1993
DOI: 10.1016/0196-8904(93)90089-s
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Theoretical and experimental investigations of heat transfer in a trombe wall

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Cited by 52 publications
(12 citation statements)
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“…The average convection heat transfer coefficient given by McAdams et al is used on the outside surface of the glass cover. In the absence of forced convection, a heat transfer coefficient of 5 W/(m 2 K) is designated [18]. The glass cover of the system is assumed to have an emissivity of 0.88 [19].…”
Section: Fluid Domainmentioning
confidence: 99%
“…The average convection heat transfer coefficient given by McAdams et al is used on the outside surface of the glass cover. In the absence of forced convection, a heat transfer coefficient of 5 W/(m 2 K) is designated [18]. The glass cover of the system is assumed to have an emissivity of 0.88 [19].…”
Section: Fluid Domainmentioning
confidence: 99%
“…(3) Glass Cover: A pv (h r,pv-g +h c )(T pv -T g )=A pv (h r,g-a +h w )(T g -T a ) ( 4 ) Electrical Power generation G=E+h w (T pv -T e ) +h c (T pv -T f ) ( 5 ) The maximum power output decreases linearly with increasing cell temperature and is proportional to the absorbed incident solar radiation as is given as: E= ( T pv +β) I r (6) The channel air temperature is assumed to vary linearly in the flow direction so that the mean temperature T f required to fix air properties is calculated as T f = (T out +T int )/2 (7) The average convective heat transfer coefficient due to wind on the outside surface of the PV glazing cover is given by [15] h w = 5.7+3.8V (8) The equations for laminar and turbulent boundary layer from Tsuji and Nagano [16] are used: N ux =0.387(G rx P r ) 1/4 for Laminar boundary layer (9) N ux =0.120(G rx P r ) 1/3 for Turbulent boundary layer (10) The heat transfer coefficient is calculated from h c (X)=(N ux λ a )/X (11) The overall heat loss coefficient U L combines the losses from the top (front) U t , bottom U b and sometimes edges U e but normally the edge losses is assumed to be negligible or included in the back loss: U L =U t +U b (12) The top heat loss coefficient U t is evaluated by considering the wind convection h w and the radiation heat exchange with sky h r,g-a from the glass cover of PV module [17]:…”
Section: Nomenclaturementioning
confidence: 99%
“…Likewise, later experimental research done by Smolec and Thomas [1993] and Onbasioglu and Egrican [2002] did not present enough information that could be used to make a direct comparison. Smolec and Thomas [1993] From all literature reviewed, only experimental data presented by Warrington and Ameel [1996] are applicable to directly compare with an existing feature for the Trombe wall in the EnergyPlus.…”
Section: Literature Reviewmentioning
confidence: 99%
“…Of those component models, the inside convection coefficient model is probably the most important as most research on the Trombe wall focused on this particular subject [Akbari and Borgers 1979;Smolec and Thomas 1993;and Warrington and Ameel 1995]. Also, it has been shown that the calculation procedures for insolation, solar radiation transmitted through a clear window, and conduction through solid materials were adequately accurate and Judkoff 1988].…”
Section: Summary Of Significant Findingsmentioning
confidence: 99%
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