Module 3 - Phasors-V3

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    Phasors

    EE 102 Circuits 2

    Module 3

    by:

    Cesar G. Manalo, Jr.

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    Rotating Vectors

    t

    v )45sin(1 ot

    45o

    45o

    1

    2

    145sin o2

    1Complex plane

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    Rotating Vectors

    t

    v )45sin(1 ot

    60o

    60o

    1

    y

    The value of y(the vertical component of the vector) always equals to the value

    of the sinusoid (v).

    v1

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    Rotating Vectors

    t

    v )45sin(1 ot

    45o

    45o

    1o45sin

    ttt o

    cossin)45sin(12

    1

    2

    1By trigonometric identities

    tcos2

    1

    tsin2

    1

    2

    1

    t

    v

    tcos2

    1 tsin2

    1

    1

    Thus sinusoids behaves like vectors (in as far a addition of sinusoids is

    concerned) with directions taken from their phase angles. A sinusoid withvector-like behavior is called a phasor.

    2

    1

    2

    1

    Complex plane

    Complex plane

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    Illustrative Problem 1

    Draw the phasor representation of the following sinusoids. Use RMS

    values of the sinusoids as the magnitude.1.

    2.

    3.

    4.

    e = 100 sin (t+75o)

    e = 100 sin (t+120o)

    e = - 100 cos (t-50o)

    e = 100 sin t + 50 cos (t -30o

    )

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    Polar Form of Phasor

    the phasor representation of vgiven in polar form is written like

    this;

    V (the angle inside the symbol )

    where (the effective value of v) and is the phase angle.2

    mV

    V

    Given a sinusoid;

    )sin( tVvm

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    Phasor Manipulation

    Given two phasors and , + is a third

    phasor equal to the vector addition of the two phasors. Later, another

    form of phasor called the Rectangular Form useful in phasor addtion,

    will be discussed.

    11 V

    Addition of Phasors

    22 V 11 V 22 V

    Given two phasors and , ( ) ( ) is a

    third phasor Vwhere,11 V

    Multiplication of Phasors

    22 V 11 V 22 V

    )())(( 2121 VVV

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    Phasor Manipulation

    Given two phasors and , ( ) / ( ) is a

    third phasor Vwhere,11 V

    Division of Phasors

    22 V 11 V 22 V

    )( 21

    2

    1 V

    VV

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    Checkpoint 1

    i

    e = Emsin (t+50o) L

    R

    Draw the phasor representation of the circuit below.

    L

    R

    oE 50

    I

    R

    XLtan

    Answer:

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    Illustrative Problem 2

    1. Draw the waveform and corresponding phasor

    diagram and polar form of

    e = 100 sin (t+20o) and i = 50 sin (t+80o).

    2. Solve for e = 100 sin t + 50 cos (t -30o) using

    phasors.

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    Phasor Representation of Circuit Components

    In a purely resistive circuit, the

    resulting current is in-phase with

    the driving source voltage. That

    would mean that if , the

    phasor representation of e, the

    Resistor i

    Re

    = Emsin t

    vR

    E

    resulting current isphasor will be whereEandIare the

    effective values of eand i, respectively. Since Im= Em/R, likewise,

    I = E/R, or using phasor representation,

    . Solving for R:

    I

    R

    EI

    o

    I

    E

    I

    ER 0

    Which means that in circuit analysis, Rcan be represented in phasor

    form with an angle of 0 degrees.

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    Phasor Representation of Circuit Components

    Resistor i

    Re

    = Emsin t

    vRo

    I

    E

    I

    ER 0

    Based on the results, R can also be treated like a phasor graphically

    represented as shown below:

    R

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    Illustrative Problem 3

    A purely resistance AC circuit has resistance R = 200and the

    sinusoidal alternating emf (voltage) device operates at amplitudeEm= 36.0 V.Find;

    a) Phasor representation of the emf.

    b) Phasor representation of the resulting current

    c) The time domain representation of the resulting current

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    Phasor Representation of Circuit Components

    In a purely capacitive circuit, the

    resulting current is leading the

    driving source voltage by 90o.

    That would mean that if ,

    the phasor representation of e, the

    Capacitive Reactance (XC)

    E

    resulting current isphasor will be whereEandIare the

    effective values of eand i, respectively. Since Im= Em/XC, likewise,

    I = E/XC, or using phasor representation,

    .Solving for XC:

    oI 90

    C

    o

    X

    EI

    90 o

    oC

    I

    E

    I

    EX 90

    )90(

    Which means that in circuit analysis, XCcan be represented in phasor

    form with an angle of -90 degrees.

    i

    Ce

    = Emsin t

    vC

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    Phasor Representation of Circuit Components

    Capacitive Reactance (XC)

    o

    oC

    I

    E

    I

    EX 90

    )90(

    i

    Ce

    = Emsin t

    vC

    Based on the results, XCcan also be treated like a phasor graphically

    represented as shown below:

    XC

    -90o

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    Illustrative Problem 4

    An AC circuit has resistance R = 200and capacitance C = 100 uF.

    What is the total impedance of the circuit at f = 50 Hz?

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    Phasor Representation of Circuit Components

    In a purely inductive circuit, the

    resulting current is lagging the

    driving source voltage by 90o.

    That would mean that if ,

    the phasor representation of e, the

    Inductive Reactance (XL)

    E

    oI 90

    o

    oL

    I

    E

    I

    EX 90

    )90(

    Thus, using similar analysis as the capacitive reactance, the inductive

    reactance can be represented by the phasor with phase angle of 90o.

    i

    L e

    = Emsin t

    vL

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    Phasor Representation of Circuit Components

    Inductive Reactance (XL)

    o

    oL

    I

    E

    I

    EX 90

    )90(

    i

    L e

    = Emsin t

    vL

    Based on the results, XLcan also be treated like a phasor graphically

    represented as shown below:XL

    +90o

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    Illustrative Problem 5

    A purely inductive AC circuit has an inductance of 230 henrys and

    the sinusoidal alternating emf (voltage) device with an effectivevalue of 70.7 volts at f = 60 Hz. Using phasor, solve for the RMS

    current.

    i

    L=23070.7 V

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    Phasor Representation of Circuit Components

    In an RC circuit, the combined effects

    of the resistance and the capacitance

    form what is called the impedance Z

    of the circuit defined as;

    Resitance + Capacitive Reactance (XC)

    )](tan[)(tan

    1

    1 R

    X

    R

    X

    C

    C Z

    E

    Z

    EI

    i

    e = Emsin t vCC

    vRsw.

    22

    CXRZ

    This impedance will produce a current that will lead the source

    voltage by an angle of less than 90o. computed as;

    R

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    Phasor Representation of Circuit Components

    In an RL circuit, the combined effects

    of the resistance and inductance form

    what is called the impedance Z of the

    circuit defined as;

    Resitance + Inductive Reactance (XL)

    )](tan[)(tan

    1

    1 R

    X

    R

    X

    L

    L Z

    E

    Z

    EI

    i

    e = Emsin t vL

    vRsw.

    22

    LXRZ

    This impedance will produce a current that will lag the source

    voltage by an angle of less than 90o, computed as;

    R

    L

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    Phasor Representation of Circuit Components

    In an RLC circuit, the combined

    effects of the resistance, capacitance

    inductance give a Z of;

    Resitance + Capacitive and Inductive Reactance

    )()](tan[)(tan

    1

    1 LCR

    XX

    R

    XX XX

    Z

    E

    Z

    EI

    LC

    LC

    i

    e = Emsin t vL

    vRsw.

    )()(

    )()(

    22

    22

    LCLC

    CLCL

    XXXXRZ

    XXXXRZ

    This impedance will produce a current that will lead the source

    voltage (XC> XL) or lag the source voltage (XL> XC).

    R

    L

    )()](tan[)(tan

    1

    1 CLR

    XX

    R

    XX XX

    Z

    E

    Z

    EI

    CL

    CL

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    Admittance

    The admittance Y of a circuit is defined as the reciprocal of its

    impedance Z.

    ZY

    1

    Admittance has SI units of Siemens or mho.

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    Thank You