Field dependence on the potential in a wire

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Homework Help Overview

The discussion revolves around the relationship between electric potential and electric field in wires, particularly in the context of cylindrical resistors with varying resistivity. Participants explore specific examples from a homework question that involves comparing electric fields and potentials at different points in a wire.

Discussion Character

  • Conceptual clarification, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants examine whether a higher potential in a wire implies a higher electric field, questioning the meaning of variables in the equation E=V/L. They also discuss the implications of current density and resistivity on electric fields in different configurations.

Discussion Status

There is an ongoing exploration of the relationship between electric fields and potentials, with some participants suggesting that the electric field is related to the potential gradient rather than the potential value itself. Multiple interpretations of the scenarios presented in the homework questions are being considered, and some guidance has been offered regarding the application of current density equations.

Contextual Notes

Participants note the complexity of the scenarios due to varying resistivity and the need for schematic representations to clarify the relationships between current densities and electric fields. There is also mention of the need for intuitive understanding versus mathematical rigor in approaching the problems.

Krushnaraj Pandya
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Homework Statement


Does a point in a wire having higher potential necessarily mean that it has a higher electric field?
For example consider the cases of question 27 and 31 in the picture attached below.

Homework Equations


E=V/L

The Attempt at a Solution


The potential at a and b is the same in 27, so can I say E is the same. What does L in E=V/L mean here in this context? In 31, I think E at a is higher since potential is higher, still not sure about what L means
 

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Can't read the text in the picture. Please type out the text content and provide close-ups of the figures
 
gneill said:
Can't read the text in the picture. Please type out the text content and provide close-ups of the figures
really sorry about that.
consider a cylindrical resistor whose resistivity increases linearly with the radial distance. it is connected to a battery as shown. (Now refer figure 1), If the electric fields at a and b are Ea and Eb then how are they related?
Now consider a thick cylinder of uniform resistivity. A battery is connected as shown. Same question, (see figure 2)
 

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Krushnaraj Pandya said:
Does a point in a wire having higher potential necessarily mean that it has a higher electric field?
No. The field goes with the potential gradient, not the potential value.
 
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haruspex said:
No. The field goes with the potential gradient, not the potential value.
So Edx=dV...but how do we compare V/l in the context of 31?
 
For 31. the current densities at A and B are (from ohm's law) ##J_A=\frac{E_A}{\rho}## and ##J_B=\frac{E_B}{\rho}## since the resistivity ##\rho## is the same. The total current through the collateral surface at A ##S_A## must be equal to the current through the collateral surface at B ##S_B##. So we have

##J_AS_A=J_BS_B##

From this equation you can figure out which of ##J_A, J_B## is bigger (depending which of ##S_A, S_B## is bigger ) and hence which of the electric field is bigger.
 
Delta² said:
For 31. the current densities at A and B are (from ohm's law) ##J_A=\frac{E_A}{\rho}## and ##J_B=\frac{E_B}{\rho}## since the resistivity ##\rho## is the same. The total current through the collateral surface at A ##S_A## must be equal to the current through the collateral surface at B ##S_B##. So we have

##J_AS_A=J_BS_B##

From this equation you can figure out which of ##J_A, J_B## is bigger (depending which of ##S_A, S_B## is bigger ) and hence which of the electric field is bigger.
From this Ja is greater and therefore Ea is greater. But by the same logic, in 27- area that charge passes through is the same for A and B therefore Ja=Jb and since resistivity increases linearly with radius, Eb should be greater than Ea which is incorrect.
Btw, I read your insight on the fundamental theorem of calculus and I really enjoyed whatever little I could grasp from it. :D
 
Hard to explain without making a schematic, but that equation with current densities and surfaces does not hold in the case of 27. Remember that equation comes from the condition that the current through different surfaces that are connected in a series-way must be equal. It is also because the vector AB is perpendicular to the direction of the current flow , while in 31 the vector AB is parallel to the direction of the current flow.
 
Delta² said:
Hard to explain without making a schematic, but that equation with current densities and surfaces does not hold in the case of 27. Remember that equation comes from the condition that the current through different surfaces that are connected in a series-way must be equal. It is also because the vector AB is perpendicular to the direction of the current flow , while in 31 the vector AB is parallel to the direction of the current flow.
Is there any intuitive way to be able to find that Ea=Eb in 27? If it's beyond what I can currently understand then we can do away with mathematical rigor- but I feel like if that question is in my book there must be simple way to understand this
 
  • #10
Krushnaraj Pandya said:
Is there any intuitive way to be able to find that Ea=Eb in 27? If it's beyond what I can currently understand then we can do away with mathematical rigor- but I feel like if that question is in my book there must be simple way to understand this

Yes the simple intuitive way is to view it as a capacitor with electric field E=V/L between the two plates (left and right cap of the cylinder) where L is the length of the cylinder. The difference of course is that there is current between the two plates (while in a capacitor there is no conventional current that is flow of charges between the two plates) but because the direction of current is axial , that is perpendicular to the direction of the variable resistivity which is radial, the variable resistivity doesn't affect the electric field.
 
  • #11
Delta² said:
Yes the simple intuitive way is to view it as a capacitor with electric field E=V/L between the two plates (left and right cap of the cylinder) where L is the length of the cylinder. The difference of course is that there is current between the two plates (while in a capacitor there is no conventional current that is flow of charges between the two plates) but because the direction of current is axial , that is perpendicular to the direction of the variable resistivity which is radial, the variable resistivity doesn't affect the electric field.
Got it! Thank you
 

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