EXAMPLEPROJECT
GroupMembers:(Listeachgroupmember’snameinabulletedlistbelow)
● PollyEsther
● GeneEric
KeyQuestion:(Whatistheprimarythingyouwanttocalculateatthepark?)(Indentandbold)
Determinetheamountofenergythathasbeenlostbetweenthebeginningofthefirst
loopandjustbeforebrakingbeginsonTheDemon.
DrivingQuestions:(Ifyouwereassignedtheabovetask,whatquestionswouldyouhave?)(Bulletedlist)
● Howwillwefindtheenergyatthesetwolocations?
● Whatdeterminestheenergyataparticularlocation?
● Shouldweusekinematicsorenergyconservationtosolvethisproblem?
● Whatdoweknowaboutwhatshouldhappentoenergyduringaride?
BackgroundPhysicsInformationNeeded:(Inparagraphform,discussthephysicsconceptsyouwilluse.)
TheLawofConservationofEnergystatesthatthetotalamountofmechanicalenergyfor
asystem,sayarollercoaster,shouldremainconstant.ThetotalMEiscomprisedof
GravitationalPotentialEnergy(GPE),ElasticPotentialEnergy(PE
el
),andKineticEnergy(KE).
GPEiscalculatedbytheformulaGPE=mgh;PE
el
iscalculatedbytheformulaPE
el
=½kx
2
;
andKEiscalculatedbytheformulaKE=½mv
2
.
AlthoughtheLawofConservationofEnergystatesthattotalenergyisconserved,this
problemindicatesthatthismaynotbetrueifenergyislost.Iffriction(boththerollercoasterwith
thetrackandairresistance)aretakenintoaccount,thentheLawofConservationofEnergy
wouldbetrue.
InordertousethisLawtosolvethisproblem,wewillneedtodeterminethetotalamount
ofenergytherollercoasterhasasitentersthefirstloop,andagainjustbeforethebraking
beginsattheendoftheride.Thedifferencebetweenthesetwovalueswillbetheamountof
energylosttofrictionwiththetrackandairresistance.
Todeterminetheenergyatthetwokeylocations,wewillneedtodecidewhattypesof
energythecoasterhasateachpoint.Asthecoasterentersthefirstloop,itisatit’slowest
verticalpointoftheride.Ifweconsiderthisheighttobe“h=0m”thenthecoasterdoesNOT
havegravitationalpotentialenergy.Thereisnoelasticpotentialenergyforthecoasteratthis
point,sotheonlytypeofenergyithasiskineticenergy.Asthecoasterentersthepartofthe
ridewherebrakingbegins,itisataheighthigherthanwhereitenteredthefirstloopsoitWILL
havesomeGPEalongwithKE,butwillstillNOThavePE
el
.
So,inordertosolvethisproblemwewillneedtobeabletohavevaluesofm,g,h,andv
ateachpoint.Theaccelerationduetogravity(g)isaconstant,theheights(h)canbemeasured
atthepark,butmassandvelocityprovemoredifficult.Uponfurtherresearch,wecanmeasure
velocityofthecoasterateachpointusingthedefinitionofvelocity.Wewillmeasurethetotal
lengthofthetrain(d)andtimehowlongittakestopassastationarypointonthetrackateach
ofthelocations.Wealsodecidedthatmasscanbeignored,becauseifwesetupanEnergy
Conservationproblem:
(mgh+½mv
2
)
initial
=(mgh+½mv
2
)
fnal
themasswillcanceloutoneachsideandtheremainingtheoreticalstatementistrue:
(gh+½v
2
)
initial
=(gh+½v
2
)
final
ThereforewewillalterouroriginalformulasforeachtypeofenergytoNOTincludemass.