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Current density J→ =
J = I / A = nqv
n = number density of electrons
q = charge per carrier
v = ΔX / Δt
A = area
Conductivity =
J / E = σ (constant)
→ J = σE
σ depends ONLY on the medium, NOT on the conductor's dimensions
Conductivity and resistivity relation =
σ = 1 / ρ
(σ depends ONLY on the medium, not the conductor's dimensions)
Resistance of a conductor =
R = (ΔX)/(σA)
ΔX = length
σ = conductivity
A = cross-section
Why does current direction matter when calculating resistance =
resistance is dependent on ΔX and A (area)
these will change based on direction of current
what is resistance in series and in parallel =
series:
Rtot = R1 + R2
Both materials have DIFFERENT voltage drop
parallel:
1/Rtot = 1/R1 + 1/R2
Both materials have SAME same voltage drop

integral form of current =
I = ∬J⋅dS→
J = current density