable membranes: both the voltage dependent K channel in frog myelinated nerve fibre (Hille, 1967; Armstrong & Hille, 1972) and the resting K permeability of barnacle muscle (Keynes et al. 1973). Friedman & Eckert (1973) showed that internal TEA+ increases membrane resistances and block the down-stroke of the Ca action potential in P. caudatum. We
12 62 YOUKO SATOW AND CHING KUNG found that the mutationally increased conductance can be blocked by internal TEA (Fig. 7), again suggesting that the mutation increases K conductance. Externally applied TEA+, though not as effective as that internally applied, also blocks the K efflux in paramecium. By reducing the short-circuiting effect, this blockage makes the Ca activation more effective. Thus, the Ca action potentials are more effective. Thus, the Ca action potentials are more sharply graded with the strength of applied current, approaching all-or-none (Fig. 5). In fact, the generation of the action potential is so efficient that spontaneous activity is recorded (Fig. 4). In contrast, in the mutant the evoked action potentials are gradually graded (Fig. 5) and spontaneous activity is absent (Fig. 4). This suggests that the outward K current of the mutant remains high when bathed in this TEA solution. This may mean that the effect of externally applied TEA+ is not strong enough to compensate for the mutationally induced K conductance. Alternatively, it is possible that the mutation increases a K conductance which is less or not sensitive to external TEA+. The mutant behaves similarly to wild type in the Ba solution (Fig. 8). In solutions of 4 mm Ba 2+ or above, the resting membrane resistance and I-V relation (Fig. 9) are not different from those of wild type. These results show that Ba 2+, like internally applied TEA+, is effective in blocking the mutationally altered K channel. This blockage is concentration dependent; lower concentration (2 mm) is less effective. Speculation on the altered K channel The mechanism of K+ permeation in normal paramecium is not well understood. For example, it is not known if the resting K conductance can be activated or if the activation is mediated through depolarization or Ca*+ or both. Mutation affecting the relative resting K permeability in the case of the 'fast-2* mutant (Satow & Kung, 1976a) can give a phenotype quite different from the ' TEA+-insensitive' mutant studied here. The increased K conductance of this mutant clearly affects the outward going rectification. It is, therefore, possible that the K channel responsible for the K delayed rectification has been mutated in such a way that it is now activated even when the membrane is at rest. Future work on this and other membrane mutants may help us identify and sort out the different K channels in Paramecium. We thank Professor S. Hagiwara for his helpful criticism in the preparation of the manuscript. Supported by PHS GM and NSF BMS REFERENCES ARMSTRONG, C. M. & HILLE, B. (1972). The inner quaternary ammonium ion receptor in potassium channels of the node of ranvier. J. gen. Physiol. 59, BROWNING, J. L. & NELSON, D. L. (1976). Studies of the excitable membrane of Parmecium aurelia. II. Direct measurement of monovalent cation fluxes. Bioclrim. Biopkyt. Acta, Biomembrana (submitted). CHANG, S. Y. & KUNG, C. (1976). Selection and analyses of a mutant lacking behavioural response to tetraethylammonium in Paramecium aurelia. Genet. Researcli (in the Press). ECKERT, R. (1972). Bioelectric control of cilia. Science, N. Y. 176, FRIEDMAN, K. & ECKERT, R. (1973). Ionic and pharmacological modification of input resistance and excitability in Paramecium. Comp. Biochem. Pltytiol. 45A, HAGIWARA, S., FUKUDA, J. & EATON, D. C. (1974). Membrane currents carried by Ca, Sr and Ba in barnacle muscle fiber during voltage clamp. J. gen. Pltytiol. 63, HAGIWARA, S., HAYASHI, H. & TAKAHASHI, K. (1969). Calcium and potassium currents of the membrane of a barnacle muscle fibre in relation to the calcium spike. J'. Physiol., Lond. 305,
13 A mutant with increased G K 63 ILLE, B. (1967). The selective inhibition of delayed potassium currents in nerve by tetraethylammonium ion. J. gen. Phytiol. 50, KEYNES, R. D., ROJAS, E., TAYLOR, R. E. & VEROARA, J. (1973). Calcium and potassium systems of a giant barnacle muscle fibre under membrane potential control. J. Phytiol., Lond. 339, KUNG, C. (1971a). Genie mutants with altered system of excitation in Paramecium aurejia. I. Phenotypes of the behavioral mutants. Z. vergl. Physiol. 71, KUNG, C. (19716). Genie mutants with altered system of excitation in Paramecium aurdia. II. Mutagenesis, screening and genetic analysis of the mutants. Genetics 69, KUNG, C, CHANG, S. Y., SATOW, Y., VAN HOUTEN, J. & HANSMA, H. (1975). Genetic dissection of behavior in Paramecium. Science, N. Y. 188, KUNG, C. & ECKERT, R. (1972). Genetic modification of electric properties in an excitable membrane. Proc. natn. Acad. Sci. Wash. 69, NAITOH, Y. & ECKERT, R. (1968a). Electrical properties of Paramecium caudatum: modification by bound and free cations. Z. vergl. Phytiol. 61, NAITOH, Y. & ECKERT, R. (19686). Electrical properties of Paramecium caudatum: all-or-none electrogenesis. Z. vergl. Phytiol. 61, NAITOH, Y. & ECKERT, R. (1972). Electrophysiology of the ciliate protozoa. In Experiments in Physiology and Biochemistry, vol. v (ed. G. A. Kerkut), pp London: Academic Press. NAITOH, Y. & ECKERT, R. (1974). The control of ciliary activity in Protozoa. In Cilia and Flagclla (ed. M. A. Sleigh), pp London and New York: Academic Press. NAITOH, Y. & KANEKO, H. (1972). ATP-Mg-reactivated Triton-extracted models of Paramecium modification of ciliary movement by calcium ions. Science, N. Y. 176, SATOW, Y. (1975). TEA-insensitive mutant in Paramecium aurelia. 5th Annual Meeting for Neuroscience (at New York), Abstracts 949. SATOW, Y., CHANG, S. Y. & KUNO, C. (1974). Membrane excitability: made temperature dependent by mutations. Proc. natn. Acad. Sci. Wash. 71, SATOW, Y., HANSMA, H. & KUNG, C. (1976). The effect of sodium on 'Paranoiac'-a membrane mutant of Paramecium. Comp. Biochem. Physiol. 54 A, SATOW, Y. & KUNO, C. (1974). Genetic dissection of the active electrogenesis in Paramecium aurelia. Nature, Lond., 347, SATOW, Y. & KUNG, C. (1976 a). A mutant of Paramecium with relative increased resting potassium permeability. J. Neurobiology (in the Press). SATOW, Y. & KUNG, C. (19766). Mutants with reduced Ca activation in Paramecium aurelia. J. memb. Biol. (in the Press). SCHEIN, S. J., KATZ, G. M. & BENNETT, M. V. L. (1976). Electrophysiological basis of the pawn trait, behavioral mutants of Paramecium aurelia (in preparation). SONNBBORN, T. M. (1970). Methods in Paramecium research. In MetJiods in Cell Physiology, vol. 4 (ed. D. Prescott), pp New York: Academic Press.
14
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 informationGenetic Modification of Electric Properties in an Excitable Membrane
Proc. Nat. Acad. Sci. USA Vol. 69, No. 1, pp. 93-97, January 1972 Genetic Modification of Electric Properties in an Excitable Membrane (paramecium/calcium conductance/electrophysiological measurements/membrane
More informationSENSORY 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 informationDIVALENT 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 informationPotential, 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 informationPeripheral 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 informationClasificador 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 informationAD-" IONIC BASIS OF POTENTIAL REGULATION(U) BAYLOR COLLO / U U ijejmedicine L HOUSTON TX DEPT OF PHYSIOLOGY AND MOLECULAR 7 MEEE"..
AD-"19 459 IONIC BASIS OF POTENTIAL REGULATION(U) BAYLOR COLLO / U U ijejmedicine L HOUSTON TX DEPT OF PHYSIOLOGY AND MOLECULAR 7 MEEE"..,E NCLA SIFIE BIOPHYSIC S D C CHANG 6 i N 1988 Neg@14-85-K-6424
More informationOSMOTIC 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 informationBRIEF 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 informationEFFECTS 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 informationBRIEF 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 informationALTERED CALCIUM CONDUCTANCE IN PAWNS, BEHAVIOURAL MUTANTS OF PARAMECIUM AURELIA
J. exp. Biol. (1976), 65, 699-724 With 13 figures Printed in Great Britain ALTERED CALCIUM CONDUCTANCE IN PAWNS, BEHAVIOURAL MUTANTS OF PARAMECIUM AURELIA BY STANLEY J. SCHEIN*. M. V. L. BENNETTf AND GEORGE
More informationPhysiology 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 information6.3.4 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 informationChannels 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 informationPhysiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES
Physiology Unit 2 MEMBRANE POTENTIALS and SYNAPSES In Physiology Today Ohm s Law I = V/R Ohm s law: the current through a conductor between two points is directly proportional to the voltage across the
More informationLecture 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 informationACTION 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 informationMembrane 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 information4. Active Behavior of the Cell Membrane 4.1 INTRODUCTION
1 of 50 10/17/2014 10:48 PM 4.1 INTRODUCTION When a stimulus current pulse is arranged to depolarize the resting membrane of a cell to or beyond the threshold voltage, then the membrane will respond with
More informationthey 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 informationAction Potentials & Nervous System. Bio 219 Napa Valley College Dr. Adam Ross
Action Potentials & Nervous System Bio 219 Napa Valley College Dr. Adam Ross Review: Membrane potentials exist due to unequal distribution of charge across the membrane Concentration gradients drive ion
More informationMEMBRANE POTENTIALS AND ACTION POTENTIALS:
University of Jordan Faculty of Medicine Department of Physiology & Biochemistry Medical students, 2017/2018 +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ Review: Membrane physiology
More informationCh. 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 informationInactivation 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 informationMembrane 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 informationELECTROGENIC Na + TRANSPORT IN A CRUSTACEAN COXAL RECEPTOR
J. exp. Biol. (1979). 78, 29-45 29 With 10 figures Printed in Great Britain ELECTROGENIC Na + TRANSPORT IN A CRUSTACEAN COXAL RECEPTOR BY MAURIZIO MIROLLI Medical Sciences Program, Indiana University,
More informationConductance 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 informationVoltage-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 informationNerve Signal Conduction. Resting Potential Action Potential Conduction of Action Potentials
Nerve Signal Conduction Resting Potential Action Potential Conduction of Action Potentials Resting Potential Resting neurons are always prepared to send a nerve signal. Neuron possesses potential energy
More information7 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 informationRahaf 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 informationmembrane, and the other to record the potential. It will be shown that the 'delayed rectification' and not to any special effect of the neuromuscular
586 J. Physiol. (I956) I32, 586-598 THlE ELECTRICAL PROPERTIES OF THE SLOW MUSCLE FIBRE MEMBRANE BY W. BURKE AND B. L. GINSBORG From the Biophysics Department, University College London (Received 10 February
More informationResearch was conducted according to the principles enunciated in the "Guide for Laboratory Animal Facilities and Care, " prepared by the National
AFRRI SCIENTIFIC REPORT AFRRI SR74-18 AUGUST 1974 INTRACELLULAR RESPONSES TO PHYSIOLOGIC STIMULI FROM APLYSIA STATOCYST RECEPTOR CELLS eo M. L Wiederhold ARMED FORCES RADIOBIOLOGY RESEARCH INSTITUTE Defense
More informationChapter 48 Neurons, Synapses, and Signaling
Chapter 48 Neurons, Synapses, and Signaling Concept 48.1 Neuron organization and structure reflect function in information transfer Neurons are nerve cells that transfer information within the body Neurons
More informationΝευροφυσιολογία και Αισθήσεις
Biomedical Imaging & Applied Optics University of Cyprus Νευροφυσιολογία και Αισθήσεις Διάλεξη 5 Μοντέλο Hodgkin-Huxley (Hodgkin-Huxley Model) Response to Current Injection 2 Hodgin & Huxley Sir Alan Lloyd
More information2401 : Anatomy/Physiology
Dr. Chris Doumen Week 6 2401 : Anatomy/Physiology Action Potentials NeuroPhysiology TextBook Readings Pages 400 through 408 Make use of the figures in your textbook ; a picture is worth a thousand words!
More informationVoltage-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 informationPOTASSIUM 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 informationAction 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 informationQUESTION? Communication between neurons depends on the cell membrane. Why is this so?? Consider the structure of the membrane.
QUESTION? Communication between neurons depends on the cell membrane Why is this so?? Consider the structure of the membrane. ECF ICF Possible ANSWERS?? Membrane Ion Channels and Receptors: neuron membranes
More informationBIOL Week 5. Nervous System II. The Membrane Potential. Question : Is the Equilibrium Potential a set number or can it change?
Collin County Community College BIOL 2401 Week 5 Nervous System II 1 The Membrane Potential Question : Is the Equilibrium Potential a set number or can it change? Let s look at the Nernst Equation again.
More informationCALCIUM 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 informationIntroduction 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 informationChapter 9. Nerve Signals and Homeostasis
Chapter 9 Nerve Signals and Homeostasis A neuron is a specialized nerve cell that is the functional unit of the nervous system. Neural signaling communication by neurons is the process by which an animal
More informationResting 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 informationEditorial. 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 informationBISTABLE MEMBRANE POTENTIAL OF THE CILIATE COLEPS HIRTUS
The Journal of Experimental Biology 23, 757 764 (2) Printed in Great Britain The Company of Biologists Limited 2 JEB2284 757 BISTABLE MEMBRANE POTENTIAL OF THE CILIATE COLEPS HIRTUS PIA RUDBERG AND OLAV
More informationNeurophysiology. 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 informationNervous Systems: Neuron Structure and Function
Nervous Systems: Neuron Structure and Function Integration An animal needs to function like a coherent organism, not like a loose collection of cells. Integration = refers to processes such as summation
More informationBiomedical 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 informationAction 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 informationNervous Lecture Test Questions Set 2
Nervous Lecture Test Questions Set 2 1. The role of chloride in a resting membrane potential: a. creates resting potential b. indirectly causes repolarization c. stabilization of sodium d. it has none,
More informationAll-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 informationMINIATURE 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(Received 31 October 1962)
156 J. Physiol. (1963), 167, pp. 156-168 With 8 text-figures Printed in Great Britain THE EFFECT OF SODIUM ION CONCENTRATION ON THE ELECTRORETINOGRAM OF THE ISOLATED RETINA OF THE FROG BY D. I. HAMASAKI*
More informationCELLULAR 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 informationNervous System Organization
The Nervous System Chapter 44 Nervous System Organization All animals must be able to respond to environmental stimuli -Sensory receptors = Detect stimulus -Motor effectors = Respond to it -The nervous
More informationLOCAL ANESTHETIC ALTERATION OF
LOCAL ANESTHETIC ALTERATION OF MINIATURE ENDPLATE CURRENTS AND ENDPLATE CURRENT FLUCTUATIONS ROBERT L. RUFF From the Department of Physiology and Biophysics, University of Washington School of Medicine,
More informationInhibition of S532C by MTSET at intracellular ph 6.8 indicates accessibility in the closed
Supplementary Text Inhibition of S532C by MTSET at intracellular ph 6.8 indicates accessibility in the closed state It is difficult to examine accessibility of cysteine-substituted mutants in the fully
More informationGeneral 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 informationBRIEF COMMUNICATION BLOCKING OF INWARD RECTIFICATION. A MODEL FOR THE EFFECTS OF POTENTIAL AND EXTERNAL K+ CONCENTRATION ON THE Cs+
BRIEF COMMUNICATION A MODEL FOR THE EFFECTS OF POTENTIAL AND EXTERNAL K+ CONCENTRATION ON THE Cs+ BLOCKING OF INWARD RECTIFICATION S. CIANI, S. KRASNE, AND S. HAGIWARA, Department ofphysiology, Ahmanson
More informationHair Cells: The Sensory Transducers of the Inner Ear
Chapter 1 Hair Cells: The Sensory Transducers of the Inner Ear Hair cells are specialized cells that transform a mechanical motion into changes in membrane potential. Such changes, whereby one form of
More informationNeurons, Synapses, and Signaling
LECTURE PRESENTATIONS For CAMPBELL BIOLOGY, NINTH EDITION Jane B. Reece, Lisa A. Urry, Michael L. Cain, Steven A. Wasserman, Peter V. Minorsky, Robert B. Jackson Chapter 48 Neurons, Synapses, and Signaling
More informationElectrical Signaling. Lecture Outline. Using Ions as Messengers. Potentials in Electrical Signaling
Lecture Outline Electrical Signaling Using ions as messengers Potentials in electrical signaling Action Graded Other electrical signaling Gap junctions The neuron Using Ions as Messengers Important things
More information! Depolarization continued. AP Biology. " The final phase of a local action
! Resting State Resting potential is maintained mainly by non-gated K channels which allow K to diffuse out! Voltage-gated ion K and channels along axon are closed! Depolarization A stimulus causes channels
More informationme239 mechanics of the cell - syllabus me239 mechanics of the cell me239 mechanics of the cell - grading me239 mechanics of the cell - overview
6 mechanotransduction wong, goktepe, kuhl [2010] me239 mechanics of the cell add l information http://biomechanics.stanford.edu and coursework 1 me239 mechanics of the cell - syllabus favorite topics in
More informationOverview 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 informationLecture goals: Learning Objectives
Title: Membrane Potential in Excitable Cells 1 Subtitle: Voltage-Gated Ion Channels and the basis of the Action Potential Diomedes E. Logothetis, Ph.D. Lecture goals: This first of two lectures will use
More informationMathematical Foundations of Neuroscience - Lecture 3. Electrophysiology of neurons - continued
Mathematical Foundations of Neuroscience - Lecture 3. Electrophysiology of neurons - continued Filip Piękniewski Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, Toruń, Poland
More informationNervous System: Part II How A Neuron Works
Nervous System: Part II How A Neuron Works Essential Knowledge Statement 3.E.2 Continued Animals have nervous systems that detect external and internal signals, transmit and integrate information, and
More informationBIOLOGY 11/10/2016. Neurons, Synapses, and Signaling. Concept 48.1: Neuron organization and structure reflect function in information transfer
48 Neurons, Synapses, and Signaling CAMPBELL BIOLOGY TENTH EDITION Reece Urry Cain Wasserman Minorsky Jackson Lecture Presentation by Nicole Tunbridge and Kathleen Fitzpatrick Concept 48.1: Neuron organization
More informationBiological membranes and bioelectric phenomena
Lectures on Medical Biophysics Dept. Biophysics, Medical faculty, Masaryk University in Brno Biological membranes and bioelectric phenomena A part of this lecture was prepared on the basis of a presentation
More informationNeuron Func?on. Principles of Electricity. Defini?ons 2/6/15
Neuron Func?on 11 Fundamentals of the Nervous System and Nervous Tissue: Part B Neurons are highly Respond to adequate s?mulus by genera?ng an ac?on poten?al (nerve impulse) Impulse is always the regardless
More informationDYNAMICS 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 informationSupplementary 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 informationTransmission of Nerve Impulses (see Fig , p. 403)
How a nerve impulse works Transmission of Nerve Impulses (see Fig. 12.13, p. 403) 1. At Rest (Polarization) outside of neuron is positively charged compared to inside (sodium ions outside, chloride and
More information9.01 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 informationQuantitative 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 informationElectrophysiology 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 informationStructure 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 informationLecture 10 : Neuronal Dynamics. Eileen Nugent
Lecture 10 : Neuronal Dynamics Eileen Nugent Origin of the Cells Resting Membrane Potential: Nernst Equation, Donnan Equilbrium Action Potentials in the Nervous System Equivalent Electrical Circuits and
More informationMn 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 informationBIOELECTRIC PHENOMENA
Chapter 11 BIOELECTRIC PHENOMENA 11.3 NEURONS 11.3.1 Membrane Potentials Resting Potential by separation of charge due to the selective permeability of the membrane to ions From C v= Q, where v=60mv and
More informationBIOLOGY. 1. Overview of Neurons 11/3/2014. Neurons, Synapses, and Signaling. Communication in Neurons
CAMPBELL BIOLOGY TENTH EDITION 48 Reece Urry Cain Wasserman Minorsky Jackson Neurons, Synapses, and Signaling Lecture Presentation by Nicole Tunbridge and Kathleen Fitzpatrick 1. Overview of Neurons Communication
More informationFundamentals of the Nervous System and Nervous Tissue
Chapter 11 Part B Fundamentals of the Nervous System and Nervous Tissue Annie Leibovitz/Contact Press Images PowerPoint Lecture Slides prepared by Karen Dunbar Kareiva Ivy Tech Community College 11.4 Membrane
More informationSTUDIES 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 informationMembrane 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 informationThree 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 informationMEMBRANE STRUCTURE. Lecture 9. Biology Department Concordia University. Dr. S. Azam BIOL 266/
MEMBRANE STRUCTURE Lecture 9 BIOL 266/4 2014-15 Dr. S. Azam Biology Department Concordia University RED BLOOD CELL MEMBRANE PROTEINS The Dynamic Nature of the Plasma Membrane SEM of human erythrocytes
More informationQuantitative 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 informationNervous System Organization
The Nervous System Nervous System Organization Receptors respond to stimuli Sensory receptors detect the stimulus Motor effectors respond to stimulus Nervous system divisions Central nervous system Command
More informationNeurons, Synapses, and Signaling
Chapter 48 Neurons, Synapses, and Signaling PowerPoint Lecture Presentations for Biology Eighth Edition Neil Campbell and Jane Reece Lectures by Chris Romero, updated by Erin Barley with contributions
More informationSimulation 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 informationfor these experiments since the inward rectifying channel is absent and Centro de Investigacion del IPN, Mecico (Received 29 April 1975)
J. Physiol. (1976), 255, pp. 435-448 435 With 8 text-figure8 Printed in Great Britain POTASSIUM AND CALCIUM CONDUCTANCE IN SLOW MUSCLE FIBRES OF THE TOAD BY E. STEFAN1* AND 0. D. UCHITEL From the Instituto
More informationIntroduction 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 informationNeurons and Nervous Systems
34 Neurons and Nervous Systems Concept 34.1 Nervous Systems Consist of Neurons and Glia Nervous systems have two categories of cells: Neurons, or nerve cells, are excitable they generate and transmit electrical
More informationCOGNITIVE 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 informationPROPERTY OF ELSEVIER SAMPLE CONTENT - NOT FINAL
CHAPTER 5 Membrane Potentials and Action Potentials UNIT II Electrical potentials exist across the membranes of virtually all cells of the body. In addition, some cells, such as nerve and muscle cells,
More information