Problem involving Coulomb's law

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Homework Help Overview

The discussion revolves around a problem involving Coulomb's law, specifically concerning the force exerted on a point charge by a uniformly charged metal sphere. The problem presents multiple-choice options regarding the relationship between the force and the distances involved, including the radius of the sphere and the distance from the point charge to the sphere's surface.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the distance from the point charge to the sphere and the radius of the sphere, questioning why the distance is expressed as the sum of the radius and the surface distance. Some participants discuss the implications of the sphere's uniform charge distribution and its effect on the force experienced by the point charge.

Discussion Status

Several participants have provided insights and clarifications regarding the relationship between the distances involved in the problem. There is an acknowledgment of the electric field's role in understanding Coulomb's law, and some participants express a shift in their understanding based on the arguments presented. However, there is no explicit consensus on the final interpretation of the problem.

Contextual Notes

Participants note that the problem's complexity increases when considering different distances relative to the sphere's radius. There are mentions of constraints related to the course material, indicating that some aspects of the discussion may extend beyond the current curriculum.

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Homework Statement


A big metal sphere has radius ##r## and charge ##Q##. The distance between a certain point charge and the surface of the sphere is equal to ##s##. The magnitude of the force exerted on the point charge is inversely proportional to:

A) ##s^2##
B) ##r^2##
C) ##(s+r)^2## (correct answer)
D) ##s^2+r^2##

(Source: Fysica Vandaag 5.2, Uitgeverij Pelckmans)

Homework Equations


Coulomb's law

The Attempt at a Solution


Let ##d## be the distance between the two charges.
##F=k\frac{|Q||Q'|}{d^2}=\frac{\mathrm{constant}}{d^2}##
This means the constant of proportionality is equal to ##d^2##.

Why is ##d=s+r##? I would expect it to be equal to ##s## since the charge in a sphere is the same everywhere.
 
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1729 said:

Homework Statement


A big metal sphere has radius ##r## and charge ##Q##. The distance between a certain point charge and the surface of the sphere is equal to ##s##. The magnitude of the force exerted on the point charge is inversely proportional to:

A) ##s^2##
B) ##r^2##
C) ##(s+r)^2## (correct answer)
D) ##s^2+r^2##

Homework Equations


Coulomb's law

The Attempt at a Solution


Let ##d## be the distance between the two charges.
##F=k\frac{|Q||Q'|}{d^2}=\frac{\mathrm{constant}}{d^2}##
This means the constant of proportionality is equal to a ##d^2##.

Why is ##d=s+r##? I would expect it to be equal to ##s## since the charge in a sphere is the same everywhere.
If the sphere is uniformly charged, then at any point external to the sphere, the electric field produced by the sphere is the same as if all of the charge would reside at the center of the sphere.
 
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Consider two extreme situations. First, take r = 1 mm, s = 10 cm. At that distance, the metal sphere looks almost like a point charge, and there is no significant difference between the interaction of the point charge with the part of the sphere that is closest, and the part that is farthest away.

Second, take r = 1 m and s = 10 cm. Since, as you correctly state, the charge Q is uniformly distributed, the point charge will feel a greater force from the part of the charge that is closest compared to that on the other side of the sphere, which is now 2 m away.

So, it can't depend only on s.

The reason why it is r + s has just been given by Sammy.
 
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Thank you for your answers! I see the error of my ways now -- your argument is convincing, DrClaude!

At first I was skeptical about the relation between the electric field property Sammy mentioned and Coulomb's law. Luckily, it then struck me that one can also define Coulomb's law in terms of the electric field force.

##F=k\frac{|Q||Q'|}{d^2}=|Q|\cdot E##
By the property Sammy mentioned, we find that the distance can be rewritten as ##s+r##, and the result follows.

(In retrospect the electric field was a good way to think about this problem, but I didn't think of using it since the concept was introduced in the following chapter)
 
1729 said:
Thank you for your answers! I see the error of my ways now -- your argument is convincing, DrClaude!

At first I was skeptical about the relation between the electric field property Sammy mentioned and Coulomb's law. Luckily, it then struck me that one can also define Coulomb's law in terms of the electric field force.

##F=k\frac{|Q||Q'|}{d^2}=|Q|\cdot E##
By the property Sammy mentioned, we find that the distance can be rewritten as ##s+r##, and the result follows.

(In retrospect the electric field was a good way to think about this problem, but I didn't think of using it since the concept was introduced in the following chapter)

Interestingly, this works only for an inverse-square force law. If the force between two charges at distance ##r## were
F = k \frac{q_1 q_2}{r^p}
for any ##p\neq 2##, then the nice property cited above would no longer hold. There is something almost magical about the special value ##p = 2##.
 
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That's beyond the scope of the course I'm taking, but interesting nevertheless. Could you expand on why that happens?
 
1729 said:
That's beyond the scope of the course I'm taking, but interesting nevertheless. Could you expand on why that happens?
If the distance far greater than the radius of the sphere, then we can assume it a point of charge. If not, there are many points of charges on the sphere to consider. Summing them all will show that it will be equalled to point of total charges at the center.
 
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