Engine Working Loads

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    ENGINE WORKING LOADSL. Introduction. Internalcombustion roduces highpressurehatactsuponapiston; heconsequencesrehereexplored.Thereare hreevariableswhichbroadlydefinehedesign f a singlecylindernternal ombustionngine theboreB,thestrolrcS= 2r and heconnectingod tength These reshownn Fig.I.

    F'igureWeare nterestedn the orquesupplied y theengine,he hrusVtensionn theconnectingod (ensure obuckling, mplicationsor fatigueof big-endbolts)and heside-thrust nthecylinder-wall implicationsor wearand nternal osses).2. SomehistoryThe 19966-cylinderWl 24)Mercedes enz8300dieselengine asboreB - 87rnm strokes = 84 mm. Thesweptvolume s

    ^ _ a7 L I I T

    x84x 6 -2.996x106mm'; but I cm=10mm, so I cm3:1000mm3, nd heasweptvolume is 2996cffi3 or 3-litres. Since he bore is greater han the stroke, heengine s saidto over-square. Early automotivepracticewas for engines o be under-s(luare; his was encouraged y the impositionof Vehicle ExciseDuty (VED) baseduponheRAChorse-powerormulaRAChp=ry where is heboren inches,2.5n isthenumber fcylinders,atherhanCO, emissionscurrentlymployed. incethis formula is independentof stroke S,t was advantageouso achievea given

    -",.I

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    capacityby having a small bore but largesfoke. For example, he JaguarXK 3.8 litreengine 1950's,1960's)hadaboreof 87 ffiffi,but a strokeof 106mm. A long strokehas he advantage f higher torqueat low speed, ower side-thrust,but thedisadvantage f higher piston speed andhencemechanical osses)andhigher pistonacceleration andhencevarious dynamicstresses)or a given enginespeed. The trendtowardsover-squareengines riginated n theUSA in the 1950's.

    3. Somecalculations. SupposeF is the net force on thepiston crown,that is gaspressurex piston crown areaminus the force necessaryo acceleratehe piston,which is

    F=p(e),q-ffi*""@'r["o,.ry)

    (b)

    Figure2 G

    From he ree-body iagram f thepiston,Fig.2a,onehasF = ecosl, orQ = FsecQ, fid G = QsinL= FtanQ whereQisthecompressiveorce n theconnectingod,andG is theside-thrust rovidedby thecylinderwall. ForagivenF, theside-thrust ill besmallwhen/ is small; or agiven and0,themagnitudeof G decreasess increases:hus a longconnectingod leads o smallerside-thrust,and so ess rictional loss,and esswear. On heotherhand,ong odengineswith aparticularstrokebuildsuctionabovehepiston essquickly,sincehepistonmovesaway rom TDC moreslowly; his resultsn a lower nlet portairvelocity,which educesow speedorque.Typically, heratio lf r rangesrom3 to 4.

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    sin =lsinl ,

    The orque ppliedo thecranks z = exoN:Fse clxoN, butoNsecQ= oM, leadingo T= l7xoM. Thus o, 1 given F,orquewill be arge fdistanceOM is large.

    ReferringtoFig., Op=/coS +lcos|,ood *=tan Q,soOPoM=oPtan0,or oM=rcosetu t+rs in l . Now s ing= ls in l , soeos{ = l - (r l t ) 'z sinzQ,snd tan|= ThusOM

    canbeexpresseds

    From heabove,t is clear hatdistance M increasess hecrank hrowr (which sone-halfof thestroke, = sl}) increases.n turno nemayconcludehata longstrokeenginewill providea larger orque,all other actorsbeingequal whichtheyneverare' Thusa long-stroke inglecylinder500ccengine,as n a 1950/60,sPanther,s ideal or amotorcycle ombination.Motorbikeandsidecar!)4. Tuming-momentdiagram. A typicar v-diagramis shownn Fig.3.

    Figure3Nextonemayconstnrct furning-moment iagram, s n Fig.4.

    l-(rlt)'zsin2Q

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    ,a *# , _r_i

    tNotethatwhen hetorque s negative,heenginemustbedrivenby anextemalsourceof energy henceheneed or a flywheel. The ncreasen torque owards heendofeachstoke s due o retardationof thepistonadding o thegaspressure.Themeanoraverageorque s

    4nt @)d0T - J - '- mean 4n5. Multi-cylinder engine.Fora 4 cylinderengine,with firing order l342,onecansuperimpose firther three orquecurves,eachshiftedby n radians.Theoveralltorquecurvewill thenbe much ess peaky"anda smaller lywheelwill berequired.

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