MAE 320 Thermodynamics HW 5 Assignment
|
|
- Russell Shields
- 6 years ago
- Views:
Transcription
1 MAE 0 Therodynaics HW 5 Assignent The hoework is due Wednesday, October 9, 06. Each proble is worth the pots dicated. Copyg o the solution ro another is not acceptable.. Multiple choices questions. There ay be ore than one answer or each question. (6 pots) (a). The st law o therodynaics cannot be applied to: (A) Control olue syste as the ass can cross the boundary. (B) A steady operation stea turbe. (C) An unsteady operation stea turbe when the energy contaed with turbe changes with tie. (D) Diuser, which has dierent let and area. (E) None o aboe (b). Please circle the alid stateent(s) ab control olue syste: (A) Both the ass and energy can cross the boundary o a control olue. (B) Under the steady-low condition, the ass and energy contaed with the control olue syste rea constants. (C) Under the steady-low condition, the luid properties at an let or always rea constant (do not change with tie) but ay be dierent at let and. (D) Under the steady-low condition, the tensie properties o the substance contaed ust be hoogeneous (unior) eerywhere a control olue. (E) Gas turbes, throttlg ales, nozzles and diusers operated under steady condition can be treated as the steady-low control olue syste. (c). Please circle the alid stateents ab heat exchangers: (A) Heat exchangers are deices where two og luid streas are ixed together. (B) Heat exchangers are deices where two og luid streas exchange ass. (C) Heat exchangers are deices where two og luid streas exchange heat (theral energy) with ixg together. (D) Heat exchangers are deices where two og luid streas exchange echanical work with ixg together. (E) There is no heat transer between the two luids o an sulated heat exchanger. (d). Stea (superheated water apor) enters an adiabatic throttlg ale at MPa, 400 C and s at 00 kpa. Neglectg the change ketic energy, the teperature o stea g this throttlg ale is (A) below 50 C (B) between 50 to 00 C (C) between 00 to 400 C (D) oer 400 C (E) Cannot be decided based on the oration proided.
2 (e). Please circle the alid stateent (s) ab a steady-low deice: (A) The ass with the control olue always reas constant (B) The energy with the control olue always reas constant (C) The luid properties ay change with location oer the cross section o the lets or s. (D) The luid low at any pot o any let and is unior and steady and the luid properties do not change with tie or location oer the cross section o an let or. (E) None o the aboe (). For diuser, we generally consider (A) W 0 (B) ke 0 (the diuser is designed to conert the low work to ketic energy) (C) Q >0 (D) pe 0 (E) None o the aboe (g). The change ketic energy can usually be ignored or (A) Diusers (B) Nozzles (C) Stea turbes (D) Throttlg ales (E) Heat exchangers (h). Stea (H O) lows through a pipe with an ner diaeter o 0 c at a pressure o 00 kpa and teperature o 00 o C. The speciic low energy ( P ) o stea the pipe is ostly close to (A) 6. / (Note: you need d the speciic olue o stea at gien T and P) (B) / (C) 07. / (D) 07. (E) None o the aboe
3 . Concept and short answer questions (0 pots) (a) Please draw a scheatic diagra o a doestic hot water tank delierg hot water to bathroo and kitchen, describe the therodynaic process oled, and list the assuptions, equations, and paraeters needed or you to d the water teperature o your hot water tank. ( pots) (b)the general equation o st law o therodynaics or control olue syste can be expressed as equation (a): de Q CV W + ( h + ke + pe) ( h + ke + pe) (a) dt Please list the assuptions needed or this general equation to be sipliied to equation (b) W turbe ( h h ) (b) Equation (b) can be used to calculate the power put o turbe. (4 pots) Answer: The assuptions clude: (a) steady operation with one let and one : de CV 0, dt (b) heat transer can be ignored: Q 0 (c) the changes ketic energy and potential energy can be ignored, so the keand pe ters can be dropped. (d) there is only one let and one, With these assuptions, Equation (a) can be re-written as: 0 W + h h 0 (c) With the known turbe, equation (c) can be urther reised to: turbe ( h ) W h h h (d) (c) Please expla i there is heat transer present with an adiabatic heat exchanger. ( pots)
4 . Hot air steadily enters a gas turbe at 5 bar, 900 K and s at bar, 600 K and a elocity o 00 /s. The ass low rate o air is 0 /s. Ignorg the heat transer, changes potential energy, and the ketic energy let, calculate (4 pots) (a) The power put ro this turbe, kw. Solution: Analysis (a) This question is associated with st law application control olue syste; (b) the syste is control olue syste understudy operation; (c) There is only one let and one, and thus ; (d) The energy balance or this steady-low syste can be expressed the rate or as V 0 V dec Q + W + h + + gz Q + W + h + + gz () dt V Or 0 V dec Q W + h + + gz h + + gz dt The ketic energy at let is negligible: V n 0. Heat transer Q 0 or Q 0 Q 0 Changes potential energy eects ( pe 0) are also negligible. Equation () can be sipliied and re-written as V W h h () V Or W ( h n h ) () You can d the enthalpy o air at let and Table A-7: h hair ( 900K) 9. 9 h hair ( 600K) Load enthalpy and elocity to equation (), you can d: W ( h h V / ) 0 / s 9.9 / / 09.kW (00 ) s J / s 000J 4
5 W ( h h V / ) J Or 0 / s 9.9 / / (00 ) s / s 000J 09.kW Note: () the positie dicates the transer o work ro syste to enironent. () I the ketic energy at ( 00 ) was ignored, the power put o this turbe is s 59. kw. The error caused by this ignorance is ab.6%, which is ery sall. This explas why the changes ketic energy can be ignored when solg therodynaic questions associated with turbe, copressor, and an. (b) The cross-section area o the,. Solution: The ass low rate is a unction o olue low rate and speciic olue or density. ρ V A V A / () The speciic olue can be ound usg ideal gas equation: P ν RT RT () P Load speciic olue to equation (), you can get: RT A () VP The gas constant R0.87 kpa. /.K can be obtaed ro Table A-. Load known ariables to equation (), you can d the area o : RT (0 / s)(0.87kpa / K)(600K) 0. 7 VP (00 / s)(00kpa) A 5
6 4. Nitrogen at 80 kpa and 400 K enters an adiabatic diuser steadily at a low rate o 6000 /h at 0 /s and leaes at 00 kpa at 0 /s. (4 pots) (a) Describe the a unction o diuser ( pots) Answer: The a unction o diuser is the slow down the high speed low through the conersion o ketic energy to ternal energy by creasg the pressure o luid. (b) Fd the teperature o nitrogen (6 pots) Solution: Analysis (a) There is only one let and one, and thus. We take diuser as the syste, which is a control olue sce ass crosses the boundary. The energy balance or this steady-low syste can be expressed the rate or as V V 0 dec Q W + h + + gz h + + gz () dt For nozzle, you can ignore the heat transer Q 0, work transer W 0, and changes potential energy gz 0, Equation () can be sipliied: or, h ( h + V / h ) 0 V V h + () You can d the speciic enthalpy at let Table A-8,640 hn (400K) kol h hn (400K) MW N 8 kol Load h and elocity at let and to equation () h V V h / + ( 0 /s) ( 0 /s) / 000 /s 44.7 / The ole-based speciic enthalpy at : kh hn, hn MWN , kol Fro Table A-8, you can d teperature o N at with the known enthalpy usg terpolation: 6
7 T 40 K (c) The cross-section area at the o the diuser (6 pots) Solution: The equation or calculation o ass low rate: AV ( 40 40) K 44. K The area o diuser can be ound ass low rate can be calculated A V The speciic olue o air at the diuser can be ound usg ideal gas equation: RT P The are can be ound: A V ( kpa / K)( K) ( 00 kpa) / (6000 h h )(.6 600s 0 /s /)
8 5. A copressor copresses the saturated R-4a apor at bar to 4 bar and 50 o C at a low rate o 0. /s. Ignorg the heat transer and the changes potential energy and ketic energy, detere (4 pots) Note to TA: Please pay attention to ass low rate when gradg this hoework. The ass low rate this question is 0. /s. I student used 0.0 /s, then this hoework should be graded as zero as it was the solution or an old hoework. (a) The olue low rate o R-4a at the. Analysis: The olue low rate is a unction o ass low rate and speciic olue V With the known ass low rate, 0. / s, you need d the speciic olue at gien teperature and pressure at prior to the calculation o olue low rate. To d the speciic olue, you need d the phase o R-4a and then the speciic olue with the proper property table. Solution: The phase o a substance can be ound by coparg the gien teperature (pressure) with saturation teperature at gien pressure (teperature): Table A-, T T 8.9 C < T 50 C 4bar 400kPa The R-4a the copressor as superheated apor. The speciic olue o R-4a at can be ound Table A- Superheated Vapor 4bar,50 0.4MPa,50 C The olue low rate can be calculated: V s s (b) The power needed or this copressor ( kw) Solution: the st law o therodynaics o a steady operation control olue syste can be expressed as: Q W + h + ke + pe h + ke + pe ( ) ( ) 0 With the ignorance o heat transer, the changes potential and ketic energy, and the assuption o one let and one, this equation can be sipliied to W copressor + ( h h ) 0 W h h copressor ( ) The speciic enthalpy o R-4a can be ound property Table. State : Saturated R-4a apor at bar00 kpa h bar 00kPa (Table A-: Pressure Table) State : Superheated R-4a Vapor, which has been ound (a) 8
9 h 4bar,50 C h@ 0.4MPa,50 C (Table A-: Superheated R-4a) The power consuption o copressor can be ound: W copressor ( h h ) 0. ( ) kW s s Note: The negatie sign dicates that copressor consues power its operation, which is consistent with our coon knowledge o copressor. 9
10 6. A condenser (heat exchanger) is designed to cool / o water apor at MPa and 500 o C to a saturated liquid at MPa. The coolg water is puped ro a local rier at 5 o C. Ater passg through the condenser, the teperature o the coolg water is restricted by the enironental code not to exceed 5 o C. Considerg the coolg water is copressible liquid, detere the iu ass low rate o coolg water. (6 pots) T 5 o C w? P MPa s/ T 4 <5 o C w? P MPa T 500 o C s/ Note to TA: Please pay attention to the axiu teperature o the coolg water when gradg this hoework. The the axiu teperature o the coolg water is 5 C. I student used 0 C, then this hoework should be graded as zero as it was the solution or an old hoework. Solution: st Law o therodynaics under steady operatg process can be expressed as: ( h + ke + pe) ( h + ke + pe) 0 Q W + (a) For heat exchanger, the heat transer between heat exchanger and enironent, work transer, changes potential energy and ketic energy can be ignored: The st law equation or this steady-low process can be re-arranged as: h h 0 or h h (b) There are two lets and two s as shown Figure, the orer equation can be urther re-written as: sh + wh sh + wh4 (c) This equation can be urther re-written to d the ass low rate o coolg water: s ( h h ) w (d) ( h4 h ) The change enthalpy o liquid water (copressible substance) can be ound usg equation: h h C ( T ) w (e) T Load equation (e) to (d), you can get; s ( h h ) s ( h h ) w () ( h h ) C ( T T ) 4 In equation (), the ass low rate o stea, the enthalpy o stea at let, and, let teperature o coolg water are either known oration or paraeters can be ound with known w 4
11 oration. Accordgly, the iu ass low rate o coolg water is obtaed with axiu teperature o coolg water, T 4 5 C At let : water, P MPa 000kPa, T 500 C, Sce 000kPa C < T, the phase o water at let is superheated apor. Fro Table A-6, h 479. / ; Exit : water, P MPa 000kPa, saturated liquid Fro table A-5, h h 76.5 / Fro Table A-, C w 4. / K Hence: ( h h ) s / ( ) /, iuw 77.5 ( ) o o C T T (4. / C) (5 5) C w 4,axiu /
12 7. A 4 L (olue) o pressure cooker a kitchen operates at 00 kpa with an area o 0. With well controlled heat transer ro range, liquid water is aporized to saturated apor, which s the pressure cooker at a constant ass low rate. Initially, the pressure cooker contas saturated water. Ater two hours o cookg, o saturated water apor let the pressure cooker. Durg this process, the heat loss ro the pressure cooker to the kitchen is 00. The changes potential and ketic energy can be ignored. (6 pots) Note to TA: Please pay attention to the heat loss ro cooker to kitchen, which is 00 this question. I student used 00, please ark this hoework as zero as the student ay hae copied ro past year solution. a) Please expla whether this pressure cooker is operatg under steady-low process or not; Answer: This pressure cooker is not operatg under steady operation as the ass o water contaed the pressure cooker is decreasg with tie. b) Fd the elocity o saturated apor, /s Solution: Notes: water s this pressure cooker as saturated stea. The elocity o stea g the pressure cooker can be ound usg the equation calculatg the ass low rate o stea: VA ρv ρva (a) This equation can be re-arranged (re-written) to calculate the elocity: V (b) A Note: With the known area, you still need d the ass low rate, speciic olue o saturated apor (c) t 600s s hour hour g kPa Load the cross-section area, ass low rate and speciic olue to equation (b), you can d the elocity: s V 4. 6 A s c) The speciic olue, quality, speciic ternal energy o water at State and State Solution: State : L V L 0. 00
13 At 00 kpa, , g The phase o water pressure tank at state can be ound by coparg the speciic olue o water with the speciic olue o saturated liquid water and saturated water apor g. Sce x u State : < < g, so the water is saturated ixture g u + xu g L V L At 00 kpa, ( ) , g The phase o water pressure tank at state can be ound by coparg the speciic olue o water with the speciic olue o saturated liquid water and saturated water apor g. Sce x < < g, so the water is saturated ixture g 0.00 With the known quality, you can d the speciic ternal energy o the saturated ixture. u u + xu g d) The heat transerred ro the range to the pressure cooker durg this one-hour process, Solution: the st law o therodynaics or a transient operation control olue syste can be expressed as: Q Q + W W + h + V + gz h + V + gz ECV, ECV, U CV, There is no work transer and ass transer to the pressure cooker. The changes the potential energy can be ignored. This equation can be sipliied to: U CV,
14 Q Q h + V E CV, E CV, U CV, U CV, u u Note: please expla i or i u u ( u u) can be applied this pressure cooker question. The heat transer to the syste can be ound: Q u u + Q + h + V J 000J 8. The concern to global issues is always debatable due to its direct and direct ipact on our counity, town, and state, etc but sees general not aectg the lie o college students. Howeer, this ay not be true West Virgia. The tuition ee WVU has been raised the past years due to the budget cut and expected reenue loss West Virgia, and other unexplaable reasons raised by our State Goernent, and Uniersity Adistrator. Please write an essay to expla the possible connection between WVU tuition ee creases with global issues, and describe how a echanical engeer with therodynaic knowledge can help solg global issues your uture career. The essay ust be at least 000 words, typed usg Ties New Roan typeace and a ont size o pot. It would be appreciated i you can clude a title your essay and list at least three reerences cited. (0 pots) Suggested Book Probles to Reiew: These probles will not be collected, but are suggested as a reiew. Chapter 5: 5, 0,, 4, 7,,, 4, 47, 57, 6, 68, 78, 87, 90, 97, 06, 7,, 4, 6 4
Number of extra papers used if any
Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa Circle your structor s last nae Diision 1 (7:0): Naik Diision (1:0): Wassgren Diision 6 (11:0): Sojka Diision (9:0): Choi Diision 4 (8:0):
More informationChapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
5- Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL OLUMES Conseration of Mass 5-C Mass, energy, momentum, and electric charge are consered, and olume and entropy are not consered durg a process. 5-C Mass
More informationME 200 Thermodynamics 1 Spring Exam 2
Last Name: First Name: Thermo no. ME 200 Thermodynamics 1 Sprg 2017 - Exam 2 Circle your structor s last name Ardekani Fisher Hess Naik Sojka (onle and on campus) INSTRUCTIONS This is a closed book and
More informationME 200 Thermodynamics 1 Fall 2017 Exam 3
ME 200 hermodynamics 1 Fall 2017 Exam Circle your structor s last name Division 1: Naik Division : Wassgren Division 6: Braun Division 2: Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer
More informationME 200 Exam 2 October 22, :30 p.m. to 7:30 p.m.
CIRCLE YOUR LECTURE BELOW: First Name Solution Last Name 7:0 a.m. 8:0 a.m. 10:0 a.m. 11:0 a.m. Boregowda Boregowda Braun Bae :0 p.m. :0 p.m. 4:0 p.m. Meyer Naik Hess ME 00 Exam October, 015 6:0 p.m. to
More informationNumber of extra papers used if any
Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa 1 Circle your instructor s last nae Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division (9:0): Choi Division
More information300 kpa 77 C. (d) If we neglect kinetic energy in the calculation of energy transport by mass
6-6- Air flows steadily a ie at a secified state. The diameter of the ie, the rate of flow energy, and the rate of energy transort by mass are to be determed. Also, the error oled the determation of energy
More informationNumber of extra papers used if any
Last Name: First Name: Thermo no. ME 200 Thermodynamics 1 Fall 2018 Exam Circle your structor s last name Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division 2 (9:0): Choi
More informationKNOWN: Pressure, temperature, and velocity of steam entering a 1.6-cm-diameter pipe.
4.3 Steam enters a.6-cm-diameter pipe at 80 bar and 600 o C with a velocity of 50 m/s. Determine the mass flow rate, in kg/s. KNOWN: Pressure, temperature, and velocity of steam entering a.6-cm-diameter
More informationENT 254: Applied Thermodynamics
ENT 54: Applied Thermodynamics Mr. Azizul bin Mohamad Mechanical Engineering Program School of Mechatronic Engineering Universiti Malaysia Perlis (UniMAP) azizul@unimap.edu.my 019-4747351 04-9798679 Chapter
More informationThe First Law of Thermodynamics. By: Yidnekachew Messele
The First Law of Thermodynamics By: Yidnekachew Messele It is the law that relates the various forms of energies for system of different types. It is simply the expression of the conservation of energy
More informationIntroduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles
Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles by James Doane, PhD, PE Contents 1.0 Course Oeriew... 4.0 Basic Concepts of Thermodynamics... 4.1 Temperature
More informationCircle your instructor s last name
ME 00 Thermodynamics Fall 07 Exam Circle your structor s last name Division : Naik Division : Wassgren Division 6: Braun Division : Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer INSTRUCTIONS
More informationME 300 Thermodynamics II Exam 2 November 13, :00 p.m. 9:00 p.m.
ME 300 Therodynaics II Exa 2 Noveber 3, 202 8:00 p.. 9:00 p.. Nae: Solution Section (Circle One): Sojka Naik :30 a.. :30 p.. Instructions: This is a closed book/notes exa. You ay use a calculator. You
More informationChapter 5. Mass and Energy Analysis of Control Volumes
Chapter 5 Mass and Energy Analysis of Control Volumes Conservation Principles for Control volumes The conservation of mass and the conservation of energy principles for open systems (or control volumes)
More informationDelft University of Technology DEPARTMENT OF AEROSPACE ENGINEERING
Delft University of Technology DEPRTMENT OF EROSPCE ENGINEERING Course: Physics I (E-04) Course year: Date: 7-0-0 Time: 4:00-7:00 Student name and itials (capital letters): Student number:. You have attended
More informationI. Concepts and Definitions. I. Concepts and Definitions
F. Properties of a syste (we use the to calculate changes in energy) 1. A property is a characteristic of a syste that can be given a nuerical value without considering the history of the syste. Exaples
More informationDaniel López Gaxiola 1 Student View Jason M. Keith
Suppleental Material for Transport Process and Separation Process Principles Chapter Principles of Moentu Transfer and Overall Balances In fuel cells, the fuel is usually in gas or liquid phase. Thus,
More informationME 200 Exam 2 October 16, :30 p.m. to 7:30 p.m.
CIRCLE YOUR LECTURE BELOW: First Name Solution Last Name 7:30 am 8:30 am 10:30 am 11:30 am Joglekar Bae Gore Abraham 1:30 pm 3:30 pm 4:30 pm Naik Naik Cheung ME 200 Exam 2 October 16, 2013 6:30 p.m. to
More informationSchool of Aerospace Engineering Equilibrium Diagrams and Saturated Liquid/Vapor Systems
School o Aerospace Enineerin Equilibriu Diaras and Saturated Liquid/Vapor Systes In equilibriu, dierent phases o atter as, liquid, solid (also ultiple solid phases, e.., dierent crystalline structures
More informationME Thermodynamics I
Homework - Week 01 HW-01 (25 points) Given: 5 Schematic of the solar cell/solar panel Find: 5 Identify the system and the heat/work interactions associated with it. Show the direction of the interactions.
More informationCHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Thermodynamics: An Engineering Approach 8th Edition in SI Units Yunus A. Çengel, Michael A. Boles McGraw-Hill, 2015 CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES Lecture slides by Dr. Fawzi Elfghi
More informationChapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 5 Mass and Energy Analysis of Control Volumes by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics:
More informationMAE 320 HW 7B. 1e. For an isolated system, please circle the parameter which will change with time. (a) Total energy;
MAE 320 HW 7B his comprehensive homework is due Monday, December 5 th, 206. Each problem is worth the points indicated. Copying of the solution from another is not acceptable. Multi-choice, multi-answer
More informationChapter 7: The Second Law of Thermodynamics
Chapter 7: he Second Law of hermodynamics he second law of thermodynamics asserts that processes occur in a certain direction and that the energy has quality as well as quantity he first law places no
More informationENERGY TRANSFER BY WORK: Electrical Work: When N Coulombs of electrical charge move through a potential difference V
Weight, W = mg Where m=mass, g=gravitational acceleration ENERGY TRANSFER BY WOR: Sign convention: Work done on a system = (+) Work done by a system = (-) Density, ρ = m V kg m 3 Where m=mass, V =Volume
More information(SP 1) DLLL. Given: In a closed rigid tank,
(SP 1) Given: In a closed rigid tank, State 1: m 1,ice = 1, m 1,g = 0.05 P1= 0.0381 kpa, T1= -30 o C State 2: the liquid vapor equilibrium line, either saturated liquid or saturated vapor Find: (a) The
More informationChapter 4: Properties of Pure Substances. Pure Substance. Phases of a Pure Substance. Phase-Change Processes of Pure Substances
Chapter 4: roperties o ure Substances ure Substance A substance that has a ixed chemical composition throughout is called a pure substance such as water, air, and nitrogen A pure substance does not hae
More informationChapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky
Chapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky School of Chemical, Biological, and Enironmental Engineering Oregon State Uniersity 1.1 (b) The olume of water
More informationd dt T R m n p 1. (A) 4. (4) Carnot engine T Refrigerating effect W COPref. = 1 4 kw 5. (A)
. (A). (C) 5. (C) 7. ( to 5) 9. (C) 6. (C). (C). (D) 6. (A) 8. (0.6 to 0.66) 50. (D) 6. (C). (A) 5. (C) 7. (A) 9. (C) 5. (D) 6. (C). () 6. (C) 8. (600) 0. (D) 5. (B) 6. (D) 5. (A) 7. (A) 9. (D). (C) 5.
More informationME 200 Final Exam December 14, :00 a.m. to 10:00 a.m.
CIRCLE YOUR LECTURE BELOW: First Name Last Name 7:30 a.m. 8:30 a.m. 10:30 a.m. 11:30 a.m. Boregowda Boregowda Braun Bae 2:30 p.m. 3:30 p.m. 4:30 p.m. Meyer Naik Hess ME 200 Final Exam December 14, 2015
More informationMain components of the above cycle are: 1) Boiler (steam generator) heat exchanger 2) Turbine generates work 3) Condenser heat exchanger 4) Pump
Introducton to Terodynacs, Lecture -5 Pro. G. Cccarell (0 Applcaton o Control olue Energy Analyss Most terodynac devces consst o a seres o coponents operatng n a cycle, e.g., stea power plant Man coponents
More informationDepartment of Civil Engineering & Applied Mechanics McGill University, Montreal, Quebec Canada
Department f Ciil ngeerg Applied Mechanics McGill Uniersity, Mntreal, Quebec Canada CI 90 THRMODYNAMICS HAT TRANSFR Assignment #4 SOLUTIONS. A 68-kg man whse aerage bdy temperature is 9 C drks L f cld
More information7. Momentum balances Partly based on Chapter 7 of the De Nevers textbook (sections ).
Lecture Notes CHE 31 Fluid Mechanics (Fall 010) 7 Moentu balances Partly based on Chater 7 of the De Neers tetbook (sections 71-73) Introduction Net to ass and energy oentu is an iortant quantity fluid
More informationENGINEERING OF NUCLEAR REACTORS. Tuesday, October 9 th, 2014, 1:00 2:30 p.m.
.31 ENGINEERING OF NUCLEAR REACTORS Tuesday, October 9 th, 014, 1:00 :30 p.m. OEN BOOK QUIZ 1 (solutions) roblem 1 (50%) Loss o condensate pump transient in a LWR condenser i) Consider the seaater in the
More informationLecture 6. Announcements. Conservation Laws: The Most Powerful Laws of Physics. Conservation Laws Why they are so powerful
Conseration Laws: The Most Powerful Laws of Physics Potential Energy gh Moentu p = + +. Energy E = PE + KE +. Kinetic Energy / Announceents Mon., Sept. : Second Law of Therodynaics Gie out Hoework 4 Wed.,
More informationAll Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.
Miscellaneous Notes he end is near don t get behind. All Excuses ust be taken to 233 Loois before 4:15, Monday, April 30. he PHYS 213 final exa ties are * 8-10 AM, Monday, May 7 * 8-10 AM, uesday, May
More informationSF Chemical Kinetics.
SF Cheical Kinetics. Lecture 5. Microscopic theory of cheical reaction inetics. Microscopic theories of cheical reaction inetics. basic ai is to calculate the rate constant for a cheical reaction fro first
More informationME 300 Thermodynamics II
ME 300 Thermodynamics II Prof. S. H. Frankel Fall 2006 ME 300 Thermodynamics II 1 Week 1 Introduction/Motivation Review Unsteady analysis NEW! ME 300 Thermodynamics II 2 Today s Outline Introductions/motivations
More informationStep 1: Draw a diagram to represent the system. Draw a T-s process diagram to better visualize the processes occurring during the cycle.
ENSC 61 Tutorial, eek#8 Ga Refrigeration Cycle A refrigeration yte ug a the workg fluid, conit of an ideal Brayton cycle run revere with a teperature and preure at the let of the copreor of 37C and 100
More informationOzone (O 3 ) in upper atmosphere blocks ultraviolet (UV) light from Sun. UV causes skin cancer and cataracts.
Unit 9: The Gas Laws The Atosphere an ocean of gases ixed together Coposition nitrogen (N ) ~78% oxygen (O ).~% argon (Ar).~0.93% carbon dioxide (CO )..~0.03% water apor (H O) ~0.% Trace aounts of: He,
More information8.012 Physics I: Classical Mechanics Fall 2008
MIT OpenCourseWare http://ocw.it.edu 8.012 Physics I: Classical Mechanics Fall 2008 For inforation about citing these aterials or our Ters of Use, isit: http://ocw.it.edu/ters. MASSACHUSETTS INSTITUTE
More informationFind: a) Mass of the air, in kg, b) final temperature of the air, in K, and c) amount of entropy produced, in kj/k.
PROBLEM 6.25 Three m 3 of air in a rigid, insulated container fitted with a paddle wheel is initially at 295 K, 200 kpa. The air receives 1546 kj of work from the paddle wheel. Assuming the ideal gas model,
More informationI affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class.
Che340 hysical Cheistry for Biocheists Exa 3 Apr 5, 0 Your Nae _ I affir that I have never given nor received aid on this exaination. I understand that cheating in the exa will result in a grade F for
More informationMAE 320 Thermodynamics HW 4 Assignment
MAE 0 Thermodynamics HW 4 Assignment The homework is de Friday, October 7 th, 06. Each problem is worth the points indicated. Copying of the soltion from any sorce is not acceptable. (). Mltiple choice
More informationMomentum, p = m v. Collisions and Work(L8) Crash! Momentum and Collisions. Conservation of Momentum. elastic collisions
Collisions and Work(L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details
More informationOutline. Example. Solution. Property evaluation examples Specific heat Internal energy, enthalpy, and specific heats of solids and liquids Examples
Outline Property ealuation examples Specific heat Internal energy, enthalpy, and specific heats of solids and liquids s A piston-cylinder deice initially contains 0.5m of saturated water apor at 00kPa.
More informationTemperature and Thermodynamics, Part II. Topics to be Covered
Teperature and Therodynaics, Part II Topics to be Covered Profiles of Teperature in the Boundary Layer Potential teperature Adiabatic Lapse Rate Theral Stratification 1/8/17 Why are We Interested in Theral
More informationMAE 110A. Homework 6: Solutions 11/9/2017
MAE 110A Hoework 6: Solutions 11/9/2017 H6.1: Two kg of H2O contained in a piston-cylinder assebly, initially at 1.0 bar and 140 C undergoes an internally ersible, isotheral copression to 25 bar. Given
More informationEXAM # 1 CIRCLE YOUR LECTURE BELOW: 8:30 am 11:30 am 2:30 pm Prof. Memon Prof. Naik Prof. Lucht INSTRUCTIONS
Last Name First Name CIRCLE YOUR LECTURE BELOW: 8: am : am : pm Prof. Memon Prof. Naik Prof. Lucht EXAM # INSTRUCTIONS. This is a closed book examination. An equation sheet and all needed property tables
More informationProblem 1 The turbine is an open system. We identify the steam contained the turbine as the control volume. dt + + =
ME Fall 8 HW olution Problem he turbe i an open ytem. We identiy the team contaed the turbe a the control volume. Ma conervation: t law o thermodynamic: Aumption: dm m m m dt + + de V V V m h + + gz +
More informationECE309 THERMODYNAMICS & HEAT TRANSFER MIDTERM EXAMINATION. Instructor: R. Culham. Name: Student ID Number:
ECE309 THERMODYNAMICS & HEAT TRANSFER MIDTERM EXAMINATION June 19, 2015 2:30 pm - 4:30 pm Instructor: R. Culham Name: Student ID Number: Instructions 1. This is a 2 hour, closed-book examination. 2. Permitted
More informationMomentum, p. Crash! Collisions (L8) Momentum is conserved. Football provides many collision examples to think about!
Collisions (L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details of the
More information1 st Law Analysis of Control Volume (open system) Chapter 6
1 st Law Analysis of Control Volume (open system) Chapter 6 In chapter 5, we did 1st law analysis for a control mass (closed system). In this chapter the analysis of the 1st law will be on a control volume
More informationc Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)
Thermodynamic Processes & Isentropic Efficiency Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-1000, Bangladesh zahurul@me.buet.ac.bd
More informationWeek 8. Steady Flow Engineering Devices. GENESYS Laboratory
Week 8. Steady Flow Engineering Devices Objectives 1. Solve energy balance problems for common steady-flow devices such as nozzles, compressors, turbines, throttling valves, mixers, heaters, and heat exchangers
More informationTwo mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW SVCET
Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW 1. What do you understand by pure substance? A pure substance is defined as one that is homogeneous and invariable in chemical composition
More informationReading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.
PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction
More informationChapter 5: The First Law of Thermodynamics: Closed Systems
Chapter 5: The First Law of Thermodynamics: Closed Systems The first law of thermodynamics can be simply stated as follows: during an interaction between a system and its surroundings, the amount of energy
More information6-5. H 2 O 200 kpa 200 C Q. Entropy Changes of Pure Substances
Canges f ure Substances 6-0C Yes, because an ternally reversible, adiabatic prcess vlves n irreversibilities r eat transfer. 6- e radiatr f a steam eatg system is itially filled wit supereated steam. e
More informationAnswers to assigned problems from Chapter 1
Answers to assigned probles fro Chapter 1 1.7. a. A colun of ercury 1 in cross-sectional area and 0.001 in height has a volue of 0.001 and a ass of 0.001 1 595.1 kg. Then 1 Hg 0.001 1 595.1 kg 9.806 65
More informationEngineering Thermodynamics. Chapter 4. The First Law of Thermodynamics
Chater 4 The First Law of Thermodynamics It is the law that relates the arious forms of energies for system of different tyes. It is simly the exression of the conseration of energy rcile The first law
More informationME 201 Thermodynamics
8 ME 0 Thermodynamics Practice Problems or Property Evaluation For each process described below provide the temperature, pressure, and speciic volume at each state and the change in enthalpy, internal
More informationLECTURE NOTE THERMODYNAMICS (GEC 221)
LETURE NOTE ON THERMODYNAMIS (GE ) Thermodynamics is the branch of science that treats the arious phenomena of energy and related properties of matter especially the relationship between heat, work and
More informationI. Understand get a conceptual grasp of the problem
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Departent o Physics Physics 81T Fall Ter 4 Class Proble 1: Solution Proble 1 A car is driving at a constant but unknown velocity,, on a straightaway A otorcycle is
More informationChapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 7 Entropy by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics: An Engineering Approach, 5th ed.,
More informationCHAPTER INTRODUCTION AND BASIC PRINCIPLES. (Tutorial). Determine if the following properties of the system are intensive or extensive properties: Property Intensive Extensive Volume Density Conductivity
More informationPhysics 102 Homework Solutions: Ch 16
Physics 0 Hoework Solutions: Ch 6. SSM REASONING Since light behaes as a wae, its speed, requency, and waelength λ are related to according to = λ (Equation 6.). We can sole this equation or the requency
More informationME 201 Thermodynamics
ME 0 Thermodynamics Solutions First Law Practice Problems. Consider a balloon that has been blown up inside a building and has been allowed to come to equilibrium with the inside temperature of 5 C and
More informationPTT 277/3 APPLIED THERMODYNAMICS SEM 1 (2013/2014)
PTT 77/3 APPLIED THERMODYNAMICS SEM 1 (013/014) 1 Energy can exist in numerous forms: Thermal Mechanical Kinetic Potential Electric Magnetic Chemical Nuclear The total energy of a system on a unit mass:
More informationfirst law of ThermodyNamics
first law of ThermodyNamics First law of thermodynamics - Principle of conservation of energy - Energy can be neither created nor destroyed Basic statement When any closed system is taken through a cycle,
More informationDishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)
HW-1 (25 points) (a) Given: 1 for writing given, find, EFD, etc., Schematic of a household piping system Find: Identify system and location on the system boundary where the system interacts with the environment
More informationME Thermodynamics I. Lecture Notes and Example Problems
ME 227.3 Thermodynamics I Lecture Notes and Example Problems James D. Bugg September 2018 Department of Mechanical Engineering Introduction Part I: Lecture Notes This part contains handout versions of
More informationKinetic Molecular Theory of. IGL is a purely empirical law - solely the
Lecture -3. Kinetic Molecular Theory of Ideal Gases Last Lecture. IGL is a purely epirical law - solely the consequence of experiental obserations Explains the behaior of gases oer a liited range of conditions.
More informationI. (20%) Answer the following True (T) or False (F). If false, explain why for full credit.
I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit. Both the Kelvin and Fahrenheit scales are absolute temperature scales. Specific volume, v, is an intensive property,
More informationPhys102 First Major-143 Zero Version Coordinator: xyz Sunday, June 28, 2015 Page: 1
Coordinator: xyz Sunday, June 28, 2015 Page: 1 Q1. A transverse sinusoidal wave propagating along a stretched string is described by the following equation: y (x,t) = 0.350 sin [1.25x + 99.6t], where x
More informationDistillation. The Continuous Column. Learning Outcomes. Recap - VLE for Meth H 2 O. Gavin Duffy School of Electrical Engineering DIT Kevin Street
Distillation The Continuous Colun Gavin Duffy School of Electrical Engineering DIT Kevin Street Learning Outcoes After this lecture you should be able to.. Describe how continuous distillation works List
More informationThe average velocity of water in the tube and the Reynolds number are Hot R-134a
hater 0:, 8, 4, 47, 50, 5, 55, 7, 75, 77, 8 and 85. 0- Refrigerant-4a is cooled by water a double-ie heat exchanger. he overall heat transfer coefficient is to be determed. Assumtions he thermal resistance
More information8-4 P 2. = 12 kw. AIR T = const. Therefore, Q &
8-4 8-4 Air i compreed teadily by a compreor. e air temperature i mataed contant by eat rejection to te urroundg. e rate o entropy cange o air i to be determed. Aumption i i a teady-low proce ce tere i
More informationMAE 11. Homework 8: Solutions 11/30/2018
MAE 11 Homework 8: Solutions 11/30/2018 MAE 11 Fall 2018 HW #8 Due: Friday, November 30 (beginning of class at 12:00p) Requirements:: Include T s diagram for all cycles. Also include p v diagrams for Ch
More informationEVALUATION OF THERMAL CONDUCTIVITY IN PITCH- BASED CARBON FIBER REINFORCED PLASTICS
16 TH INTERNATIONA CONFERENCE ON COMPOSITE MATERIAS EVAUATION OF THERMA CONDUCTIVITY IN PITCH- BASED CARBON FIBER REINFORCED PASTICS Shinji Ogihara*, Makoto Yaaguchi**, Takahito Chiba**, Junichi Shiizu****,
More informationMolecular Speeds. Real Gasses. Ideal Gas Law. Reasonable. Why the breakdown? P-V Diagram. Using moles. Using molecules
Kinetic Theory of Gases Connect icroscopic properties (kinetic energy and oentu) of olecules to acroscopic state properties of a gas (teperature and pressure). P v v 3 3 3 But K v and P kt K v kt Teperature
More informationPhysics Momentum: Collisions
F A C U L T Y O F E D U C A T I O N Departent o Curriculu and Pedagogy Physics Moentu: Collisions Science and Matheatics Education Research Group Supported by UBC Teaching and Learning Enhanceent Fund
More informationQuotes. Review - First Law. Review - First Law. Review - First Law. Review - First Law. Thermodynamics Lecture Series
8//005 herodynaics ecture Series Entropy uantifyg Energy Degradation Applied Sciences Education Research Group (ASERG) Faculty of Applied Sciences Universiti eknologi MARA eail: drjjlanita@hotail.co http://www3.uit.edu.y/staff/drjj/
More informationTHERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.
THERMODYNAMICS, FLUID AND PLANT PROCESSES The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial. THERMODYNAMICS TUTORIAL 2 THERMODYNAMIC PRINCIPLES SAE
More informationKey Terms Electric Potential electrical potential energy per unit charge (JC -1 )
Chapter Seenteen: Electric Potential and Electric Energy Key Ter Electric Potential electrical potential energy per unit charge (JC -1 ) Page 1 of Electrical Potential Difference between two points is
More informationKinetic Molecular Theory of Ideal Gases
Lecture -3. Kinetic Molecular Theory of Ideal Gases Last Lecture. IGL is a purely epirical law - solely the consequence of experiental obserations Explains the behaior of gases oer a liited range of conditions.
More informationReadings for this homework assignment and upcoming lectures
Homework #3 (group) Tuesday, February 13 by 4:00 pm 5290 exercises (individual) Thursday, February 15 by 4:00 pm extra credit (individual) Thursday, February 15 by 4:00 pm Readings for this homework assignment
More information(b) The heat transfer can be determined from an energy balance on the system
8-5 Heat is transferred to a iston-cylinder device wit a set of stos. e work done, te eat transfer, te exergy destroyed, and te second-law efficiency are to be deterined. Assutions e device is stationary
More informationCRITICAL MASS FLOW RATE THROUGH CAPILLARY TUBES
Proceedings o the ASME 010 rd Joint US-European Fluids Engineering Summer Meeting and 8th International Conerence FESM-ICNMM010 August 1-5, 010, Montreal, Canada Proceedings o ASME 010 rd Joint US-European
More informationm potential kinetic forms of energy.
Spring, Chapter : A. near the surface of the earth. The forces of gravity and an ideal spring are conservative forces. With only the forces of an ideal spring and gravity acting on a ass, energy F F will
More informationCHAPTER 7 IMPULSE AND MOMENTUM
CHAPTER 7 IMPULSE AND MOMENTUM PROBLEMS 1. SSM REASONING The ipulse that the olleyball player applies to the ball can be ound ro the ipulse-oentu theore, Equation 7.4. Two orces act on the olleyball while
More information5/6/ :41 PM. Chapter 6. Using Entropy. Dr. Mohammad Abuhaiba, PE
Chapter 6 Using Entropy 1 2 Chapter Objective Means are introduced for analyzing systems from the 2 nd law perspective as they undergo processes that are not necessarily cycles. Objective: introduce entropy
More informationincreases. In part (b) the impulse and initial momentum are in opposite directions and the velocity decreases.
8IDENTIFY and SET U: p = K = EXECUTE: (a) 5 p = (, kg)( /s) = kg /s 5 p kg /s (b) (i) = = = 6 /s (ii) kg =, so T T SUV SUV, kg ( /s) 68 /s T SUV = T = = SUV kg EVALUATE:The SUV ust hae less speed to hae
More informationDESIGN & DEVELOPMENT OF COMBINED UNIT FOR AN AIR CONDITIONING & REFRIGERATION AND SIMULATION OF SYSTEM
http:// ESIGN & EVELOPMENT OF COMBINE UNIT FOR AN AIR CONITIONING & REFRIGERATION AN SIMULATION OF SYSTEM Arif O. Hannure 1, Avinash M. Patil 2 1 PG Student PVPIT, Budhgaon, Sangli. (India) 2 Vice Principal
More informationME 2322 Thermodynamics I PRE-LECTURE Lesson 10 Complete the items below Name:
Lesson 10 1. (5 pt) If P > P sat (T), the phase is a subcooled liquid. 2. (5 pt) if P < P sat (T), the phase is superheated vapor. 3. (5 pt) if T > T sat (P), the phase is superheated vapor. 4. (5 pt)
More informationME Thermodynamics I = = = 98.3% 1
HW-08 (25 points) i) : a) 1 Since ν f < ν < ν g we conclude the state is a Saturated Liquid-Vapor Mixture (SLVM) 1, from the saturation tables we obtain p 3.6154 bar. 1 Calculating the quality, x: x ν
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More informationElectronics Lecture 8 AC circuit analysis using phasors
Electronics Lecture 8 A circuit analysis usg phasors 8. Introduction The preious lecture discussed the transient response of an circuit to a step oltage by switchg a battery. This lecture will estigate
More informationME 2322 Thermodynamics I PRE-LECTURE Lesson 23 Complete the items below Name:
Lesson 23 1. (10 pt) Write the equation for the thermal efficiency of a Carnot heat engine below: T η = T 1 L H 2. (10 pt) Can the thermal efficiency of an actual engine ever exceed that of an equivalent
More information