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Thermodynamics of Open Systems: Energy Equations and Problems, Lecture notes of Law

Steady Flow Energy EquationsFirst Law of ThermodynamicsMass Balance in ThermodynamicsThermodynamics of Open Systems

Detailed information on the energy equations for open thermodynamic systems, including steady flow energy equations and first law equations for unsteady systems. It includes various problems to help understand the concepts.

What you will learn

  • What is the first law of thermodynamics for open systems?
  • How do you determine the mass balance in an open system?
  • What is the difference between steady flow and unsteady flow in thermodynamics?
  • How do you calculate the exit temperature in an adiabatic nozzle?
  • What is the role of energy in thermodynamics?

Typology: Lecture notes

2021/2022

Uploaded on 09/27/2022

melanchony
melanchony 🇬🇧

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Download Thermodynamics of Open Systems: Energy Equations and Problems and more Lecture notes Law in PDF only on Docsity! ( ) same thebemust msenergy ter theall of units the )365(W) 2 V(hmQ Wgz) 2 Vpv(umQ W)gz 2 Vvp(um)gz 2 Vvp(umQ gz 2 Vu(T)PEKEu(T)E vp mvp mWWWWW vp mVpVVppdVW LawFirstW∆EQ shaft 2 shaft 2 shaft1 2 1 1111 2 2 222 2 2211shaftout flowin flowshaft 1111final 1initial 11in flow −+++∆= ++++∆×= ++++×−+++×= ++=++= −+=++= ==−== += ∫ gz FIRST LAW IN OPEN SYSTEMS Steady Flow Energy Equation Open, steady flow thermodynamic system - a region in space Q shaftW p1 v2 1V 2V 1z 2z p2 Steady Flow Processes Devices EquationEnergy FlowSteady Wgz) 2 V(hmQ shaft 2 +++∆= Turbine, Compressor, Pump ( )outin hhmW −= ∆== =∆∆ hm∆HW 0Q Elevation, Velocity, ( )outin hhmQ −= == =≅≅ h m∆∆HQ 0 Work0,∆Elevation 0,∆Velocity Boiler, Condenser, Heat Exchanger Diffuser, Nozzle Valve - throttling process outin hh = = = ==== outin HH 0∆H 0W0,Q0,∆Elevation0,∆Velocity 2 Vh 2 Vh 2 2 2 2 1 1 +=+ ==≅ 0W0,Q0,∆Elevation 4.233 An adiabatic air compressor is to be powered by a direct coupled adiabatic steam turbine that is also driving a generator. Steam enters the turbine at 12.5 MPa and 500 C at a rate of 25 kg/sec and exits at 10 kPa and a quality of .92. Air enters the compressor at 98 kpa and 295 K at a rate of 10 kg/sec and exits at 1 MPa. Determine the net power delivered to the generator by the turbine. airsteam v v g2393.2kJ/k2392.8.92191.83h @10kPaxh@10kPahh 3341.812.5)p500,(Tsuperheat@h 628.1kJ/kg620)Tairtable@(h 210.5kJ/kg295)Tairtable@(h t2 fgft2 t1 c2 c1 =×+= += ==== === === 12.5 kPa 500 C 10 kPa x=.92 netW compressor turbinegenerator p1 Mpa 620 K p 98 kPa 295 K ( ) ( ) ( ) ( ) kJ/sec 19539W 210.5628.1 sec kg102393.23341.8 sec kg 25W hhmhhmWWW net net c2c1ct2t1tcompressorturbinenet = −−−×= −−−=−= 4.65 Steam at 3Mpa and 400 C enters an adiabatic nozzle steadily with a velocity of 40 m/sec and leaves at 2.5 MPa and 300 m/sec. Determine (a) the exit temperature and (b) the ratio of inlet to exit area. Open thermodynamic system - a region in space 1 3 MPa 400C 40m/sec 2.5MPa 300m/sec p 2 v /kgm 09936.v kJ/kg 3203.9h 3.)P400.,(T @superheat v&h 3 1 1 11 = = === ( ) ( ) .1517 1.1757 .1783 A A 273.15364.78 300 A 2.5 273.15400 40 A 3 V A RT pV A RT p AV RT pρAVm b) C 364.78T 2.5)p3159.7,(h @superheat T a) 1 2 21 21 2 2 11 1 1 2 2 == + = +       =           == = === kJ/kg 3159.744.23203.9h /secm 1000 kJ/kg 1 sec m 2 300 2 40kJ/kgm 3203.9h 2 V 2 Vhh equationenergy flowsteady 2 Vh 2 Vh 2 222 222 2 2 2 2 1 12 2 2 2 2 1 1 =−=             −+=       −+= +=+ Steam at 3Mpa and 400 C enters an adiabatic nozzle steadily with a velocity of 40 m/sec and leaves at 2.5 MPa and 300 m/sec. Determine (a) the exit temperature and (b) the ratio of inlet to exit area. Open thermodynamic system - a region in space 1 3 MPa 400C 40m/sec 2.5MPa 300m/sec p 2 v .1872 74.535 13.951 A A 11626. 300 A 2.5 09938. 40 A 3 V A V A ρAVm b) 11626. v 2.5)p3187.5,(h @ v C, 376.5T 2.5)p3187.5,(h @ T a) 1 2 21 2 21 1 11 2 2 2 2 == = = = = == = == vv /kgm 09938.v kJ/kg 3231.7h Mpa) 3.P400.,(T @superheat v&h 3 1 1 11 = = === kJ/kg 3187.544.23231.71h /secm 1000 kJ/kg 1 sec m 2 300 2 40kJ/kgm 3231.71.9h 2 V 2 Vhh equationenergy flowsteady 2 Vh 2 Vh 2 222 222 2 2 2 2 1 12 2 2 2 2 1 1 =−=             −+=       −+= +=+ 4.65 im A 200 cubic ft tank contains 2. lbm carbon dioxide and .1 mole helium at an initial temperature of 70 F. 3 lbm of air at 14.7 and 70 F are admitted to the tank. What is the final temperature of the tank? ( )fi1 1 1 1 mmm T u h −= 1p ( )( ) ( ) ( ) ( ) ( ) ( ) F167T R627T 0381.6323.831.125TQ 381.670460.243hmm 323.8370460.745.4.15652um 1.125TT.745.4.15652.1743um hmmumumQ o f o f f 1fi ii ffff iifiiff = = =−−= =+××=− =+××+×= =×+×+×= −−−= 4-153 kJ/kg 3167.7h C350 MPa, @.5 kJ/kg 2292.51h 2163.8.8561.47h hxhh kJ/kg 2725.3vh C 133.55 @300kPaTT kPa 300 @ o o 1 1 fgf1 g2 saturation2 = = ×+= ×+= == == ( ) ( ) kg 9.78kg 10kg 19.78mm kg 19.78 kJ/kg 2725.3kJ/kg 3167.7 kJ/kg 2292.51kJ/kg 3167.710kgm )h(h )h(hmm )h(hm)h(hm0 pv,usince vpmumhmvpmumhm0 vpmvpmumumhmhm0 umumh )m(m)vpmvp(m0 ,for W ngsubstituti vpmvpm W umumh )m(mWQ m cylinder,piston in thefinally mass theis system the 12 2 1o 1o 12 1o1o22 11111o122222o2 1112221122o1o2 1122o12111222 boundary 111222boundary 1122o12boundary 2 =−=− = − − = − − = −+−= += −−+++−= −+−++−= −=−+−− −= −=−+− boundaryW8 kg liquid water and 2 kg vapor at 300 kPa are contained in an insulated piston cylinder. Steam at .5 MPa and 350 C are admitted until the piston cylinder contains only vapor. Determine the final temperature and the amount of steam admitted. oh steam ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 1 hhmHH W0,Qfor hhmHHQ 0,for W EEWWQQ WWW 0 233) (page UUEEWWQQ W∆EQ WUUQ UUWWQQ 0 173) (page UUEEWWQQ 32)-(2 UUEEWWQQ UKE, PE, W,Q, forms, all is E 72) (page ∆EEE conservedEnergy , definedEnergy 212net 1212net in massout massoutinoutin flowshaft 12out massin massoutinoutin 12 12outinoutin 12out massin massoutinoutin 12massoutmassinoutinoutin outin −=−== −=−== −=−+− += −=−+−+− += +−= −=−+− −=−+−+− −=−+−+− =− space in region a SYSTEM OPEN mass of quantity contained a SYSTEM CLOSED LawFirst
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