Mathematical Problems in Engineering
Volume 2017 (2017), Article ID 4063810, 7 pages
https://doi.org/10.1155/2017/4063810

Research Article

A Modified Floor Field Model and Pareto Optimum of Pedestrian Evacuation Efficiency

Yan Xu,¹ Li-Jun Tian,² and Gui Yong¹

¹School of Statistics and Mathematics, Inner Mongolia University of Finance and Economics, Hohhot 010070, China
²School of Economics and Management, Fuzhou University, Fuzhou 350108, China

Correspondence should be addressed to Gui Yong; nmyonggui@163.com

Received 3 December 2016; Accepted 30 May 2017; Published 27 June 2017

Academic Editor: Alessandro Gasparetto

Copyright © 2017 Yan Xu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

A modified floor field model is proposed to simulate the pedestrian evacuation behavior in a room with multiple exits. The modification relies upon introduction of a so-called semidynamical floor field which additionally embodies two cognition coefficients related to exit width and pedestrian distribution around exits. The energy consumption and time requirement of evacuees are numerically investigated and the Pareto optimum of evacuation efficiency is obtained by selecting the combinations of the two cognition coefficients.

1. Introduction

Study on pedestrian dynamics has attracted many physicists over the past few years. Various collective behaviors and self-organization phenomena have been observed from the view point of complexity of the pedestrian flow system. For understanding these phenomena, many models have been developed, for example, the social force model [1–3], the fluid dynamic model [4–9], and the cellular automata model [10–21].

The social force model is a deterministic continuum model in which the interactions between pedestrians are governed by the social force or social field [1, 2]. Using this model, such phenomena as the arching around exit, the lane formation in counter flow, and the oscillation of flow direction at narrow door can be reproduced.

The fluid dynamic model describes how density and velocity change over time with the use of partial differential equation. This model can be used to investigate exactly the dynamics at the exits during an evacuation [7] and study some typical pedestrian behaviors, for example, the “thinking fluid” behavior and the overcompression effect [8, 9].

The rule-based cellular automata model is discrete in space and time. All pedestrians are represented by particles. Such typical phenomena as arching, jamming, kin behavior, faster-is-slower, lane formation, and sidle effect can be simulated by this kind of models [10–21]. Floor field model is one kind of discrete simulation models. At each time step, every pedestrian moves from one lattice to the neighboring lattice in terms of a transition probability. This model can be used to investigate various collective effects and the self-organization encountered in pedestrian dynamics [10, 11].

Modeling the evacuation process of pedestrians in a room with multiple exits has to consider the strategy of selecting exits. In the conventional floor field models, the exit selection strategy is mainly based on the herding behavior and the use of knowledge about the shortest path to each exit [10, 11]. In some works, the occupant density around each exit is considered as an important factor affecting the exit selection strategy [15, 16]. In this paper, we improve the floor field model through introducing two cognition coefficients associated with the exit width and the pedestrian distributions around exits, respectively.

The energy consumed in evacuation process is seldom studied by previous researches. However, if a space for evacuation is large enough to make some pedestrians expend more energy than their capabilities, he or she will fail to evacuate successfully and, on the contrary, they may become obstacles to other pedestrians. In this study, we will investigate the energy consumption of evacuees besides the time requirement and find the Pareto optimum of evacuation efficiency.

2. Model

Let a space for evacuation be represented by two-dimensional square lattices. The size of each lattice is approximately  cm². Each lattice can be either empty or occupied by one pedestrian. Each time step is real time of evacuation based on different movement velocity of pedestrians. The length of one time step is 0.3 seconds in this study. This implies a walking speed of approximately 1.33 m/s.

In each time step, pedestrians move only one lattice site in the forward, backward, left, or right direction or remain unmoving. They probabilistically select a neighboring lattice site in these directions to move using the transition probability. The transition probability is computed using the static and dynamic floor fields of those lattices.

In the simulation of evacuation process, the static floor field represents the degree of attractiveness of each lattice for pedestrians. The static floor field does not evolve with time and is not changed by the presence of the pedestrians. It is often given by the value depending on the distance from the exit. The dynamic floor field represents the characteristic that pedestrians tend to follow their predecessors. This is implemented using bosons dropped by pedestrians, having their own dynamics through diffusion and decay controlled by probabilities σ and δ. The dynamic floor field is the number of bosons remaining on the cell at each time step. These two types of floor fields have been historically used as fundamental and essential components of the floor field model.

The static floor field defined above reflects the attractiveness degree of each lattice for pedestrians, but the exit width and the pedestrian distribution around exits have not been considered. These two factors should have impacts on the attractiveness of some lattices and eventually influence the movement behavior of pedestrians. For this reason, the floor field model has to be improved so as to simulate the evacuation process more precisely.

2.1. Occupant Density

The occupant density around exit is introduced to characterize the pedestrian distribution around exits in the evacuation process. The occupant density of exit m can be defined as the number of occupied cells in the effect area of exit m with radius r. The effect area is a special region around the exit. Figure 1 provides an illustration for calculating the occupant density [16]. The width of the exit is 2 cells. The effect area contains sixteen intact cells which are located within a half-round with radius of 4 cells. Five black colored cells are occupied. Thus, the occupant density of this exit is 5.

Figure 1: Illustration for calculating occupant density .

2.2. Semidynamical Floor Field

The semidynamical floor field is introduced for considering the effects of exit width and pedestrian distribution around exit. Let be the total width of all exits, the width of exit , and the total number of exits. We have .

The semidynamical floor field of lattice site to exit m is defined as

where is a lattice. is determined by the shortest distance from lattice to exit , the width of exit , and the occupant density of exit , that is,

where , is the coordinate of the nth cell of exit m. The parameter is a cognition coefficient which indicates the pedestrian’s capability of perceiving the effect of exit width. A larger value means a bigger consideration of the effect of exit width or pedestrian being more sensible to the width effect. The parameter is another cognition coefficient which indicates the pedestrian’s sensitivity to the people distribution around each exit. A larger means more consideration on the occupant density. When and , the effects of both exit width and pedestrian distribution are not considered and the semidynamical floor field is reduced to the static floor field.

2.3. Transition Probability

The transition probability from a lattice site to its neighboring lattice site toward exit , , is computed using the following:

where is a normalization factor for ensuring . and are two sensitivity parameters for scaling and , respectively. The value of can be regarded as a measure of the pedestrians’ perception about the attractiveness of each lattice site for each exit. The parameter for coupling to the dynamic field governs the tendency to follow the lead of others. A large value of implies a strong herding behavior. The parameter indicates whether the neighboring lattice is occupied or not. It equals 1 if the lattice is occupied and 0 otherwise. The parameter is related to the existence of obstacles. It is 0 if is occupied by obstacles (e.g., walls) and 1 otherwise.

2.4. Unit Energy Consumed

We use the total movement steps of all pedestrians, rather than the total evacuation time, to represent the energy consumption. This says that when a pedestrian moves to one of neighboring lattices, one unit of energy consumption is added to the counter. The average energy consumed per person is termed as unit energy consumed. These two performance indexes are generally not equivalent to each other because, in congested situation, some pedestrians may not move if their neighboring sites are occupied by others while the time is spent. In addition, if some pedestrians change the exit choice frequently in the evacuation process, the energy consumption may increase although the evacuation time is reduced.

2.5. Pareto Optimum

The multicriteria optimization method has widely been applied in designing various mechanical structures and dynamic systems. Due to the basic nature of conflict among multiple objectives, a set of compromising solutions called Pareto optima exists. The determination of this set is essential for decision-makers to understand the trade-off relationship among alternatives [21].

In this study, we use two criteria, namely, the unit energy consumed and the evacuation time, to measure the efficiency of evacuation mechanism. We investigate how the two criteria are affected by the cognition coefficients and . We certainly hope to achieve such a result that these two indexes are simultaneously minimized by optimizing the two parameters and . However, this is basically impossible as discussed in the previous subsection, and we have to turn to finding the Pareto optimum of the evacuation mechanism.

3. Simulation

Consider a special zone in a room and suppose pedestrians are randomly distributed in the zone and attempt to escape. Without loss of generality, in Figure 2, the room is discretized into cells and has four exits allocated at the centre of each wall. The width of exit n is n cells, . In the specified zone (the small square marked by dotted line, with a size cells), there are 400 pedestrians at the initial stage of the simulation.

Figure 2: Room structure.

The sensitivity parameters adopted here are and . The decay probability is and the diffusion probability . The radius of effect area is cells. We carry out 10 simulations for each set of parameters and compute the averages.

To investigate the role of each exit, the pedestrian number evacuated from each exit is shown in Figures 3 and 4, when and take different values. It can be observed from Figures 3(a)–3(d) that, for each value, with increase of value, Exits 2 and 3 are first chosen by many pedestrians and then by less ones. This is because the special zone is located closer to these two exits and pedestrians do not care much about the occupant densities around exits. A larger value means pedestrians are more sensitive to the occupant densities; as a result, some pedestrians turn to choosing exits 1 and 4. Another important finding is that the value influences the number of pedestrians evacuated from each exit, but the influence degree is not linear and monotonic.

(a)

(b)

(c)

(d)

Figure 3: Pedestrian number evacuated from each exit against cognition coefficient for different values.

(a)

(b)

(c)

(d)

Figure 4: Pedestrian number evacuated from each exit against cognition coefficient for different values.

Figure 4 shows that, with the increase of value, for each value, the numbers of pedestrians evacuated from Exits 1 and 2 decrease, the one from Exit 4 increases, and the one from Exit 3 first ascends and then descends basically. This is because in the evacuation process, the occupant density in the effect area of each exit intends to be identical and the cognitive coefficient gradually comes to play a role. Consequently, more pedestrians turn to evacuating from Exit 4 due to its width.

Figure 5 shows that the unit energy consumed monotonically increases with for each value. This verifies such a view point that the energy consumption is proportional to the attitude toward congestion degree.

Figure 5: Unit energy consumed against for different values.

Finally, we investigate the two criteria for evaluating the evacuation efficiency. Due to the conflict of the two criteria, it is difficult to find the optimal and values that simultaneously minimize the unit energy consumed and evacuation time. For solving this problem, the Pareto concept is used here. Figure 6 depicts these two indexes against combination of and values. The Pareto optimum points are , , .

Figure 6: Pareto optima between unit energy consumed and evacuation time.

4. Conclusions

In this paper, two criteria, namely, the unit energy consumed and the evacuation time, are exploited to evaluate the evacuation mechanism. The unit energy consumed is seldom mentioned by previous researchers. An improved floor field model is proposed to simulate the evacuation process in a room with multiple exits where pedestrians are distributed heterogeneously. The improvement relies on the modification to the conventional static floor field by incorporating such new factors as exit width and the pedestrian distribution around exits. Simulation results show that the evacuation capacity of each exit is sensitive to the pedestrians’ cognition to these two factors. The Pareto optima are numerically obtained, which verifies the conflict of the two criteria.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

This study was supported by the National Natural Science Foundation of China (Grants nos. 71401083, 71301028, and 71661024) and the Program for Young Talents of Science and Technology in Universities of Inner Mongolia Autonomous Region (NJYT15B06).

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