431 Gausss Law in the Presence of Dielectrics











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When we add in the concept of free charge, and then apply Gauss's Law, we uncover a new vector, D, that represents a useful quantity, the electric displacement. This makes solving certain classes of problems rather easy, skipping the part where we have to calculate the bound charge within a dielectric. • Next:    • 4.3.2 A Deceptive Parallel   • Previous:    • 4.2.3 The Field Inside a Dielectric   • Playlist:    • Introduction to Electrodynamics  

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