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?
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.
PREREQUISITESElectrical 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.
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.)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?
That's because they are dealing with ordinary bulk properties under DC and low frequency conditions.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).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.
Consider the flow of electrons through a wire analogous to the flow of water through a pipe.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?