Power Electronics chapter02-1

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    1

    Power

    Electronics

    CHAPTER 2

    Power Computat ions

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    2

    Power

    Electronics

    Power & Energy

    Instantaneous power

    Absorbing

    Power

    Supplying

    Power

    )()()(   t it vt  p   Time-varying quantity

    • PASSIVE SIGN CONVENTION

    0)(   t  p   0)(   t  p

    Energy

      2

    1

    )(t 

    t dt t  pW 

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    3

    Power

    Electronics

    Power

    Electronics

    Power & Energy

    Average power (real power, active power)

     

      T t 

    T t 

    o

    o

    o

    o

    dt t it vT 

    dt t  pT 

     P    )()(1

    )(1

     P  

    Periodic voltage and current produce a periodic instantaneous power.

    Power generally

    means average power.

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    Power

    Electronics

    Inductors & Capacitors Inductors

    )(2

    1)(   2 t  Lit w  

    t 0   t 0+T t 0+2T 

    i L(t 0)

    i L(t 0+T )

    i L(t ) In the steady state, the

    inductor current is periodic

    )()( 00   t iT t i  L L  

    )()(1

    )( 000

    0

    t idt t v L

    T t i  LT t 

    t   L L  

     

    0)(1

    )()(  0

    000  

      dt t v

     Lt iT t i

    T t 

    t   L L L

      0)()()(1   0

    0

     

    t vt vavg dt t vT 

      L L

    T t 

    t   L

    In the steady state,

    - the average inductor voltage is zero.

    - the net change of the inductor current during one switching period is zero.

    - no net energy transfer, i.e. the average power of the inductor is zero (PL = 0)

    Inductor volt-second balance

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    Power

    Electronics

    Inductors & Capacitors

    • Volt-seconds over T  equal zero. 

    v L

    i L

    Increasing inductor current

     Inductor absorbs power

    and energy from externalcircuits

    v L

    i L

    Decreasing inductor current

     Inductor supplies power

    and energy to external

    circuits

    dt 

    di Lv   L L  

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    Power

    Electronics

    Inductors & Capacitors Capacitors

    In the steady state, the

    capacitor voltage is periodic

    t 0   t 0+T t 0+2T 

    vC (t 0)

    vC (t 0+T )

    vC (t )

    )()( 00   t vT t v C C   

    )()(1

    )( 000

    0

    t vdt t iC 

    T t v C T t 

    t   C C   

     

    0)(1

    )()(  0

    000  

      dt t i

    C t vT t v

    T t 

    t   C C C      0)()()(

    1   0

    0

     

    t it iavg dt t iT 

      C C 

    T t 

    t   C 

    In the steady state,

    - the average capacitor current is zero.

    - the net change of the capacitor voltage during one switching period is zero.

    - no net energy transfer, i.e. the average power of the capacitor is zero (PC = 0)2

    2

    1)(   Cvt w  

    Capacitor ampere-second balance

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    Power

    Electronics

    Inductors & Capacitors

    • Amp-seconds over T  equal zero. 

    Increasing capacitor

    voltage

    Capacitor absorbs

    power and energy

    from external circuits

    (charging)

    Decreasing

    capacitor voltage

    Capacitor

    supplies power

    and energy to

    external circuits

    (discharging)

    dt 

    dvC i   C C  

    vC 

    iC 

    vC 

    iC 

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    Energy Recovery

    Fuel injector solenoid in automobile

    freewheeling pathfor induct current

    continuity

    Inductors and capacitors must be energized and de-energized by switching

    operations

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    • Reminding

    • Without freewheeling path, the Tr is damaged by the overvoltage when it turns off.

    • Inductor current continuity must be provided by circuit design

    Energy Recovery During Tr on (0 < t < t1)

    CC  L   V v  

        t 

    CC 

    CC  L

     L L  L

    t V 

    d V  Lid v Lt i 00 0

    1

    )0()(

    1

    )(      )(

    2

    1)(   2 t  Lit w  

    Inductor current linearly

    increases.

    Inductor stores energy inside

    itself.

    freewheeling path

    for induct current

    continuity

    dt 

    di Lv   L L 

    )()(   t it i  L s  

    (+)

    Source supplies

    power

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    Power

    Electronics

    Energy Recovery During Tr off (t1 < t < T)

    diode turns on due to

    the inductor current

    continuity

     L

    t V t i   CC  L

    )()(   11  

    T t t e L

    t V et it i

      t t CC t t 

     L L

       

      

       

    1

    /)(1/)(

    1

    11)()(    

    Inductor current exponentially decreases.

    Inductor releases its energy to resistor.

     R L 

     LT 

    t V dt 

    T dt 

     L

    t V 

    T V 

    dt t iT 

    V  I V  P 

    CC t T 

    CC CC 

     sCC S S S 

    20

    11

    )(1

    2

    1

    0

    0

    1

    1

    0S i

    average power

    supplied by

    source

     LT 

    t V  P  P    CC S  R

    2

    2

    1

    average power

    absorbed by

    resistor

    0)(    L P 

    Heat

    energy

    Power

    loss

    lossy element

    (+)

    Source supplies

    power

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    Energy Recovery

    Recycle energy

    stored in elements

    energystorageelement

    re overeuse

    store

    energyenergy

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    Electronics

    Energy Recovery During Tr on (0 < t < t1)

    CC  L   V v  

        t 

    CC CC  L

     L L L

    t V d V 

     Lid v

     Lt i

    000

    1)0()(

    1)(      

    • Inductor current linearly increases.

    • Inductor stores energy inside itself.

    )()(   t it i  L s  

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    Energy Recovery

    • The inductor current linearly decreases.

    • The energy stored in the inductor is recovered to the source &

    the source is absorbing power.

    During Tr off (t1 < t < T)

    CC  L   V v  

      1111

    1   2211

    )(11

    t t t t t  L

     L

    t V d V 

     Lt id v

     Lt i   CC CC 

    t   CC  L

    t   L L  

     

      

           

    )()(   t it i  LS   

    No power

    loss

    (+)

    Source supplies

    power

    (-)

    Source absorbs

    power

    14

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    Electronics

    Effective value (RMS)

    Effective value (Root-Mean-Square value)

    The effective value of a periodic voltage (current) delivers the sameaverage power to a resistor as dc voltage (current) does.

     R

    V  P    dc

    2

     R

    V  P 

      eff  

    2

    T T T 

    dt t vT  R

    dt  R

    t v

    T dt t it v

    T dt t  p

    T  P 

    0

    2

    0

    2

    00

    )(11

    )(1)()(

    1)(

    1

    • For a dc voltage • For a ac voltage

    V eff 2

      T 

    rmseff     dt t vT 

    V V 0

    2 )(1

      T 

    rms   dt t iT 

     I 0

    2)(

    1

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