Example (A poorly maintained system)

Slides:



Advertisements
Similar presentations
Use of Regeneration in Vapor Power Cycles
Advertisements

Second Law Analysis of Open Systems Isentropic Device Efficiency
Entropy changes of pure substances: retrieving data from property tables. Tds relations relate properties of any pure substance exactly to entropy change.
EGR 334 Thermodynamics Chapter 6: Sections 9-10
EGR 334 Thermodynamics Chapter 4: Section 6-8
Entropy balance for Open Systems
The First Law of Thermodynamics
Lecture# 9 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
ENERGY CONVERSION ES 832a Eric Savory Lecture 12 – Large-scale plants Department of Mechanical and Material Engineering.
Example 1 - Superheat Rankine Cycle
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical
EXERCISE 1 CHAPTER 12.
Second Law of Thermodynamics
A Vapor Power Cycle Boiler T Turbine Compressor (pump) Heat exchanger
Vapor and Combined Power Cycles (2)
The First Law of Thermodynamics
A Vapor Power Cycle Boiler T Turbine Compressor (pump) Heat exchanger
1 So far… We’ve developed a general energy balance We’ve developed a general material balance We’ve only actually looked at systems that are under steady.
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,
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?

ChemE 260 Entropy Balances On Open and Closed Systems
Gas Turbines for Aircraft Propulsion. AIR CRAFT ENGINE The turbojet engine consists of three main sections: the diffuser, the gas generator, and the nozzle.
Refrigeration Cycles (YAC: 7-13 trough 7-16)
Lecture Objectives: Finish with absorption cooling Power generation Rankine cycles Connect power generation with heating and cooling –CHP –CCHP.
Chapter 10 Vapor and Combined Power Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus.
ME 200 L23: Clausius Inequality and Control Volume Example Problems Kim See’s Office ME Gatewood Wing Room 2172 Please check your HW Grades on Blackboard.
Thermodynamics and Energy The First Law The Second Law Dimensions and Units Dimensions Units – English and SI Example: In Europe, many tanks are rated.
Chapter 7 ENTROPY Dr. Kagan ERYURUK
Refrigeration Cycles A Carnot cycle in reverse QL QH T s 2
The Rankine Cycle: An Alternate Ideal Thermodynamic Model P M V Subbarao Professor Mechanical Engineering Department IIT Delhi A Feasible Mathematical.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Problems 3 Dr. Kagan ERYURUK.
The Second Law of Thermodynamics Entropy and Work Chapter 7c.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
1 A 英 Consider a regenerative cycle using steam as the workingfluid. Steam leaves the boiler and enters the turbine at 4 MPaand 400 ℃. After expansion.
Superheat Rankine Cycle Example Turbine pump condenser Q out Q in W out W in boiler Consider the superheat Rankine power cycle as we analyzed before.
Reversibility Thermodynamics Professor Lee Carkner Lecture 14.
Example: Electric heater is often used in houses to provide heating during winter months. It consists of a simple duct with coiled resistance wires as.
Example The internal energy of a closed system can be increased by adding heat or doing work. In the following example, 1 kg of saturated liquid water.
1 Chapter 5 Mass and Energy Analysis of Control Volumes.
Vapor ,Gas and Combined Power Cycles
7–12 ISENTROPIC EFFICIENCIES OF STEADY-FLOW DEVICES
Lecture Objectives: Answer question related to Project 1 assignment
Mass and Energy Analysis of Control Volumes
prepared by Laxmi institute tech. Mechanical eng. Department.
RANKINE CYCLE IMPROVISATIONS BY PRABHAKARAN.T AP/MECH
Power and Refrigeration Systems
Power Plant Technology Steam and Gas Cycle Power Plant (Assignment 1)
ES 211: Thermodynamics Tutorial 5 & 6
ES 211:Thermodynamics Tutorial 10
Chapter 5 The First Law of Thermodynamics for Opened Systems
Chapter 7 Entropy: A Measure of Disorder
Entropy of a Pure Substance
Chapter 6 THE MECHANICAL ENERGY BALANCE.
Maximum work or available energy from a system
QUIZ 2 The quality of steam at 7 MPa and enthalpy of 2600 kJ/kg: 0.526
Example: Unrestrained Expansion
Phase Transition Example
Chapter Four: Energy transfer by Heat, Work and Mass
Example 3 (A poorly maintained system)
Chapter Seven: Entropy
Example 1 The internal energy of a closed system can be increased by adding heat or doing work. In the following example, 1 kg of saturated liquid water.
(a) Find the PE at A PE = m g h = ( 500 kg )( 9.8 m/s2 )( 30 m )
Internal Combustion Engineering Division
Presentation transcript:

Example (A poorly maintained system) Following the same turbine example from previous lecture note. Let us consider that steam enters a turbine with the same pressure of 3 MPa, the same temp. of 400°C, and the same velocity of 150 m/s. The exit conditions remain the same as 100% saturated vapor exits at 100°C with velocity of 50 m/s. Due to poor maintenance, the turbine now develops less work than previously at 450 instead of 500 kJ per kg of steam. There is now more heat transfer between the turbine and its surroundings at an averaged surface temperature of 550 K. The higher temperature is reasonable since there should be more heat generation due to the imperfect operating condition. Determine the new rate at which entropy is produced within the turbine per kg of steam. dQ/dt at 550 K dW/dt 1 2 T s 1 2

Solution

Solution

Example Determine the work required to compressed steam isentropically from 100 kPa to 1 MPa if the steam is (a) saturated liquid and (b) saturated vapor at the inlet state. Negelct change in KE and PE. T s 100 kPa 1 MPa

Example(cont.)