Laserfiche WebLink
<br />EM 1110-2-1406 <br />5 Jlln 6l) <br /> <br />and B is the thermsI quality, For a melting mountain snowpack (thermal qnality assumed to be <br />0.97), tbe melt equation for shortwave radiation is <br /> <br />e <br /> <br />M,,=O.00508I,(I-a) <br /> <br />(3: <br /> <br />In the middle latitud,'s during late spring, the maximum solar radiation for a clear day for a hori. <br />zontal surface is about 800 langlrys. With a minimum albedo of 40 percent, the rrsulting possible <br />shortwave radiation melt for an unforested area is in the order of 2.4 inches per day, We shull <br />see in the next paragrnph, however, that generally some of this energy is lost from the snowpaek <br />by longwave radiation, <br /> <br />No!e: <br />Tronsr."li$!Iion cu,-v~s ore For doily ins%llon <br />ornoun.fs. They represent mean condilions <br />during !h! sprinfl snow..m~U season. Acfual <br />fronsfT"SSton 0; msolahon may diFFer rrom <br />fho! indicofl1d due ;0 d;f'f'erenC'~s in the solor <br />o/fiflJd~ ~ heigh! ond 6pocing of' frees. and <br />dirrerences in types of' frees. <br /> <br />'00 <br /> <br /> <br />~ <br />z <br />w <br />U <br />~ <br />w <br />~ eo <br /> <br />i . I <br />~--!. -------L-t-.- <br />I · I I <br />I! i <br />r- .-- _L. - ---"---- ---'--- <br /> <br />. <br />'- <br />. <br /> <br /> <br />Lo.: 60 __ <br />~ <br />w <br />o <br />u <br />z <br />~ 40 <br />~ <br />'i <br />~ <br />z <br />< <br />~ 20 <br />~ <br />::J <br />~ <br />o <br />~ <br /> <br /> <br />i <br />-+- <br /> <br />I <br />0.2 0.4 0.6 o.e <br />F'aREST CANOPY DENSITY <br />(HORIZONTAL PROJECTION) <br /> <br />0.0 <br /> <br />o <br /> <br />~ <br />z <br />w <br />u <br />o <br />20 :r <br /> <br />'" <br /> <br />o' <br />w <br />> <br />403 <br />> <br />" <br />o <br />z <br />< <br />60 u <br />~ <br />~ <br />w <br />o <br />o <br />" <br />80 ~ <br />~ <br />u <br />w <br />" <br />" <br />w <br />'00 <br />..a <br /> <br />e <br /> <br />Figure 4-. Transmission of solar radiation by forest canopy, based on daily insolation for coniferous forest during <br />spring snowmelt season. <br /> <br />2-06. LONGW A VE :RADIATION. Snow is very nearly a perfect blnck body with respect to <br />longwave (terrestial) radiation, absorbing all such radiation incident upon it and emitting tbe <br />maximum possible radiation in accordance with Stefan's law. This is expressed by th" ('quat ion <br /> <br />E=uT4 <br /> <br />(4) <br /> <br />where E is the total energy of all wavelengths, u is Stefan's constant, * and T is the black body <br />temperature in degrees absolute. A rnelting sno\vpack has a surfuce temperature of 00 C., and, <br />according to Stefan's law, it loses energy at the rate of 0.-1.59 ly/min. Opposed to this loss is tbe <br />back radiation from the atmosphere Dr forest.. For ckar skies, the heat gain from back radiation <br />is gene.rally less than the heat loss, so thnt Hlt'r'- i" :1P[. IJ('ut loss from the snowpack by longwave <br />radiation. With cloudy skies or b12nl'l1:L :~-ll\.:::it canopy, however, the back radiation may be <br />greater or less than tbe loss from tb" sllowpack, depending principally upon the ambient air <br />temperature. <br /> <br />....=O.826Xlo--IO(ly!min)!(" K;-II, <br /> <br />6 <br /> <br />e <br />