INGENIA

TRN-01

Greenshields speed–density

Linear v = vf (1 − k/kj); q has a parabolic maximum.

Reading speed
Traffic flowGreenshields 1935HCM

Governing equation

v=vf(1−kkj),q=kv,qmax⁡=vfkj4v=v_f\left(1-\dfrac{k}{k_j}\right),\quad q=kv,\quad q_{\max}=\dfrac{v_f k_j}{4}

k∈[1,200]k \in \left[1, 200\right]

where

v_f
Free speed (km/h)
k_j
Jam density (veh/km)
k
Density (veh/km)
v
Speed (km/h)
q
Flow (veh/h)
q_{\max}
Capacity (veh/h)

The figure, part by part

Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.

TRN-01 · curve
00:0 / 00:08
①

Governing law — red

v=vf(1−kkj),q=kv,qmax⁡=vfkj4v=v_f\left(1-\dfrac{k}{k_j}\right),\quad q=kv,\quad q_{\max}=\dfrac{v_f k_j}{4}

k∈[1,200]k \in \left[1, 200\right]

k=1k = 1v=99.29v = 99.29

②

Domain of the variable — blue

kmin⁡=1,kmax⁡=200k_{\min} = 1,\quad k_{\max} = 200

k∈[1,200]k \in \left[1, 200\right]

k=1k = 1k=1k = 1

③

Response curve — green

v=vf(1−kkj),q=kv,qmax⁡=vfkj4v=v_f\left(1-\dfrac{k}{k_j}\right),\quad q=kv,\quad q_{\max}=\dfrac{v_f k_j}{4}

k∈[1,200]k \in \left[1, 200\right]

k=1k = 1v=99.29v = 99.29

④

Rate of change — amber

dvdk\frac{\mathrm{d}v}{\mathrm{d}k}

k∈[1,200]k \in \left[1, 200\right]

k=2.252k = 2.252v′=96.78v^{\prime} = 96.78

Lecture brief

Historical brief

Highway and traffic theory crystallized with Greenshields’ 1935 speed–density line, then AASHTO stopping sight and equivalent axles. The lab is that operational arithmetic of flow, braking and pavement load. This sheet (TRN-01 — Greenshields speed–density) is the form associated with Greenshields 1935 · HCM. Working symbols: vfv_f, kjk_j, kk →\rightarrow vv, qq, qmax⁡q_{\max}. Greenshields postulated a linear drop of speed with density. Flow q = k v then peaks at k = kj/2 with qmax = vf kj / 4.

Purpose

Purpose: compute vv, qq, qmax⁡q_{\max} from vfv_f, kjk_j, kk in Transport via v=vf(1−kkj),q=kv,qmax⁡=vfkj4v=v_f\left(1-\dfrac{k}{k_j}\right),\quad q=kv,\quad q_{\max}=\dfrac{v_f k_j}{4} Linear v = vf (1 − k/kj); q has a parabolic maximum. Use it when a real transport question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given vf=100.000 km/hv_f = 100.000\,\mathrm{km/h}, kj=140.000 veh/kmk_j = 140.000\,\mathrm{veh/km}, k=40.000 veh/kmk = 40.000\,\mathrm{veh/km}, the governing relation v=vf(1−kkj),q=kv,qmax⁡=vfkj4v=v_f\left(1-\dfrac{k}{k_j}\right),\quad q=kv,\quad q_{\max}=\dfrac{v_f k_j}{4} yields v=71.429 km/hv = 71.429\,\mathrm{km/h}, q=2857.143 veh/hq = 2857.143\,\mathrm{veh/h}, qmax⁡=3500.000 veh/hq_{\max} = 3500.000\,\mathrm{veh/h}. Single homogeneous lane, no ramps. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Speed v71.429 km/h
  • Flow q2857.143 veh/h
  • Capacity q_{\max}3500.000 veh/h
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TRN-01 · curve
00:0 / 00:08

Narration of this film

Single homogeneous lane, no ramps.

Greenshields postulated a linear drop of speed with density. Flow q = k v then peaks at k = kj/2 with qmax = vf kj / 4.

Reading speed

Watch on YouTube