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Neurology Edited by Professor Emeritus Desire' Dubounet, IMUNE

Neurology Edited by Professor Emeritus Desire' Dubounet, IMUNE

Neurology Edited by Professor Emeritus Desire' Dubounet, IMUNE

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The distances between the poles of the dipoles of excitation and recoveryare expected to be different. By using a specific global area such as the wrists andankles the relative distance of each patient is the same.The dipole concept predicting the potential recorded with a monopolarelectrode is obviously very greatly simplified. We must use caution in extrapolatingit to all in vivo situations. It is extremely complex. Consider what might happen ifboth electrodes are in the environment of the active tissue (i.e., one electrode not ina region of zero potential). Realize that the in vivo environmental conductingmedium does not extend to infinity in all directions and is constituted <strong>by</strong>inhomogeneous tissue. Thus a relatively complex wave form, reflecting excitationand recovery, can be detected <strong>by</strong> extracellular electrodes. Accurate prediction ofthe wave form is impossible in many practical circumstances. But our theoriesgenerate an approximate "map" to guide us in our intervention.Extracellular Potentials Across the Membrane. There is no easy way torelate the action potential detected <strong>by</strong> an external monopolar electrode (i.e., onepaired with an indifferent electrode) to the transmembrane potential. No simple andconstant relationship can be attained since there are environmentalinhomogeneities of various kinds.If an irritable tissue in a volume conductor becomes active, there is a currentflow in the environment and a potential field results. A monopolar electrode detectsthe potential due to the flow of current through the resistance of the environmentalmaterial. The current surge starts the active region of the membrane, whichexperiences an excursion in potential. In the field theory (Lorente de Nù, 1947;Clark and Plonsey, 1968; Plonsey, 1969) and with the cable analog (Huxley andSt_mpfil, 1949; Tasaki, 1959; Clark and Plonsey, 1966) we show that themembrane current does not have the same wave form as the excursion intransmembrane potential. The mathematical analysis puts forward the case of acylindrical irritable tissue located in a uniform volume conductor, showed that themembrane current is proportional to the second derivative of the transmembranepotential.Membrane~ Current~ =~ d sup 2 over dT~ (Transmembrane~ Volt.)The cable analog for a long, cylindrical, irritable cell can be used to show thatthe external action potential detected <strong>by</strong> a near<strong>by</strong> monopolar electrode in theenvironmental volume conductor is proportional to the second derivative of thetransmembrane action potential. Allow the environment as a resistance having avalue rlˆ/unit length; similarly, the resistance per unit length of the cytoplasm isdesignated r2.During activity there is a current flow in the environment il, in the cytoplasm i2, andthrough the membrane im. If the currents are identified, along with the coordinatesystem in which x increase to the right. There is a decrement in current within andwithout the cell, and this decrement reflects the current im flowing through themembrane. Because of the current flow, at any point there are potentials17

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