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Charge of uniform surface density 8.00nC/m2is distributed over an entire x-yplane; charge of uniform surface densityis 3.00nC/m2distributed over the parallel plane defined by z = 2.00 m. Determine the magnitude of the electric field at any point having a z-coordinate of

(a)1.00 m and

(b) 3.00 m.

Short Answer

Expert verified
  1. The magnitude of the electric field at any point having a z-coordinate of 1m is 2.82×102N/C.
  2. The magnitude of the electric field at any point having a z-coordinate of 3m is 6.21×102N/C.

Step by step solution

01

The given data

  1. Surface charge density 8.00nC/m2is distributed over an entire x-y plane.
  2. Surface charge density 3.00nC/m2is distributed over the parallel plane defined by: z = 2.00 m
02

Understanding the concept of the electric field

Using the concept of the electric field of a Gaussian surface, we can calculate the electric fields at the given z-coordinates. The net electric field, due to the presence of two surface charge densities σ, is used for the net electric field.

Formula:

The electric field of a non-conduction sheet,

E=σ2ε0 (i)

03

a) Calculation of the electric field having z = 1 m

Both sheets are horizontal (parallel to the x-y plane), producing vertical fields (parallel to the z-axis). At points above the z = 0 sheet (sheet A), its field points upward (toward +z); at points above the z = 2 sheet (sheet B), its field does likewise. However, below the z = 2 sheet, its field is oriented downward.

The magnitude of the net field in the region between the sheets is given using equation (i) as follows:

E=σA2ε0-σA'2ε0=8.00×10-9C/m2-3.00×10-9C/m22(8.85×10-12C2/Nm2)=2.82×102N/C

Hence, the value of the electric field is 2.82×102N/C.

04

b) Calculation of the electric field having z = 3 m

The magnitude of the net field at points above both sheets is given using equation (i) as follows:

E=σA2ε0+σA'2ε0=8.00×10-9C/m2-3.00×10-9C/m22(8.85×10-12C2/Nm2)=6.21×102N/C

Hence, the value of the electric field is 6.21×102N/C.

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Most popular questions from this chapter

In Fig. 23-45, a small circular hole of radiusR=1.80cmhas been cut in the middle of an infinite, flat, non-conducting surface that has uniform charge densityσ=4.50pC/m2. A z-axis, with its origin at the hole’s center, is perpendicular to the surface. In unit-vector notation, what is the electric field at point Patz=2.56cm? (Hint:See Eq. 22-26 and use superposition.)

Figure 23-27 shows four solid spheres, each with charge Quniformly distributed through its volume. (a) Rank the spheres according to their volume charge density, greatest first. The figure also shows a point for each sphere, all at the same distance from the center of the sphere. (b) Rank the spheres according to the magnitude of the electric field they produce at point P, greatest first.

Figure 23-47 shows cross-sections through two large, parallel, non-conducting sheets with identical distributions of positive charge with surface charge densityσ=1.77×10-22C/m2. In unit-vector notation, what is the electric field at points (a) above the sheets, (b) between them, and (c) below them?

Equation 23-11 (E=σ/ε0) gives the electric field at points near a charged conducting surface. Apply this equation to a conducting sphere of radius rand charge q, and show that the electric field outside the sphere is the same as the field of a charged particle located at the center of the sphere.

The box-like Gaussian surface shown in Fig. 23-38 encloses a net charge of+24.0ε0Cand lies in an electric field given by role="math" localid="1657339232606" E=[(10.0+2.00)j^+bzk^]N/Cwith xand zin meters and ba constant. The bottom face is in the plane; the top face is in the horizontal plane passing through y2=1.00m. For x1=1.00m, x2=4.00m,z1=1.00m , andz2=3.00m, what is b?

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