SlideShare una empresa de Scribd logo
1 de 29
TRUBA INSTITUTE OF ENGG. & INFO. TECHNOLOGY
                     BHOPAL




                              A
                      TECHNICAL SEMINAR
                             ON
                   “TESTING OF DC MACHINE”


  SUBMITTED TO:-                            SUBMITTED BY:-
MR. PRIYANK NEMA                          MRITYUNJAI KUMAR ANAND
                                          ROLL NO. 0114EX101035



        DEPARTMENT OF ELECTRICAL & ELECTRONICS ENGG.

                   SESSION-2012-13
CONTENTS
1. Testing method of dc m/c.
2. simple/direct test .
     (a) Explanation,(b) Numerical (C)
   Disadvantage .
3 .Swinburne’s test.
4.Hopkinsion’s test
TESTING OF DC MACHINE
 Q:- Why testing are required ?


Ans-Machines are tested for finding out losses,
    efficiency and temperature rise. For
    small m/c we used DIRECT LOADING
    test and for large shunt m/c, INDIRECT MET-
    HOD are used.
TESTING METHOD ARE


 Simple / Direct test.


 Swinburne’s / Indirect Method test.

 Hopkinson’s / Regenerative / Back - to -
  Back / Heat –run test.
Simple / Direct test
 This method is suitable
  only for SMALL DC
  m/c. In direct, method
  the DC m/c is
  subjected to rated load
  and the entire o/p
  power is wasted. The
  ratio of o/p power to i/p
  power gives the
  efficiency of DC m/c.
EFFICIENCY MOTOR
 Motor o/p={ω(s1-s2)r× 9. 81}
 Motor i/p= VtI.
 ή(motor)={o/p}/{i/p}.
           = [{ω(s1-s2)r× 9. 81}×100]/VtI
where; s1&s2 are the tension on the belt.
       ω=2πn(motor speed in rad/sec
        r=radius of pulley in meters(=1/2 out
 side pulley dia+1/2 belt thickness)
       Vt=terminal voltage & I=line current.
NUMERICAL

 A full load break test on a small d.c m/c shunt
  motor ,give the following data
   Spring balance readings 25 kg & 9 kg
   Out side pulley diameter 19.5 cm
   Belt thickness 0.50 cm
   Motor speed 1500 rpm
   Applied voltage 230 v
   Line current 12.5 A
Calculate the shaft torque, shaft power & motor
 efficiency at rated load.
SOLUTION
 Shaft torque=(S1-S2)×Effective radius
    =(25.9)[(19.5/2)+(0.5/2)]×(1/100)kg-m
    =16×0.1×9.81 Nm=15.7 Nm
  Shaft power=ω×Shaft torque
                =[(2π×1500)/60]×15.7=2470w
  Motor i/p=Vti=230×12.5=2875w
  ή(motor efficiency at rated
  load)=[2470/2875]×100=85.6%
DISADVANTAGES
 The spring balance readings are not steady.


 Friction torque does not const. At a particular
  setting of handwheels H1&H2
INDIRECT METHOD

 In this method ,no load m/c losses are first
  measured by a suitable test and then
  additional losses on load are determined
  from the m/c data ,in order to calculate the
  m/c efficiency .
 The simplest method of measuring the no
  load m/c losses is by SWINBURNE’S
  METHOD.
SWINBURNE’S METHOD
 As this is no load
  test ,it can’t be
  performed on a dc
  series motor
 In this method, the
  m/c whether it is a
  MOTOR or
  GENERATOR, is run
  as a no load shunt
  motor at rated
  speed
 If Ia0 and If are the no load armature and
  field current respectively .Then power
  absorbed by the armature (=Vt×Iao) is equal
  to the no load rotational loss W0 plus a small
  amount armature circuit loss Ia0^2 ×ra.
 No load rotational loss W0=Vt×Iao- Ia0^2 ×ra.
 Here armature circuit resistance ra includes
  the brush contact resistance also.
 Shunt field loss=Vt×If.
 Let IL be the load current at which m/c
  efficiency is required.
 Generator efficiency
       Generator o/p=Vt×IL
       Armature current Ia=IL+If
      Armature circuit loss= Ia^2×ra
      ra=armature circuit resistance when hot.
 Total loss=W0+ Ia^2×ra+Vt×If
  ή(Generator)=[1-{(W0+
  Ia^2×ra+Vt×If)}/{(Vt×IL+ W0+ Ia^2×ra+Vt×If)}]
 Motor efficiency
 When m/c is working as a motor then
    Ia=IL-If
  Motor i/p=Vt×IL
 ή(motor efficiency)=[1-
 {(W0+Ia^2×ra+If×Vt)}/{(Vt×IL)}]
NUMERICAL
 A 400 v,20kw dc shunt motor takes 2.5 A
  when running light. For an armature
  resistance of 800Ω and brush drop 2V,find full
  load efficiency.
SOLUTION
 Field current If=400/800=.5A
  No load armature current Ia0=2.5-0.5=2.0A
  Constant no load rotational loss
  W0=Vt×Ia0-Ia0^2×ra-Vb×Ia.
      =400×2.0-2^2×0.5-2×2=794w.
  Total constant loss=W0+Vt×If=794+400×0.5
                                  =994w
  At full load, let IL=Line current=Ia+If
Power i/p=Power o/p +total loosses
  Vt×IL =20,000+994+Ia^2×ra+Vb×Ia
 400(Ia+0.5)=20,000+994+Ia^2+2×Ia
        Ia=56.22A
Armature ohmic losses=56.22^2×0.5=1580.34w
Brush drop losses=56.22×2=112.44w.
Total losses=994+1580.34+112.44=2686.78w.
Power i/p=20,000+2686.78=22686..78w.
ή(motor at full load)
  =(20.000/22686.78)×100=88.157%
ADVANTAGES
 Low power is required for testing even large
  m/c, since only no load losses are to be
  supplied from the main.

 It is convenient and economical.


 The efficiency can be calculated at any load
  because constant losses are known.
DISADVANTAGES
 As the test is on no load, it doesn’t indicate whether
  the commutation on full load is satisfactory and
  whether the temperature rise would be within
  specified limit.
 THIS TEST CAN’T BE APPLIED FOR A SERIES
  MOTOR because speed of series motor is very high at
  no load ,it is not possible to run series motor on no
  load.
 Note:-In comparison to other the armature cu
  losses is so small that it may be neglected &
  constant loss may be take equal to no load i/p
Regenerative/Hopkinson’s
method.
  In this method ,two identical d.c m/c are
   coupled ,both mechanically & electrically and
   are tested simultaneously. One of the m/c
   made to run as a MOTOR and it derives the
   other m/c as GENERATOR .
 For this test m/c 1 is as
  a dc shunt motor by a
  starter & brought upto
  rated speed with
  switch S open .Bothe
  the m/c run at same
  speed ,because these
  are MECHANICALLY
  coupled .
TO PERFORM THE TEST FOLLOWING
PROCEDURE IS ADOPTED

 M/c 1(motor) is started through starter & its
  field rheostat is adjusted so that it runs at
  normal speed. The m/c 1(Motor) will drive m/c
  2(Generator).The switch S is initially kept
  open.
 The excitation of m/c 2 is gradually increased
  ( by decreasing the field circuit resistance).till
  the volt metre 1 reads ZERO.Then switch S is
  closed.
 M/c 2 is now floating neither taking any
 current from the supply nor delivering any
 current .Any desired load can be put on the
 set by adjusting the shunt field regulators.The
 m/c with lower excitation will act as a MOTOR
 and other m/c will act as a GENERATOR.
Let V=supply voltage
      I2=Armature current of m/c 2(Generator)
      I1= Armature current of m/c 1(motor) .
      If2=Field current of m/c 2(Generator).
       If1=Field current of m/c 1(Motor).
       Ra=Armature resistance of each m/c
 Motor i/p power =V(I+I2)=V×I1
 Generator o/p power=V×I2. ............(1)
  If both the m/c have same efficiency ή,then
  o/p of motor =ή×i/p
               =ήV(I+I2)= V×I1 =Generator i/p .
  o/p of Generator =ή×i/p .

  =ή×ήV×I1=ή^2V(I1)............(2)
From equ (1) & (2).
ή^2V(I1)=V×I2.
sqrt{(I2/(I1)}
EFFICIENCY
Armature circuit loss in Generator =I2^2×ra .
 Armature circuit loss in Motor=I1^2×ra .
 Power drawn from supply= V×I.
No load rotational loss in two m/c=W0=
       V×I-ra(I1^2+I2^2) .
No load rotational loss for each m/c=W0/2 .
Generator o/p= I2^2×ra.
Generator loss=Wg=(W0/2)+V×If2+ I2^2×ra.
ή(g)=[1-(Wg)/(V×I2+Wg)]
 Motor i/p=V(I1+If1)
 Total motor losses Wm=(W0/2)+ V×If1
 +I1^2×ra .
ή( Motor)=[1-(Wm)/V(I1+If2)]
ADVANTAGE
 Total power taken from the supply is very
  low. Therefore this method is very
  economical.
 The temperature rise and the commutation
  condition can be checked under rated load
  condition.
 Large m/c can be tested at rated load
  without consuming much power from the
  supply.
 Efficiency at different load can be determine.
DISADVANTAGES
 The main disadvantage of this method is the
  necessity two practically identical m/c to be
  available
THANK
        YOU....

Más contenido relacionado

La actualidad más candente

La actualidad más candente (20)

Operating Principle of DC Generator
Operating Principle of DC GeneratorOperating Principle of DC Generator
Operating Principle of DC Generator
 
Active, reactive and apparent power
Active, reactive and apparent powerActive, reactive and apparent power
Active, reactive and apparent power
 
Power factor improvement
Power factor improvement Power factor improvement
Power factor improvement
 
Transient in Power system
Transient in Power systemTransient in Power system
Transient in Power system
 
Transformer
TransformerTransformer
Transformer
 
Phase Controlled Rectifiers
Phase Controlled RectifiersPhase Controlled Rectifiers
Phase Controlled Rectifiers
 
Electrical machines lecture notes
Electrical machines lecture notesElectrical machines lecture notes
Electrical machines lecture notes
 
Braking methods of induction motor
Braking methods of induction motorBraking methods of induction motor
Braking methods of induction motor
 
single phase energy meter.pptx
single phase energy meter.pptxsingle phase energy meter.pptx
single phase energy meter.pptx
 
O.C & S.C Test, Sumpner or back to back Test, Condition for maximum efficienc...
O.C & S.C Test, Sumpner or back to back Test, Condition for maximum efficienc...O.C & S.C Test, Sumpner or back to back Test, Condition for maximum efficienc...
O.C & S.C Test, Sumpner or back to back Test, Condition for maximum efficienc...
 
Choppers
ChoppersChoppers
Choppers
 
speed control of three phase induction motor
speed control of three phase induction motorspeed control of three phase induction motor
speed control of three phase induction motor
 
Representation of loads
Representation of loadsRepresentation of loads
Representation of loads
 
Three Point Starter: Diagram and Working Principle
Three Point Starter: Diagram and Working PrincipleThree Point Starter: Diagram and Working Principle
Three Point Starter: Diagram and Working Principle
 
Testing of DC Motors
Testing of DC MotorsTesting of DC Motors
Testing of DC Motors
 
Transformer
TransformerTransformer
Transformer
 
Motor starter
Motor starterMotor starter
Motor starter
 
Chapter 4
Chapter 4Chapter 4
Chapter 4
 
Armature windings
Armature windingsArmature windings
Armature windings
 
VSC based DSTATCOM
VSC based DSTATCOMVSC based DSTATCOM
VSC based DSTATCOM
 

Destacado

ee2259-lab-manual
 ee2259-lab-manual ee2259-lab-manual
ee2259-lab-manual
surya721327
 
53669836 brake-test-on-a-d
53669836 brake-test-on-a-d53669836 brake-test-on-a-d
53669836 brake-test-on-a-d
thicman
 

Destacado (20)

ee2259-lab-manual
 ee2259-lab-manual ee2259-lab-manual
ee2259-lab-manual
 
D.c. machine[1]
D.c. machine[1]D.c. machine[1]
D.c. machine[1]
 
Dc motor
Dc motorDc motor
Dc motor
 
Dc motor ppt
Dc motor pptDc motor ppt
Dc motor ppt
 
Dc motors and its types
Dc motors and its typesDc motors and its types
Dc motors and its types
 
Speed control of DC Machine
Speed control of DC MachineSpeed control of DC Machine
Speed control of DC Machine
 
Dc machines 1
Dc machines 1Dc machines 1
Dc machines 1
 
Electrical machines I (II-EEE)
Electrical machines I (II-EEE)Electrical machines I (II-EEE)
Electrical machines I (II-EEE)
 
53669836 brake-test-on-a-d
53669836 brake-test-on-a-d53669836 brake-test-on-a-d
53669836 brake-test-on-a-d
 
Huminity and Social Science Lab Manual
Huminity and Social Science Lab ManualHuminity and Social Science Lab Manual
Huminity and Social Science Lab Manual
 
Corrected1
Corrected1Corrected1
Corrected1
 
Lab manual psd v sem experiment no 1
Lab manual psd v sem experiment no 1Lab manual psd v sem experiment no 1
Lab manual psd v sem experiment no 1
 
Lab manual psd v sem experiment no 3
Lab manual psd v sem experiment no 3Lab manual psd v sem experiment no 3
Lab manual psd v sem experiment no 3
 
Lab manual psd v sem experiment no 4
Lab manual psd v sem experiment no 4Lab manual psd v sem experiment no 4
Lab manual psd v sem experiment no 4
 
Dc machines 3
Dc machines 3Dc machines 3
Dc machines 3
 
Lab manual psd v sem experiment no 2
Lab manual psd v sem experiment no 2Lab manual psd v sem experiment no 2
Lab manual psd v sem experiment no 2
 
OPTIMAL PID CONTROLLER DESIGN FOR SPEED CONTROL OF A SEPARATELY EXCITED DC MO...
OPTIMAL PID CONTROLLER DESIGN FOR SPEED CONTROL OF A SEPARATELY EXCITED DC MO...OPTIMAL PID CONTROLLER DESIGN FOR SPEED CONTROL OF A SEPARATELY EXCITED DC MO...
OPTIMAL PID CONTROLLER DESIGN FOR SPEED CONTROL OF A SEPARATELY EXCITED DC MO...
 
AUXILIARY POWER SUPPLY SCHEME FOR THERMAL POWER PLANT
AUXILIARY POWER SUPPLY SCHEME FOR THERMAL POWER PLANTAUXILIARY POWER SUPPLY SCHEME FOR THERMAL POWER PLANT
AUXILIARY POWER SUPPLY SCHEME FOR THERMAL POWER PLANT
 
Experiment 1 DC Machine
Experiment 1 DC MachineExperiment 1 DC Machine
Experiment 1 DC Machine
 
Blackboard at Blackboard – Swinburne’s LMS migration
Blackboard at Blackboard – Swinburne’s LMS migrationBlackboard at Blackboard – Swinburne’s LMS migration
Blackboard at Blackboard – Swinburne’s LMS migration
 

Similar a testing of dc machine

Synchronous machines and Induction motors
Synchronous machines and Induction motorsSynchronous machines and Induction motors
Synchronous machines and Induction motors
James Dunford
 

Similar a testing of dc machine (20)

SWINBURNE’S TEST
SWINBURNE’S TESTSWINBURNE’S TEST
SWINBURNE’S TEST
 
Electrical machines-lab-i-ee0209
Electrical machines-lab-i-ee0209Electrical machines-lab-i-ee0209
Electrical machines-lab-i-ee0209
 
UNIT-III-Testing of DC Machines.ppt
UNIT-III-Testing of DC Machines.pptUNIT-III-Testing of DC Machines.ppt
UNIT-III-Testing of DC Machines.ppt
 
Field test
Field test Field test
Field test
 
Emii
EmiiEmii
Emii
 
Nonlinear integral control for dc motor speed control with unknown and variab...
Nonlinear integral control for dc motor speed control with unknown and variab...Nonlinear integral control for dc motor speed control with unknown and variab...
Nonlinear integral control for dc motor speed control with unknown and variab...
 
Nonlinear integral control for dc motor speed control
Nonlinear integral control for dc motor speed controlNonlinear integral control for dc motor speed control
Nonlinear integral control for dc motor speed control
 
Experimental results of vector control for an asynchronous machine
Experimental results of vector control for an asynchronous machineExperimental results of vector control for an asynchronous machine
Experimental results of vector control for an asynchronous machine
 
Traction Motors and Control
Traction Motors and ControlTraction Motors and Control
Traction Motors and Control
 
Synchronous machines
Synchronous machinesSynchronous machines
Synchronous machines
 
Synchronous machines and Induction motors
Synchronous machines and Induction motorsSynchronous machines and Induction motors
Synchronous machines and Induction motors
 
Performance of dc motors experiment 2
Performance of dc motors experiment 2Performance of dc motors experiment 2
Performance of dc motors experiment 2
 
269010454 electrical-machines-lab-manual-for-petrochemaical
269010454 electrical-machines-lab-manual-for-petrochemaical269010454 electrical-machines-lab-manual-for-petrochemaical
269010454 electrical-machines-lab-manual-for-petrochemaical
 
PARAMETER IDENTIFICATION AND MODELLING OF SEPARATELY EXCITED DC MOTOR
PARAMETER IDENTIFICATION AND MODELLING OF SEPARATELY EXCITED DC MOTOR PARAMETER IDENTIFICATION AND MODELLING OF SEPARATELY EXCITED DC MOTOR
PARAMETER IDENTIFICATION AND MODELLING OF SEPARATELY EXCITED DC MOTOR
 
Pe lab converted
Pe lab convertedPe lab converted
Pe lab converted
 
Third lecture of a three phase induction machine
Third lecture of a three   phase induction machineThird lecture of a three   phase induction machine
Third lecture of a three phase induction machine
 
Torque - Slip Characteristic of a three phase induction motor
Torque - Slip Characteristic of a three   phase induction motorTorque - Slip Characteristic of a three   phase induction motor
Torque - Slip Characteristic of a three phase induction motor
 
Torque - Slip Characteristic of a three phase induction motor
Torque - Slip Characteristic of a three phase induction motorTorque - Slip Characteristic of a three phase induction motor
Torque - Slip Characteristic of a three phase induction motor
 
Performance Characteristics of SEIGUsed In Wind Energy Conversion System
Performance Characteristics of SEIGUsed In Wind Energy Conversion SystemPerformance Characteristics of SEIGUsed In Wind Energy Conversion System
Performance Characteristics of SEIGUsed In Wind Energy Conversion System
 
DC Motors
DC MotorsDC Motors
DC Motors
 

testing of dc machine

  • 1. TRUBA INSTITUTE OF ENGG. & INFO. TECHNOLOGY BHOPAL A TECHNICAL SEMINAR ON “TESTING OF DC MACHINE” SUBMITTED TO:- SUBMITTED BY:- MR. PRIYANK NEMA MRITYUNJAI KUMAR ANAND ROLL NO. 0114EX101035 DEPARTMENT OF ELECTRICAL & ELECTRONICS ENGG. SESSION-2012-13
  • 2. CONTENTS 1. Testing method of dc m/c. 2. simple/direct test . (a) Explanation,(b) Numerical (C) Disadvantage . 3 .Swinburne’s test. 4.Hopkinsion’s test
  • 3. TESTING OF DC MACHINE Q:- Why testing are required ? Ans-Machines are tested for finding out losses, efficiency and temperature rise. For small m/c we used DIRECT LOADING test and for large shunt m/c, INDIRECT MET- HOD are used.
  • 4. TESTING METHOD ARE  Simple / Direct test.  Swinburne’s / Indirect Method test.  Hopkinson’s / Regenerative / Back - to - Back / Heat –run test.
  • 5. Simple / Direct test  This method is suitable only for SMALL DC m/c. In direct, method the DC m/c is subjected to rated load and the entire o/p power is wasted. The ratio of o/p power to i/p power gives the efficiency of DC m/c.
  • 6. EFFICIENCY MOTOR  Motor o/p={ω(s1-s2)r× 9. 81}  Motor i/p= VtI.  ή(motor)={o/p}/{i/p}. = [{ω(s1-s2)r× 9. 81}×100]/VtI where; s1&s2 are the tension on the belt. ω=2πn(motor speed in rad/sec r=radius of pulley in meters(=1/2 out side pulley dia+1/2 belt thickness) Vt=terminal voltage & I=line current.
  • 7. NUMERICAL  A full load break test on a small d.c m/c shunt motor ,give the following data Spring balance readings 25 kg & 9 kg Out side pulley diameter 19.5 cm Belt thickness 0.50 cm Motor speed 1500 rpm Applied voltage 230 v Line current 12.5 A Calculate the shaft torque, shaft power & motor efficiency at rated load.
  • 8. SOLUTION  Shaft torque=(S1-S2)×Effective radius =(25.9)[(19.5/2)+(0.5/2)]×(1/100)kg-m =16×0.1×9.81 Nm=15.7 Nm Shaft power=ω×Shaft torque =[(2π×1500)/60]×15.7=2470w Motor i/p=Vti=230×12.5=2875w ή(motor efficiency at rated load)=[2470/2875]×100=85.6%
  • 9. DISADVANTAGES  The spring balance readings are not steady.  Friction torque does not const. At a particular setting of handwheels H1&H2
  • 10. INDIRECT METHOD  In this method ,no load m/c losses are first measured by a suitable test and then additional losses on load are determined from the m/c data ,in order to calculate the m/c efficiency .  The simplest method of measuring the no load m/c losses is by SWINBURNE’S METHOD.
  • 11. SWINBURNE’S METHOD  As this is no load test ,it can’t be performed on a dc series motor  In this method, the m/c whether it is a MOTOR or GENERATOR, is run as a no load shunt motor at rated speed
  • 12.  If Ia0 and If are the no load armature and field current respectively .Then power absorbed by the armature (=Vt×Iao) is equal to the no load rotational loss W0 plus a small amount armature circuit loss Ia0^2 ×ra.  No load rotational loss W0=Vt×Iao- Ia0^2 ×ra.  Here armature circuit resistance ra includes the brush contact resistance also.  Shunt field loss=Vt×If.
  • 13.  Let IL be the load current at which m/c efficiency is required.  Generator efficiency Generator o/p=Vt×IL Armature current Ia=IL+If Armature circuit loss= Ia^2×ra ra=armature circuit resistance when hot. Total loss=W0+ Ia^2×ra+Vt×If ή(Generator)=[1-{(W0+ Ia^2×ra+Vt×If)}/{(Vt×IL+ W0+ Ia^2×ra+Vt×If)}]
  • 14.  Motor efficiency When m/c is working as a motor then Ia=IL-If Motor i/p=Vt×IL ή(motor efficiency)=[1- {(W0+Ia^2×ra+If×Vt)}/{(Vt×IL)}]
  • 15. NUMERICAL  A 400 v,20kw dc shunt motor takes 2.5 A when running light. For an armature resistance of 800Ω and brush drop 2V,find full load efficiency.
  • 16. SOLUTION  Field current If=400/800=.5A No load armature current Ia0=2.5-0.5=2.0A Constant no load rotational loss W0=Vt×Ia0-Ia0^2×ra-Vb×Ia. =400×2.0-2^2×0.5-2×2=794w. Total constant loss=W0+Vt×If=794+400×0.5 =994w At full load, let IL=Line current=Ia+If
  • 17. Power i/p=Power o/p +total loosses Vt×IL =20,000+994+Ia^2×ra+Vb×Ia 400(Ia+0.5)=20,000+994+Ia^2+2×Ia Ia=56.22A Armature ohmic losses=56.22^2×0.5=1580.34w Brush drop losses=56.22×2=112.44w. Total losses=994+1580.34+112.44=2686.78w. Power i/p=20,000+2686.78=22686..78w. ή(motor at full load) =(20.000/22686.78)×100=88.157%
  • 18. ADVANTAGES  Low power is required for testing even large m/c, since only no load losses are to be supplied from the main.  It is convenient and economical.  The efficiency can be calculated at any load because constant losses are known.
  • 19. DISADVANTAGES  As the test is on no load, it doesn’t indicate whether the commutation on full load is satisfactory and whether the temperature rise would be within specified limit.  THIS TEST CAN’T BE APPLIED FOR A SERIES MOTOR because speed of series motor is very high at no load ,it is not possible to run series motor on no load.  Note:-In comparison to other the armature cu losses is so small that it may be neglected & constant loss may be take equal to no load i/p
  • 20. Regenerative/Hopkinson’s method.  In this method ,two identical d.c m/c are coupled ,both mechanically & electrically and are tested simultaneously. One of the m/c made to run as a MOTOR and it derives the other m/c as GENERATOR .
  • 21.  For this test m/c 1 is as a dc shunt motor by a starter & brought upto rated speed with switch S open .Bothe the m/c run at same speed ,because these are MECHANICALLY coupled .
  • 22. TO PERFORM THE TEST FOLLOWING PROCEDURE IS ADOPTED  M/c 1(motor) is started through starter & its field rheostat is adjusted so that it runs at normal speed. The m/c 1(Motor) will drive m/c 2(Generator).The switch S is initially kept open.  The excitation of m/c 2 is gradually increased ( by decreasing the field circuit resistance).till the volt metre 1 reads ZERO.Then switch S is closed.
  • 23.  M/c 2 is now floating neither taking any current from the supply nor delivering any current .Any desired load can be put on the set by adjusting the shunt field regulators.The m/c with lower excitation will act as a MOTOR and other m/c will act as a GENERATOR. Let V=supply voltage I2=Armature current of m/c 2(Generator) I1= Armature current of m/c 1(motor) . If2=Field current of m/c 2(Generator). If1=Field current of m/c 1(Motor). Ra=Armature resistance of each m/c
  • 24.  Motor i/p power =V(I+I2)=V×I1  Generator o/p power=V×I2. ............(1) If both the m/c have same efficiency ή,then o/p of motor =ή×i/p =ήV(I+I2)= V×I1 =Generator i/p . o/p of Generator =ή×i/p . =ή×ήV×I1=ή^2V(I1)............(2) From equ (1) & (2). ή^2V(I1)=V×I2. sqrt{(I2/(I1)}
  • 25. EFFICIENCY Armature circuit loss in Generator =I2^2×ra . Armature circuit loss in Motor=I1^2×ra . Power drawn from supply= V×I. No load rotational loss in two m/c=W0= V×I-ra(I1^2+I2^2) . No load rotational loss for each m/c=W0/2 . Generator o/p= I2^2×ra. Generator loss=Wg=(W0/2)+V×If2+ I2^2×ra. ή(g)=[1-(Wg)/(V×I2+Wg)]
  • 26.  Motor i/p=V(I1+If1) Total motor losses Wm=(W0/2)+ V×If1 +I1^2×ra . ή( Motor)=[1-(Wm)/V(I1+If2)]
  • 27. ADVANTAGE  Total power taken from the supply is very low. Therefore this method is very economical.  The temperature rise and the commutation condition can be checked under rated load condition.  Large m/c can be tested at rated load without consuming much power from the supply.  Efficiency at different load can be determine.
  • 28. DISADVANTAGES  The main disadvantage of this method is the necessity two practically identical m/c to be available
  • 29. THANK YOU....