Abstract

To study the impact of traffic sign on pedestrian walking behavior, the paper applies cellular automaton to simulate one-way pedestrian flow. The channel is defined as a rectangle with one open entrance and two exits of equal width. Traffic sign showing that exit is placed with some distance in the middle front of the two exits. In the simulation, walking environment is set with various input density, width of exit, width and length of the channel, and distance of the traffic sign to exit. Simulation results indicate that there exists a critical distance from the traffic sign to exit for a given channel layout. At the critical distance, pedestrian flow fluctuates. Below such critical distance, flow is getting larger with the increase of input density. However, the flow drops sharply when the input density is over a critical level. If the distance is a little bit further than the critical distance, the largest flow occurs and the flow can remain steady no matter what input density will be.

1. Introduction

Pedestrian’s walking behavior is much more complicated compared with the vehicle traffic due to the fact that there is no designated trail to constrain pedestrians’ moving space. However, we still need to understand and predict such behavior very well to conduct sound evacuation management in emergency or to keep pedestrian facility in good operation.

In the past several decades, modeling pedestrian flow has attracted considerable attention and numerous models were proposed. Normally, pedestrian models can be in a macroscopic nature or microscopic nature. Macroscopic models are often in the form of partial differential equations. Instead of describing individual pedestrian’s behavior, this type of models treats crowd as a whole and applies the conservation law to capture the relationship among speed, flow, and density of pedestrian flow. Applying conservation law, Hughes [1] derived partial differential equations for flows with single or multiple pedestrian types. How to solve Hughes’ model has been attracted by many researchers thereafter [2, 3]. Colombo and Rosini [4] proposed another type of partial differential equation model for pedestrian flow with a new parameter called characteristic density that revealing the maximal density in panic. Jiang et al. [5] developed an extended reactive dynamic user equilibrium model for pedestrian counter flow. Some phenomena such as lane formation in crowd were observed in numerical simulation. Another model proposed by Jiang et al. is a two-dimension high-order macroscopic model derived from fluid dynamics. Simulation results showed capability of the model to describe complex phenomena such as stop-and-go waves [6]. Henderson [7] took pedestrian in crowd as gas molecules and applied the Maxwell-Boltzmann theory to describe the velocity distribution of people movements. Without using the conservation assumptions in Henderson's study, Helbing [8] developed a fluid dynamic model for the collective movement of pedestrians based on the Boltzmann-like approach.

Microscopic pedestrian model can be described in detail as the interactions among pedestrians, or between pedestrians and obstacles. Those models include, among others, cellular automaton (CA) model [916], lattice gas model [1721], social force model [22], centrifugal force model [23, 24], floor field model [25, 26], and other rule-based models [2732]. In CA models, the walking space is set as a two-dimensional system and divided into cells. Each cell can either be empty, occupied by exactly one pedestrian, or occupied by wall or obstacle. For each time-step, pedestrian can move to adjacent cells or stand still complying with the route choice rule and conflicting with the avoidance rule. In recent years, CA models are widely used for capturing pedestrian walking behaviors, such as bidirection movement [9, 10], counter flow with paired pedestrians [11], movement with right-moving preference [12, 13], counter flow with different velocities [14], impact of surrounding environment [15], and teaming-moving impact [16]. Nagatani [9] presented a bidirectional CA model for facing pedestrian flow on a wide passage. It was found that the dynamical phase transitions occurred at three stages with increasing density. Blue and Adler [10] simulated three bidirectional pedestrian flows, including flows in separated lanes, interspersed flow, and dynamic multilane flow. Results showed that the emergent fundamental parameters of speed, flow, and density produced from the model were reasonable compared with field data. Xiong et al. [11] simulated walking behavior with paired pedestrians. Considering right-hand side walking preference, Fang et al. [12] studied bidirectional pedestrian movement. Results indicated that the critical density when phase transition occurred increased as the probability of backstepping rose, and the critical density declined with the increase of the system size. Yang et al. [13] concluded that right-preference was effective when the density was below critical value. Weng et al. [14] simulated pedestrian counterflow with different walk velocities through updates at different time-step intervals. Simulation results revealed three phases of pedestrian patterns, including freely moving phase, lane formation phase, and perfectly stopped phase. Considering the impact of surrounding environment on pedestrian flow, Yu and Song [15] introduced interaction radius parameter to route choice rules. It concluded that the critical entrance density at the transition point did not depend on the system size when the radius was large. Wang et al. [16] revealed that team-moving could significantly influence corridor capacity by means of teaming manner.

Pedestrian’s walking behavior is affected by many factors including walker’s characteristic and walking channel environment. Among these factors, traffic sign is a key impact factor to those who are not familiar with the walking environment. A case study showed that pedestrian walking behavior was affected by content and position of the sign [33]. According to a questionnaire survey we conducted, as high as 97.4% (74 of 76) subway riders reported that traffic sign showing exit were helpful and they would change their moving direction accordingly in an unfamiliar station. Liu et al. [34] proposed a computational model for determination of the effective distance of emergency evacuation signs. Nassar [35] proposed an optimization framework for signs location to increase their detectability in public space. The aim of this paper is to study the impact of traffic sign on pedestrian behavior by means of CA model.

The paper is structured as follows. Section 2 develops the cellular automaton model and defines walking rules for pedestrians with traffic sign in system. Section 3 applies the model to simulate pedestrian movement in various scenarios. In this section, some meaningful phenomena relating to the function of traffic sign are studied. The conclusions are presented in Section 4.

2. Model

We apply a two-dimensional cellular automaton to define the walking channel. The underlying structure is a cell grid, where is the width of the channel and is the length of the channel. The entrance is at the left with width of , and two exits, denoted by and , are at the right boundary with equal width of . Each cell can either be empty or occupied by wall, obstacle, or exactly one pedestrian. The size of a cell is set to be  m2. This is a typical space occupied by a person in a dense crowd [28]. Each pedestrian can move only one cell per time-step. In practice, the average velocity of a pedestrian is about 1.0 ms−1 under normal circumstances [29]. So the time-step is approximately 0.4 s.

The channel is illustrated in Figure 1. In Figure 1(a), there is no traffic sign and pedestrians can recognize exits only when they crossed the dashed line in area . In Figure 1(b), we set traffic sign in the middle front of the two exits. Pedestrians who are in area can see the traffic sign pointing at the proper exit.

Two types of walkers are taken into account: walkers who take exit and walkers who take exit . The numbers of the two types of walkers entering from the left entrance are equal. The channel is confined with walls at top and bottom boundaries. Anyone can walk only from left to right, but no one can cross the top or bottom boundaries.

Taking pedestrians who are choosing exit for example, there are three typical positions for each pedestrian; see Figure 2. With traffic sign, pedestrian and pedestrian are in the area with impact of traffic sign, whereas pedestrian is out of such area. In this case, and keep walking forward and will adjust its direction to get close to exit . Probability of a pedestrian moving forward is denoted by , and probabilities of moving left forward, right forward, and left are denoted by , , and , respectively.

The update is random sequential for all pedestrians at every time-step. Usually a parallel update rule is considered to be more realistic, but it might lead to conflicts in the update [36]. Figure 3 shows all the possible configurations that pedestrians and may encounter. If the front adjacent cells are not totally occupied, the probabilities to move forward, left forward, and right forward are determined by the angle between moving direction and the horizontal line. In Figure 3(a), if all front cells are empty, the walker will select the one of the three front cells with probability denoted by , , and , where , , and are expressed as , is normalization parameter to assure , and is angle between moving direction and the horizontal line. In Figure 3(b), if both the upper cell and the front cell are free, the walker will select any of the two cells to move in with probability or . For configuration (c), the probability of selecting the left, right adjacent cell or waiting is denoted by , , and , respectively, where . For configuration (d), the probability of selecting the right adjacent cell or waiting is and , respectively, where . For configuration (e), the probability of selecting the left rear, right rear, back adjacent cell, and waiting is denoted by , , , and , respectively, where . For configuration (f), the probability of selecting the left rear or back adjacent cell or waiting is denoted by , , and , respectively, where .

Figure 4 shows all the possible configurations that pedestrian may encounter. In Figure 4(a), if all front cells are empty, the walker will select the one of the three front cells with probability denoted by , , and , where , , and are expressed as , is normalization parameter to assure , and is angle between moving direction and the horizontal line. In Figure 4(b), if the front cell is occupied, the walker will select the left or left front cell to move in with probability or . For configuration (c), the probability of selecting the left rear, right front adjacent cell, or waiting is , , and , respectively, where . For configuration (d), the probability of selecting the right front adjacent cell or waiting is and , respectively, where . For configuration (e), the probability of selecting the rear, right rear, right adjacent cell, or waiting is , , , and , respectively, where . For configuration (f), the probability of selecting the right rear, right adjacent cell, or waiting is , , and , respectively, where .

3. Simulation and Results

To study the impact of traffic sign on pedestrian walking behavior, we analyze changes of pedestrian flow with various input density, impact area of the sign, and channel configuration. Pedestrian flow is defined as the number of pedestrians crossing the right boundary at each time-step. Input density is defined as the number of entering pedestrians at each time-step over the width of the channel. Input density is set as a constant in each scenario. Impact distance is defined as the furthest distance for a pedestrian to recognize the traffic sign, denoted as in Figure 1(b). At the very beginning, the channel is empty. For each simulation, total 150,000 time-steps are carried out, and the value of averaged flow is calculated according to the results of the last 5,000 time-steps. We take the average of the 10 iteration results as the final value.

Pedestrians are assumed to recognize the sign as soon as they stepped into the impact area. Simultaneously, they started to adjust moving direction towards the preferred exit. Kretz et al. [37] analyzed such psychological act in a tunnel fire simulation. For the sake of simplicity, we ignored decision process from cognition to perception. In simulation, the height of a pedestrian is not considered, which means the front pedestrian will never block the sight of the follower.

Figure 5 shows pedestrians’ moving state with impact of traffic sign at different distances. It shows that, with impact distance of 10 cells, pedestrians are blocked in front of the exits. Those who are aiming at taking exit are blocked in front of exit and vice versa. In this case, no one can get out of the channel. If we set impact distance at a further distance, say 30 cells, pedestrian can recognize his/her exit in advance and adjust the moving direction accordingly within the space to the exit. The further we set the traffic sign to the exits, the earlier pedestrians recognize the proper exit, and the easier it is to move out of the channel.

In Figure 6 we show relationship between flow and input density with different exit width or different impact distance. If we set the impact distance as 10 cells and input density as 0.1, pedestrian flow will be about 2.0 no matter what width of the exit we set. But with input density of 0.2 or larger, the flow decreases dramatically to 0. On the other hand, if we set impact distance further and further, we can see that with the same input density, flow is getting lower and lower. It indicates that, in real world, traffic sign should be set at an appropriate distance to exit. It is of no use to set traffic sign too far or too close to the exits.

We can see the fluctuation of flow versus input density. In reality, flow is influenced by input density, width of the channel and exits, location of the sign, and so on. Pedestrians tried to change moving direction when they noticed the sign. In some circumstances, pedestrians blocked each other. Such situation is well described by the asymmetric simple exclusion process (ASEP) [3841].

To study impact of the exit width on the relationship between flow and impact distance, we conduct simulation with input density as 0.5 and the length of channel as 80 and the width as 30. It is clear that the further the traffic sign is, the larger the flow is within a critical distance. Beyond such distance, flow is getting less and less with increase of the distance. No matter whether the width is 5 or 7, the largest flow occurs under the condition that impact distance is equal to 30. If we enlarge the width of the exit to 10, we find the largest flow occurs when impact distance equals 40. It concludes that the largest flow occurs when impact distance is equal to or a little bit larger than the channel width. See Figure 7.

Figure 8 shows relationship between flow and input density with various channel lengths. The channel width is set as 30 cells and the length is 60 in Figure 9(a) and 100 in Figure 9(b), respectively. Simulation results show that pedestrian flow remains unchanged with variation of channel length.

To study impact of channel width and traffic sign impact distance on the relationship between flow and input density, we conduct simulation with channel length of 80 cells and exit width of 7 cells. Channel width is set as 20 and 40 cells corresponding to Figures 9(a) and 9(b), respectively. Results show that the largest flow occurs on condition that the width of exit is less than half of the channel width and d is not less than the channel width if the input density is high. This conclusion agrees with results we have got in Figure 7.

To further study the impact of channel size on flow characteristics, we conduct simulation experiments with different channel sizes.

Setting the width of the channel as 40 cells and the width of each exit as 10 cells, we notice that flow fluctuates when impact distance is 40 cells far from the boundary. See Figure 10. It demonstrates that a critical distance for traffic sign exists. At this distance, pedestrian flow will fluctuate, and, below which, the flow will drop sharply with the increase of input density. With the same input density, the largest flow can only occur on condition that d is a little bit further than the channel width.

Figures 11(a) and 11(b) are two states in such condition we set above. In Figure 11(a), pedestrians can recognize the exits and move freely to the forward direction, whereas, in Figure 11(b), there is a block area between pedestrians turning left and those turning right. In Figure 11(c), dead block occurs if the input density is higher than 0.2 without traffic sign.

4. Conclusion

In this paper, the impact of traffic sign on pedestrian walking behavior through a channel with two exits has been studied. The pedestrians are modeled by a cellular automaton model. Two types of pedestrians are considered according to which exit they intend to go through.

We conduct simulation experiments in various scenarios with different channel length, channel width, width of exit, input density, and impact distance. Simulation results indicate that a critical distance of the traffic sign to exit exists for a given channel layout. At the critical distance, pedestrian flow fluctuates. Below such critical distance, flow is getting larger with the increase of input density. However, the flow drops sharply if the input density is over a critical level. If the distance is a little bit further than the critical distance, the largest flow occurs and the flow can remain steady no matter what input density will be. Under some conditions in terms of the channel layout, position of traffic sign, and input density, block area between pedestrians turning left and right exists. Without traffic sign, the block area turns into a dead block with some higher input density.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The authors acknowledge the support from Beijing Municipal Natural Science Foundation with Grant no. 8092026. The authors are grateful to reviewers for the invaluable comments.