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    Department of Engineering Physics, Faculty of Engineering, Gadjah Mada University

    (Study Programs of Engineering Physics & Nuclear Engineering)

    Jl. Grafika 2, Yogyakarta 55281,(+62 274) 580882, http://www.tf.ugm.ac.id/

    The First Law of

    Thermodynamics

    THD

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    DepartmentofEngineeringPhysic

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    rogramsofEngineeringPh

    ysics&NuclearEngineerin

    g

    First Law of Thermodynamics

    Energy can neither be created nor destroyed It can change forms

    2

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    Energy Balances

    3

    energysystem

    totalin theChange

    SystemtheLeaving

    EnergyTotal

    SystemtheEntering

    EnergyTotal

    EEE outin

    How can energy get into or out of a system?

    Heat, Work and Energy Transfer with Mass

    12 EE

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    DepartmentofEngineeringPhysic

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    g

    Lets Look at Closed Systems First

    There is no mass transfer into a closed system The only way energy can get into or out of a

    closed system is by heat transfer or work

    4

    EWQ outnet,innet,

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    What is E equal to?

    Since

    5

    pk EEUE

    pk EEUE

    Usually we dont need to worry about kineticenergy or potential energy

    pkoutin EEUWQ

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    DepartmentofEngineeringPhysic

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    rogramsofEngineeringPh

    ysics&NuclearEngineerin

    g

    How to solve problems

    Draw a picture

    List the data you know

    Identify the goal (What do you want to solve for)

    List the equations you know

    Draw a Process Diagram

    Solve for the unknowns

    6

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    rogramsofEngineeringPh

    ysics&NuclearEngineerin

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    Do some homework problems

    We have covered all the material you need to doany of the problems in the book, up through 4-55.

    Do the homework problems for Wednesday.

    Do as many additional problems as you need to

    do to feel comfortable

    7

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    Now we can move on to Control Volumes

    How are control volumes different from closedsystems?

    What effect does this have on the energybalance?

    8

    Energy can flow in with the matter

    We are interested in rates

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    Total Energy of a flowing fluid

    9

    gzc

    ueeue pk

    2

    2

    The fluid possesses an additional form of

    energythe flow energy (flow work)

    pk eeupvepv

    Methalpy

    Rememberthis fromlastchapter?

    pk eeh

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    We can rewrite the energy balance

    10

    cvee

    eeii

    ii Egzc

    hmWgzc

    hmQ

    22

    22

    This work represents everything but

    the flow work

    The flow work

    is included in

    the enthapyterm

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    mentofEngineeringPhysic

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    This is getting pretty complicated !

    Lets look at a special case

    The Steady flow process

    o A process during which a fluid flows through a controlvolume steadily

    o Steady means no change with time

    11

    0

    0

    cv

    cv

    E

    m

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    g

    outin mm

    022

    22

    e

    e

    eeneti

    i

    iinet gz

    c

    hmgz

    c

    hm WQ

    ii

    iiee

    ee

    gzc

    hmgzc

    hm

    netnetWQ

    22

    22

    Steady Equation

    12

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    Some common steady flow devices

    13Only one in and one out

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    Nozzles

    Diffusers

    Turbines

    Compressors

    Throttling Valve

    14

    ieie

    ie zzgcc

    hhmWQ

    2

    22

    Often the change in kinetic energy

    of the fluid is small, and the

    change in potential energy of the

    fluid is small

    Single Stream Steady Flow System

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    Nozzles and Diffusers

    15

    A nozzle is a device that

    increases the velocity of a

    fluid at the expense of

    pressure

    A diffuser is a device that

    slows a fluid down

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    16

    ieie

    ie zzgcc

    hhmWQ

    2

    22

    Is there work in this system? NO

    Is there heat transfer? Usuallyit can be ignored

    Does the fluid change

    elevation?NO

    What happened to the m?

    It divided out

    Nozzles and Diffusers

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    20

    22

    ieie cchh

    How can you find the mass flow rate in a nozzle?

    e

    ee

    i

    ii

    v

    Ac

    v

    Acm

    In a nozzle, enthalpy is converted into

    kinetic energy

    17

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    Turbines and Compressors

    18

    A turbine is a device that

    produces work at the

    expense of temperature

    and pressure

    A compressor is a device

    that increases the pressure

    of a fluid by adding workto the system

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    DepartmentofEngineeringPhysics,

    FacultyofEngineering

    StudyProgramsofEngineeringPhysics&NuclearEngineering

    ieie

    ie zzgcc

    hhmWQ

    2

    22

    19

    Is there work in this system? Yes!

    Is there heat transfer? Usuallyit can be ignored

    Does the fluid change elevation? NO

    Does the kinetic energy change? Usuallyit can be ignored

    Turbines and Compressors

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    DepartmentofEngineeringPhysics,

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    Turbines and Compressors

    20

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    Throttling Valve

    21

    A throttling valve reduces

    the fluid pressure

    For example, the water

    that comes into your house

    goes through a throttling

    valve, so it doesnt have

    excessive pressure in your

    home.

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    DepartmentofEngineeringPhysics,

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    ProgramsofEngineeringPhysics&NuclearEngineering

    ieie

    ie zzgcc

    hhmWQ

    2

    22

    22

    Is there work in this system? NO

    Is there heat transfer? Usuallyit can be ignored

    Does the fluid change elevation? NO

    What happened to the m? It divided out

    Does the fluid change velocity? Usuallyit can be ignored

    Throttling Valve

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    Throttling Valves

    hin

    = hout

    pin > pout

    For gases that are not ideal, the temperaturegoes down in a throttling valve

    23

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    Throttling Valves

    What happens if the gas is ideal?

    For ideal gases

    o h = CpT

    o But h = 0

    o So T = 0o The inlet and outlet temperatures are the same!!!

    24

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    Throttling Valve

    25

    For an ideal gas, the temperature does not

    change in a throttling valve!!!

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    Mixing Chamber

    26

    Mixing two or more fluids

    is a common engineering

    process

    Mixing

    Chamber

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    Mixing Chamber

    27

    ii

    iiee

    eegz

    chmgz

    chm

    netnet WQ 22

    22

    We no longer have only one inlet and one exit stream

    Is there any work done? No

    Is there any heat transferred?

    NoIs there a velocity change? No

    Is there an elevation change? No

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    Mixing Chamber

    Material Balance

    28

    ie

    mm

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    Mixing Chamber

    29

    332211 hmhmhm

    321 mmm

    Energy

    Balance

    Material

    Balance

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    Heat Exchanger

    30

    A heat exchanger is a

    device where twomoving fluids

    exchange heat

    without mixing.

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    Heat Exchangers

    31

    Your analysis approach will depend on how you

    define your system

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    Heat Exchangers

    Energy balance is the same as a mixing chamber,

    buto Two inlets

    o Two outlets

    Material Balanceo Divide into two separate streams with equal inlet and

    outlet flow rates

    32

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    Pipe Flow

    33

    A steady flow model

    is usually a good

    approximation

    Q W

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    Pipe Flow

    34

    .

    Theres work going into

    the pump

    Theres an elevation

    change

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    ieie

    ie zzgcc

    hhmWQ

    2

    22

    Pipe Flow

    35

    Is there work in this system? Sometimes

    Is there heat transfer? Usually

    Does the fluid change elevation? Sometimes

    Does the kinetic energy change? Not usually

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    For example..

    36

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    We need to make some assumptions

    Uniform flow

    o The system can change with time, but the inletconditions are constant

    o Everything in the system is in the same state

    o

    Fluid exiting the system is at the same state as thesystem

    37

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    We need to look at our balances again

    38

    mmmmm systemexitin 12

    cvee

    eeii

    ii EgzchmWgzchmQ

    22

    22

    We arent using the rate form of the

    balances here. Why?

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    cvee

    eeii

    ii EgzchmWgzchmQ

    2222

    pk EEUE

    pk EEUE

    This is the kinetic energy of

    the system

    This is the potential

    energy of the system

    Usually, they both equal 0

    39

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    cvee

    eeii

    ii EgzchmWgzchmQ

    2222

    Usually both the kinetic energy and potential energy of

    thefluidare zero too

    1122 umumhmhmWQ eeii

    Time 1 and time 2Inlet and Exit conditions,

    assuming only a single

    inlet and a single exit

    stream 40

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    Consider a bottle filling problem

    What happens to the temperature when you fill anempty tank with air?

    41

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    Consider a bottle filling problem

    What happens to the temperature when you fill anempty tank with air?

    o The air gets hot

    o Why?

    o It takes energy to push the air into the tank (flow work).That energy is converted into internal energy

    42

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    For our bottle filling problem

    43

    1122 umumhmhmWQ eeii

    2mmi

    2uhi

    hi is bigger than ui,so

    u2 is bigger than ui

    That means thetemperature in the tank

    is higher than the inlet

    temperature

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    What if

    How would we handle inlet or exit conditions thatchange with time?

    The best we can do at this point is to take theaverage

    If we knew more, we could integrate over time

    44

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    For example

    What happens to the temperature when you use

    a bottle of canned air? The bottle gets cold.

    Why?

    It takes energy to push the air out of the can (flowwork)o That energy comes from the energy of the air that

    remains in the can

    45

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    rtmentofEngineeringPhysics,

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    ing

    But.

    The air coming out of the can gets colder withtime

    That means the exit conditions are not constant

    1122 umumhmhmWQ eeii What conditions should you

    2

    12 hhhave