ALTITUDE EFFECTS ON HEAT TRANSFER PROCESSES IN

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ALTITUDE EFFECTS ON HEAT TRANSFER PROCESSESIN AIRCRAFT ELECTRONIC EQUIPMENT COOLINGbyDoron Bar-ShalomB.Sc., Ben-Gurion University, Israel (1979)Diploma , Tel-Aviv University , Israel (1985)SUBMITTED TO THE DEPARTMENT OFAERONAUTICS AND ASTRONAUTICS IN PARTIALFULFILLMENT OF THE REQUIREMENTS FOR THEDEGREE OFMASTER OF SCIENCE IN AERONAUTICS AND ASTRONAUTICSat theMASSACHUSETTS INSTITUTE OF TECHNOLOGYFebruary 1989Copyright 1989 Doron Bar-ShalomThe author hereby grants M.I.T. permission to reproduce and todistribute copies of this thesis document in whole or in part.Signature of AuthorDepartment of Aeronautics and AstronauticsJanuary 20, 1989Certified by'rotessorux-,.n HansmanThesis Supervisor,Department of Aeronautics and astronauticsAccepted byProfessor Harold Y. Wachman"" M " Ib(OlaientOF TE.H.N.,V1THDRAWNMIAR 10 1989UBRMIESA.-.M.I.T.I LIBRARIESGradiulate Committee

ALTITUDE EFFECTS ON HEAT TRANSFER PROCESSESIN AIRCRAFT ELECTRONIC EQUIPMENT COOLINGbyDoron Bar-ShalomSubmitted to the Department of Aeronautics and Astronautics onJanuary 20, 1989 in partial fulfillment of the requirements for the degree ofMaster of Science in Aeronautics and Astronautics.AbstractAltitude dependent changes of aircraft heat transfer processes in electronic equipmentboxes in equipment bays were investigated to examine the compatibility of currentspecifications for avionics thermal design with the thermal environment encountered inhigh performance aircraft.Steady state equipment and bay air temperature were analyzed as a function ofaltitude based on known sea level thermal conditions and design parameters, by usingstandard atmospheric models and aircraft altitude Mach number flight envelope. Thisanalysis was used to generate temperature-altitude envelopes which give the temperature ofthe equipment and the bay air as a function of altitude, based on typical altitude profiles ofthe bay wall temperature. Analysis of an unconditioned bay, containing ambient cooledequipment, was conducted. The optimal temperature difference between the equipment andthe bay wall was identified. Analysis of a conditioned bay, containing both ambient andforced-air cooled avionics, showed a tendency towards isothermal bay air temperaturealtitude profiles as the fraction of forced-air cooling was increased. The results showed thatthe temperature difference between the equipment and the bay wall grows exponentiallywith altitude in natural convective cooling and can be approximated as a function of theexternal pressure only. Radiation heat transfer was shown to serve as a "thermal pressurerelief valve" and to improve the thermal performance of the system at high altitude.The isothermal tendency of the bay air in a conditioned bay implies that ambientcooled equipment designed in accordance with MIL-E-5400 would not be compatible withthe bay environment and additional cooling would be required. The results of this thesisprovide guidance in determining the thermal design parameters which improve altitudeperformance of the avionics cooling system and in identifying the flight conditions resultingin critical thermal conditions.Thesis Supervisor:Title:Professor R. John HansmanAssociate Professor of Aeronautics and Astronautics

AcknowledgementsFirst, I would like to thank Professor RJ. Hansman, my advisor, for providing"guidance and control" over the past eighteen months, and for offering valuableadvice and criticism, as well as a warm working atmosphere despite the surroundingicing conditions. I would also like to thank Mr. Jerry Hall of McAir for the valuabledata he has provided, and for the time we spent discussing and sharing his extensiveexperience in the field of avionics cooling. I would also like to thank Mr. CharlesLeonard of Boeing for sharing his ideas and test data in the area of passive cooling,introducing an additional important point of view. To the friends in the AeronauticalSystems Lab, who have provided lots of friendship and fun: may your effort fly upand away.I would like to express my appreciation to my parents, Rachel and Avigdor,who have had their fingers crossed for the past several months while waiting "in thedark" across the sea. To my wife Edna: there is not enough space to express thegratitude you deserve for being so patient, understanding, and most of all for caring.Last but certainly not least, to our children Liron and Zohar, who have left their littlefriends behind and come to see the big world: I hope that the huge pile of scrap paperwill give you a chance to express your artistic talents.

Table of ContentsAbstractAcknowledgementsTable of ContentsList of FiguresNomenclature234691. Introduction1.1 Overview12122. Avionics Cooling2.1 Background2.2 The Importance of Avionics Thermal Control2.3 The Optimization Problem2.4 The Cooling Problem2.5 The Avionics Bay Environment2.5.1 The External Atmospheric Environment2.5.1.1 Atmospheric Temperature Model2.5.1.2 Atmospheric Pressure Model2.5.1.3 Atmospheric Humidity Model2.5.2 Aerodynamic Heating2.5.3 Aircraft Thermal Zones2.6 Avionics Cooling Techniques2.6.1 Ambient Cooled Equipment2.6.1.1 Cooling Requirements2.6.2 Forced-Air Cooled Equipment2.6.2.1 Cooling Requirements2.7 Environmental Control System1414181920222425252529313336384141433. Unconditioned Bay Configuration - Ambient Cooled Avionics3.1 Introduction3.2 Modes of Heat Transfer3.2.1 Dependence of Radiation and Convection Parameters on Altitudeand Configuration3.2.1.1 Convective Heat Transfer Coefficient3.2.1.2 Radiative Heat Transfer Coefficient3.3 Results3.3.1 Equipment Temperature Versus Altitude For a Single SegmentConvection Path System Configuration3.3.2 Equipment Temperature Versus Altitude for a Single SegmentConvection and Radiation Paths System Configuration3.3.3 Equipment Temperature Versus Altitude for a Double SegmentConvection and Radiation Paths System Configuration464646524. Conditioned Bay Configuration - Ambient and Forced-Air CooledAvionics4.1 Introduction92525456566881

-5-4.24.34.44.5Thermal Configuration of a Conditioned Avionics BayControl Volume Analysis For a Conditioned BayAnalysis of Altitude Dependent Effects on Bay TemperatureResults5. Summary and Conclusions5.1 Summary5.2 Conclusions and Implications9297101101108108110

List of FiguresFigure 2-1: Aircraft growth curve magnifies effects of weight increments[16]Figure 2-2: Trends in cabin and avionics heat load and aircraft mass [14].Figure 2-3: Illustration of order of aircraft penalty of an E.C.S. designedto cool 30 KW [14]Figure 2-4: Thermal acceleration factor for bipolar digital devices [1].Figure 2-5: Example - The influence of temperature on componentreliability (PNP Silicon transistor)Figure 2-6: Electronic component temperature buildupFigure 2-7: Illustration of responsibilities of aircraft and avionicsdesigners for thermal designFigure 2-8: Hot and cold atmosphere models - Temperature vs. altitude[23]Figure 2-9: Atmospheric model - Pressure vs. altitude [23]Figure 2-10: Atmospheric model - Design moisture conditions [23]Figure 2-11: Adiabatic wall air temperature versus Mach number andaltitudeFigure 2-12: Typical flight envelope of modem fighter aircraftFigure 2-13: Typical adiabatic wall temperature profile of modem fighteraircraftFigure 2-14: Typical aircraft thermal zones [7]Figure 2-15: Typical electronic equipment bay arrangements [10]Figure 2-16: Ambient cooled and forced-air cooled avionicsFigure 2-17: Temperature rise per unit heat flux vs. convective heattransfer coefficientFigure 2-18: Temperature-altitude operational requirements -- bay airtemperature versus altitude, MIL-E-5400 Class II [21]Figure 2-19: Forced-air cooled avionics cooling requirements - airflowvs. cooling air temperatureFigure 2-20: Environmental control system schematicFigure 2-21: Typical ECS cooling air temperature control scheduleFigure 3-1: Ambient cooled equipment: modes of heat transfer andthermal resistors modelFigure 3-2: Natural convection - avionics units vs transition to turbulentFigure 3-3: Single convection segment configuration schematicFigure 3-4: Numerical analysis flow diagramFigure 3-5: Effects of bay wall temperature and temperature difference onthe changes of (W 86062with altitude in a single segmentconvection7 ath configuration)ew ,'versus altitude, as a function of pressure onlyFigure 3-6: (Figure 3-7: Equipment temperature simulation based on MIL-E-5400class II temperature altitude envelope for a single segment convectionpathFigure 3-8: Single convection segment and radiation configurationschematic646670

Figure 3-9: Numerical analysis flow diagram for single convection andradiation systemFigure 3-10: Effects of radiation factor a, on the changes of ( Tew)at'with altitudeFigure 3-11: Equipment temperature simulation based on MIL-E-5400class H temperature altitude envelope for a single segment convectionpath and radiation, radiation factor a 0.01Figure 3-12: Equipment temperature simulation based on MIL-E-5400class H temperature altitude envelope for a single segment convectionpath and radiation, radiation factor a O0.1Figure 3-13: Equipment temperature simulation based on MIL-E-5400class II temperature altitude envelope for a single segment convectionpath and radiation, radiation factor a z1.0Figure 3-14: Equipment temperature simulation based on MIL-E-5400class II temperature altitude envelope for a single segment convectionpath and radiation, radiation factor a 10.0Figure 3-15: Equipment temperature simulation based on MIL-E-5400class II temperature altitude envelope for a single segment convectionpath and radiation, radiation factor rc 100.0Figure 3-16: Optimal temperature difference versus radiation factor aFigure 3-17: Double convection segment and radiation configurationschematicFigure 3-18: Numerical analysis flow diagram for double convection andradiation systemFigure 3-19: Effects of convection balance factor, y, on the changes of( ( Tw)ak\7173757677787980828486with altitude (without radiation)y for the system considered87in Fig. 3-19Figure 3-21: Effects of convection balance factor, y, on the changes ofin a system with radiation factor a 0.0188Figure 3-20: The changes in(ATewa))P,1/4versuswith altitudeFigure 3-22: Effects of convection balance factor, y, on the changes offactor a 0.1( A(T )S with altitude in a system with radiationFigure 3-23: Effects of convection balance factor, y, on the changes ofu with altitude in a system with radiation factor a 1.0( &Tewa"89Figure 3-24: Effects of convection balance factor, y, on the changes of91(ATew)st )((ATew )j)90with altitude in a system with radiation factor a 10.0Figure 4-1: Thermal configuration of a conditioned bay -- Ambient andforced-air cooled avionicsFigure 4-2: Control volume analysis for a conditioned avionics bay.Figure 4-3: Numerical analysis flow diagram for conditioned bayconfigurationFigure 4-4: The changes of bay air temperature with altitude for constantwall temperatureFigure 4-5: Bay air temperature vs. altitude for a simple temperaturealtitude profile as the wall temperature9398102104105

-8Figure 4-6: Bay air temperature vs. altitude and forced-air cooled heatload ratio in comparison with MIL-E-5400106

NomenclatureaACCdPFrghch,H hAkLmmM u/anPpqq" q/ArRst, TyLocal velocity of sound, [m/sec]Surface area, [m2]ConstantSpecific heat at constant pressure, [J/Kg"K]Diameter,[m]Radiation heat transfer factor, defined by equation (3.13), [W/OK 4 ]Acceleration of gravity, [m/s2 ]Average convective heat transfer coefficient, [W/m2 C]Average radiative heat transfer coefficient, [W/m2 "C]Heat transfer conductance factor (1/R), [W/oC]Thermal conductivity, [W/moC]Length, [m]mass, [Kg]Mass flow rate, [Kg/sec]Mach numberExponent - used for Rayleigh number in free convection 1/4 for laminar flow 1/3 for turbulent flowPressure - absolute, [N/m2 ]Pressure - atmospheres, [dimensionless]Heat transfer rate, [W]Heat flux, [W/m2 ]Recovery factor, defined by equation (2.5), [dimensionless]Thermal resistance, [OC/W]A characteristic dimension (in conduction path), [m]Absolute temperature, [OK]Elevation - altitude, [Ft]Dimensionless GroupsBi hskBiot modulusGrx p2pgrpGrashof numberI2Gr. p2 q-"x4Modified Grashof number for uniform heat flux (q")N, -Forced-air cooling influence numberhxxNux -h"Local Nusselt numberhLLNuL -"kAverage Nusselt number

-10-Prandtl numberPr CPk3RaL - spaOLRayleigh numberRa , Ra.,vkModified Rayleigh number for uniform heat flux (q")Greeka Radiation factor, Eq.E (3.7)a kThermal diffusivity, [m 2/sec](3Volumetric expansion coefficient, [oK-'],( 1/T for ideal gasses)Convection balance factor, Eq. (3.7)Normalized convective heat transfer coefficient, Eq. (3.7).Y6, he lt)8.ATp.pvaThermal boundary layer thickness, [m]Temperature difference, ["C]Dynamic viscosity of air, [Nsec/m 2 ] [Kg/msec]Density of air, [Kg/m 3]Kinematic viscosity of air, [m2/sec]Stefan - Boltzmann constantSuperscripts(C)()"( )Per unit time, [sec- ']Per unit area, [m- 2]Normalized parameter, P Paameter at atitdreParameter at sea levelSubscripts()alt()a()ambEvaluated at altitudeRefers to ambient temperature(),()bAdiabatic wall conditionsEvaluated at bulk temperatureConductionConvectionBased on diameterRefers to equipment surface temperatureRefers to the external airEvaluated at the film temperature, given by equation utInSummation conventionBased on length of plateMean flow conditionsOut

-11-()r()so)w()x()o()o(LRadiationEvaluated at sea levelRefers to wall temperatureLocal valueDenotes reference conditions(usually ambient pressure and temperature at sea level)Denotes stagnation flow conditionsEvaluated at free stream conditions

Chapter 1Introduction1.1 OverviewThe objective of this thesis is to examine the compatibility of the currentspecifications for avionics thermal design with the thermal environment encounteredin modem high performance jet aircraft.A subsequent goal is to examine thepossibility of improving the environmental control system (ECS) effectiveness bytailoring avionics specifications to meet actual environmental conditions.Two types of aircraft bays are examined. The first type is an unconditionedbay where the internal environment (temperature, pressure, humidity) is not activelycontrolled and ECS cooling air is not supplied to any of the equipment in the bay.The second type is a conditioned bay where cooling air is provided by the ECS forcontrolling the environment, or as a cooling fluid. The electronic equipment is alsoseparated into two categories by the cooling method used.The two coolingtechniques considered in this thesis are ambient cooling (where heat is transferred byfree convection and radiation) and forced air cooling (where heat is transferred tocold air supplied by the aircraft ECS).The analyses are presented in two chapters, distinguished by bay type. Chapter3 includes the analysis of the unconditioned bay. In this type of bay, only ambientcooled avionics equipment are considered. Chapter 4 includes the analysis of theconditioned bay. For this type of bay, both ambient and force cooled avionics areexamined.For each bay type the effects of altitude variation on equipment and internal

-13bay temperatures are analyzed.Temperature-Altitude performance curves aregenerated, and discussed in light of the requirements found in existing military andaircraft manufacturers specifications for avionics thermal design of recent aircraft(e.g. MIL-E-5400 [21] and F-15 [6]).

-14-Chapter 2Avionics Cooling2.1 BackgroundThe demand for avionics cooling in aircraft has increased in recent years, as thequantity and complexity of electronic equipment installed aboard has increased. Thisis brought about mainly by the rapid development of new electronic systems, and thetrends towards more sophisticated aircraft and engine electronic control systems.Furthermore, increases in aircraft performance have resulted in increasedaerodynamic (kinetic) heat loads due to the higher speeds flown by modem aircraft.The increased heat load imposed on aircraft requires larger and heavier coolingequipment. At the same time aircraft mass has reduced, resulting in cooling systemscomprising a higher fraction of the vehicle mass.The total mass of coolingequipment in a modem high performance aircraft can be as much as 300 Kg (660 lb)[14] [18]. The ECS mass is undesirable for the following reason: if the performanceof the aircraft (range, maneuverability, payload) are to be maintained, additional wingarea, thrust, and fuel are required to compensate for the added weight. Thus, theactual weight penalty of an aircraft can be 1.5 - 7 times larger than the basic increasein the specific system weight, as shown in Fig. 2-1 [16]. It can also be seen from Fig.2-1 [16] that the smaller aircraft with higher performance are typically the mostsensitive.The other aspect concerning aircraft mass is the limited use of the airframe as apotential heat sink due to the reduction in airframe mass. The importance of airframeas a heat sink is mainly for transient conditions where temporary high heat loads canbe absorbed by the airframe and thus moderate the effects of transient heatingextremes.

EIIIII-1576zC52:I-0zaz2RANGE/PAYLOADFIXEDALL PERFORMANCEFIXEDFigure 2-1: Aircraft growth curve magnifies effects of weight increments [16]A summary of the trends in avionics and aircraft design compiled from a broadselection of American and European combat aircraft over the years 1955-1976 isshown in Fig. 2-2 [14]. It can be seen that avionics and cabin heat loads have beenincreased by a factor of 3 while aircraft mass has reduced by a factor ofapproximately 3.In addition to the weight penalty there are two other major performancepenalties resulting from the use of engine bleed air as a conditioning fluid by mostenvironmental control systems.The first penalty is associated with the directreduction of engine thrust which results from bleeding off engine compressor air.The second penalty is due to the drag which results from cooling the high pressure,high temperature bleed air through a ram-air heat exchanger before it is used as aconditioning fluid. The magnitude of the combined penalty of using engine bleed air

-16-AAALUU40300zU,10020zU--c10 C01950196019701980YEARFigure 2-2: Trends in cabin and avionics heat load and aircraft mass [14].is typically in the order of 20 KW per 1 KW of power being cooled, which representsa system coefficient of performance of 5 percent, as depicted in Fig. 2-3 [14], but canbe much higher (more than 200 KW per KW extracted) for the more advancedengines at high speeds [16].The conclusion is straightforward:engine bleddedcooling air is extremely expensive and therefore should be used efficiently.

-17-80(60Cn-40C020(Figure 2-3: illustration of order of aircraft penalty of an E.C.S.designed to cool 30 KW [14]

-182.2 The Importance of Avionics Thermal ControlAs the aircraft dependence on avionics has increased, electronic componentreliability has become one of the most significant factors which determinessatisfactory aircraft operation.The relationship between individual componenttemperature level and reliability is considered to be understood [22]. Failure rate istypically assumed to increase exponentially with temperature. Example is shown inFig. 2-4 [1].20406080100120140Temperature ,*CFigure 2-4: Thermal acceleration factor for bipolar digital devices [1].The effect on reliability is seen in Fig. 2-5 which presents reliability curves ofPNP Silicon transistor for two different temperatures. It can be seen that reliability ofthe specific component decreases with increasing temperature.

-19-1.21.00.8.0.60.40.20.0020406080100120Time in million hoursFigure 2-5: Example - The influence of temperature on component reliability(PNP Silicon transistor)Temperature cycling has also been found to reduce reliability, almostindependently of the influence of the average temperature level. Increased failurerates, by a factor of 8 were reported by Hilbert and Kube [12] for temperature cyclingin excess of 150C.In addition to thermal factors vibration, moisture, humidity, and altitude arealso known to degrade electronic components reliability [25].2.3 The Optimization ProblemSince avionics reliability is very sensitive to the operating temperatures, andaircraft penalties are very sensitive to the avionics cooling requirements, it isimportant to optimize the integrated avionics/ECS system.The goal of such anoptimization is to maintain desired level of avionics reliability while minimizing ECScooling air requirements.The important parameters which are required for theoptimization process are the bay internal environment, ECS cooling air temperature,

-20-and the electronic components temperatures.Unfortunately, the decision aboutavionics heat loads and operating temperatures, as well as ECS cooling capacity andoperating temperatures, has to be made in an early stage of the development phase ofboth the aircraft and the avionics [14] [20] [21] [22]. It is therefore essential thatinformation about the aircraft thermal environment and component temperatures areavailable as accurately as possible, and as early in the design process as possible.In this thesis these two points are addressed, first, a method is developed tomodel the integrated equipment/aircraft system and to analyze bay and equipmenttemperatures. The results can be used in identifying the critical points for thermaldesign purposes.The method helps in predicting the maximum or worst casetemperature that may be expected during flight conditions at altitude based on knownperformance of the system at sea level.The thermal predictions may also beapplicable for reliability prediction purposes as well.The second point is addressed by analyzing the expected change of theenvironment within the aircraft bay as a function of flight envelope and altitude byassuming standard atmospheric models. The result of such an analysis are presentedas temperature-altitude environment curves.2.4 The Cooling ProblemSince individual electronic components (e.g. diodes or transistors), are the heatsources within the electronic boxes, they will be the hottest points. The componenttemperatures depend on two major factors: first, the environment in which theequipment operates and the ability to transfer heat to the external air, and second, thethermal control design of the equipment.While the first establishes the heat sink temperature, the second determines the

-21temperature difference (AT) between the heat sink temperature and the specificcomponent temperature, as shown in Fig. 2-6.------------------------------- IAVIONICS BOXAIRCRAFTENVIRONMENT -IUII------------ --H-TAH------A TTHCOMPONENTTEMPERATUREELECTRONICTACOMPONENTP I:BAY TEMPERATUREII------------------------- MIIIIIIIIIIIIIIIIIIIIII------.Figure 2-6: Electronic component temperature buildupThe relation between the the electronic component temperature, TH, and theenvironment (heat sink) temperature, TA, is given by:qcomponen, Hover(TH-TA)(2.1)where qcopoe., is the heat dissipated from the component, and Ho,,oa is the overallheat transfer coefficient which includes geometry factors and reflects an equivalentheat transfer coefficient for the combined coefficients of the various heat transfermodes that take place in this process (e.g. conduction, convection, radiation). Thus,for a given heat dissipation, qcom,,onn,, to be removed from the component, bothHow,,1and TA have a direct effect on the component temperature TH.In practice, equipment thermal control design and the environment lie under

-22separate responsibilities, i.e. the avionics designer is responsible for transferring heatfrom power dissipating components within the box to a suitable heat sink, and theaircraft designer has to provide an aircraft atmosphere or cooling services compatiblewith the equipments needs to transfer heat from the box, as shown schematically inFig. 2-7. Therefore, it is convenient to separate between the environment and thethermal control design of the avionics box, and to analyze them independently. Thephysical interface between the equipment and the aircraft replaced for designpurposes by specifications (interface control documents) to enable each party topursue independent designs. The thermal environment which is used both as an inputto the avionics thermal control design, and as a requirement for the ECS design, isone of the most important elements of such a specification.Furthermore, during the past few decades, many of the specifications fromdifferent applications have been grouped into design standards. This is mostly thecase for military aviation and in many cases for civilian aviation as well[1] [18] [21] [25] [30]. MIL-E-5400 [21], for example, is one of the most commonused specifications for defining environment temperatures as function of altitude.2.5 The Avionics Bay EnvironmentThe avionics bay environment including temperature, pressure (density), andhumidity, is of primary importance for the design of airborne electronic equipment.These parameters are strongly dependent on the altitude, which therefore is also animportant parameter in the determination of the thermal environment.As wasexplained in the previous section, the bay and the cooling fluid (environmentalfactors) temperatures, TA, are related to the electronic component temperature(avionics thermal design factors), TH by the following equation:qcomponen Hov ri(TH- TA)(2.2)

-23-AVIONICSAIRCRAFTTTwlFigure 2-7: Illustration of responsibilities of aircraft and avionics designersfor thermal designHence, the bay temperature or the cooling fluid temperature set the datum line for theelectronic component temperature.The contribution of pressure and humidity isexplained below. The primary importance of density is in heat transfer by naturalconvection where buoyancy forces are the fluid driving forces. Since air may beconsidered as an ideal gas, there is a direct relation between its absolute pressure (P)and its density (p) for a given temperature (T):P pRT(2.3)were R is the gas constant. Thus, since pressure reduces with increasing altitude thedensity also decreases. This in turn, results in a reduction of the effectiveness ofnatural convective heat transfer with altitude.

-24Humidity, on the other hand affects the integrated ECS/avionics system designproblem differently. Moisture and humidity have been found to have a significantadverse effect on equipment performance and reliability [1] [18] [30] and thereforeshould be avoided. Condensation can occur when atmospheric air is cooled below itsdew point. This condensation typically determines the lowest temperature used bythe environmental control system if no other means (such as water separators) areintroduced. It is worth mentioning here that humidity is also a function of altitude,and hence there is an additional coupling between temperature and altitude.Three factors influence the parameters which drive the bay environment. Thefirst is the external ambient environment which constitutes the ultimate heat sink forthe aircraft. The second factor is the aerodynamic heating which should be added onthe basic environment. High speed flight combined with high external atmospherictemperature may result in aircraft skin temperatures above 100 oC due to energyrecovery in the boundary layer. The third component to be considered is the effect ofthe specific configuration of the aircraft/avionics system which includes bay location,internal heating by equipment dissipation, or cooling by the environmental controlsystem if used. These three aspects of the environment are described in the followingparagraphs. Other factors such as solar radiation and engine heat may affect the baythermal environment as well.2.5.1 The External Atmospheric EnvironmentSeveral atmospheric models exist for various applications, however, for thepurpose of this thesis the models of MIL-STD-210 [23] which are included in manymilitary specification and standards are being used.

-25-2.5.1.1 Atmospheric Temperature ModelTwo atmospheric models are given, cold and hot, which provide probableextreme minimum and probable extreme maximum temperature-altitude data.The model is presented in Fig. 2-8. It can be seen that highest temperatures(hot atmosphere) are expected at sea level (40 oC), and temperature decreases at a rateof about 2 OC/1000 ft up to an altitude of 40,000 feet then rather constant temperaturelevels are encountered (-43 to -20 OC).2.5.1.2 Atmospheric Pressure ModelThe pressure - altitude model given in MIL-STD-210 [23] for the hotatmosphere is used in this thesis and it is presented in Fig. 2-9. Fig. 2-9 shows thatpressure decreases in an exponential manner with increasing altitude.2.5.1.3 Atmospheric Humidity ModelFig. 2-10 describes the design humidity conditions to be considered for thedesign of the environmental control system. Absolute content of water in externalatmospheric air decreases exponentially with altitude and therefore at higher altitudethe air temperature can be reduced to lower temperature without condensation. Thisenables cooling temperature of the environmental control system to be set at a lowervalue at higher altitude resulting in increased cooling capacity of the system.

40-2002040Te perature * CFigure 2-8: Hot and cold atmosphere models - Temperature vs. altitude [23]

-27-.2.4.RELATIVE PRESSURE (PALT/PO)ATMOSPHERIC PRESSURE GRADIENTFigure 2-9: Atmospheric model - Pressure vs. altitude [23]

-28-.026II1.022Ili!------nI--.01---- I-2t L 10515,.TITUr . m.-,m --'--.mijiiiiino2030- T"usAN DO7 fET3540Figure 2-10: Atmospheric model - Design moisture conditions [23]

-29-2.5.2 Aerodynamic HeatingThe most important external aerodynamic effect relevant to the bay thermalenvironment is th

Figure 3-12: Equipment temperature simulation based on MIL-E-5400 76 class H temperature altitude envelope for a single segment convection path and radiation, radiation factor a O0.1 Figure 3-13: Equipment temperature simulation based on MIL-E-5400 77 class II temp

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