Electrical circuit analysis lecture

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  • Phasor Relationships for Circuit Elements (8.4); Impedance and Admittance (8.5)Dr. HolbertFebruary 1, 2006

    ECE201 Lect-5

  • Phasor Relationships for Circuit Elements Phasors allow us to express current-voltage relationships for inductors and capacitors much like we express the current-voltage relationship for a resistor.A complex exponential is the mathematical tool needed to obtain this relationship.

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  • I-V Relationship for a ResistorSuppose that i(t) is a sinusoid:i(t) = IM ej(wt+q)Find v(t)Rv(t)+i(t)

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  • Computing the Voltage

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  • Class ExampleLearning Extension E8.5

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  • I-V Relationship for a CapacitorSuppose that v(t) is a sinusoid:v(t) = VM ej(wt+q)Find i(t)

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  • Computing the Current

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  • Phasor RelationshipRepresent v(t) and i(t) as phasors:V = VM qI = jwC VThe derivative in the relationship between v(t) and i(t) becomes a multiplication by jw in the relationship between V and I.

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  • Examplev(t) = 120V cos(377t + 30) C = 2mF

    What is V?What is I?What is i(t)?

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  • Class ExampleLearning Extension E8.7

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  • I-V Relationship for an InductorV = jwL ILv(t)+i(t)

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  • Examplei(t) = 1mA cos(2p 9.15107t + 30) L = 1mH

    What is I?What is V?What is v(t)?

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  • Class ExampleLearning Extension E8.6

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  • Circuit Element Phasor Relations(ELI and ICE man)

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    Element

    V/I Relation

    Phasor Relation

    Phase

    Capacitor

    I = C dV/dt

    I = j C V

    = CV (90

    I leads V

    by 90

    Inductor

    V = L dI/dt

    V = j L I

    = LI (90

    V leads I

    by 90

    Resistor

    V = I R

    V = R I

    = R I (0

    In-phase

  • ImpedanceAC steady-state analysis using phasors allows us to express the relationship between current and voltage using a formula that looks likes Ohms law:V = I ZZ is called impedance (units of ohms, W)

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  • ImpedanceResistor:V = I R

    The impedance is ZR = R

    Inductor:V = I jL

    The impedance is ZL = jwL

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  • ImpedanceCapacitor:

    The impedance is ZC = 1/jwC

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  • Some Thoughts on ImpedanceImpedance depends on the frequency, w=2fImpedance is (often) a complex number.Impedance is not a phasor (why?).Impedance allows us to use the same solution techniques for AC steady state as we use for DC steady state.

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  • Impedance Example:Single Loop Circuitw = 377Find VC20kW+1mF10V 0VC+

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  • Impedance ExampleHow do we find VC?First compute impedances for resistor and capacitor:ZR = 20kW= 20kW 0 ZC = 1/j (3771mF) = 2.65kW -90

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  • Impedance Example20kW 0+2.65kW -9010V 0VC+

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  • Impedance ExampleNow use the voltage divider to find VC:

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  • Low Pass Filter:A Single Node-pair CircuitFind v(t) for w=2p 30001kW0.1mF5mA 0+V

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  • Find Impedances1kW-j530W5mA 0+V

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  • Find the Equivalent Impedance5mA 0+VZeq

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  • Parallel Impedances

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  • Computing V

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  • Impedance Summary

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    Element

    Impedance

    Capacitor

    ZC = 1 / j(C = -1/(C ( 90(

    Inductor

    ZL = j(L = (L ( 90(

    Resistor

    ZR = R = R ( 0(

  • Class ExamplesLearning Extension E8.8Learning Extension E8.9

    ECE201 Lect-5