Titlebook: Electrogenesis of Biopotentials in the Cardiovascular System; In the Cardiovascula Nicholas Sperelakis Book 1995 Springer Science+Business

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https://doi.org/10.1007/978-3-658-23845-2orce and the electrical force. Because the electrical force is the PD across the cell membrane (.), the net driving force for any ionic species then is equal to (.-.). The driving forces for Na., Ca., and K. are illustrated in Figure VII-1 for a cardiac muscle cell having a resting potential of ?80

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Religion in der US-amerikanischen Politiks for K. (.) and Na. (.) are about ?94 mV and +60 mV, respectively (although some estimates of . go as high as +130 mV). The resting potential value is usually near ., because the K. permeability (.) is much greater than . in a resting membrane. The exact resting membrane potential (.) depends on th

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Birgit Verworn,Bernhard Hausberge (Fig. XII-1B). The max ./. is usually close to its maximal value at the normal resting potential (about ?80 mV for myocardial cells) but decreases markedly with small depolarizations, as shown in the figure. The max ./. goes to zero at about ?50 mV; i. e., membrane excitability is lost. The reason

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