Electric field strength and potential gradient

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Discussion Overview

The discussion revolves around the relationship between electric field strength (E) and electric potential (V), specifically examining the formulas E = -(dV/dx) and E = -(V/d). Participants explore the implications of these equations in the context of parallel plate capacitors and the conditions under which they apply.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant expresses confusion about how E = -(dV/dx) transforms into E = -(V/d), questioning the logical connection between the two equations.
  • Another participant notes that if the rate of change of V is constant over the distance, -dV/dx can be approximated as -V/d, but emphasizes that they are not strictly equal.
  • A follow-up comment clarifies that for parallel plates, E is constant, and thus Eparallel plates = -(V/d) is a specific case of the general relationship.
  • One participant argues that there is no change in potential difference (p.d.) as one moves between the plates, suggesting that dV/dx should be zero, which raises further questions about the application of the formulas.
  • A participant distinguishes between the different meanings of V in the equations, suggesting that the V in E = -dV/dx represents the potential at a specific position, while the V in E = V/d represents the potential difference between the plates.
  • Another participant reiterates that the first equation describes the electric field and potential at each point, while the second is a macroscopic relationship valid under specific assumptions.
  • One participant suggests that the equation E = -V/d should be more accurately written as E = -ΔV/d to clarify that V represents the potential difference between the plates, highlighting a common source of confusion.

Areas of Agreement / Disagreement

Participants generally agree that the two equations represent different contexts and meanings of potential, but there is no consensus on the implications of these differences or the conditions under which they apply. The discussion remains unresolved regarding the interpretation of dV/dx in the context of parallel plates.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the constancy of the electric field and potential difference, as well as the definitions of the variables used in the equations. These factors contribute to the ongoing debate and lack of resolution.

zinc79
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A bit of a problem. My book teaches me that E = -(dV/dx), where E is the electric field strength, V is the electric potential, and x represents displacement.

But, it also suggests along with the above formula that E = -(V/d) and displays a circuit with a battery of p.d. V and two parallel metal plates of distance (d) from each other.

My question is, HOW did E = -(dV/dx) become E = -(V/d)? The former formula, proven via differentiation, says that the electric field strength is negative of the potential gradient i.e. rate of change of electric potential with respect to the displacement. Then how does this transform into the electric field strength simply being equal to the negative of the ratio of the potential difference to the distance? It makes no sense to me!

And yet, I've seen the latter formula being used in practice questions.
 
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If the rate of change of V is constant over the distance x (or d), then -dV/dx can be stated as -V/d. -V/d is not equal to -dV/dx, but in a parallel plate capacitor it usually is.
 
To follow up on Gear300's comment...

the general relation is E = -(dV/dx)...
for parallel plates, one really should write Eparallel plates = -(V/d)

Recall for parallel plates, Eparallel plates is a constant [between the plates].

(Don't merely match symbols or abbreviations.
Not all "E"s mean the same thing.
For each "formula", understand what the variable represents.)
 
Hey, thank you for replying.

See, what I forgot to mention was my perspective on the parallel plate capacitor, which yes, has a uniform electric field. There is NO change in the p.d. as we move from one plate to the other, so shouldn't dV/dx become zero?
 
Er.. Unless I misread the OP, the confusion here comes from the fact that these are NOT the same "V".

In E = -dV/dx, this V is the electrostatic potential at a position x, i.e. V(x). It has a particular value depending on geometry.

In E = V/d, this "V", really is the potential difference between the two plates. If I call this V' instead of V, then here you can equate V' to dV in the first equation, and d to dx.

So it is important to know what those symbols really mean, rather than simply looking at the symbol. Often the same symbol represents different things.

Zz.
 
Exactly, the first equation is about the electrical field E(x) and potential V(x) at each point in space along the direction x, while the second is a macroscopic relationship between an allegedly constant field E and a voltage V which is a quantity defined for the whole system.

The first one is the general relationship between electric field and potential, and is valid in any scenario.

The second one is a particular case of the general relationship. You can obtain it by assuming E(x)=E constant and integrating in dx.
 
The parallel-plate equation E = -V/d really should read E = -\Delta V/d to indicate that the voltage is the difference in potential between the two plates. Unfortunately it's a long-standing custom to use V to represent both potential (at a point) and potential difference (between two points) in different contexts.
 
jtbell said:
The parallel-plate equation E = -V/d really should read E = -\Delta V/d to indicate that the voltage is the difference in potential between the two plates. Unfortunately it's a long-standing custom to use V to represent both potential (at a point) and potential difference (between two points) in different contexts.

good answer.
 

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