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This chapter explores electric potential energy and the concept of electric potential. It discusses how electric potentials are defined and how they interact with point charges, emphasizing the superposition principle. Important concepts such as equipotential surfaces—which are crucial for understanding electric fields—and their relationship with electric field lines are thoroughly examined. The chapter also connects these principles to biomedical applications, including how electrical signals in neurons work, the significance of potential differences in the body, and techniques used in medical diagnostics like electrocardiograms and electroencephalograms.
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Chapter 19 Electric Potential Energy and the Electric Potential
q1 q2 q2 3) Point Charges If V = 0 at r = ∞, then V r q Superposition: potentials add as scalars
4) Equipotential surfaces • Definition Surface with constant potential e.g. For a point charge, equipotential surfaces are spheres
e.g. parallel plates E is uniform, and W = qEs, so equipotential surfaces are planes
c) Electric field direction and equipotential surfaces If W = 0, and E ≠ 0, then E is perpendicular to equipotential surfaces
Electric field lines Equipotential lines
d) Electric field as a potential gradient units: V/m = J/(Cm) = N/C
In general, Electric field points in the direction of maximum change of the potential
Resting state (selective permeability) 5) Biomedical examples a) Conduction of electrical signals in neurons V=-70mV
Stimulated cell Signal travels at ~ 50 m/s
b) Medical diagnostics - body is not an equipotential surface - Flow of Na+, K+, Cl- ions; potential differences ~ 30 - 500 µV - depend on stimuli and can form regular patterns