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Vergara - 1976 - Physiological and morphological adaptability of ri

Vergara - 1976 - Physiological and morphological adaptability of ri

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142 (rut-tars mo arcs<br />

closely related to our own expe<strong>ri</strong>ence <strong>and</strong> which we believe me<strong>ri</strong>t attention in<br />

future design <strong>and</strong> operation <strong>of</strong> controlled-environment facilities.<br />

For a number <strong>of</strong> reasons we have chosen the latter course. These include the<br />

belief that research results available in this field need further development before<br />

they are ready for coordination to b<strong>ri</strong>ng out major p<strong>ri</strong>nciples. With the<br />

approach adopted we can provide information which may be new <strong>and</strong> <strong>of</strong> i1n1nediate<br />

assistance in the development <strong>and</strong> use <strong>of</strong> phytotrtin facilities.<br />

We shall consider first certain aspects <strong>of</strong> the basic physics in the strategy <strong>of</strong><br />

design, <strong>and</strong> thcn some aspects <strong>of</strong> the interaction <strong>of</strong> controlled-environment<br />

conditions with the plants themselves.<br />

In the va<strong>ri</strong>ous types <strong>of</strong> phytotrons which have been constructed to date there<br />

has been a wide diversity <strong>of</strong> design solutions. Table l, which is taken predominantly<br />

from data assembled by" de Bilderling (pers. comm), illustrates this. It<br />

presents representative data for major installations in va<strong>ri</strong>ous parts <strong>of</strong> the world<br />

<strong>and</strong> is not intended to cover all facilities <strong>of</strong> this nature.<br />

lt is apparent from Table l that a major design difference is whether an i11-<br />

stallation has a large proportion <strong>of</strong> its controlled space naturally lit, or whether<br />

it is completely artificially lit. This is a fundamental distinction for most environments.<br />

First. it has a major effect on heat exchange physics <strong>and</strong> their costs.<br />

Second, it generally has a major effect on the amount <strong>of</strong> environmental ‘va<strong>ri</strong>ability<br />

that both the plants <strong>and</strong> the control machinery have to cope with. Third, it<br />

may substantially influence uncertainties as to how far conditions in a phytotron<br />

are duplicating or controlling the important factors <strong>of</strong> the natural environment,<br />

i.e. will plants grow <strong>and</strong> respond as they would in a supposedly similar<br />

natural environment‘? Accordingly. each <strong>of</strong> these three aspects Will be considered.<br />

HEAT EXCHANGE PHYSICS<br />

In phyitotrtiits. removal <strong>of</strong> excess heat from the plant-growing area is the dominant<br />

load both in quantity <strong>and</strong> in costs. The naturally lit space design must allow<br />

for the maximum heat load coming from the external environment while the<br />

artificially lit space design can be for the mean heat load.<br />

Naturally lit rooms<br />

Machinery for a naturally lit space must h<strong>and</strong>le the maximum summer solarheat<br />

load. This will vary somewhat with location. but for a representative figure<br />

we have taken the design level quoted for the SEPEL Phytotrons. i.e. those at<br />

Duke <strong>and</strong> North Carolina State Universities. USA. (DOWIIS et al.._ 1972). This<br />

was for 283 BTU - ftr? -hr' per sq ft per hour for incoming radiation onto a ho<strong>ri</strong>zontal<br />

surface which equates to approximately 2.830 BTU - rnr? - hrl. Additionally.<br />

allowance in cooling capacity has to be made for inward heat transfer through<br />

the glass surfaces when outside temperature conditions are substantially above<br />

those <strong>of</strong> the rooms. This will ‘vary with the conditions in the va<strong>ri</strong>ous rooms. but

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