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Published byAlan Marshall Modified over 6 years ago
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Lecture Objectives: Finish with review of radiation Learn about
External long wave radiation Soar radiation components
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Radiative heat flux between two surfaces
Simplified equation for non-closed envelope Exact equations for closed envelope ψi,j - Radiative heat exchange factor
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From the previous class View (shape) factors
For closed envelope – such as room
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View factor relations F11=0, F12=1/2 F22=0, F12=F21 F31=1/3, F13=1/3
A1=A2=A3 A1
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Boundary Conditions at External Surfaces
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External Boundaries
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Radiative heat exchange at external surfaces
View (shape) factors for: 1) vertical surfaces: - to sky 1/2 to ground 1/2 2) horizontal surfaces: - to sky - to ground 3) Tilted surfaces - to sky (1+cosb)/2 - to ground (1-cosb)/2 surface b ground General equations:
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Ground and sky temperatures
Swinbank (1963, Cole 1976) model Cloudiness CC [0-1] 0 – for clear sky , 1 for totally cloud sky Air temperature Tair [K] Tsky4 = · 10−6(1 − CC) Tair6+ Tair4CC·eclouds Emissivity of clouds: eclouds = (1 − 0.84·CC)( *exp[8.45·(1 − 273/ Tair)]) CC For modeled T sky the esky =1 (Modeled T sky is for black body)
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Ground and sky temperatures
Berdahl and Martin (1984) model - Cloudiness CC [0-1] 0 – for clear sky , 1 for totally cloud sky Air temperature Tair [K] Dew point temperature Tdp [C] !!! Tclear_sky = Tair (eClear0.25) eClear = (Tdp/100) (Tdp/100) emissivity of clear sky Ca = *CC *CC *CC3 – effect of cloudiness Tsky = (Ca)0.25 * Tclear_sky esky =1
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Ground and sky temperatures
For ground temperature: - We often assume: Tground=Tair
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Solar radiation Direct Diffuse Reflected (diffuse)
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Solar Angles qz - Solar altitude - Angle of incidence - Azimuth
b - Inclination
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Direct and Diffuse Components of Solar Radiation
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Solar components Global horizontal radiation IGHR
Direct normal radiation IDNR Direct component of solar radiation on considered surface: Diffuse components of solar radiation on considered surface: qz Total diffuse solar radiation on considered surface:
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