Dependence of resistance on cross section area

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SUMMARY

The resistance of a resistor is primarily determined by its cross-sectional area (S) as described by the formula R = ρ*L/S, where R is resistance, ρ is specific resistance, and L is the length of the resistor. This relationship holds true under direct current (DC) and low-frequency conditions. However, in high-frequency scenarios where the skin effect dominates, the resistance may become inversely proportional to the diameter of the conductor rather than the cross-sectional area. Understanding the impact of skin depth is crucial for accurately calculating resistance in alternating current (AC) applications.

PREREQUISITES
  • Understanding of electrical resistance and Ohm's Law
  • Familiarity with the concepts of direct current (DC) and alternating current (AC)
  • Knowledge of skin effect and skin depth in conductors
  • Basic grasp of the relationship between cross-sectional area and resistance
NEXT STEPS
  • Research the concept of skin depth in conductors and its effect on AC resistance
  • Explore the differences between DC and AC resistance calculations
  • Learn about the application of the formula R = ρ*L/S in various frequency conditions
  • Investigate the use of round wire AC resistance calculators for practical applications
USEFUL FOR

Electrical engineers, physicists, and students studying circuit design or materials science will benefit from this discussion, particularly those interested in the effects of frequency on resistance in conductors.

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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