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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 1 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Bruce Mayer, PE Registered Electrical & Mechanical Engineer BMayer@ChabotCollege.edu Engineering 43 Chp 9 [5-7] Complex Power
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 2 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Outline – AC SS Power cont. Effective or RMS Values Heating Value for Sinusoidal Signals Power Factor A Measure Of The Angle Between Current And Voltage Phasors within a Load Power Factor Correction Improve Power Transfer To a Load By “Aligning” Phasors Single Phase Three-Wire Circuits Typical HouseHold Power Distribution
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 3 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Outline – AC Steady State Power Instantaneous Power Concept For The Special Case Of Steady State Sinusoidal Signals Average Power Concept Power Absorbed Or Supplied During in Integer Number of Complete Cycles Maximum Average Power Transfer When The Circuit Is In Sinusoidal Steady State
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 4 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor Consider A Complex Current Thru a Complex Impedance Load The Current and Load-Voltage Phasors (Vectors) Can Be Plotted on the Complex Plane By Ohm & Euler in the Electrical Power Industry θ Z is the Power Factor Angle, or Simply the Phase Angle
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 5 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor cont The Phase Angle Can Be Positive or Negative Depending on the Nature of the Load Typical Industrial Case is the INDUCTIVE Load Large Electric Motors are Essentially Inductors Now Recall The General Power Eqn Measuring the Load with an AC DMM yields V rms I rms V is the BaseLine
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 6 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor cont.2 The Product of the DMM Measurements is the APPARENT Power The Apparent Power is NOT the Actual Power, and is thus NOT stated in Watts. Apparent Power Units = VA or kVA Now Define the Power Factor for the Load Some Load Types
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 7 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis pf – Why do We Care? Consider this case V rms = 460 V I rms = 200A pf = 1.5% Then P apparent = 92kVA P actual =1.4 kW This Load requires The Same Power as a Hair Dryer However, Despite the low power levels, The WIRES and CIRCUIT BREAKERS that feed this small Load must be Sized for 200A! The Wires would be nearly an INCH in Diameter
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 8 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example Power Factor The Local Power Company Services this Large Industrial Load Find I rms by Pwr Factor Then the I 2 R Loses in the 100 mΩ line Improving the pf to 94% Power company I lags V
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 9 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Power Factor cont For This Ckt The Effect of the Power Factor on Line Losses
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 10 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Complex Power Consider a general Ckt with an Impedance Ld Mathematically For this Situation Define the Complex Power for the Load: Converting to Rectangular Notation Active Power Reactive Power
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 11 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Complex Power cont Thus S in Shorthand Alternatively, Reconsider the General Sinusoidal Circuit S & Q are NOT Actual Power, and Thus all Terms are given Non-Watt Units S→ Volt-Amps (VA) Q → Volt-Amps, Reactive (VAR) P is Actual Power and hence has Units of W First: U vs. U rms
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 12 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Complex Power cont.2 Now in the General Ckt By Ohm’s Law In the Last Expression Equate the REAL and Imaginary Parts And Again by Ohm
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 13 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Complex Power cont.3 And by Complex Power Definition Using the Previous Results for P Similarly for Q So Finally the Alternative Expression for S
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 14 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Complex Power Triangle The Expressions for S Plotting S in the Complex Plane From The Complex Power “Triangle” Observe Note also That Complex Power is CONSERVED
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 15 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex Power For the Circuit At Right Z line =0.09 Ω + j0.3 Ω P load = 20 kW V load = 220 0° pf = 80%, lagging f = 60 Hz → ω = 377s -1 Lagging pf → Inductive From the Actual Power Thus inductive capacitive And Q from Pwr Triangle
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 16 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex Power cont Then S L Recall the S Mathematical Definition Alternatively Note also that [U*]* = U In the S Definition, Isolating the Load Current and then Conjugating Both Sides Lagging
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 17 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex Pwr cont.2 Now Determine V S Then V S Then The Phase Angle To find the Src Power Factor, Draw the I & V Phasor Diagram
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 18 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex Power kVAR For the Circuit At Right, Determine Real And Reactive Power losses in the Ln Real And Reactive Power at the Source Lagging pf → Inductive From the Actual Power Thus inductive capacitive And by S Definition
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 19 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex kVAR cont. Also from the S Relation Now the Power Factor Angle Then for Line Loses Quantitatively pf = cos(θ v − θ i ); hence I Lagging V
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 20 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example - Complex kVAR cont.2 Find Power Supplied by Conservation of Complex Power Then to Summarize the Answer P line = 4.685 kW Q line = 11.713 kVAR P S = 44.685 kW Q S = 37.552 kVAR In this Case
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 21 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor Correction As Noted Earlier, Most Industrial Electrical Power Loads are Inductive The Inductive Component is Typically Associated with Motors The Motor-Related Lagging Power Factor Can Result in Large Line Losses The Line-Losses can Be Reduced by Power Factor Correction To Arrive at the Power Factor Correction Strategy Consider A Schematic of a typical Industrial Load
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 22 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor Correction cont. Prior to The Addition of the Capacitor For The Capacitive Load After Addition of the Capacitor
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 23 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Power Factor Correction cont.2 Find θ new Cap is a Purely REACTIVE Load The Vector Plot Below Shows Power Factor Correction Strategy Use Trig ID to find Q C to give desired θ new QLQL QCQC Q L -Q C P Q new
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 24 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Trig ID Digression Start with the ID Solve for tan Recall tanθ new Or But: cosθ new = pf new Substituting
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 25 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example – pf Correction Kayak Centrifugal Injection-Molding Power Analysis Improve Power Factor to 95% Find S old Now Q old Adding A Cap Does NOT Change P Use Trig ID to Find Tan( new ) And by S Relation Roto-molding process
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 26 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis Example – pf Correction cont Then the Needed Q C Recall The Expression for Q C Roto-molding process Then C from Q C
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 27 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis WhiteBoard Work Let’s Work (w/ 2-changes) Problem 9.81 Determine at the input SOURCE –Voltage & Current –Complex Power –Δθ & pf 60 kVA
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 28 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 29 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 30 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 31 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 32 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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BMayer@ChabotCollege.edu ENGR-43_Lec-09-2_Complex_Power.ppt 33 Bruce Mayer, PE Engineering-43: Engineering Circuit Analysis
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