10a. Magnetic Induction

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    MAGNETIC|

    INDUCTION

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    Magnetic induction

    INTRODUCTION

    During the 1830s, several pioneeringexperiments with magnetically inducedemf were carried out by Michael

    Faraday (in England) and JosephHenry (in the US).

    They discovered that changing magnetic fieldinduces current.

    TERMINOLOGY INDUCE to produce (an electric current, electric

    charge, or magnetic change) without direct

    contact.

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    Magnetic Flux Flux is the number of field

    lines passing through anarea.

    fF cosBAABm ==rr

    == S nSm dABdAnB r

    F

    UNITS: 1Wb(Weber)=1Tm2

    If the surface is a plane

    with area A, and B isconstant in magnitude anddirection over the surfaceand makes an angle f

    fF cosNBAm=

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    Gauss law for magnetism

    fF cosBAABm

    ==rr

    0,

    === dABdAnB nnetmr

    F

    REMARKS Electric monopoles exists, but magnetic monopoles do

    not.

    The fundamental unit of magnetism is the magneticdipole.

    Magnetic field lines are always continuous, they neverhave end points.

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    INDUCTION EXPERIMENTS

    Induced emf

    If the magnetic flux through an area bounded by a circuit ischanged by any means, an emf equal in magnitude to the rateof change of the flux is induced in the circuit.

    We usually detect the emf by observing a current in the circuit.

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    Induced emf and Faradays law The common element in all induction effect is changing

    magnetic fluxthrough a circuit.

    The magnetic flux can be changed in many ways:

    The current producing the magnetic field may beincreased or decreased.

    The area of the circuit in a fixed magnetic field maybe increased or decreased.

    Changing the orientation of the circuit with respect tothe magnetic field.

    Magnets may be moved toward or away from thecircuit

    AdBBdAABddm

    rrrrrr

    +==F

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    FARADAYS LAW OF INDUCTION The induced emf in a circuit equals the negative time

    rate of change of magnetic flux through the circuit.

    dt

    dm

    F

    e -=

    dt

    d

    Nm

    F

    e -=

    DIRECTION OF INDUCED EMF

    Define a positive direction for the vector are A.

    The directions of A and the B determine the sign of themagnetic flux Fmand its rate of change dFm/dt.

    Curl the fingers of your right hand around A with yourright thumb in the direction of A. An emf or current in the

    circuit that has the same direction as your curled fingersis positive.

    Induced emf and Faradays law

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    Electromagnetic induction

    E does NOT depend on the resistance of the loop

    Iinduced depends on the resistance of the loop

    Iinduced

    =e

    R

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    Electromagnetic induction

    The () sign is related to the polarity ofe

    related to right-hand rule and Lenzs law

    To know the polarity of e, it is important to know whetherFB is increasing or decreasing

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    Lenzs Law is a convenient alternative method fordetermining the sign or direction of an induced current oremf or the direction of the associated non-electrostaticfield.

    Lenzs Law states that:

    The direction of any magnetic induction effect is suchas to oppose the cause producing it.

    Heinrich Friedrich Emil Lenz (1804-1865)

    Russian physicist

    1833: formulated Lenzs law

    Lenzs law

    The induced current tends to keep the original magnetic flux through the loop fro

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    Lenzs lawa simple principle

    If FBincreasese must create an induced magneticfield to decreaseFB !!!

    If FBdecreasese must create an induced magneticfield to increaseFB !!!

    Right-hand rule must be utilized.

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    Test run on Lenzs lawSSS

    NNN

    SSS

    NNN

    NNN

    SSS

    NNN

    SSS