The expression for the drift velocity vdv_dvd of an electron in a conductor can be derived as follows:
- When an electric field EEE is applied across a conductor, the force FFF on an electron (charge −e-e−e) is:
F=−eEF=-eEF=−eE
- Using Newton's second law, the acceleration aaa of the electron is:
a=Fm=−eEma=\frac{F}{m}=\frac{-eE}{m}a=mF=m−eE
where mmm is the mass of the electron.
- Electrons in a conductor experience collisions at intervals, characterized by the relaxation time τ\tau τ, which is the average time between collisions.
- The drift velocity vdv_dvd is the average velocity gained by an electron under acceleration during the time τ\tau τ:
vd=aτ=−eEmτv_d=a\tau =\frac{-eE}{m}\tau vd=aτ=m−eEτ
This means the electrons drift opposite to the direction of the electric field. In summary, the drift velocity is given by:
vd=−eEτm\boxed{v_d=-\frac{eE\tau}{m}}vd=−meEτ
Where:
- eee is the magnitude of the electron charge,
- EEE is the applied electric field,
- τ\tau τ is the relaxation time,
- mmm is the electron mass.
This is the fundamental expression for the drift velocity of electrons in a conductor under an applied electric field.
