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Consider a rectangular sample, a metal or an n-type semiconductor, with a length L, width W, and thickness D. A current I is passed along L, perpendicular to the cross-sectional area WD. The face W X L is exposed to a magnetic field intensity B. A voltmeter is connected across the width to read the Hall voltage VH.
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Solution
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Consider a slab of length L, width W, and thickness D as shown above. Let us take a small element "dX" in the length; its volume is given by dV = WDdX
If n = number of charge carriers per unit volume, then the total number of charge carriers in this volumetric element of thickness dX will be nWDdX
Therefore, total charge (dQ) = enWDdX
Thus, current (I) = dQ/dt = enWD(dX/dt)
Or, I = enWDv (where v is the charge velocity)
Or, ne = I/WDv
Magnetic force (Fm) = q(v x B)
Or, Fm = nevB = (I/WDv) x (vB) = IB/WD
Electrostatic force (Fe) = qE = neE
A potential develops across the width W, and is given by VH = EW. VH is called as the Hall potential.
It gives the value of the electric field E = VH/W
Therefore, Fe = neVH/W
In equilibrium, Fe = Fm
That is, neVH/W = IB/WD
Or, VH = IB/neD
This equation shows that the Hall potential is independent of the length and the width of the conductor slab. -
The atomic weight of gold is 196.97 grams.
i.e., 6.023 x 1023 atoms weigh 196.97 grams
or, 1 gram gold has 6.023 x 1023/196.97 atoms
The density of gold is 19.32 g/cm3.
i.e., 1 cm3 of gold weighs 19.32 grams.
Therefore, 1 cm3 has [6.023 x 1023/196.97] x 19.32 atoms
i.e., n = 5.9077 x 1022 atoms/cm3 or 5.9077 x 1028 atoms/m3
Gold is monovalent (valency = 1), therefore, total number of conduction electrons = total number of atoms
Thus, total number of conduction electrons per m3 = 5.9077 x 1028.
Therefore, total charge = ne = 5.9077 x 1028 x 1.6 x 10-19
VH = IB/neD
Or, B/VH = neD/I = 10-6 x 5.907728 x 1.6 x 10-19 / 100 x 10-3 (Given thickness = 1 micron and current = 100 mA)
B/VH = 94523.2 Tesla/Volt
Or, B/VH = 94523.2 x 10-6 / 10-6 Tesla/Volt
Or, B/VH= 0.0945232 Tesla/micro Volt



