Current at a Junction: Does Current Density Change?

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SUMMARY

The discussion centers on the behavior of current density at electrical junctions, specifically through the lens of Kirchhoff's Current Law and the equation i = n.e.A.vd. It is established that while the number of charge carriers (n) and electronic charge (e) remain constant, the cross-sectional area (A) can change, affecting current density. The drift velocity (vd) is influenced by the electric field (E), which is derived from current (i) and the physical parameters of the conductors. The consensus is that current density does not remain constant at a junction unless specifically designed to do so.

PREREQUISITES
  • Understanding of Kirchhoff's Current Law
  • Familiarity with the equation i = n.e.A.vd
  • Knowledge of electric field calculations in conductors
  • Basic concepts of charge carriers and drift velocity
NEXT STEPS
  • Research the impact of cross-sectional area changes on current density
  • Explore advanced applications of Kirchhoff's Current Law in circuit design
  • Study the relationship between electric field and drift velocity in conductors
  • Investigate specific designs that maintain constant current density at junctions
USEFUL FOR

Electrical engineers, physics students, and professionals involved in circuit design and analysis will benefit from this discussion, particularly those focused on current behavior at junctions.

erisedk
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From the very straightforward kirchhoffs current law, based on conservation of charge, currents entering the junction is equal to the currents leaving the junction.

I was wondering how using the equation i = n.e.A.vd, we could justify that the currents change between different paths at a junction.

n is the number of charge carriers per unit volume, that clearly doesn't change
e= electronic charge, doesn't change
A, cross-sectional area of the wire, I believe this changes, but I'm not too sure
vd, drift velocity = eEτ/m, where e is electronic charge, τ is relaxation time, m is mass, and E is electric field across the conductor, i don't think τ changes, but E I'm not sure about again.

Furthermore, does current density stay the same at a junction??
 
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erisedk said:
From the very straightforward kirchhoffs current law, based on conservation of charge, currents entering the junction is equal to the currents leaving the junction.

I was wondering how using the equation i = n.e.A.vd, we could justify that the currents change between different paths at a junction.

n is the number of charge carriers per unit volume, that clearly doesn't change
e= electronic charge, doesn't change
A, cross-sectional area of the wire, I believe this changes, but I'm not too sure
vd, drift velocity = eEτ/m, where e is electronic charge, τ is relaxation time, m is mass, and E is electric field across the conductor, i don't think τ changes, but E I'm not sure about again.

Furthermore, does current density stay the same at a junction??
I think the problem with this approach is getting E. Normally, E would be calculated from i (via Kirchoff's law) and the physical parameters of the conductors.

The current density would normally not stay the same through the node unless the node were designed specifically to produce that result.
 

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