The
CAE-system (Computer Aided Engineering) is the computer technology modeling and
visualizing space-time progress of the studied process. At present
similar technologies find their application in different areas of knowledge:
mechanics, hydro-, gas- and thermodynamics, construction, processing of
materials, medicine, nuclear physics, hydrometeorology, micro and macro world
etc. The basis of CAE-system is the numerical solver of systems of the
differential equations describing behavior previously sampled (it is normal in
the finite element formulation) areas of space (environment, body). At the same
time, it should be noted that in addition to the proven numerical methods
convergence of the solution here is also provided with special «artificial»
program procedures, algorithms and functions.
The essentially
significant stage of such technologies is the postprocessing, realizing the
analysis of results of modeling by means of scientific visualization. The tools
of the postprocessor are three-dimensional graphics, animation, and also the
graphic processor creating different nodal and elemental space-time functions.
The whole complex
of tasks of sea and river icebreakers belongs to the extensive class of
deformable environments mechanics problems. In this field of modeling the first
commercial CAE-systems are appeared and now remain the most reliable and
therefore demanded. The basic scientific novelty of CAE-technologies by
consideration of mechanics problems consists in modeling of interaction of
objects in contradistinction to modeling of loadings that offer a traditional
semi-empirical and the majority of numerical methods. In problems of assessment
and forecasting of ice fleet qualities it allows to pass for implementation of
non-autonomous interaction of the vessel's hull and its thrust steering complex
(TSC) with ice water environment. Unlike the classical autonomous solutions
[1-8] considering influence of only quantitatively static isotropic environment
on the vessel, CAE-models describe the interference of the vessel and
environment taking into account stochasticity of this process in space and
time. As the important advantage of the CAE-analysis, it is also necessary to
acknowledge the possibility of division of hydrodynamic and ice load that is
unavailable to a model experiment and full-scale tests.
In the field of
ice navigation there is a considerable number of private tasks of safety.
Generally, they are caused by requirements of optimization of maneuvering of
vessels (including joint) in different ice conditions during the short period
of time (ranging from several minutes to several tens of minutes). The
experience of the author showed that in such cases the forecast of safe
conditions from positions of averaging of influence of set of ice arguments (as
traditional solutions propose) will have a low forecast success rate [9-12].
Thus, when it is impossible to carry out full-scale tests, the alternative way
of reliable forecasting of several vessels interaction in ices is the numerical
experimentation with application of CAE-technologies.
To demonstrate
this the author has executed a series of experiments on the basis of the models
described below. In this work the LS-DYNA CAE-system adapted by authors for the
solution of ice problems is used [15]. Modeling is executed using an explicit
finite-element method. Predicted data for the subsequent
post-processing are stored in the binary files database.
Theoretical
bases of CAE-modeling of problems of a sea and river ice technology (types and
formulations of finite elements, models of materials, algorithms of contact
interaction, finite element mesh, procedures of decrease in a resource
investment of problems) are developed by the author in the monograph [9].
For the
subsequent analysis several tens of discrepancy options have been calculated,
the ice channel laying and dressing of vessels in different ice and navigation
conditions have also been considered.
In the numerical
experiments a river-sea operation dry cargo ship «Sormovsky» (project 1557; ice
class «Ice-1») and the shallow-draft river icebreaker «Captain Evdokimov»
(project 1191) acted as prototypes of model vessels.
In the
calculations some parameters ranged. The ice thickness was 0,2-0,8 m. Its
degree of size changed as a small ice cake, ice cake (the ice floes having the
average size in the plan to 20 m) and compact ice. Initial distances between
diametral planes of vessels were 5-60 m. The general directions of the mutually
movement of vessels and their speed varied 1,0-5,0 m/s. The number of
maneuvering vessels in a zone of interaction at the same time was 2-3. The
orders operating them were «with pullout» (the control mode a rudder which is
in addition considering the angular speed and acceleration of the vessel at
turn) and «without pullout» (the control mode a rudder considering only angular
displacement of the vessel at turn). The relative length and width of the ice
channel (the field of a compact ice) in all options slightly fluctuated within
3,5 lengths and 6,0 width of the greatest vessels respectively.
The form of ice
floes has no influence on the level of vessel’s ice loads. Such an influence
has the floes’ size. In both real and virtual modeling it is common to cover
the water area with rectangular «tiles» of ice sized within studied
fragmentation level [1–3]. That approach makes modeling more efficient. In this
work square ice floes no more than 20 m wide were used. They correspond to the
small ice cakes and ice cakes in the nature.
The action of
ship thrust steering complexes, hydrodynamic loads on hulls of the vessels and
an ice cover have been described by nodal forces according to recommendations
of work [9-12].
Any
safe vessels passing can be considered as the counter and parallel movement
within strictly established lanes (traffic separation zones). In ices
this maneuver is carried out on straight sections of ice routes only (ice
channels). The level of safety of passing in this case is determined by route
(leading) stability of each vessel in this ice environment and beam distance
between them. The first parameter can quantitatively be evaluated through
transverse displacement of the vessel and behavior of an angle of its yaw,
which are directly connected with the operation of the vessel.
Generally, in ice
conditions the automatic driving of the vessel is unacceptably, but the human
factor always brings identity in the mentioned law. The analysis of natural
observations on operational yaw stability of the studied vessels [13,14] showed
that for conditions of ice cakes and small ice cakes at some proven, average
and almost implementable law of the thrust steering complex operation the yaw
does not surpass the size of 3,0 degrees with probability of 95%. Taking this
into account, at a preliminary stage the autonomous movement of vessels in ices
for the purpose of working off of the control law providing full-scale
confirmed parameters of their yaw was modelled. The example of CAE-assessment
of route stability of the motor ship type «Sormovsky» in ice cakes 0,5 m thick
at their different concentration and degree of size for several control laws is
given in fig. 1.
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Fig. 1. Behavior of a yaw angle of the motor ship type
«Sormovsky» in ice cakes
(A-E - ice cake of different degree of size and
concentration at the control law «without pullout»; F - ice cake
concentration 2 balls at the control law «with pullout»)
The note to
fig. 1: Concentration of ices is the relation of total area of ice floes to
the area of the water area covered with evenly distributed ice. It can be
evaluated on a 10-ball scale: 0 - open water; 10 - compact ice.
|
Processing of
results of modeling showed that in thin ices (up to 0,2 m thick) at the chosen
control laws of vessels their ice interference at a passing is negligible. It
can be illustrated with the characteristic curves shown in fig. 2.
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a)
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b)
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Fig. 2. Behavior of a yaw angle (a) and transverse
displacement (b) of dry cargo ships type «Sormovsky» at a passing in ice
cakes 0,2 m thick
(A-C– «irregular» ice cake concentration of 9-10 balls at
different speeds of a passing and the control law «without pullout»; D –
«regular» ice cake concentration of 9-10 balls at the control law «without
pullout»)
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The analysis of
characteristic curves of fig. 2 showed that in the specified ice conditions
even at maximum ratings of a yaw angle and transverse displacement of vessels
(curves of A and C, fig. 2) a width of band occupied by the vessel at a passing
will not exceed size more than 1,33 of its own width.
In behavior of
the passing motor ships in thick small ice cakes (from 0,5 m thick and more)
danger of collision is also not expected even at the minimum initial beam
distances (to 10 m) though quantitative characteristics of route stability get
noticeably worse in comparison with similar parameters in thin ices (Fig. 3).
|
a)
|
|
b)
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Fig. 3. Behavior of a yaw angle (a) and transverse
displacement (b) of dry cargo ships type «Sormovsky» at a passing in small
ice cakes 0,5 m thick
(A-H - options of the movement in small ice cakes
concentration of 9-10 balls at different vessel speeds, passing distances and
the control law «without pullout»)
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The numerical
forecast shows that directly in the course of a passing the maximum yaw angle
of vessels and their transverse displacements are in limits of 4,0 degrees and
4,0 m respectively (lines E, fig. 3). These parameters of the movement generate
almost double width of a traffic lane (24,6 m) in relation to vessel width.
The probability
of adverse reaction of the vessel at the movement in thick small ice cakes
(especially at small beam distances) is high and consists in «high drift angle»
of its stern towards an axis of the ice channel directly after a passing of
motor ships (Fig. 4). It is possible to explain it with the fact that control
according to the established law of vessels aim to return, whenever possible,
rather to the leading (route) line with shift in the course of which passing is
inevitable. Additionally, during this period the yaw angle and transverse
displacement of vessels increase (lines B, fig. 3).
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Fig. 4. «High drift angle» of a stern of vessels after a
passing in thick small ice cakes
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For thick ice
cakes finite element modeling quite often predicts steady smooth drift of
vessels in local zones of the smallest ice resistance, and also significant
random «spikes» in characteristics of yaw (Fig. 5).
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a)
|
|
b)
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Fig. 5. Behavior of a yaw angle (a) and transverse
displacement (b) of dry cargo ships type «Sormovsky» at passing in ice cakes
0,5 m thick
(A-H - options of the movement in ice cakes concentration of
9-10 balls at different vessel speeds, passing distances and the control law
«without pullout»)
|
So, for example,
in option E (Fig. 5) with an amplitude of transverse displacement of 7,5 m and
a yaw angle of 5,5 degrees the width of a traffic lane of the vessel reaches
31,0 m. Therefore at small beam distances there is a probability of a slow
impact of vessels at a passing (Fig. 6). It is recommended to keep a beam
distance in such ices not less than 25,0-30,0 m.
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Fig. 6. A slow impact of vessels at a passing in thick ice
cakes
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On the
constrained water areas covered with small ice cakes, in case of emergency the
safe passing can be provided with performance of maneuver of mutual
"evasion" of vessels. Numerical experiments did not find any
contraindications of its implementation in these conditions. It is illustrated
in fig. 7 with animation of process of vessels passing in thick very compacted
small ice cakes.
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Fig. 7. Vessels passing in thick small ice cakes by
performing of an «evasive» action
(A control law of vessels –«with pullout»)
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But in thick very
compacted ice cakes the maneuver described above can hardly be recommended as
safe. For these conditions the numerical model predicts obviously excessive
rapprochement of vessels (time ≈ 60 c, fig. 8).
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Fig. 8. Vessels passing in thick ice cakes by performing of
an «evasive» action
(A control law of vessels – «with pullout»)
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Initially bigger
heterogeneity of ice environment from ice cakes, in comparison with small ice
cakes, in addition is being aggravated by the maneuvering meeters can
significantly affect their propulsion ability. In the example shown in fig. 8
and 9, the ratio in attainable speed of the movement of the same motor ships
directly at a stage of a passing fluctuates within 1,25 - 5,0. It should be
noted that the similar phenomena are short, but in the solution of short-term
safety problems, at expert assessment of acceptable conditions of maneuvering
their ignoring is incorrect.
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Fig. 9. The speed of vessels passing in thick ice cakes
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The
requirement for the numerical prediction of the consequences of vessels' joint
maneuvering in ices at small distances is caused by inability of autonomous
analytical techniques to the description of dynamics of progress of similar
processes.
Thin ices of
different degree of size and thick small ice cakes are not dangerous to the
dispersing vessels (including at the emergency passing an «evasive» action).
In thick ice
cakes it is required to keep an interleading passing distance of transport
ships not less than 30 m. The emergency maneuvering by «evasion» is not recommended.
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