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Ch 22: Gauss' Law
Chapter 22, Problem 26

A very large, horizontal, nonconducting sheet of charge has uniform charge per unit area σ = 5.00×10−6 C/m2. (a) A small sphere of mass m = 8.00×10−6 kg and charge q is placed 3.00 cm above the sheet of charge and then released from rest. (b) What is q if the sphere is released 1.50 cm above the sheet?

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1
Identify the forces acting on the sphere when it is placed above the charged sheet. The forces include the gravitational force downward (F_g = mg) and the electric force upward due to the electric field created by the sheet of charge (F_e = qE).
Calculate the electric field (E) generated by the sheet of charge using the formula for the electric field due to an infinite sheet of charge, E = \( \frac{\sigma}{2\epsilon_0} \), where \( \sigma \) is the surface charge density and \( \epsilon_0 \) is the permittivity of free space.
Set up the equilibrium condition for the sphere when it is in balance above the sheet. This is when the electric force equals the gravitational force, i.e., qE = mg.
Solve for the charge q on the sphere using the equilibrium condition. Rearrange the equation to q = \( \frac{mg}{E} \).
Substitute the values for m, g, and E into the equation to find the charge q for each scenario: when the sphere is 3.00 cm and 1.50 cm above the sheet.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Electric Field due to a Charged Sheet

A uniformly charged infinite sheet creates a constant electric field perpendicular to its surface, given by the formula E = σ / (2ε₀), where σ is the surface charge density and ε₀ is the permittivity of free space. This electric field is uniform and does not depend on the distance from the sheet, which is crucial for analyzing the forces acting on the charged sphere.
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Force on a Charged Object in an Electric Field

When a charged object is placed in an electric field, it experiences a force given by F = qE, where q is the charge of the object and E is the electric field strength. This force will determine the motion of the sphere after it is released, as it will accelerate due to the electric field created by the charged sheet.
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Newton's Second Law of Motion

Newton's Second Law states that the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass, expressed as F = ma. This principle is essential for calculating the motion of the sphere after it is released, as it allows us to relate the force due to the electric field to the resulting acceleration and displacement of the sphere.
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Related Practice
Textbook Question
Charge q is distributed uniformly throughout the volume of an insulating sphere of radius R = 4.00 cm. At a distance of r = 8.00 cm from the center of the sphere, the electric field due to the charge distribution has magnitude E = 940 N/C. What are (b) the electric field at a distance of 2.00 cm from the sphere's center?
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Textbook Question
A conductor with an inner cavity, like that shown in Fig. 22.23c, carries a total charge of +5.00 nC. The charge within the cavity, insulated from the conductor, is −6.00 nC. How much charge is on (a) the inner surface of the conductor and (b) the outer surface of the conductor?
1445
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Textbook Question
A very large, horizontal, nonconducting sheet of charge has uniform charge per unit area σ = 5.00×10−6 C/m2. (a) A small sphere of mass m = 8.00×10−6 kg and charge q is placed 3.00 cm above the sheet of charge and then released from rest. (a) If the sphere is to remain motionless when it is released, what must be the value of q?
1036
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Textbook Question
An infinitely long cylindrical conductor has radius r and uniform surface charge density σ. (a) In terms of σ and R, what is the charge per unit length λ for the cylinder?
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Textbook Question
An infinitely long cylindrical conductor has radius r and uniform surface charge density σ. (b) In terms of σ, what is the magnitude of the electric field produced by the charged cylinder at a distance r > R from its axis? (c) Express the result of part (b) in terms of λ and show that the electric field outside the cylinder is the same as if all the charge were on the axis.
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Textbook Question
A very long conducting tube (hollow cylinder) has inner radius A and outer radius b. It carries charge per unit length +α, where α is a positive constant with units of C/m. A line of charge lies along the axis of the tube. The line of charge has charge per unit length +α. (b) What is the charge per unit length on (i) the inner surface of the tube and (ii) the outer surface of the tube?
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