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COLLEGEOFENGINEERINGROORKEE
-: Presentation on :-
METHOD OF TESTING OF I.C. ENGINE
SUBMITTED BY
MAYANK CHAUHAN
Mech. Deptt.
College of Engineering Roorkee
INTRODUCTION
 Engineperformance isan indication
of thedegreeof successof theengine
performs itsassigned task,
 theconversionof thechemical
energycontained in the fuel intothe
useful mechanical work.
The performanceof anengine is
evaluated on the
basisof the following;
 (a) Specific Fuel Consumption.
 (b) Brake Mean Effective Pressure.
 (c) Specific Power Output.
 (d) Specific Weight.
 (e) Exhaust Smokeand Other
Emissions.
BASIC MEASUREMENTS
 Thebasicmeasurementstobeundertakento
evaluatetheperformanceof anengineonalmost
all testsarethefollowing:
 (a) Speed
 (b) Fuelconsumption
 (c) Airconsumption
 (d) Smokedensity
 (e) Brake horse-power
 (f) Indicated horsepowerand friction horse
power
 (g) Heat balancesheetorperformanceof SI and
CI engine
 (h) Exhaustgasanalysis
MEASUREMENT OF SPEED
 Oneof the basic measurementsisthatof speed. A
widevarietyof speed measuringdevicesareavailable
in the market. Theyrangefroma mechanical
tachometertodigital and triggeredelectrical
tachometers.
 The bestmethodof measuring speed istocount
the numberof revolutionsinagiventime. Thisgives
anaccuratemeasurementof speed. Manyenginesare
fittedwithsuchrevolutioncounters.
 A mechanical tachometeroranelectrical
tachometercanalso beused formeasuring thespeed
FUEL CONSUMPTION MEASUREMENT
Fuelconsumptionismeasured intwo
ways:
 (a) Thefuel consumptionof anengine is
measured bydetermining thevolumeflow ina
given time interval and multiplying it by the
specificgravityof the fuel whichshould be
measured occasionallytogetanaccuratevalue.
 (b) Anothermethod is to measurethetime
required forconsumptionof agiven massof fuel
MEASUREMENT OF AIR
CONSUMPTION
 In ICengines, thesatisfactorymeasurementof air
consumption isquitedifficultbecausethe flow is
pulsating,duetothecyclicnatureof theengineand
becausetheairacompressiblefluid.
 Therefore, thesimple methodof using anorifice
in the inductionpipeis notsatisfactorysincethe
readingwill bepulsating and unreliable.
 Thevarious methodsand metersused forairflow
measurementinclude,
 (a) Airbox method,and
 (b) Viscous-flowairmeter
MEASUREMENT OF BRAKE
POWER
 The brakepower measurement involves the
determinationof the torqueand theangularspeed
of theengineoutputshaft. The torque measuring
device iscalled a dynamometer.
 Dynamometerscan be broadlyclassified into
two main types, powerabsorptiondynamometers
and transmissiondynamometer.
Absorption Dynamometers
 Thesedynamometersmeasureandabsorbthe
poweroutputof theenginetowhichtheyarecoupled.
Thepowerabsorbed isusuallydissipatedas heat by
some means. Exampleof suchdynamometersispony
brake, ropebrake, hydraulicdynamometer,etc.
Transmission Dynamometers
 In transmissiondynamometers, thepoweris
transmitted tothe load coupled totheengineafterit is
indicatedonsometypeof scale. Thesearealsocalled
torque-meters
PRONY BRAKE DYNAMOMETER
 Oneof thesimplestmethodsof measuring brake
power(output) istoattempttostoptheengineby
meansof a brakeontheflywheeland measurethe
weightwhichanarmattachedtothebrakewill
support,as ittriestorotatewiththeflywheel.
 Itconsistsof woodenblockmountedonaflexiblerope
orband thewoodenblockwhenpressed intocontact
withtherotatingdrumtakestheenginetorqueand
thepowerisdissipated in frictionalresistance. Spring
loaded boltsareprovidedtotightenthewoodenblock
and henceincreasethefriction.
MEASUREMENT OF FRICTION POWER
 Thedifferencebetween indicated powerand the brake
poweroutputof anengineisthefrictionpower.
 Almostinvariably, thedifferencebetweenagoodengine
and a badengineisduetodifferencebetweentheirfrictional
losses.
 Thefrictional lossesareultimatelydissipated tothe
cooling system(and exhaust)astheyappearintheform
of frictional heatand thisinfluencesthecoolingcapacity
required. Moreover, lowerfriction meansavailabilityof more
brakepower; hencebrakespecificfuelconsumptionis lower
MORSE TEST
 TheMorsetestisapplicableonlytomulticylinderengines.
 Inthistest,theengineisfirstrunattherequiredspeedand the
outputismeasured.
 Then,onecylinderiscutoutbyshortcircuitingthesparkPlugorby
disconnecting theinjectorasthecasemaybe.
 Inthistest,theengineisfirstrunattherequiredspeedand the
outputismeasured.
 Then,onecylinderiscutoutbyshortcircuitingthesparkplugorby
disconnecting theinjectorasthecasemaybe.
INDICATED POWER
 Thepowerdeveloped in thecylinderis known
as Indicated Horse Powerand isdesignatedasIP.
 The IPof anengineataparticularrunning
condition isobtained from the indicatordiagram.
 The indicatordiagram is the p-v diagramfor
onecycleat that load drawnwith the helpof
indicatorfitted on theengine. Theconstruction
and useof mechanical indicatorforobtaining p-v
diagram isalreadyexplain.
•
areas,thepositiveloopand negativeloop,aremeasuredwiththe
helpof aplani meterand letthesebeApand Ancm2 respectively,
thenetpositiveareais(Ap–An).
 h=(Ap-An)/Lincentimetre.
 Theheightmultipliedbyspring-strength(orspring number)
givestheindicated meaneffectivepressureof thecycle.
 Imep=(Ap-An)*S/L
 Pm=Ap*Sp/L-An*Sn/L
 Sp= Springstrengthused fortaking p-vdiagramof positive
loop, (N/m2percm)
 Sn= Springstrengthused fortaking p-vdiagramof negative
loop, (N/m2percm)
 Ap= AreainCm2of positivelooptakenwithspringof strength
Sp
 An= AreainCm2of positivelooptakenwithspringof strength
Sn
 IPdeveloped bytheengineisgivenby IP=PmLAn/L
FUEL CONSUMPTION
 Twoglassvesselsof 100ccand 200cccapacityare
connected in betweentheengineand main fuel tank
throughtwo, three-waycocks.Whenoneissupplying the
fuel totheengine, theotherisbeing filled.Thetimeforthe
consumptionof 100or200ccfuel ismeasuredwiththe
helpof stopwatch.
 Asmallglasstubeisattached tothemain fuel tankas
shown in figure.When fuel rateistobemeasured, the
valveisclosedsothatfuel isconsumed fromtheburette.
 Thetimefora knownvalueof fuelconsumptioncan be
measuredand fuelconsumptionratecan becalculated.
 Fuelconsumptionkg/hr= Xcc XSp.gravityof
fuel/1000xt
Friction Power
 Frictionpowerincludesthe frictional lossesand
thepumping losses. During suctionand exhaust
strokesthepiston must moveagainstagaseous
pressureand powerrequired todothis iscalled the
“pumping losses”.
 Thefriction loss is madeupof theenergy loss
dueto friction between thepistonand cylinderwalls,
pistonringsand cylinderwalls,and between the
crankshaftand camshaftand theirbearings,aswell
as by the loss incurred bydriving theessential
accessories,suchaswaterpump, ignitionunitetc.
Willan’s Line Method
 This method isalso knownas fuel rateextrapolation
method. In this methodagraphof fuelconsumption
(verticalaxis) versus brakepower(horizontalaxis) is
drawnand itisextrapolatedon the negativeaxisof brake
power.
 The interceptof the negativeaxisistakenas the
frictionpowerof theengineatthatspeed.
 Asshown in thefigure, in mostof thepowerrange
therelation betweenthe fuelconsumptionand brake
poweris linearwhenspeedof theengineis held constant
and thispermitsextrapolation. Furtherwhentheengine
does notdeveloppower, i.e. brakepower= 0,
 The maindraw back
of this method is the
long distanceto be
extrapolated fromdata
between 5 and 40 %
load towards
thezero lineof the fuel
input.
 Thedirectional
marginof errorisrather
wide becausethegraph
is notexactly linear
Heat balance sheet
 Theperformanceof anengineisusually
studied by heatbalance-sheet.Themain
componentsof the heatbalanceare:
 Heatequivalenttotheeffective(brake) workof
theengine,
 Heatrejected tothecooling medium,
 Heatcarried away from theenginewith the
exhaustgases, and
 Unaccounted losses.
 Theheatsupplied totheengineisonlyinthe
formof fuel-heatand thatisgivenby
 Qs = mf X CV
 valueof thefuel.
 Thevariousways inwhich heat isused up in the
system isgiven by
 (a) Heatequivalentof BP = kW = kJ/sec. = 0
kJ/min.
 (b) Heatcarriedaway bycoolingwater= Cpw X mw
(Two–Twi) kJ/min.
 Wheremw isthe massof coolingwaterin kg/minor
kg/seccirculated through thecooling.
 (c) Heatcarried away byexhaustgases =
mg Cpg (Tge –Ta) (kJ/min.)or(kJ/sec).
 Where mg is the massof exhaustgases
in kg/min.
 Tg = Temperatureof burntgases
coming outof the
engine.
 Ta = AmbientTemperature.
 Cpg = Sp. Heatof exhaustgases in
(kJ/kg-K)
 A partof heat is lost byconvectionand radiation
aswell adueto the leakageof gases. Partof the
powerdeveloped insidetheengineisalsoused to
run theaccessoriesas lubricating pump,camshaft
and watercirculating pump.
 Thesecannot be measured preciselyand sothis
is knownasunaccounted ‘losses’. Thisunaccounted
heatenergy iscalculated by thedifferentbetween
heatsupplied Qs and thesumof (a) + (b) (c).
 Theresultsof theabovecalculationsare
tabulated inatableand this table is knownas “Heat
BalanceSheet”.
Thank you.

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Different Measurement and Method of testing of ic engine for 2 stroke engine or 4 stroke engine

  • 1. COLLEGEOFENGINEERINGROORKEE -: Presentation on :- METHOD OF TESTING OF I.C. ENGINE SUBMITTED BY MAYANK CHAUHAN Mech. Deptt. College of Engineering Roorkee
  • 2. INTRODUCTION  Engineperformance isan indication of thedegreeof successof theengine performs itsassigned task,  theconversionof thechemical energycontained in the fuel intothe useful mechanical work.
  • 3. The performanceof anengine is evaluated on the basisof the following;  (a) Specific Fuel Consumption.  (b) Brake Mean Effective Pressure.  (c) Specific Power Output.  (d) Specific Weight.  (e) Exhaust Smokeand Other Emissions.
  • 4. BASIC MEASUREMENTS  Thebasicmeasurementstobeundertakento evaluatetheperformanceof anengineonalmost all testsarethefollowing:  (a) Speed  (b) Fuelconsumption  (c) Airconsumption  (d) Smokedensity  (e) Brake horse-power  (f) Indicated horsepowerand friction horse power  (g) Heat balancesheetorperformanceof SI and CI engine  (h) Exhaustgasanalysis
  • 5. MEASUREMENT OF SPEED  Oneof the basic measurementsisthatof speed. A widevarietyof speed measuringdevicesareavailable in the market. Theyrangefroma mechanical tachometertodigital and triggeredelectrical tachometers.  The bestmethodof measuring speed istocount the numberof revolutionsinagiventime. Thisgives anaccuratemeasurementof speed. Manyenginesare fittedwithsuchrevolutioncounters.  A mechanical tachometeroranelectrical tachometercanalso beused formeasuring thespeed
  • 6. FUEL CONSUMPTION MEASUREMENT Fuelconsumptionismeasured intwo ways:  (a) Thefuel consumptionof anengine is measured bydetermining thevolumeflow ina given time interval and multiplying it by the specificgravityof the fuel whichshould be measured occasionallytogetanaccuratevalue.  (b) Anothermethod is to measurethetime required forconsumptionof agiven massof fuel
  • 7. MEASUREMENT OF AIR CONSUMPTION  In ICengines, thesatisfactorymeasurementof air consumption isquitedifficultbecausethe flow is pulsating,duetothecyclicnatureof theengineand becausetheairacompressiblefluid.  Therefore, thesimple methodof using anorifice in the inductionpipeis notsatisfactorysincethe readingwill bepulsating and unreliable.  Thevarious methodsand metersused forairflow measurementinclude,  (a) Airbox method,and  (b) Viscous-flowairmeter
  • 8. MEASUREMENT OF BRAKE POWER  The brakepower measurement involves the determinationof the torqueand theangularspeed of theengineoutputshaft. The torque measuring device iscalled a dynamometer.  Dynamometerscan be broadlyclassified into two main types, powerabsorptiondynamometers and transmissiondynamometer.
  • 9. Absorption Dynamometers  Thesedynamometersmeasureandabsorbthe poweroutputof theenginetowhichtheyarecoupled. Thepowerabsorbed isusuallydissipatedas heat by some means. Exampleof suchdynamometersispony brake, ropebrake, hydraulicdynamometer,etc. Transmission Dynamometers  In transmissiondynamometers, thepoweris transmitted tothe load coupled totheengineafterit is indicatedonsometypeof scale. Thesearealsocalled torque-meters
  • 10. PRONY BRAKE DYNAMOMETER  Oneof thesimplestmethodsof measuring brake power(output) istoattempttostoptheengineby meansof a brakeontheflywheeland measurethe weightwhichanarmattachedtothebrakewill support,as ittriestorotatewiththeflywheel.  Itconsistsof woodenblockmountedonaflexiblerope orband thewoodenblockwhenpressed intocontact withtherotatingdrumtakestheenginetorqueand thepowerisdissipated in frictionalresistance. Spring loaded boltsareprovidedtotightenthewoodenblock and henceincreasethefriction.
  • 11. MEASUREMENT OF FRICTION POWER  Thedifferencebetween indicated powerand the brake poweroutputof anengineisthefrictionpower.  Almostinvariably, thedifferencebetweenagoodengine and a badengineisduetodifferencebetweentheirfrictional losses.  Thefrictional lossesareultimatelydissipated tothe cooling system(and exhaust)astheyappearintheform of frictional heatand thisinfluencesthecoolingcapacity required. Moreover, lowerfriction meansavailabilityof more brakepower; hencebrakespecificfuelconsumptionis lower
  • 12. MORSE TEST  TheMorsetestisapplicableonlytomulticylinderengines.  Inthistest,theengineisfirstrunattherequiredspeedand the outputismeasured.  Then,onecylinderiscutoutbyshortcircuitingthesparkPlugorby disconnecting theinjectorasthecasemaybe.  Inthistest,theengineisfirstrunattherequiredspeedand the outputismeasured.  Then,onecylinderiscutoutbyshortcircuitingthesparkplugorby disconnecting theinjectorasthecasemaybe.
  • 13. INDICATED POWER  Thepowerdeveloped in thecylinderis known as Indicated Horse Powerand isdesignatedasIP.  The IPof anengineataparticularrunning condition isobtained from the indicatordiagram.  The indicatordiagram is the p-v diagramfor onecycleat that load drawnwith the helpof indicatorfitted on theengine. Theconstruction and useof mechanical indicatorforobtaining p-v diagram isalreadyexplain.
  • 14. • areas,thepositiveloopand negativeloop,aremeasuredwiththe helpof aplani meterand letthesebeApand Ancm2 respectively, thenetpositiveareais(Ap–An).  h=(Ap-An)/Lincentimetre.  Theheightmultipliedbyspring-strength(orspring number) givestheindicated meaneffectivepressureof thecycle.  Imep=(Ap-An)*S/L  Pm=Ap*Sp/L-An*Sn/L  Sp= Springstrengthused fortaking p-vdiagramof positive loop, (N/m2percm)  Sn= Springstrengthused fortaking p-vdiagramof negative loop, (N/m2percm)  Ap= AreainCm2of positivelooptakenwithspringof strength Sp  An= AreainCm2of positivelooptakenwithspringof strength Sn  IPdeveloped bytheengineisgivenby IP=PmLAn/L
  • 15. FUEL CONSUMPTION  Twoglassvesselsof 100ccand 200cccapacityare connected in betweentheengineand main fuel tank throughtwo, three-waycocks.Whenoneissupplying the fuel totheengine, theotherisbeing filled.Thetimeforthe consumptionof 100or200ccfuel ismeasuredwiththe helpof stopwatch.  Asmallglasstubeisattached tothemain fuel tankas shown in figure.When fuel rateistobemeasured, the valveisclosedsothatfuel isconsumed fromtheburette.  Thetimefora knownvalueof fuelconsumptioncan be measuredand fuelconsumptionratecan becalculated.  Fuelconsumptionkg/hr= Xcc XSp.gravityof fuel/1000xt
  • 16. Friction Power  Frictionpowerincludesthe frictional lossesand thepumping losses. During suctionand exhaust strokesthepiston must moveagainstagaseous pressureand powerrequired todothis iscalled the “pumping losses”.  Thefriction loss is madeupof theenergy loss dueto friction between thepistonand cylinderwalls, pistonringsand cylinderwalls,and between the crankshaftand camshaftand theirbearings,aswell as by the loss incurred bydriving theessential accessories,suchaswaterpump, ignitionunitetc.
  • 17. Willan’s Line Method  This method isalso knownas fuel rateextrapolation method. In this methodagraphof fuelconsumption (verticalaxis) versus brakepower(horizontalaxis) is drawnand itisextrapolatedon the negativeaxisof brake power.  The interceptof the negativeaxisistakenas the frictionpowerof theengineatthatspeed.  Asshown in thefigure, in mostof thepowerrange therelation betweenthe fuelconsumptionand brake poweris linearwhenspeedof theengineis held constant and thispermitsextrapolation. Furtherwhentheengine does notdeveloppower, i.e. brakepower= 0,
  • 18.  The maindraw back of this method is the long distanceto be extrapolated fromdata between 5 and 40 % load towards thezero lineof the fuel input.  Thedirectional marginof errorisrather wide becausethegraph is notexactly linear
  • 19. Heat balance sheet  Theperformanceof anengineisusually studied by heatbalance-sheet.Themain componentsof the heatbalanceare:  Heatequivalenttotheeffective(brake) workof theengine,  Heatrejected tothecooling medium,  Heatcarried away from theenginewith the exhaustgases, and  Unaccounted losses.
  • 20.  Theheatsupplied totheengineisonlyinthe formof fuel-heatand thatisgivenby  Qs = mf X CV  valueof thefuel.  Thevariousways inwhich heat isused up in the system isgiven by  (a) Heatequivalentof BP = kW = kJ/sec. = 0 kJ/min.  (b) Heatcarriedaway bycoolingwater= Cpw X mw (Two–Twi) kJ/min.  Wheremw isthe massof coolingwaterin kg/minor kg/seccirculated through thecooling.
  • 21.  (c) Heatcarried away byexhaustgases = mg Cpg (Tge –Ta) (kJ/min.)or(kJ/sec).  Where mg is the massof exhaustgases in kg/min.  Tg = Temperatureof burntgases coming outof the engine.  Ta = AmbientTemperature.  Cpg = Sp. Heatof exhaustgases in (kJ/kg-K)
  • 22.  A partof heat is lost byconvectionand radiation aswell adueto the leakageof gases. Partof the powerdeveloped insidetheengineisalsoused to run theaccessoriesas lubricating pump,camshaft and watercirculating pump.  Thesecannot be measured preciselyand sothis is knownasunaccounted ‘losses’. Thisunaccounted heatenergy iscalculated by thedifferentbetween heatsupplied Qs and thesumof (a) + (b) (c).  Theresultsof theabovecalculationsare tabulated inatableand this table is knownas “Heat BalanceSheet”.