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1 
Power Distribution SystemPower Factor ImprovementBYDr. MunthearAlqaderi
GENERAL EQUATION 
FIG. 19.1 Defining the power delivered to a load.
RESISTIVE CIRCUIT 
For a purely resistive circuit (such as that in Fig. 19.2), vand i are in phase, and θ= 0°, as appearing in Fig. 19.3. 
FIG. 19.2 Determining the power delivered to a purely resistive load.
RESISTIVE CIRCUIT 
FIG. 19.3 Power versus time for a purely resistive load.
RESISTIVE CIRCUIT 
FIG. 19.4 Example 19.1.
RESISTIVE CIRCUIT 
FIG. 19.5 Power curve for Example 19.1.
APPARENT POWER 
FIG. 19.6 Defining the apparent power to a load.
 Most plant loads are Inductive and require a magnetic field to 
operate: 
 Motors 
 Transformers 
 Florescent lighting 
 The magnetic field is necessary, but produces no useful work 
 The utility must supply the power to produce the magnetic field and 
the power to produce the useful work: You pay for all of it! 
 These two types of current are the ACTIVE and REACTIVE 
components 
ACTIVE & REACTIVE POWERS
Advantages of Phasor Analysis 
0 
2 2 
Resistor ( ) ( ) 
( ) 
Inductor ( ) 
1 1 
Capacitor ( ) (0) 
C 
Z = Impedance 
R = Resistance 
X = Reactance 
X 
Z = =arctan( ) 
t 
v t Ri t V RI 
di t 
v t L V j LI 
dt 
i t dt v V I 
j C 
R jX Z 
R X 
R 
 
 
 
 
  
  
  
    
 
 
Device Time Analysis Phasor 
(Note: Z is a 
complex number but 
not a phasor)
INDUCTIVE CIRCUIT AND REACTIVE POWER 
FIG. 19.8 Defining the power level for a purely inductive load.
INDUCTIVE CIRCUIT AND REACTIVE POWER 
FIG. 19.9 The power curve for a purely inductive load.  QSVARindP
CAPACITIVE CIRCUIT 
For a purely capacitive circuit (such as that in Fig. 19.12), i leads vby 90°, as shown in Fig. 19.13. 
FIG. 19.12 Defining the power level for a purely capacitive load.
CAPACITIVE CIRCUIT 
FIG. 19.13 The power curve for a purely capacitive load. SQ  PVARcap
Power Factor Fundamental 
Definitions: 
Working /Active Power: Normally measured in kilowatts (kW). It does the "work" for the system-- providing the motion, torque, heat, or whatever else is required. 
Reactive Power:Normally measured in kilovolt- amperes-reactive (kVAR), doesn't do useful "work." It simply sustains the electromagnetic field. 
Apparent Power: Normally measured in kilovolt- amperes (kVA).Working Power and Reactive Power together make up apparent power.
Complex Power 
  
* 
cos( ) sin( ) 
P = Real Power (W, kW, MW) 
Q = Reactive Power (var, kvar, Mvar) 
S = Complex power (VA, kVA, MVA) 
Power Factor (pf) = cos 
If current leads voltage then pf is leading 
If current 
V I V I 
V I 
S V I j 
P jQ 
    
 
   
 
 
 
 
lags voltage then pf is lagging 
(Note: S is a complex number but not a phasor)
Power Factor 
P 
V 
P 
I 
I 
V 
(a) Purely Resistive Load (b) Resistive and Reactive Load 
 
Pav = VavIav cos()
Power Factor:The Beer Analogy 
Mug Capacity = Apparent Power (KVA) 
Foam = Reactive Power (KVAR) 
Beer = Real Power (kW) 
Power Factor = 
Beer (kW) 
Mug Capacity (KVA) 
Capacitorsprovide the Foam (KVAR), freeing up Mug Capacity so you don’t have to buy a bigger mug and/or so you can pay less for your beer ! 
kVAR 
Reactive 
Power 
kW 
Active 
Power 
kVA 
Apparent 
Power
18 
WHAT IS POWER FACTOR? 
PowerFactoristheratioofACTIVEPOWERtotheTOTALPOWER(apparentpower): 
=ActivePower=PTotalPowerS 
S=TotalpowerofGenerator(orused) 
P=Powerconsumedintheload(activepower) 
Q=Reactive power stored in magnetic field. Or wasted power 
Power Factor
19 
WHAT IS POWER FACTOR? 
VectorialRepresentation: 
S 
P.Q 
Φ 
P 
S 
Q 
j=90o 
Generator 
Load 
Total power = S = VI= (units = KVA) Active power = P = VI CosΦ = (units = KW) Reactive power= Q = VI SinΦ = (units = KVAR) 
Φ 
V 
I 
V = Voltage : VoltsI = Current : AmpereΦ = Physical displacement of V&I 
Power Factor = CosΦ
20 
WHAT IS LOW POWER FACTOR? 
Iftheratioofactivepower(P)tototalpower(S)islessthanone(unity)thenthepowerfactorislow,whichmeanstotalpowerisnotbeingconsumed. 
Generator 
Generator 
S = 100KVA 
P = 80KW 
P.F = 0.8 
Q = 60-KVAR 
S = 100KVA 
P = 100KW 
P.F = 1.0 
Q = 0 
Example: 
P.F. = 
P 
S
21 
WHAT IS LOW POWER FACTOR? 
Theaboveexampleclearlyindicatesthatageneratoroftotalpowerof100-KVAwillsupplymaximumof80-KWofactivepowertoaloadwithP.F.=0.8andthesamegeneratorwillsupplymaximumof100-KWofactivepowertoloadwithP.F=1.0.
22 
HOW TO IMPROVE THE POWER FACTOR ? 
ThepowerfactorcanbeimprovedbysupplyingKVARtotheloads(inductivetype) 
“CapacitorissourceofKVARs” 
Thereforethepowerfactorofconnectedloadcanbeimprovedbyinstallingpowerfactorimprovementcapacitors/capacitorbanks
59.7 kV 
17.6 MW 
28.8 MVR 
40.0 kV 
16.0 MW 
16.0 MVR 
17.6 MW 16.0 MW 
28.8 MVR -16.0 MVR 
Power System Notation 
Power system components are usually shown as 
“one-line diagrams.” Previous circuit redrawn 
Arrows are 
used to 
show loads 
Generators are 
shown as circles 
Transmission lines 
are shown as a 
single line
Reactive Compensation 
44.94 kV 
16.8 MW 
6.4 MVR 
40.0 kV 
16.0 MW 
16.0 MVR 
16.8 MW 16.0 MW 
6.4 MVR 0.0 MVR 
16.0 MVR 
Key idea of reactive compensation is to supply reactive 
power locally. In the previous example this can 
be done by adding a 16 Mvar capacitor at the load 
Compensated circuit is identical to first example with 
just real power load
Reactive Compensation, cont’d 
Reactive compensation decreased the line flow from 564 Amps to 400 Amps. This has advantages 
Lines losses, which are equal to I2 R decrease 
Lower current allows utility to use small wires, or alternatively, supply more load over the same wires 
Voltage drop on the line is less 
Reactive compensation is used extensively by utilities 
Capacitors can be used to “correct” a load’s power factor to an arbitrary value.
26 
HOW TO IMPROVE THE POWER FACTOR ? 
LOAD 
LOW POWER FACTOR 
LOAD 
IMPROVED POWER FACTOR 
CAPACITOR 
Fig.I
Calculation 
If the original inductive load has apparent power S1, then 
P = S1cos 1and Q1= S1sin 1= P tan 1 
If we desired to increased the power factor from cos1to cos2without altering the real power, then the new reactive power is 
Q2= P tan 2 
The reduction in the reactive power is caused by the shunt capacitor is given by 
QC= Q1–Q2= P (tan 1-tan 2)
28 
Calculation 
rms 
2 
1 2 
rms 
2 
C 
ωV 
P(tanθ tanθ ) 
ωV 
Q 
C 
 
  
The value of the required shunt capacitance is 
determined by the formula 
Notice that the real power, P dissipated by the 
load is not affected by the power factor correction 
because the average power due to the capacitor 
is zero
29 
Example 11.15 
When connected to a 120V (rms), 60Hz power line, a load absorbs 4 kW at a lagging power factor of 0.8. Find the value of capacitance necessary to raise the pf to 0.95.
30 
Solution 
5000VA 
0.8 
4000 
cos 1 
1    
 
P 
S 
If the pf = 0.8 then, 
cos1 = 0.8  1 = 36.87o 
where 1 is the phase difference between the voltage and current. 
We obtained the apparent power from the real power and the pf 
as shown below. 
The reactive power is 
sin 5000sin 36.87 3000VAR 1 1 1 Q  S   
31 
Solution 
4210.5VA 
0.95 
4000 
cos 2 
2    
 
P 
S 
When the pf raised to 0.95, 
cos2 = 0.95  2 = 18.19o 
The real power P has not changed. But the apparent power has 
changed. The new value is 
The new reactive power is 
sin 1314.4VAR 2 2 2 Q  S  
32 
Solution 
3000 1314.4 1685.6VAR 1 2 Q Q Q    C 
The difference between the new and the old reactive power is 
due to the parallel addition of the capacitor to the load. 
The reactive power due to the capacitor is 
The value of capacitance 
added is 
310.5μF 
2 (60)(120) 
1685.6 
2 2 
   
 rms  
C 
V 
Q 
C
In this example, demand was reduced to 8250 kVA from 10000 kVA. 1750KVA Transformer Capacity Release. The power factor was improved from 80% to 97% 
Before 
After 
Why do we install Capacitors?
34 
DISADVATAGES OF LOW POWER FACTOR 
1.Foragivenpowertobesupplied,thecurrentisincreased. 
2.Thecurrentthusincreasedin-returncausesincreaseincopperlosses(PL=I2R)anddecreaseintheefficiencyofbothapparatusandthesupplysystem,whichresultsinoverloadingandhenceburningoftheassociatedequipment.
35 
DISADVATAGES OF LOW POWER FACTOR 
3.Copperlossesintransformersalsoincreases. 
4.Generators,transformers,switches,transmissionlinesandotherassociatedswitchgearbecomesover-loaded. 
5.Voltageregulationofgenerators,transformersandtransmissionlinesincreases. 
6.Hence,costofgeneration,transmissionanddistributionincreases.
36 
NATURAL POWER FACTORS 
oCEILING FAN 0.5 TO 0.7 
oCABIN FAN0.5 TO 0.6 
oEXAUST FAN0.6 TO 0.7 
oSEWING MACHINE0.6 TO 0.7 
oWASHING MACHINE0.6 TO 0.7 
oRADIO0.9 
oVACUUM CLEANER0.6 TO 0.7 
oTUBE LIGHT0.5 TO 0.9 
oCLOCK0.9 
oELECTRONIC EQUIPMENT0.4 TO 0.95
37 
NATURAL POWER FACTORS 
oNEON SIGN0.5 TO 0.55 
oWINDOW TYPE AIR CONDITIONER0.62 TO 0.85 
oHAIR DRYERS0.7 TO 0.8 
oLIQUIDISER0.8 
oMIXER0.8 
oCOFFEE GRINDER0.75 
oREFRIGERATOR0.65 
oFREEZER0.7 
oSHAVER0.6 
oTABLE FAN0.5 TO 0.6
38 
NATURAL POWER FACTORS 
oMERCURY VAPOUR LAMPO.4 TO 0.6 
oINDUSTRIAL INDUCTION MOTOR: 
◘NO LOADO.18 
◘25% FULL LOAD0.56 
◘75% FULL LOAD0.81 
◘100% FULL LOAD0.85 
◘125% FULL LOAD0.86 
oCOLD STORAGEO.76 TO 0.80 
oCINEMAS0.78 TO 0.80 
oMETAL PRESSINGO.57 TO 0.72
MOTOR LOAD CHARACTERISTICS
40 
NATURAL POWER FACTORS 
oOIL MILLSO.51 TO 0.59 
oWOOLEN MILLSO.70 
oPOTTERIES0.61 
oCIGARETTE MANUFACTURING 0.80 
oFOUNDRIES0.59 
oSTRUCTURAL ENGINEERING0.53 TO 0.68 
oCHEMICALS0.72 TO 0.87 
oMUNICIPAL PUMPING STATIONS0.65 TO 0.75 
oOIL TERMINALS0.64 TO 0.83 
oROLLING MILLS0.60 TO 0.72
41 
NATURAL POWER FACTORS 
oPLASTIC MOLDING0.57 TO 0.73 
oFILM STUDIOSO.65 TO 0.74 
oHEAVY ENGINEERING WORK0.48 TO 0.75 
oRUBBER EXTRUSION AND MOLDING0.48 
oPHARMACEUTICALS0.75 TO 0.86 
oOIL AND PAINT MANUFACTURING 0.51 TO 0.69 
oBISCUIT FACTORY0.60 
oLAUNDRIES0.92 
oFLOUR MILLS 0.61 
oGLASS WORKS 0.87
42 
NATURAL POWER FACTORS 
oIRRIGATIONS PUMPSO.62 TO 0.80 
oREPAIR SHOP, AUTOMATIC LATHE,0.6 
WORKSHOP, SPINNING MILLS, 
WEAVING MILL 
oWELDING SHOP0.5 TO 0.6 
oHEAT TREATMENT SHOP, STEEL0.65 TO 0.8 
WORKS, ROLLING MILLS 
oTEXTILE0.65 TO 0.75 
oCEMENT0.8 TO 0.85 
oOFFICE BUILDING O.8 TO 0.85
Three Options for Applying Power Factor Capacitors: 
A) Fixed capacitors @ individual motors or @ MCC 
B) Automatic Banks at Main Switch Board 
C) De-tuned Automatic Capacitor Bank at Main Switch Board 
M 
M 
M 
M 
M 
A 
B 
C 
A 
Harmonic Source e.g. Variable Speed Drive 
Capacitor Locations
44 
ADVANTAGES OF POWER FACTOR IMPROVEMENT 
i.Addingcapacitor,releasescircuitcapacityformoreloadorrelievestheoverloadedcircuit.ThecapacitorKVARperKVAofloadincreaseisofparticularinterestasthisestablishestheaveragecostofsupplyingeachadditionalKVAofload. ThiscostcanbecomparedwiththecostperKVAofincreasingthetransformerorsupplycircuitratingandwouldjustifytheapplicationofcapacitors. 
PFI Capacitor’s addition, thus can be viewed in two lights.
45 
ADVANTAGES OF POWER FACTOR IMPROVEMENT 
ii.CapacitorsappliedtogivenloadreducetheI2Rlossesinthesupplycircuit.Fora70percentpowerfactorloadwith40-KVARofcapacitorsaddedforeach100KVAofcircuitcapacity,theI2Rlosswillbe59%ofitsformervalue.Thelossesarenotonlyreducedinthecircuitinwhichthecapacitorsareappliedbutinallthecircuitbacktoandincludingthesourcegenerator.
46 
ADVANTAGES OF POWER FACTOR IMPROVEMENT 
AutomaticPowerFactorimprovementcapacitorsorcapacitorbanksappliedontheloadendofcircuit, withlaggingpowerfactor(morethan95%loads), haveparticulareffects,oneormoreofwhichmaybethereasonfortheapplication. 
1.Improves the power factor at the source. 
2.Reduces system losses as current in conductors decreases.
47 
ADVANTAGES OF POWER FACTOR IMPROVEMENT 
3.Improves voltage level at the load. 
4.Decreases KVA loading on the source. 
5.Reduces investment in system facilities per KW of load supplied.

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Power factor

  • 1. 1 Power Distribution SystemPower Factor ImprovementBYDr. MunthearAlqaderi
  • 2. GENERAL EQUATION FIG. 19.1 Defining the power delivered to a load.
  • 3. RESISTIVE CIRCUIT For a purely resistive circuit (such as that in Fig. 19.2), vand i are in phase, and θ= 0°, as appearing in Fig. 19.3. FIG. 19.2 Determining the power delivered to a purely resistive load.
  • 4. RESISTIVE CIRCUIT FIG. 19.3 Power versus time for a purely resistive load.
  • 5. RESISTIVE CIRCUIT FIG. 19.4 Example 19.1.
  • 6. RESISTIVE CIRCUIT FIG. 19.5 Power curve for Example 19.1.
  • 7. APPARENT POWER FIG. 19.6 Defining the apparent power to a load.
  • 8.  Most plant loads are Inductive and require a magnetic field to operate:  Motors  Transformers  Florescent lighting  The magnetic field is necessary, but produces no useful work  The utility must supply the power to produce the magnetic field and the power to produce the useful work: You pay for all of it!  These two types of current are the ACTIVE and REACTIVE components ACTIVE & REACTIVE POWERS
  • 9. Advantages of Phasor Analysis 0 2 2 Resistor ( ) ( ) ( ) Inductor ( ) 1 1 Capacitor ( ) (0) C Z = Impedance R = Resistance X = Reactance X Z = =arctan( ) t v t Ri t V RI di t v t L V j LI dt i t dt v V I j C R jX Z R X R                 Device Time Analysis Phasor (Note: Z is a complex number but not a phasor)
  • 10. INDUCTIVE CIRCUIT AND REACTIVE POWER FIG. 19.8 Defining the power level for a purely inductive load.
  • 11. INDUCTIVE CIRCUIT AND REACTIVE POWER FIG. 19.9 The power curve for a purely inductive load.  QSVARindP
  • 12. CAPACITIVE CIRCUIT For a purely capacitive circuit (such as that in Fig. 19.12), i leads vby 90°, as shown in Fig. 19.13. FIG. 19.12 Defining the power level for a purely capacitive load.
  • 13. CAPACITIVE CIRCUIT FIG. 19.13 The power curve for a purely capacitive load. SQ  PVARcap
  • 14. Power Factor Fundamental Definitions: Working /Active Power: Normally measured in kilowatts (kW). It does the "work" for the system-- providing the motion, torque, heat, or whatever else is required. Reactive Power:Normally measured in kilovolt- amperes-reactive (kVAR), doesn't do useful "work." It simply sustains the electromagnetic field. Apparent Power: Normally measured in kilovolt- amperes (kVA).Working Power and Reactive Power together make up apparent power.
  • 15. Complex Power   * cos( ) sin( ) P = Real Power (W, kW, MW) Q = Reactive Power (var, kvar, Mvar) S = Complex power (VA, kVA, MVA) Power Factor (pf) = cos If current leads voltage then pf is leading If current V I V I V I S V I j P jQ             lags voltage then pf is lagging (Note: S is a complex number but not a phasor)
  • 16. Power Factor P V P I I V (a) Purely Resistive Load (b) Resistive and Reactive Load  Pav = VavIav cos()
  • 17. Power Factor:The Beer Analogy Mug Capacity = Apparent Power (KVA) Foam = Reactive Power (KVAR) Beer = Real Power (kW) Power Factor = Beer (kW) Mug Capacity (KVA) Capacitorsprovide the Foam (KVAR), freeing up Mug Capacity so you don’t have to buy a bigger mug and/or so you can pay less for your beer ! kVAR Reactive Power kW Active Power kVA Apparent Power
  • 18. 18 WHAT IS POWER FACTOR? PowerFactoristheratioofACTIVEPOWERtotheTOTALPOWER(apparentpower): =ActivePower=PTotalPowerS S=TotalpowerofGenerator(orused) P=Powerconsumedintheload(activepower) Q=Reactive power stored in magnetic field. Or wasted power Power Factor
  • 19. 19 WHAT IS POWER FACTOR? VectorialRepresentation: S P.Q Φ P S Q j=90o Generator Load Total power = S = VI= (units = KVA) Active power = P = VI CosΦ = (units = KW) Reactive power= Q = VI SinΦ = (units = KVAR) Φ V I V = Voltage : VoltsI = Current : AmpereΦ = Physical displacement of V&I Power Factor = CosΦ
  • 20. 20 WHAT IS LOW POWER FACTOR? Iftheratioofactivepower(P)tototalpower(S)islessthanone(unity)thenthepowerfactorislow,whichmeanstotalpowerisnotbeingconsumed. Generator Generator S = 100KVA P = 80KW P.F = 0.8 Q = 60-KVAR S = 100KVA P = 100KW P.F = 1.0 Q = 0 Example: P.F. = P S
  • 21. 21 WHAT IS LOW POWER FACTOR? Theaboveexampleclearlyindicatesthatageneratoroftotalpowerof100-KVAwillsupplymaximumof80-KWofactivepowertoaloadwithP.F.=0.8andthesamegeneratorwillsupplymaximumof100-KWofactivepowertoloadwithP.F=1.0.
  • 22. 22 HOW TO IMPROVE THE POWER FACTOR ? ThepowerfactorcanbeimprovedbysupplyingKVARtotheloads(inductivetype) “CapacitorissourceofKVARs” Thereforethepowerfactorofconnectedloadcanbeimprovedbyinstallingpowerfactorimprovementcapacitors/capacitorbanks
  • 23. 59.7 kV 17.6 MW 28.8 MVR 40.0 kV 16.0 MW 16.0 MVR 17.6 MW 16.0 MW 28.8 MVR -16.0 MVR Power System Notation Power system components are usually shown as “one-line diagrams.” Previous circuit redrawn Arrows are used to show loads Generators are shown as circles Transmission lines are shown as a single line
  • 24. Reactive Compensation 44.94 kV 16.8 MW 6.4 MVR 40.0 kV 16.0 MW 16.0 MVR 16.8 MW 16.0 MW 6.4 MVR 0.0 MVR 16.0 MVR Key idea of reactive compensation is to supply reactive power locally. In the previous example this can be done by adding a 16 Mvar capacitor at the load Compensated circuit is identical to first example with just real power load
  • 25. Reactive Compensation, cont’d Reactive compensation decreased the line flow from 564 Amps to 400 Amps. This has advantages Lines losses, which are equal to I2 R decrease Lower current allows utility to use small wires, or alternatively, supply more load over the same wires Voltage drop on the line is less Reactive compensation is used extensively by utilities Capacitors can be used to “correct” a load’s power factor to an arbitrary value.
  • 26. 26 HOW TO IMPROVE THE POWER FACTOR ? LOAD LOW POWER FACTOR LOAD IMPROVED POWER FACTOR CAPACITOR Fig.I
  • 27. Calculation If the original inductive load has apparent power S1, then P = S1cos 1and Q1= S1sin 1= P tan 1 If we desired to increased the power factor from cos1to cos2without altering the real power, then the new reactive power is Q2= P tan 2 The reduction in the reactive power is caused by the shunt capacitor is given by QC= Q1–Q2= P (tan 1-tan 2)
  • 28. 28 Calculation rms 2 1 2 rms 2 C ωV P(tanθ tanθ ) ωV Q C    The value of the required shunt capacitance is determined by the formula Notice that the real power, P dissipated by the load is not affected by the power factor correction because the average power due to the capacitor is zero
  • 29. 29 Example 11.15 When connected to a 120V (rms), 60Hz power line, a load absorbs 4 kW at a lagging power factor of 0.8. Find the value of capacitance necessary to raise the pf to 0.95.
  • 30. 30 Solution 5000VA 0.8 4000 cos 1 1     P S If the pf = 0.8 then, cos1 = 0.8  1 = 36.87o where 1 is the phase difference between the voltage and current. We obtained the apparent power from the real power and the pf as shown below. The reactive power is sin 5000sin 36.87 3000VAR 1 1 1 Q  S   
  • 31. 31 Solution 4210.5VA 0.95 4000 cos 2 2     P S When the pf raised to 0.95, cos2 = 0.95  2 = 18.19o The real power P has not changed. But the apparent power has changed. The new value is The new reactive power is sin 1314.4VAR 2 2 2 Q  S  
  • 32. 32 Solution 3000 1314.4 1685.6VAR 1 2 Q Q Q    C The difference between the new and the old reactive power is due to the parallel addition of the capacitor to the load. The reactive power due to the capacitor is The value of capacitance added is 310.5μF 2 (60)(120) 1685.6 2 2     rms  C V Q C
  • 33. In this example, demand was reduced to 8250 kVA from 10000 kVA. 1750KVA Transformer Capacity Release. The power factor was improved from 80% to 97% Before After Why do we install Capacitors?
  • 34. 34 DISADVATAGES OF LOW POWER FACTOR 1.Foragivenpowertobesupplied,thecurrentisincreased. 2.Thecurrentthusincreasedin-returncausesincreaseincopperlosses(PL=I2R)anddecreaseintheefficiencyofbothapparatusandthesupplysystem,whichresultsinoverloadingandhenceburningoftheassociatedequipment.
  • 35. 35 DISADVATAGES OF LOW POWER FACTOR 3.Copperlossesintransformersalsoincreases. 4.Generators,transformers,switches,transmissionlinesandotherassociatedswitchgearbecomesover-loaded. 5.Voltageregulationofgenerators,transformersandtransmissionlinesincreases. 6.Hence,costofgeneration,transmissionanddistributionincreases.
  • 36. 36 NATURAL POWER FACTORS oCEILING FAN 0.5 TO 0.7 oCABIN FAN0.5 TO 0.6 oEXAUST FAN0.6 TO 0.7 oSEWING MACHINE0.6 TO 0.7 oWASHING MACHINE0.6 TO 0.7 oRADIO0.9 oVACUUM CLEANER0.6 TO 0.7 oTUBE LIGHT0.5 TO 0.9 oCLOCK0.9 oELECTRONIC EQUIPMENT0.4 TO 0.95
  • 37. 37 NATURAL POWER FACTORS oNEON SIGN0.5 TO 0.55 oWINDOW TYPE AIR CONDITIONER0.62 TO 0.85 oHAIR DRYERS0.7 TO 0.8 oLIQUIDISER0.8 oMIXER0.8 oCOFFEE GRINDER0.75 oREFRIGERATOR0.65 oFREEZER0.7 oSHAVER0.6 oTABLE FAN0.5 TO 0.6
  • 38. 38 NATURAL POWER FACTORS oMERCURY VAPOUR LAMPO.4 TO 0.6 oINDUSTRIAL INDUCTION MOTOR: ◘NO LOADO.18 ◘25% FULL LOAD0.56 ◘75% FULL LOAD0.81 ◘100% FULL LOAD0.85 ◘125% FULL LOAD0.86 oCOLD STORAGEO.76 TO 0.80 oCINEMAS0.78 TO 0.80 oMETAL PRESSINGO.57 TO 0.72
  • 40. 40 NATURAL POWER FACTORS oOIL MILLSO.51 TO 0.59 oWOOLEN MILLSO.70 oPOTTERIES0.61 oCIGARETTE MANUFACTURING 0.80 oFOUNDRIES0.59 oSTRUCTURAL ENGINEERING0.53 TO 0.68 oCHEMICALS0.72 TO 0.87 oMUNICIPAL PUMPING STATIONS0.65 TO 0.75 oOIL TERMINALS0.64 TO 0.83 oROLLING MILLS0.60 TO 0.72
  • 41. 41 NATURAL POWER FACTORS oPLASTIC MOLDING0.57 TO 0.73 oFILM STUDIOSO.65 TO 0.74 oHEAVY ENGINEERING WORK0.48 TO 0.75 oRUBBER EXTRUSION AND MOLDING0.48 oPHARMACEUTICALS0.75 TO 0.86 oOIL AND PAINT MANUFACTURING 0.51 TO 0.69 oBISCUIT FACTORY0.60 oLAUNDRIES0.92 oFLOUR MILLS 0.61 oGLASS WORKS 0.87
  • 42. 42 NATURAL POWER FACTORS oIRRIGATIONS PUMPSO.62 TO 0.80 oREPAIR SHOP, AUTOMATIC LATHE,0.6 WORKSHOP, SPINNING MILLS, WEAVING MILL oWELDING SHOP0.5 TO 0.6 oHEAT TREATMENT SHOP, STEEL0.65 TO 0.8 WORKS, ROLLING MILLS oTEXTILE0.65 TO 0.75 oCEMENT0.8 TO 0.85 oOFFICE BUILDING O.8 TO 0.85
  • 43. Three Options for Applying Power Factor Capacitors: A) Fixed capacitors @ individual motors or @ MCC B) Automatic Banks at Main Switch Board C) De-tuned Automatic Capacitor Bank at Main Switch Board M M M M M A B C A Harmonic Source e.g. Variable Speed Drive Capacitor Locations
  • 44. 44 ADVANTAGES OF POWER FACTOR IMPROVEMENT i.Addingcapacitor,releasescircuitcapacityformoreloadorrelievestheoverloadedcircuit.ThecapacitorKVARperKVAofloadincreaseisofparticularinterestasthisestablishestheaveragecostofsupplyingeachadditionalKVAofload. ThiscostcanbecomparedwiththecostperKVAofincreasingthetransformerorsupplycircuitratingandwouldjustifytheapplicationofcapacitors. PFI Capacitor’s addition, thus can be viewed in two lights.
  • 45. 45 ADVANTAGES OF POWER FACTOR IMPROVEMENT ii.CapacitorsappliedtogivenloadreducetheI2Rlossesinthesupplycircuit.Fora70percentpowerfactorloadwith40-KVARofcapacitorsaddedforeach100KVAofcircuitcapacity,theI2Rlosswillbe59%ofitsformervalue.Thelossesarenotonlyreducedinthecircuitinwhichthecapacitorsareappliedbutinallthecircuitbacktoandincludingthesourcegenerator.
  • 46. 46 ADVANTAGES OF POWER FACTOR IMPROVEMENT AutomaticPowerFactorimprovementcapacitorsorcapacitorbanksappliedontheloadendofcircuit, withlaggingpowerfactor(morethan95%loads), haveparticulareffects,oneormoreofwhichmaybethereasonfortheapplication. 1.Improves the power factor at the source. 2.Reduces system losses as current in conductors decreases.
  • 47. 47 ADVANTAGES OF POWER FACTOR IMPROVEMENT 3.Improves voltage level at the load. 4.Decreases KVA loading on the source. 5.Reduces investment in system facilities per KW of load supplied.