l6 alternators and synchronous motors

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    Alternators and

    Synchronous Motors

    Amit Mishra

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 2

    Topics to be DiscussedTopics to be Discussed

    Electro-mechanical Energy-conversion(EMEC) Machines.

    Power Considerations for

    A Generator.

    A Motor.

    Power Flow Diagram of

    A Generator.

    A Motor.

    Construction of Alternator

    Stator.

    Rotor.

    Cylindrical or Non-Salient Rotor.

    Salient or Projected Pole Rotor.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 3

    Rotating Magnetic Flux due to Three-Phase Currents.

    EMF Equation.

    Equivalent Circuit of

    A generator.

    A Motor.

    Synchronous Motor.

    Constant Speed Operation.

    Effect of Change in Mechanical Load.

    Effect of Change in Excitation.

    Synchronous Condenser.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 4

    Electro-mechanical Energy-conversion

    (EMEC) Machines

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 5

    AC and DC

    Generators and Motors

    When the electrical system is characterized by direct

    current, the machines are called dc motors and dc

    generators.

    Similarly, if the electrical system is characterized by

    alternating current, the machines are called ac

    motors and ac generators.

    Basically, the ac machines are not different from the

    dc machines.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 6

    Electrical Rotary Machine It has two parts :

    (1) the fixed part, called the stator, and

    (2) the moving part, called the rotor.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 7

    Generator Action

    Whenever the conductors of a coil cut across the

    magnetic flux (or are cut by it), an emfe is induced

    in it.

    This emf can supply a current i to an electricalload.

    Thus, an electrical powerei is generated.

    This is the Generator Action.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 8

    Motor Action

    Whenever current-carrying conductors of a coil areplaced (perpendicularly) in a magnetic flux, a force

    is experienced by each conductor.

    This gives rise to an electromagnetic torque Xe.

    This torque can rotate a mechanical load at anangular speed .

    Thus, a mechanical powerXe is generated.

    This is the motor action.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 9

    Both the generator action and motor action go hand

    in hand in an electro-mechanical energy-conversionmachine.

    Only the direction of power flow decides whetherthe machine is a generator or a motor.

    eei X [!

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 10

    Power Considerations for a Generator

    Large-size generators are usually called

    alternators.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 11

    Current-carrying coil in the armature kept in magnetic

    field experiences a torque,X

    e.

    This is the reaction torque and it opposes the applied

    torque Xm.

    In addition, there is also a frictional torque Xfthat

    opposes the applied toque Xm.

    m e fX X X!

    m e fX X X!

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 12

    Output Side I

    fris the resistance of the coil, the current i inthe circuit is given as

    L

    L

    ei e ir iRr R! !

    2 2 2

    orLei i r i ei i r iV ! !

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 13

    Power Flow Diagram

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 14

    Power Considerations for a Motor

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 15

    The conductors of the coil are cut through the

    magnetic field.

    An emfe is induced.

    This is the reaction emfand it opposes the applied

    voltage V.

    The difference ofVand emfe causes current i to

    flow in the coil.

    V ei V e ir r

    ! !

    2Vi ei i r !

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 16

    Output Side The motor converts electrical powerei into

    mechanical powerXe.

    A portionX

    f is lost in overcoming the friction. The remaining part Xm is supplied to the

    mechanical load.

    e f mX [ X [ X [ !

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 17

    Power Flow Diagram

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 18

    How a Generator Differs

    from a Motor1. EMF e and current iare in the same direction

    in generator, but opposite in motor.

    2. Torque Xe and rotation are opposite in ageneratorbut in same direction in a motor.

    3. Torque Xe and Xf are in same direction in a

    generatorbut opposite in a motor.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 19

    Synchronous Machines

    The rotor speed is exactly fixed by the supply

    frequency.

    They are synchronized with supply frequency.

    The other type of ac machines are called

    asynchronous (orInduction) motors.

    The synchronous generator(also called alternator) is

    the workhorse of the electric power industry.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 20Next

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 21

    General Characteristics of the Synchronous

    Machine The dc field circuit (on the rotor), is a rotatingelectromagnet controlled by the dc exciting current.

    The power supplied to the dc field circuit does notenter directly into the energy-conversion process.

    The armature circuit is placed on the stator and carriesthree-phase currents.

    The flow of real power through the system isdetermined by the mechanical input because themechanical system exchanges real power only.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 22

    Synchronous Speed

    For two-pole machine, one revolution of rotor represents 360mechanical degrees, and one cycle of emf represents 360

    electrical degrees.

    If the machine has 4 poles, one cycle of emf would be

    generated when the field structure (on the rotor) rotates

    through one-half revolution only. Thus, in a 4-pole machine two cycles of emf is generated when

    the rotor completes one revolution.

    If the machine has Ppoles, the number of cycles of emf in one

    revolution will be P/2.

    Thus,

    2e m

    PU U !

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 23

    If the rotor has a speed ofns revolutions per second,

    the frequency fof the induced emf would be

    2s

    Pf n!

    Synchronous speed(expressed in

    revolutions per minute) is

    2 120

    60s

    fN f

    P P! v v !

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 24

    What can be the maximum speed of a synchronous

    machine in India ?

    Ans. 3000 rpm. A machine cannot have less than 2

    poles.

    What can be the maximum speed of a synchronous

    machine in USA ?

    Ans. 3600 rpm.

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 25

    Example 1

    A six-pole ac generator is running and producing

    voltage at a frequency of 60 Hz.

    Calculate the revolutions per minute of the

    generator. If the frequency of the generated voltage is required

    to be decreased to 20 Hz, how many poles would be

    needed on the generator, if it still runs at the same

    speed ?

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    Tuesday, November 02, 2010 Ch. 14 Alternators and Synchronous Motors 26

    Solution

    120 120 60

    6

    s

    fN

    P

    v! ! ! 1200 rpm

    120 120 20

    1200

    fP

    N

    v

    ! ! ! 2

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