logging in or signing up ThermCh03 Aric85 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 1485 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 04, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: Thermodynamics An Engineering Approach Fourth Edition Yunus A. Çengel Michael A. Boles Professor H.K. Ma National Taiwan University Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.Slide2: Properties of Pure Substances 3.1 Pure Substance: 3.1 Pure Substance A substance that has a fixed chemical composition throughout is called a Pure Substance. Pure Substance: - N2, O2, gaseous Air -A mixture of liquid and gaseous water is a pure substance, but a mixture of liquid and gaseous Air is not. 3.2 Phases of a Pure Substance: 3.2 Phases of a Pure Substance Solid: -The molecules in a solid are kept at their positions by the large springlike intermolecular forces. -The attractive and repulsive forces between the molecules tend to maintain them at relatively constant distances from each other. Liquid: Groups of molecules move about each other. Gas: Molecules move about at random. 3.3 Phase-Change Processes of Pure Substance: 3.3 Phase-Change Processes of Pure Substance Compressed liquid or a subcooled liquid: A liquid that is not about to vaporize. Saturated liquid: A liquid that is about to vaporize. Saturated vapor: A vapor that is about to condense. Saturated liquid-vapor mixture: the liquid and vapor phases coexist in equilibrium. Superheated vapor: A vapor that is not about to condense Slide6: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-1 FIGURE 3-11 T-v diagram for the heating process of water at constant pressure.3.3 Phase-Change Processes of Pure Substance: 3.3 Phase-Change Processes of Pure Substance Saturated temperature, Tsat: At a given pressure, the temperature at which a pure substance changes phase. Saturated pressure, Psat: At a given temperature, the pressure at which a pure substance changes phase. Latent heat: the amount of energy absorbed or released during a phase-change process. Latent heat of fusion: the amount of energy absorbed during melting. Latent heat of vaporization: the amount of energy absorbed during vaporization. 3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The T-v diagram: -Critical point: the point at which the saturated liquid and saturated vapor states are identical. -Saturated liquid line: -Saturated vapor line: -Compressed liquid region: -Superheated vapor region: -Saturated liquid-vapor mixture region: 3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The critical-point properties of water: - Pcr= 22.09MPa - Tcr= 374.14C - vcr= 0.003155 m3 /kg The critical-point properties of helium: - Pcr= 0.23MPa - Tcr= -267.85C - vcr= 0.01444 m3/kg Slide10: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-2 FIGURE 3-16 T-v diagram of constant-pressure phase-change processes of a pure substance at various pressures (numerical values are for water).Slide11: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-3 FIGURE 3-18 T-v diagram of a pure substance.3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The P-v diagram: - The triple line: three phases of a pure substance coexist in equilibrium, these triple-phase states forms a line. - The triple point: the triple line appears as a point on the P-T diagrams. For water, 0.01C & 0.06113 kPa -Sublimation: Passing from the solid phase directly into the vapor phase. The P-T diagram(phase diagram): The P-v-T surface: Slide13: FIGURE 3-19 P-v diagram of a pure substance. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-4Slide14: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-5 FIGURE 3-21 P-v diagram of a substance that contracts on freezing.Slide15: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-6 FIGURE 3-22 P-v diagram of a substance that expands on freezing (such as water).EVALUATING THERMODYNAMIC PROPERTIES: EVALUATING THERMODYNAMIC PROPERTIES The P-V-T Surface for WaterDescription of thermodynamic state: Description of thermodynamic stateExperimental basis: Experimental basis One independent property for each way that the energy of the system can be varied independently. Experimental basis: Experimental basis The number of independent properties that uniquely describes the state of the system is the number of relevant work interactions plus one.Simple, compressible systems: Simple, compressible systemsSimple chemical systems: Simple chemical systemsSimple compressible systems: Simple compressible systems f(p,V,T) = 0 p = p(V,T) V = V(p,T) State and Equilibrium: State and Equilibrium A simple compressible system: The state of a simple compressible system is completely specified by two independent, intensive properties. -two properties specified be independent to fix the state. -Once the two properties are fixed, all the other properties become dependent properties. p-V-T surfaces...: p-V-T surfaces...P-v-T Surfaces: P-v-T SurfacesState Equations : State Equations f(p,V,T) = 0 p(V,T) = p v(p,T) = V T(p,V) = T f(U,V,T) = 0 U = U(V,T) V = V (U, T) T = T(U,V)The p-V-T surface for water... : The p-V-T surface for water... The P-v-T surface for water: The P-v-T surface for waterSlide29: At a total constant pressure.... pThe p-V-T surface for water: The p-V-T surface for water Solid in equilibrium with vapor (0 oC) Solid in equilibrium with vapor and liquid (0 oC) Liquid and vapor in equilibrium ( 0 < T < 100 oC) Saturated Vapor (T = 100 oC) Superheated Vapor (T > 100 oC)The P-v-T Surface for Water: The P-v-T Surface for WaterThe p-T plane for water, Phase diagram: The p-T plane for water, Phase diagramWater: WaterWater: WaterSlide35: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-7 FIGURE 3-25 P-T diagram of pure substances.Slide36: FIGURE 3-26 P-v-T surface of a substance that contracts on freezing. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-8Slide37: FIGURE 3-27 P-v-T surface of a substance that expands on freezing (like water). Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-93.5 Property Tables: 3.5 Property Tables Table A-4: Saturated water-Temperature table Table A-5: Saturated water-Pressure table Table A-6: Superheated water Enthalpy, H H= U + PV (kj) h= u + Pv (kj/kg) Entropy, S Slide39: FIGURE 3-30 A partial list of Table A–4. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-10Slide40: FIGURE 3-40 A partial listing of Table A–6. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-11Quality...: Quality...Liquid-vapor equilibrium : Liquid-vapor equilibrium Quality: QualityThe two-phase region for water: The two-phase region for water Quality defined: Quality defined Quality, x, allows location of states inside the vapor-liquid region.Water: WaterQuality: QualityInternal energy in the vapor-liquid region: Internal energy in the vapor-liquid regionKey concepts and terms: Key concepts and terms Critical point P - v - T surface Quality Saturation pressure Saturation temperature State equation State surface The State Principle Triple point ADDITIONAL ASPECTS OF THE P-V-T SURFACE FOR WATER: ADDITIONAL ASPECTS OF THE P-V-T SURFACE FOR WATERThe P-v-T surface for water: The P-v-T surface for water Liquid Vapor- Liquid Critical Point Water: WaterAt the critical point for water: At the critical point for waterCompressed liquids: Compressed liquids3.6 The Ideal-Gas Equation of State: 3.6 The Ideal-Gas Equation of State Equation of state: Any equation that relates the pressure, temperature, and specific volume of a substance. Gas: The vapor phase of a substance Vapor: A gas that is not far from a state of condensation Definition of gas...: Definition of gas...Fluids and gases: Fluids and gases What is gas?: What is gas?The ideal gas...: The ideal gas...P-V-T relation for ideal gases: P-V-T relation for ideal gasesThe ideal gas equation of state: The ideal gas equation of state This implies: (1) very little molecular interaction (p = 0), (2) molecules are point masses, i.e., zero volume.The universal gas constant: The universal gas constantThe ideal gas state surface: The ideal gas state surfaceThe perfect gas: The perfect gas3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior: 3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior Compressibility Factor, Z Z = Pv/RT Z = vactual/videal Ideal gas: Z = 1 Real gases: Z > 1 Z = 1 Z < 13.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior: 3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior The normalization: -Reduced pressure, PR PR = P/ Pcr -Reduced temperature, TR TR = T/ Tcr The principle of corresponding states: The Z factor for all gases is approximately the same at the same reduced pressure and temperature.Real gases...: Real gases...Real Gases: Real Gases PReduced pressure and temperature: Reduced pressure and temperature Generalized Compressibility Chart (14.6)The virial form for compressibility: The virial form for compressibilitySlide71: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. FIGURE 3-49 Percentage of error involved in assuming steam to be an ideal gas, and the region where steam can be treated as an ideal gas with less than 1 percent error. 2-12Slide72: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-13 FIGURE 3-51 Comparison of Z factors for various gases.Slide73: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-14 FIGURE 3-60 Percentage of error involved in various equations of state for nitrogen.Slide74: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. FIGURE Ideal-gas constant-pressure specific heats for some gases (see Table A–2c for Cp equations). 2-153.8 Other Equations of State: 3.8 Other Equations of State Van der Waals Equation of state: Beattie-Bridgeman Equation of state: Benedict-Webb-Rubin Equation of state: Virial Equation of state:Key concepts and terms: Key concepts and terms Fluid Gas Ideal gas Perfect gas Compressibility factor Compressibility chart Local equilibrium Reduced pressure Reduced temperature Thermodynamic pressure Virial equation of state You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
ThermCh03 Aric85 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 1485 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 04, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: Thermodynamics An Engineering Approach Fourth Edition Yunus A. Çengel Michael A. Boles Professor H.K. Ma National Taiwan University Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.Slide2: Properties of Pure Substances 3.1 Pure Substance: 3.1 Pure Substance A substance that has a fixed chemical composition throughout is called a Pure Substance. Pure Substance: - N2, O2, gaseous Air -A mixture of liquid and gaseous water is a pure substance, but a mixture of liquid and gaseous Air is not. 3.2 Phases of a Pure Substance: 3.2 Phases of a Pure Substance Solid: -The molecules in a solid are kept at their positions by the large springlike intermolecular forces. -The attractive and repulsive forces between the molecules tend to maintain them at relatively constant distances from each other. Liquid: Groups of molecules move about each other. Gas: Molecules move about at random. 3.3 Phase-Change Processes of Pure Substance: 3.3 Phase-Change Processes of Pure Substance Compressed liquid or a subcooled liquid: A liquid that is not about to vaporize. Saturated liquid: A liquid that is about to vaporize. Saturated vapor: A vapor that is about to condense. Saturated liquid-vapor mixture: the liquid and vapor phases coexist in equilibrium. Superheated vapor: A vapor that is not about to condense Slide6: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-1 FIGURE 3-11 T-v diagram for the heating process of water at constant pressure.3.3 Phase-Change Processes of Pure Substance: 3.3 Phase-Change Processes of Pure Substance Saturated temperature, Tsat: At a given pressure, the temperature at which a pure substance changes phase. Saturated pressure, Psat: At a given temperature, the pressure at which a pure substance changes phase. Latent heat: the amount of energy absorbed or released during a phase-change process. Latent heat of fusion: the amount of energy absorbed during melting. Latent heat of vaporization: the amount of energy absorbed during vaporization. 3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The T-v diagram: -Critical point: the point at which the saturated liquid and saturated vapor states are identical. -Saturated liquid line: -Saturated vapor line: -Compressed liquid region: -Superheated vapor region: -Saturated liquid-vapor mixture region: 3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The critical-point properties of water: - Pcr= 22.09MPa - Tcr= 374.14C - vcr= 0.003155 m3 /kg The critical-point properties of helium: - Pcr= 0.23MPa - Tcr= -267.85C - vcr= 0.01444 m3/kg Slide10: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-2 FIGURE 3-16 T-v diagram of constant-pressure phase-change processes of a pure substance at various pressures (numerical values are for water).Slide11: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-3 FIGURE 3-18 T-v diagram of a pure substance.3.4 Property Diagrams for Phase-Change Processes: 3.4 Property Diagrams for Phase- Change Processes The P-v diagram: - The triple line: three phases of a pure substance coexist in equilibrium, these triple-phase states forms a line. - The triple point: the triple line appears as a point on the P-T diagrams. For water, 0.01C & 0.06113 kPa -Sublimation: Passing from the solid phase directly into the vapor phase. The P-T diagram(phase diagram): The P-v-T surface: Slide13: FIGURE 3-19 P-v diagram of a pure substance. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-4Slide14: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-5 FIGURE 3-21 P-v diagram of a substance that contracts on freezing.Slide15: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-6 FIGURE 3-22 P-v diagram of a substance that expands on freezing (such as water).EVALUATING THERMODYNAMIC PROPERTIES: EVALUATING THERMODYNAMIC PROPERTIES The P-V-T Surface for WaterDescription of thermodynamic state: Description of thermodynamic stateExperimental basis: Experimental basis One independent property for each way that the energy of the system can be varied independently. Experimental basis: Experimental basis The number of independent properties that uniquely describes the state of the system is the number of relevant work interactions plus one.Simple, compressible systems: Simple, compressible systemsSimple chemical systems: Simple chemical systemsSimple compressible systems: Simple compressible systems f(p,V,T) = 0 p = p(V,T) V = V(p,T) State and Equilibrium: State and Equilibrium A simple compressible system: The state of a simple compressible system is completely specified by two independent, intensive properties. -two properties specified be independent to fix the state. -Once the two properties are fixed, all the other properties become dependent properties. p-V-T surfaces...: p-V-T surfaces...P-v-T Surfaces: P-v-T SurfacesState Equations : State Equations f(p,V,T) = 0 p(V,T) = p v(p,T) = V T(p,V) = T f(U,V,T) = 0 U = U(V,T) V = V (U, T) T = T(U,V)The p-V-T surface for water... : The p-V-T surface for water... The P-v-T surface for water: The P-v-T surface for waterSlide29: At a total constant pressure.... pThe p-V-T surface for water: The p-V-T surface for water Solid in equilibrium with vapor (0 oC) Solid in equilibrium with vapor and liquid (0 oC) Liquid and vapor in equilibrium ( 0 < T < 100 oC) Saturated Vapor (T = 100 oC) Superheated Vapor (T > 100 oC)The P-v-T Surface for Water: The P-v-T Surface for WaterThe p-T plane for water, Phase diagram: The p-T plane for water, Phase diagramWater: WaterWater: WaterSlide35: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-7 FIGURE 3-25 P-T diagram of pure substances.Slide36: FIGURE 3-26 P-v-T surface of a substance that contracts on freezing. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-8Slide37: FIGURE 3-27 P-v-T surface of a substance that expands on freezing (like water). Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-93.5 Property Tables: 3.5 Property Tables Table A-4: Saturated water-Temperature table Table A-5: Saturated water-Pressure table Table A-6: Superheated water Enthalpy, H H= U + PV (kj) h= u + Pv (kj/kg) Entropy, S Slide39: FIGURE 3-30 A partial list of Table A–4. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-10Slide40: FIGURE 3-40 A partial listing of Table A–6. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-11Quality...: Quality...Liquid-vapor equilibrium : Liquid-vapor equilibrium Quality: QualityThe two-phase region for water: The two-phase region for water Quality defined: Quality defined Quality, x, allows location of states inside the vapor-liquid region.Water: WaterQuality: QualityInternal energy in the vapor-liquid region: Internal energy in the vapor-liquid regionKey concepts and terms: Key concepts and terms Critical point P - v - T surface Quality Saturation pressure Saturation temperature State equation State surface The State Principle Triple point ADDITIONAL ASPECTS OF THE P-V-T SURFACE FOR WATER: ADDITIONAL ASPECTS OF THE P-V-T SURFACE FOR WATERThe P-v-T surface for water: The P-v-T surface for water Liquid Vapor- Liquid Critical Point Water: WaterAt the critical point for water: At the critical point for waterCompressed liquids: Compressed liquids3.6 The Ideal-Gas Equation of State: 3.6 The Ideal-Gas Equation of State Equation of state: Any equation that relates the pressure, temperature, and specific volume of a substance. Gas: The vapor phase of a substance Vapor: A gas that is not far from a state of condensation Definition of gas...: Definition of gas...Fluids and gases: Fluids and gases What is gas?: What is gas?The ideal gas...: The ideal gas...P-V-T relation for ideal gases: P-V-T relation for ideal gasesThe ideal gas equation of state: The ideal gas equation of state This implies: (1) very little molecular interaction (p = 0), (2) molecules are point masses, i.e., zero volume.The universal gas constant: The universal gas constantThe ideal gas state surface: The ideal gas state surfaceThe perfect gas: The perfect gas3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior: 3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior Compressibility Factor, Z Z = Pv/RT Z = vactual/videal Ideal gas: Z = 1 Real gases: Z > 1 Z = 1 Z < 13.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior: 3.7 Compressibility Factor- A Measure of Derivation from Ideal-Gas Behavior The normalization: -Reduced pressure, PR PR = P/ Pcr -Reduced temperature, TR TR = T/ Tcr The principle of corresponding states: The Z factor for all gases is approximately the same at the same reduced pressure and temperature.Real gases...: Real gases...Real Gases: Real Gases PReduced pressure and temperature: Reduced pressure and temperature Generalized Compressibility Chart (14.6)The virial form for compressibility: The virial form for compressibilitySlide71: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. FIGURE 3-49 Percentage of error involved in assuming steam to be an ideal gas, and the region where steam can be treated as an ideal gas with less than 1 percent error. 2-12Slide72: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-13 FIGURE 3-51 Comparison of Z factors for various gases.Slide73: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 2-14 FIGURE 3-60 Percentage of error involved in various equations of state for nitrogen.Slide74: Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. FIGURE Ideal-gas constant-pressure specific heats for some gases (see Table A–2c for Cp equations). 2-153.8 Other Equations of State: 3.8 Other Equations of State Van der Waals Equation of state: Beattie-Bridgeman Equation of state: Benedict-Webb-Rubin Equation of state: Virial Equation of state:Key concepts and terms: Key concepts and terms Fluid Gas Ideal gas Perfect gas Compressibility factor Compressibility chart Local equilibrium Reduced pressure Reduced temperature Thermodynamic pressure Virial equation of state