- #1
erisedk
- 374
- 7
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 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??