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Fire ventilation

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The hydrodynamic pressure difference between point 1 and point 3 is:<br />

v 1 = 0 ρ 1 = ρ 3 = ρ g h 1 = h 3 = h u<br />

ρ 3v 2<br />

3<br />

P 1– P 3 = −−−−−<br />

2<br />

ρgv g 2<br />

ΔP u = −−−−− Equation 2<br />

2<br />

We can obtain the speed through the upper opening by using the equations<br />

1 and 2:<br />

ρ gv 2 g<br />

−−−−− = h u g (ρ a− ρ g)<br />

2<br />

32<br />

√<br />

2h ug(ρ a–ρ g)<br />

vg = −−−−−−−−−−− Equation 3<br />

ρg The relationship between temperature and density is given by the gas law, and<br />

we can use this to determine the relationship between the density and temperature.<br />

At normal atmospheric pressure we obtain the relationship:<br />

ρPM = RT gas law<br />

P = 101.3 kPa normal atmospheric pressure<br />

M = 0.0289 kg/mol molar density for air<br />

R = 8.314 J/Kmol gas constant<br />

353<br />

ρ = −−−−− relationship between density and<br />

T<br />

temperature<br />

The mass fl ow in the opening is given by m˙ = CdAvρ By doing the same thing for the fl ow into the lower opening and equalising<br />

the obtained expression with equation 3, an expression is obtained for the<br />

position of the neutral plane in relation to the size of the openings:<br />

hn Au 2<br />

ρg −−− = −−− × −−−− Equation 4<br />

hu An ρa

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