Unsteady RANS method for ship motions with application to roll for a surface combatant
Introduction
Recent progress in Reynolds-averaged Navier–Stokes (RANS) CFD code development and application is making simulation based design an imminent reality. Development of such a tool will allow the merging of traditionally separate naval architecture sub-disciplines for resistance and propulsion, maneuvering, and seakeeping, and when combined with CFD-based optimization, will likely revolutionize the ship design process.
Of the three sub-discipline areas, application of RANS methods to resistance and propulsion is the most advanced with nearly two decades of experience. Existing approaches are able to predict ship resistance with reasonable accuracy as shown from results for three steady flow test cases at the recent Gothenburg 2000 Workshop on CFD in Ship Hydrodynamics [1]. Methods have recently been applied to optimize hull forms for a variety of objective functions for ships with steady forward speed in calm seas [2].
In comparison, application of RANS methods to maneuvering and seakeeping is less mature due to obstacles from unsteady flows, ship motions, complex environment (e.g., incident waves, wave breaking, bubbly flow) and increased required computer resources. Also, methods developed for resistance and propulsion may not be easily extended into these areas. Application of RANS methods for steady maneuvers (e.g., off-design yaw, steady turn) can be found in [3], [4], [5], [6], [7]. However, application of viscous methods to more complex unsteady maneuvers is rare and most investigations rely on motion simulation programs with empirically derived coefficients.
Typical seakeeping solution techniques are based on assumptions of small amplitude motions and potential flow so that the general 6DOF non-linear equations of motions are reduced to two separate sets of linear equations (i.e., vertical plane motions become uncoupled from horizontal plane motions) and are solved in the frequency domain. Within those assumptions, predictions show good agreement for vertical plane motions. For horizontal plane motions, seakeeping codes based on potential flow methods model viscous effects by incorporating empirically derived roll damping data. For example, [8] used a linear frequency-dependent hydrodynamics model augmented by empirically derived linear and non-linear roll damping data from [9] and non-linear roll and heave/pitch restoring forces. Predictions with these methods are limited to the range of geometry, frequency, and operating parameters from the empirical data and suffer from scale effects. Simulations in the time-domain have been performed to predict larger non-linear roll motions, but most suffer from use of potential flow methods with empirical damping data, e.g., [10]. Thus, there is a critical need for development of numerical methods for viscous flows and prediction of larger amplitude motions for surface ships with appendages.
In an effort to develop a physics-based approach to seakeeping problems, RANS methods have recently been applied to the prediction of ship motions, although most studies have focused on 2D oscillating bodies. These methods have the potential to produce superior results since effects due to viscosity, creation of vorticity in the boundary layer, vortex shedding, and turbulence are naturally included. RANS methods have been used to study the flow around 2D oscillating cylinders, e.g., [11], [12], [13]. Accurate prediction of forces and moments on a 3D submerged cylinder fitted with bilge keels and with prescribed roll motion was demonstrated in [14]. Prediction of pitch and heave motions for ships in regular head waves was demonstrated for the Wigley hull and Series 60 cargo ships using density function free surface modeling [15]; a container ship using overlapping structured grids and density function free surface modeling [16]; and a container ship using level-set free surface modeling [7]. Simulations of free roll decay motion of a barge in calm sea and incident waves were performed using a Chimera RANS method in [17].
Development of unsteady RANS methods within the ship hydrodynamics group at IIHR—Hydroscience and Engineering Lab (IIHR) enables extensions from previous work for resistance and propulsion to applications for seakeeping and maneuvering. A step-by-step approach was followed towards this goal by initially performing unsteady RANS simulations for the forward speed diffraction (ship advancing in waves but constrained from motions) and radiation (prescribed ship motions in calm water) problems. In the former case, simulations were performed for the Wigley hull for a wide range of conditions [18] and for the surface combatant, David Taylor Model Basin (DTMB) model 5512 (5512), for medium speed/long wave and high speed/short wave conditions [19] including comparisons with IIHR towing tank data [20], [21]. In the latter case, simulations were performed for a double body 5512 model with prescribed vertical (pitch and heave) and horizontal (roll) plane motions as part of a DoD challenge project on 6DOF motions and maneuvering for surface ships [22]. Pitch and heave motions for the Wigley hull in incident waves were predicted and the RANS results were compared to those from strip theory [23].
As an initial step towards prediction of general ship motions, simulations are performed for a barehull and bilge keel appended surface combatant model (subsequently referred to as 5512) for predicted and prescribed roll motions. Simulations with free roll decay are used to predict roll damping and resonant frequencies for the surface combatant and to verify and validate the simulations. Simulations with prescribed motions are used to quantify the unsteady response of the flow and free surface fields to roll motion using a Fourier analysis. Simulations are performed using the RANS CFD code, CFDSHIP-IOWA, which was shown to be one of the better codes at the recent Gothenburg 2000 Workshop on CFD in Ship Hydrodynamics for the surface combatant test case [24].
The contributions of the present work are in (i) extending the previous work to unsteady RANS simulations of general 6DOF ship motions and maneuvering (with focus on applications for predicted and prescribed roll motions), (ii) performing verification and validation to quantify numerical and modeling errors, (iii) explaining the unsteady response of the boundary layer, axial vortices, and free surface to roll motion, (iv) predicting roll decay motion and analyzing seakeeping properties of the ship model using a spring–mass-damper model, and (v) guiding experimental measurements currently underway at the IIHR and filling-in the sparse experimental dataset.
Section snippets
6DOF RANS method
Unsteady RANS simulations are performed with CFDSHIP-IOWA, which is a general-purpose, multi-block, high-performance parallel computing code developed for computational ship hydrodynamics and applied to surface ships and complex propulsors without ship motions. The basic methodology is given in detail in [25], and the reader is referred to this paper when solution details are omitted. CFDSHIP-IOWA was recently extended to predict general 6DOF ship motions with larger amplitude, non-linear,
Geometry
Unsteady RANS simulations are performed for the Model 5512 geometry which is representative of a modern full-scale naval combatant with sonar dome and transom stern (Fig. 3a). Simulations are performed for two model configurations: barehull (BH) (i.e., without rudder, shafts, propellers, etc.) and barehull geometry appended with bilge keels (BK). Geometric properties for the BH model are given in Table 1.
Data
A large experimental database exists for steady flow over the surface combatant without
Grid and time step design
Computational grids for the BH and BK models are designed to accurately resolve geometric features of the model and the unsteady turbulent boundary layer, wake, and wave fields. The BH and BK grids were generated using the commercial code GRIDGEN (Pointwise, Inc.), where clustering was used near the bow and stern in the ξ-direction, at the hull in the η-direction, and near the free surface in the ζ-direction. Grid topology was selected so that the block fixed to the transom face could be
Verification and validation
Numerical and modeling errors and uncertainties for the unsteady roll motion simulations are estimated by using the verification and validation (V&V) procedures given in [36], demonstrated in [37], and recently in this journal for the Esso-Osaka tanker ship in [3]. Later, corrections to uncertainty estimates were provided in [38]. The simulation with BK geometry and predicted roll decay motion at low speed (Fr = 0.138) was selected for V&V since this case corresponds to the experimental base case
Motions
The roll damping characteristics of the surface combatant are quantified by fitting an exponentially damped sinusoidal function to both the prediction and datawhere AD and ωD are the motion amplitude and angular frequency. The exponential damping is characterized by an nth order polynomial with damping coefficient βi corresponding to the ith order term. The damping coefficients βi and amplitude AD are found by fitting the exponential function to the
Acknowledgements
This research was sponsored by Office of Naval Research grant N00014-01-1-0073 under the administration of Dr. Patrick Purtell. The authors would like to acknowledge the DoD High Performance Computing Modernization Office and the DoD Challenge Program. Simulations were performed at the Army Research Lab Major Shared Resource Center using both the SGI Origin 2000 and 3000 machines.
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