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9/18/2009 1 Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements in energy systems 2. Able to distinguish between work or energy and 1 power 3. Able to explain why work and heat are path functions as opposed to pt functions 4. Able to calculate work know a functional or graphical relationship of P vs. V or F vs. x Class MMap

Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

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Page 1: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

1

Lect 6 – Thermo I – Work and Heat Introduction

1. Able to identify forces and displacements in energy systems

2. Able to distinguish between work or energy and

1

power3. Able to explain why work and heat are path

functions as opposed to pt functions 4. Able to calculate work know a functional or

graphical relationship of P vs. V or F vs. x

Class MMap

Page 2: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

2

Thermo Engineer in a Nutshell

“The biggest bang for the buck.”

“Most work or heat for the least cost.”

“Cost is complicated.”

Drip, drip, drip – The efficiency story

4

Page 3: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

3

Work andHeat Overview

04 07

Page 4: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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04 04

Is this fan assembly doing work?

04_01

Page 5: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

5

Is this NEW system doing work?

New

04_02

Page 6: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Work….graphically shown

Three Quasi-Equilibrium Paths…is the work equivalent?

Page 7: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

7

Spring Work –Garage Door

Spring Work –Garage Door

Page 8: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

8

Lect 7 – Thermo I – Work and Heat Introduction

1. Able to calculate work for polytropic process2. Able to distinguish between an quasi equilibrium

process and a nonequilibrium process ( equilibrium process doesn't make sense to me )

15

process doesn t make sense to me )3. Able to identify and explain the three different

modes of heat transfer4. Able to calculate heat transfer by conduction using

Fourier's law

Compression or Expansion work

(+)

(-)

04 05

Page 9: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Example Problem

Example Problem

PROBLEM STATEMENT:A piston cylinder device contains 50 kg of water at 150A piston-cylinder device contains 50 kg of water at 150 kPa and 25oC. The cross-sectional area of the piston is 0.1 m2. Heat is now transferred to the water, causing part of it to evaporate and expand. When the volume reaches 0.2 m3, the piston reaches a linear spring whose spring constant is 100 kN/m. More heat is transferred to the water until the piston rises 20 cm morewater until the piston rises 20 cm more

Page 10: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Work Done - Graphical

Class MMap

Page 11: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Polytropic Processes - EXPANSION

n = 0 2

n =± ∞ n = 1

n = 1 3

1

n 1.3

http://www.ac.wwu.edu/~vawter/PhysicsNet/Topics/Thermal/ImportantThermalProcess.html#Isobaric

Page 12: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Polytropic Processes at Work – Adiabatic Compression

Fire Piston

Page 13: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Work MMap

Torsion Work

04 03

Page 14: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

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Film Work

04_16

Tension Work

04_34

Page 15: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

9/18/2009

15

P 1 P 2P 2

Two chambers separated by a membrane

_ __

Work Done?

1. If entire interior is system – no boundary work2. If green = system – no resistance at system boundary

04 08

Quasi-Equilibrium process ?

2. If green system no resistance at system boundary

http://jersey.uoregon.edu/vlab/Thermodynamics/therm1d.html

1. “Because nonequilibrium effects are inevitably present during actual processes, systems of

Expert Comments

p g p , yengineering can at best approach, but never realize a quasi equilibrium process.” Moran et al. Fundamentals of Engineering Thermodynamics – 6th

ed.

2. “This assumption [quasi-equilibrium] is valid in the vast majority of cases encountered inthe vast majority of cases encountered in engineering applications.” Schmidt et al. Thermodynamics an Integrated Learning System”.

Page 16: Lect 6 – Thermo I – Work and Heat Introductionusers.rowan.edu/~merrill/Lect6_7s.pdf · Lect 6 – Thermo I – Work and Heat Introduction 1. Able to identify forces and displacements

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Modes of Heat Transfer

Modes of Heat Transfer ?