chapter 07 self and mutual inductances

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  • 8/2/2019 Chapter 07 Self and Mutual Inductances

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    Self and MutualInductances

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    Friday, April 20, 2012 Ch. 8 DC Transients 2

    Topics to be Discussed

    Self Inductance. Mutual Inductance.

    Magnetic Coupling.

    Coefficient of Coupling (k). Sign of Mutual Voltage.

    Dot Convention.

    Coupled Coils in Series.

    Coupled Coils in Parallel.

    Measurement of M.

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    Friday, April 20, 2012 Ch. 8 DC Transients 3

    Self Inductance

    It is the property of a coil, due to which anemf is induced in itself whenever there is achange in the current flowing through it.

    The self-induced emf is directly proportionalto the rate of change of current,

    The constantLis called the coefficient of selfinductance or simply inductance.

    ordt

    diLe

    dt

    die

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    Friday, April 20, 2012 Ch. 8 DC Transients 4

    The SI unit of inductance is henry (H).

    For a linear inductor, the magnitude ofinductance is independent of the magnitudeof current.

    An air-cored inductor is linear.

    When iron is used as core, the inductorbecomes nonlinear.

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    Friday, April 20, 2012 Ch. 8 DC Transients 5

    Energy stored in an Inductor :

    212

    W LI

    Inductance from Geometrical Viewpoint :

    l

    ANL

    2

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    Friday, April 20, 2012 Ch. 8 DC Transients 6

    Example 1

    A coil of 150 turns is linked with a flux of 0.01

    Wb when carrying a current of 10 A.

    Calculate the inductance of the coil.

    If this current is uniformly reversed in 0.01 s,

    calculate the emf induced

    Solution :

    H0.15

    10

    01.0150

    I

    NL

    10 ( 10)0.15

    0.01

    die L

    dt

    300 V

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    Example 2

    An air-cored solenoid with length 30 cm andinternal diameter 1.5 cm has a coil of 900turns wound on it.

    Estimate its inductance.

    Also, calculate the amount of energy storedin it when the current through the coil risesfrom 0 to 5 A.

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    Solution :

    Cross-sectional area of the solenoid,

    24222m1077.1)1075.0(

    rA

    mH0.6

    30.0

    )1077.1(104)900(472

    0

    2

    l

    ANL

    The energy stored,

    Next

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    Example 3

    The resistance and inductance of a coil are3 and 0.1 mH, respectively.

    What potential difference exists across the

    terminals of this coil at the instant when thecurrent is 1 A, but increasing at the rate of10 000 A per second ?

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    Solution :

    The potential difference across the coil will be dueto the drop across its resistance as well as the emfinduced in the inductance. Thus,

    V4

    100010101.031

    3

    dtdiLiRV

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    MUTUAL INDUCTANCE

    When interchange of energy takes placebetween two circuits, we say that the twocircuits are mutually coupled.

    Conductively coupledcircuits.

    Electrostaticallycoupled circuits.

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    Magnetically Coupled Circuits

    A part of magnetic flux produced by a coil in one circuitinterlinks with the coil in other circuit.

    Energy may be transferred from one circuit to the otherthrough the medium of magnetic flux that is common to bothcircuits.

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    Friday, April 20, 2012 Ch. 8 DC Transients 13

    When current in one coil changes, there occurs achange in the flux linking with the other. As a result, there

    is an induced emf in the other coil,

    or 121

    2dt

    diMe

    dt

    die

    The constant of proportionality M is calledcoefficient of mutual inductance, or simplymutual inductance.

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    Friday, April 20, 2012 Ch. 8 DC Transients 14

    A circuit element called mutual inductor does notexist.

    It is defined with reference to two pairs ofterminals. The physical device whose operation is basedinherently on mutual inductance is called transformer.

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    Friday, April 20, 2012 Ch. 8 DC Transients 15

    Magnetic Coupling

    Current i1 flowing in coil establishes a totalmagnetic flux 1.

    Only a part of this flux, 12, links with the

    coil

    . The remaining flux 11 is confined to coil

    itself.

    Thus, 1

    =11

    + 12

    .

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    Friday, April 20, 2012 Ch. 8 DC Transients 16

    The emf induced in coil due to the current i1 is

    given as

    dt

    dNe 1222 Also,

    1

    2dt

    diMe

    1

    12212

    122

    112 or

    did

    NMdt

    d

    NdtdiM

    Similarly, the expression for mutual inductancefrom coil to coil is

    2

    21

    121di

    dNM

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    Friday, April 20, 2012 Ch. 8 DC Transients 17

    l

    ANkNMMM

    121221

    Mutual Inductance

    from Geometrical Viewpoint :

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    Friday, April 20, 2012 Ch. 8 DC Transients 18

    Coefficient of Coupling (k)

    It is a measure of how close is the couplingbetween two coils.

    It gives an idea of what portion of the flux

    produced by one coil links with the other coil. The flux that links with the coil is only a

    part of 1.

    That is,

    where 0 k 1.112

    k

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    Friday, April 20, 2012 Ch. 8 DC Transients 19

    If k= 1, the coils are tightly coupled.

    The entire flux produced in one coil links withthe other

    If k= 0, the coils are magnetically isolated.

    It can be shown that

    21LL

    Mk

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    Friday, April 20, 2012 Ch. 8 DC Transients 20

    Example 4

    A solenoid consists of 2000 turns of wirewound on a length of 70 cm.

    A search coil of 500 turns having a meanarea of 30 cm2 is placed centrally inside thesolenoid.

    Assuming k= 1, calculate

    (a) the mutual inductance, and

    (b) the emf induced in the search coil if the currentin the solenoid uniformly changes at a rate of 260A/s.

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    Friday, April 20, 2012 Ch. 8 DC Transients 21

    Solution :

    mH5.38

    70.0

    103010450020001

    )(

    47

    21

    l

    ANkN

    Ma

    V1.4

    260105.38

    )(

    3

    1

    2dt

    diMeb

    Next

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    Friday, April 20, 2012 Ch. 8 DC Transients 22

    Example 5

    The numbers of turns in two coupled coils are600 and 1700, respectively.

    When a current of 6 A flows in the secondcoil, the total magnetic flux produced in this

    coil is 0.8 mWb, and the flux that links withthe first coil is only 0.5 mWb.

    Calculate L1, L2, kand M.

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    Friday, April 20, 2012 Ch. 8 DC Transients 23

    Solution :

    H0.226

    6

    108.01700

    3

    2

    222

    I

    NL

    0.625

    3

    3

    2

    21

    108.0

    105.0

    k

    H0.0282

    2

    2

    2

    2

    1

    21

    )1700(

    )600(226.0

    N

    NLL

    Since the self-inductance of a coil is proportional tothe square of number of turns,

    H0.05

    226.0028.0625.0

    21LLkM

    Next

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    Friday, April 20, 2012 Ch. 8 DC Transients 24

    DOT CONVENTION

    Note that the voltage due to mutualinductance is present independently of and inaddition to any voltage due to self-induction.

    In other words, the voltage across the

    terminals of coil is composed of two terms,

    dt

    diM

    dt

    diLv 2111

    Similarly,dt

    diM

    dt

    diLv 1222

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    Friday, April 20, 2012 Ch. 8 DC Transients 25

    Sign of Mutual Voltage

    The sign depends not only on the currentdirections, but also on the way the two coils arewound.

    Dot convention is a convenient way of

    determining the sign of mutual voltage, withoutgoing into the physical construction of the twocoils.

    The existence of mutual coupling betweentwo coils is indicated by a double-headedarrow.

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    Friday, April 20, 2012 Ch. 8 DC Transients 26

    A currententering thedotted terminal of one coilproduces an open-circuit voltage which is

    positively sensed at the dotted terminal of thesecond coil.

    DOT CONVENTION

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    Friday, April 20, 2012 Ch. 8 DC Transients 27

    (a) (b)

    (c) (d)

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    Friday, April 20, 2012 Ch. 8 DC Transients 28

    Fig. (a) is equivalent to Fig. (d), and

    Fig. (b) is equivalent to Fig. (c)

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    Friday, April 20, 2012 Ch. 8 DC Transients 29

    COUPLED COILS IN SERIES

    There are two ways of connecting two

    coupled coils in series.

    Current flowing in the series combinationmay produce the two fluxes

    either in the same direction (series aiding),

    or in the opposite direction (series opposing)

    MLLLsa 221

    MLLLso 221

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    Friday, April 20, 2012 Ch. 8 DC Transients 30

    COUPLED COILS IN PARALLEL

    1. Parallel aiding combination,

    2. Parallel opposing combination,

    MLL

    MLLLpa

    221

    2

    21

    MLL

    MLLLpo

    221

    2

    21

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    Friday, April 20, 2012 Ch. 8 DC Transients 31

    Measurement ofM

    4

    sosa LL

    M

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    Review

    Self Inductance. Mutual Inductance.

    Magnetic Coupling.

    Coefficient of Coupling (k).

    Sign of Mutual Voltage.

    Dot Convention.

    Coupled Coils in Series.

    Coupled Coils in Parallel. Measurement of M.

    N