Field dependence on the potential in a wire

In summary: E=V/L. 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... field is still E=V/L.
  • #1
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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  • #2
Can't read the text in the picture. Please type out the text content and provide close-ups of the figures
 
  • #3
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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  • #4
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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  • #5
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?
 
  • #6
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.
 
  • #7
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
 
  • #8
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.
 
  • #9
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
 

FAQ: Field dependence on the potential in a wire

1. What is meant by "field dependence on the potential in a wire"?

"Field dependence on the potential in a wire" refers to the relationship between the electric field and the potential difference (or voltage) in a wire. In simple terms, it describes how the electric field affects the movement of charges in the wire, leading to a potential difference between two points.

2. How is the potential in a wire affected by the electric field?

The potential in a wire is directly proportional to the electric field strength. This means that as the electric field increases, the potential difference also increases. This relationship is described by the equation V = Ed, where V is the potential difference, E is the electric field strength, and d is the distance between the two points.

3. What factors can influence the field dependence on the potential in a wire?

The field dependence on the potential in a wire can be influenced by several factors, including the length and thickness of the wire, the material of the wire, and the magnitude and direction of the electric field. Additionally, the presence of other charges or conductors near the wire can also affect the field dependence.

4. How does field dependence on the potential in a wire relate to Ohm's Law?

Field dependence on the potential in a wire is a fundamental concept in understanding Ohm's Law. Ohm's Law states that the current flowing through a wire is directly proportional to the potential difference and inversely proportional to the resistance of the wire. The field dependence on the potential in a wire explains the relationship between potential and current, while resistance is determined by the properties of the wire itself.

5. How is field dependence on the potential in a wire used in practical applications?

The understanding of field dependence on the potential in a wire is crucial in various practical applications, such as in electrical circuits and power transmission. By manipulating the electric field and potential difference in wires, we can control the flow of current and power in a system. This knowledge is also essential in designing and optimizing electrical devices and systems for maximum efficiency and safety.

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