What Is the Potential Energy of a Charge Near an Infinite Sheet and a Long Wire?

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Homework Help Overview

The discussion revolves around calculating the potential energy of a charge in the presence of an infinite sheet of charge and a long wire. The problem involves understanding the implications of given charge densities and potentials, as well as the relationships between them.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the use of the given potential and charge densities in calculating potential energy. Some express confusion about the application of the 1.3 kV potential and its relevance to the problem setup. Others question the assumptions regarding the equipotential nature of the infinite sheet in the presence of additional charges.

Discussion Status

There is an ongoing exploration of the problem, with some participants reporting success in their calculations while others express uncertainty and seek clarification on the problem's conditions. The discussion reflects a mix of attempts to reconcile different interpretations of the potential and the effects of the charge distributions.

Contextual Notes

Participants note potential issues with the problem statement, particularly regarding the uniformity of the potential across the plane and the implications of having multiple charge sources. There are also mentions of significant figures in calculations, indicating a focus on precision in the context of the problem.

wml
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An infinite sheet of charge that has a surface charge density of 21 nC/m2 lies in the yz plane, passes through the origin and is at a potential of 1.3 kV.
A long wire having a linear charge density of 50 nC/m lies parallel to the y-axis and intersects the x-axis at 3.2m.
The permittivity of a vacuum is 8.85419*10^-12 C2/N.m2

What is the potential energy of a 2.4 nC charge placed at x = 1.5 m in units of J.


can anybody help me..
I don't know how to use the 1.3 kV potential
I used V=(入/ 2Eoл)× Ln(r1/r2) , U=V×q
but I entered the answer, it was wrong
:cry:
 
Last edited:
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wml said:
An infinite sheet of charge that has a surface charge density of 21 nC/m2 lies in the yz plane, passes through the origin and is at a potential of 1.3 kV.
A long wire having a linear charge density of 50 nC/m lies parallel to the y-axis and intersects the x-axis at 3.2m.
The permittivity of a vacuum is 8.85419*10^-12 C2/N.m2

What is the potential energy of a 2.4 nC charge placed at x = 1.5 m in units of J.


can anybody help me..
I don't know how to use the 1.3 kV potential
I used V=(入/ 2Eoл)× Ln(r1/r2) , U=V×q
but I entered the answer, it was wrong
:cry:
The problem is not stated correctly.
If the infinite sheet has a uniform charge density, and there are other charges present, it can’t be an equipotential.
 
never mind~ I got the right answer~! ^^: finally

Vb-Va=-21n×1.5/2Eo -> Vb=1300-1779.661= -479.661

VB-VA(0)=50n/ (2лEo) × Ln(3.2/1.7) = 568.7519 3.2-1.5=1.7

U=q(Vb+VB) = 2.4n × (568.7519-479.661)=2.13818×10^-7
 
But that answer is wrong because of my first post.
If there is a charged wire and a point charge present, the plane cannot be at a constant potential of 1.3 kV.
Is it stated that that is the potential at the origin or on the whole plane?
Also, watch your sig. figs.
 
well, actually I'm still confused but I entered the answer and it was right >,< I didn't skip any words... what I put on the first post is exactly I have on my paper
 

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