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Consider three identical metal spheres, A, B, and C. Sphere A carries a charge of \(+5 q\) . Sphere B carries a charge of \(-q,\) Sphere \(C\) carries no net charge. Spheres A and \(\mathrm{B}\) are touched together and then separated. Sphere C is then touched to sphere A and separated from it. Last, sphere C is touched to sphere B and separated from it. (a) How much charge ends up on sphere C? What is the total charge on the three spheres (b) before they are allowed to touch each other and (c) after they have touched?

Short Answer

Expert verified
Sphere C ends with +1.5q of charge; total charge before and after is +4q.

Step by step solution

01

Initial Charges

Determine the initial charges on each sphere. Sphere A starts with a charge of \(+5q\), Sphere B starts with \(-q\), and Sphere C carries a charge of 0.
02

Sphere A and B Touch

When Sphere A and B touch, the total charge redistributes equally across the two spheres. The total initial charge on A and B is \(+5q - q = +4q\). Thus, after touching, each sphere has \(+2q\) charge.
03

Touch Sphere C to Sphere A

Upon touching Sphere A (which now has \(+2q\)) with Sphere C (neutral, 0 charge), the charge distributes equally: each gets \(+1q\) after separation.
04

Touch Sphere C to Sphere B

Now, Sphere C \((+1q)\) touches Sphere B \((+2q)\). The total charge for both spheres is \(+3q\), so each ends up with \(+1.5q\) after touching and separation.
05

Total Initial Charge

The total charge before any spheres touch is the sum of individual charges: \(+5q - q + 0 = +4q\).
06

Total Final Charge

After all interactions, the total charge remains the same; each interaction simply redistributes charge. Final charges: Sphere A: \(+1q\), Sphere B: \(+1.5q\), Sphere C: \(+1.5q\). The total is still \(+4q\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Charge Distribution
In electrostatics, understanding how charge distributes across objects when they come into contact is crucial. When two conductive objects touch, their charges distribute themselves over the combined surface of both objects. This distribution is typically even because like charges repel each other. Therefore, they spread out to maintain equilibrium.

For example, consider metal spheres like in the problem. Spheres A and B initially have charges of \(+5q\) and \(-q\), respectively. When they touch, the charges average out across the two. The initial total charge of \(+4q\) is divided evenly: each sphere ends up with \(+2q\). Thus, simply touching rearranges the charges between the spheres, highlighting the natural tendency for equilibrium in conductive systems.

Let's also consider the neutral sphere C. When it contacts sphere A, with its \(+2q\) charge, the charge also splits evenly between the two, leaving both spheres with \(+1q\). Charged objects will share their charge with neutral ones until the charge is equally distributed.
  • Conductive objects share charge upon contact
  • The goal is even distribution of charge
Conservation of Charge
The principle of conservation of charge is one of the fundamental laws of physics. It states that the total charge in an isolated system remains constant, even if charge moves from one object to another within the system. This means charges can neither be created nor destroyed, only transferred.

In our three-sphere example, before any interactions, the system's total charge sums up to \(+4q\) (adding \(+5q, -q,\) and \(0\) from spheres A, B, and C). Throughout the touching and separating process, charge moves between the spheres but never leaves the system.

Even after the spheres have touched and separated as outlined in the steps, the total charge remains \(+4q\). Such a scenario perfectly demonstrates the conservation of charge principle, illustrating that while individual sphere charges change, the total system charge does not.
  • Total charge is constant; only re-distributed
  • Charge remains the same before and after interactions
Conductors in Electrostatics
Conductors play an essential role in electrostatics because they allow for free movement of charge throughout their material. Metals, such as the spheres in our example, are good conductors. This means that when they come into contact, any excess charge spreads over the entire surface of the conductors to minimize the repulsion between like charges.

When a charged conductor touches a neutral conductor, the charge redistributes to achieve equilibrium. This occurs because the mobile charge carriers within the conductor spread out as far apart as possible.

In this exercise, all charge exchanges occur because the spheres are metallic and thus, conductive. After each contact, the charges on these metallic spheres adjusted themselves quickly and evenly. This rapid redistribution upon contact highlights the responsive nature of conductors in electrostatic scenarios.
  • Metallic conductors enable charge movement
  • Charges spread to minimize repulsion

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Most popular questions from this chapter

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