written 3.9 years ago by |
The motion of carriers in the presence of electric and magnetic fields gives rise to a number of galvanometric effects. The most important of these effects is the Hall Effect.
When a semiconductor sample carrying a current I is placed in a transverse magnetic field B, then an electric field E0 is induced in the specimen, in the direction perpendicular to both B and I. This phenomenon is called the Hall Effect.
The Hall Effect may be used for determining whether a semiconductor is n-type or p-type by finding the carrier concentration and calculating the mobility μ, by measuring the conductivity σ.
Expression for Hall voltage:
In equilibrium condition the electric field intensity EH due to Hall Effect exerts a force on charge carriers which just balance the magnetic force.
qEH=BqVd
q is the magnitudeof charge carrier and Vd is the drift speed
EH=BVd....(1)
If d is the width of the conductor i.e., distance between upper and lower surfaces, then the Hall voltage is
VH=EHd
VH=VdBd....(2)
Thus, the measured Hall voltage gives a value for the drift speed of the charge carriers if d and B are known.
If J is the current density, nq is the charge carrier density, I is the current, w is the width of specimen in direction of magnetic field then,
J=nqVd.....(3)
J=Iwd.....(4)
Vh=VdBd.....from (2)
VH=JBdnq.....from (3)
VH=Iwd×Bdnq.....from(4)
∴ VH=BInqw
As,
J=IA.....(5)
We can obtain the charge carrier density n by measuring the current in the sample. We can express the drift speed from (3) and (5) as-
Vd=InqA
Where A=wd and A is the cross-sectional area of the conductor.
VH=IBdnqA
As,
VH=BInqw
VH=RHIBw
Therefore hall voltage is given by -
VH=RHIBw
where RH=1nq is the Hall coefficient.
This relationship shows that a properly calibrated conductor can be used to measure the magnitude of an unknown magnetic field.