Test: Hall Effect - Electronics and Communication Engineering (ECE) MCQ

Hall coefficient is defined as:

ρ_c = charge density
σ_n = nμ_nq and σ_p = Pμ_pq
Hall coefficient depends on the hole and electron concentration, and also on the mobility of carriers.
In a metal, the gap between the conduction band and the valence band is very low.
The concentration of ions (n) is very high in metals.
So, the Hall coefficient will be zero almost for the metal as the Hall coefficient is inversely proportional to the concentration (n).

• Hall effect is the production of a voltage difference across an electrical conductor that is transverse to an electric current and to an applied magnetic field perpendicular to the current
• When current flows in a semiconductor and magnetic field are applied perpendicularly, then the voltage is produced across the two side plates of the semiconductor bar, this is known as the Hall effect
• The Voltage produced is known as Hall voltage

The following diagram resembles an experimental setup for the observation of the Hall effect

 

Here we could observe that 

• Hall voltage VH is developed transverse to the current in the conductor
• The hall voltage is also developed perpendicular to the applied magnetic field

Hall effect finds major applications in

• Hall sensors
• Used for proximity and displacement measurements
• Used in RPM,speed measurements

Hall Effect is basically the production of voltage (known as hall voltage) across conductor transverse to an electric current and to an applied magnetic field perpendicular to the current.
Application of Hall Effect:

• To determine the type of semiconductor
• To calculate the carrier concentration
• To determine mobility (hall mobility)
• To Measure magnetic flux density

From Hall Effect we have:

Where the hall coefficient is given as:

Hall Effect can be used to measure the carrier concentration and type of semiconductor.

Concept:
The hall voltage VA is given by:

ρ_c: Charge density
R_H: Hall coefficient

W is the side across which the magnetic field is applied.
Calculation:
W = Thickness = 4 mm, I = 1 mA, VH = 0.005 V, B = 0.1 Wb/m²

Since hall voltage is positive, the majority charge carriers will be holes, with the concentration calculated as:

p ≈ 3 × 10¹⁹ m^-3

Hall coefficient is defined as:



We can find the electron concentration as:


ρc = charge density
σ_n = nμ_nq and σ_p = pμ_pq

• Hall coefficient depends on the hole and electron concentration, and also on the mobility of carriers.
• In an insulator, the gap between the conduction band and the valence band is very high.
• Conductivity will be almost zero in the insulator
• As conductivity zero in insulator then mobility also almost zero.
• So, the hall coefficient will be zero almost for the insulator.

Hall Effect Transducers:

• when a conductor is kept perpendicular to the magnetic field and a direct current is passed through it, It results in an electric field perpendicular to the directions of both the magnetic field and current with a magnitude proportional to the product of the magnetic field strength and current. The voltage so developed is very small and it is difficult to detect it. But in semiconductors such as germanium, this voltage is enough for measurement with a sensitive moving coil instrument. This phenomenon is called the Hall effect.
• Commercial Hall effect transducers are made from germanium or other semiconductor materials.
• Hall effect transducers find applications in instruments that measure magnetic field with small flux densities.
• Hall effect pick up can be used for measurement of current by magnetic field produced due to flow of current.   
• Hall effect element may be used for measuring a linear displacement or location of the structural elements in cases where it is possible to change the magnetic field strength by variation in geometry of the magnetic structure.
• The main advantage of hall effect transducers is that they are non-contact device with small size and high resolution.
• The main drawback of hall effect transducers is highly sensitive to temperature variation and variation of Hall coefficient from plate to plate, thereby requiring individual calibration in each case.

Vh=BI/wρ
=5=2/ (5*10^-2*10⁵*1.6*10^-19)
=0.002V.

R=1/ρ
=1/(1.6*10^-19*10²⁰)
=0.0625.

µ=σR
σ =µ/R
=5*10^-4/5
=0.0001 S/m.