11.07.2015 Views

Book - School of Science and Technology

Book - School of Science and Technology

Book - School of Science and Technology

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Heat losses 27Temperature °C1.813.4–0.5–0.21.413.916.917.919.019.0–1.0 –1.0(a)(b)Figure 2.2 Surface <strong>and</strong> interface temperaturesbeing illustrated in part (a). In this case, the overall resistance would be made up asfollows:Outside surface, R so ˆ 0:06Brickwork (1/0:84) (210/1000) ˆ 0:25Inside surface, R si ˆ 0:12R ˆ 0:43 m 2 K/WThe temperature gradient, including the components at the surfaces, will be pro rata tothe resistances <strong>and</strong>, for inside <strong>and</strong> outside air temperatures <strong>of</strong> 21 C <strong>and</strong> 1 C, respectively,would be:Outside air to outside surface ˆ 22 (0:06/0:43) ˆ 3:1 CAcross the brickwork ˆ 22 (0:25/0:43) ˆ 12:8 CInside surface to inside air ˆ 22 (0:12/0:43) ˆ 6:1 CThe surface temperature <strong>of</strong> the brickwork inside the enclosure would thus be21 6:1 ˆ 14:9 C.The more complexcase <strong>of</strong> the curtain wall construction in the previous example is dealtwith in the same way, the surface <strong>and</strong> the interface temperatures being as shown in part(b) <strong>of</strong> Figure 2.2.ApplicationHaving established the transmittance coefficients for the various structural elementsenclosing a space, it is then possible to evaluate the conduction component <strong>of</strong> the heatrequirement. This process is best illustrated by an example.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!