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= I ΔV.
Resistance
I ≡ dq / dt
is measured in Amperes (1 A ≡ 1 C / s).
Its direction is conventionally the direction of movement positive charge carriers would have,
from positive to negative potential, even though the charge carriers are actually negative. So electrons move in the opposite direction to the current!
Viewed as charges "drifting" down a wire, I = ρ vdrift A, where A is the cross-sectional area of the wire.
J = σ E = E / ρ
where here σ is the conductivity of the conductor and ρ is now the
resistivity.
Note that E is no longer zero
inside the conductor: it is the cause of the current. Assuming a uniform electric field, we have
J = ΔV / (ρ l)
and Ohm's law:
ΔV = I (ρ l / A)
where R is measured in Ω (Ohms).
≡ I R
ρ(T) = ρ0 + dρ/dT (T0) * (T - T0)
where α is the temperature coefficient of resistivity.
≡ ρ0 (1 + α (T - T0))
P = dU/dt
= d(q ΔV)/dt
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©2010, Kenneth R. Koehler. All Rights Reserved. This document may be freely reproduced provided that this copyright notice is included.
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