Understanding the Attractive Force of a Positive Charge Near a Neutral Conductor

AI Thread Summary
A positive charge near a neutral conductor experiences an attractive electrostatic force due to charge redistribution on the conductor's surface. When the positive charge is introduced, negative charges within the conductor are drawn closer, creating a net attraction. This phenomenon highlights that an isolated charge can indeed attract neutral atoms through induced polarization. The resulting potential from this interaction decreases with distance, following a 1/r^4 relationship, unlike typical dipole interactions which follow a 1/r^2 pattern. Understanding this concept is crucial for grasping the fundamentals of electrostatics and molecular interactions.
dzza
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I am just reviewing some E&M because i took the class before I ever thought i had that big of an interest in physics and just memorized formulas, etc. Anyway, this is from a "which of the following statements is true" question.

The true statement is: A positive charge experiences an attractive electrostatic force near a neutral conductor.

The alternatives were that it experiences a repulsive force, no force, ...

How come the true statement is indeed true as opposed to a positive charge experiencing no electrostatic force near a neutral conductor?
 
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Charge redistributes itself on the surface of the conductor in response to the presence of the charge. Negative charges are brought close to the positive charge, resulting in a net attraction.
 
dzza said:
The true statement is: A positive charge experiences an attractive electrostatic force near a neutral conductor.
Is that true? I wouldn't have expected that "true statement". That would mean that an isolated charge (like an electron) is attracted to neutral atoms... I didn't know that was true...
 
There must be a redistribution of charge if the surface of the conductor is to remain an equipotential. This induced polarization results in a potential that goes as 1/r4 (the usual dipole goes as 1/r2, plus an extra 1/r2 to account for the decreasing strength of the induced dipole with distance). This does have an analog in atomic/molecular interactions, often referred to as charge-induced dipole forces.
 
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