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An automatic fire searching and suppression system for large spaces

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ARTICLE IN PRESS<br />

298<br />

T. Chen et al. / Fire Safety Journal 39 (2004) 297–307<br />

Nomenclature<br />

D chamber length of the <strong>fire</strong> monitor<br />

d measured distance between a <strong>fire</strong> <strong>and</strong> the pivot point of the <strong>fire</strong> monitor<br />

d c calculated distance between a <strong>fire</strong> <strong>and</strong> the pivot point of the <strong>fire</strong> monitor<br />

f focal length of the CCD camera<br />

e distance between a <strong>fire</strong> <strong>and</strong> the shooting spot of the <strong>fire</strong> monitor<br />

(i 1 , j 1 ) pixel coordinates of a <strong>fire</strong> in the image at time t 1<br />

(i 2 , j 2 ) pixel coordinates of a <strong>fire</strong> in the image at time t 2<br />

H maximum pixel number per row of the CCD<br />

h actual width of the CCD<br />

T time of extinguish after the water is issued<br />

T s time of <strong>searching</strong> process<br />

V maximum pixel number per column of the CCD<br />

v actual height of the CCD<br />

X–Y–Z fixed object space coordinate <strong>system</strong><br />

X 1 –Y 1 –Z 1 camera coordinate <strong>system</strong> at time t 1<br />

X 2 –Y 2 –Z 2 camera coordinate <strong>system</strong> at time t 2<br />

(X,Y,Z) coordinates in X-Y-Z coordinate <strong>system</strong><br />

(X 1 ,Y 1 ,Z 1 ) coordinates in X 1 -Y 1 -Z 1 coordinate <strong>system</strong><br />

(X 2 ,Y 2 ,Z 2 ) coordinates in X 2 -Y 2 -Z 2 coordinate <strong>system</strong><br />

x–y image plane of the camera<br />

(x,y) coordinates in x–y image plane<br />

(x 1 ,y 1 ) coordinates in image plane at time t 1<br />

(x 2 ,y 2 ) coordinates in image plane at time t 2<br />

a angle to Z-axis in Y–Z plane of the <strong>fire</strong> spot<br />

b visual angle of the CCD camera<br />

o 1 angle to Z-axis in Y–Z plane of Z 1 -axis<br />

angle to Z-axis in Y–Z plane of Z 2 -axis<br />

o 2<br />

recent years, with the increasing <strong>large</strong> space buildings, the suitability of sprinkler use<br />

in such <strong>large</strong> space situations has been challenged.<br />

Commonly, thermally activated sprinklers are not suitable <strong>for</strong> high ceiling space<br />

use. The height of the ceiling in <strong>large</strong> space will greatly affect the sprinklers so that<br />

they cannot provide effective protection. The main problem is the activation delays<br />

of the sprinklers in <strong>large</strong> <strong>spaces</strong>, particularly high ceiling <strong>spaces</strong>. For example, even a<br />

5 MW <strong>fire</strong> on the atrium floor would not generate a smoke temperature high enough<br />

to activate the sprinklers on an atrium ceiling higher than 15 m [1, 2]. Due to the<br />

distance between the potential <strong>fire</strong> source <strong>and</strong> the sprinkler heads which are mounted<br />

near the ceiling, sprinkler activation may be too late to minimize the <strong>fire</strong> hazards or<br />

damage. Even the early <strong>suppression</strong> fast response (ESFR) sprinklers have the<br />

recommended height limit [3–5]. Moreover, the height may also affect how<br />

much water can reach the flame be<strong>for</strong>e vaporized or blown away by the <strong>fire</strong><br />

plume [6]. In those <strong>large</strong> <strong>spaces</strong> where the combustible materials are distributed

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