T. Boulard et al., NATURAL VENTILATION BY THERMAL EFFECT IN A ONE-HALF SCALE-MODEL MONO-SPAN GREENHOUSE, Transactions of the ASAE, 41(3), 1998, pp. 773-781
Airflow and temperature patterns induced by natural convection were ch
aracterized in a 1/2 scale model mono-span greenhouse model simulating
the absorption of solar radiation at the floor surface. Temperatures
were studied by means of thermocouples and airflows by means of hot wi
re anemometry. The main features of the temperature and flow patterns
were observed in permanent regime for Grashof numbers based on the Del
ta T between inside and outside and on the width of the opening, rangi
ng from 10(6) to 10(7). With a single sided vent situated on the roof
inflows at the lower part of the opening were always observed, and a s
ingle airflow loop which followed the walls, the floor and the roof of
the greenhouse before escaping through the upper part of the vent ope
ning. With a two sided vent opening, a single airflow loop always prev
ailed with a large recirculation rate, some outside air coming in thro
ugh the lower parts of the openings, compensated by air exiting throug
h the upper parts of the same openings. In all situations, thermal gra
dients extended over thinner layers (5-6 cm) than velocity gradients (
about 50 cm). In these conditions, the vertical temperature profile wa
s characterized by a strong temperature drop just above the heated soi
l surface which represents about 70% of the total temperature differen
ce between the soil surface and the outside. Values for the ventilatio
n rates were deduced by expressing the thermal balance of the greenhou
se and compared with those deduced from Bernoulli's theorem. More gene
rally the measured flow patterns were compared with those reported in
the literature for ventilation and heat transfers in closed greenhouse
s. The similitude of the inside patterns observed in each case suggest
s that both the exchanges between inside and outside the greenhouse an
d between the warm soil and the roof can be considered as driving forc
es influencing the flow.