Bound charges - PowerPoint PPT Presentation

Capacitance

Capacitance. b. a. L. Capacity to store charge C = Q/V. Q = L l E = l/2pe 0 r V = -( l /2 pe 0 )ln(r/a) C = 2 pe 0 L/ln(b/a). Dimension e 0 x L (F/m) x m. Capacitance. Capacity to store charge C = Q/V. Q = A r s E = r s /e 0 V = Ed C = e 0 A/d. A. d. (F/m) x m.

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Chapter 9. Magnetic Forces, Materials, and Inductance

Chapter 9. Magnetic Forces, Materials, and Inductance. Forces on a Moving Charge The electric field effects an energy transfer between electrical field and partical The acceleration vector by the magnetic field is always normal to the velocity vector

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How do fields create dipoles?

How do fields create dipoles?. E. -. +. Charges are not free to move in a dielectric! But electrons can be driven by E a bit away from the Nucleus without completely leaving it, creating an excess Charge on one side and a deficit on the other, ....

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