Waa5g(a)H64321(b)LFigure 1. Functional scheme of systemThe CPC module consists of a complexcylindrical-parabolic reflection surface and a coppertube with ø15 mm outside diameter used as theabsorber. Cylindrical cooper absorber is surroundedby a glass surrounding layer for lowering convectiveloss from the collector pipe. The area between thepipe absorber and glass surrounding layer isevacuated. Conversion of solar energy into heat isconducted on the pipe collector. Pipe absorber iscolored with selective color of high absorbingproperties and low emissivity (ε r ). The area of thereflector has high reflection ratio (ρ m ). Between thepipe absorber and the reflector there is a gap (hole)which stops heat transfer from the collector pipe tothe reflector. Water is the working fluid, with alaminar flow through the pipe of the collector.Apparatus of the collector is covered by transparentcover layer made of glass (Plexiglass) so the reflectorarea could be saved from wearing and to lower thevalue of heat loss from the assembly pipe absorbersurroundingpipe layer. The collector consists of sixCPC modules which are connected parallel to theflow paths, so flow properties inside them may beconsidered equal.III.A. IntroductionMATHEMATICAL MODELBased on the physical model represented by theCPC collector, through whose absorber pipe a laminarflow of water occurs, and which is subjected to solarradiation, a mathematical model is proposed. Themathematical model consists of the energy balanceequations for four CPC module components: (1)working fluid, (2) collector pipe- absorber, (3)surrounding pipe layer, (4) transparent cover. Duringthe set-up of mathematical model only one module ofCPC collector was analyzed.B. Basic assumption according to which the modelwas basedThe following assumptions were introduced forthe definition of mathematical model:- The sky was treated as an absolute blackobject, which is the source of infraredradiation during an equivalent skytemperature - Reflected radiation from surroundingobjects was considered negligible andwas not taken into account;- Diffusive insulation on the apparatus ofthe cover is isotropic;- CPC collector has permanent Suntracking, thus Sun rays are normal to theplane of transparent cover (apertureplane);- Radiation to the collector is unified;- CPC module is constructed with idealgeometry, thus the concentration ratio isgiven by: [13]: (1)- Heat transport in the transparent cover,surrounding cover layer, collectorsurrounding layer, pipe absorber and thefluid is transient- Transparent cover, transparent coverlayer, collector surrounding layer, andpipe absorber are homogenous andisotropic objects;- Heat transport by conduction in thetransparent cover layer and the glasslayer is negligible due to small heatconductivity of glass;- Thermo-physical properties of the CPCcollector component material (ρ * , c, λ)as well as optic properties (ρ, τ, ε, α) ofthe components of CPC collector are donot depend on coordinates, temperaturenor time;- Fluid flow is steady state and it isconducted only in the axial direction,thus the velocity field is related just tothe speed component w z ;- Fluid flow shape is the same in everyaxial cross sections, thus the tangentialvelocity component w φ does not exist;- Radial velocity component w r isneglected as a value of smaller order andthus the convection in radial direction isalso neglected;- Fluid flow may be consideredincompressible;- Conduction in the axial direction has anegligibly small contribution to theresulting heat transport compared to theconvection.102
C. Energy balance equationMathematical model consists of equations ofenergy balance for all of the four components of theCPC modle, relations for determining heat transfercoefficient, relations for radiation absorbed by therelevant system components. In order to gain a unifiedsolution from the system of equations, initial andboundary conditions are defined. With apredetermined assumptions, equations of energybalance may be written as:(1) For the working fluidEnergy balance for an elementary fluid volumeof dz length in the axial direction, after sorting, maybe written as:T* * f c A *c A*wf p f f f p f f ztU T 2/ r T rr f f r , oTfzWhere ∗ , i w z represent density, specificheat, velocity in the axial direction of the elementary*fluid volume, respectively A 2 f r r , iis the area ofthe cross section of the elementary fluid particle. Thesecond term on the right hanside of the equation (2)represents heat gained from the outer side of thecollector pipeBoundary condition for this equation is:za z = 0,fin(2)T T . (3)(2) For the collector absorber pipeEnergy balance for elementary part of the collector ofdz length in the axial direction may be written as;* * TrTr* r cr Ar r Ar hc, r / ehr, r / et z zTr Te 2 rr , o-U r / fTr Tf2 rr , o qb, rqd , r2 rr , o (4)Where λ r , ∗ i c r are head conductioncoefficient, density and specific heat for elementary* 2 2pipe volume, respectively. Ar rr, o rr, i is thearea of the cross section of elementary part of thecollector pipe. The first term on the right hand side ofthe equation (4) represents heat transport byconduction in the axial direction of the collector, thesecond is the heat loss due to convention and radiationbetween the collector pipe and the surrounding layerof the collector pipe, the third term represents heatgiven to the working fluid, and the fourth representsheat gained via solar radiationBoundary conditions for this equation are:T za z 0, r 0 ; (5)zza z L,T r 0(6)z(3) For the transparent cover of the pipecollectorEnergy balance for the elementary part of thesurrounding layer of the collector pipe of dz length iswritten as:* * T eece Ae hc, r/ ehr, r/eTr Te 2 r,ot-hc, e/ chr, e/cTeTc2 re , o qb, eqd , e2 r(7)r,o∗Where i c e are density and specific heat og the* 2 2surrounding layer of the collector Ar re, o re, iis the area of the cross section of elementary part ofthe surraounding layer of the collector. The secondterm on the right hand side of the equation (7) is theheat lost due to radiation from the surrounding layerof the collector to the transparent cover(4) For the transparent coverEnergy balance for the elementary part of thetransparent cover of the concentrating collector, withdz length in the z direction and W width, may bewritten as:* * T cccc Ac hc, e/ chr, e/cTe Tct2 re , o h c, c/ aTc Ta W hr, c/sTc TsWq b , cq d , c2 r r , o(8)*A c W is the area of the cross section ofelementary part of the transparent cover of thecollector. The second term on the right hand side ofthe equation (8) is the heat lost due to convectionfrom the transparent cover to the environment, thethird term is the heat lost due to radiation between thetransparent cover and the sky.D. Initial conditionsIt was assumed for the initial conditions that inthe initial time point the temperature field in allcomponents is equal to the environment temperatureT a , while the fluid temperature at the inlet is constantin timeZa t 0, TfTr Te Tc Ta(9)Za z 0, T fT in(10)103
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Toward Future: Positive Net-Energy
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