Force per Unit Length on a Half Part of an Infinite Charged Cylinder Consider an infinite charged cylinder with radius (r) in a vacuum. The charge is distributed uniformly inside the cylinder. The cylinder moves with velocity () parallel to its symmetrical axis. If the value of the electrical field on the surface is (Eo), find the force per unit length (f) applied by itself on a half part of it! (Hint: Use the Maxwell's Stress Tensor) E(R) = E, %3D R Figure 1: A moving infinite charged cylinder
Force per Unit Length on a Half Part of an Infinite Charged Cylinder Consider an infinite charged cylinder with radius (r) in a vacuum. The charge is distributed uniformly inside the cylinder. The cylinder moves with velocity () parallel to its symmetrical axis. If the value of the electrical field on the surface is (Eo), find the force per unit length (f) applied by itself on a half part of it! (Hint: Use the Maxwell's Stress Tensor) E(R) = E, %3D R Figure 1: A moving infinite charged cylinder
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Transcribed Image Text:Force per Unit Length on a Half Part of an Infinite Charged Cylinder
Consider an infinite charged cylinder with radius (r) in a vacuum. The
charge is distributed uniformly inside the cylinder. The cylinder moves with
velocity (7) parallel to its symmetrical axis. If the value of the electrical field
on the surface is (E.), find the force per unit length (f) applied by itself on
a half part of it! (Hint: Use the Maxwell's Stress Tensor)
E(R) = E,
%3D
R
Figure 1: A moving infinite charged cylinder
Figure 2: Force per unit length applied on a half part of the cylinder
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