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The HDM-4 speed-flow model presented in Figure 1 shows that
as flows increase, there is an increase in vehicle interactions and a decrease in speeds.
These interactions are accompanied by an increase in the frequency and magnitude of the
vehicle accelerations and decelerations. The HDM-4 congestion model is built around this
theory.
The magnitude of vehicle interactions are to be represented
in HDM-4 by the acceleration noise, i.e. the standard deviation of acceleration. The total
acceleration noise for a vehicle can be considered to be comprised of the following two
components:
a =
where a is the total acceleration noise in m/s2
at is the noise due to fast-moving vehicle interactions in
m/s2
an is the natural noise ascribed to the driver and road in
m/s2
Figure 2 illustrates the different acceleration distributions
which arise with congested and uncongested conditions.
Figure 2: Congested and
Uncongested Acceleration Distributions
The natural noise can be
described as:
an = f(adr, aal, asf, anmt, airi)
where adr is the noise due to natural variations in the driver's speed in m/s2
aal is the noise due to the road alignment in m/s2
asf is the noise due to side friction in m/s2
anmt is the noise due to non-motorised transport in m/s2
airi is the noise due to roughness in m/s2
In HDM-4 traffic noise is considered to be due to motorised transport. On the basis
of previous research and experiments conducted by the ISOHDM HTRS team in Malaysia, the
following equation was developed which gives the traffic noise as a function of relative
flow - namely the volume to capacity ratio (NDLI, 1995):
at = atmax
RELFLOW =
where RELFLOW is the relative flow (i.e. volume to capacity
ratio)
a0 and a1 are regression coefficients quantified as:
a0 = 4.2 + 23.5
a1 = -7.3 - 24.1
Figure 3 illustrates the predictions for various
relative flows.
Figure 3: Effect of Relative Flow on Traffic
Noise
In HDM-4 the driver noise (adr) and the
alignment noise (aal) are combined into a single value as it is difficult to differentiate
between these two components. The other three components of natural noise - side friction
(asf), non-motorised transport (anmt) and roughness (airi) - will be modelled as linear
functions such as those shown in Figure 4. The maximum values preliminarily estimated for
these components are:
asf = 0.20 m/s2
anmt = 0.40 m/s2
airi = 0.30 m/s2
Figure 4: Proposed HDM-4 Natural
Noise Models
These maximums apply at side friction and
non-motorised transport ratios of 1.0 and a roughness of 20 IRI m/km.
The total natural noise is given by:
an =
Using the above equations, the total acceleration noise at
any relative flow can be characterised by the natural noise (an) and the maximum traffic
noise (atmax).
The maximum traffic noise is calculated as:
atmax =
Experiments were conducted in Malaysia with cars, medium
trucks and buses led to a value of 0.60 m/s2 being recommended for the maximum
total acceleration noise (amax) and a minimum value of 0.10 m/s2 for the
natural noise. These were adopted as the default parameters for all vehicle classes. |