University of Bristol, Bristol BS8 1TD

Size: px
Start display at page:

Download "University of Bristol, Bristol BS8 1TD"

Transcription

1 J. Physiol. (1976), 255, pp With 11 text-ft ure Prined in Great Britain THE EFFECT OF CARBON DIOXIDE ON THE INTRACELLULAR ph AND BUFFERING POWER OF SNAIL NEURONES BY R. C. THOMAS From the Department of Physiology, Medical School, University of Bristol, Bristol BS8 1TD (Received 18 August 1975) SUMMARY 1. Intracellular ph (phi) was measured using ph-sensitive glass microelectrodes. The effects on phi of CO2 applied externally and HCO3-, H+ and NH4+ injected iontophoretically, were investigated. 2. The transport numbers for iontophoretic injection into aqueous micro-droplets were found by potentiometric titration to be 0 3 for HCO3- and 0 94 for H+. 3. Exposure to Ringer, ph 7 5, equilibrated with 2-2 % CO2 caused a rapid, but only transient, fall in phi. Within 1 or 2 min phi began to return exponentially to normal, with a time constant of about 5 min. 4. When external CO2 was removed, phi rapidly increased, and then slowly returned to normal. The phi changes with CO2 application or removal gave a calculated intracellular buffer value of about 30 m-equiv H+/pH unit per litre. 5. Injection of HCO3- caused a rise in phi very similar to that seen on removal of external CO2. 6. The phi responses to CO2 application, CO2 removal and HCO3- injection were slowed by the carbonic anhydrase inhibitor acetazolamide. 7. H+ injection caused a transient fall i phi. In CO2 Ringer ph1 fell less and recovered faster than in C02-free Ringer. Calculation of the internal buffer value from the phi responses to H+ and HCO3- injection gave very similar values. 8. The internal buffer value (measured by H+ injection) was greatly increased by exposure to CO2 Ringer. Acetazolamide reduced this effect of CO2, suggesting that the function of intracellular carbonic anhydrase may be to maximize the internal buffering power in CO2. 9. It was concluded that the internal HCO3- was determined primarily by the CO2 level and phi, that internal HC03- made a large contribution to the buffering power, and that after internal acidification phi was

2 716 R. C. THOMAS restored to normal by active transport of H+, OH- or HC03- across the cell membrane. The active transport was much faster in C02 than in C02- free Ringer. INTRODUCTION It is now established that H+ ions are not passively distributed across nerve cell membranes, but little is known about the way that intracellular ph (ph,) is regulated. A constant phi is desirable because of the high chemical reactivity of the H+ ion, especially with substances such as proteins. The two most important factors in the control of phi are the active transport of H+ (or OH- or HCO3-) ions across the cell membrane and the intracellular buffering power. (The buffering power or buffer value of a solution is a measure of its ability to resist ph changes in response to added acid or base. The higher the buffer value the less will the ph change.) The intracellular buffering power will determine the immediate ph1 response to the addition of acid or base, while active transport will determine the longer-term response (see Woodbury, 1965). Carbon dioxide may be related to phi in two ways, directly and indirectly. Directly, through its effect on carbonic acid, and indirectly through its possible role in intracellular buffering. In solution, C02 readily crosses cell membranes (Jacobs, 1940) so that an alteration in extracellular C02 will rapidly alter internal C02. In the absence of carbonic anhydrase, the alteration in internal C02 will then slowly change internal H2CO3 and hence ph1 and internal HCO3-. If snail neurones do contain carbonic anhydrase, then the ph1 change will be faster. The size of the phi change will be related to, and may be used to estimate, the intracellular buffering power. It is well known that extracellularly the C02-bicarbonate system is an important physiological buffer. Intracellularly, however, its role is uncertain, but it could be very important in conditions in which the external C02 is constant, especially if the internal HC03- concentration is determined principally by the C02 and ph1 (as shown in skeletal muscle by Khuri, Bogharian & Agulian, 1974). If C02 is able to cross the cell membrane and react with water sufficiently rapidly, the internal H2CO3 level will be fixed by the external C02. In this situation, internal HC03- will have four times the normal molar buffer value (see Woodbury, 1965) and could well contribute over half the total intracellular buffering power. Intracellular buffer values at constant external C02 levels have not been measured previously, so the extent to which HC03- may contribute is unknown. In an earlier study of the phi of snail neurones (Thomas, 1974a) the

3 C02 AND INTRACELLULAR ph 717 snail Ringer used had a normal ph of 8-0. This ph was too alkaline for stable C02-bicarbonate solutions, and in fact Burton (1969) has found that the blood of aestivating snails has a ph of about 7 5, and a bicarbonate level close to 20 mm. In the present experiments the ph of the Ringer was therefore changed to 7-5, so that it has been possible to investigate the effects of C02 at a constant extracellular ph. The internal buffering power was measured both by changing the external C02 and by iontophoretic injection of KHCO3 and HCl. The transport numbers for KHCO3 and HCl iontophoresis were therefore determined, using a specially developed microtitration method. The results show that the cell membrane must contain a H+-pump, or its equivalent, which can be very active, especially when the cell is in CObicarbonate Ringer. When exposed to C02, the cell accumulates HCO3- ions and the buffering power is greatly increased. Acetazolamide, an inhibitor of carbonic anhydrase, slows down the phi responses to C02 addition or removal, and reduces the internal buffer value in cells exposed to CO2. Preliminary reports of some of this work have been published (Thomas, 1974b, 1975c). METHODS These were generally the same as previously described (Thomas, 1974a) except that the ph of the normal snail Ringer was changed from 8-0 to 7-5. Details will be given only where they differ from the earlier descriptions. General. Most of the experiments were done on the large nerve cell 1 of Helix aspersa (Neild & Thomas, 1974) located at the rear of the right pallial ganglion. Special care was taken to expose the cell as completely as possible. At least 1 hr was allowed for the preparation to equilibrate before the experiment, with about half of this time being allowed for electrode equilibration outside the cell. The cell diameter was measured at two angles using an eyepiece micrometer in the dissecting microscope, magnification 80 x. The ph-sensitive micro-electrode was inserted first, then the reference (or membrane potential) micro-electrode, and finally the current-passing electrodes, if required. The ph electrode was inserted perpendicularly, but the other electrodes were usually inserted sideways, that is each electrode was lowered vertically, to make a small dimple in the cell surface, and then carefully moved horizontally until it suddenly penetrated the cell. It was then moved horizontally back to its original position. This technique, rather surprisingly, usually caused less damage than direct penetration. Results were rejected if, on removal from the cell, the voltage of the membranepotential or ph-sensitive electrode was more than 3 mv different from its value at the beginning of the experiment. In practice, the ph-sensitive electrodes were far more stable than the conventional micro-electrodes. Solutions. The normal (nominally C02-free) Ringer had a ph of 7-5, was in equilibrium with air, and had the following composition (in mm): KC1, 4; NaCl, 80; CaC12, 7; MgCl2, 5; Tris maleate or Na salt of HEPES, 2-N-2-hydroxyethyl piperaxine-n'-yl ethanesulphonic acid, 20. The CO2 Ringer solutions were saturated with 0-9, 2-2 or 4-4 % CO2 in 02, and had

4 718 R. C. THOMAS the same composition as the normal Ringer except that they contained NaHCO3 instead of Tris or HEPES, and contained 0 1 mm phosphate to prevent precipitation of bicarbonates (Burton, 1975). NaHCO3 was added as follows: 0 9 % Co2 had 8-4 mm; 2-2 % had 20mM; and 4-4% had 40 mm. The NaCl content was adjusted to keep the total NaCl + NaHCO3 to 100 mm. Conventional micro-electrodes. Potential-recording electrodes were filled first with distilled water, as previously described, and then with boiled 2-5 m-kc1, buffered to about ph 8-5 with 10 mm glycyl-glycine. Current-passing electrodes were filled directly with a 2 m solution of the required salt, and tested for their ability to carry a 100 na current in either direction. Electrode resistances were between 20 and 40 Mn. c ec HO Injection current dt (KHCO)Fl a e orkhco3 i. 10m n ph KCI~~~~~~~- (reference) Ag Droplet j6.5 Ag~~ 7Thait 7.5 UL 'LI L_...U A m la0 i- Droplet 10smm- Droplet 10 mm- HCO; diameter HCO- diameter HCO; 3.50 pm 290 pm Fig. 1. Interbarrel iontophoresis of KHCO.. A, diagram of the experimental arrangement for ph measurement during the injection of KHCO3 into an aqueous droplet mounted on a silver wire under liquid paraffin. B, penrecording of part of an experiment to measure KHCO3 output. The ph changes during KHCO injection into two droplets are shown: between each injection the ph and reference electrodes were placed in a droplet containing 10 mm-hc03e. The arrowheads indicate the point at which the KHCO3 micro-electrode was placed in the droplet: some leakage of KHCO3 then occurred before the current was switched on. ph-senlitive micro-electrodes. These were made as previously described, except that the exposed length of ph glass aimed at was about 25am, and the electrodes were filled and aged in one operation by gentle boiling in distilled water for 2-3 hr. The water was then sucked out and replaced with the final filling solution. (For a recent detailed account of the construction and properties of the recessed-tip ph-sensitive micro-electrode see Thomas, 1975b.) Electrical arrangements. These were the same as before. The circuit of the floating current clamp has now been published (Thomas 1975a). -wr Estimation of intracellular HCO3- concentration. Graphs of ph against HC03 constructed by titration. The ph of an initially HC03 -free CO2 Ringer solution,

5 CO2 AND INTRACELLULAR ph 719 bubbled with 0-9, 2-2 or 4-4% CO. in 0,, was followed while measured aliquots of solid NaHCO were added and dissolved. Intracellular HCO3- concentrations were than taken from these graphs. Measurement of transport numbers for HCO3- and H+ iontophoresi8. The quantity of HCl or KHCO, released by interbarrel iontophoresis was determined by titration, using an un-insulated ph-sensitive micro-electrode to follow changes in the ph of droplets of aqueous solution under liquid paraffin. The current-passing and reference micro-electrodes were the same as used for snail neurones; the arrangement is illustrated in Fig. 1A. Droplets mm in diameter were made on the ends of earthed PTFE-coated silver wires. The solution was ejected from siliconized micropipettes on to the wires by air pressure from a hand-operated syringe. Droplet diameters were measured by the method described above for snail neurones. For HCO3- determinations the experimental droplets contained 100 mm-kcl and 2 mm-nacl, and the reference droplets 100 mm-kcl and 10 mm-nahco. Since HCO,- solutions are only stable in the presence of a fixed level of CO, the liquid paraffin was continuously bubbled with 2-2% CO2 in 02. The titrations were done by measuring the ph of an experimental droplet while injecting HCO3- ions with a constant current, as shown in Fig. I B. The end-point was the ph equal to that of the reference droplets, which remained constant for many hr. In this way the charge required to inject HCO,- to a concentration of 10 mm into a droplet of known diameter was measured. For the H+ determinations the experimental droplets contained 100 mm-kcl and 20 mm-nahco3 or NaOH. The liquid paraffin was in equilibrium with air. The reference droplets contained citrate buffer, adjusted to ph 3-8, the ph of the titration end-point. Since there were only short periods between injections when the injection electrodes were in a droplet, no attempts were made to stop leakage from the electrodes by the use of backing-off currents. RESULTS Transport number for HCO3- and H+ iontophoresis If during an iontophoretic injection all the current flowing through a KHCO3-filled micro-electrode is carried by HCO3- ions leaving the electrode, and no other HC03- movement occurs, the transport number will be 1-0. The equivalents of HCO3- ejected will be given by the charge in coulombs divided by 96,500. If, however, some of the current is carried by cations entering the electrode, the transport number will be less than unity. The results obtained when HC03- or H+ was injected into aqueous droplets are shown in Fig. 2. The amount of HC03- determined from the ph change was much less than expected from the charge passed, if the transport number had been unity. The mean ratio of HCO3- calculated from the charge to that calculated from the titration was With HC1 iontophoresis, however, there was much better agreement between HCl calculated from the charge and from the titration: the mean ratio was Thus when calculating the quantity of HC03- or H+ injected into snail

6 720 R. C. THOMAS neurones in the experiments described below, the transport number for ECO3- was taken to be 0 3, and that for He to be The effect of 2*2 % C02 on the internal ph (Thomas, 1974a) C02 applied externally rapidly de- As shown earlier creases the ph, of snail neurones. This occurs through the well-known reaction inside the cell: C02 + H2O=H2CO3=H+ + HCO3-. The H+ produced intracellularly is, of course, the direct cause of the fall in ph. In these earlier experiments the normal Ringer ph 8-0 was too high to enable significant levels of C02 to be applied without changing the external ph. In the present experiments, however, it was possible to make, stable solutions in equilibrium with C02 levels up to 4-4% at the normal ph of o 600 HCI 0 -w Calculated from charge (p-equiv) Fig. 2. Relationship between calculated and measured quantities of HC1 or KHCOO injected iontophoretically from three different HCI-filled and five different KHCO3-filled micro-electrodes into aqueous droplets. Vertical axis shows the quantity found by titration, horizontal axis shows that calculated from the charge, assuming a transport number of one. The continuous line has a slope of 1P0, the dashed line a slope of 0*3. A complete, although unusually brief experiment, in which 2-2 % C02 was applied for 18 min and then for three short periods is shown in Fig. 3. The record starts with both electrodes outside the cell. Then the ph-

7 C02 AND INTRACELLULAR ph 721 sensitive micro-electrode was inserted. Inside the cell it recorded the sum of the membrane potential and the equilibrium potential for H+ ions, giving a negative deflexion of about 20 mv. Next the reference microelectrode was inserted into the same cell. This caused a deflexion of about 40 mv downwards on the upper trace, and a similar simultaneous upward deflexion of the lower trace as the membrane potential was subtracted from the ph-electrode output. From this point the ph trace had no membrane potential component. 10 > 20 E E Em min p I 8 0l-02-2 % CO2, U 1 I U U ph 6-S ph 7 5 CO2 CO2 CO2 Fig. 3. Pen-recording of an experiment to measure the effects of C02 application and removal on the internal ph, phi, of a snail neurone. The voltage recorded by the KCl-filled membrane potential electrode (Em) is shown at the top, and the voltage recorded by the ph-sensitive microelectrode is shown at the bottom. Except where indicated in this and later Figs., the preparation was superfused by a nominally C02-free Ringer of ph 7.5. The long time constant of the pen-recorder has reduced the size of the spontaneously-occurring action potentials to only a few mv. At the beginning and end of the record illustrated, both micro-electrodes were outside the cell. The ph response was checked at the end of the experiment. The initial ph1 was 7-2. It slowly rose until, about 12 min after the begging of the experiment, the solution flowing through the bath was changed from normal snail Ringer, ph 7-5, to one equilibrated with 2-2 % C02 at the same ph. As the C02 reached the cell, phi fell rapidly by a total of 0-17 units. But this fall was only transient; within 2 min ph1 began to increase towards a higher value than before the CO2 application. A similar increase in ph during a long exposure to C02 has recently been observed in squid giant axons (Boron & de Weer, 1975) and crab muscle fibres (Aickin & Thomas, 1975), but the time course of the phi changes

8 722 R. C. THOMAS was very much slower. In the experiment illustrated in Fig. 3 the ph, increase was roughly exponential, with a time constant of about 2-9 mi, although this was unusually fast (cf. Figs. 4, 5, 6, 7 and 11). The membrane potential was also increased during the exposure to C02, but without any initial fall. The high permeability of the cell membrane to C02, as shown by the rapid phi responses, suggests that after some time in C02 Ringer the internal C02 would be virtually the same as the external C02. The speed of the phi response to C02 also suggests that the internal HCO3- concentration would be determined primarily by phi and the C02 level. Assuming that the relevant equilibrium constants are the same inside and outside the cell, the internal HCO3- concentration after 15 min in C02 was about 15 mm, the internal ph being When the solution was changed back to the normal C02-free Ringer, phi rapidly increased, reaching a peak value of 7-84 within 2 min. Presumably, removal of external C02 caused C02 to leave the cell interior, and upset the equilibrium between internal C02 and HC03-. Thus internal HCO3- took up H+ ions (causing the increase in ph1) and left the cell as C02. Three further applications of C02 were made before the end of the experiment. The lower the ph, at which the C02 was applied, the smaller the ph change observed. The first brief C02 application caused a ph decrease of 0-48 units, the second 0-36, and the third At the end of the experiment both electrodes were withdrawn from the cell and their response to ph 7-5 Ringer was tested. Buffering power. If HCO3-, H+ and OH- do not cross the cell membrane actively or passively, the size of the rapid ph, response to CO2 application will depend only on the initial ph, and buffering power. Intracellular hydration of CO2 will produce equal numbers of H+ and HCO3 ions. It can be assumed that when ph, stops decreasing, there will be an approximate equilibrium between the ph1 and the internal CO2 and HC03-. Thus the HC03- produced can be calculated from the minimum ph, reached in C02, assuming that the carbonic acid dissociation constant and C02 concentration are the same inside as outside the cell. The estimated internal buffering power is then the HCO3- produced divided by the ph change. For the first CO2 application shown in Fig. 3, the buffering power calculated in this way was 40-6 m-equiv H+/pH unit per litre, and for the other three applications it was 27-6, 25-0 and The effect of different levels of CO2 on the internal ph In most of the experiments described in this paper, C02 was applied at 2-2 % in 02, but some experiments were done with more or less C02, as illustrated in Fig. 4. It is clear that the higher the level of C02 the larger were the ph changes observed. In all three exposures to C02, the internal

9 CO2 AND INTRACELLULAR ph 723 acidification was only transient. During the period in C02, phi returned roughly exponentially towards the normal value of about 7 4, with time constants for the three CO2 levels of 4-6, 7-3 and 8-9 min respectively. E E 40 E ~~~~~ ~~~~~~~~~~30. min 7-0 ' % C2 2-2 % CO2 4.4 % CO2 Fig. 4. Pen-recording of part of an experiment to show the effects on the membrane potential, Ems and internal ph, phi, of exposures to 0-9, 2-2 and 4-4% Co2. The external ph was maintained at 7-5 throughout. Internal buffering power by extrapolation In estimating the buffering power from the results illustrated in Fig. 3, it was assumed that there was no movement of H+, OH- or HCO3- across the cell membrane. For any but the shortest of exposures to C02, this is clearly wrong; the transient nature of the phi changes during a long exposure to C02 suggests that there was active transport of H+, OH- or HC03-. Thus to obtain a more accurate estimate of the phi change on application or removal of C02, the ph trace was extrapolated on each side of the minimum or maximum point to give a sharp peak. This was done for all phi changes occurring at the beginning or end of long exposures to C02. The buffering powers calculated from the three C02 exposures shown in Fig. 4 were in reasonable agreement: for 0-9 % C02 they were 28-9 m- equiv H+/pH unit per litre for the C02 application and 25-3 for the C02 removal; for 2-2% they were 26-9 and 32-4; and for 4-4% they were 26-1 and Similar measurements were made with 2-2% C02 on fourteen cells. From fifteen applications of C02 the mean buffering power was (S.E. of mean) while from fifteen removals of C02 it was There have been few previous measurements of the intracellular buffer value of nerve cells, and none in which allowance has been made for active transport. Using the DMO technique to measure the phi of cat brain,

10 724 R. C. THOMAS Roos (1965) obtained a value for the internal buffering power of 36-7 m- equiv H+/pH unit per litre, but this may well be too high. With the snail neurones, if phi had been measured only before and perhaps 30 min after changing the external CO2, active transport would have made the buffer value appear very large indeed min > 20 - E_ w 40 _ m X 7 phi e vacetazolamide (10 #H) % CO2 22% CO2 Fig. 5. Pen-recording of part. of an experiment to show the effects of 10-6 m acetazolamide on the response to CO2 application and removal. The effect of acetazolamide on the response to C02 The speed of the response of phi to C02 application or removal suggests that the hydration of C02 and dehydration of H2CO3 was being catalysed by carbonic anhydrase. Perhaps the simplest way of testing this is to apply an inhibitor such as acetazolamide (Diamox; Lederle), well known to specifically block carbonic anhydrase activity. Fig. 5 shows that acetazolamide did indeed considerably slow the phi response to both C02 addition and removal. It appears to have little effect on the change in phi during C02, but greatly slows the return to normal after C02 removal. The slowing of the ph, increase following CO2 removal is somewhat surprising: the uncatalysed dehydration of H2CO3 is much faster than the reverse reaction (Woodbury, 1965). To check that acetazolamide was not reducing the membrane permeability to dissolved gases, the experiment shown in Fig. 6 was done. The result shows that the ph response to injected NH4+ ions was not changed by acetazolamide. The fall in ph following NH4+ injection is caused by the intracellular conversion of NH4+ to H+ and NH3, the latter then leaving the cell. The ph1 responses to both C02 removal and HC03- injection were considerably slowed. In some preliminary experiments communicated to the Physiological Society

11 CO2 AND INTRACELLULAR ph 725 (Thomas, 1974b) 1 used NH,+4 injections to measure the intracellular buffering power, with the assumption that the transport number was 10. Later, however, when making H+ and NH4+ injections into the same cell, I found that NH4+ gave a higher apparent buffering power than with H+ injection. Possibly the transport number for NH4+ is significantly lower than that for H+. I have found the ph of aqueous droplets containing NH4+ too unstable to allow me to measure the transport number for NH4+. 'E 20 l- _ > NH4HCO E 30 uj Injection current thco- I % CO ph >E 20 r E 30 _ Em Lu40.,..- _ 50 ] oo ph i o - 10-SM 2-2 % CO,. ph Fig. 6. Pen-recording of a complete experiment to compare the effects of acetazolamide on the response to C02 application and removal with the responses to NH4+ or HCO3- injection. The bottom half of the Fig. is a continuation of the top half. The two arrows above the top record indicate the points at which the two current-carrying micro-electrodes were inserted. In each half of the figure the first trace is the membrane potential, E., the second is the injection current, and the third is the internal ph, phi. Comparison of HCO3- injection and CO2 removal If the ph1 increase seen on removal of CO2 from outside a cell is caused by internal HCO3- taking up H+ ions and leaving the cell as C02, it should be possible to mimic the phi response by injecting HC03- ions. Fig. 7 illustrates an experiment in which three injections of HC03- were made, followed by a 20 min exposure to 2-2 % CO2. The results show that the

12 726 R. C. THOMAS more HCO3- is injected, the bigger is the rise in phi, and that the time courses of the responses are similar to those seen on removal of external C02. In making quantitative comparisons a major problem is the need to know the cell volume to calculate the HCO3- concentrations resulting from the injections. In this paper cell volumes have been estimated by measuring the apparent cell diameter and then calculating the volume of the equivalent sphere. When this is done, injected HCO3- appears to be 30 min 10 _ KHCO. electrode 5~ out E, 320 E Infection current (KHCOJ ph1 [18 6] C* 7.8 8* % C02, ph 7-5 Fig. 7. Pen-recording of part of an experiment to compare the effects of HCO3- injection with the effects of C02 removal. The arrow above the top trace indicates the point at which the KHCO3-filled micro-electrode was withdrawn from the cell to prevent any leakage of KHCO3 into the cell. Before that, leakage was minimized by the passage of a 5 na back-off current, in the reverse direction to that used for HCO3- injection. The numbers in square brackets are the calculated HCO3- concentrations. more effective than HC03- accumulated in C02. The results from a total of five experiments similar to that of Fig. 7 are plotted in Fig. 8. It is clear that injected HC03- always causes a larger phi change than would be expected from the apparently equivalent amount of HCO3- accumulated during exposure to C02. Thus the buffering power calculated from the sixteen HC03- injections was m-equiv H+/pH unit per litre, while that calculated from the seven responses to C02 removal was

13 CO2 AND INTTRACELLULAR ph * (The discrepancy between these values is considered fully in the Discussion.) Measurement of buffering power by HCl injection The most direct way of measuring the buffering power of a solution is to add acid or alkali and measure the ph change. So far I have been unable to inject KOH, but HC1 is one of the easiest compounds I have ever tried to inject iontophoretically. Thus I have used HC1 to measure the buffering power with and without CO2 outside the cell, the cell volume being estimated from the apparent cell diameter, as described above El*05 ~ /4 -/ El 0 o 00O4 0J 0 bo r U injection 03 Ca; removal / Calculated intracellular HCO-3 (mm) Fig. 8. The relationship between the intracellular ph change and internal HC03-: the HCO3- being either injected (circles) or accumulated during exposure to CO2 (triangles). The two lines are drawn to fit the average buffering power calculated from each set of points: 10-7 for the injections, and 30-7 for the C02 withdrawal. A transport number of 0-3 was used in calculating the quantity of HCO3- injected, and the cell contents were assumed to be essentially the same as the external environment, except for ph, in calculating the internal HCO3- in CO2. Buffering power in the absence of CO2 Fig. 9 shows the effect on phi of three equal injections of HCl, and also illustrates some of the procedures used and problems encountered. The ph-sensitive and KCl-filled reference micro-electrodes were inserted first. Next a second KCl-filled micro-electrode was inserted, causing little change in the internal ph but a transient fall in the membrane potential. Then the HCl-filled micro-electrode was pushed into the cell, causing

14 728 R. C. THOMAS another transient depolarization. As HCl began to leak out of the microelectrode into the cell, phi began to fall. Then a 5 na braking current was switched on between the two current-passing electrodes, and phi began to recover. 10 L ~20 E~ ~~~E -_ Injection current ph1 %% 7.3 II C.7.5 % min Fig. 9. Pen-recording of the beginning and end of an experiment to measure the intracellular buffering power by the injection of HCl. The two arrows indicate the points at which the two current-passing electrodes (filled with KCl and HCl) were inserted. The central portion of the experiment, about 110 min long, is not shown. (During this section the HC1 micro-electrode was removed and replaced with one of a higher resistance to reduce leakage, the cell was exposed to C02 and acetazolamide, and a total of four further injections of HCl were made.) The injection current was reversed 10 min later and increased to 35 na for 60 sec, and then returned to its previous value. If the cell had had no buffering capacity, this injection would have increased the internal H+ concentration by 5-75 mm (and ph, would have decreased by over 3 units): in fact ph, changed by 0-43 units, giving a buffering power of 13-4 m- equiv H+/pH unit per litre. The recovery of the ph after this injection was rather slow, suggesting that HCl was again leaking from the electrode, in spite of the 5 na braking current. Thus, in the part of the experiment not illustrated, the HCl micro-electrode was withdrawn and replaced with one having a higher resistance. In the last part of the experiment two more injections of HOl

15 C02 AND INTRACELLULAR ph 729 were made, giving calculated buffering powers of 15-0 and The three HOl injections covered the ph range , suggesting that the buffering power did not vary near the normal internal ph. (See also Fig. 5 of Thomas, 1975c.) For the last two injections one of the current-passing micro-electrodes was incompletely inserted, or partially blocked, so that the membrane potential was slightly affected by the injection current. This happened relatively infrequently, but when it did the only reliable remedy was replacement of the relevant micro-electrode. The normal lack of effect of the injection current on the membrane potential can be seen in Figs. 6, 7 and 11, and the earlier injections of Fig. 10. The mean calculated buffering power from eighteen HCl injections into seven cells in normal Ringer was '7, which agrees well with the figure of obtained from the HCO3- injections. The effect of C02 on the internal buffering power The molar buffering power of a bicarbonate solution in equilibrium with a fixed level of C02, and hence having a constant H2CO3 concentration, is 2x3. This is four times higher than that of a normal buffer (Woodbury, 1965). If C02 is able to cross the cell membrane sufficiently rapidly, the HCO3- accumulated intracellularly during exposure to CO2 should greatly increase the cell's buffering power. If the internal buffer value in C02-free Ringer was 30, it would be more than doubled in C02 Ringer if the internal HCO3- was 15 mm. Fig. 10 shows the effects of HCl injection into a cell during and after exposure to C02. The buffering power was much higher in the 2-2 % C02 Ringer than in the nominally C02-free Ringer. For example, the second and fifth injections were of the same quantity of HCl; phi changed by 021 units in C02 Ringer, but by 0 57 units in normal Ringer. For a total of fourteen HOl injections into seven cells exposed for some time to 2-2 % C02 Ringer the average buffering power was 31' , while for the same cells in C02-free Ringer it was only The recovery of the ph after an HCl injection was faster in C02 Ringer than in normal Ringer. In the normal Ringer the recovery time constant was about 12 min, but for C02 Ringer it was only about 5 min (calculated from the experiment shown in Fig. 10). The effect of acetazolamide If rapid dehydration of H2CO3 is essential to enable C02 to reduce the ph response to injected acid, carbonic anhydrase inhibition should reduce

16 730 R. C. THOMAS the effectiveness of C02. Fig. 11 shows that acetazolamide treatment does lower the internal buffering power from its high value in C02 Ringer. (The transient increase in phi when the acetazolamide was applied was probably due to loss of C02 by the solution in the tubing.) min I.., 30 EM< 76 (24r7r(270 ecio (32.3) 80 22%CO2. ph75 Fig. 10. Pen-recording of part of an experiment to show the effect of CO2 on 10-2the internal buffering power. Between the first and second injections of HCl the H~l-ifilled micro-electrode was moved so that its tip was less close to the ph-sensitive electrode. The numbers in parentheses under the ph record are the calculated buffering powers for each injection. 10 r 30 min E 20 E > ;~ ~ Injection current (HCI) 307m3 0 ecf 80 Fig. 11. Pen-recording of part of an experiment to show the effect on the intracellular buffering power of 002 and 002 plus acetazolamide. The numbers in parentheses under the ph record are the calculated buffering powers for ech injection.

17 CO2 AND INTRACELLULAR ph7 731 For three cells treated with acetazolamide the buffering power in C02 fell from 34-6 m-equiv H+/pH unit per litre to a mean of Acetazolamide had no effect on the buffering power in C02-free Ringer. TABLE 1. Intracellular buffering power of snail neurones (m-equiv H+/pH unit per litre) External solution CO2 + C02-free 2.2 %CO2 acetazolamide Method used (m-equiv) (m-equiv) (m-equiv) Application of 2-2 % CO Application of 0 9 % CO Removal of 2.2 % CO2 28-9±1 0 Removal of 0 9 % CO KHCO3 injection, volume not 10-7 ± corrected* HCl injection, volume not 10-9 ± ± corrected* HCl injection, volume (29 5) correctedt Results are shown as mean + s.e. of mean. * Volume of the cell assumed to be the same as that of a sphere of the same diameter as the cell. v t Volume corrected by assuming true internal buffering power is DISCUSSION Perhaps the most interesting conclusions to be drawn from the above results concern the part played by carbonic anhydrase in increasing the internal buffer value in C02, and the high activity of the 'H+-pump' (a convenient term for H+, OH- or HCO3- active transport across the cell membrane) especially in C02-Ringer. Before discussing these points, however, I will consider the large difference between buffer values as measured by C02 application and by HOl injection, and the accumulation of HCO3- by cells exposed to C02. The various values for internal buffering power are collected together in Table 1. The internal buffering power from CO2 application or removal As mentioned in the Results section, the accuracy of the estimation of the buffering power by the C02 method depends on the following assumptions: the C02 levels and H2CO3 dissociation constant were the same inside and outside the cell; before and soon after a period of exposure to C02 the

18 732 R. C. THOMAS internal C02 and thus the internal HCOG3- were negligible; there was no significant passive entry or exit of HC03- ions; and active transport of H+, OH- or HCO3- ions could be allowed for by extrapolation of the phi trace. The first three assumptions seem reasonable, so that the only likely source of error is the allowance made for the H+-pump. The time course of the recovery of phi after displacement from normal appears to be exponential, at least for ph, decreases. Thus linear extrapolation will tend to underestimate the phi change, and, in the case of C02 addition, over-estimate the HCO3- produced. These errors will both cause overestimation of the internal buffer value. The over-estimation is unlikely to be large, however; errors of extrapolation will be smaller with small ph changes, and the buffering powers calculated from the ph changes with 0 9 % C02 are not much less than with 2 2 % CO2. For C02 applications the average value for 0 9 % C02 was 27*1 m-equiv H+/pH unit per litre, as against 30-1 for 2-2 0C02, and for C02 removal the value for 0-9 % C02 was 24-7 as against It is perhaps worth noting that in earlier experiments when the external C02 and ph were changed simultaneously, and there was no need for extrapolation, the internal buffering power was estimated to be at least 25 (Thomas, 1974a). Internal buffering power from HCl injection There is a large difference between the buffering power measured by C02 and measured by iontophoretic injection. The simplest explanation for this is that the intracellular volume is much smaller than that of a sphere having the same apparent diameter as the cell. A large fraction of the sphere volume is probably, by analogy with Aplysia neurones, occupied by extracellular space in membrane infoldings (Coggeshall, 1967) and many subcellular organelles are likely to be relatively impermeable to H+ or other ions. If the buffer value of the contents of the 'HCl accessible space' is that given by the responses to C02, then its volume can be estimated by multiplying the sphere volume by a correction factor. This correction factor will be the ratio of buffer value measured by injection to that measured by C02. Taking the latter figure as 29-5, the mean correction factor is Thus the HCl accessible space is on average only 36% of the volume of a sphere of the same diameter as the cell. If this average correction factor is used to correct the buffer values determined by HCl injection into cells in 2-2 % C02, the very high value of 86 is obtained. Such a high buffer value cannot be accounted for even if all the accumulated HCO3- makes its maximum possible contribution, which would give at most a mean internal buffer value of Presumably, because C02 can readily cross the membrane of subcellular

19 C02 AND INTRACELLULAR ph 733 organelles (cf. Elder & Lehlninger, 1973), the effective intracellular volume will be larger in C02. It seems probable, then, that CO2 increases the internal buffering power not only by enabling internal HC03- in the HCl-accessible space to make a large contribution, but also by enabling the buffers inside subcellular organelles to participate. The internal HCO3- in a cell exposed to C(2 Cell membranes are highly permeable to C02, so that, except when it is being taken up or released very rapidly, the internal and external CO2 levels will be the same. The speed of the initial response of the snail neurone phi to CO2 addition or removal shows that internal CO2 is rapidly hydrated or dehydrated, so that the internal HCO3- concentration will be determined simply by phi and the internal CO2. (The bicarbonate equilibrium potential will be the same as that for H+ ions, so that any net passive movement of HC03- ions across the cell membrane will be outwards. Such movements are unlikely to be large enough to reduce internal HCO3- concentration significantly.) If the HC03- accumulated by a cell in C02 is estimated by comparing the ph1 changes seen with C02 removal with those caused by HC03- injection, the values obtained are much lower than estimated from the phi and external CO2. But the internal buffering power determined by KHCO3 injection is very similar to that determined by HCl, so the internal space accessible to injected KHCO3 is probably the same as the HCl assessible space. Correcting for this gives good agreement between the two ways of estimating internal HC03- concentration. Thus in snail neurones, as well as in frog and rat skeletal muscle (Khuri et al. 1974) the internal bicarbonate is determined by the CO2 and phi, not the membrane potential and the external HC03-. The role of intracellulakr carbonic anhydrase Since acetazolamide decreases the buffering power measured by HCl injection into cells exposed to C02, carbonic anhydrase activity must be required to enable C02 and intracellular HC03- to contribute fully. The rapidity of the ph, responses to C02 addition and removal also appears to depend on carbonic anhydrase, but it is hard to see any physiological advantage in this. The function of intracellular carbonic anhydrase in many cells is unknown (Carter, 1972): perhaps its primary role, at least in nerve cells, is to maximize internal buffering in cells exposed to a constant level of C PHY 255

20 734 R. C. THOMAS Activity of the H+-pump One of the more striking aspects of the response of phi to CO2 application is the speed at which phi recovers from the initial fall. There must be some active process involved in this ph change: the extrusion of H+ ions, or uptake of OH- ions, or uptake of HCO3- ions would all be against their electrochemical gradients. In the experiment shown in Fig. 3, phi had recovered to 7-36 after 10 min in C02, and the cell should have accumulated over 14 mm internal HCO3-. Thus the H+-pump must have effectively extruded at least an equivalent number of H+ ions in increasing phi to this value. That the H+ ions must have been extruded rather than sequestered is perhaps clearer from the HCl injection experiments. Considerable quantities of HCl could be injected repeatedly into the same cell, and phi always recovered, as shown in Figs. 9, 10 and 11. The HCl experiments also show clearly that the H+-pump is much more active in CO2 Ringer than in C02-free; not only does phi recover more rapidly, but the higher buffering power in CO2 means that more H+ ions must be extruded for a similar phi change. It would be fruitless to speculate much at this stage on the mechanism of the H+-pump. There is a striking similarity, however, between the ph1 responses to HCl injection and the intracellular Na+ concentration, [Na+]i, responses to Na+ injection (see Fig. 12 of Thomas, 1972). The time courses of the exponential recoveries of ph1 or [Na+]i after an injection are very similar, with time constants of around 5 min. These points suggest that the H+-pump may work in much the same way as the Na+-pump. Finally, it is worth pointing out that the snail neurones as well as having a higher buffering power, were less susceptible to damage when in the CO2 Ringer. This suggests that for Ringer solutions C02-bicarbonate buffers are physiologically the best. Note added in proof. W. F. Boron & P. de Weer (J. gen. Phy8iol., in the press) have shown that the increase in ph, in squid axon during a long exposure to CO2 must be due to a H+ pump or its equivalent. More recentiy (Nature, Lond. in the press) they have also found that this H+ pump is stimulated by CO2 and HCO3. I wish to thank Mrs Vicky Martin for technical assistance, Miss Lilian Patterson for analysing gas mixtures, and Miss Pat Cragg for lending un-insulated microelectrodes. I am grateful to Professor A. J. Buller and Dr C. C. Ashley for reading the manuscript, and to the Medical Research Council for money.

21 C02 AND INTRACELLULAR ph 735 REFERENCES AimN, C. C. & THOMAS, R. C. (1975). Micro-electrode measurement of the internal ph of crab muscle fibres. J. Physiol. 252, BORON, W. F. & DE WEER, P. (1975). Studies on the intracellular ph of squid giant axons. Biophy8. J. 15, 42a. BURTON, R. F. (1969). Buffers in the blood of the snail, Helix pomatia L. Comp. Biochem. Phyesol. 29, BURTON, R. F. (1975). Ringer Solutionm and Phytiological Salines8, p. 48. Bristol: Scientechnica. CARTER, M. J. (1972). Carbonic anhydrase: isoenzymes properties, distribution, and functional significance. Biol. Rev. 47, COGGESHALL, R. E. (1967). A light and electron microscope study of the abdominal ganglion of Aply8ia californica. J. Neurophy8iol. 30, ELDER, J. A. & LEHINGER, A. L. (1973). Energy-linked uptake of Ca2+ supported by CO: inhibition by diamox. In Mechanism8 in Bioenergetic8, ed. AzoNE, G. F., ERNsTER, L., PAPA, S., QUAGLIARIELLO, E. & SILIPRANDI, N., pp New York and London: Academic Press. JACOBS, M. H. (1940). Some aspects of cell permeability to weak electrolytes. Cold Spring Harb. Symp. quaint. Biol. 8, KHuRI, R. N., BOGHARIAN, K. K. & AGULIAN, S. K. (1974). Intracellular bicarbonate in single skeletal muscle fibres. Pfluger8 Arch. ge8. Physiol. 349, NEILD, T. 0. & THOMAS, R. C. (1974). Intracellular chloride activity and the effects of acetylcholine in snail neurones. J. Phyeiol. 242, Roos, A. (1965). Intracellular ph and intracellular buffering power of the cat brain. Am. J. Phyeiol. 209, THOMAS, R. C. (1972). Intracellular sodium activity and the sodium pump in snail neurones. J. Phyeiol. 220, THOMAS, R. C. (1974a). Intracellular ph of snail neurones measured with a new ph-sensitive glass micro-electrode. J. Phy-iol. 238, THOMAS, R. C. (1974b). The effect of bicarbonate on the intracellular buffering power of snail neurons. J. Physiol. 241, P. THOMAS, R. C. (1975a). A floating current clamp for intracellular injection of salts by interbarrel iontophoresis. J. Phyeiol. 245, 20-22P. THOMAS, R. C. (1975b). Construction and properties of recessed-tip micro-electrodes for Na+, ph and Cl-. In Proceeding8 of International Workshop on Ion-eelective Electrodes, Reisenburg, ed. KESSLER, M. Munich: Urban and Schwarzenberg (in the Press). THOMAS, R. C. (1975c). The effects of CO. and bicarbonate on the intracellular ph of snail neurones. In Proceedings of International Worskshop on Ion-seletive Electrodes, Reisenburg, ed. KESSLER, M. Munich: Urban and Schwarzenberg (in the Press). WOODBURY, J. W. (1965). Regulation of ph. In Physiology and Biophysic, ed. RUCH, T. C. & PATrON, H. D., pp Philadelphia and London: Saunders. 24-2

ph1 recovery from internal acidification investigated.

ph1 recovery from internal acidification investigated. J. Physiol. (1977), 273, pp. 317-338 317 With 12 text-figurem Printed in Great Britain THE ROLE OF BICARBONATE, CHLORIDE AND SODIUM IONS IN THE REGULATION OF INTRACELLULAR ph IN SNAIL NEURONES BY R. C.

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

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

[Na+]1, but K-free or 0'25 mm-k Ringer caused a rise in [Na+]1.

[Na+]1, but K-free or 0'25 mm-k Ringer caused a rise in [Na+]1. J. Phy8iol. (1972), 22, pp. 55-71 55 With 13 text-figurew Printed in Great Britain INTRACELLULAR SODIUM ACTIVITY AND THE SODIUM PUMP IN SNAIL NEURONES BY R. C. THOMAS From the Department of Physiology,

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

ph1 recovery following acidification. 90 % or complete removal of external micro-electrodes, fell on application of (NH4)2SO4 and increased

ph1 recovery following acidification. 90 % or complete removal of external micro-electrodes, fell on application of (NH4)2SO4 and increased J. Phy8iol. (1977), 273, pp. 295-316 295 With 12 text-figure Printed in Great Britain AN INVESTIGATION OF THE IONIC MECHANISM OF INTRACELLULAR ph REGULATION IN MOUSE SOLEUS MUSCLE FIBRES BY C. CLAIRE AICKIN

More information

phi decreased. (HEPES) and the rate at which weak bases, applied to the superfusate, were able to

phi decreased. (HEPES) and the rate at which weak bases, applied to the superfusate, were able to Journal of Physiology (1989), 409, pp. With 11 text-figures 103-120 103 Printed in Great Britain THE EFFECT OF EXTRACELLULAR WEAK ACIDS AND BASES ON THE INTRACELLULAR BUFFERING POWER OF SNAIL NEURONES

More information

ELECTROCHEMICAL PROPERTIES OF NA+- AND

ELECTROCHEMICAL PROPERTIES OF NA+- AND ELECTROCHEMICAL PROPERTIES OF NA+- AND K+-SELECTIVE GLASS MICROELECTRODES CHIN OK LEE, Department ofphysiology and Biophysics, Cornell University Medical College, New York 10021 U.S.A. ABSTRACT Electrochemical

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

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

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

10/16/17 ACIDS AND BASES, DEFINED WATER IS AMPHOTERIC OUTLINE. 9.1 Properties of Acids and Bases. 9.2 ph. 9.3 Buffers

10/16/17 ACIDS AND BASES, DEFINED WATER IS AMPHOTERIC OUTLINE. 9.1 Properties of Acids and Bases. 9.2 ph. 9.3 Buffers ACIDS AND BASES, DEFINED A hydrogen atom contains a proton and an electron, thus a hydrogen ion (H + ) is a proton: Acids: Proton (H + ) transfer between molecules is the basis of acid/base chemistry Ø

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

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

RATE OF ANTAGONISM OF TUBOCURARINE BY POTASSIUM IONS

RATE OF ANTAGONISM OF TUBOCURARINE BY POTASSIUM IONS Brit J Pharmacol (1961), 17, 11-16 RATE OF ANTAGONISM OF TUBOCURARINE BY POTASSIUM IONS BY R CREESE, D B TAYLOR AND B TILTON From the Department of Pharmacology, University of California Medical Center,

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

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

The Membrane Potential

The Membrane Potential The Membrane Potential Graphics are used with permission of: adam.com (http://www.adam.com/) Benjamin Cummings Publishing Co (http://www.aw.com/bc) ** It is suggested that you carefully label each ion

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

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

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

Draw one line from each solution to the ph value of the solution. Solution ph value of the solution

Draw one line from each solution to the ph value of the solution. Solution ph value of the solution 1 The ph scale is a measure of the acidity or alkalinity of a solution. (a) Draw one line from each solution to the ph value of the solution. Solution ph value of the solution 5 Acid 7 9 Neutral 11 13

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

BIOELECTRIC PHENOMENA

BIOELECTRIC 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 information

5.1 Module 1: Rates, Equilibrium and ph

5.1 Module 1: Rates, Equilibrium and ph 5.1 Module 1: Rates, Equilibrium and ph 5.1.1 How Fast? The rate of reaction is defined as the change in concentration of a substance in unit time Its usual unit is mol dm 3 s 1 When a graph of concentration

More information

STEIN IN-TERM EXAM -- BIOLOGY FEBRUARY 12, PAGE 1 of 7

STEIN IN-TERM EXAM -- BIOLOGY FEBRUARY 12, PAGE 1 of 7 STEIN IN-TERM EXAM -- BIOLOGY 3058 -- FEBRUARY 12, 2009 -- PAGE 1 of 7 There are 25 questions in this Biology 3058 exam. All questions are "A, B, C, D, E, F, G, H" questions worth one point each. There

More information

NEURONS, SENSE ORGANS, AND NERVOUS SYSTEMS CHAPTER 34

NEURONS, SENSE ORGANS, AND NERVOUS SYSTEMS CHAPTER 34 NEURONS, SENSE ORGANS, AND NERVOUS SYSTEMS CHAPTER 34 KEY CONCEPTS 34.1 Nervous Systems Are Composed of Neurons and Glial Cells 34.2 Neurons Generate Electric Signals by Controlling Ion Distributions 34.3

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

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

Stoichiometry. Percent composition Part / whole x 100 = %

Stoichiometry. Percent composition Part / whole x 100 = % Stoichiometry Conversion factors 1 mole = 6.02 x 10 23 atoms (element) 1 mole = 6.02 x 10 23 molecules (covalent compounds) 1 mole = 6.02 x 10 23 formula units (ionic compounds) 1 mole (any gas @ STP)

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

Electro Analytical Methods

Electro Analytical Methods CH 2252 Instrumental Methods of Analysis Unit II Electro Analytical Methods Dr. M. Subramanian Associate Professor Department of Chemical Engineering Sri Sivasubramaniya Nadar College of Engineering Kalavakkam

More information

Principles Of Acid-Base Balance

Principles Of Acid-Base Balance Principles Of Acid-Base Balance I. Introduction A. For normal body function the free H+ concentration [H+] or ph must be kept within a narrow normal range. Some reasons why: 1. The proton "pump" within

More information

BIOLOGY 101. CHAPTER 3: Water and Life: The Molecule that supports all Live

BIOLOGY 101. CHAPTER 3: Water and Life: The Molecule that supports all Live BIOLOGY 101 CHAPTER 3: Water and Life: The Molecule that supports all Live The Molecule that Supports all Life CONCEPTS: 3.1 Polar covalent bonds in water molecules result in hydrogen bonding 3.2 Four

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

BIOL Week 5. Nervous System II. The Membrane Potential. Question : Is the Equilibrium Potential a set number or can it change?

BIOL 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 information

The Membrane Potential

The Membrane Potential The Membrane Potential Graphics are used with permission of: Pearson Education Inc., publishing as Benjamin Cummings (http://www.aw-bc.com) ** It is suggested that you carefully label each ion channel

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

(pho) of 7-35 and at 22 'C.

(pho) of 7-35 and at 22 'C. J. Physiol. (1983), 345, pp. 175-187 175 With 6 text-figures Printed in Great Britain THE INTRACELLULAR ph OF FROG SKELETAL MUSCLE: ITS REGULATION IN ISOTONIC SOLUTIONS BY RONALD F. ABERCROMBIE*, ROBERT

More information

(Received 31 October 1962)

(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 information

Renal handling of substances. Dr.Charushila Rukadikar Assistance Professor Physiology

Renal handling of substances. Dr.Charushila Rukadikar Assistance Professor Physiology Renal handling of substances Dr.Charushila Rukadikar Assistance Professor Physiology GENERAL PRINCIPLES OF RENAL TUBULAR TRANSPORT Transport mechanisms across cell membrane 1) Passive transport i. Diffusion

More information

Water, water everywhere,; not a drop to drink. Consumption resulting from how environment inhabited Deforestation disrupts water cycle

Water, water everywhere,; not a drop to drink. Consumption resulting from how environment inhabited Deforestation disrupts water cycle Chapter 3 Water: The Matrix of Life Overview n n n Water, water everywhere,; not a drop to drink Only 3% of world s water is fresh How has this happened Consumption resulting from how environment inhabited

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

Full file at Chapter 2 Water: The Solvent for Biochemical Reactions

Full file at   Chapter 2 Water: The Solvent for Biochemical Reactions Chapter 2 Water: The Solvent for Biochemical Reactions SUMMARY Section 2.1 Summary Water is a polar molecule, with a partial negative charge on the oxygen and partial positive charges on the hydrogens.

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

Basic Chemistry. Chemistry Review. Bio 250: Anatomy & Physiology

Basic Chemistry. Chemistry Review. Bio 250: Anatomy & Physiology Basic Chemistry Bio 250: Anatomy & Physiology Chemistry Review It is going to be your responsibility to review the basic principles of chemistry you learned in BIO 101 This basic set of notes will help

More information

Nernst Equation and Equilibrium Potentials

Nernst Equation and Equilibrium Potentials CELLULAR AND AUTONOMIC PHYSIOLOGY 13 Case 3 Nernst Equation and Equilibrium Potentials This case will guide you through the principles underlying diffusion potentials and electrochemical equilibrium. veil

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

THALLIUM AND CESIUM IN MUSCLE CELLS COMPETE FOR THE ADSORPTION SITES NORMALLY OCCUPlED BY K+

THALLIUM AND CESIUM IN MUSCLE CELLS COMPETE FOR THE ADSORPTION SITES NORMALLY OCCUPlED BY K+ THALLIUM AND CESIUM IN MUSCLE CELLS COMPETE FOR THE ADSORPTION SITES NORMALLY OCCUPlED BY K+ GILBERT N. LING Department of Molecular Biology. Pennsylvania Hospital. Philadelphia, Pennsylvania 19107 Reprit~red

More information

Chapter-2 (Page 22-37) Physical and Chemical Properties of Water

Chapter-2 (Page 22-37) Physical and Chemical Properties of Water Chapter-2 (Page 22-37) Physical and Chemical Properties of Water Introduction About 70% of the mass of the human body is water. Water is central to biochemistry for the following reasons: 1- Biological

More information

Fundamentals of the Nervous System and Nervous Tissue

Fundamentals 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 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

Homework: 14, 16, 21, 23, 27, 29, 39, 43, 48, 49, 51, 53, 55, 57, 59, 67, 69, 71, 77, 81, 85, 91, 93, 97, 99, 104b, 105, 107

Homework: 14, 16, 21, 23, 27, 29, 39, 43, 48, 49, 51, 53, 55, 57, 59, 67, 69, 71, 77, 81, 85, 91, 93, 97, 99, 104b, 105, 107 Homework: 14, 16, 21, 23, 27, 29, 39, 43, 48, 49, 51, 53, 55, 57, 59, 67, 69, 71, 77, 81, 85, 91, 93, 97, 99, 104b, 105, 107 Chapter 15 Applications of Aqueous Equilibria (mainly acid/base & solubility)

More information

Experiment 8 - Double Displacement Reactions

Experiment 8 - Double Displacement Reactions Experiment 8 - Double Displacement Reactions A double displacement reaction involves two ionic compounds that are dissolved in water. In a double displacement reaction, it appears as though the ions are

More information

phi recovery must originate from an HCO3--independent acid-extrusion mechanism.

phi recovery must originate from an HCO3--independent acid-extrusion mechanism. J. Physiol. (1986), 374, pp. 137-151 137 With 8 text-figures Printed in Great Britain THE IONIC MECHANISM OF INTRACELLULAR ph REGULATION IN CRAYFISH MUSCLE FIBRES BY STEFAN GALLER* AND HANS MOSER From

More information

Name Date. 9. Which substance shows the least change in solubility (grams of solute) from 0 C to 100 C?

Name Date. 9. Which substance shows the least change in solubility (grams of solute) from 0 C to 100 C? Solubility Curve Practice Problems Directions: Use the graph to answer the questions below. Assume you will be using 100g of water unless otherwise stated. 1. How many grams of potassium chloride (KCl)

More information

Chapt. 12, Movement Across Membranes. Chapt. 12, Movement through lipid bilayer. Chapt. 12, Movement through lipid bilayer

Chapt. 12, Movement Across Membranes. Chapt. 12, Movement through lipid bilayer. Chapt. 12, Movement through lipid bilayer Chapt. 12, Movement Across Membranes Two ways substances can cross membranes Passing through the lipid bilayer Passing through the membrane as a result of specialized proteins 1 Chapt. 12, Movement through

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

III. Voltage Independence of Basolateral Membrane Na - Efflux

III. Voltage Independence of Basolateral Membrane Na - Efflux Na' and K+ Transport at Basolateral Membranes of Epithelial Cells III. Voltage Independence of Basolateral Membrane Na - Efflux THOMAS C. COX and SANDY I. HELMAN From the Department of Physiology and Biophysics,

More information

Buffers, Electrochemistry. Jan Pláteník & Tomáš Navrátil 2010/2011

Buffers, Electrochemistry. Jan Pláteník & Tomáš Navrátil 2010/2011 Buffers, Electrochemistry Practical Lesson on Medical Chemistry and Biochemistry General Medicine Jan Pláteník & Tomáš Navrátil 2010/2011 1 BUFFERS AND BUFFER CAPACITY 1.1 Principle of buffering: A buffer

More information

S4 CHEMISTRY SUMMARY NOTES

S4 CHEMISTRY SUMMARY NOTES S4 CHEMISTRY SUMMARY NOTES 1. The Mole One mole of a substance = GRAM FORMULA MASS e.g. H 2 SO 4 RAM from databook pg.7 2H 2 x 1 = 2 1S 1 x 32 = 32 4O 4 x 16 = 64 98g Mass = number of moles x Mass of 1

More information

لجنة الطب البشري رؤية تنير دروب تميزكم

لجنة الطب البشري رؤية تنير دروب تميزكم 1) Hyperpolarization phase of the action potential: a. is due to the opening of voltage-gated Cl channels. b. is due to prolonged opening of voltage-gated K + channels. c. is due to closure of the Na +

More information

Equilibri acido-base ed equilibri di solubilità. Capitolo 16

Equilibri acido-base ed equilibri di solubilità. Capitolo 16 Equilibri acido-base ed equilibri di solubilità Capitolo 16 The common ion effect is the shift in equilibrium caused by the addition of a compound having an ion in common with the dissolved substance.

More information

Basic Chemistry for Biology. Honors Biology

Basic Chemistry for Biology. Honors Biology Basic Chemistry for Biology Honors Biology 2013-2014 Composition of Matter Matter - Everything in universe is composed of matter Matter is anything that occupies space or has mass Mass quantity of matter

More information

Try this one Calculate the ph of a solution containing M nitrous acid (Ka = 4.5 E -4) and 0.10 M potassium nitrite.

Try this one Calculate the ph of a solution containing M nitrous acid (Ka = 4.5 E -4) and 0.10 M potassium nitrite. Chapter 17 Applying equilibrium 17.1 The Common Ion Effect When the salt with the anion of a is added to that acid, it reverses the dissociation of the acid. Lowers the of the acid. The same principle

More information

6 Mechanotransduction. rotation

6 Mechanotransduction. rotation rotation inflow outflow Figure 6.3: Circumferential and uniaxial flow devices applying shear stress to the cell culture. They are stimulated through a circumferential fluid flow generating by a rotating

More information

E09. Exp 09 - Solubility. Solubility. Using Q. Solubility Equilibrium. This Weeks Experiment. Factors Effecting Solubility.

E09. Exp 09 - Solubility. Solubility. Using Q. Solubility Equilibrium. This Weeks Experiment. Factors Effecting Solubility. E09 Exp 09 - Solubility Solubility Solvation The reaction coefficient Precipitating Insoluble Substances Comparing Q to Ksp Solubility Equilibrium Solubility Product, Ksp Relating Molar Solubility Factors

More information

2002NSC Human Physiology Semester Summary

2002NSC Human Physiology Semester Summary 2002NSC Human Physiology Semester Summary Griffith University, Nathan Campus Semester 1, 2014 Topics include: - Diffusion, Membranes & Action Potentials - Fundamentals of the Nervous System - Neuroanatomy

More information

Acids, Bases, Salts, Buffers

Acids, Bases, Salts, Buffers Acids, Bases, Salts, Buffers Acids, Bases, Salts, Buffers An acid is any solute that dissociates in a solution and releases hydrogen ions, thereby lowering ph Since a hydrogen ion consist solely of a proton,

More information

PRACTICAL 3 ph AND BUFFERS

PRACTICAL 3 ph AND BUFFERS PRACTICAL 3 ph AND BUFFERS ph and Buffers Structure 3.1 Introduction 3.2 ph and Buffers: Basic Concept 3.2.1 ph 3.2.2 Buffers and Buffer Solutions 3.3 Methods for Determining ph Experiment 1: Measurement

More information

Lab 8 Dynamic Soil Systems I: Soil ph and Liming

Lab 8 Dynamic Soil Systems I: Soil ph and Liming Lab 8 Dynamic Soil Systems I: Soil ph and Liming Objectives: To measure soil ph and observe conditions which change ph To distinguish between active acidity (soil solution ph) and exchangeable acidity

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

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

Chapter 10. Acids, Bases, and Salts

Chapter 10. Acids, Bases, and Salts Chapter 10 Acids, Bases, and Salts Topics we ll be looking at in this chapter Arrhenius theory of acids and bases Bronsted-Lowry acid-base theory Mono-, di- and tri-protic acids Strengths of acids and

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

AP CHEMISTRY 2009 SCORING GUIDELINES

AP CHEMISTRY 2009 SCORING GUIDELINES 2009 SCORING GUIDELINES Question 1 (10 points) Answer the following questions that relate to the chemistry of halogen oxoacids. (a) Use the information in the table below to answer part (a)(i). Acid HOCl

More information

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

Physiology 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 information

Chapter 02 The Basics of Life: Chemistry

Chapter 02 The Basics of Life: Chemistry Chapter 02 The Basics of Life: Chemistry Multiple Choice Questions 1. An atom that has gained electrons is a A. reactant. B. negative ion. C. positive ion. D. compound ion. 2. An atom with twelve electrons,

More information

Ch 7 Chemical Reactions Study Guide Accelerated Chemistry SCANTRON

Ch 7 Chemical Reactions Study Guide Accelerated Chemistry SCANTRON Ch 7 Chemical Reactions Study Guide Accelerated Chemistry SCANTRON Name /80 TRUE/FALSE. Write 'T' if the statement is true and 'F' if the statement is false. Correct the False statments by changing the

More information

exposed to CO2 and C02/HCO3- solutions. During CO2 exposures phi was regulated

exposed to CO2 and C02/HCO3- solutions. During CO2 exposures phi was regulated J. Physiol. (1985), 362, pp. 23-38 23 With 9 text-figures Printed in Great Britain INTRACELLULAR ph REGULATION IN THE SENSORY NEURONE OF THE STRETCH RECEPTOR OF THE CRAYFISH (ASTACUS FLUVIATILIS) BY HANS

More information

Chapter 2 Cellular Homeostasis and Membrane Potential

Chapter 2 Cellular Homeostasis and Membrane Potential Chapter 2 Cellular Homeostasis and Membrane Potential 2.1 Membrane Structure and Composition The human cell can be considered to consist of a bag of fluid with a wall that separates the internal, or intracellular,

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

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

AP Chemistry. CHAPTER 17- Buffers and Ksp 17.1 The Common Ion Effect Buffered Solutions. Composition and Action of Buffered Solutions

AP Chemistry. CHAPTER 17- Buffers and Ksp 17.1 The Common Ion Effect Buffered Solutions. Composition and Action of Buffered Solutions AP Chemistry CHAPTER 17- Buffers and Ksp 17.1 The Common Ion Effect The dissociation of a weak electrolyte is decreased by the addition of a strong electrolyte that has an ion in common with the weak electrolyte.

More information

Hiroshi HASUO and Kyozo KoKETSU. Department of Physiology, Kurume University School of Medicine, Kurume, 830 Japan

Hiroshi HASUO and Kyozo KoKETSU. Department of Physiology, Kurume University School of Medicine, Kurume, 830 Japan Japanese Journal of Physiology, 35, 89-100, 1985 Potential Dependency of the Electrogenic Na+ in Bullfrog Atrial Muscles -pump Current Hiroshi HASUO and Kyozo KoKETSU Department of Physiology, Kurume University

More information

Acid-Base Equilibria and Solubility Equilibria Chapter 17

Acid-Base Equilibria and Solubility Equilibria Chapter 17 PowerPoint Lecture Presentation by J. David Robertson University of Missouri Acid-Base Equilibria and Solubility Equilibria Chapter 17 The common ion effect is the shift in equilibrium caused by the addition

More information

DOUBLE DISPLACEMENT REACTIONS. Double your pleasure, double your fun

DOUBLE DISPLACEMENT REACTIONS. Double your pleasure, double your fun DOUBLE DISPLACEMENT REACTIONS Double your pleasure, double your fun Industrial processes produce unwanted by-products. Dissolved toxic metal ions-copper, mercury, and cadmium-are common leftovers in the

More information

Chapter 9: Acids, Bases, and Salts

Chapter 9: Acids, Bases, and Salts Chapter 9: Acids, Bases, and Salts 1 ARRHENIUS ACID An Arrhenius acid is any substance that provides hydrogen ions, H +, when dissolved in water. ARRHENIUS BASE An Arrhenius base is any substance that

More information

Ch 8: Neurons: Cellular and Network Properties, Part 1

Ch 8: Neurons: Cellular and Network Properties, Part 1 Developed by John Gallagher, MS, DVM Ch 8: Neurons: Cellular and Network Properties, Part 1 Objectives: Describe the Cells of the NS Explain the creation and propagation of an electrical signal in a nerve

More information

CHEMISTRY Matter and Change

CHEMISTRY Matter and Change CHEMISTRY Matter and Change UNIT 18 Table Of Contents Section 18.1 Introduction to Acids and Bases Unit 18: Acids and Bases Section 18.2 Section 18.3 Section 18.4 Strengths of Acids and Bases Hydrogen

More information

Introduction to Physiology II: Control of Cell Volume and Membrane Potential

Introduction to Physiology II: Control of Cell Volume and Membrane Potential Introduction to Physiology II: Control of Cell Volume and Membrane Potential J. P. Keener Mathematics Department Math Physiology p.1/23 Basic Problem The cell is full of stuff: Proteins, ions, fats, etc.

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

Equation Writing for a Neutralization Reaction

Equation Writing for a Neutralization Reaction Equation Writing for a Neutralization Reaction An Acid-Base reaction is also called a Neutralization reaction because the acid (generates H + or H 3 O + ) and base (generates OH ) properties of the reactants

More information

Shifting Equilibrium. Section 2. Equilibrium shifts to relieve stress on the system. > Virginia standards. Main Idea. Changes in Pressure

Shifting Equilibrium. Section 2. Equilibrium shifts to relieve stress on the system. > Virginia standards. Main Idea. Changes in Pressure Section 2 Main Ideas Equilibrium shifts to relieve stress on the system. Some ionic reactions seem to go to completion. Common ions often produce precipitates. > Virginia standards CH.3.f The student will

More information

Chemistry 265 December Exam 2011 Smith-Palmer

Chemistry 265 December Exam 2011 Smith-Palmer 1 Chemistry 265 December Exam 2011 Smith-Palmer NAME: [1] 1. Define an anode [1] Define a cathode [2] What is the E o for the following reaction: Ag + + Cu Ag (s) + Cu 2+ Ag + + e - Ag (s) E o = 0.799

More information

CHEM134- Fall 2018 Dr. Al-Qaisi Chapter 4b: Chemical Quantities and Aqueous Rxns So far we ve used grams (mass), In lab: What about using volume in lab? Solution Concentration and Solution Stoichiometry

More information

Acid - Base Equilibria 3

Acid - Base Equilibria 3 Acid - Base Equilibria 3 Reading: Ch 15 sections 8 9 Ch 16 sections 1 7 * = important homework question Homework: Chapter 15: 97, 103, 107, Chapter 16: 29*, 33*, 35, 37*, 39*, 41, 43*, 49, 55, 57, 61,

More information

Νευροφυσιολογία και Αισθήσεις

Νευροφυσιολογία 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 information

Nervous Lecture Test Questions Set 2

Nervous 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 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