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ReproducedfromtheUnitGuidesforSEP101andSEP115
physicslabreport
DeterminationoftheGravitationConstantg
byMeansofaSimplePendulum
Aim
Thisexperimentwasperformedtodeterminethegravitationalaccelerationofobjectsclosetothesurfaceoftheearth,byobservingthemotionofasimplependulum.
Introduction
Asimplependulum,figure1,displacedthroughasmallangle,willoscillatebackandforthaboutitsequilibriumpositionwithperiodT.Tisthetimethependulumtakestomakeonecompleteback-and-forthmotion.ThebobishungfromarigidsupportonastringoflengthL.
Figure1:Thesimplependulum.
Foroscillationswheretheangleissmall,theperiodTisrelatedtothelengthLofthestringandthegravitationconstantgby
Squaringbothsidesofthisequationyields
Ifonemeasurestheperiodofapendulumasafunctionofthelengthofthestring,thenaplotofT2asafunctionofLwillyieldastraightlinewithagradientG;and
ExperimentalMethod
Asimplependulumwasproducedfromalengthofstringandafishingsinker.Thesinkerwasdisplacedthroughananglelessthan10degreesandreleased.Forfivedifferentlengthsofstringbetween23and100cm,theperiodofoscillationwasmeasured.Ineachmeasurement,thependulumwasallowedtooscillate50times.Thetotaltimefor50oscillationswasmeasuredwithastopwatch,andtheperiodwascalculatedbydividingthetotaltimefor50oscillationsby50.Thestopwatchmeasurestimeto0.01seconds.However,itisestimatedthatthetotalreactiontimeoftheexperimenterwas0.2seconds.Thustheuncertaintyofanyoriginalmeasurementoftimewastakentobe0.2seconds.Withametrerule,thelengthofthestringwasmeasuredtothenearestmillimetre.Thelengthofthestringwasmeasuredfromthesupporttothecentreofthebob.
ResultsandCalculations
Table1showstheresultsoftheexperiment,andtheplotofT2versusLisgiveninfigure2.
String
Length(m)
Timefor50
oscillations(s)
TimeTforone
oscillation(s)
Period
squared(s2)
0.975
97.3
1.95
3.80
0.812
88.7
1.77
3.13
0.597
75.6
1.51
2.28
0.411
61.9
1.24
1.54
0.235
45.9
0.918
0.843
Table1:Pendulumdata.
Theuncertaintyineachmeasurementoflengthis0.001m.Theuncertaintyineachmeasurementoftimefor50oscillations,T1is0.2
s.Thustheuncertaintyinanymeasurementoftheperiodis
Theperiodissquaredpriortoplotting.Therelativeuncertaintyintheperiodsquaredistwicetherelativeuncertaintyintheperiod:
SolvingforT,
ThustheuncertaintyinT2isproportionaltoT.ThelargestdatapointisforT2
=
3.80
s2.Theuncertaintyinthisdatumis.ThemaximumuncertaintyinT2isthus0.4
%.TheerrorbarsassociatedwithT2aretoosmalltoplotonagraph.Similarly,theerrorbarsassociatedwithLarealsotoosmalltoplotonthegraph.
Figure2:PlotofT2asafunctionofL.
Astraightlinefitsthedatawell.Thegradientofthelineofbestfitcanbecalculatedfrom
and
Toworkouttheuncertaintyinthegradient,analternativelineofbestfitwasselected,anditsgradientisgivenby
TheuncertaintyinGisthedifferenceofthese2gradients:
ThepercentuncertaintyinG,andthusingis
Thustheexperimentallydeterminedvalueofthegravitationconstantisg
=
9.99
m/s2
2%.
Discussion
Theacceptedvalue
ofgis9.81m/s2.Theaccuracyoftheresultsis
Theexperimentallydeterminedvalueofgagreeswiththeacceptedvaluetowithintheexperimentaluncertainty.Thusthisexperimentwasasuccessfulandaccuratedeterminationofg,evenwiththesimpleapparatus.
Thebobusedinthisexperimentisintheshapeofatriangularwedge.Thecentreofmasswasestimated(guessed)forthebob,andthelengthofthestringwasconsistentlymeasuredtothatpoint.Theaccuracyofthelengthofthestringdidnotmatterinthisexperimentsolongasthelengthwasalwaysmeasuredinthesameway.ThegravitationconstantwasdeterminedfromthechangeinT2asLchanged.Thischangeisstatic,regardlessofwheretheendofthestringwastakentobe.Anyerrorsinestimatingwherethestringendedwillmerelyshifttheplotupordown.Itwillnotaffectthegradient.AninterestingfurtherexperimentwouldbetocollectmoredatapointsforsmallL,andseeiftheplotteddatapassthroughtheorigin.
Anotherinterestinginvestigationwouldbetoperformtheexperimentforlargeanglesofdisplacement.Thetheoryassumesthatthisangleissmall.Furtherexperimentscouldinvestigatehowthedeterminationofginthistechniqueisaffectedbyanincreasingangleofdisplacement.
Conclusion
Bymeansofasimplependulum,thevalueofthegravitationconstantwasdeterminedtobeg
=
9.99
m/s2
2%.Thisagreedwiththeacceptedvalue,9.81m/s2,towithintheexperimentalunc
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