Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯.

Slides:



Advertisements
Similar presentations
Second Law Analysis of Open Systems Isentropic Device Efficiency
Advertisements

Chapter Seven Compressible Fluid.
Chapter 17 Compressible Flow Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and.
Entropy balance for Open Systems
The First Law of Thermodynamics
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
First Law of Thermodynamics - Open Systems
Chapter 4 Mass and Energy Analysis of Control Volumes (Open Systems)
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Lecture# 9 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
CHAPTER 5: Mass and Energy Analysis of Control Volumes
Lec 13: Machines (except heat exchangers)
Jet Engine Design Idealized air-standard Brayton cycle
16 CHAPTER Thermodynamics of High-Speed Gas Flow.
Chapter 7 Entropy (Continue).
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Jet Engine Design diffuser compressor combustion chamber turbine nozzle P=constant q out q in T s 1-2 Isentropic compression in.
Lesson 4 THERMODYNAMIC SYSTEMS AND PROCESSES DESCRIBE the following types of thermodynamic systems: – Isolated system – Closed system – Open system DEFINE.
Refrigeration Cycles Chapter 11.
Advanced Thermodynamics Note 4 The Second Law of Thermodynamics
Advanced Thermodynamics Note 5 Thermodynamic Properties of Fluids
Mass and Energy Analysis of Control Volumes. 2 Conservation of Energy for Control volumes The conservation of mass and the conservation of energy principles.
Chapter 7 Continued Entropy: A Measure of Disorder Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition.
Chapter 5 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition.
Eng. Samra Essalaimeh Philadelphia University 2nd Semester
EGR 334 Thermodynamics Chapter 6: Sections 11-13
PTT 201/4 THERMODYNAMIC SEM 1 (2013/2014) CHAPTER 7: Entropy.
5. MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Calculating Entropy Change
The First Law of Thermodynamics
Chapter 6 Using Entropy.
Lecture slides by Mehmet Kanoglu
Lesson 8 SECOND LAW OF THERMODYNAMICS
CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Entropy Rate Balance for Closed Systems
Entropy of a Pure Substance Entropy is a thermodynamic property, the value of entropy depends on the state of the system. For example: given T & P, entropy,
CHAPTER 5: Mass and Energy Analysis of Control Volumes
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Thermodynamics I Inter - Bayamon Lecture 5 Thermodynamics I MECN 4201 Professor: Dr. Omar E. Meza Castillo
Last Time Where did all these equations come from?
Chapter 4 Control Volume Analysis Using Energy. Learning Outcomes ►Distinguish between steady-state and transient analysis, ►Distinguishing between mass.
Entropy Rate Balance for Closed Systems
Chapter 7 ENTROPY Dr. Kagan ERYURUK
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
The Second Law of Thermodynamics Entropy and Work Chapter 7c.
Reversibility Thermodynamics Professor Lee Carkner Lecture 14.
Flow of Compressible Fluids. Definition A compressible flow is a flow in which the fluid density ρ varies significantly within the flowfield. Therefore,
Dr. Owen Clarkin School of Mechanical & Manufacturing Engineering Summary of Energy Topics Chapter 1: Thermodynamics / Energy Introduction Chapter 2: Systems.
Chapter 7. Application of Thermodynamics to Flow Processes
Mid-Term Review. Classical Thermodynamics The science of the conversion of energy from one form to another. The science of energy and entropy.
Chapter 6 FIRST-LAW ANALYSIS FOR A CONTROL VOLUME.
Chapter 5 Part 2 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition.
1 Chapter 5 Mass and Energy Analysis of Control Volumes.
First Law of Thermodynamics applied to Flow processes
Consequence Analysis 1.2.
Objectives Develop the conservation of mass principle.
Chapter: 06 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES.
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
7–12 ISENTROPIC EFFICIENCIES OF STEADY-FLOW DEVICES
Energy balance for the compressor in this figure:
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Chapter 5 The First Law of Thermodynamics for Opened Systems
Chapter 7 Entropy: A Measure of Disorder
Chapter 5 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 6th edition.
Thermodynamics: An Engineering Approach Yunus A. Cengel, Michael A
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Mass and Energy Analysis of Control Volumes (Open Systems)
4 CHAPTER The First Law of Thermodynamics: Control Volumes.
Chapter 6: Entropy First law: Energy conservation concept.
Presentation transcript:

Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯

The discipline Principles: “Fluid mechanics” and “Thermodynamics” Contrast Flow process inevitably result from pressure gradients within the fluid. Moreover, temperature, velocity, and even concentration gradients may exist within the flowing fluid. Uniform conditions that prevail at equilibrium in closed system. Local state An equation of state applied locally and instantaneously at any point in a fluid system, and that one may invoke a concept of local state, independent of the concept of equilibrium.

Duct flow of compressible fluids Equations interrelate the changes occurring in pressure, velocity, cross-sectional area, enthalpy, entropy, and specific volume of the flowing system. Consider an adiabatic, steady-state, one dimensional flow of a compressible fluid: The continuity equation:

From physics, c is the speed of sound in a fluid The Mach number Relates du to dS and dA

Pipe flow For subsonic flow, M2 < 1, , the pressure decreases and the velocity increases in the direction of flow. For subsonic flow, the maximum fluid velocity obtained in a pipe of constant cross section is the speed of sound, and this value is reached at the exit of the pipe.

Consider the steady-state, adiabatic, irreversible flow of an incompressible liquid in a horizontal pipe of constant cross-sectional area. Show that (a) the velocity is constant. (b) the temperature increases in the direction of flow. (c) the pressure decreases in the direction of flow. Control volume: a finite length of horizontal pipe, with entrance (1) and exit (2) incompressible The continuity equation: const. cross-sectional area Entropy balance (irreversible): incompressible liquid with heat capacity C Energy balance with (u1 = u2): If reversible adiabatic: T2 = T1; P2 = P1. The temperature and pressure change originates from flow irreversibility.

Nozzles: Reversible flow Reversible flow For subsonic flow in a converging nozzle, the velocity increases as the cross-sectional area diminishes. The maximum value is the speed of sound, reached at the throat.

isentropic

A high-velocity nozzle is designed to operate with steam at 700 kPa and 300°C. At the nozzle inlet the velocity is 30 m/s. Calculate values of the ratio A/A1 (where A1 is the cross-sectional area of the nozzle inlet) for the sections where the pressure is 600, 500, 400, 300, and 200 kPa. Assume the nozzle operates isentropically. Initial values from the steam table: The continuity equation: Energy balance: Since it is an isentropic process, S = S1. From the steam table: 600 kPa: Similar for other pressures

Consider again the nozzle of the previous example, assuming now that steam behaves as an ideal gas. Calculate (a) the critical pressure ratio and the velocity at the throat. (b) the discharge pressure if a Mach number of 2.0 is required at the nozzle exhaust. (a) The ratio of specific heats for steam, We have u1, P1, V1, P2/P1, γ (b)

Throttling Process: When a fluid flows through a restriction, such as an orifice, a partly closed valve, or a porous plug, without any appreciable change in kinetic or potential energy, the primary result of the process is a pressure drop in the fluid. Constant enthalpy For ideal gas: For most real gas at moderate conditions of temperature and pressure, a reduction in pressure at constant enthalpy results in a decrease in temperature. If a saturated liquid is throttled to a lower pressure, some of the liquid vaporizes or flashes, producing a mixture of saturated liquid and saturated vapor at the lower pressure. The large temperature drop results from evaporation of liquid. Throttling processes find frequent application in refrigeration.

Propane gas at 20 bar and 400 K is throttled in a steady-state flow process to 1 bar. Estimate the final temperature of the propane and its entropy change. Properties of propane can be found from suitable generalized correlations. Constant enthalpy process: Final state at 1 bar: assumed to be ideal gas and And based on 2nd virial coefficients correlation ???

Throttling a real gas from conditions of moderate temperature and pressure usually results in a temperature decrease. Under what conditions would an increase in temperature be expected. Define the Joule/Thomson coefficient: When will μ < 0 ??? Sign of ??? Always negative Same sign Always positive The condition may obtain locally for real gases. Such points define the Joule/Thomson inversion curve.

Fig 7.2

Turbine (Expanders) A turbine (or expander): Consists of alternate sets of nozzles and rotating blades Vapor or gas flows in a steady-state expansion process and overall effect is the efficient conversion of the internal energy of a high-pressure stream into shaft work. Turbine

The turbine efficiency The maximum shaft work: a reversible process (i.e., isentropic, S1 = S2) The turbine efficiency Values for properly designed turbines: 0.7~ 0.8

A steam turbine with rated capacity of 56400 kW operates with steam at inlet conditions of 8600 kPa and 500°C, and discharge into a condenser at a pressure of 10 kPa. Assuming a turbine efficiency of 0.75, determine the state of the steam at discharge and the mass rate of flow of the steam. Turbine

A stream of ethylene gas at 300°C and 45 bar is expanded adiabatically in a turbine to 2 bar. Calculate the isentropic work produced. Find the properties of ethylene by: (a) equations for an ideal gas (b)appropriate generalized correlations. (a) Ideal gas iteration

(b) General correlation based on 2nd virial coefficients correlation Assuming T2 = 370.8 K based on 2nd virial coefficients correlation iteration

Compression process compressor Pressure increases: compressors, pumps, fans, blowers, and vacuum pumps. Interested in the energy requirement The minimum shaft work: a reversible process (i.e., isentropic, S1 = S2) The compressor efficiency Values for properly designed compressors: 0.7~ 0.8

Saturated-vapor steam at 100 kPa (tsat = 99 Saturated-vapor steam at 100 kPa (tsat = 99.63 °C ) is compressed adiabatically to 300 kPa. If the compressor efficiency is 0.75, what is the work required and what are the properties of the discharge stream? For saturated steam at 100 kPa: Isentropic compression 300 kPa 300 kPa

If methane (assumed to be an ideal gas) is compressed adiabatically from 20°C and 140 kPa to 560 kPa, estimate the work requirement and the discharge temperature of the methane. The compressor efficiency is 0.75. iteration

Pumps Liquids are usually moved by pumps. The same equations apply to adiabatic pumps as to adiabatic compressors. For an isentropic process: With For liquid,

Water at 45°C and 10 kPa enters an adiabatic pump and is discharged at a pressure of 8600 kPa. Assume the pump efficiency to be 0.75. Calculate the work of the pump, the temperature change of the water, and the entropy change of water. The saturated liquid water at 45°C: