HALL
EFFECT
Hall effect, named after its discoverer Edwin Herbert Hall (U.S
Physicist) in 1879, is a conduction phenomenon which is defined as the development of a transverse electric field in a solid
conducting material when it is placed under the influence of mutually
perpendicular electric and magnetic fields.
Hall effect is observed a the result of force due to magnetic field in a
moving electric charge carrier. No matter we consider current as the movement
of electrons, holes or as a combination of both ( in the case of semi
conductors) a perpendicular magnetic field displaces the moving electric charge
in the same direction side ways at right angles to it.
Thus, the accumulation of a specific polarity in one side results
in the development of a measureable potential difference within the conductor
which is indicated as positive or negative by the detector.
Besides solids Hall effect is observed in plasma ( ionised gases) also, but it is
significantly different from what we observe in solids.
Then,
Fnet = q (E + v x B )
The net force experienced by a hole moving along y- direction is
the sum of forces due to electric field and Magnetic field along y- direction
Force due to electric field
= qEy
Force due to magnetic field
= q x y- component of v x B
= q [ - vx Bz - Bz vz]
= q [ -vx Bz] ( since vz = 0 )
Fnet = Fy = q( Ey – vxBz)
In order to maintain steady state condition, Ey must balance the product vx Bz. Then, Fnet = 0. This condition occurs when the holes are shifted slightly in
the negative y direction due to B. As the forces are
now balanced, the lateral force becomes zero as they drift along the bar.
This establishment of Ey is known as Hall
effect and the resulting voltage is known as Hall
voltage Vhall = Ey w
Drift velocity Vx= Jx / q po
So, Ey= Jx Bz /q po= RH Jx Bz
Po = JxBz/qEy
= (Ix/wt )Bz / q (v/w )
No comments:
Post a Comment