PHYS 102 Chapter 23: Sears & Zemansky's University Physics with Modern Physics 14th Edition: Chapter 23 Notes
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When a charged particle moves in an electric field, the field exerts a force that can do work on the particle. This can be expressed in terms of electric potential energy. Electric potential energy depends on the position of the charged particle in the electric field. The difference in potential from one point to another is often called voltage. Wa b = (cid:1832) (cid:1856) (cid:3029)(cid:3028) = (cid:1832)(cid:1855)(cid:1856) (cid:3029)(cid:3028: work done by a force, dl is an infinitesimal displace(cid:373)e(cid:374)t alo(cid:374)g the pa(cid:396)ti(cid:272)le"s path a(cid:374)d is the angle between f and dl at each point along the path. If the force f is conservative, the work done by f can always be expressed interms of a potential energy u. Wa b = - u: where u is the change in potential energy. Ka + ua = kb + ub: total mechanical energy is conserved if only conservative forces do work.