steam tables tutorial

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r-- CHEE 221 Tutorial: Saturation and Steam Tables What do they really mean by Saturation? Upon reaching and enthalpy of 2676 only saturated vapour will remain. Further increases in enthalpy will now cause further increases in temperature above 100°C and the vapour is a superheated vapour or superheated steam, meaning that the vapour has been heated above its saturation temperature. 1. Saturation conditions are those under which two or more phases of a pure substance can exist together in equilibrium. However, note that a second phase need not actually be present. A phase is considered saturated so long as it is at conditions where another phase could exist in equilibrium. In the case where a single phase is found, it is in a condition where any system changes (temperature, pressure, enthalpy) will cause some material to change phase. Important note: 419+2257=2676 Question: Why is this important? (this is the change in enthalpy between saturated liquid water and saturated vapour at 100°C) Here are some examples. Question: If, at I atm and 100°C with no vapour present, 1000 KJ of heat is added to I kg of water, what percent is converted to vapour? (no vapour means that the enthalpy is that of liquid water at 419 kJlkg, then we add 1000 kJ which is entirely used to convert a quantity of liquid water into steam. Since it takes a total of 2257 kJ to convert I kg of water, 1000 kJ will convert 1000/2257. 100% = 44.3%) Question: What would you call I kg of water at I atm with the following enthalpies: Another way of looking at saturation conditions is that a change of phase can occur without a change in pressure or temperature (what occurs is a change in enthalpy). Yet another approach is to consider a saturation state to be the conditions at which a phase change begins, takes place, or ends. .. 2. Liquid water (a single phase) can exist in equilibrium at various temperatures (between slightly above 0 and 100°C) while under a pressure Qf I atm. However, liquid water cannot exist at temperatures higher than 100°C while at I atm. Water vapour can exist at this pressure only at temperature of 100°C and higher. Therefore at I atm, three possible phase compositions can exist: (I) only water; (2) only water vapour; (3) water and water vapour in equilibrium. Lets take a closer look at these situations. a) 4 KJ (cold liquid water) b) 419.1 KJ (slightly above saturated liquid water) c) 1500 KJ (a mix ofliquid water and water vapour) d) 2675 KJ (almost saturated water vapour) e) 2677 KJ (just above saturation, superheated water vapour) I) 3000KJ (superheated water vapour) Consider I kg of water with an enthalpy of 3000 KJ at I atm. It is a superheated vapour. Question: What is its temperature? (262°C, by interpolation from table B.7) Suppose we have a system at a temperature below 100°C while at I atm, with only I kg ofliquid water. There is no gas phase (we are not considering the presence of air... yet). At this point the water is below its saturation temperature and is called a subcooled liquid. Heat can be added and the temperature will increase. At 100°C the following enthalpies are reported (relative to water at its triple point O°C, where the relative enthalpy is taken to be 0). As energy is removed and the temperature decreases it will eventually reach its saturation point (100°C with an enthalpy of2676KJ). 11is then a saturated vapour. Water Evaporation Steam (Vapour) 419.1 kJlkg 2257 kJlkg :2676kJlkg As more energy is removed, the temperature will remain constant and saturated vapour and saturated liquid will exist in equilibrium until the enthalpy drops to 419.1 KJ. OK this is really great and I'm happy that the water went from superheated to saturated and went through vapour to liquid phase... but what about those steam tables? Upon arriving at 100°C with an enthalpy of 419.1 kJ,the liquid water is said to be saturated water (there is no water vapour at this point). Additional heat (latent heat of vaporization) will cause no further increase in temperature, but water vapour will begin to form (saturated vapour) and will be in equilibrium with the liquid water so long as the enthalpy is between 419.1 and 2676 kJ. All right, here we go. (turn the page)

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    CHEE 221Tutorial:SaturationandSteamTables

    WhatdotheyreallymeanbySaturation?

    Upon reachingand enthalpy of 2676 only saturatedvapour will remain. Further increasesin enthalpy will now causefurther increasesin temperatureabove 100C and the vapouris a superheated vapour or superheated steam, meaning thatthe vapour has beenheatedabove its saturationtemperature.

    1. Saturationconditionsarethoseunderwhichtwoormorephasesof a puresubstancecanexisttogetherinequilibrium.However,notethatasecondphaseneednotactuallybepresent.A phaseis consideredsaturatedso long as it is at conditionswhereanotherphasecouldexistin equilibrium.In thecasewherea singlephaseis found,it is in aconditionwhereanysystemchanges(temperature,pressure,enthalpy)will causesomematerialtochangephase.

    Important note: 419+2257=2676

    Question: Why is this important?(this is thechange in enthalpybetweensaturatedliquid waterand saturatedvapour at 100C)

    Here aresome examples.

    Question: If, at I atm and 100C with no vapour present, 1000KJ of heat is addedto Ikg of water, what percentis convertedto vapour?(no vapour means that the enthalpy is that of liquid water at 419 kJlkg, then we add1000kJ which is entirely used to convert a quantity of liquid water into steam.

    Since it takes a total of 2257 kJ to convert I kg of water,1000kJ will convert 1000/2257. 100%= 44.3%)

    Question: What would you call I kg of water at I atm with the following enthalpies:

    Anotherway of lookingat saturationconditionsis thata changeof phasecanoccurwithoutachangein pressureor temperature(whatoccursis a changein enthalpy). Yetanotherapproachis to considera saturationstateto betheconditionsatwhicha phasechangebegins,takesplace,orends. ..

    2. Liquid water (a singlephase)can exist in equilibriumat varioustemperatures(betweenslightlyabove0 and100C)whileundera pressureQf I atm. However,liquidwatercannotexistattemperatureshigherthan100Cwhileat I atm.Watervapourcanexistatthispressureonlyattemperatureof 100Candhigher.Thereforeat I atm,threepossiblephasecompositionscanexist:(I) onlywater;(2) onlywatervapour;(3) waterandwatervapourinequilibrium.

    Lets takea closer look at thesesituations.

    a) 4 KJ (coldliquidwater)b) 419.1KJ (slightlyabovesaturatedliquidwater)c) 1500KJ (amixofliquidwaterandwatervapour)d) 2675KJ (almostsaturatedwatervapour)e) 2677KJ (justabovesaturation,superheatedwatervapour)I) 3000KJ (superheatedwatervapour)

    ConsiderI kgof waterwithanenthalpyof 3000KJ at I atm.It is asuperheatedvapour.Question:Whatis itstemperature?(262C,by interpolationfromtableB.7)Supposewehaveasystematatemperaturebelow100Cwhileat I atm,withonly I kg

    ofliquid water.Thereis nogasphase(wearenotconsideringthepresenceof air... yet).At this pointthewateris below its saturationtemperatureandis calleda subcooledliquid. Heatcanbeaddedandthetemperaturewill increase.At 100Cthefollowingenthalpiesare reported(relativeto waterat its triplepoint OC, wherethe relativeenthalpyis takentobe0).

    As energyis removedandthetemperaturedecreasesitwill eventuallyreachitssaturationpoint(100Cwithanenthalpyof2676KJ). 11is thenasaturatedvapour.

    WaterEvaporationSteam (Vapour)

    419.1kJlkg2257kJlkg:2676kJlkg

    As more energy is removed, the temperaturewill remain constantand saturatedvapourand saturatedliquid will exist in equilibrium until the enthalpydrops to 419.1 KJ.

    OK this is really great and I'm happy that the water went from superheatedto saturatedand went throughvapour to liquid phase... but what about thosesteamtables?

    Upon arrivingat 100Cwith an enthalpyof 419.1kJ,the liquidwateris said to besaturatedwater(thereis no watervapouratthispoint). Additionalheat(latentheatofvaporization)will causenofurtherincreaseintemperature,butwatervapourwill begintoform(saturatedvapour)andwill bein equilibriumwiththeliquidwaterso longastheenthalpyisbetween419.1and2676kJ.

    All right, herewe go.(turn thepage)

  • SaturatedSteamtablesTwo types: Pressurebasedand Temperaturebased.

    Conversely you could look up thepressureon B.6.

    - If thetemperatureis higher the steamis superheated.- If it is thesame, you havesaturatedsteam.- If it is lower somebody lied to you and you don't have steam atall but a sub cooled liquid.Table B.5: TemDeraturebasedSaturatedSteam:

    For the temperatureslisted, we are at saturation conditions (along the Vapour-LiquidEquilibrium Curve). The corresponding saturation pressure is also listed here. Anychange in T, P, or H will cause material to changephases.

    The temperaturemust exactly match the given pressure in order to havesaturatedsteam.

    Information on this table:

    Saturationpressureat the listed temperatureSpecific Volume (inverse of density)Internal EnergyEnthalpy: Saturatedwater

    Evaporation/condensationSaturatedSteam

    LookatthePT phasediagramonpage327toconvinceyourselfthatthisistrue.

    You can also look on B.7. If theT and P you are interestedin, intersectin

    the boxed region, you have a liquid not a vapour and someone lied to youagain. If you are right on the line then it's a saturatedvapour, and if youareoutside thebox, you've got superheatedsteam.

    TableB6:PressurebasedSaturatedSteam:The only differenceis thatthe pressureis the indexby which you are lookingupconditions.Forgivenpressures,youcanlookupsaturationtemperatures.(therangeofTableB.6is moreextensive,whichcanbeusefuldependingontheinformationsought).

    4. You aretoldthatyouhavewateratacertaintemperatureandnopressureis given.Enthalpyis a veryweakfunctionof pressureso valuesfromB5 canbeused. Evenif thewateris "subcooled"thevaluesfrom B5 arecloseenough.

    Informationonthetable:SaturationtemperatureatthelistedpressureSpecifieVolume(inverseof density)InternalEnergyEnthalpy: Saturatedwater

    Evaporation/condensationSaturatedSteam

    4. You aretold thatyou have a subcooled liquid.You cannot use the values from B.5 and B.6 becausewe are interestedin

    the enthalpy difference between the subcooled and the saturation state(this won't happenvery often in CHEE22I ). You may just be betteroffusing the Cp integrals. However, you could use the Cp integrals to findtheheatneededto get you to saturationconditions and thenuse thetables.

    Uses:I. For a situation where you have saturatedsteamata certain T.

    All propertiescan be found on B.S.

    5. You havesuperheatedsteamandthe pressureand temperaturevalues arenot in TableB.7.

    Seethenext Section on how B.5 can help in this situation.

    SuperheatedSteamTables2. ForasituationwhereyouhavesaturatedsteamatacertainP.

    All properties.canbefoundonB.6.

    3. May havesteam~ta certaintemperatureand pressureandneedto know if it issaturated.

    Look up the temperatureon B.5 and compare your pressure with the onefrom the table.

    - If your pressureis lower, you have superheatedsteam.- If it is thesame,you have saturatedsteam.- If it is higher, somebody lied and you havesub cooled liquid.

    TableB.7To be superheated,you are at a temperaturein excessof the saturationtemperature. Thistable is a little morecomplicated, so I'll go into more detail on eachcolumn.

    ColumnIThis is whereyoulocatethesystempressure.Thetemperatureatwhichthesteamwillbecomesaturatedis listedin brackets.This temperatureis alsothedew point for thesystem.

  • Columns 2 and 3

    The saturatedpropertiesare listed. This is the same information you would find on B.5and B6.. It is here for convenience. You will frequently run into questions where

    superheated steamis being cooled past saturation. This information savesyou having tolook on otherchartsand table.

    The restof the table

    The system temperature is located across the top row. Intersect it with the systempressure and thereyou find the propertiesat the systemT & P. If the T and P you areatintersectwihtin the boxed region, it's a liquid not a vapour. If you are exactly on the linethen it's saturated vapour (check column 2 and 3 for the properties) and if you areoutside the box, it's superheated steam! And then you can determine the degrees ofsuperheat (which is the difference between the temperatureof your vapour and its dewpoint... The dew point is the temperatureat which this vapour becomessaturated).

    OhNO! thetemperatureandPressureI wantarenotinTableB.7! Whateverwill I do!

    Don't jump just yet, there is still hope. Table BS can save you. If you areat less than 10bar or if the pressure is not given then use the saturatedenthalpy values from Table B5.If the pressureis greaterthan 10bar thenuse theformula H = U+ PV and the values fromB5 to getthe enthalpy.

    Terms to Remember,and be able to differentiatebetween:

    Subcooled waterSaturatedwaterSaturatedstearn

    SuperheatedsteamDegreesof superheatSuperheatedwater

    See definitions and furtherdetails in your textbook.