Chapter 5 - Conservation of Charge
OVERVIEW
Conservation of charge is the focus of Chapter 5.� The challenge problem is neuroprosthetic
devices;� worked example problems include
a transistor sensor that converts a chemical signal to an electrical signal and
modeling a neuron.� Kirchhoff�s Current
Law is the reduction of the conservation of rate of charge for a steady-state
system.� Classical examples in circuit
analysis are used to illustrate Kirchhoff�s Current Law.� Radioactive decay, acid and base dissociation,
and electrochemical reactions illustrate reacting systems.� The charging of a capacitor is given as an
example of a dynamic system.� The
electrical energy accounting statement is then developed.� The concept of resistance and Kirchhoff�s
Voltage Law are illustrated in several circuit examples.� Analogous sections to those described above
delineate examples of reacting systems and dynamic systems such as those
including inductors.�
EXAMPLE PROBLEMS
2.� Einthoven�s Triangle:� During an ECG, the potential of three limbs is taken relative to the average electric potential of the body.� The right arm has a potential of �0.15 mV, the left arm has a potential of +0.55 mV, and the potential of the left leg is +0.93 mV.� What is the magnitude and angle of deflection of the cardiac vector?
3.� Iodine-131, a radioactive isotope of iodine, is used to test thyroid function and treat thyroid disorders, such as hyperthyroidism or cancer.�
A.) The decay of 131I results in release of a beta particle and gamma radiation as well as a stable element.� What is this stable element? Write out the decay reaction of 131I.
B.) Given that the half-life of 131I is approximately 8 days, how much negative charge does 25 g of iodine lose as beta particles in 15 days as it decays? (A decay reaction may be modeled by the equation:
where k is the rate constant, t is time, [A] is the quantity of interest of substance A, [A]0 is the initial quantity of substance A.)
����������������������� Fig. 5.**
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The resistors represent the resistance through the ion channels to ion flow.� The voltage sources (batteries) represent the potential difference across the membrane caused by concentration gradients of each type of ion.
����������� Given this model of the cell membrane, derive an equation for the current across of the cell membrane, im, in terms of the capacitance, potential differences and resistances of the ions in the model, and the overall potential difference across the membrane.
[1] Modified from http://cancer.rutgers.edu/courses/neurobiology/material/membranepotential.pdf