We’re sorry, something doesn't seem to be working properly.

Please try refreshing the page. If that doesn't work, please contact support so we can address the problem.

Skip to main content
Log in

Using FDS to Simulate Smoke Layer Interface Height in a Simple Atrium

  • Published:
Fire Technology Aims and scope Submit manuscript

Abstract

This study examines the possible effects of various make-up air supply arrangements and velocities in an atrium smoke management system. Variations include velocities ranging from 0.5 to 3.0 m/s. The arrangement of make-up air supply injection points include symmetrically located vents placed low in the spaced, an array of vents distributed from the floor to the ceiling, and asymmetrically located vents. Fire Dynamic Simulator version 4.06 is applied to simulate ten scenarios in a 30.5 m cubical domain with a fire source simulating a stack of pallets with an approximate peak heat release rate of 5 MW. Results show that make-up air supply velocities should be diffused such that little to no velocity effects reach the fire. Make-up air should be supplied to the fire symmetrically for the best chance of not disturbing the fire plume. Disturbing the fire and smoke plume results in a significant increase in the smoke production rate, as evidenced by a deeper smoke layer.

We’re sorry, something doesn't seem to be working properly.

Please try refreshing the page. If that doesn't work, please contact support so we can address the problem.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Institutional subscriptions

Figure 1.
Figure 2.
Figure 3.
Figure 4.
Figure 5.
Figure 6.
Figure 7.
Figure 8.
Figure 9.
Figure 10.
Figure 11.
Figure 12.
Figure 13.
Figure 14.
Figure 15.
Figure 16.
Figure 17.
Figure 18.
Figure 19.
Figure 20.
Figure 21.
Figure 22.
Figure 23.
Figure 24.
Figure 25.
Figure 26.
Figure 27.
Figure 28.
Figure 29.
Figure 30.
Figure 31.
Figure 32.

Similar content being viewed by others

References

  1. J.A. Milke, “Smoke Management in Covered Malls and Atria,” SFPE Handbook of Fire Protection Engineering, 3rd edn., P.J. DiNenno (ed.), National Fire Protection Association, Quincy, MA, 2002.

    Google Scholar 

  2. NFPA 92B, Standard for Smoke Management Systems in Malls, Atria, and Large Areas. National Fire Protection Association, Quincy, MA, 2005.

    Google Scholar 

  3. G. Heskestad, “Engineering Relations for Fire Plumes,” Fire Safety Journal, vol. 7, 1984, pp. 25–32.

    Article  Google Scholar 

  4. C. Beyler, “Fire Hazard Calculations for Large, Open Hydrocarbon Fires,” SFPE Handbook of Fire Protection Engineering, 3rd edn., P.J. DiNenno (ed.), National Fire Protection Association, Quincy, MA, 2002.

    Google Scholar 

  5. K.B. McGrattan and G.P. Forney, 2004a, Fire Dynamics Simulator—User's Manual, National Institute of Standards and Technology, NIST Special Publication 1019, Gaithersburg, MD, 2004.

  6. K.B. McGrattan, H.R. Baum, R.G. Rehm, A. Hamins, and G.P. Forney, “Fire Dynamics Simulator – Technical Reference Guide,” National Institute of Standards and Technology, NIST Special Publication 1018. Gaithersburg, MD, 2004.

    Google Scholar 

  7. G.P. Fourney and K.B. McGrattan, “User's Guide for Smokeview Version 4—A Tool For Visualizing Fire Dynamics Simulator Data,” National Institute of Standards and Technology. NIST Special Publication 1017. Gaithersburg, MD, 2004.

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to James A. Milke.

Additional information

1. Growth time refers to the time required for the heat release rate of the fire to increase to 1055 kW. The 150 s growth time is in the middle of the range of growth times noted in NFPA 92B for 1.5 m high stacks of pallets [2].

2. For the purpose of this paper, a ‘peak’ heat release rate is determined based on the maximum sustained heat release rate, neglecting the instantaneous spikes of the heat release rate.

Appendix A: Detailed Calculations

Appendix A: Detailed Calculations

Figure 33.
figure 33

Asymmetric vs. corner vent heat release rate at 2.0 m/s.

$$ \displaylines{ \dot m = C_1 Q_c^{1/3} z^{5/3} + C_2 Q_C \cr \dot m = 0.071(3500)^{1/3} (22.6)^{5/3} + 0.0018(3500) \cr \dot m = 201.0\,{\rm kg}/{\rm s} \cr T_p = T_a + \frac{{Q_c }}{{\dot mc_p }} \cr T_P = 20 + \frac{{3500}}{{201.0(1.0)}} \cr T_P = 37.4^\circ {\rm C} = 310.6\,{\rm K} \cr \rho _p = \frac{{352.8}}{{T_p }} \cr \rho _P = \frac{{352.8}}{{310.6}} \cr \rho _P = 1.14\,{\rm kg}/{\rm m}^3 \cr \dot V = \frac{{\dot m}}{{\rho _p }} \cr \dot V = \frac{{201.0}}{{1.14}} \cr \dot V = 176.3\,{\rm m}^3/{\rm s} \cr \dot V_i = \frac{{\dot m}}{{\rho _{amb} }} \cr \dot V_i = \frac{{201.0}}{{1.1}} \cr \dot V_i = 182.7\,{\rm m}^3/{\rm s} \cr v = \dot V_i /A_v \cr A_v = \frac{{182.7}}{{1.0}} \cr A_v = 182.7\,{\rm m}^2} $$

Rights and permissions

Reprints and permissions

About this article

Cite this article

Kerber, S., Milke, J.A. Using FDS to Simulate Smoke Layer Interface Height in a Simple Atrium. Fire Technol 43, 45–75 (2007). https://doi.org/10.1007/s10694-007-0007-7

Download citation

  • Received:

  • Accepted:

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/s10694-007-0007-7

Keywords

Navigation