Draft Objectives – ES201 Page 1 of 3 Conservation of Energy (Supplement) 1. Define, illustrate, and compare and contrast the following terms and concepts: Thermodynamic cycles Definition ( three parts) Classifications Working fluid: single vs two-phase Structure: Closed, periodic vs Closed-loop, steady-state Purpose: Power vs Refrigeration vs Heat Pump cycles Measures of Performance General definition Power cycles Æ Thermal efficiency – η Refrigeration cycle Æ Coefficient of Performance – COPref Heat pump cycles Æ Coefficient of Performance – COPhp 2. Given a device that operates in a closed-periodic or closed-loop, steady-state cycle, • determine whether the device operates as a power cycle (heat engine) or a refrigerator or a heat pump, and • calculate the appropriate measure of performance for the specific device, i.e. a thermal efficiency for a power cycle and a coefficient of performance (COP) for a refrigerator or heat pump. File-Size, Template, Date Printed: Exam_Final_Objective(Entropy).doc - 288768; DER_12.dot; 1-Jun-01 Draft Objectives – ES201 Page 2 of 3 Entropy Production and Accounting 1. Define, illustrate, and explain the following terms and concepts: Second Law of Thermodynamics Reversible processes internally reversible vs internally irreversible Entropy units: kJ/K ; Btu/oR specific entropy: s units: kJ/(K·kg); Btu/(oR·lbm) Thermodynamic temperature Application of Accounting Principle for Entropy rate of accumulation of entropy within the system amount of entropy within the system: S sys = ∫ s ρ dV V transport rate of entropy across system boundaries Q j ∑T transport rate of entropy by heat transfer: b, j transport rate of entropy by mass flow: ∑ m s − ∑ m s i i in e e out production/consumption of entropy EMPIRICAL EVIDENCE ---- Entropy can only be produced and in the limit of an internally reversible process entropy is conserved. Rate of entropy production: S gen > 0 Internally irreversible = 0 Internally reversible Accounting Equation for Entropy rate form: dSsys dt = Q j ∑T b, j + ∑ m s − ∑ m s i i in e e + S gen out Carnot Efficiency for a Power Cycle Isentropic Processs 2. Apply the accounting equation for entropy in conjunction with the conservation of energy equation to calculate the entropy generation rate or entropy generation for a steady-state device or cycle. 3. Given sufficient information, determine the specific entropy change ∆s for a substance when one of the following models apply: File-Size, Template, Date Printed: Exam_Final_Objective(Entropy).doc - 288768; DER_12.dot; 1-Jun-01 Draft Objectives – ES201 Page 3 of 3 Ideal gas with room-temperature specific heats Incompressible substance with room-temperature specific heats 4. Apply the entropy accounting equation in conjunction with the conservation of energy equation to calculate the entropy generation or the entropy generation rate for a system when all other necessary information is known 5. Apply the accounting equation for entropy in conjunction with the conservation of energy equation to determine the theoretical “best” performance, i.e. theoretical maximum thermal efficiency or coefficient of performance for a cycle. 6. Determine if a specific device or system is operating in a reversible fashion, an irreversible fashion, or is not physically possible. 7. Evalute the performance of a device or system when it is operating in an internally reversible fashion. File-Size, Template, Date Printed: Exam_Final_Objective(Entropy).doc - 288768; DER_12.dot; 1-Jun-01