Heat loss through the exterior walls of a heated space increases when there exists a partition-wall in the space, due to the additional heat transfer from the partition-wall to the main walls. However, as the mean radiant temperature (MRT) in a space with partition is higher than that without partition, the lower air temperature in such a space may still be acceptable from the viewpoints of thermal comfort. The purpose of this study is to clarify the effects of some environmental as well as architectural parameters on the ratio of heat loss from the aforementioned spaces when analyzing them under the equivalent thermal environment. The space model assumed in this study is the simplest kind, consisting of two parallel, symmetrical and infinite planes-to be called partitioned space if there exists a partition-wall between two planes parallely, and non-partitioned space unless to be so. Moreover, for evaluating the thermal environment a spherical element has been assumed in the space, of which surface-temperature accounts for indicating the thermal environment. In this paper, effects of diverse environmental and architectural parameters will be examined by means of numerical calculation, first of all, on the heat loss ratio of partitioned and non-partitined spaces. Then the critical convective heat transfer coefficient (α_<cg>)_<cr>, that is between the walls and air in the space, will be introduced as an index to grade the energy savings which is due to the existance of partition-wall in the space. When comparing the partitioned and non-partitioned spaces from the energy conservation points of view, there exist two distinguishable zones before and after (α_<cg>)_<cr>. One zone accounts for the values of α_<cg> less than (α_<cg>)_<cr> in which non-partitined space indicates the lesser energy loss. Another zone accounts for the values of α_<cg> greater than (α_<cg>)_<cr> in which the partitioned space shows tendency towards the energy savings- when warming up the space. This (α_<cg>)_<cr>, has found to be proportional to α_<cs>/ε_s where α_<cs> is the convective heat transfer coefficient and ε_s is emissivity of the spherical element, whereas it follows the changes of emissivity of the internal surface of the exterior wall ε_g through a quadratic function which has been approximated by means of numerical calculation. Besides, other than α_<cs>, ε_s and ε_g effects of the other parameters may be summerized as follows. Convective heat transfer coefficient in the vicinity of partition-wall α_<cp>, emissivity of partition-wall ε_p and the overall heat transfer coefficient of the exterior walls have no effect on the value of (α_<cg>)_<cr>, though they certainly impose distinct changes upon the heat loss ratio of partitioned and non-partitioned spaces. However internal heat production and surface-temperature of shperical element as well as ambient temperature not only do not influence the value of (α_<cg>)_<cr> but also have no essential effect on the ratio of heat loss. Nevertheless, it seems necessary to mention here that, although the space models applied in this study differs comparatively from the actual ones, the results concluded in this paper can be reasonably accepted on a qualitative basis. Thus, as a matter of course, they have to be similarly examined on some model analogous to the existing spaces in order to be confirmed quantitatively as well.
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