1.1. Historical Development of Fire Modeling
Amongst the many incidents of uncontrollable fires, unwanted fires in enclosures are the most frequently encountered. Significant examples of some major fire disasters recorded in history are the Kings Cross Fire in the London Underground, which occurred on 18 November 1987, and the collapse of the World Trade Center Towers in New York on 11 September 2001. The hazard that these fires represent is usually associated with the uncontrolled nature of the exothermic chemical reactions, especially between organic or combustible materials and air and their interaction with the structural components. What follows from the analysis of this fire hazard is that it cannot, in general, be totally eliminated, but it can be reduced to an acceptably low level via appropriate design considerations and procedures.
Fire dynamics embraces numerous complicated physical and chemical interactions, which include fluid dynamics, thermodynamics, combustion, radiation, or even multi-phase effects. During the early investigations of enclosure fire development, a great deal of attention has been focused on better understanding the fire behaviors using experimental techniques and theoretical approaches. Experiments provide useful observations and measurements of the flaming process, while theoretical models employ a mathematical description of the physical phenomena through the input of experimental data. There are, however, limitations in fully applying experimental techniques and theoretical approaches to a range of fire problems. Conducting full-scale experiments can be rather expensive due to the high costs of construction of a fire facility and the instrumentation and hardware required for data collection. On the other hand, in spite of the low computational costs associated with the use of theoretical approaches, these models are still highly dependent on the experimental data from which they are correlated and the specific geometrical configuration where the fire experiments are carried out.
With the advent of digital computers, the use of numerical methodologies in fire modeling offers fire modelers the flexibility of aptly simulating the fire behaviors in different enclosure configurations, hence overcoming the constraints in experimental techniques and theoretical approaches. There are essentially two major categories of computer models for analyzing enclosure fire development. The first category is the stochastic or probabilistic models, which treat the fire growth as a series of sequential events or states. Here, mathematical rules are established to govern the transition from one event to anotherâfor example, from ignition to established burningâand probabilities are assigned to each transfer point based on the analysis of relevant experimental data, historical fire incident data, and computer model results. The second category, which is the primary focus of this book, is the deterministic models. Through these models, the processes encountered in a compartment fire are represented by interrelated mathematical expressions based on physics and chemistry. Generally speaking, these modelsânormally known as room fire, computer fire, or mathematical fire modelsâcan provide an accurate estimate of the impact of fire and, more importantly, suggested measures for fire prevention or control.
In fire modeling, the most widely used physically based fire model is the âzoneâ or âcontrol volumeâ model. Zone modeling has proven to be a practical methodology in providing estimates to the fire processes in enclosure. Essentially, it solves the conservations equations for distinct and relatively large control volumes. On the basis of the âTwo Layers Assumption,â the dominant characteristic of this type of model is exemplified in
Figure 1.1. The zone model assumes that the burn room is divided into two layers (i.e., the upper layer of hot gases and the bottom layer of cold gases). Within the enclosure, the hot layer contains all the combustion products, which are taken to be well mixed and homogenous in temperature, while the cold layer is filled with the entrained ambient air. The transient layer height and temperature change (i.e., h
L and T
L) are calculated by considering the global conservation of mass and energy. Invoking the mass conservation, the mass accumulated in the hot layer
is given by
where
is the mass flow rate of the combustion products from the plume entering the hot layer and
is the mass flow rate of the exhausting hot gases. Similarly, the net energy gain in the hot layer
through applying the energy conservation is calculated according to
where
is the energy gain due to the exothermic chemical reaction between the fuel and air,
is the energy loss to the surroundings, and
is the energy loss due to the convective heat transfer to the boundaries of enclosure.
The beginnings of zone modeling can be traced back to the mid-1970s with the description of the fundamental equations in Quintiere (1977). Based on these equations, the very first zone model published was RFIRES by Pape et al. (1981). This was followed by the Harvard series of models developed by Emmons, Mitler, and co-workers (Mitler and Emmons, 1981, Mitler and Rockett, 1987), ASET model and ASET-B model in Walton (1985), FPETOOL, a descendant of the FIREFORM model, by Nelson (1986, 1990), CFAST model from the National Institute of Standards and Technology (NIST) as reported in Peacock et al. (1993), and a variety of other different models (Babrauskas, 1979, Davis and Cooper, 1991). The development of these zone models has been facilitated by advancements both in the understanding of the basic physics of fire growth in a compartment and in the computational technology. While most of the zone models are based on the same fundamental principals, significant variation in features exists among these modelsâsingle-room or multi-room enclosure, sprinkler/detector activation, smoke filling through openings, and many others. As aforementioned, typical model outputs of the zone models are the prediction of the evolution of the gas temperatures (TL) and the thickness of the upper smoke layer (hL). Comprehensive investigations on the use of zone models to specific fire problems can be found in Friedman (1991), Cox (1995), Walton (1995), and Novozhilov (2001).
Although zone models have been widely adopted and have demonstrated considerable success, they still remain a prescriptive approach to fire modeling. These models generally require the necessity of a priori knowledge of the flow pattern and the vanishing of the local effect within the two zones. In spite of their ease of usage, they are very likely to be imprecise in predicting fire scenarios where the empirical correlations are breachedâfor example, fires that have restricted entrainment areas or irregular geometrical structures. Owing to global averaging that is performed on the variables of interest over the two zones within the computational domain, these models are generally unable to predict the local physical quantities as required. The field model, an alternative to deterministic modeling, improves the spatial resolution of the zone model by further dividing the computational domain into a three-dimensional mesh comprised of many tiny cells. Field modeling of fires calculates changes in each cell by using the fundamental equations of fluid dynamics. They consist generally of a set of three-dimensional, time-dependent equations, non-linear partial differential equations expressing the conservation of mass, momentum, and energy. This process of solving the fundamental dynamics with digital computers is commonly referred as Computational Fluid Dynamics (CFD). Field model calculates the physical conditions in each cell, which results from changes in adjacent cells. In hindsight, the ability to simulate a range of fire scenarios without the limitations associated with empirical correlations and the feasibility of accommodating complex geometries represent some of the many advantages that the field model has over the zone model. Owing to the evolution of computer technology, there have been intensifying activities toward the concerted development of CFD-based fire models. The enormous contribution of CFD in fire modeling is reviewed in the next section.