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In Fig. 23-49, a small, non-conducting ball of massm=1.0mgand charge q=2.0×10-8C (distributed uniformly through its volume) hangs from an insulating thread that makes an angle θ=30owith a vertical, uniformly charged non-conducting sheet (shown in cross-section). Considering the gravitational force on the ball and assuming the sheet extends far vertically and into and out of the page, calculate the surface charge density s of the sheet.

Short Answer

Expert verified

The surface charge density of the sheet is5.0×10-9C/m2 .

Step by step solution

01

The given data

  1. Mass of the ball,1mg
  2. Charge on the ball,role="math" localid="1657350162514" q=2×10-8C
  3. The angle of the insulation thread,role="math" localid="1657350181635" θ=30O
02

Understanding the concept of the electrostatic force and Newton’s law

Using the electrostatic force value in the equations of the horizontal and vertical components of the free body diagram, we can get the expression of the electric field. Again, using the value of the electric field of a non-conducting sheet in this calculated expression, we can get the value of the required surface charge density.

Formula:

The electrostatic force of a charged particle,F=qE (1)

The force due to the gravity, F=mg (2)

The electric field of a non-conducting shell,E=σ2ε0 (3)

03

Calculation of the surface charge density of the sheet

The forces acting on the ball are shown in the diagram to the right. The electric field produced by the plate is normal to the plate and points to the right. Since the ball is positively charged, the electric force on it also points to the right. The tension in the thread makes the angle with the vertical. Since the ball is in equilibrium the net force on it vanishes.

The sum of the horizontal components from the free body diagram using equation (i) for force yields

qE-T²õ¾±²Ôθ=0........................(4)

The sum of the vertical components yields,

T³¦´Ç²õθ-mg=0.................(5)

The expression of the tension from equation (4) is given as:

T=qE²õ¾±²Ôθ

This value is substituted into equation (5) to get the following value:

qE=T³Ù²¹²Ôθ

As the tension of the body is equal to the body weight, so using equation (2) and equation (3), the surface density of the sheet is given as follows:

qσ2εo=mg³Ù²¹²Ôθσ=2εomg³Ù²¹²Ôθqσ=298.85×10-12C2/N.m2)(1.0×10-6kg)(9.8,m/s2)tan30o2.0×10-8Cσ=5.0×10-9C/m2

Hence, the value of the surface charge density is 5.0×10-9C/M2 .

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Most popular questions from this chapter

Three infinite non-conducting sheets, with uniform positive surface charge densitiesσ,2σ,and 3σ,are arranged to be parallel like the two sheets in Fig. 23-19a. What is their order, from left to right, if the electric field produced by the arrangement has magnitudeE=0in one region andE=2σ/ε0in another region?

Figure 23-29 shows four Gaussian surfaces consisting of identical cylindrical midsections but different end caps. The surfaces are in a uniform electric fieldE→that is directed parallel to the central axis of each cylindrical midsection. The end caps have these shapes:S1, convex hemispheres;S3, concave hemispheres;S3, cones;S4, flat disks. Rank the surfaces according to (a) the net electric flux through them and (b) the electric flux through the top end caps, greatest first.

An electric field given by E=4.0i^-3.0(y2+2.0)j^, pierces a Gaussian cube of edge length 2.0mand positioned as shown in Fig. 23-7. (The magnitude Eis in Newton per coulomb and the position xis in meters.) What is the electric flux through the (a) top face, (b) bottom face, (c) left face, and (d) back face? (e) What is the net electric flux through the cube?

Figure 23-28 shows a section of three long charged cylinders centered on the same axis. Central cylinder Ahas a uniform chargeqA=+3q0. What uniform chargesqBandqCshould be on cylinders Band Cso that (if possible) the net electric field is zero at

(a) point 1,

(b) point 2, and

(c) point 3?

In Fig. 23-25, an electron is released between two infinite non-conducting sheets that are horizontal and have uniform surface charge densitiesσ(+)andσ(-), as indicated. The electron is subjected to the following three situations involving surface charge densities and sheet separations. Rank the magnitudes of the electron’s acceleration, greatest first.

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