F L O W D E N S I T Y Amalor – J Orillo R E L A T I O N S H I P S GENERAL EQUATION: q = kūs WHERE: q = FLOW k = DENSITY ūs = SPACE MEAN SPEED Other relationships that exist among the traffic flow variables are: _ k = qt WHERE: q = FLOW k = DENSITY t = TRAVEL TIME FOR UNIT DISTANCE GENERAL EQUATION: q = kūs WHERE: q = FLOW k = DENSITY ūs = SPACE MEAN SPEED Other relationships that exist among the traffic flow variables are: _ _ t dk==ūq h s WHERE: d AVERAGE SPEED q = FLOW k = DENSITY HEADWAY t = TRAVEL TIME FOR SPACE MEAN UNIT ūs =DISTANCE SPEED h = AVERAGE TIME HEADWAY GENERAL EQUATION: q = kūs WHERE: q = FLOW k = DENSITY ūs = SPACE MEAN SPEED Other relationships that exist among the traffic flow variables are: __ ___ dh==ūds h t WHERE: WHERE: d = AVERAGE SPEED d = AVERAGE SPEED HEADWAY HEADWAY t = AVERAGE TRAVEL ū = SPACE MEAN TIME s FOR UNIT SPEED DISTANCE h = AVERAGE TIME h = AVERAGE TIME HEADWAY HEADWAY Fundamental Diagram of Traffic Flow 1. When the density on the highway is 0, the flow is also 0 because there are no vehicles on the highway. 2. As the density increases, the flow also increases. 3. When the density reaches its maximum, generally referred to as the jam density (kj), the flow must be 0 because vehicles will tend to line up end to end. 4. It follows that as density increases from 0, the flow will also initially increase from 0 to a maximum value. Further continuous increase in density will then result in continuous reduction of the flow, which will eventually be 0 when the density is equal to the jam density. SHOCK WAVES IN TRAFFIC STREAMS Types of Shock Waves Frontal stationary shock waves ↳ Formed when the capacity suddenly reduces to zero at an approach or set of lanes having the red indication at a signalized intersection or when a highway is completely closed because of a serious incident. ↳ For example, at a signalized intersection, the red signal indicates that traffic on the approach or set of lanes cannot move across the intersection, which implies that the capacity is temporarily reduced to zero resulting in the formation of a frontal stationary shock wave as shown in Figure Backward forming shock waves ↳ Formed when the capacity is reduced below the demand flow rate resulting in the formation of a queue upstream of the bottleneck. The shock wave moves upstream with its location at any time indicating the end of the queue at that time. Rear stationary and forward recovery shock waves ↳ Formed when demand flow rate upstream of a bottleneck is first higher than the capacity of the bottleneck and then the demand flow rate reduces to the capacity of the bottleneck. ↳ For example, consider a four-lane (one direction) highway that leads to a two-lane tunnel in an urban area as shown in Figure. ↳ During the off-peak period when the demand capacity is less than the tunnel capacity, no shock wave is formed. Rear stationary and forward recovery shock waves ↳ This shock wave continues to move upstream of the bottleneck as long as the demand flow is higher than the tunnel capacity as shown in Figure. ↳ At this point, a rear stationary shock wave is formed until the demand flow becomes less than the tunnel capacity resulting in the formation of a forward recovery shock wave as shown in Figure.