(a)lettherebeaspringwithaforceconstantksotheforceonalockattachedtothespringwhichhasbeenelongatedbyadistancexis=−kxsotheworkdonebythespringforceinelongatingittoadistancexis,W=∫x0−kxdx=−kx22nowbydefinitionthepotentialenergystoredinthespringatanyelongationisthenegativeoftheworkdonebythespringforceinproducingtheelongationsothestoredpotentialenergyinthespringis=−(−kx22)=kx22(b)springforceisconservativeforce:Astheworkdonebythespringforcedependsonlyonthefinalpositionandtheinitialpositionsowecansaythatthespringforceisaconservativeforce.theworkdonebythespringispathindependentforaparticularspringmasssystemlettheelongationinthespringbexsothestoredspringpotentialenergyinit=kx22(c)nowspringisreleasedwhenthespringreturnstoitsmeanposition,theattachedmassgainssomevelocity,letthevelocitybevmsothekineticenergyinthebody=mv22thus,byconservationofenergydecreaseinthespringpotentialenergy=increaseinthekineticenergyoftheblocksosomv22=kx22orv=x√kmatthemeanposition