Force on a Current Carrying Conductor
Step 1: Consider a conductor placed in a magnetic field.
Let
\[
n
\]
be the number density of free electrons.
In a small volume
\[
AL,
\]
number of electrons is
\[
N=nAL.
\]
Step 2: Magnetic force on one electron.
Lorentz force is
\[
\vec F_e=-e(\vec v_d\times \vec B).
\]
Magnitude:
\[
F_e=e v_d B\sin\theta.
\]
Step 3: Force on all electrons.
\[
F=N e v_d B\sin\theta.
\]
Substituting \(N=nAL\),
\[
F=nALev_dB\sin\theta.
\]
Using
\[
I=neAv_d,
\]
we obtain
\[
F=BIL\sin\theta.
\]
Hence
\[
\boxed{
F=BIL\sin\theta
}
\]
and in vector form
\[
\boxed{
\vec F=I(\vec L\times\vec B)
}
\]