Surface current density problem

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SUMMARY

The surface current density, K, is mathematically defined as K = v·σ, where v represents the velocity of the surface charge and σ is the surface charge density. This formula can be intuitively understood by visualizing a long rectangular sheet of charge moving with a constant speed, where the current through a stationary imaginary line across the sheet is calculated. The derivation shows that the total charge passing the line in a time interval is ΔQ = (σ)(vΔt)(w), leading to the conclusion that K = σv. The discussion clarifies the unambiguous nature of current measurement across a ribbon of width dl, even if the current varies along its length.

PREREQUISITES
  • Understanding of surface charge density (σ)
  • Familiarity with basic concepts of electric current
  • Knowledge of kinematics, specifically velocity (v)
  • Basic grasp of units in physics, particularly amperes per meter (A/m)
NEXT STEPS
  • Explore the implications of surface charge density in electromagnetic theory
  • Study the relationship between current density and electric fields
  • Investigate the effects of varying surface charge density on current flow
  • Learn about the applications of surface current density in materials science
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism or materials science will benefit from this discussion, particularly those interested in the behavior of surface currents and charge distributions.

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The surface current density, K, is defined as the the current through a unit width perpendicular to the flow. In particular:
K = v\cdotσ
where σ is the surface charge density. Now I have a little trouble understanding this formula intuitively. Can someone describe in pictures how it is interpreted physically?
Also as a side note: Why can you unambigously speak of the current through a ribbon of width dl parallel to the current - what if the current changes as we move parallel to it?
 
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One way to justify that formula is to consider the units: (A/m) = (m/s)(C/m2).

Or: Imagine a long rectangular sheet of charge with width w and uniform surface charge density σ. Draw an imaginary line at right angles across the width of the sheet. Set the sheet in motion with constant speed v while keeping the imaginary line stationary.

In a time interval Δt, a length vΔt of the sheet passes the imaginary line. The total charge contained in that length is ΔQ = (σ)(vΔt)(w). The current passing the imaginary line is I = ΔQ/Δt = σvw. The surface current density along the imaginary line is K = I/w = σv.
 
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