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Chapter 3 Electric Potential - MIT

Chapter 3 Electric Potential Potential and Potential Electric Potential in a Uniform Electric Potential due to Point Potential Energy in a System of Continuous Charge Deriving Electric field from the Electric Gradient and Example : Uniformly Charged Example : Uniformly Charged Example : Uniformly Charged Example : Calculating Electric field from Electric Problem-Solving Strategy: Calculating Electric Solved Electric Potential Due to a System of Two Electric Dipole Electric Potential of an Charge Moving Near a Charged Conceptual Additional Three Work Done on Calculating E from Electric Potential of a Electric Calculating Electric field from the Electric Electric Potential and Electric Potential Electric field , Potential and 3-1 Electric Potential Potential and Potential Energy In the introductory mechanics course, we have seen that gravitational force from the Earth on a particle of mass m loca

equipotential line.” A more complete discussion of equipotential will be given in Section 3.5. AC→→B VB=VC r ∆=Uq∆V 3.3 Electric Potential due to Point Charges Next, let’s compute the potential difference between two points A and B due to a charge +Q. The electric field produced by Q is 2 0 E=(/Q4πεr)ˆ JG, where is a unit vector

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Transcription of Chapter 3 Electric Potential - MIT

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