Advaned Cooling System for Heavy Vehicles

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  • 7/29/2019 Advaned Cooling System for Heavy Vehicles

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    Advanced cooling system for

    heavy vehicles heat exchangers/coolers

    Wamei Lin

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    Outline

    Introduction of my project

    Energy distribution in vehicle

    Methods for saving energy

    New material for heat exchangersConclusion of graphite foam heat

    exchanger

    Future work

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    Introduction of my project The aim of my PhD project is to develop a new cooling

    system for heavy vehicles, so that the fuel consumptionand CO2 emission would be reduced.

    This project includes two parts:

    Flow field: Chalmers University of Technology (LennartLfdahl, Lisa Larsson)

    Heat transfer: Lund university (Bengt sundn, Wamei

    Lin)

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    Energy distribution in vehicle In order to save fuel

    consumption in vehicles,

    what can be done?

    (1)Can we reuse some energyfrom the engine coolant?

    (2)Can we recover someenergy from the exhaust gas?

    (3)Can we recover somemechanical energy?

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    Engine cooling Radiator: to make sure the

    engine works at its optimaltemperature (80-90C).

    Intercooler: to cool downthe fresh air, whosetemperature is increasedafter through a

    turbocharger.

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    Methods for saving energyEngine cooling: thermal management

    14.5 kW power wassaved in a standarddiesel vehicle (Cho

    2007)

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    Methods for saving energyExhaust gas (vary between 250 and 680)

    (1) Heatingcompartment

    (2) Absorption cooling:

    7.1 billion gallons ofgasoline was saved inU.S. vehicles (2002J ohnson)

    (3) Thermoelectric

    device:

    Peltier-Seebeck effect.

    3-8% of fuelconsumption can be

    saved (2007 Smith)

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    Methods for saving energy

    During the braking process, we canstore the mechanical energy and use itto drive vehicle later.

    (1)Transfer the mechanical energy intoelectricity

    (2)During the braking process, thekinetic energy is used to generate ahigh pressure gas, which is used todrive vehicles later.

    80% of kinetic energy lost in thebraking process can be recovered

    The mechanical work

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    With the increasing power of vehicles and the increase of electric orhybrid electric vehicles, less heat will be dissipated in the exhaust gas,more heat has to be brought away by the cooling system.

    Heatingcompartment

    Absorptioncooling

    Thermoelectricdevice (3-10%fuel reduced)

    Thermalmanagement

    Methods for saving energy

    The regenerativebraking system (10-25% fuel reduced)

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    New material for heat exchangers

    The thermal management development

    Aluminum and copper

    heat exchanger(180 W/(m.K) for aluminum

    6061 and 400 W/(m.K) forcopper)

    The utilization ofmicrocellular foam materialssuch as metal or graphitefoams

    (the enhancement of heat transferby huge fluid-solid contact surfacearea and the fluid mixing)

    Coolingpowerincreasing

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    Graphite foam

    New material for heat exchangers

    An

    appropriatematerial forthe thermal

    management

    High thermal

    conductivity:(Ksolid=1700W/(m.K).

    Keff=150W/(m.K) >Keff.Al=2-26W/(m.K))

    Low density:0.2-0.6g/cm3,20% of that of

    AluminumLarge specific

    surface area:5000-50000m2/m3

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    New material for heat exchangers

    Problems

    The high pressure drop

    The effective area of heat transfer is reduced; A large input of pumping power, a low coefficiency of performance.

    Weak mechanical properties

    The tensile strength of graphite foam with porosity of 75 % is only0.69 MPa. However, the tensile strength of nickel foam with thesame porosity is 18.44 Mpa.

    The dust blocking

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    New material for heat exchangers In order to reduce the pressure drop of graphite foams, four different

    configurations of foams (pin-finned, blind-holes, corrugated andbaffle) are analyzed.

    Graphite

    foam

    Porosity () Pore

    diameter

    (Dp) (um)

    Specific

    surface

    area

    ()(m2/m3)

    Effective

    thermal

    conductivity

    (keff)(W/m.K)

    Permeability

    () (m2)

    Forchheimer

    coefficient

    (CF)

    POCO 0.82 500 5240 120 6.13x10-10

    0.4457

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    Verification of the simulation model

    The pressure drop values ofthe present simulation modelare justified to be comparableto experiment.

    The Nusselt numbers of thepresent simulation model areslightly higher than theexperimental results.

    0

    5

    10

    15

    0 0.02 0.04 0.06 0.08 0.1

    Frontal velocity (m/s)

    Pressuredrop(kPa)

    Experiment [6]

    Simulation0

    20

    40

    60

    80

    100120

    140

    160

    0 0.02 0.04 0.06 0.08 0.1

    Frontal velocity (m/s)

    NusseltnumberN

    u

    Experiment [6]

    Simulation

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    Pressure drop of graphite foam The pressure loss through

    the graphite foam is basedon the Forchheimer

    extended Darcy equation

    f f F

    i i i

    CdPu u u

    dx

    The corrugated and pin-finned foams have lowerpressure drop, due to theshort flow length

    (corrugated) and smoothflow path (pin-finned).

    The configuration hasimportant effect on thepressure drop of foams.

    15times

    Frontal air velocity (m/s)

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

    Pressuredrop(P

    a)

    corrugated

    blind-holes

    baffle

    pin-finned

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    Thermal performance of graphite foam

    Nusselt number (Nu) is calculatedby

    Np h removed

    f f b base inlet

    h D D Qu

    k k A T

    Due to the low flow resistancethrough the corrugated and the

    pin-finned foams, more cold air canreach the surface inside the foamand bring away the heat from thefoam.Thus, the effective heat transfersurface is larger in the corrugatedand the pin-finned foams

    removedQ . .effhA T

    The corrugated and pin-finnedfoams have higher Nu

    Frontal air velocity (m/s)

    0

    20

    40

    60

    80

    100

    120

    140

    160

    0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

    Nus

    seltnumberNu

    corrugated

    blind-holes

    baffle

    pin-finned

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    Comparison between graphite foam and

    aluminium louver fin

    Lp(mm)

    (degree)

    Fp(mm)

    Tp(mm)

    Lw(mm)

    FL(mm)

    1 29 2.5 14 12 50

    removed removed

    pum in in

    Q QCOP

    P u A P

    1000

    removed

    HEX

    QPD

    m

    1000

    removed

    HEX

    QCF

    V

    (1) coefficient of performance (COP,how much heat can be removed bya certain input pump power)

    (2) power density (PD, how muchheat can be removed by a certainmass of fins)

    (3) compactness factor (CF, howmuch heat can be removed in acertain volume)

    Aim of comparison

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    Comparison of COP (coefficient of

    performance)

    The louver finheat exchanger

    has a largerCOP valuethan thecorrugated andpin-finned foamheat

    exchangers atlow velocity.

    Frontal velocity (m/s)

    10

    60

    110160

    210

    260

    310

    360410

    460

    510

    5 6 7 8 9 10 11 12 13 14 15

    COP

    pin-finned

    louver fin

    corrugated

    At highvelocity,the COP

    values aresimilar

    Thus, by applying an appropriate configuration for graphitefoam, it is possible to reduce the input pumping power, andhave similar COP value as aluminium louver fin.

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    Comparison of PD (power density)

    Frontal velocity (m/s)

    20

    30

    40

    50

    60

    70

    80

    90

    100

    5 6 7 8 9 10 11 12 13 14 15

    PD(kW/kg

    pin-finned

    louver fin

    corrugated The corrugatedand pin-finnedfoams havehigher PD valuesthan the louver

    fin

    This means that the corrugated or pin-finned graphitefoamheat exchanger is lighter than the louver fin heatexchanger, when the removed heat is the same.(Because of the low density)

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    Comparison of CF (compactness factor )

    When the removed heat is the same, the volume of thecorrugated or pin-finned foam is much smaller than that of thelouver fin.

    Because of the open cells in the foam, the heat transfer surface is

    larger in the corrugated or pin-finned foam than in the louver fin.

    The CF value of

    the corrugated orpin-finned foam ishigher than that ofthe louver fin.

    Frontal velocity (m/s)

    2000

    4000

    6000

    8000

    10000

    1200014000

    16000

    18000

    5 6 7 8 9 10 11 12 13 14 15

    CF(kW/m3

    pin-finned

    louver fin

    corrugated

    Highcompactness in graphite

    foam

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    Conclusion of graphite foam heat

    exchanger Low pressure drop and high thermal performance have

    been provided by the corrugated and pin-finned graphitefoams.

    The corrugated and pin-finned graphite foams have

    higher PD and CF values than the aluminium louver fin.This implies a light or compact cooling system in vehicles.

    By using an appropriate configuration of the graphitefoam, it is possible to have the similar COP value as thealuminum louver fin.

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    Future work New structure for heat exchangers

    Due to space limitation, it might be good to change the position of heatexchanger. But when the position of the heat exchanger is changed,maybe a new structure of the heat exchanger is appropriate for the newposition.

    1) Maybe a countercurrent exchanger is good for the radiator which is on thetop of driver compartment.

    2) Designing a new configuration of heat exchanger, first the aluminum heatexchanger will be considered and analyzed. Later the graphite foam heatexchanger will be considered.

    radiator 2

    compartment

    radiator 3

    Radiator 1:

    countercurrent

    exchanger

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    Ideas about countercurrent HEX

    a.Louverfin(crossflow) b.Louverfin(countercurrentflow)

    d.Wavefin(countercurrentflow)c.Pinfin(countercurrentflow)

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    Thank youDiscussion and Questions