Question

1. what is the electric field at the centre (r = 0) of a hemisphere bounded by r = a, 0 < θ < π/2 and 0 < φ < 2m, that carries a uniform volumetric charge density P3(The charges are distributed in this hemispherical 3D space. Use spherical coordinates due to the hemispherical geometry.) Consider some charges that are lined up in a straight line. This line of charge carries a uniform linear charge density. Lets make Pl = 2/y (Coulombs/metre). To make it easier for us to mark, line up this line of charge along the y-axis, going from y -0 to y- L 2. Derive an equation that represents the electric field at any point P that is located along the z-axis (0,0,2). For this question, you will notice that the x-component of the electric field is zero, but that there is both a y-component and a z-component. Solve the integral for the y-component. As for the z-component, just write the proper integral but you dont have to solve it. [In order to get points for this question, you must (1) include a schematic showing the described geometry; (2) identify the relevant integral equation, (3) clearly state the values ofF,F, dl,etc. and (4) solve the integral for the y-component. Use rectangular coordinates.] a. 3. Calculate the electric flux produced by D (459302) m2 through a . This cylindrical surface defined by 0 < z < 5 m , -0.5 m and 0 < ф < is not a closed surface (only consider the curve surface).4. A spherical region of space of radius 0.1 m has a volumetric charge density py kr2 where k-4x 10-5 C/m-5. The charge density is zero elsewhere in space (r >0.1 m). Assume that the permittivity is Eo everywhere Calculate the electric flux density (D) at r-0.02m Determine the distance r outside the sphere at which the magnitude of the electric flux density is equal to what you found in part (a). a. b.

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Final answer is boxed. Direct integration is needed for this question.

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