An infinite grounded conducting plane is located at z = 0 and fills the x – y plane so that the electrostatic potential in the plane V (x, y, 0) is zero for all x and y. A single charge q is placed a distance a above the plane at the point (0,0, a). There are no other charges in the region z>0. (a) Using the boundary conditions and the first uniqueness theorem, find the electrostatic potential V (x, y, z) for all points above the plane: all x and y, and all z > 0. (b) Using the formula E = -V, calculate the electric field É also for all points above the plane. What is the electric field below the plane for z < 0? (c) Find the charge density per area o(x, y) for all x and y on the grounded plane, by using Gauss' law and the value of E just above the plane. (d) Integrate your result for o(x, y) to find the total amount of charge that is on the grounded plane wi charge q that was placed above the plane. This means that you should find the a circle of radius R, whose center is directly below the

An infinite grounded conducting plane is located at z = 0 and fills the x – y plane so that the electrostatic potential in the plane V (x, y, 0) is zero for all x and y. A single charge q is placed a distance a above the plane at the point (0,0, a). There are no other charges in the region z>0. (a) Using the boundary conditions and the first uniqueness theorem, find the electrostatic potential V (x, y, z) for all points above the plane: all x and y, and all z > 0. (b) Using the formula E = -V, calculate the electric field É also for all points above the plane. What is the electric field below the plane for z < 0? (c) Find the charge density per area o(x, y) for all x and y on the grounded plane, by using Gauss' law and the value of E just above the plane. (d) Integrate your result for o(x, y) to find the total amount of charge that is on the grounded plane wi charge q that was placed above the plane. This means that you should find the a circle of radius R, whose center is directly below the