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Physics302L

Course: PHY 2030, Spring 2011
School: Maple Springs
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= MAPUAINSTITUTEOFTECHNOLOGY DepartmentofPhysics E302:HeatandCalorimetry XXXXXXXXXXXXX 2005XXXXXXXXXX,Group1 PHY130LXX XXXXXXX SAMPLECOMPUTATIONS PartI.DeterminingtheSpecificHeatofMetals Given: mm 31.6 g mc = 47 g m w = 198.8 g T0 m = 81 C 0 Solution: T0 w = 27 0 C Tmix = 290 C Cw = 1cal g C0 T0c = Tw = Tmix T0 w Tm = Tmix Tm T0c = Tw = 29 0 C 27 0 C Tm = 29 0 C 810 C T0c = Tw = 2 0 C Tm = 52 0 C...

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= MAPUAINSTITUTEOFTECHNOLOGY DepartmentofPhysics E302:HeatandCalorimetry XXXXXXXXXXXXX 2005XXXXXXXXXX,Group1 PHY130LXX XXXXXXX SAMPLECOMPUTATIONS PartI.DeterminingtheSpecificHeatofMetals Given: mm 31.6 g mc = 47 g m w = 198.8 g T0 m = 81 C 0 Solution: T0 w = 27 0 C Tmix = 290 C Cw = 1cal g C0 T0c = Tw = Tmix T0 w Tm = Tmix Tm T0c = Tw = 29 0 C 27 0 C Tm = 29 0 C 810 C T0c = Tw = 2 0 C Tm = 52 0 C m c T + m w c w Tw C m exp erimental = c c c m m Tm ExperimentalSpecificHeatofMetal ( 47 g ) 0.217cal 2 0 C + (198.8 g ) 1cal 0 0 g C g C C m exp erimental = ( 31.6 g ) 52 0 C cal C m exp erimental = 0.254380477 g C0 ( ) ( % error = % error % error AV EV AV ) 0 2 C x100% cal cal 0.2174 0.254380477 0 g C g C0 = cal 0.2174 g C0 = 17.01% x100% ( ) PartII.LatentHeatofFusionofIce Given: mc = 47 g T0 w = 29 0 C m w = 187.7 g T = 22 0 C mix mi = 14 g 1cal Cw = 0 T0i = 0 C g C0 mc c c Tc + m w c w Tw + mi c w Tice water mi Tice water = Tmix T0 w T0c = Tw = Tmix T0 w 0.217cal 0 0 1cal 0 7C ( 47Tc = Tw0 = 22 7C C 29 (0187.7 g )icewater =0 22 C0 0 0+C(14 g ) 1cal 0 g )0 + C T g C g C g C = Tc = Tw = 7 0 C Tice water = 22 0 C 0 (14 g ) cal = 76.9495 g C0 ExperimentalLatentHeatofFusion L f exp erimental = Solution: L f exp erimental L f exp erimental % error = % error AV EV AV ( ) x100% cal cal 80 g C 0 76.9495 g C 0 = cal 80 g C0 % error = 3.81% ( x100% ) 0 22 C ( ) GUIDEQUESTIONS PartI. 1. Expressequation1intermsofmass,specificheats,finalandinitialtemperature. Qloss = Q gained mcT = mcT mc(T f Ti ) = mcT (T f Ti ) 2. Whyisitimportanttoimmersethemetalintheboilingwaterforalongtime? Whathappensifthemetalwasimmersedonlyforashortwhile? Itisimportanttoimmersethemetalinboilingwaterforalongtimeinorder forthemetaltoattainthermalequilibrium,Ifthemetalwasimmersedonlyfora shortwhiletheinitialtemperatureofthemetalwouldhavebeenfalse. 3. Why do you need to wipe of the metal surface before taking the initial temperature? Youneedtowipeofthewatersothattheinitialtemperatureofthemetal isntaffectedbythetemperatureofthewater. 4. What is your computed specific heat and percentage error? Is it acceptable? Why? ThecomputedC=0.254cal/g 0Cand17%errorisacceptable;sinceitisnotan isolatedsystemandmanyfactorssetin,itishardtogetanaccuratereading. 5. Whatarethesourcesoferrors?Whatareyourrecommendations? Irecommendhavingsomeonewithanaccurateyetfasteyetomonitorthe temperaturereadingsandrepeattheexperimentstogetanaccurateresult. PartII. 1. Showyourderivedformulaindeterminingthelatentheatoffusionoficeusing thelawofheatexchange. Qloss = Q gained mcT + mL = mcT + mL mc(T f Ti ) + mL = mcT (T f Ti ) + mL 2. Whatistheinitialtemperatureoftheice?Whatassumptionsdidyoumaketo determinetheinitialtemperatureoftheice? 00C,sinceiceandwatercoexistonlyat00Cweeassumeditwascorrect. 3. Whyisitimportantowipeoffthewaterfromtheicessurfacebeforeputtingitin thecalorimeter? The surface of the ice waswiped of to remove the thermal change of watertogetherwiththeice,bydoingsowecanconcentratepurelyonthephase changeofice. 4. Hadthemassoficebeengreater,howwoulditaffecttheresultoftheexperiment andthecomputedlatentheatoffusion? Hadthemassoftheicebeengreaterthecomputedlatentheatoffusion andexperimentalvalueswouldhavebeenthesame. 5. Whatarethesourcesoferrorsandyourrecommendation? Irecommendhavingsomeonewithanaccurateyetfasteyetomonitorthe temperaturereadingsandrepeattheexperimentstogetanaccurateresult. REMARKSANDCONCLUSION Thermodynamics is the study of energy and its transformations; of particular interestisthe relationship between heat and work.One of the fundamental tools thermochemistry, in a branch of thermodynamics, is calorimetry. Calorimetry is the measurementofheatflow. Heatcanonlybeidentifiedasitisbeingtransferredfromonesystemtoanother. Heattransferisapathfunction(processquantity),asopposedtoapointfunction(state quantity). Heatflowsbetween systemsthatare notin thermal equilibriumwith each other; it spontaneously flows from the areas of high temperature to areas of low temperature. All systems (matter) have acertainamount of internal energy.Internal energyisapropertythatisameasureofallmicroscopicwaysbywhichasystemcan possessenergy,forexampletherandommotionofitsatomsormolecules.Whentwo bodiesofdifferenttemperaturecomeintothermalcontact,theywillexchangeinternal energy until their temperatures are equalized; that is, until they reach thermal equilibrium.Theamountofheattransferredisequaltotheamountofenergyexchanged betweenthetwobodies.Itisacommonmisconceptiontoconfuseheatwithinternal energy.Ahotobjectdoesntcontainheatitcontainsinternalenergy.Theadjective hotis usedasarelativetermtocomparetheobjectstemperaturetothatofthesurroundings (orthatofthepersonusingtheterm).Thetermheatisusedtodescribetheflowof energy.Intheabsenceofworkinteractions,theheatthatistransferredtoanobject endsupgettingstoredintheobjectinforminternalenergy. Specificheatisdefinedastheamountofheatthathastobetransferredtoor fromoneunitofmassormoleofasubstancetochangeitstemperaturebyonedegree. Specific heat is a property, which means that it depends on the substance under considerationanditsstateasspecifiedbyitsproperties.Fuelswhenburned,release muchoftheenergyinthechemicalbondsoftheirmolecules.Uponchangingfromone phasetoanother,apuresubstancereleasesorabsorbsheatwithoutitstemperature changing.Theamountofheattransferduringaphasechangeisknownaslatentheat anddependsprimarilyonthesubstanceanditsstate. Calorimetersaredesignedtobewellinsulated,sonoheatisgainedfromorlost tothesurroundings.Ifnoheatingelementisusedtointroduceheatinthesystem,the totalheattransferred(q)fortheentirecalorimetersystemmustequalzero. Toensure the validity of the experiment one must have an accurate and precise temperature readingandavoidanymovementsthatmayleadtothermalleakage.Thetotalheatcan be split into heats for each component in the system, which is heat loss and heat gained. Calorimetrycanbeappliedineverydaylife,fromthereactionsinsideourbodyto thepowerplantsusedtopowerourhomes. FREESPACE REFERENCE http://en.wikipedia.org http://www.britannica.com http://www.chm.davidson.edu http://www.space.com/scienceastronomy.html AmazingEarthFacts We live on a sphere of extremes and oddities. In fact it's not really a sphere, but it is a wild planet, mottled with deadly volcanoes, rattled by killer earthquakes, drenched in disastrous deluges. But do you know which were the worst? 1. What is the hottest place on Earth? Count one wrong if you guessed Death Valley in California. True enough on many days. But El Azizia in Libya recorded a temperature of 136 degrees Fahrenheit (57.8 Celsius) on Sept. 13, 1922 -- the hottest ever measured. In Death Valley, it got up to 134 Fahrenheit on July 10, 1913. 2. And the coldest place around here? Far and away, the coldest temperature ever measured on Earth was -129 Fahrenheit (-89 Celsius) at Vostok, Antarctica, on July 21, 1983. 3. What makes thunder? If you thought, "Lightning!" then hats off to you. But I had a more illuminating answer in mind. The air around a lightning bolt is superheated to about five times the temperature of the Sun. This sudden heating causes the air to expand faster than the speed of sound, which compresses the air and forms a shock wave; we hear it as thunder.
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