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  • OPTIMAL FUNCTIONING PARAMETERS FOR A STIRLING ENGINE

    HEATER

    1 Universit de Valenciennes et du Hainaut-Cambrsis, ENSIAME, TEMPO (EA 4542) - DF2T Valenciennes France

    2 GEPEA (UMR 6144), cole des Mines de Nantes, DSEE, 4 rue Alfred Kastler - BP20722 , 44307 Nantes Cedex 03 France

    3 Universit de Monastir, Laboratoire LESTE, ENIM, Monastir - Tunisia

    * E-mail : [email protected]

    R. GHEITH 2,3, * F. ALOUI 1,2 and S. BEN NASRALLAH 3

    10th EUROPEAN CONFERENCE

    ON COAL RESEARCH AND ITS

    APPLICATIONS: 10th ECCRIA

  • VI. Conclusions

    II. Experimental device

    III. Some experimental results

    I. Introduction Objectives of the study

    OUTLINE

  • Robert Stirling

    Invention

    Stirling engine (1816)

    - A quiet engine (no vibrations because no internal combustion),

    - Ecological engine (closed gas circuit),

    - Any heating source can be used to heat the working fluid,

    - Its efficiency is more important than that of an internal

    combustion engine (between 30 and 40%)

    This Stirling engine is:

    1

  • The different Stirling engine configurations

    Alpha type Heating

    Cooling

    Regenerator

    Heating Cooling

    Beta type

    Regenerator

    Gamma type

    Heating

    Cooling

    Regenerator

    2

  • The Stirling Cycle

    1 2 : Isochoric heating 2 3 : Isothermal expansion

    3 4 : Isochoric cooling 4 1 : Isothermal compression

    Q340

    V1

    1

    d

    a b

    c

    3

  • Example of some applications using a Stirling engine 4

    Stirling engine - generator Stirling engine dish Space domain (salellites) Submarine domain

    Exchanger

    To heating system

    Electricity

    Electricity

    Stirling engine

    Mean burner Gas valves

    Natural

    gas

    From heating system

    Micro -cogenerator system Liquefaction of gases (receipt machines)

  • GLOBAL THERMODYNAMIC MODELS

    Isothermal model

    Adiabatic model

    Quasi-steady model

    - Real gas assumption

    - Thermal losses

    - Mechanical losses Adiabatic model +

    Compression

    Space

    Expansion Space

    Regenerator

    Cooler

    Heater

    l

    D k

    r h

    5

  • - Studying heat transfers in:

    - The regenerator (porous medium),

    - The expansion room (hot source),

    - The compression room (cold source).

    - Seeing the effect of porous medium on the

    efficiency, the heating and cooling temperatures.

    Optimization of the heat transfer inside the Stirling engine in

    order to increase its global efficiency, by:

    Objectives of the study:

    6

  • 7

    Hot source Tch Cold source Tfr Q1 < 0 Q2 > 0 Driven

    machine

    W < 0

    2

    2 2 2

    ' '. .

    ' 'glob mca th cal

    QW W W

    Q W Q Q

    The amount of heat

    supplied by the

    electrical heating

    (electrical resistance)

    The amount of

    heat actually

    received by the

    air

    The

    indicated

    work

    Mechanical work

    effectively

    recovered on the

    brake shaft

    2 'Q U I dt 2Q W'W

    cal th mca

    Operation of Stirling engine

  • Operation of Stirling engine

    First law of thermodynamics on a cycle 0QQWU 21

    Second law of thermodynamics on a cycle 0ST

    Q

    T

    QS c

    2

    2

    1

    1

    Efficiency 1Q

    W

    1

    Heating source S1

    at T1

    Cold source S2

    at T2

    Stirling

    Machine

    W < 0

    Q1 > 0 Q2 < 0

    8

  • Compression Space

    Expansion Space

    Crank-Rod System

    Regenerator

    Cooler

    Heater

    Heating system

    The Gamma type Stirling engine

    9

  • PDet.

    TE-input.

    TE-input

    PComp.

    Tcold

    Water input

    Water output

    Regenerator

    Heating system

    Expanxion Space

    Compression space

    TR2

    TR4 TR3

    TR1

    TR6

    TR8 TR7

    TR5

    Thot

    Porous media

    8 thermocouples 4 in each side

    TR1

    TR2

    TR3

    TR4

    TR5 TR6

    TR7

    TR8

    Cold working fluid

    Hot working fluid

    Hot working fluid

    Porous media (Rgnrateur)

    Cold working fluid

    Dissipation energy system

    Oscillant plate

    Transmission belt

    Alternateur

    Force transducer

    crank angle transducer

    10

  • p

    4

    jjpjpj

    jC

    TVT

    x

    T

    Cxt

    p

    C

    1

    x

    TV

    t

    T

    .

    .''

    ..

    air

    air

    11

  • Composed of: - 20 curved pipes (internal diameter: 1cm)

    - 20 tubes (length 0.50m each one)

    - 3 thermocouples located: inside the heater, outside the heat

    and in heating system.

    The heater exchange

    13

  • PExpansion

    TW-entrance

    TW-Exit

    PComp.

    TCold

    Water input

    Water exit

    Regeneratorr

    Heating

    system

    Expansion space

    Compression space

    TR2

    TR4 TR3

    TR1

    TR6

    TR8

    TR7

    TR5

    THot

    Matrix

    (regenerator)

    1st series of 4

    thermocouples 2nd series of 4

    thermocouples Regenerator

    Series of 8

    thermocouples

    Pourous media

    (regenerator)

    TR5

    TR6

    TR7

    TR8

    TR1

    TR2

    TR3

    Cold working fluid

    Hot working fluid

    TR4

    Cold working fluid

    Hot working fluid

    The heater exchange

    14

  • Two thermocouples are located at the input and the

    output of cooling water circuit

    Composed of 225 strips

    (or fins) in the inner

    cylinder

    For increasing the heat

    transfer exchange

    between the working

    fluid and water (cold

    source)

    II. Experimental

    The cooler exchanger (cold source)

    15

  • The regenerator (porous medium)

    16

    Porous media

    8 thermocouples (4 in each side)

    TR1

    TR2

    TR3

    TR4

    TR5

    TR6

    TR7

    TR8

    Cold working fluid

    Hot working fluid Hot working fluid

    Porous medium (Regenerator)

    Cold working fluid

  • Materials with porosity of 90%

    Proprieties \ Material Stainless Steel (304L) Copper Aluminium Monel 400

    Density (kg.m-3) 7,850 8,920 2,700 8,800

    Specific heat Cp (J.kg-1.K-1) 477 385 902 430

    Thermal conductivity (W.m-1.K-1) 26 390 237 21.7

    Melting point ( C) 1530 1084 660 1300

    The properties of used regenerator materials for a temperature of 300 C are:

    Copper

    Aluminum Monel

    Stainless Steel

    p

    4

    j

    jpjpj

    jC

    TVT

    x

    T

    Cxt

    p

    C

    1

    x

    TV

    t

    T

    .

    .''

    ..

    4 matrices, with differents constituting materials, were used as Stirling engine regenerator:

    - Stainless Steel matrix

    - Copper matrix

    - Aluminum matrix

    - Monel matrix

    Properties of the differents used matrices (regenerators)

    Copper

    Aluminum Monel

    Stainless Steel

    17

  • 4 matrices, with differents constituting materials, were used as Stirling engine regenerator:

    - Stainless Steel matrix

    - Copper matrix

    - Aluminum matrix

    - Monel matrix

    Properties of the differents used matrices (regenerators)

    Materials with porosity of 90%

    Proprieties \ Material Stainless Steel (304L) Copper Aluminium Monel 400

    Density (kg.m-3) 7,850 8,920 2,700 8,800

    Specific heat Cp (J.kg-1.K-1) 477 385 902 430

    Thermal conductivity (W.m-1.K-1) 26 390 237 21.7

    Thermal Diffusivity a (m/s) 6.94 . 10-6 1.14 10-4 9.73 10-5 5.73 10-6

    The properties of used regenerator materials for a temperature of 300 C are:

    Copper

    Aluminum Monel

    Stainless Steel

    4

    j

    jjj

    j

    T..a'V'T

    x

    T.a

    xt

    pa

    x

    TV

    t

    T

    18

  • 0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16136.08

    136.1

    136.12

    136.14

    136.16

    136.18

    136.2

    136.22

    0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16243.95

    244

    244.05

    244.1

    244.15

    244.2

    244.25

    244.3

    Acquisition time [s]

    TR1

    TR4

    TR1-4

    mean TR1

    mean TR4

    Working fluid temperature evolution vs. acquisition time for a copper matrix

    The temperature of

    the working fluid in

    the regenerator

    increases in the

    first half cycle until

    a maximum value

    (TR1 and TR4)

    The temperature

    decreases during the

    second half cycle

    until a temperature

    which is close to that

    of the cold source

    The Stirling engine regenerator has two roles:

    - Accumulating heat 1 and 4)

    - Forming a thermal barrier between both heat and cold sources 1-4)

    Temperature evolution in each kind of matrix regenerator)

    Pourous media

    (regenerator)

    TR5

    TR6

    TR7

    TR8

    TR1

    TR2

    TR3

    Cold working fluid

    Hot working fluid

    TR4

    Cold working fluid

    Hot working fluid

    19

  • The regenerator formed of the material Monel 400 is the best heat accumulator.

    The stainless steel represents the highest temperature gradient, and the Aluminum

    the smallest temperature gradient.

    Temperature evolution in each kind of matrix regenerator)

    Working fluid gradient temperature between the thermocouples TR1 and TR4

    Best Heat

    accumulator

    Highest

    temperature

    gradient

    Working fluid gradient temperatures given by the thermocouples TR1 during one cycle

    20

  • 100

    150

    200

    250

    300

    Bra

    ke

    po

    we

    r [W

    ]

    TH

    = 300C

    TH

    = 400C

    TH

    = 500C

    CopperStainlessSteel

    Aluminum Monel

    The Aluminum

    regenerator

    presents the

    worst brake

    power

    regardless the

    heating

    temperature

    The Stainless steel

    has the best brake

    power regardless

    the heating

    temperature

    The brake power increases with the heating temperature, but at different

    levels of each kind of regenerator.

    Influence of each type of matrix on the engine performance versus heating temperature

    Brake power = 281 W TH = 500C

    21

  • For all experimented regenerators, the brake power increases with the

    initial charge pressure but at different levels.

    100

    150

    200

    250

    300

    350

    Bra

    ke

    po

    we

    r [W

    ]

    Pi = 3 bar

    Pi = 5 bar

    Pi = 8 bar

    Stanless

    Steel

    Copper Aluminum Monel

    The Aluminum

    regenerator presents the

    worst brake power

    regardless the initial

    charge pressure

    The Stainless Steel

    regenerator has the

    best brake power

    Influence of each type of matrix on the engine performance versus charge pressure

    22

  • The regenerator thermal efficiency is calculated as the ratio of real heat

    transferred through the regenerator by the ideal heat, which must be transferred

    through the regenerator.

    The copper presents the best regenerator thermal efficiency and the

    Monel 400 presents the worst regenerator thermal efficiency.

    Regenerator thermal efficiencies

    0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.160.25

    0.3

    0.35

    0.4

    0.45

    0.5

    0.55

    0.6

    0.65

    Acquisition time fo one cycle [s]

    Effic

    ien

    cie

    s [%

    ]

    Eff

    Monel

    EffCuivre

    EffInox

    Eff-Alum

    Copper

    Monel

    Steel

    Allum

    23

  • Regenerator matrixes after about 15 hours of use

    Copper Stainless Steel

    Monel Aluminum

    The copper oxidizes quickly because of the working fluid (air) which contains about 21%

    of oxygen. This material oxidation changes the physical properties of the copper, and

    then leads to bad heat exchanges inside the regenerator.

    The stainless steel and the Aluminum, used as regenerators, have good

    thermal efficiencies (about 44%).

    These two materials do not present a problem of oxidation, but the use of

    regenerator in Aluminum is limited by its melting temperature.

    Regenerator thermal efficiencies

    24

  • Four regenerator matrices were tested on a Gamma Stirling engine :

    Stainless steel, Copper, Aluminum and Monel 400

    - The Monel matrix presents the best thermal sponge, and the Stainless Steel

    represents the best thermal barrier between hot and cold heat sources.

    - The copper regenerator has the best thermal efficiency, but its oxidation

    decreases extremely the brake power of the Stirling engine.

    - Using an Experimental Design Approach (OCC or DOE), the impotant

    parameters of the Stirling engine can be optimised to obtain a good

    efficiency of this machine.

    25