International Lighting in Controlled Environments Workshop

  T.W.Tibbitts (editor)  1994   NASA-CP-95-3309               home | contents


HEAT DISSIPATION IN WATER-COOLED REFLECTORS  (Short Report)

Toyoki Kozai

The energy balance of a high pressure sodium lamp with and without a reflector is given in Fig. 1. The energy balance of a lamp varies with the thermal and optical characteristics of the reflector. The photosynthetic radiation efficiency of lamps, defined as input power divided by photosynthetically active radiation (PAR, 400-700 nm) emitted from the lamp ranges between 0.17 and 0.26. The rest of the energy input is wasted as longwave (3000 nm and over) and non-PAR shortwave radiation (from 700 nm to 3000 nm), convective, and conductive heat from the lamp, reflector, and ballast, and simply for increasing the cooling load.

Furthermore, some portion of the PAR is uselessly absorbed by the inner walls, shelves, vessels, etc. and some portion of the PAR received by the plantlets is converted into sensible and latent heat. More than 98% of the energy input is probably converted into heat, with only less than 2% of the energy input being converted into chemical energy as carbohydrates by photosynthesis. Therefore, it is essential to reduce the generation of heat in the culture room in order to reduce the cooling load.

Through use of a water-cooled reflector, schematically shown in Fig. 1, the generation of convective and conductive heat and longwave radiation from the reflector can be reduced, without reduction of PAR.

With the water temperatures at the inlet being 13o C and the water flow rate being 3.2 g/s, 50% of the energy input was removed by the water, resulting in a water temperature at the outlet of 25oC. The temperature distribution of the lamps with different reflectors is given in Table 1.

The warmed water coming out of the reflector can be used as a low-temperature heat source and for washing, because the water will not be polluted in the closed-water distribution system. Details of this study are provided in Kozai (1991).

TABLE 1. Temperatures of lamp, reflector and surroundings.

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Lamp type

(For lamp types, see legend to Fig.2)

 

A

B

C

D

E

Lamp bulb

Inner surface of reflector

Outer surface of reflector

Ballast

Room air

Floor

Wall

Ceiling

160

-

 

-

62.6

25.1

24.7

25.7

25.1

177

46.6

 

-

62.6

25.0

25.5

25.0

25.0

175

58.0

 

57.0

62.6

25.1

25.2

25.2

24.7

205

92.3

 

78.8

62.6

25.0

25.2

25.0

24.7

180

30.4

 

24.6

62.6

25.0

25.2

24.7

24.7


 

 

 

 

 

 

 

 

 

 

 

 

Fig KozB 1.jpg (57206 bytes)

Fig. 1. Schematic diagram of a lamp bulb with normal and water-cooled reflectors.

 

Fig KozB 2.jpg (177636 bytes)

Fig. 2. Energy distribution of a high pressure sodium lamp bulb with or without a reflector Lamp type: A lamp without reflector; B lamp with polished aluminum reflector; C lamp with white-colored aluminum reflector; D lamp with white-colored enameled iron reflector; E lamp with water-cooled white-colored enameled iron reflector.

 

REFERENCE

Kozai, T. 1991. Autotrophic micropropagation. p. 313-343. In Y.P.S. Bajaj (ed.) Biotechnology in agriculture and forestry 17: High-Tech and Micropropagation I. Springer-Verlag, N.Y., U.S.A.

 


Kozai, T. 1994. Heat dissipation in water-cooled reflectors, p 379-380. In: T.W.Tibbitts (ed.). International Lighting in Controlled Environments Workshop, NASA-CP-95-3309. 


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