Guidelines for Managing Wake Wash from High ... - PIANC USA
Guidelines for Managing Wake Wash from High ... - PIANC USA
Guidelines for Managing Wake Wash from High ... - PIANC USA
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
INTERNATIONAL NAVIGATION ASSOCIATION<br />
GUIDELINES FOR MANAGING WAKE WASH<br />
FROM HIGH-SPEED VESSELS<br />
Report of Working Group 41<br />
of the<br />
MARITIME NAVIGATION COMMISSION<br />
INTERNATIONAL NAVIGATION<br />
ASSOCIATION<br />
© COPYRIGHT <strong>PIANC</strong><br />
ASSOCIATION INTERNATIONALE<br />
DE NAVIGATION<br />
2003
<strong>PIANC</strong> has Technical Commissions concerned with inland waterways and ports (InCom), coastal and ocean<br />
waterways (including ports and harbours) (MarCom), environmental aspects (EnviCom) and sport and pleasure<br />
navigation (RecCom).<br />
This Report has been produced by an international Working Group convened by the Maritime Navigation<br />
Commission (MarCom). Members of the Working Group represent several countries and are acknowledged<br />
experts in their profession.<br />
The objective of this report is to provide in<strong>for</strong>mation and recommendations on good practice. Con<strong>for</strong>mity is not<br />
obligatory and engineering judgement should be used in its application, especially in special circumstances.<br />
This report should be seen as an expert guidance and state of the art on this particular subject. <strong>PIANC</strong> disclaims<br />
all responsibility in case this report should be presented as an official standard.<br />
© COPYRIGHT <strong>PIANC</strong><br />
<strong>PIANC</strong> General Secretariat<br />
Graaf de Ferraris-gebouw – 11th floor<br />
Boulevard du Roi Albert II 20, B.3<br />
B-1000 Brussels<br />
BELGIUM<br />
http://www.pianc-aipcn.org<br />
VAT/TVA BE 408-287-945<br />
ISBN 2-87223-142-0<br />
All rights reserved
CONTENT<br />
Working group members . . . . . . . . . . . . . . . . . . . . . . .4<br />
Technical expert . . . . . . . . . . . . . . . . . . . . . . . . . . . . .4<br />
1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . .5<br />
1.1 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . .5<br />
1.2 Method of undertaking the task . . . . . . . . . . . .5<br />
1.3 Definition of high-speed vessel . . . . . . . . . . . .5<br />
2. International experience with high-speed<br />
vessel wake . . . . . . . . . . . . . . . . . . . . . . . . . . . . .5<br />
3. Wave generation and vessel wake . . . . . . . . . . . . . .6<br />
3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . .6<br />
3.2 Wave generation and wake characteristics . . . .6<br />
3.2.1 Conventional wake patterns –<br />
sub-critical wash . . . . . . . . . . . . . . . .6<br />
3.2.2 Near-critical wash . . . . . . . . . . . . . . .6<br />
3.2.3 Super-critical wave pattern . . . . . . . . .7<br />
3.2.4 General mechanisms . . . . . . . . . . . . .8<br />
3.3 Propagation and trans<strong>for</strong>mation<br />
of high-speed vessel wake . . . . . . . . . . . . . . . .9<br />
3.3.1 Direction of wave propagation . . . . . .9<br />
3.3.2 Composition of wash and its frequency<br />
components . . . . . . . . . . . . . . . . . . .10<br />
3.3.3 Wave trans<strong>for</strong>mation and<br />
wave decay . . . . . . . . . . . . . . . . . . .10<br />
3.4 <strong>Wake</strong> in coastal areas . . . . . . . . . . . . . . . . . .11<br />
3.4.1 General wave trans<strong>for</strong>mation . . . . . .11<br />
3.4.2 Propagation of vessel wake<br />
in coastal zone . . . . . . . . . . . . . . . . .11<br />
3.5 <strong>Wake</strong> generated by non-steady operation . . . .12<br />
3.5.1 Acceleration, deceleration,<br />
and extent of wash . . . . . . . . . . . . . .12<br />
3.5.2 Change of wake regime with<br />
constant speed . . . . . . . . . . . . . . . . .12<br />
3.5.3 Focusing the wash during course<br />
changes . . . . . . . . . . . . . . . . . . . . . .12<br />
3.5.4 Impact of bathymetry on<br />
operational procedures . . . . . . . . . . .13<br />
3.6 Bernoulli wake and soliton waves . . . . . . . . .13<br />
3.7 <strong>Wake</strong> prediction, analysis, and assessment . .13<br />
3.7.1 Numerical prediction of wake . . . . .13<br />
3.7.2 Full-scale trials and measurements . .15<br />
3.7.3 Model scale trials . . . . . . . . . . . . . . .17<br />
3.7.4 <strong>Wake</strong> analysis . . . . . . . . . . . . . . . . .17<br />
3.7.5 <strong>Wake</strong> assessment . . . . . . . . . . . . . . .17<br />
4.3 Environmental impact of wake . . . . . . . . . . .20<br />
4.3.1 Overview . . . . . . . . . . . . . . . . . . . . . . .20<br />
4.3.2 Potential impacts . . . . . . . . . . . . . . .20<br />
4.3.3 Differentiating between causes . . . . .22<br />
4.3.4 Predicting environmental impact . . .22<br />
5. <strong>Managing</strong> vessel wake . . . . . . . . . . . . . . . . . . . . . .22<br />
5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . .22<br />
5.2 Management measures . . . . . . . . . . . . . . . . .23<br />
5.2.1 Vessel design . . . . . . . . . . . . . . . . . .23<br />
5.2.2 Operational measures . . . . . . . . . . . .23<br />
5.2.3 Non-operational measures . . . . . . . .24<br />
5.3 Route assessment . . . . . . . . . . . . . . . . . . . . .24<br />
5.3.1 Overview . . . . . . . . . . . . . . . . . . . . .24<br />
5.3.2 Route characterization . . . . . . . . . . .24<br />
5.3.3 Impact identification . . . . . . . . . . . .25<br />
5.3.4 Developing and assessing potential<br />
management measures . . . . . . . . . . .27<br />
5.3.5 Monitoring . . . . . . . . . . . . . . . . . . . .28<br />
6. Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . .28<br />
References . . . . . . . . . . . . . . . . . . . . . . . . . . . .29<br />
Annex A – Terms of reference . . . . . . . . . . . . . . . . . .32<br />
© COPYRIGHT <strong>PIANC</strong><br />
4. Impacts associated with vessel wake . . . . . . . . . . .17<br />
4.1 Overview . . . . . . . . . . . . . . . . . . . . . . . . . . .17<br />
4.2 Safety impacts . . . . . . . . . . . . . . . . . . . . . . . .18<br />
4.2.1 Safety of people . . . . . . . . . . . . . . . .18<br />
4.2.2 Safety of vessels . . . . . . . . . . . . . . . .18<br />
4.2.3 Structural damage . . . . . . . . . . . . . .19<br />
3 Report of Working Group 41 - MARCOM
WORKING GROUP MEMBERS<br />
Christian Aage, Technical University of Denmark,<br />
Denmark<br />
Adrian Bell (Chair until September 2002), Kirk McClure<br />
Morton, Northern Ireland, United Kingdom<br />
Lars Bergdahl, Chalmers University of Technology,<br />
Sweden<br />
Alan Blume (Chair), U.S. Coast Guard, United States of<br />
America<br />
Ernst Bolt, Ministry of Public Works, Transport and Water<br />
Management, Netherlands<br />
Hendrik Eusterbarkey, Federal Waterways and Shipping<br />
Administration, Germany<br />
Tetsuya Hiraishi, Port and Harbour Research Institute,<br />
Ministry of Transport, Japan<br />
Henrik Kofoed-Hansen, DHI Water & Environment,<br />
Denmark<br />
Denis Maly, Port Authority Bruges-Zeebrugge, Belgium<br />
Martin Single, University of Canterbury, New Zealand<br />
Jorma Rytkönen, VTT Manufacturing Technology,<br />
Finland<br />
Trevor Whittaker, Queen’s University, Northern Ireland,<br />
United Kingdom<br />
TECHNICAL EXPERT<br />
Björn Elsäßer, Queen’s University, Northern Ireland,<br />
United Kingdom<br />
© COPYRIGHT <strong>PIANC</strong><br />
Report of Working Group 41 - MARCOM<br />
4
1. INTRODUCTION<br />
1.1 SUMMARY<br />
The intent of this report is to provide an overview of the<br />
hydrodynamic and physical aspects of high-speed vessel<br />
wake and to provide guidance <strong>for</strong> its effective management.<br />
This guidance does not prescribe a solution. Rather,<br />
it provides a process that waterway management authorities<br />
and vessel operators can use to develop an appropriate<br />
solution <strong>for</strong> managing high-speed vessel wake. This guidance<br />
is consistent with the International Maritime<br />
Organization’s (IMO) <strong>High</strong>-Speed Craft Code (2000)<br />
and may be used to support the development of the route<br />
operational manual required by Regulation 18.2.2 of that<br />
Code.<br />
The report does not address other issues associated with<br />
the operation of high-speed vessels that are within the<br />
purview of other organisations (e.g., IMO, the<br />
International Association of Marine Aids to Navigation<br />
and Lighthouse Authorities (IALA)); nor does it address<br />
issues related to vessel design since they are beyond the<br />
expertise of <strong>PIANC</strong>.<br />
Although these guidelines were developed in response to<br />
concern about the potential impacts of high-speed vessel<br />
wake (see Annex A), they can be used as the basis <strong>for</strong><br />
managing potential impacts of wake generated by any vessel.<br />
1.2 METHOD OF<br />
UNDERTAKING THE TASK<br />
The working group accomplished its task through a series<br />
of three meetings and correspondence. Members of the<br />
working group also corresponded with experts in their<br />
respective countries.<br />
© COPYRIGHT <strong>PIANC</strong><br />
1.3 DEFINITION<br />
OF HIGH-SPEED VESSEL<br />
For the purpose of this report, the term “high-speed vessel”<br />
includes vessels that meet the definition of a highspeed<br />
craft in the IMO <strong>High</strong>-Speed Craft Code (a vessel<br />
capable of a maximum speed equal to or exceeding<br />
3.7 ∇ 0.1667 (m/s), where ∇(m 3 ) is the displacement of the<br />
vessel at the design waterline), or a definition adopted by<br />
a national maritime authority.<br />
2. INTERNATIONAL<br />
EXPERIENCE WITH<br />
HIGH-SPEED VESSEL WAKE<br />
Real or perceived safety and environmental impacts associated<br />
with high-speed vessel wake in confined waters<br />
have been reported in many locations including Canada<br />
(Sandwell, 2000), Denmark (Kofoed-Hansen, 1996;<br />
Danish Maritime Authority, 1997; Kirkegaard et al., 1998;<br />
Kofoed-Hansen and Mikkelsen, 1997), Great Britain<br />
(Marine Accident Investigation Branch, 2000), Ireland<br />
(Maritime and Coastguard Agency, 1998), Sweden (Strom<br />
and Ziegler, 1998; Allenström et al., 2003), The<br />
Netherlands (Anonymous, 2000), New Zealand (Croad<br />
and Parnell, 2002; Kirk and Single, 2000; Parnell, 1996;<br />
Single and Kirk, 1999), Finland and Estonia (Peltoniemi et<br />
al., 2002), and the United States (Anonymous, 1999;<br />
Stumbo et al., 1999). To date, much of the research undertaken<br />
on high-speed vessel wake wash has appeared only<br />
as unpublished reports <strong>for</strong> various authorities and management<br />
agencies.<br />
<strong>Wake</strong> effects on rivers, lakes, and other inland waters<br />
also can be substantial. For example, see Nanson et al.<br />
(1994), Gadd (1994), Pickrill (1985), and references<br />
therein.<br />
As a result of these reported impacts, vessel operators and<br />
waterway managers alike have tried a number of different<br />
approaches <strong>for</strong> managing high-speed vessel wake. These<br />
include establishing standards <strong>for</strong> maximum allowed wave<br />
heights, maximum allowed wave energy, speed limits, and<br />
risk assessments. Other measures that have been used<br />
include the installation of wave-absorbing materials on sea<br />
walls and other harbour structures as well as ef<strong>for</strong>ts to educate<br />
other waterway users about the potential impacts of<br />
high-speed vessel wake. Based on the experience to date<br />
<strong>from</strong> these different ef<strong>for</strong>ts, it is increasingly apparent that<br />
the effective management of high-speed vessel wake is a<br />
multi-faceted problem that defies a simple “one size fits<br />
all” solution. It is also apparent that a means of managing<br />
high-speed vessel wake wash that addresses legitimate<br />
concerns related to waterway safety and protection of the<br />
marine environment, while also not unduly restricting<br />
their operation, must be identified to realize the full contribution<br />
of high-speed vessels to the national and global<br />
marine transportation systems.<br />
5 Report of Working Group 41 - MARCOM
3. WAVE GENERATION AND<br />
VESSEL WAKE<br />
3.1 INTRODUCTION<br />
This section provides a description of the fundamentals of<br />
wake wave generation by vessels and wave mechanics. It<br />
contains the basic in<strong>for</strong>mation necessary to understand the<br />
effects of wake on the coastline and on other vessels. The<br />
description primarily deals with the free wave system<br />
sometimes referred to as Kelvin, Havelock, and Bernoulli<br />
wave systems and does not discuss near-vessel or bound<br />
wave system problems.<br />
3.2 WAVE GENERATION AND<br />
WAKE CHARACTERISTICS<br />
3.2.1 Conventional wake<br />
patterns – sub-critical wash<br />
© COPYRIGHT<br />
In 1887, Lord Kelvin described the wave system produced<br />
by a moving vessel in deep water. This wave pattern is<br />
confined to a wedge shape known as the Kelvin wedge<br />
(Fig. 3-1). Within this wedge, which has an apex angle of<br />
±19.5°, it is possible to distinguish between diverging<br />
waves, propagating at an angle of θ = 90º to 35º <strong>from</strong> the<br />
vessel’s track, and transverse waves, propagating at an<br />
angle of θ = 35º to 0º <strong>from</strong> the vessel’s track. Under<br />
steady conditions, the transverse waves along the vessel’s<br />
track travel at the same speed as the vessel.<br />
<strong>PIANC</strong><br />
V<br />
Fn l = ,<br />
gL<br />
where V (m/s) is the vessel speed, g (m/s 2 ) is the acceleration<br />
of gravity, and L (m) is the vessel waterline length.<br />
The Kelvin wave pattern is strictly correct only <strong>for</strong> a moving<br />
point source. The wash of a vessel will be the superposition<br />
of a number of these patterns <strong>from</strong> many sources,<br />
of which the bow and stern wave system will generally be<br />
dominant.<br />
When the length Froude number is 0.4 (Fn l = 2π ) in deep<br />
water, the wavelength of the transverse waves is equal to<br />
the vessel’s length. The pressure peaks at the bow and<br />
stern amplify each other while the wave-making resistance,<br />
which is the net longitudinal <strong>for</strong>ce due to the fluid<br />
pressure of the water acting on the hull, increases significantly<br />
(Lewis, 1988). This speed is called the hump speed<br />
and <strong>for</strong>ms a firm barrier <strong>for</strong> most ‘conventional’ vessels<br />
(Fig. 3-2). Basically the vessel continuously tries to move<br />
‘uphill’, which requires more energy. In practice the resistance<br />
hump speed most often occurs when length Froude<br />
numbers are between approximately 0.4 and 0.6. <strong>High</strong>speed<br />
vessels, the subject of these guidelines, are able to<br />
pass through this ‘hump speed’ in deep water. This<br />
requires a relatively high ratio of propulsion power to vessel<br />
displacement.<br />
Figure 3-2 Resistance of a typical ship hull<br />
in deep and shallow water<br />
Figure 3-1 Steady state Kelvin wave pattern<br />
(Ekman, 1906; Newman, 1977)<br />
All vessels operating in deep water produce a Kelvin type<br />
wave pattern. In deep water the wavelength is a function<br />
of the wave speed. The higher the vessel’s speed, the<br />
longer the generated waves become. The most important<br />
parameter <strong>for</strong> the characterisation of the Kelvin wave pattern<br />
is the vessel’s speed related to its waterline length<br />
given in dimensionless terms by the length Froude number<br />
(Fn l ). The length Froude number is defined as:<br />
The Kelvin wave pattern is only valid <strong>for</strong> deep-water<br />
conditions. Deep water in this context means that the<br />
vicinity of the bottom does not affect the propagation<br />
speed of the waves produced.<br />
3.2.2 Near-critical wash<br />
In 1908, Havelock investigated the wave pattern generated<br />
by a single point source in shallow water. He introduced<br />
the depth Froude number, stating that the characteristics of<br />
the wave pattern in depth-limited water are a function of<br />
Report of Working Group 41 - MARCOM<br />
6
vessel speed and water depth. The depth Froude number<br />
(Fn h ) is defined as the ratio of the vessel speed to the wave<br />
propagation speed in shallow water:<br />
V<br />
Fn h = ,<br />
gh<br />
where: V (m/s) is the vessel speed, g (m/s 2 ) is the acceleration<br />
of gravity, and h (m) is the water depth. The classical<br />
Kelvin wave pattern will be generated at depth Froude<br />
numbers under 0.57. The length of the transverse waves,<br />
which are the longest waves in the pattern, will increase as<br />
the depth Froude number becomes larger.<br />
As the depth Froude number approaches 1.0, the vessel’s<br />
speed becomes equal to the maximum wave propagation<br />
speed in the given depth of water. This speed is often<br />
referred to as the critical speed. At this stage, all transverse<br />
waves are left behind the vessel and a wave builds perpendicular<br />
to the vessel as shown in Figure 3-3. If the vessel<br />
stays at critical speed, this wave will extend further <strong>from</strong><br />
the vessel’s track and build in height. All diverging waves<br />
are found behind this critical wave. The conventional<br />
Kelvin wave pattern is often referred to as sub-critical.<br />
Where the water depth starts to change the wave pattern<br />
significantly (Fn h > 0.85), the range is often referred to as<br />
the near-critical speed range.<br />
3.2.3 Super-critical wave pattern<br />
At higher depth Froude numbers (Fig. 3-4) the transverse<br />
waves disappear. They simply cannot keep up with the<br />
vessel since the water depth limits their speed. In water of<br />
constant depth, the first wave crest in the pattern is straight<br />
and the crest length is related to the time the vessel has<br />
been travelling at the particular depth Froude number. The<br />
following waves have curved crests and troughs and are<br />
also continuous.<br />
Figure 3-4 Super-critical wave pattern<br />
in constant water depth<br />
The angle of propagation θ <strong>for</strong> the first wave is determined<br />
by:<br />
cos θ = 1 / Fn h .<br />
There<strong>for</strong>e, as the depth Froude number increases, the<br />
waves bend further backwards and their angle of propagation<br />
becomes increasingly perpendicular to the vessel’s<br />
track. For example, whereas at a depth Froude number of<br />
1.5 the angle of propagation is approximately 48º; at a<br />
depth Froude number of 2.0 the angle of propagation is<br />
60°.<br />
Figure 3-3 Critical wave pattern<br />
in constant water depth<br />
At critical speed there is one transverse wave that moves<br />
with the vessel and dramatically increases the wave-making<br />
resistance. This is because the energy in the longest<br />
wave can no longer disperse generating more waves<br />
behind, as was the case at lower speeds. This is the main<br />
reason most conventional vessels are not capable of<br />
exceeding the critical speed. It also needs to be mentioned<br />
that the critical wave pattern is unsteady and changes with<br />
time. The shape of the first wave is a function of the distance<br />
the vessel has been travelling at critical speed.<br />
The wash generated by a high-speed vessel operating<br />
above the critical depth Froude number in shallow water<br />
has some unique peculiarities. A typical wave time trace<br />
of wash <strong>from</strong> a high-speed vessel operating in shallow<br />
coastal waters measured 2700 meters <strong>from</strong> its track is<br />
shown in Figure 3-5. The trace has been divided into<br />
zones according to wave period and grouping. The first<br />
group, Zone I, comprises the long period super-critical<br />
wash waves and is peculiar to high-speed vessels operating<br />
above the critical depth Froude number. The second<br />
group, Zone II, comprises waves similar in size and height<br />
to the wash waves produced by conventional vessels of<br />
comparable displacement and length. Finally there is a<br />
group of tail waves in Zone III. These are peculiar to highspeed<br />
vessels with transom sterns.<br />
7 Report of Working Group 41 - MARCOM
Figure 3-5 Typical wave trace of a large high-speed vessel at super-critical depth<br />
Froude number with wash zones indicated<br />
©<br />
The time series was measured at a distance of 2700 meters<br />
<strong>from</strong> a catamaran. The average wave periods are 11 seconds<br />
(s), 5s, and 3s, <strong>for</strong> Zone I, II and III respectively.<br />
3.2.4 General mechanisms<br />
The basic mechanism of wash propagation is discussed in<br />
the following section. For simplicity, linear wave theory is<br />
used, though there is an argument to use higher order wave<br />
theory in very shallow water.<br />
With regards to the propagation of surface water waves the<br />
water depth plays a significant role. In deep water the<br />
wave celerity is a function of the wavelength, but in shallow<br />
water the water depth limits the wave celerity. Water<br />
depths of more than half the wavelength can be considered<br />
as deep water, whereas water depths of less than 1/20 th the<br />
wavelength is commonly regarded as shallow water.<br />
COPY-<br />
RIGHT<br />
a) b)<br />
Figure 3-6 a) illustrates the deep-water propagation of<br />
waves generated by a point source moving <strong>from</strong> A to B at<br />
speed V. Waves generated at A would have travelled as<br />
far as the outer circle if they had propagated at the individual<br />
wave phase speed (celerity). The fastest and<br />
longest waves would have moved along the track to B<br />
while shorter and slower waves would have travelled to<br />
locations such as C and D. However, in deep water the<br />
wave energy travels at only one-half the phase speed. As a<br />
result, the locus of wave energy, and there<strong>for</strong>e the largest<br />
wave, moves only as far as the inner circle, to points such<br />
as B’, C’, and D’. In the meantime, the point source has<br />
generated new waves along its way to B. The energy <strong>from</strong><br />
these waves propagates outward in progressively smaller<br />
inner circles. The resulting limit of wave propagation <strong>for</strong><br />
all waves generated as the ship moves <strong>from</strong> A to B is tangent<br />
to the inner circle <strong>for</strong>ming the Kelvin wedge. For any<br />
value of V, this <strong>for</strong>ms an apex angle of ±sin -1 (1/3) =<br />
±19.5°.<br />
<strong>PIANC</strong><br />
Figure 3-6 a) Wave rays <strong>for</strong> sub-critical operation b) Wave rays <strong>for</strong> super-critical operation at Fn h = 1.3<br />
Report of Working Group 41 - MARCOM<br />
8
The visible wave pattern then lies mainly inside and along<br />
the wedge. As individual waves propagate outward at<br />
their phase speed and attempt to outrace the wedge, they<br />
die out and disappear. The largest waves, there<strong>for</strong>e, <strong>for</strong>m<br />
along the wedge and wave amplitudes diminish within a<br />
short distance outside the wedge (Lighthill, 1978;<br />
Newman, 1977).<br />
A similar wave ray diagram can be drawn <strong>for</strong> a shallow<br />
water wave pattern and a depth Froude number greater<br />
than 1 with the important difference, however, that in shallow<br />
water the celerity and speed of energy propagation are<br />
equal. This is shown in Figure 3-6 b) <strong>for</strong> a depth Froude<br />
number of 1.3. There are no waves travelling <strong>from</strong> A at an<br />
angle θ of less than 39.7° in this example. All waves radiated<br />
at A have travelled as far as the outer semicircle. As<br />
waves in shallow water are non-dispersive, the energy of<br />
the wave ray A – C has travelled to C. The wave travelling<br />
in the direction of D is in intermediate water depth.<br />
Hence, the energy has travelled more than half the distance<br />
A – D, as this wave is partially dispersive. The wave travelling<br />
towards F is a deep-water wave, as its wavelength is<br />
short compared to the water depth and, hence, it is fully<br />
dispersive. As a result the energy has travelled only half<br />
the distance to F'.<br />
3.3 PROPAGATION AND<br />
TRANSFORMATION OF<br />
HIGH-SPEED VESSEL WAKE<br />
The following sections focus on propagation of the free<br />
wave field generated by a vessel at super-critical speed.<br />
© COPYRIGHT<br />
3.3.1 Direction of wave propagation<br />
The direction of propagation <strong>for</strong> the leading wave in the<br />
super-critical wash is only a function of the depth Froude<br />
number. This was originally proposed by Havelock (1908)<br />
and proven by various other authors. This relationship is<br />
plotted in Figure 3-7.<br />
Whittaker et al. (2000) studied the divergence between the<br />
first and the following waves and determined that this<br />
angle is dependent on the depth Froude number. The theoretical<br />
divergence between the first and second leading<br />
crest is shown in Figure 3-8. The divergence angle is<br />
defined as the difference in propagation direction between<br />
successive waves. Whittaker et al. (2000) has shown that<br />
this relationship is valid <strong>for</strong> real wave patterns. At high<br />
super-critical Froude numbers the waves are more parallel<br />
than at lower super-critical depth Froude numbers. The<br />
divergence decreases with perpendicular distance <strong>from</strong> the<br />
vessel; the rate of decrease also depends on the water<br />
depth. In deeper water the change in wave pattern is less<br />
than with the same distance in shallow water.<br />
wave direction [°]<br />
<strong>PIANC</strong><br />
Figure 3-7 Angle of wave propagation<br />
at outer edge of stationary pattern (sub-critical)<br />
and leading wave (super-critical)<br />
Figure 3-8 Divergence of second wave compared to first with varying depth<br />
Froude number and perpendicular distance <strong>from</strong> vessel normalised by water depth<br />
9 Report of Working Group 41 - MARCOM
With each successive wave the divergence angle decreases<br />
at constant perpendicular distance <strong>from</strong> the vessel’s track.<br />
Thus, the waves further back in the pattern become<br />
increasingly parallel to each other. Finally, the pattern<br />
contains waves whose crests are almost parallel to the vessel's<br />
track. The slight change in the propagation direction<br />
of the waves leads to an apparent lengthening of the waves<br />
farther <strong>from</strong> the vessel. Hence, the peak-to-peak distance<br />
of the wave increases with distance <strong>from</strong> the vessel’s track.<br />
Waves with a period in excess of 40 seconds have been<br />
measured 2.7 kilometres <strong>from</strong> the vessel (MCA, 1998).<br />
Though the wash measured as a time series often appears<br />
as a series of sinusoidal waves each with a slightly shorter<br />
period, the surface elevation is in fact a superposition of an<br />
infinite number of waves. Using the zero crossing period<br />
on its own to calculate the wave speed will lead to slightly<br />
smaller values of wave celerity. Most importantly it has<br />
to be recognised that the period of the waves in a vessel’s<br />
wake is not a function of hull design, but rather of vessel<br />
speed, water depth, and the distance the wave travels <strong>from</strong><br />
the point where it was generated. In contrast, the height of<br />
the waves in the wake is a function of the hull design. In<br />
general, <strong>for</strong> vessels with a similar hull <strong>for</strong>m but different<br />
lengths, the height of waves generated by the shorter vessel<br />
will be lower than those generated by the longer vessel.<br />
The implication is that the period of the waves generated<br />
by vessels of different lengths operating at the same depth<br />
Froude number will be the same. However, the waves<br />
generated by the shorter vessel will be less pronounced<br />
when compared to the waves generated by the longer vessel<br />
since they will not be as high.<br />
3.3.2 Composition of wash and<br />
its frequency components<br />
So far these guidelines have only focused on the location<br />
of crests and troughs in the wave pattern. The wave-making<br />
resistance, which is a significant part of the total resistance<br />
of a vessel, corresponds to the energy used to generate<br />
the wave pattern. This resistance is spread as a continuous<br />
spectrum over the wave rays radiated <strong>from</strong> the vessel.<br />
The distribution of the wave-making resistance is often<br />
referred to as the free wave spectrum or the amplitude<br />
function. In deep water this distribution is a function of<br />
the vessel speed, the hull length and displacement, and the<br />
hull shape.<br />
Figure 3-9 a) shows such a distribution <strong>for</strong> a typical ship<br />
hull in deep water. There is a different distribution <strong>for</strong><br />
each vessel speed <strong>for</strong> a given hull, or to be more precise,<br />
<strong>for</strong> each length Froude number. In shallow water the distribution<br />
is a function of the vessel speed, water depth, hull<br />
length, displacement, and shape. A shallow water distribution<br />
<strong>for</strong> the same vessel speed is given in Figure 3-9 b)<br />
<strong>for</strong> a depth Froude number of 1.3. Note that there are no<br />
wave resistance components between θ = 0° and 39.7°,<br />
and a large amount of energy is concentrated between<br />
39.7° and 60°. These resistance components <strong>for</strong>m the<br />
leading waves in the super-critical wave pattern. The area<br />
underneath these curves is proportional to the wave pattern<br />
resistance. In this case, the area under both curves is<br />
almost equal.<br />
3.3.3 Wave trans<strong>for</strong>mation and wave decay<br />
Havelock (1908) investigated the decay of wave height<br />
with distance at sub-critical depth Froude numbers. He<br />
found that the decay of both the transverse and diverging<br />
waves is proportional to ϖ n , where ϖ is the distance <strong>from</strong><br />
the vessel and n is a constant value. He showed that the<br />
theoretical decay inside the Kelvin wedge has the exponent<br />
n = -1/2 and the waves along the outer edge of the<br />
wedge decay have an exponent of n = -1/3.<br />
Figure 3-10 Decay of wave amplitude<br />
as investigated by Havelock<br />
© COPYRIGHT <strong>PIANC</strong><br />
Figure 3-9 a) Distribution of wave-making resistance over propagation angle (θ)<br />
b) the resistance is here made dimensionless as resistance coefficient (C w )<br />
Report of Working Group 41 - MARCOM<br />
10
Kofoed-Hansen et al. (1999) suggested a decay rate of<br />
n = -0.55 based on a best fit through a wide range of wake<br />
measurements <strong>for</strong> catamarans operating at super-critical<br />
speeds. They also stated that a decay rate of n = -1/3 close<br />
to the vessel (less than 3 vessel lengths) would be more<br />
appropriate. Whittaker et al. (2001) concluded <strong>from</strong> a<br />
series of towing tank tests in shallow water that the decay<br />
rate could be substantially less. The lowest decay rate<br />
observed was as low as n = - 0.2. While Havelock compared<br />
the wave height at a straight ray <strong>from</strong> the vessel (Fig.<br />
3-10), the later comparisons are based on the maximum<br />
wave height found in wave cuts at different distances perpendicular<br />
<strong>from</strong> the vessel’s track.<br />
3.4 WAKE IN COASTAL AREAS<br />
3.4.1 General wave trans<strong>for</strong>mation<br />
There are a number of processes that can affect the wave<br />
as it propagates into coastal and shallow water areas. The<br />
most important are listed as follows:<br />
• Refraction - the bending of wave fronts and wave height<br />
reductions as they travel into shallower water<br />
• Diffraction - the lateral transfer of energy along the<br />
wave crest<br />
• Shoaling - the alteration in wave height as waves propagate<br />
into shallow water<br />
• Wave-current interaction - the alteration of wave celerity<br />
and height due to currents<br />
• Breaking - energy dissipation due to increased wave<br />
steepness<br />
• Friction - energy dissipation due to friction on seabed or<br />
obstacles or due to percolation through a porous seabed<br />
• Reflection - alteration in wave height due to full or<br />
partial reflection <strong>from</strong> structures or seabed<br />
© COPYRIGHT <strong>PIANC</strong><br />
All these processes are general coastal processes and are<br />
not discussed in detail as part of these guidelines. For<br />
more details see Vincent et al. (2002).<br />
3.4.2 Propagation of vessel wake<br />
in coastal zone<br />
The propagation of waves <strong>from</strong> a vessel to the shore can be<br />
divided into two processes:<br />
• Vessel speed - depth Froude number based trans<strong>for</strong>mation<br />
of wake. As described in Section 3.2.3, the first<br />
wave crest of the supercritical wave pattern is straight in<br />
constant water depth, and the angle of propagation<br />
depends only on the ratio of vessel speed to maximum<br />
wave speed. The following waves trans<strong>for</strong>m, and as a<br />
result the wave period changes with distance <strong>from</strong> the<br />
vessel in water of constant depth.<br />
• Trans<strong>for</strong>mation of wake due to change in bathymetry.<br />
Variations in waterway bathymetry can cause the<br />
height, propagation direction, and celerity of waves to<br />
change. These are common coastal processes as listed<br />
in Section 3.4.1.<br />
Both the depth Froude number based trans<strong>for</strong>mation and<br />
the bathymetric trans<strong>for</strong>mation need to be combined to<br />
predict the wash. The leading wave can be treated as a<br />
monochromatic shallow water wave. The following waves<br />
are a superposition of an infinite number of wave components<br />
(see Section 3.3.1). Even in shoaling water, the<br />
waves <strong>for</strong>ming the pattern have different celerities, which<br />
results in the dispersion of energy <strong>from</strong> one wave to the<br />
next further back in the trace.<br />
Once in the breaker zone the linear wave theory is no<br />
longer valid. This means that the waves can no longer be<br />
considered as being sinusoidal. Several wave theories<br />
have been developed in the past century, which deal with<br />
shallow water waves like Boussinesq wave theory, or<br />
higher order wave theory (Demirbilek and Vincent, 2002).<br />
In some cases the long waves propagating into areas with<br />
extremely shallow water, e.g., on mud flats or salt<br />
marshes, can be approximated as solitary waves.<br />
In some studies the leading group of long-period waves,<br />
which are often the most critical waves in terms of risk,<br />
have been treated as waves with a very narrow spectrum<br />
(Kofoed-Hansen et al., 1996 and 1999; MCA, 1998). The<br />
correlation between the modelling and some full-scale<br />
measurements proved to be sufficient <strong>for</strong> most practical<br />
problems.<br />
<strong>Wash</strong> and wind waves will superimpose causing local<br />
steepening that can lead to breaking and energy loss.<br />
Otherwise, they will pass through each other unchanged.<br />
In general, high-speed wash is very small compared to<br />
fully developed wind waves. Thus, high-speed wash can<br />
hardly be detected in wash measurements with the presence<br />
of pronounced wind waves or swells. Vessel wash<br />
can, however, still be a problem on the shoreline even<br />
under storm conditions as the very long period waves are<br />
still present but masked. No evidence has been found that<br />
suggests that wind affects the long wave components in<br />
high-speed wash because the interactive time is too short<br />
and the steepness is too small.<br />
11 Report of Working Group 41 - MARCOM
3.5 WAKE GENERATED BY<br />
NON-STEADY OPERATION<br />
3.5.1 Acceleration, deceleration,<br />
and extent of wash<br />
During acceleration in water of constant depth the wave<br />
pattern and the wave resistance will change. When accelerating<br />
<strong>from</strong> sub-critical to super-critical speeds the vessel<br />
has to pass through a resistance hump at critical speed (see<br />
Fig. 3-2). While at near-critical or critical speeds, the<br />
wake generated is more energetic vis-à-vis the wake generated<br />
at either sub- or super-critical speeds. It is, there<strong>for</strong>e,<br />
desirable to pass through the near-critical speed<br />
range as quickly as possible. The same applies to deceleration,<br />
where the operator should aim <strong>for</strong> a quick decrease<br />
in speed near the critical wake regime. The different wake<br />
regimes are shown in Figure 3-11. If possible, the operator<br />
should avoid operation at depth Froude numbers<br />
between approximately 0.85 and 1.1.<br />
unacceptable waves were being generated when the vessel<br />
was abeam of location A and reduced speed immediately,<br />
it is likely that substantial wash would still propagate to<br />
location A.<br />
Figure 3-12 Outer envelope and extent of wash<br />
3.5.2 Change of wake regime<br />
with constant speed<br />
Figure 3-11 <strong>Wake</strong> regime depending<br />
on speed and water depth<br />
When accelerating the vessel will produce a wave pattern<br />
with a transitional zone. This transitional zone is nonsteady<br />
and will change its position and area with time. A<br />
simplified wave pattern generated by a high-speed vessel<br />
with instantaneous acceleration in constant water depth is<br />
shown in Figure 3-12. It is assumed the vessel started its<br />
passage at the left and instantly accelerated to a super-critical<br />
speed. Three zones can be identified in the graph. An<br />
object at location A will encounter the full wash waves.<br />
An object at location B will experience the same leading<br />
waves as location A; however, with reduced wave heights.<br />
An object at location C may be subjected to little or no<br />
wave action <strong>from</strong> the leading waves. As the vessel continues<br />
to operate, some waves will continue to travel toward<br />
locations A, B, and C with the boundary of the wash continuously<br />
moving outward. Finally, location C will<br />
encounter the short tail waves (Fig. 3-5, Zone III). The<br />
implication is that even if the operator recognised that<br />
Report of Working Group 41 - MARCOM<br />
© COPY-<br />
RIGHT <strong>PIANC</strong><br />
12<br />
Although a high-speed vessel may continue to operate at<br />
constant speed, the wake regime may change with variation<br />
of water depth along the vessel’s route. A vessel<br />
approaching a fairway <strong>from</strong> deep water may operate at<br />
sub-critical speeds. Continuation of operation at high<br />
speeds into shallow water results in the transition to critical<br />
speed. Depending on the bathymetry the vessel might<br />
operate <strong>for</strong> a considerable time at near-critical speeds and<br />
finally proceed to super-critical speed or decelerate. It is<br />
extremely important to recognise that the wash progressing<br />
toward the shoreline may have been caused by operating<br />
at near-critical depth Froude numbers along an earlier<br />
part of the passage.<br />
3.5.3 Focusing the wash during course changes<br />
When a vessel changes course, the energy density on the<br />
inside of the turn will be higher than the energy density on<br />
the outside of the turn. The difference is more pronounced<br />
<strong>for</strong> larger course changes than smaller changes as well as<br />
when the vessel is operating at higher speeds. This is<br />
because although the energy transferred into the wake is<br />
equal on both sides of the vessel’s track, it becomes<br />
focused on the inside of the turn insofar as it is transferred<br />
into a smaller area. As a result, the waves generated by the<br />
vessel will also be higher on the inside of the turn than<br />
those generated when the vessel is operating on a straight<br />
course. Similarly, the waves on the outside of the turn will<br />
be lower.
To mitigate the higher energy density and waves on the<br />
inside of a turn, it may be necessary to increase the radius<br />
of the turn or to make the change in a number of smaller<br />
changes with sufficient distance between them to avoid<br />
creating areas of increased wash concentration. It may<br />
also be necessary to reduce speed during the change of<br />
course. Particular care should be taken where the focused<br />
wash of the inner bend will propagate onto shoaling areas,<br />
such as banks or headlands, as a further increase in wave<br />
height can be expected. On the other hand, turns can be<br />
used to decrease wash heights on the outer bend, if the<br />
operational area allows such manoeuvres.<br />
confined water are capable of producing large Bernoulli<br />
wakes. Figure 3-13 is an example of a Bernoulli wake generated<br />
by a large container vessel in water approximately<br />
15 meters deep operating at sub-critical speeds.<br />
3.5.4 Impact of bathymetry<br />
on operational procedures<br />
While the variation of water depth along the passage may<br />
change the wake regime it also has a significant impact on<br />
the power requirement of the vessel. As described in<br />
Section 3.2.2 and illustrated in Figure 3-2, the resistance<br />
of the vessel increases close to the critical depth Froude<br />
number. Hence, the vessel needs sufficient propulsion to<br />
overcome this resistance peak. A vessel approaching shallow<br />
water might, there<strong>for</strong>e, proceed at near-critical depth<br />
Froude number with constantly decreasing speed while<br />
generating a wake with higher energy compared to supercritical<br />
operation at the same water depth. This is most<br />
likely if the vessel’s speed is reduced <strong>for</strong> some reason, e.g.,<br />
extra drag due to hull fouling, the vessel is loaded higher<br />
beyond its normal service load, or partial power loss<br />
(Cain, 2000).<br />
Sudden bathymetric changes can be used to transition<br />
quickly <strong>from</strong> either a sub- or super-critical wake regime to<br />
the other without prolonged operation at near-critical<br />
speed. One means of accomplishing this is to construct a<br />
steep depth contour in the channel as described by<br />
Feldtmann and Garner (1999).<br />
3.6 BERNOULLI WAKE<br />
AND SOLITON WAVES<br />
The dynamic displacement of water caused by the <strong>for</strong>ward<br />
movement of a vessel through water results in a velocity<br />
field around the hull (bound wave field). While this velocity<br />
field is responsible <strong>for</strong> the pressure distribution along<br />
the surface and, hence, the generation of waves, it has little<br />
effect on the far field propagation and trans<strong>for</strong>mation of<br />
the Kelvin wave pattern (free wave field). However, in a<br />
confined environment, e.g., fairway, shallow water or<br />
canal, the flow field can be restricted by the surrounding<br />
boundaries. This is very distinct in inland canals and is<br />
directly related to the blockage.<br />
© COPY-<br />
RIGHT <strong>PIANC</strong><br />
Theoretically any type of vessel will produce such a displacement<br />
wave. However, in particular large vessels in<br />
Figure 3-13: Bernoulli wake and Kelvin wake<br />
generated by a large container vessel<br />
A vessel operating close to critical speed (i.e., depth<br />
Froude number between 0.85 and 1.1) is capable of generating<br />
a solitary wave, which in fact can be faster than the<br />
vessel. Both conventional vessels and high-speed vessels<br />
can produce solitary type waves, which are of very long<br />
period and can travel several vessel lengths ahead in very<br />
shallow open water. Large displacement vessels operating<br />
in shallow water are particularly prone to generating this<br />
type of wave (Scott-Russell, 1865; Dand et al., 1999;<br />
Whittaker et al., 2001).<br />
3.7 WAKE PREDICTION,<br />
ANALYSIS, AND ASSESSMENT<br />
3.7.1 Numerical prediction of wake<br />
A numerical non-linear time-domain model capable of<br />
calculating vessel-generated waves, wave propagation,<br />
and wave trans<strong>for</strong>mation in non-homogeneous media is<br />
the ultimate tool <strong>for</strong> evaluating the potential <strong>for</strong> vessel<br />
wake to have adverse safety or environmental impacts.<br />
Besides predicting the unstationary flow field and the<br />
associated wave pattern around the vessel hull, the same<br />
model (preferably) will be able to calculate the dynamics<br />
of the transient waves in the surf zone including the maximum<br />
wave height be<strong>for</strong>e wave breaking as well as run-up<br />
on beaches and river banks. Such models do not exist yet;<br />
however, if they did, they would be far too computationally<br />
demanding <strong>for</strong> practical use.<br />
In recent years, the use of computational fluid dynamic<br />
(CFD) codes has provided a valuable supplement to more<br />
classic methods <strong>for</strong> design and optimisation of vessel<br />
hulls. Comparisons between results <strong>from</strong> various CFD<br />
codes, full-scale measurements, and towing tank tests have<br />
increased confidence in using these models <strong>for</strong> prediction<br />
of wake wash caused by multi-hull vessels at varying<br />
13 Report of Working Group 41 - MARCOM
water depths. A general limitation of these models is that<br />
they do not permit calculations of the far-field wave pattern.<br />
Most often, the calculation is limited to an area within<br />
approximately three to five vessel lengths.<br />
Furthermore, the codes usually only provide a stationary<br />
solution of the potential flow field at a constant depth.<br />
Predicting the impact of the wake <strong>for</strong> a certain vessel operating<br />
on a given route requires, in most cases, the solution<br />
of an unsteady problem in a three-dimensional domain.<br />
This is, in most cases, not feasible with one particular<br />
numerical model. Hence, the numerical prediction of the<br />
wake problem is divided into two different problems:<br />
• Prediction of the wave field near the vessel.<br />
• Prediction of the wave trans<strong>for</strong>mation and propagation<br />
in the far field and coastal zone.<br />
Very few numerical models predict both problems; those<br />
that have been developed to date are coupled methods<br />
(Raven, 2000; Kofoed-Hansen et al., 2000).<br />
3.7.1.1 Prediction of the wave field near the vessel<br />
The wave field generated by a vessel can be derived by<br />
numerical methods in several ways. These methods can be<br />
grouped in principle in two categories: panel codes and<br />
thin vessel theory models. Because of the inherent limitations<br />
associated with each type of model, several research<br />
institutions are working on hybrid models.<br />
Potential Flow Panel Codes<br />
These codes use a non-linear free-surface potential flow<br />
method, where the hull and water surfaces are represented<br />
by a large number of panels. As the pressure along the hull<br />
is calculated, sinkage and trim can be predicted. Since the<br />
boundary conditions are non-linear the problem cannot be<br />
solved directly. The actual wave surface is derived by<br />
means of iteration starting with a flat surface and an estimated<br />
trim and sinkage. Shallow water effects can be<br />
implemented. However, as in most codes, the grid moves<br />
with the vessel and only steady state or quasi-steady state<br />
conditions can be computed. Only panel codes with timestepping<br />
treatment have the potential of solving fully nonsteady<br />
conditions. The computational ef<strong>for</strong>t is rather large<br />
and, thus, the computation time can be considerable. Most<br />
models calculate the wave elevation or free surface profile<br />
up to a few vessel lengths distance <strong>from</strong> the vessel. A<br />
review of the current capabilities of panel codes can be<br />
found in Raven (2000) and Hughes (2001) as well as more<br />
detailed literature.<br />
Thin ship theory code<br />
This theory, which is often referred to as slender body theory,<br />
assumes the vessel hull(s) to be slender compared to<br />
their length. Most theories represent the body of the vessel<br />
as a series of Kelvin sources along the centreline of the<br />
hull assuming a linear free surface condition. As such the<br />
theory is limited to linear wave theory and in particular<br />
small waves compared to the wavelength. The theory<br />
behind these programs originates <strong>from</strong> work carried out by<br />
Lord Kelvin, Havelock (1908), Mitchell (1898) and<br />
Eggers et al. (1967). The strength of each of the sources<br />
is derived <strong>from</strong> the local slope of the hull at a number of<br />
water lines. The locations where the local slope is determined<br />
are often referred to as panels. The underlying<br />
equations are multiple integrals and are solved directly by<br />
numerical integration. The code can compute only steady<br />
state (constant speed) conditions and shallow water problems.<br />
Some programs include the input of reflective<br />
boundaries to simulate tank walls and, thus, allow the<br />
results to be compared with narrow tank experiments.<br />
Trim and sinkage is usually user defined. More recent<br />
codes derive the sinkage and trim by means of calculating<br />
the <strong>for</strong>ces on the hull <strong>from</strong> the surrounding surface elevation<br />
through iteration. Difficulties occur with transom<br />
sterns, as basic thin vessel theory cannot deal with flow<br />
separation. Adjustments to the code like artificial appendices<br />
(virtual stern) or the use of potential flow methods<br />
have helped to improve the predictions significantly. Very<br />
high length Froude numbers seem to produce numerical<br />
instabilities with certain codes or the accuracy decreases.<br />
Thin ship theory still is heavily used and produces good<br />
results <strong>for</strong> many vessel wash problems. There is no limitation<br />
to the distance <strong>from</strong> the vessel at which a wave elevation<br />
can be computed. However, some programs can<br />
only derive entire wave fields and the computation is<br />
restricted to constant water depth. Other effects like surface<br />
tension, wave breaking, and seabed shear stress are<br />
usually neglected. In particular, due to numerical damping<br />
and other numerical inaccuracies, the error can become<br />
too large in the far field to be acceptable.<br />
Most thin ship theory programs can be run on a normal<br />
desktop computer and results are obtained within seconds.<br />
A description of current programs can be found in Gadd<br />
(1999), Molland et al. (2000), Tuck et al. (2001) and<br />
Doctors (1997) as well as more detailed literature.<br />
© COPYRIGHT <strong>PIANC</strong><br />
3.7.1.2 Prediction of wave trans<strong>for</strong>mation and propagation<br />
in the far field and coastal zone<br />
Once the generated waves are no longer influenced by the<br />
vessel, other coastal engineering tools can be used to compute<br />
the wash propagation over a variable bathymetry. To<br />
date only a few successful approaches have been published:<br />
Report of Working Group 41 - MARCOM<br />
14
• Kofoed-Hansen et al. (1996, 1999 and 2000) and MCA<br />
(1998) used a spectral wave model, which describes the<br />
propagation, growth, and decay of short-period waves<br />
in near shore areas to predict the wave height contours<br />
over a variable bathymetry. The model includes the<br />
effects of refraction and shoaling due to varying depth,<br />
wave generation due to wind, and energy dissipation<br />
due to bottom friction and wave breaking. The basic<br />
equations in the model are derived <strong>from</strong> the conservation<br />
equation <strong>for</strong> the spectral wave action density.<br />
• The model boundary allows <strong>for</strong> the variable spectral<br />
<strong>for</strong>ms and permits the wave conditions to vary along the<br />
boundary. For wash studies, waves were specified in<br />
terms of mean wave height, mean wave period, mean<br />
wave direction as well as parameters <strong>for</strong> spreading <strong>from</strong><br />
the mean direction. The code also can be modified to<br />
allow <strong>for</strong> the input of empirical decay rates derived<br />
<strong>from</strong> experiments. A linear refraction-diffraction<br />
model also has been used to calculate the wave disturbance<br />
patterns of the time history as the wave propagates<br />
<strong>from</strong> the vessel to the shore (MCA, 1998).<br />
• Raven (2000) suggested a number of analytical techniques<br />
<strong>for</strong> calculating wave propagation in the far field,<br />
where effects <strong>from</strong> banks or bottom topography can be<br />
neglected. He also demonstrated the successful coupling<br />
of a steady state panel code with a space domain<br />
Boussinesq-type model. A similar approach is discussed<br />
in Kofoed-Hansen et al. (2000). The principle<br />
behind the Boussinesq-type models is to eliminate the<br />
vertical dimension in the flow description without losing<br />
important effects like the influence of the vertical<br />
acceleration on the wave propagation. The non-uni<strong>for</strong>m<br />
distribution of the velocity profile is responsible<br />
<strong>for</strong> the frequency dispersion. The idea is to couple the<br />
two types of models in order to utilise the computational<br />
cost effectiveness of the two-dimensional Boussinesq<br />
model where it is possible, and to apply the detailed,<br />
but time-consuming Navier-Stokes (or Euler/CFD)<br />
based free surface model only in areas where the flow<br />
field is three-dimensional.<br />
© COPYRIGHT <strong>PIANC</strong><br />
To calculate the essential boundary conditions <strong>for</strong> the<br />
Boussinesq model, the full three-dimensional velocity<br />
field and the free surface elevation is required. The free<br />
surface elevation is not generally sufficient as pointed out<br />
by Kofoed-Hansen et al. (2000).<br />
The great advantage of using a Boussinesq-type model is<br />
the possibility of simulating the wash sequence including<br />
both Bernoulli and Kelvin wake. The tool has proven to<br />
be very powerful. However, it still has its restrictions and<br />
requires further development.<br />
• Chen and Sharma (1995) investigated the wave generation<br />
of a slender vessel in a shallow channel at near critical<br />
speed using a combination of thin-ship theory and<br />
simplified Boussinesq equations. In particular the periodic<br />
generation of solitary waves was presented, which<br />
required the use of a non-steady model. The methods<br />
produced good results <strong>for</strong> a shallow channel with variable<br />
cross section. Jiang (2000) combined the thin-ship<br />
approximation with an enhanced Boussinesq method<br />
with improved results, and Jiang et al. (2002) expanded<br />
the model <strong>for</strong> a moving ship, accelerating or decelerating,<br />
in an arbitrary bottom topography, although with<br />
simplified Boussinesq equations.<br />
In general there is some agreement that Boussinesq-type<br />
models will give more realistic results, particularly if the<br />
phase relationship of the successive waves is modelled<br />
correctly. More complex wave models based on<br />
Boussinesq-type equations with a wider applicability in<br />
terms of wavelengths are currently being developed.<br />
Together with improved algorithms and faster desktop<br />
computers these models will be more applicable to a wider<br />
range of cases.<br />
Regardless of what type of numerical model is determined<br />
to be the most appropriate, it is necessary to calibrate it<br />
against either full- or model-scale experiments and then<br />
validate its output with field data be<strong>for</strong>e it can be used as<br />
a practical tool <strong>for</strong> managing wake wash.<br />
3.7.2 Full-scale trials and measurements<br />
3.7.2.1 Measurement techniques<br />
A range of measurement techniques can be used to obtain<br />
wave elevations generated by a vessel. It is beyond the<br />
scope of these guidelines to discuss all the techniques in<br />
detail. An overview of the techniques applied so far is<br />
given and some of the difficulties and criticisms are discussed.<br />
The basic types of point measurement techniques<br />
are listed in Table 3-1. Three different types of techniques<br />
are listed in Table 3-2 that can be used to map a whole<br />
wave field. Not all devices are suitable <strong>for</strong> all locations,<br />
i.e., near field, far field or shoreline. The basic difficulty<br />
is accessibility and range as listed in Table 3-1. The equipment<br />
used to measure the wake should undergo a rigorous<br />
calibration procedure. It is important that the device is<br />
capable of measuring long-period waves (over 20 seconds)<br />
with small amplitude. If possible, validation should be<br />
undertaken with a different type of equipment, particularly<br />
<strong>for</strong> those devices not measuring elevation directly.<br />
15 Report of Working Group 41 - MARCOM
Table 3-1 Single point measurement techniques <strong>for</strong> ship wave measurements<br />
Type: Quantity measured: Technique: Requirements: Constrains: Reference: (examples)<br />
Wave staff Water elevation Capacitance Mounting pole, Shallow water Parnell & Kofoedlogger<br />
only Hansen (2001)<br />
Surveying rod Water elevation Optical Accessibility, Very labour Hannon & Varyani<br />
& camera solid structure intensive (1999)<br />
Altimetry Distance <strong>from</strong> Laser, Solid structure Location Kirk McClure Morton<br />
above surface Ultra-sound, <strong>for</strong> transducer (1998), Koushan<br />
Radar et al. (2001)<br />
Subsurface Water elevation / Echo sound Watertight -<br />
water depth<br />
device<br />
Subsurface Water pressure Piezo transducer Watertight Depth limitation Whittaker (2001),<br />
device <strong>for</strong> short waves Stumbo et al. (1999)<br />
Aqua Particle velocity Acoustic Doppler Watertight device Depth limitation Fissel et al. (2001)<br />
Doppler<br />
<strong>for</strong> short waves<br />
Wave Acceleration Accelerometer Floating buoy Small signal <strong>for</strong> Koushan et al. (2001)<br />
riding Buoy with adequate very long waves<br />
size/weight<br />
Table 3-2 Area measurement techniques (3 dimensional)<br />
Type: Technique: Reference:<br />
Stereo photogrammetry Optical, two pictures taken at different locations Inui (1962).<br />
of same area at same time<br />
LIDAR Fast scanning laser beam across surface Bolt (2001)<br />
and time delay of reflection measured<br />
RADAR<br />
Microwave beam scanning surface<br />
and time delay of reflection measured<br />
3.7.2.2 Monitoring and trial procedures<br />
Full-scale trials can serve two different purposes and as a<br />
result the necessary procedures <strong>for</strong> undertaking such<br />
assessments may differ.<br />
General vessel per<strong>for</strong>mance measurements<br />
Measurement of the wave generation by the vessel and the<br />
wave profile at a given distance <strong>from</strong> the sailing line may<br />
be carried out. In such cases a steady state wave pattern is<br />
of interest. These trials are similar to tank tests and, hence,<br />
are subject to similar procedures. However, it has to be<br />
recognised that conditions are not as controlled as in a<br />
towing tank. Apart <strong>from</strong> the vessel speed over ground,<br />
course over ground, and continuous recording of the vessel's<br />
position after constant time intervals, it is recommended<br />
to record still water trim, overall displacement,<br />
and operation / control of trim flaps, stabilisers, and foils.<br />
It has to be ensured that the vessel has been operating at<br />
constant speed <strong>for</strong> a distance long enough (in particular<br />
close to critical speed). The vessel needs to continue <strong>for</strong><br />
sufficient distance with constant speed after passing the<br />
monitoring location (persistence of wash). It is also desirable<br />
that the seabed is smooth and constant in water depth<br />
along the vessel's track unless deep-water trials are carried<br />
out. The slope of the seabed perpendicular to the vessel’s<br />
track should be uni<strong>for</strong>m. However, constant water depth<br />
would be desirable. Preferably trials should be undertaken<br />
with no or minimal current. In any case a repetition of<br />
Report of Working Group 41 - MARCOM<br />
16
at least one trial in opposite directions is recommended <strong>for</strong><br />
repeatability (assuming the vessel is symmetrical). The<br />
background wave climate, with particular attention to<br />
other vessels’ wake, wind generated waves and swells,<br />
needs to be minimal to reduce post-processing of the data.<br />
<strong>Wake</strong> assessment of a vessel along its operational route<br />
It may be necessary to monitor the wake of a vessel along<br />
a given route <strong>for</strong> risk assessment or numerical modelling<br />
purposes. Due to the variability of the operation, several<br />
passages may need to be monitored to cover different tidal<br />
stages, variable loading of the vessel or different operational<br />
procedures. The monitoring might, there<strong>for</strong>e, be<br />
undertaken over a period of several days. The length of<br />
the monitoring window needs to be sufficient to cover the<br />
full extent of wash (possibly more than 40 minutes). It is<br />
recommended to start monitoring well be<strong>for</strong>e the vessel<br />
passes the monitoring location. The primary reason is that<br />
waves could travel ahead of the vessel or the change of<br />
operation further out causes larger disturbance than the<br />
nearby passage. Monitoring should be continued after the<br />
passage of the concerned vessel until no significant waves<br />
have been measured <strong>for</strong> a considerable time. It is recommended<br />
to record at least still water trim, overall displacement,<br />
and operation of trim flaps, stabilisers, and foils.<br />
3.7.3 Model scale trials<br />
<strong>Guidelines</strong> on tank testing have been published by the<br />
International Towing Tank Conference and are not discussed<br />
in detail in these guidelines. In<strong>for</strong>mation can be<br />
obtained through the Naval Architecture Institutions and<br />
major naval research institutes and departments. Attention<br />
may be drawn to the effects caused by the narrow tank<br />
width in shallow water tests, which are discussed in Inui<br />
(1954). Close to critical speed the towed model is capable<br />
of producing a number of solitary waves depending on the<br />
distance towed at such speed Dand et al. (1999). However,<br />
this has limited practical relevance. The propulsion system<br />
has also significant effect on the wave generation by the<br />
vessel as shown by Taatø et al. (1998). It was found that<br />
the wave amplitude generated by a water jet propelled<br />
model increased by 10 to 40 percent compared to the wave<br />
amplitude generated by a towed model. Several research<br />
groups have used wide shallow water tanks with a tank<br />
width of up to 10 vessel lengths to establish an unreflected<br />
free wave pattern behind the vessel. Again the towing<br />
length needs to be long enough to generate a steady-state<br />
pattern (persistence of waves).<br />
(moreover the event is transient and not periodic). Modern<br />
wavelet analysis might, however, be a good tool <strong>for</strong> mapping<br />
both frequency and time in<strong>for</strong>mation.<br />
• Signal preparation: For the removal of high frequency<br />
noise, a filter method of higher order is recommended.<br />
A more efficient filter technique that does not result in<br />
a phase lag is to make a fast Fourier trans<strong>for</strong>m, cut the<br />
high frequency noise and make an inverse trans<strong>for</strong>m.<br />
Moving averages may also be used, but are less<br />
favourable as the signal is not removed but only<br />
smoothed. Tidal variations or varying offsets may be<br />
best removed with moving averages or high frequency<br />
pass filter.<br />
• Wave cuts in the space domain derived <strong>from</strong> numerical<br />
steady state simulations may be converted into the time<br />
domain.<br />
• Wave-by-wave analysis: Complying with standard<br />
engineering procedures the zero-crossing technique<br />
should be adopted. Thus, the wake can be characterised<br />
in terms of zero-crossing period and zero-crossing<br />
wave height. Otherwise a peak-to-peak analysis can be<br />
used.<br />
3.7.5 <strong>Wake</strong> assessment<br />
The wave generation of the vessel can be assessed using<br />
the wave-making resistance (denoted using either R w or<br />
the wave resistance coefficient C w ) as well as the ratio of<br />
the distribution of resistance R w to the propagation direction<br />
θ (∆R w /∆θ).<br />
As the wave trace is transient, the use of significant wave<br />
height (H 1/3 or H m0 ) and average wave energy (energy per<br />
unit area) is ambiguous. While significant wave height<br />
deceptively suggests an average height throughout the<br />
wash trace, both values depend on the sample length and<br />
become smaller with large sample lengths <strong>for</strong> the same<br />
wash event. In general, using maximum wave height<br />
(H max ) and relating maximum wave period (T max ) and distribution<br />
of wave height and period through the entire<br />
wave trace, e.g., Fig. 3-5, are good measures to characterize<br />
the wake at a given location <strong>for</strong> risk assessment purposes.<br />
© COPYRIGHT <strong>PIANC</strong><br />
4. IMPACTS ASSOCIATED<br />
WITH VESSEL WAKE<br />
3.7.4 <strong>Wake</strong> analysis<br />
Due to the short period of the event and the large spreading<br />
of periods, wave data needs to be analysed in the fulltime<br />
domain on a wave-by-wave basis. Frequency domain<br />
analysis of super-critical wash using Fourier trans<strong>for</strong>ms is<br />
not recommended due to the low-frequency content of<br />
super-critical wash relative to the required sampling time<br />
4.1 OVERVIEW<br />
The objective of this section is to highlight some of the<br />
potential safety and environmental impacts associated<br />
with wake <strong>from</strong> high-speed vessels. Many of these impacts<br />
are based on reported incidents that have been attributed to<br />
17 Report of Working Group 41 - MARCOM
Some examples are discussed in Kofoed-Hansen and<br />
Mikkelsen (1997) and Marine Accident Investigation<br />
Branch report (2000). Although potential impacts associated<br />
with wake <strong>from</strong> high-speed vessels are a legitimate<br />
concern, it is important to note that many of the impacts<br />
discussed in this section are not unique to these vessels.<br />
<strong>Wake</strong> <strong>from</strong> other types of vessels can have the same, or<br />
very similar, impacts. Although every ef<strong>for</strong>t has been<br />
made to identify the most significant impacts, it is possi<br />
ble that there may be others.<br />
The potential <strong>for</strong> wake wash to have an adverse impact on<br />
safety or the environment is related to the physical characteristics<br />
of the waterway and adjacent shoreline as well as<br />
the characteristics of the wake. It is also related to how the<br />
wake interacts with the people and vessels that use the<br />
waterway, the structures that are built on, or near the<br />
waterway, and the near-shore flora and fauna. The implication,<br />
whether wake will have an adverse impact on safety<br />
or the environment, is site specific.<br />
4.2 SAFETY IMPACTS<br />
Safety impacts associated with wake generally involve:<br />
• People on or near the shoreline;<br />
• Vessels underway or moored; or,<br />
• Structures located in, on, or adjacent to the waterway.<br />
4.2.1 Safety of people<br />
<strong>Wake</strong> characteristics in combination with shoreline features<br />
and waterway topography can be used to identify<br />
potential impacts to the safety of people on or near the<br />
shoreline. In general, impacts involving people on or near<br />
the shoreline are primarily associated with transverse<br />
waves generated by vessels operating at or near critical<br />
speed and the long-period waves that comprise the first<br />
group of waves generated by vessels operating at supercritical<br />
speeds. Impacts that can be attributed to these<br />
waves based on shoreline characteristics are summarised<br />
in Table 4-1. Some of these impacts may be of more concern<br />
during certain times of the year, e.g., summer months<br />
when beaches are being used by bathers, or more pronounced<br />
during certain environmental conditions, e.g.,<br />
high or low tide or during calm weather, when large waves<br />
may be unexpected.<br />
4.2.2 Safety of vessels<br />
4.2.2.1 Overview<br />
Just as the characteristics of the wake generated by a vessel<br />
is related to its physical characteristics (e.g., length,<br />
beam, draft, displacement), how another vessel will be<br />
impacted by wake is related to its own physical characteristics<br />
(Bolt, 2002). How a vessel responds to wake also<br />
depends on how it is operated when wake is encountered<br />
and is there<strong>for</strong>e related to the knowledge and skill of the<br />
vessel’s operator. Consequently the specific risk to each<br />
vessel must be assessed individually. This is true regardless<br />
of the type of vessel that generated the wake.<br />
However, there are several general observations that can<br />
be made about wake generated by high-speed vessels or<br />
other vessels operating at or near critical speeds (MCA,<br />
2001):<br />
• All vessels are affected by some part of the near- or<br />
super-critical wash due to the wide range of wave periods<br />
(see Fig. 3-5).<br />
• Small craft are particularly at risk of being swamped,<br />
broached, or capsized by the steep, near breaking waves<br />
produced by vessels operating in the near-critical zone.<br />
© COPYRIGHT <strong>PIANC</strong><br />
Table 4-1 Impacts related to the safety of people based on shoreline characteristics<br />
(Kofoed-Hansen, 1996; MCA, 1998)<br />
Shoreline Characteristics Potential Risk Probable Cause<br />
Shallow sloping beach People may be caught in Rapid inundation of large<br />
water or knocked down areas <strong>from</strong> run up of long-period waves<br />
Moderate / steep People knocked down Plunging and breaking waves<br />
beaches, boat ramps<br />
Damage to boats and<br />
vehicles on ramp<br />
Shorelines with sea walls People on narrow beaches Rapid inundation of exposed beach<br />
trapped against sea wall <strong>from</strong> run up of long-period waves<br />
Breaking waves that overtop the seawall<br />
Report of Working Group 41 - MARCOM<br />
18
• Long period wash waves may cause large vessels to<br />
yaw and alter course, which in a confined channel can<br />
increase the risk of grounding, or when passing other<br />
vessels in close proximity can increase the risk of collision.<br />
• Maximum pitch motions are expected <strong>for</strong> most vessels<br />
when the super-critical wash is encountered as either<br />
head or following waves.<br />
• Maximum heave motions are expected <strong>for</strong> bigger vessels<br />
when the super-critical wash is encountered as<br />
beam waves.<br />
• <strong>Wash</strong> induced roll can increase the risk of grounding at<br />
the turn of the bilge of deep draft, wide beam vessels,<br />
such as container vessels, operating in confined channels<br />
with small under-keel clearances.<br />
• Orbital motions of fluid particles in shallow water are<br />
elliptical rather than circular so that a vessel’s horizontal<br />
motion is larger than its vertical motion.<br />
4.2.2.2 Vessels underway<br />
© COPYRIGHT<br />
<strong>Wake</strong> characteristics, in combination with the topography<br />
of the waterway, can be used to identify potential impacts<br />
to the safety of vessels. In general, impacts related to the<br />
safety of vessels are primarily associated with transverse<br />
waves generated by vessels operating at or near critical<br />
speed as well as the long-period waves comprising the first<br />
<strong>PIANC</strong><br />
group of waves and the short-period waves comprising the<br />
third group of waves generated by vessels operating at<br />
super-critical speeds. Impacts to vessels that can be attributed<br />
to these waves are summarised in Table 4-2. Some of<br />
these impacts may be more pronounced during certain<br />
environmental conditions (e.g., calm weather, high or low<br />
tide, or certain times of year when large numbers of small,<br />
recreational vessels are using a waterway).<br />
4.2.2.3 Vessels on moorings and in harbours<br />
The wave pattern reaching moored vessels is usually more<br />
complicated compared to open water due to the influence<br />
of coastal structures and the local bathymetry. The angle<br />
of propagation is due to wave refraction, reflection, and<br />
diffraction around solid obstacles and, unless the berth is<br />
open to the incoming waves, these changes need to be considered.<br />
The wavelength can be shorter due to diffraction,<br />
which can increase the height at the same time. Potential<br />
impacts of wake on moored vessels are summarized in<br />
Table 4-3.<br />
4.2.3 Structural damage<br />
The effect of wake on floating structures depends on the<br />
response characteristics of the object. Consequently the<br />
risk to each structure must be assessed individually. Of<br />
particular concern is the possibility that the waves will<br />
cause excessive movement of floating structures. There is<br />
also the possibility that the impact of breaking waves may<br />
undercut pier footings.<br />
Table 4-2 Impacts related to the safety of vessels (Kofoed-Hansen, 1996; MCA, 1998)<br />
Waterway Topography Potential Impact Probable Cause<br />
Open water Small craft may be swamped, Waves generated by vessel operating at<br />
broached or capsized<br />
critical speed, or short-period, high-amplitude<br />
waves in the third set of waves<br />
Larger vessels may have<br />
difficulty maintaining course<br />
Long-period waves can cause<br />
larger vessels to yaw<br />
Harbour or estuary Vessels with small under keel Long-period waves result in considerable<br />
entrances with clearances may ground seiching over large areas with shallow water<br />
shallow bars<br />
Small craft may have<br />
difficulty maintaining course<br />
<strong>Wash</strong> generated by vessels operating at<br />
trans- and super-critical speeds can create an<br />
oscillating current over bars and shallow banks<br />
Shallow banks (
Table 4-3 Potential impacts on moored vessels (MCA, 2001)<br />
Activity Potential Impact Probable Cause<br />
Moored vessels Excessive movement Transverse waves generated by vessels operating<br />
(surge, heave and roll) may at or near trans-critical speeds and both<br />
cause moorings to fail, damage long-period and tail waves generated by vessels<br />
to vessels as well as docks and operating at super-critical speeds<br />
piers, vessels to touch bottom<br />
Vessels with small under keel<br />
clearance may ground<br />
Long-period waves result in considerable<br />
seiching over large areas with shallow water<br />
Loading / discharging cargo Disruption of cargo operations Long-period waves generated by vessels operating<br />
that are sensitive to vessel at super-critical speeds<br />
movement<br />
Vessels alongside a moored Damage to either or both vessels Transverse waves generated by vessels operating<br />
vessel (tugs, bunker barges, due to large relative motion due at or near trans-critical speeds and both<br />
etc.) to different response to waves long-period and tail waves generated by vessels<br />
operating at super-critical speeds<br />
4.2.3.1 Historic and archaeological monuments<br />
The possibility of damage to sites of cultural significance,<br />
including historic monuments and archaeological sites, on<br />
the seabed (such as old historical sites and wrecks), and<br />
the shoreline (<strong>for</strong>ts and other historical sites) is prevalent<br />
in several countries including Denmark, New Zealand, and<br />
Sweden. For example, in the archipelago of Göteborg,<br />
Sweden, many bays are sheltered <strong>from</strong> large wind waves<br />
and the tide is minimal. After the introduction of highspeed<br />
ferries a several-hundred-year-old burial ground <strong>for</strong><br />
sailors close to the sea was threatened by wake erosion.<br />
Although the erosion was halted in 1997 when the speed<br />
of the fast ferries was limited, there is evidence suggesting<br />
that wake <strong>from</strong> large container ships may be a heavier<br />
threat (Svensson, 1999).<br />
4.3 ENVIRONMENTAL<br />
IMPACT OF WAKE<br />
© COPY-<br />
4.3.1 Overview<br />
All waves, whether generated by the wind or a vessel, can<br />
have some impact on the marine environment. As indicated<br />
in Section 4.3.2, there are characteristics of high-speed<br />
vessel wake that contribute to its higher propensity vis-àvis<br />
wake <strong>from</strong> other vessels to impact the marine environment.<br />
However, <strong>for</strong> the reasons raised in Section 4.3.4 it<br />
cannot be assumed a priori that high-speed vessel wake is<br />
the cause of any adverse impacts to the marine environment<br />
that might be observed in areas where these vessels<br />
are operating. Determining the cause of adverse impacts<br />
RIGHT<br />
<strong>PIANC</strong><br />
to the marine environment that are observed in a given<br />
area requires detailed, local studies.<br />
The severity of any environmental impact caused by wake<br />
will depend on how the wash regime differs <strong>from</strong> the natural<br />
wave climate. It is also dependent on the susceptibility<br />
of the recipient shores to wave attack. Naturally sheltered<br />
environments and soft sedimentary shores are more<br />
likely to be adversely impacted than naturally exposed<br />
environments with rocky shores.<br />
The available literature on the ecological impacts of highspeed<br />
vessel wake is limited insofar as most studies have<br />
focused on the wash generated by watercraft other than<br />
high speed vessels, i.e. conventional ferries, boats, and<br />
personal water craft (jet skis and wave riders). However,<br />
the studies that have been conducted are useful since they<br />
highlight potential effects of high-speed vessel wake on<br />
the marine environment.<br />
4.3.2 Potential impacts<br />
4.3.2.1 Physical change<br />
In general, an increase in wave action, whether <strong>from</strong> natural<br />
causes (e.g., storm events) or vessel wake will result<br />
in higher energy within the coastal system. This increase<br />
can result in an adjustment to the beach environment<br />
including beach orientation, erosion, accretion, and<br />
increasing the envelope of dynamic change in the attainment<br />
of a new equilibrium to the wave conditions. One<br />
factor influencing the vulnerability of a shoreline to being<br />
changed by waves is its morphological state. In general,<br />
Report of Working Group<br />
41 - MARCOM<br />
20
a stable shoreline is less vulnerable to attack than one that<br />
has been previously disturbed, either because of prior<br />
storm events or human activity (e.g., shoreline construction<br />
or sediment removal). The vulnerability of a coastal<br />
zone to wave attack is also dependent upon its material<br />
composition and typical particle size.<br />
The addition of energy to the system <strong>from</strong> wake can cause<br />
sediment mobilisation and accelerated weathering of<br />
rocky shores. The probable wake related causes of these<br />
impacts are summarised in Table 4-4.<br />
© COPY-<br />
Changes to the physical environment, with particular<br />
emphasis on sediment transport, can cause a variety of different<br />
environmental impacts. Mobilisation of larger sediments<br />
can result in rapid changes to biological communities.<br />
Sedentary organisms may be relocated, crushed, and<br />
damaged as the rocks and boulders on which they are<br />
attached are rolled around. Resuspension of finer sediments<br />
can create an abrasive environment that may damage<br />
soft-bodied animals and algae and prevent spores <strong>from</strong><br />
settling. When sediments do settle out, they can potentially<br />
smother benthic organisms and cover fish eggs and<br />
spawning grounds. Aquatic plants can be physiologically<br />
RIGHT<br />
impaired if their surfaces are covered with silt.<br />
Resuspension of sediments also increases the turbidity of<br />
the water, and by blocking the light that reaches the bottom<br />
can have an adverse impact on benthic organisms.<br />
<strong>PIANC</strong><br />
4.3.2.2 Impacts on flora and fauna<br />
The flora and fauna that inhabit coastal environments are<br />
subject to inundation as well as the hydrodynamic <strong>for</strong>ces<br />
associated with both wind and vessel generated waves.<br />
Waves are a primary agent of ecological disturbance that<br />
affect individuals, populations, and communities to varying<br />
degrees. The potential biological impacts of wake on<br />
coastal and shoreline habitats, which are summarised in<br />
Table 4-5, are a consequence of changes to the natural<br />
physical environment or natural wave climate. Without<br />
external influences, near-shore and intertidal habitats may<br />
exist in a state of long-term equilibrium. Although an<br />
increase in the energy within a coastal system by introducing<br />
vessel wake can be sufficient to upset the equilibrium<br />
(Kirk McClure Morton, 2000), it is usually difficult<br />
to assess changes caused by a changed wave regime due to<br />
vessel wake.<br />
Table 4.4 Physical impacts of vessel wake<br />
(Bell et al., 2000; Kirk McClure Morton, 2000; Single, 2002)<br />
Potential Impact<br />
Probable Cause<br />
Sediment Transport<br />
Sediment resuspension<br />
and associated increase<br />
in turbidity<br />
Cross-shore and long-shore<br />
transport of bottom sediment<br />
and associated accretion<br />
or erosion<br />
Weathering of Rocky Shores<br />
Long-period waves penetrate deeper into the water column than<br />
shorter-period waves and can disturb bottom sediments farther<br />
off-shore than would likely occur under normal conditions.<br />
Large, steep waves similar to storm generated waves can move sediment<br />
seaward; if they attack the beach at an angle, the material will be transported<br />
along the shore. Short, steep waves may transport material onto higher<br />
sections of the beach. Depending on the angle of attack, wake wash<br />
encountering the shore can result in either cross-shore or long-shore transport<br />
of sand and other shoreline material. Large, steep waves, similar to those<br />
generated by storm waves, can move material seaward and <strong>for</strong>m a bar<br />
in front of the beach. If the waves attack the beach at an angle,<br />
the material will be moved along the beach. Short, steep waves can move<br />
material higher up on the beach. <strong>High</strong>-speed vessel wake wash has been<br />
observed to result in both accretion and erosion.<br />
The impact of the incoming wave and the resulting fluctuations in cracks<br />
can separate layers of rock <strong>from</strong> the bedrock. Laboratory measurements suggest<br />
that regular waves, e.g., vessel wake wash, generate higher crack pressures<br />
than mixed waves, e.g., wind generated waves, of similar magnitude.<br />
Hence the weathering of rocky shores by the leading waves of the wake<br />
<strong>from</strong> high-speed vessels may be larger than the weathering induced<br />
by comparable natural seas.<br />
21 Report of Working Group 41 - MARCOM
Table 4-5 Biological impacts of vessel wake<br />
(Danish Maritime Institute, 1997; Bell et al., 2000; Hotchkiss et al., 2002)<br />
Potential Impact<br />
Probable Cause<br />
Fixed and mobile organisms may be dislodged and stranded;<br />
plants may be broken and or uprooted. Overtime species<br />
distribution within the intertidal and near shore zone may change;<br />
some species may be removed<br />
Smothering of plants, sedimentary animals, and spawning grounds<br />
Loss of sea grasses<br />
Altered distribution of species within the intertidal zone<br />
Localized algal blooms and associated increase in turbidity<br />
Reduced productivity and loss of bird nesting areas; change in<br />
feeding behaviour of birds, lower over wintering survival rates<br />
Reduced productivity of seal rookeries; loss of haul-out areas<br />
Waves with higher than ambient energy<br />
due to wake wash breaking on individual<br />
plants and animals. Sediment mobilisation<br />
can damage individual organisms as well as<br />
cause habitat loss.<br />
Settling out of fine, suspended sediment<br />
Turbidity <strong>from</strong> sediment mobilisation can<br />
reduce the amount of light reaching<br />
the bottom<br />
Increased immersion due to regular<br />
inundation of intertidal zone<br />
Resuspension of nutrients associated with<br />
sediment mobilisation<br />
Beach nesting and shoreline feeding areas<br />
inundated by run up of long period waves;<br />
cliff nesting areas inundated by<br />
breaking waves<br />
Inundation by breaking waves<br />
4.3.3 Differentiating between causes<br />
Although high-speed vessels (e.g., high-speed ferries)<br />
have been in operation <strong>for</strong> over ten years, relatively little is<br />
known about the impact of their wake on the marine environment<br />
vis-à-vis the wake <strong>from</strong> other types of vessels.<br />
This is mainly due to the difficulty of distinguishing<br />
between impacts that result <strong>from</strong> different causes including<br />
normal wind generated waves, storms, high-speed and<br />
non high-speed vessel wake, and other human activities.<br />
Making such a distinction is particularly difficult since the<br />
coastal environment naturally is always undergoing some<br />
change (Kirk McClure Morton, 2000).<br />
4.3.4 Predicting environmental impact<br />
© COPY-<br />
Even though most coastal areas are always undergoing<br />
some change, the physical and biological environment of<br />
a beach or a coastline generally is shaped by the predominant<br />
wave climate, which is the product of both regular<br />
wind and storm generated waves as well as vessel wake.<br />
Hence, if the wave climate changes significantly, it is reasonable<br />
to expect that the coastline and its physical and<br />
biological properties will also change, although it is not<br />
always immediately apparent how the change will become<br />
Report of Working Group 41<br />
- MARCOM<br />
RIGHT<br />
manifest. The implication is that any ef<strong>for</strong>t to assess how<br />
high-speed vessel wake may impact the marine environment<br />
will require the comparison of data obtained both<br />
be<strong>for</strong>e and after a particular shoreline is exposed to wake<br />
<strong>from</strong> these vessels. It should be noted that in many cases<br />
the physical impact could be initially large and then<br />
become more stable; there<strong>for</strong>e, any assessed impacts<br />
based on initial trends could possibly result in overestimating<br />
the impact. Although models can be developed to<br />
help predict how wake might impact a particular shoreline,<br />
given the complexity of shoreline systems, model results<br />
should not be generalized to similar shorelines in other<br />
areas (Bell et al., 2000).<br />
5. MANAGING VESSEL WAKE<br />
<strong>PIANC</strong><br />
5.1 INTRODUCTION<br />
Concern about the potential safety and environmental<br />
impact of high-speed vessel wake are causing high-speed<br />
vessel operators and waterway managers to establish<br />
either voluntary or mandatory management measures.<br />
Establishing effective management measures <strong>for</strong> highspeed<br />
vessel wake requires an understanding of the causal
elationship between a vessel’s wake and its actual or<br />
potential impact. As discussed in Sections 3 and 4, establishing<br />
this causal relationship is a multi-faceted problem<br />
that requires understanding how wake interacts with other<br />
vessels, people, structures, and near-shore flora and fauna<br />
as well as the bottom and shoreline of the waterway. This<br />
requires knowledge of the physical characteristics of the<br />
wake generated by the vessel as well as how the wake is<br />
affected by the physical characteristics of the waterway as<br />
it propagates away <strong>from</strong> the vessel’s line of travel and<br />
shoals to break at the shore. It also requires understanding<br />
the effect of the management measures that are considered<br />
on wake generation to ensure that the measures implemented<br />
will be effective and that they will not result in<br />
unintended consequences. The implication is that there is<br />
not a simple, universal solution <strong>for</strong> managing high-speed<br />
wake insofar as how wake interacts with the physical environment<br />
and human activities is site specific. In addition,<br />
there are differences in the wake generated by different<br />
hull <strong>for</strong>ms and sizes and operating speeds – differences<br />
that may permit alternative ways of mitigating the potential<br />
impact.<br />
5.2 MANAGEMENT MEASURES<br />
Mitigation measures can be divided into three categories:<br />
vessel design, operational measures, and non-operational<br />
measures. It is likely that the management regime adopted<br />
<strong>for</strong> any given route will involve a combination of operational<br />
and non-operational measures.<br />
5.2.1 Vessel design<br />
Insofar as the wake generated by a vessel is directly related<br />
to its hull <strong>for</strong>m, vessel design is a primary means of<br />
managing wake. Although it is possible to modify a vessel<br />
after it is constructed (e.g., increasing its length or<br />
installing trim tabs or interceptors) to improve the characteristics<br />
of the wake that is generated, the cost of doing so<br />
may be prohibitive. Similarly, modifications may be prohibited<br />
by regulatory requirements or physical constraints.<br />
There<strong>for</strong>e, naval architects should understand the potential<br />
implications of the wake generated by a given hull design<br />
<strong>for</strong> wake management and consider any wash criteria<br />
related to the intended route including design requirements,<br />
along with emissions, speed, and other limiting factors.<br />
There are, however, key features of high-speed vessel<br />
wake that cannot be reduced or removed by optimising<br />
the hull <strong>for</strong>m and design ratios. An example is the wave<br />
period, which generally increases with vessel speed and<br />
distance <strong>from</strong> the navigation line and is a particularly<br />
important parameter in wave impact in shallow water<br />
areas.<br />
5.2.2 Operational measures<br />
Operational measures can be used to reduce both the safety<br />
and environmental impacts of wake. Because the potential<br />
impacts of wake are related to the physical characteristics<br />
of both the vessel and the waterway, operational<br />
measures are generally related to the route or the vessel’s<br />
operational profile. Insofar as ferry routes are a function<br />
of geography, it is usually not possible to reduce potential<br />
impacts by selecting an alternate route. However, there are<br />
some changes that might be possible, including<br />
• Moving a route farther <strong>from</strong> shore to increase the distance<br />
between the vessel’s track and the area where<br />
wake impacts are of concern.<br />
• Establishing route segments so that changes in water<br />
depth do not cause the vessel to transition <strong>from</strong> subcritical<br />
or super-critical speeds into the critical speed<br />
range.<br />
• Relocating where course or speed changes are made to<br />
avoid focusing wake at a particular location or to avoid<br />
generating wash associated with the critical speed<br />
range.<br />
• Altering the orientation of a route relative to the shoreline<br />
to change the angle at which the wake encounters<br />
an area of concern.<br />
• Modifying the schedule to reduce the potential <strong>for</strong><br />
impacts that may be associated with predicable shoreline<br />
use or environmental factors (e.g., tide or sustained<br />
winds <strong>from</strong> a particular direction).<br />
Although the characteristics of the wake generated by a<br />
vessel are a function of the hull <strong>for</strong>m and cannot be altered<br />
unless the vessel undergoes modifications after it is constructed,<br />
there are several operational measures related to<br />
the vessel’s operational profile that can be used to reduce<br />
the potential impacts of vessel wake. These include<br />
© COPYRIGHT <strong>PIANC</strong><br />
• Training vessel masters and mates so that they understand<br />
the relationship between the navigation of the<br />
vessel and the generation of wake.<br />
• Ensuring that the navigation of the vessel con<strong>for</strong>ms<br />
with the courses and speeds established <strong>for</strong> each leg of<br />
the route.<br />
• Ensuring that the vessel is trimmed on each run to minimize<br />
the wake that is generated.<br />
• Establishing contingency plans <strong>for</strong> situations (e.g., loss<br />
of engine power), or other situations when it may not be<br />
possible to follow normal operating procedures.<br />
23 Report of Working Group 41 - MARCOM
5.2.3 Non-operational measures<br />
The intent of non-operational management measures is to<br />
reduce safety related impacts of wake by lessening the<br />
potential <strong>for</strong> people and small craft to interact directly<br />
with wake. Some non-operational measures include:<br />
• Posting signs on shore or including notices on navigation<br />
charts in areas where high-speed vessel wake<br />
might reasonably be encountered.<br />
• Engaging in outreach activities to ensure the public is<br />
aware of the potential impacts associated with wake.<br />
• Designing new sea walls and quay walls or retro-fitting<br />
existing ones with wave absorbing materials to reduce<br />
wave amplification by reflection. And,<br />
• Coordinating with other operators and harbour authorities<br />
or owners to identify impacts and means of mitigation.<br />
Non-operational measures intended to in<strong>for</strong>m the public<br />
are particularly important in areas where wake <strong>from</strong> highspeed<br />
vessels is not actively managed or is a new activity.<br />
5.3 ROUTE ASSESSMENT<br />
5.3.1 Overview<br />
Developing appropriate management measures <strong>for</strong> highspeed<br />
vessel wake requires identifying the potential safety<br />
and environmental impacts the wash may have. This<br />
requires ensuring that the interrelationship of wake generation,<br />
trans<strong>for</strong>mation, and impact is understood. Since the<br />
impacts that may occur are the result of a number of factors,<br />
including wake generation and trans<strong>for</strong>mation, the<br />
physical characteristics of the waterway and its shoreline,<br />
as well as how the waterway and shoreline are used, this<br />
interrelationship is route dependent. The route assessment<br />
is an objective, systematic process <strong>for</strong> identifying potential<br />
impacts and <strong>for</strong> developing management measures that<br />
may be implemented by vessel operators and waterway<br />
managers that are appropriate <strong>for</strong> a particular route.<br />
© COPYRIGHT <strong>PIANC</strong><br />
A route assessment is intentionally flexible so that it can<br />
be applied to different waterways and different vessels. It<br />
is also flexible with regard to the outcome. In other words,<br />
it does not favour one measure <strong>for</strong> reducing potential wake<br />
impacts over any other. Similarly, whereas in some<br />
instances a single management measure may be sufficient<br />
to prevent an impact <strong>from</strong> occurring, there may be other<br />
cases where a suite of different measures may be needed.<br />
Another aspect of the model is that it is scaleable so the<br />
level of ef<strong>for</strong>t is appropriate <strong>for</strong> the safety and environmental<br />
impacts being considered. The process involves<br />
four steps:<br />
1. Characterizing the route.<br />
2. Identifying the potential impacts and severity of wake.<br />
3. Developing and assessing potential management measures.<br />
4. Implementing and monitoring management measures.<br />
Conducting a route assessment requires an understanding<br />
of specific vessel and route variables. The in<strong>for</strong>mation<br />
needed to conduct the route assessment can be grouped<br />
into five general areas:<br />
1. The characteristics of the vessel’s wake in its entire<br />
operational envelope.<br />
2. The bathymetry and shoreline topography of the proposed<br />
route.<br />
3. Waterway activities along the route.<br />
4. Shore activities along the route.<br />
5. Properties of the physical and biological environment<br />
of the adjacent coastline.<br />
5.3.2 Route characterization<br />
Route characterization involves dividing the planned route<br />
or routes, if alternatives are available, into segments.<br />
Although there are a number of ways this can be accomplished,<br />
the most practical approach is to segment the<br />
route according to where the vessel will be operating at<br />
sub-critical, near-critical, and super-critical speeds based<br />
on the ranges of depth Froude numbers described in<br />
Figure 5-1. In addition, deep-water operation might be<br />
segmented by ‘conventional low speed’ and ‘high speed<br />
sub-critical’ speeds (MCA, 1998). Stumbo et al. (2000)<br />
have observed that in deep water the transition <strong>from</strong> conventional<br />
low speed to high speed sub-critical speed<br />
occurs when vessels have a length Froude number<br />
between 0.65 and 0.9. Using depth Froude numbers, and<br />
length Froude numbers when appropriate, to segment the<br />
route provides a means of conducting a first order assessment<br />
of potential wake impacts along a planned route. It<br />
may identify places where some change to the route (e.g.,<br />
a speed or course change), may eliminate or at least significantly<br />
reduce some of the potential wake impacts.<br />
Report of Working Group 41 - MARCOM<br />
24
Figure 5-1 Operational zones <strong>for</strong> route characterization based on wash regimes<br />
©<br />
5.3.3 Impact identification<br />
Once the route is divided into segments, the type and location<br />
as well as the likelihood and severity of the potential<br />
impacts that wake may have on each segment of the route<br />
must be identified. It is also necessary to identify the<br />
aspect of wake that may cause the impact and then determine<br />
whether wake <strong>from</strong> high-speed vessels is a primary,<br />
secondary, or tertiary cause of the identified impact.<br />
5.3.3.1 Identifying potential impacts<br />
Identifying potential wake impacts requires first ascertaining<br />
who, (e.g., swimmers or people near the shore), or<br />
what, (e.g., small-craft underway or moored in marinas,<br />
near-shore or coastal marine habitats, or waterfront structures)<br />
may be impacted. It also requires determining the<br />
locations where wake impacts can reasonably be expected<br />
to occur. The description of where an impact may occur<br />
should include some reference to the shoreline (e.g., offshore,<br />
near-shore, on-shore), as well as a geographic reference<br />
(e.g., the name of a location or other landmark).<br />
Although latitude and longitude may be useful <strong>for</strong> providing<br />
more precise locations, the use of common names provides<br />
a means to quickly identify areas where wake may<br />
have an adverse impact.<br />
COPY-<br />
RIGHT<br />
Identifying potential wake impacts requires understanding<br />
of how the waterway is used as well as in<strong>for</strong>mation about<br />
the characteristics of the waterway’s natural and physical<br />
environment. There are any number of ways that this can<br />
be accomplished, including site surveys and meeting with<br />
representatives of different waterway users, natural<br />
resource agencies, and land owners. It is likely that the<br />
level of ef<strong>for</strong>t required to identify potential safety and<br />
environmental impacts will vary between routes and<br />
between different segments of the same route. Regardless<br />
of the means and level of ef<strong>for</strong>t employed, it is important<br />
that the result is a complete picture of the type and location<br />
of the potential safety and environmental impacts that<br />
wake may have on each segment of the route.<br />
When identifying potential impacts, it is helpful to establish<br />
when a particular impact may occur. Determining<br />
when an impact might occur is needed <strong>for</strong> determining the<br />
frequency that high-speed vessel wake might cause a<br />
potential impact. It also might help to highlight possible<br />
causal relationships that have to exist <strong>for</strong> an impact to<br />
occur (e.g., state of the tide or sustained winds <strong>from</strong> a<br />
given direction). Several different timeframes can be used<br />
when identifying when an impact might occur. Whereas<br />
some potential impacts might occur multiple times a day,<br />
others might occur infrequently, <strong>for</strong> example, those that<br />
are related to seasonal weather patterns. Establishing the<br />
timeframe might also help highlight impacts that are not<br />
exclusively related to wake <strong>from</strong> high-speed vessels.<br />
<strong>PIANC</strong><br />
Report of Working Group 41 - MARCOM
Table 5-1 Likelihood and consequence scores<br />
Likelihood<br />
Score Description Examples<br />
5 Very Likely Every passage<br />
4 Likely Most passages<br />
3 Quite Possible <strong>High</strong> tide during passage<br />
2 Possible During storms or other periodic<br />
environmental conditions<br />
1 Unlikely Only during unusual /<br />
unpredictable circumstances<br />
Consequence<br />
Score Description Examples<br />
5 Very <strong>High</strong> Unacceptable impact, people may receive<br />
serious injuries or die, small craft cannot<br />
navigate safely, waterfront structures cannot<br />
be occupied / used, marine environment<br />
disrupted<br />
4 <strong>High</strong><br />
3 Moderate Noticeable impact, people may be injured,<br />
moored vessels or waterfront structures may<br />
be damaged, marine environment likely<br />
to be damaged<br />
2 Slight<br />
1 Minimal No noticeable impact, use of shoreline /<br />
waterway not interrupted, any damage<br />
to marine environment is minimal<br />
©<br />
5.3.3.2 <strong>Wake</strong> components<br />
To develop appropriate management measures it is necessary<br />
to determine both the component of wake (i.e., wave<br />
height, wave length, energy, and the magnitude of the<br />
high-speed vessel’s wake) in terms of characteristic wave<br />
height/energy, wave period/length and wave direction that<br />
might be expected to cause each of the potential impacts<br />
that are identified. In some instances there may be more<br />
than one component that might be of concern. Failure to<br />
identify the component, or components, of wake that reasonably<br />
can be expected to cause a potential impact can<br />
result in developing management measures that are not<br />
appropriate.<br />
5.3.3.3 Likelihood and consequence of potential impacts<br />
COPY-<br />
After the potential impacts and the responsible component<br />
of high-speed vessel wake have been identified, it is necessary<br />
to assess both the likelihood that a particular impact<br />
will occur and its potential consequence. Suggested scales<br />
<strong>for</strong> assigning likelihood and consequence scores are<br />
shown in Table 5-1. It is recognized that the descriptions<br />
and definitions <strong>for</strong> the different scores are somewhat subjective.<br />
This is unavoidable since, <strong>for</strong> the most part, there<br />
RIGHT<br />
Report of Working Group 41 - MARCOM<br />
will be limited site-specific data available upon which to<br />
base assessment. There<strong>for</strong>e, the assessment must be based<br />
on the best available in<strong>for</strong>mation and the experience of<br />
those who are conducting it.<br />
<strong>PIANC</strong><br />
26<br />
5.3.3.4 How important is wake<br />
Once the preceding steps have been completed, a determination<br />
should be made whether high-speed vessel wake is<br />
a primary, secondary, or tertiary cause of the potential<br />
impacts that are identified. Making such a determination<br />
is necessary to help provide some basis <strong>for</strong> establishing the<br />
extent to which a high-speed vessel operator should reasonably<br />
be expected to be responsible <strong>for</strong> preventing a<br />
potential impact <strong>from</strong> occurring. Making this determination<br />
will require having an understanding of the impacts<br />
that may be caused by other vessels as well as those that<br />
result <strong>from</strong> natural processes. It will also require an<br />
understanding of the physical differences of waves generated<br />
by other vessels as well as those generated by natural<br />
processes vis-à-vis those generated by high-speed vessels.<br />
As discussed in Section 4.3.3, it is recognized that it may<br />
not always be possible to make this determination with a<br />
high degree of certainty.
5.3.3.5 Priority<br />
Since it may not be reasonable to develop mitigation measures<br />
<strong>for</strong> every potential impact, it is necessary to establish<br />
a prioritised list of those that are identified. An initial prioritised<br />
list can be established based on an index number<br />
(I n ) calculated using the following equation:<br />
L<br />
I n = s x C s<br />
,<br />
CF s<br />
where L s is the likelihood score, C s is the consequence<br />
score and CF s is the causal factor score. CF s values are<br />
provided in Table 5-2. An example of potential management<br />
actions based on the index number is provided in<br />
Table 5-3.<br />
5.3.4 Developing and assessing potential<br />
management measures<br />
<strong>PIANC</strong><br />
© COPYRIGHT<br />
5.3.4.1 Overview<br />
The route assessment is the foundation of any measures<br />
that are developed to managing wake. To be effective, the<br />
management measures that are employed should reduce<br />
the identified impact by<br />
• Focusing on the component of wake that is responsible<br />
<strong>for</strong> the potential impact; and<br />
•<br />
Ensuring the magnitude of the component that is of<br />
concern is maintained within acceptable limits.<br />
In addition, management measures should be appropriate<br />
<strong>for</strong> the location where they will be implemented.<br />
Management measures may be mandated by government<br />
agency regulations, company operating policies, or both.<br />
Establishing management measures should involve agencies<br />
responsible <strong>for</strong> waterways management, vessel operators,<br />
and effected stakeholders.<br />
5.3.4.2 Establishing management measures<br />
The first step in the process of developing a management<br />
regime <strong>for</strong> wake is to determine whether there is adequate<br />
data available to establish a maximum value or standard<br />
<strong>for</strong> the component or components that are of concern that<br />
Table 5-2 Causal factor scores<br />
Causal Factor Score (CF s )<br />
Description<br />
1 <strong>High</strong>-speed vessel wake wash is the primary cause of the impact<br />
2 <strong>High</strong>-speed vessel wake wash is a secondary cause of the impact<br />
3 <strong>High</strong>-speed vessel wake wash is a tertiary cause of the impact<br />
Table 5-3 Index numbers and recommended actions (MCA, 1998)<br />
Index Number (I n )<br />
Recommended Action<br />
1-5 Minimal No mitigation required<br />
6 – 10 Acceptable No mitigation required. Monitoring is required to ensure controls<br />
are maintained.<br />
11 - 15 Moderate Mitigation is required, but the costs of prevention may be taken into<br />
account. Mitigation measures should be implemented within a defined<br />
period. Monitoring is also required. Where moderate risk is associated<br />
with high or very high consequences further assessment may be necessary<br />
to establish more precisely the likelihood of harm as basis <strong>for</strong> determining<br />
the need <strong>for</strong> mitigation.<br />
16 - 20 Significant Vessel should not operate on route until risk has been reduced.<br />
21 -25 Unacceptable Vessel should not operate on route until risk has been reduced.<br />
If it is not possible to reduce risk even with unlimited resources,<br />
the vessel should be prohibited <strong>from</strong> operating on the route.<br />
27 Report of Working Group 41 - MARCOM
cannot be exceeded when measured at a specified location<br />
(e.g., a minimum water depth or distance <strong>from</strong> the shoreline).<br />
The ultimate responsibility <strong>for</strong> making this determination<br />
resides with the agencies responsible <strong>for</strong> waterways<br />
management. However, vessel operators and effected<br />
stakeholders should participate in this process.<br />
Insofar as the route assessment may identify a number of<br />
different wake related impacts that are of concern, a single<br />
standard may not be appropriate <strong>for</strong> the entire route.<br />
There<strong>for</strong>e, to avoid overprotecting some portions of a<br />
route while not providing enough protection along other<br />
portions, it will be necessary to establish different standards<br />
<strong>for</strong> different portions of a route. This is particularly<br />
true if the identified impacts are related to different components<br />
of wake. An advantage of standards is that compliance<br />
can be verified by measuring the wake. However,<br />
it is probable that in many areas sufficient data may not be<br />
available to establish a standard or set of standards. In<br />
these instances, it is necessary to either establish a value<br />
based on the best available data <strong>for</strong> the component of wake<br />
that is of concern or, if the data cannot support a standard,<br />
establish general criteria to minimize the potential that<br />
wake will have an adverse impact on safety or the marine<br />
environment.<br />
Many areas where high-speed vessels have been introduced<br />
have had conventional commercial vessel traffic <strong>for</strong><br />
some time, and the environment is likely to have been<br />
modified by wakes <strong>from</strong> those vessels as well as by<br />
numerous other human activities and natural processes. In<br />
most cases the wakes of conventional vessels generally<br />
cause few complaints, presumably due to familiarity over<br />
time. For such locations the wake <strong>from</strong> conventional commercial<br />
vessels may be used as a reference <strong>for</strong> establishing<br />
a standard <strong>for</strong> high-speed vessel wake.<br />
Despite the fact that wake generated by high-speed vessels<br />
is substantially different <strong>from</strong> wash caused by conventional<br />
ships and ferries, the choice of a standard should reflect<br />
a connection between these two types of wake.<br />
Characteristic measures such as wave energy (Stumbo et<br />
al., 1999), maximum wave height prior to breaking<br />
(Kofoed-Hansen, 1996; Parnell and Kofoed-Hansen,<br />
2001), particle velocity at the seabed, and wave run-up on<br />
the shorelines can be used in a <strong>for</strong>mulation of standard.<br />
Standards based on this approach have been implemented<br />
in Denmark, Sweden, New Zealand, and the United States.<br />
© COPYRIGHT <strong>PIANC</strong><br />
After acceptable standards or criteria have been established,<br />
the next step is to identify an appropriate suite of<br />
management measures. It is likely that this suite will<br />
include both operational and non-operational measures.<br />
Since the measures that may be employed to comply with<br />
the established standards and criteria are linked directly to<br />
the vessel and its operation, vessel operators should have<br />
the primary responsibility <strong>for</strong> identifying specific management<br />
measures. However, it is expected that the management<br />
measures will be subject to review by the agency<br />
responsible <strong>for</strong> waterways management.<br />
Once potential management measures are identified, new<br />
likelihood, consequence, and causal factor scores should<br />
be assigned and the index number recalculated to determine<br />
whether it is within an acceptable level <strong>for</strong> the vessel<br />
to operate on the route in question.<br />
5.3.5 Monitoring<br />
A monitoring program should be developed to determine<br />
whether the management measures that are implemented<br />
are effective in preventing or reducing impacts associated<br />
with wake. Although the details of the monitoring program<br />
are site specific, at a minimum the program should<br />
provide a means of determining or verifying whether wake<br />
<strong>from</strong> high-speed vessels is having adverse impacts on<br />
safety or the marine environment. In some instances, this<br />
will require having access to baseline data so that impacts<br />
that occur over time (e.g., shoreline erosion or habitat<br />
degradation), can be detected. It may also be necessary <strong>for</strong><br />
the monitoring program to provide data that can be used to<br />
differentiate between impacts associated with high-speed<br />
vessel wake and impacts associated with wake <strong>from</strong> other<br />
vessels or natural processes. This is particularly important<br />
<strong>for</strong> impacts where high-speed vessel wake is considered to<br />
be a secondary or tertiary factor.<br />
6. CONCLUSION<br />
The characteristics of wake <strong>from</strong> high-speed vessels are<br />
fundamentally different <strong>from</strong> the wake generated by ‘conventional’<br />
displacement vessels. Although wake <strong>from</strong> any<br />
type of vessel can potentially have adverse impacts on<br />
waterway safety or the marine environment, wake <strong>from</strong><br />
high-speed vessels has received a significant amount of<br />
attention in countries around the world. In addition to<br />
concerns about the potential safety and environmental<br />
impacts of high-speed vessel wake, there is also concern<br />
that ef<strong>for</strong>ts to manage wake might result in the development<br />
of standards that are inappropriate and which might<br />
also unduly restrict the operation of these vessels. As a<br />
result, vessel operators and waterway managers alike have<br />
tried a number of different approaches <strong>for</strong> managing highspeed<br />
vessel wake.<br />
Based on the experience to date <strong>from</strong> these different<br />
ef<strong>for</strong>ts, it is apparent that the effective management of<br />
high-speed vessel wake is a multi-faceted problem that<br />
defies a simple “one size fits all” solution. It is also apparent<br />
that a means of managing high-speed vessel wake that<br />
addresses the legitimate concerns related to waterway<br />
safety and protection of the marine environment while also<br />
not unduly restricting their operation must be identified <strong>for</strong><br />
the full benefits of high-speed vessels to be realized.<br />
Waterway managers and high-speed vessel operators are<br />
encouraged to follow the guidelines <strong>for</strong> conducting a route<br />
assessment and developing management measures that are<br />
outlined in this report.<br />
Report of Working Group 41 - MARCOM<br />
28
REFERENCES<br />
Allenström et al., 2003. “The interaction of large and highspeed<br />
vessels with the environment in archipelagos - Final<br />
report.” SSPA Research Report No 122, Göteborg,<br />
Sweden.<br />
Anonymous, 1999. “Speed restriction fails to halt<br />
<strong>Wash</strong>ington State Ferries.” Fast Ferry International,<br />
38(8):22-25.<br />
Anonymous, 2000. “Early problems <strong>for</strong> Dutch service.”<br />
Fast Ferry International, 39(1):47.<br />
Bell, A., Elsaesser, B., and Whittaker, T. J. T., 2000.<br />
“Environmental Impact of Fast Ferry <strong>Wash</strong> in Shallow<br />
Water.” Hydrodynamics of <strong>High</strong> Speed Craft <strong>Wake</strong> <strong>Wash</strong><br />
& Motions Control, London, 1-14.<br />
Bolt, E., 2001. “Fast Ferry <strong>Wash</strong> Measurement and<br />
Criteria.” Fast 2001 The 6th International Conference on<br />
Fast Sea Transportation, Southampton, 135-148.<br />
Croad, R. and Parnell, 2002. “Proposed Controls on shipping<br />
activity in the Marlborough Sound - A review under<br />
s32 of the Resource Management Act.” Report to the<br />
Marlborough District Council, September 2002. Available<br />
at http://www.marlborough.govt.nz/documents.html<br />
Cain, C., 2000. “<strong>Wake</strong> <strong>Wash</strong> - An Operators Viewpoint -<br />
Passage Plans & Risk Assessment,” Hydrodynamics of<br />
<strong>High</strong> Speed Craft <strong>Wake</strong> <strong>Wash</strong> & Motions Control. The<br />
Royal Institution of Naval Architects, London, pp. 1-16.<br />
Chen, X.-N. and Sharma, S.D., 1995. “A Slender Ship<br />
Moving at a Near-critical Speed in a Shallow Channel.”<br />
Journal of Fluid Mechanics, 291: 263-285.<br />
Dand, I.W., Dinham-Peren, T.A. and King, L., 1999.<br />
“Hydrodynamic Aspects of a Fast Catamaran Operating in<br />
Shallow Water”, Hydrodynamics of <strong>High</strong> Speed Craft. The<br />
Royal Institution of Naval Architects, London, pp. 1-17.<br />
© COPYRIGHT <strong>PIANC</strong><br />
Danish Maritime Authority, 1997. Report on the Impact<br />
of <strong>High</strong>-Speed Ferries on the External Environment (in<br />
Danish).<br />
Demirbilek, Z., and Vincent, L., 2002. “ Water waves<br />
mechanics.” Coastal Engineering Manual, Part II,<br />
Hydrodynamics, Chapter II-1, L. Vincent, ed., U.S. Army<br />
Corps of Engineers, <strong>Wash</strong>ington, DC., 1 - 115.<br />
Doctors, L.J., 1997. "Resistance Predictions <strong>for</strong> Transomstern<br />
Vessels.” Fast 2001 The 6th International Conference<br />
on Fast Sea Transportation, Southampton.<br />
Eggers, K.W.H., Sharma, S.D. and Ward, L.W., 1967. “An<br />
Assessment of Some Experimental Methods <strong>for</strong><br />
Determining the Wavemaking Characteristics of a Ship<br />
Form.”<br />
Ekman, V.W. 1906., “On Stationary Waves in Running<br />
Water.” Arkiv för Matematik, Astronomi och Fysik, Vol. 3,<br />
No. 2, Stockholm, pp. 1-30.<br />
Feldtmann, M. and Garner, J., 1999. “Seabed<br />
Modifications to Prevent <strong>Wake</strong> <strong>Wash</strong> <strong>from</strong> Fast Ferries,<br />
Coastal Ships and Inland Waterways.” Royal Institution of<br />
Naval Architects, London.<br />
Fissel, D., Billenness, D., Lemon, D., and Readshaw, J.,<br />
2001. “Measurement of the Wave <strong>Wash</strong> Generated by Fast<br />
Ferries with Upward Looking Sonar Instrumentation.”<br />
17th International Fast Ferry Conference, New Orleans<br />
<strong>USA</strong>.<br />
Gadd, G.E., 1994. “The <strong>Wash</strong> of Boats on Recreational<br />
Waterways.” Transactions of the Royal Institution of<br />
Naval Architects.<br />
Gadd, G.E., 1999. “Far Field Waves Made by <strong>High</strong> Speed<br />
Ferries,” Hydrodynamics of <strong>High</strong> Speed Craft. The Royal<br />
Institution of Naval Architects, London, pp. 1-9.<br />
Hannon, M. A., and Varyani, K. S., 1999. “The <strong>Wash</strong><br />
Effect of <strong>High</strong> Speed Ferries in Coastal and Inland<br />
Waterways.” International Conference on Coastal Ships<br />
and Inland Waterways, London, 1-12.<br />
Havelock, T.H., 1908. “The Propagation of Groups of<br />
Waves in Dispersive Media, with Application to Waves on<br />
Water produced by a Travelling Disturbance.”<br />
Proceedings of the Royal Society of London, Series A, Vol.<br />
LXXXI, pp. 398-430.<br />
Hotchkiss, S., Braithwaite, R., Fletcher, B., Elsaesser, B.,<br />
and Whittaker, T. J. T., 2002. “Assessing the<br />
Environmental Impact of Fast Ferry <strong>Wash</strong> on Rocky Shore<br />
Communities.” Ship Design and Operation <strong>for</strong><br />
Environmental Sustainability, London, 1-13.<br />
Hughes, M., 2001. “CFD Prediction of <strong>Wake</strong> <strong>Wash</strong> in<br />
Finite Water Depth.” HIPER'01 2nd International<br />
EuroConference on <strong>High</strong> Per<strong>for</strong>mance Marine Vehicles,<br />
Hamburg, pp. 200-211.<br />
<strong>High</strong>-Speed Craft Code, 2000. “International Code of<br />
Safety <strong>for</strong> <strong>High</strong>-Speed Craft.” International Maritime<br />
Organization, London.<br />
Inui, T., 1954. “Wave-Making Resistance in Shallow Sea<br />
and in Restricted Water, with Special Reference to its<br />
Discontinuities.” Journal of the Society of Naval<br />
Architects of Japan, 76: 1-10.<br />
29 Report of Working Group 41 - MARCOM
Jiang T., 2000. “Investigation of Waves Generated by<br />
Ships in Shallow Water.” In Twenty-Second Symposium on<br />
Naval Hydrodynamics. The National Academies Press,<br />
<strong>Wash</strong>ington, D.C., United States.<br />
Jiang, T., Henn, R. and Sharma, S.D., 2002. “<strong>Wash</strong> waves<br />
generated by ships moving on fairways of varying topography.”<br />
In Twenty-Forth Symposium on Naval<br />
Hydrodynamics, Fukuoka Japan 8-13 July 2002.<br />
Kirk McClure Morton, 2000. “Investigation of Coastal<br />
Processes in Loch Ryan.” Loch Ryan Advisory<br />
Management Forum, Dumfries.<br />
Kirk, R. M. and M. B. Single, 2000. “Coastal Effects of<br />
New Forms of Transport: the Case of the Interisland Fast<br />
Ferries.” Chap. 21 in Environmental Planning and<br />
Management in New Zealand, eds. P.A. Memon and H.C.<br />
Perkins , Palmerston North, NZ: Dunmore Press Ltd.<br />
Kirkegaard, J., Kofoed-Hansen, H., and B. Elfrink, 1998.<br />
“<strong>Wake</strong> <strong>Wash</strong> of <strong>High</strong>-Speed Craft in Coastal Areas.” In<br />
Proceedings of the 26th International Coastal Engineering<br />
Conference, 22-26 June 1998, Copenhagen, Denmark.<br />
Kofoed-Hansen, H., 1996. “Technical Investigation of<br />
<strong>Wake</strong> <strong>Wash</strong> <strong>from</strong> Fast Ferries Summary & Conclusions.”<br />
5012, Danish Hydraulic Institute, Hørsholm.<br />
Kofoed-Hansen, H., Jensen, T., Kirkegaard, J. and Fuchs,<br />
J., 1999. “Prediction of <strong>Wake</strong> <strong>Wash</strong> <strong>from</strong> <strong>High</strong>-Speed<br />
Craft in Coastal Areas,” Hydrodynamics of <strong>High</strong> Speed<br />
Craft. The Royal Institution of Naval Architects, London,<br />
pp. 1-10.<br />
Kofoed-Hansen, H., Jensen, T., Sørensen, O.R. and Fuchs,<br />
J., 2000. “<strong>Wake</strong> <strong>Wash</strong> Risk Assessment of <strong>High</strong>-Speed<br />
Ferry Routes - A Case Study and Suggestions <strong>for</strong> Model<br />
Improvements.” The Royal Institution of Naval Architects,<br />
London.<br />
Kofoed-Hansen, H. and Mikkelsen, A.C., 1997. “<strong>Wake</strong><br />
<strong>Wash</strong> <strong>from</strong> Fast Ferries in Denmark.” In Proceedings of<br />
the 4th International Conference on Fast Sea<br />
Transportation, Sydney, Australia.<br />
© COPYRIGHT <strong>PIANC</strong><br />
Koushan, K., Werenskiold, P., Zhao, R., and Lawless, J.,<br />
2001. “Experimental and Theoretical Investigation of<br />
<strong>Wake</strong> <strong>Wash</strong>.” Fast 2001 The 6th International Conference<br />
on Fast Sea Transportation, Southampton, 165-179.<br />
Lighthill, J., 1978. “Waves in Fluids.” Cambridge<br />
University Press, Cambridge.<br />
Marine Accident Investigation Branch, 2000. “Report on<br />
the Investigation of the Man Overboard Fatality <strong>from</strong> the<br />
Angling Boat PURDY at Shipwash Bank, off Harwich on<br />
17 July 1999.” MAIB Report No. 17/2000.<br />
Maritime and Coastguard Agency (MCA), 1998.<br />
“Research Project 420 - Investigation of <strong>High</strong> Speed Craft<br />
on Routes Near to Land or Enclosed Estuaries.” Maritime<br />
and Coastguard Agency.<br />
Maritime and Coastguard Agency (MCA), 2001.<br />
“Research Project 457 - A Physical Study of Fast Ferry<br />
<strong>Wash</strong> Characteristics in Shallow Water.” Final Report,<br />
Maritime and Coastguard Agency.<br />
Mitchell, J.H., 1998. “The Wave Resistance of Ships.”<br />
Philosophical Magazine, 45 (Series 5): 106-123.<br />
Molland, A.F., Wilson, P.A. and Chandraprabha, S., 2000.<br />
“The Prediction of Ship Generated Near-Field <strong>Wash</strong><br />
Waves Using Thin Ship Theory,” Hydrodynamics of <strong>High</strong><br />
Speed Craft. The Royal Institution of Naval Architects,<br />
London, pp. 1-13.<br />
Nanson, G. C., Von Krusenstierna, A., and Bryant, E. A.,<br />
1994. “Experimental Measurements of River-Bank<br />
Erosion Caused by Boat-Generated Wave on the Gordon<br />
River, Tasmania.” Regulated River: Research &<br />
Management, 9:1-14.<br />
Newman, J. N., 1977: “Marine Hydrodynamics”. The<br />
MIT Press, Cambridge, Massachusetts, pp. 270-278.<br />
Parnell, K. 1996. “Monitoring Effects of Ferry <strong>Wash</strong> in<br />
Tory Channel and Queen Charlotte Sound.” Unpublished<br />
report to Marlborough District Council, April 1996.<br />
Parnell, K. E. and H. Kofoed-Hansen, 2001. “<strong>Wake</strong>s <strong>from</strong><br />
Large <strong>High</strong>-Speed Ferries in Confined Coastal Waters:<br />
Management Approaches with Examples <strong>from</strong> New<br />
Zealand and Denmark,” Coastal Management, Vol. 29, pp.<br />
217 – 237.<br />
Peltoniemi, H., A. Bengston, J. Rytkönen and T. Kõuts,<br />
2002. “Measurements of Fast Ferry Waves in Helsinki -<br />
Tallinn Run.” The Changing State of the Gulf of Finland<br />
Ecosystem Symposium, Tallinn, Estonia.<br />
Lewis, E. V., 1988. “Principles of Naval Architecture,”<br />
Vol. II: Resistance, Propulsion and Vibration. Society of<br />
Naval Architects and Marine Engineers, Jersey City, New<br />
Jersey.<br />
Pickrill, R.A. 1985 “Beach Changes on Low Energy Lake<br />
Shorelines, Lakes Manapouri and Te Anau, New Zealand.”<br />
Journal of Coastal Research, Vol 1, No 4 pp 353-363.<br />
Report of Working Group 41 - MARCOM<br />
30
Raven, H.C., 2000. “Numerical <strong>Wash</strong> Prediction Using a<br />
Free-surface Panel Code”, Hydrodynamics of <strong>High</strong> Speed<br />
Craft <strong>Wake</strong> <strong>Wash</strong> & Motion Control. The Royal Institution<br />
of Naval Architects, London, pp. 1-12.<br />
Sandwell Engineering, Inc., 2000. British Columbia Ferry<br />
Corp. Fast Ferry Program - <strong>Wake</strong> and <strong>Wash</strong> Project.<br />
Scott-Russell, J., 1965. “The Modern System of Naval<br />
Architecture,” London,Vol.1.<br />
Single, M.B. and Kirk, R.M., 1999. “Coastal Change and<br />
Human Processes in Tory Channel, Marlborough Sounds.”<br />
in P.C. Forer and P.J. Perry (eds) Proceedings of the 18th<br />
New Zealand Geography Society Conference 1995.<br />
Single, M. B., 2002. “Effects on the Shoreline of Fast<br />
Ferries in Tory Channel, New Zealand.” Proceedings of<br />
the 30th <strong>PIANC</strong> Congress, Sydney, Australia.<br />
Ström, K. and F. Ziegler, 1998. “Environmental Impacts of<br />
<strong>Wake</strong> <strong>Wash</strong> <strong>from</strong> <strong>High</strong> Speed Ferries in the Archipelago of<br />
Göteborg.” Environmental Office, Göteborg (In Swedish).<br />
Stumbo, S., Fox, K., Dvorak, F., and Elliot, L., 1999. “The<br />
Prediction, Measurement, and Analysis of <strong>Wake</strong> <strong>Wash</strong><br />
<strong>from</strong> Marine Vessels,” Marine Tech., Vol. 36, No. 4, pp.<br />
248 – 260.<br />
Stumbo, S., Fox, K., and Elliot, L., 2000. “An Assessment<br />
of <strong>Wake</strong> <strong>Wash</strong> Reduction of Fast Ferries at Supercritical<br />
Froude Numbers and at Optimised Trim.” RINA, The<br />
Royal Institution of Naval Architects, London.<br />
Svensson, U., 1999. “Environmental Impacts of Large and<br />
Fast Ships.” SSPA, Maritime Consulting Report, No<br />
984798-01 (in Swedish).<br />
Taatø, S.H., Aage, C. and Arnskov, M.M., 1998. “Waves<br />
<strong>from</strong> Propulsion Systems of Fast Ferries.” 14th Fast Ferry<br />
International Conference, Copenhagen.<br />
© COPYRIGHT <strong>PIANC</strong><br />
Tuck, E.O., Scullen, D.C. and Lazauskas, L., 2001. “Ship-<br />
Wave Patterns in the Spirit of Michell.” In: Y.<br />
Shikhmurzaev (Editor), IUTAM Conference on Free<br />
Surface Flows. The University of Birmingham,<br />
Birmingham.<br />
Whittaker, T.J.T., Doyle, R. and Elsaesser, B., 2000. “A<br />
Study of the Leading Long Period Waves in Fast Ferry<br />
<strong>Wash</strong>,” Hydrodynamics of <strong>High</strong> Speed Craft <strong>Wake</strong> <strong>Wash</strong><br />
& Motions Control. RINA, The Royal Institution of Naval<br />
Architects, London.<br />
Whittaker, T.J.T., Doyle, R. and Elsaesser, B., 2001. “An<br />
Experimental Investigation of the Physical Characteristics<br />
of Fast Ferry <strong>Wash</strong>.” In: V. Bertram (Editor), HIPER'01<br />
2nd International EuroConference on <strong>High</strong> Per<strong>for</strong>mance<br />
Marine Vehicles, Hamburg, pp. 480-491.<br />
Vincent, L., Bratos, S., Demirbilek, Z. and Weggel, J.R.,<br />
2002. “Estimation of Nearshore Waves.” L. Vincent<br />
(Editor), Coastal Engineering Manual, Part II,<br />
Hydrodynamics, Chapter II-3. Engineer Manual 1110-2-<br />
1100. U.S. Army Corps of Engineers, <strong>Wash</strong>ington, DC.,<br />
pp. 1-34.<br />
31 Report of Working Group 41 - MARCOM
ANNEX A<br />
TERMS OF REFERENCE<br />
The introduction of high-speed ferries in the mid-nineties<br />
has led to wake conditions not known earlier.<br />
The vessels in question are characterised by a travelling<br />
speed of 35 to 45 knots. They may be catamaran types but<br />
can also be single hull vessels.<br />
According to observations by the general public in<br />
Denmark, the waves created by the wake are more dangerous<br />
than the waves created by traditional ferries. They<br />
are higher and they may appear without warning and suddenly<br />
rise in shallow waters, then break and cause run-up<br />
on the coast. Danish newspapers and television news have<br />
shown dangerous situations <strong>for</strong> small boats and <strong>for</strong><br />
bathers, and large numbers of complaints and protests<br />
<strong>from</strong> coastal house owners and landowners, <strong>from</strong> fishermen,<br />
anglers, sailors, rowers, hunters, divers, swimmers/holidaymakers<br />
were received by the authorities.<br />
Anxieties were also voiced regarding coastal erosion, subsidence<br />
of natural stone reefs and disturbance of bird sanctuaries<br />
and dike safety.<br />
In 1995 the Danish Maritime Authority commissioned the<br />
Danish Hydraulic Institute to carry out a technical investigation<br />
of wake wash <strong>from</strong> fast ferries.<br />
This investigation concluded that<br />
• the new high speed vehicle ferries generate waves,<br />
which, in coastal and shallow water regions, are considered<br />
by the general public as being considerably different<br />
to the waves caused by conventional vessels.<br />
• this view has been widely confirmed by the measurements<br />
and calculations which have been made.<br />
The report also mentions that wake wash problems have<br />
appeared in Sweden, Ireland, Australia, New Zealand,<br />
England, Portugal, and U.S.A. In Denmark regulations<br />
were issued in 1998 concerning the effects of waves <strong>from</strong><br />
high-speed ferries on leisure activities, on the environment<br />
in general and in particular on erosion and dike safety<br />
problems.<br />
• categorize problems met<br />
• analyse in which ways such problems may be <strong>for</strong>eseen<br />
and avoided<br />
• gather in<strong>for</strong>mation on regulations established in various<br />
countries and regions<br />
• coordinate study with IMO working groups on problems<br />
in relations to high-speed ferries;<br />
all in order to set up guidelines <strong>for</strong> traffic planners, ship<br />
owners, and relevant public authorities, including waterway<br />
managers.<br />
© COPYRIGHT <strong>PIANC</strong><br />
<strong>PIANC</strong> started in 1995 a working group that deals with<br />
harbour facilities <strong>for</strong> high-speed ferries. The task <strong>for</strong> this<br />
new working group is there<strong>for</strong>e limited to high-speed ferries<br />
in motion. This working group was requested to<br />
• gather in<strong>for</strong>mation internationally about experiences<br />
with high-speed ferries<br />
Report of Working Group 41 - MARCOM<br />
32