Engineering Electromagnetics
Engineering Electromagnetics
9th Edition
ISBN: 9780078028151
Author: Hayt, William H. (william Hart), Jr, BUCK, John A.
Publisher: Mcgraw-hill Education,
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Chapter 4, Problem 4.26P

Let us assume that we have a very thin, square, imperfectly conducting plate 2 m on a side, located in the plane z = 0 with one corner at the origin such that it lies entirely within the first quadrant. The potential at any point in the plate is given as V= -e-x sin y. (a) An electron enters the plate at x = 0, y = đ�œ‹/3 with zero initial velocity, in what direction is its initial movement? (b) Because of collisions with the particles in the plate, the electron achieves a relatively low velocity and little acceleration (the work, that the field does on it is converted largely into heat). The electron therefore moves approximately along a streamline. Where does it leave the plate and in what direction is it moving at the time?

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Two parallel plates are positioned 5.00 cm apart with 3.00 x104 volts across them. The positive plate is at x = -2.50 cm and the negative plate is at x = +2.50 cm. (Assume negative is to the left and positive is to the right.) A point charge of 2.50 x106 C and 2.61 x10 14 kg is released from rest at x = 0.00 m. The electric potential where the point charge is released from is V. The point charge will be accelerated to the (left/right) When the point charge reaches the plate, it will have a kinetic energy of J, or eV. This means the point charge will be traveling at m-s1 when it hits the plate.
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