ES 202 Fluid and Thermal Systems Lecture 23: Power Cycles (2/4/2003)

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Presentation transcript:

ES 202 Fluid and Thermal Systems Lecture 23: Power Cycles (2/4/2003)

Lecture 23ES 202 Fluid & Thermal Systems2 Assignments Homework: Reading assignment –ES 201 notes (Section 7.9 and 8.4)

Lecture 23ES 202 Fluid & Thermal Systems3 Announcements Lab #3 this week in DL-205 (Energy Lab) –4 lab groups over 3 periods (6 students per group) –group formation (let me know by the end of today) –schedule sign-up –EES program for property lookup (download from course web) I am available for discussion during evenings this week (in preparation for Exam 2 next Monday) – me in advance to set up a meeting time

Lecture 23ES 202 Fluid & Thermal Systems4 Road Map of Lecture 23 Power cycle –use Rankine cycle as an example –the ideal Rankine cycle –representation on a T-s diagram –divergence of constant pressure lines –analysis of individual components (energy balance) –effects of irreversibility in turbine and compressor Comments on Quiz 4

Lecture 23ES 202 Fluid & Thermal Systems5 Power Cycles The integration of turbines, compressors, heat exchangers and combustors can generate power. For example, the gas turbine engine: –identify the different components The process path of any thermodynamic cycles form a closed loop on any phase/property diagram. The direction of process path determines what kind of cycle it is (extracting power versus refrigeration, etc.)

Lecture 23ES 202 Fluid & Thermal Systems6 Rankine Cycle Schematic of a typical Rankine cycle: For an ideal Rankine cycle: –from State 1 to State 2: isentropic compression (pump) –from State 2 to State 3: isobaric heating (boiler) –from State 3 to State 4: isentropic expansion (turbine) –from State 4 to State 1: isobaric cooling (condenser) pump/compressorturbine heat exchanger (heat addition) heat exchanger (heat removal)

Lecture 23ES 202 Fluid & Thermal Systems7 Questions of Interests Representation on a T-s diagram How do we get a net work output from the cycle? Effects of irreversibilities on cycle performance (graphical representation) Analysis of individual components –definition of thermal efficiency –back work ratio

Lecture 23ES 202 Fluid & Thermal Systems8 The T-s Diagram Advice on problem solving: start with a process diagram on a T-s plane: T s isentropic expansion through turbine 2 isentropic compression through pump isobaric heating through boiler isobaric cooling through condenser P 4 = P 1 P 2 = P 3

Lecture 23ES 202 Fluid & Thermal Systems9 Energy Conversion With reference to the T-s diagram on previous slide, a few observations are noteworthy: –the divergence of constant pressure lines at high temperatures implies that the mechanical power extracted from the turbine outweighs that required by the pump –in most situations, a fraction of the turbine work output is used to drive the pump and this fraction is called the back work ratio: –the Rankine cycle can be viewed as an energy conversion process from thermal energy to mechanical energy –the ratio between the net power output (turbine power – pump power) and the heat addition at the boiler is termed the thermal efficiency:

Lecture 23ES 202 Fluid & Thermal Systems10 Effects of Irreversibilities Irreversibilities in the pump and turbine for non-ideal processes result in higher entropy at the exit of pump (2a) and turbine (4a). –higher temperature at pump exit implies more pump work –higher temperature at turbine exit implies less turbine work T s 1 3 2s 4s 4a 2a

Lecture 23ES 202 Fluid & Thermal Systems11 Energy Analysis Adopt a “divide and conquer” approach to analyze the Rankine cycle. Apply energy balance to the four individual components in the cycle. Depending on the particular component, different terms in the energy balance are active while others are suppressed. Typical assumptions common to all four components are: –steady state operation –negligible changes in kinetic and potential energy –Caution: changes in kinetic energy are not negligible for nozzle and diffusers For these components, the energy balance can be reduced to a simple form: steady state (due to mass conservation)

Lecture 23ES 202 Fluid & Thermal Systems12 Summary of Energy Analysis