Dependence of resistance on cross section area

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Discussion Overview

The discussion centers on the dependence of electrical resistance on the cross-sectional area of conductors, particularly in the context of different frequency regimes, such as DC versus AC. Participants explore the implications of the skin effect on resistance and question the conventional understanding presented in textbooks.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that resistance depends on the cross-sectional area, while others question why it does not depend on the perimeter, particularly in the context of skin effect.
  • One participant notes that the relationship between resistance and cross-sectional area may only hold true for certain types of resistors and under specific conditions, such as low frequency.
  • There is a suggestion that doubling the width of a wire may lead to a reduction in resistance, but participants express uncertainty about whether this reduction is linear with respect to cross-section or perimeter.
  • Another participant emphasizes that resistance is typically measured with DC current, where the entire cross-section is utilized, contrasting this with AC conditions where the skin effect alters current distribution.
  • Some participants reference the formula R = ρ*L/S, indicating that textbooks generally present resistance in terms of cross-sectional area under standard conditions, but this may not apply in all scenarios.
  • One participant proposes that if the skin depth is small compared to the diameter, resistance may be inversely proportional to the diameter rather than the square of the diameter.
  • A metaphor comparing electron flow in a wire to water flow in a pipe is introduced to illustrate the relationship between cross-sectional area and resistance.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between resistance and cross-sectional area versus perimeter, with no consensus reached on the implications of skin effect or the applicability of standard formulas in varying conditions.

Contextual Notes

Participants highlight limitations in understanding the relationship between DC and AC resistance, particularly regarding the influence of frequency and cross-sectional geometry on resistance measurements.

Yoni
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The electrons flow on the outer surface of the resistor, why then does the resistance of a resistor depend on it's cross sectional area and not on it's perimeter?
 
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That is only true for certain kinds of resistors in certain regimes. For example, it may be true for high frequency electronics where the current is mostly at the skin of the conductor.
 
I though all metals have this property... Anyway if I take these types of materials, where the flow of electrons is at the skin, and double the width of the wire, will I get half the resistance or a quarter of the resistance? That is, is resistance linearly dependent on the cross section or on the perimeter?

I think it should be perimeter, but all textbooks show that R = ρ*L/S, where R is the resistance, ρ is specific resistance, L is the resistor length, and S is the cross section.
 
Yoni said:
I though all metals have this property... Anyway if I take these types of materials, where the flow of electrons is at the skin, and double the width of the wire, will I get half the resistance or a quarter of the resistance? That is, is resistance linearly dependent on the cross section or on the perimeter?
I presume roughly proportional to perimeter for frequencies/conditions where skin effect dominates. (I think I've read that skin effect can be seen on massive power transmission cables, such that current density near the core may be, say, half what it is nearer the surface. So a high tensile steel core need not reduce an aluminium cable's resistance appreciably.)

all textbooks show that R = ρ*L/S, where R is the resistance, ρ is specific resistance, L is the resistor length, and S is the cross section.
That's because they are dealing with ordinary bulk properties under DC and low frequency conditions.
 
Resistance is measured with DC current. When a conductor is subjected to DC, the current uses the entire cross section. It is only when you start using AC that the current stops using the inner part of the conductor (read up on skin depth)...in this cases, you need to find the relationship between your DC-resistance and AC-resistance to ease further calculations...this relationship will depend on the frequency you are working with and the cross-sectional geometry of your conductor.
 
Yoni said:
I though all metals have this property... Anyway if I take these types of materials, where the flow of electrons is at the skin, and double the width of the wire, will I get half the resistance or a quarter of the resistance? That is, is resistance linearly dependent on the cross section or on the perimeter?

I think it should be perimeter, but all textbooks show that R = ρ*L/S, where R is the resistance, ρ is specific resistance, L is the resistor length, and S is the cross section.
If the skin depth is small compared with the diameter yes, the resistance is approximately inverse proportional to the diameter (and not diameter squared).
See here for example:
http://chemandy.com/calculators/round-wire-ac-resistance-calculator.htm
 
Yoni said:
The electrons flow on the outer surface of the resistor, why then does the resistance of a resistor depend on it's cross sectional area and not on it's perimeter?
Consider the flow of electrons through a wire analogous to the flow of water through a pipe.
More the cross-sectional area, more the amount of water that can flow in a specific time. Lesser the CSA, lesser the amount of water, i.e., more the resistance.
 

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