Abstract
Fires with a heat release rate that grows quadratically in time and levels off after the first automatic fire sprinkler is activated are routinely used in evaluating the consequences of fire in performance based design projects. In order to calculate the sprinkler activation time one needs to solve the differential equation that governs the heat transfer between the ceiling jet and the sensing element of the automatic fire sprinkler, an equation that depends on the temperature and velocity of the gas. Well-known empirical correlations between ceiling jet properties and heat release rate as well as numerical simulations can be used to determine the temperature and velocity of the gas. Here a comparison and discussion of the results obtained for the activation time and activation heat release rate using both approaches is presented, which can help authorities having jurisdiction to assess safety reports when there are no clear regulations about which method should be applied.
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Notes
For a viscous fluid the velocity must vanish on the ceiling and hence there must be a maximum at a short distance from the ceiling. To resolve the maximum in a simulation one should take cell sizes smaller than 5 cm, which is beyond the scope of this work.
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Appendix A Models Simulated with FDS
Appendix A Models Simulated with FDS
The geometry simulated with FDS is that of a \(16\times 12\times 6\) m\(^3\) room without lateral walls (open boundaries) and with a flat ceiling. The fire is located on a \(4 \times 4\) m\(^2\) platform raised from the floor between 0.5 m and 3.0 m. That provides a H changing from 3.0 m to 5.5 m. Using the constant HRRPUA method we have simulated a total of 16 models shown in Table 5, for every fuel. Using the constant surface method we have simulated as well a total of 16 models shown in Table 6, for every fuel. Finally Table 7 shows the combustion reaction properties.
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Toldrà, R. Automatic Fire Sprinkler Activation Time with Quadratic Fire Growth. Fire Technol 59, 2645–2666 (2023). https://doi.org/10.1007/s10694-023-01441-4
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DOI: https://doi.org/10.1007/s10694-023-01441-4