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HALL EFFECT TRANSDUCERS -Priya Srivastava 090105801 E.I.E, 4 th yr.

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Page 1: C cp ppt

HALL EFFECT TRANSDUCERS

-Priya Srivastava

090105801

E.I.E, 4th yr.

Page 2: C cp ppt

TRANSDUCERS

It converts one form of energy into another form of energy,

either for measurement or for control.

If it is for measurement, then it is called as Input transducer

or sensor.

And if for control, then, Actuator.

Page 3: C cp ppt

Passive Transducers.

Active Transducers. TYPES

Page 4: C cp ppt

Active Transducers

Those which provide electrical signals in the

form of voltage & current.

Page 5: C cp ppt

HALL EFFECT TRANSDUCERS

It was discovered in 1879.

It belongs to one of the

Galvanomagnetic phenomena.

Page 6: C cp ppt

CONTD.

In which interaction between magnetic field & moving electrical charges

results in the development of forces that alter the motion of the charge.

The Hall effect is observed in all metals, but it is

prominent in semiconductor materials.

Page 7: C cp ppt

CONTD.

A thin strip of bismuth or n-type germanium is subjected to

magnetic field B normal to its surface, while it carries a current along the length of the strip, but

normal to B.

Page 8: C cp ppt

CONTD.

The magnetic field exerts a force(known as Lorentz force) on the electrons moving at a velocity

v, with the result that some of them drift towards the edges of

the strip.

The edge surfaces act like charged electrodes and the potential

difference measured b/w P & Q is known as Hall potential Eh, which increases with increase of B & I.

Page 9: C cp ppt

CONTD.The build up of the charge

on the edge surfaces will, in turn, develop an electric field(Hall field) of such a polarity that counteracts

the collection of charges on the surfaces.

The force on the electrons due to Hall field & Lorentz force balance each other

finally.

Page 10: C cp ppt

CONTD.

The time required to reach this equilibrium is about 10

to the power -14 s.

If e is the charge of the electron, then the Lorentz

force Bev & the force due to Hall field are equal to each

other.

Page 11: C cp ppt

• Hence, Bev = e /b• Or, = Bbv(volts)• If mobility of the charge carriers is represented by

χ, then v is given by• V= χ /L• The Hall coefficient depends on the no. of free

charge carriers per unit volume.• = ( )/(n )

n

)

Page 12: C cp ppt

APPLICATIONS

The Hall effect transducer is primarily suited for the

measurement of magnetic fields.

It is preferred for mapping of magnetic field around conductors carrying large currents under different

flow conditions,

With & wihtout the presence of metallic objects

in their vicinity.

Page 13: C cp ppt

CONTD. This transducer has made it possible to measure dc & ac

currents in conductors without interruption of the circuit and without making any electrical contact with the conductor.

The range of current that can be measured in this manner can be as low as 0-1 mA or as high as 0-1 kA.

Page 14: C cp ppt

CONTD.

In Instrumentation, the Hall element is highly valued for

its speed of response in detection of changes in the magnetic field to which it is

exposed.

The advantages are its small size & high sensitivity.

It is used as a Proximity detector, and also to

measure the change in the strength or direction of the

magnetic field due to displacement or nearness

of the test object.

Page 15: C cp ppt

THANK YOU