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A Fast Simulation Tool for Ships Towed by Kites

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Beyond the Sea project team (from left to right): Christian Jochum, Nedeleg Bigi, Morgan Behrel, Guy Leblanc, Damien Grelon, Yves Parlier and Richard Leloup, at ENSTA Bretagne (15 December 2017)

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Beyond the Sea⃝R project by Yves Parlier

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Antoine Morvan

Research Fellow ENSTA Bretagne

Institut de Recherche Dupuy de Lôme 2 Rue François Verny

29200 Brest France

antoine.morvan@ensta-bretagne.org www.ensta-bretagne.org

A Fast Simulation Tool for Ships Towed by Kites:

Assessment of Propulsion Efficiency

Antoine Morvan, Nedeleg Bigi, Jean-Baptiste Leroux, Christian Jochum

IRDL ENSTA-Bretagne CNRS FRE 3744 Over the past decades, more and more research

pro-grams are developing innovative and green propulsion systems for maritime transportation. This is also the ap-plication background of the present work, which aims at reducing the consumption of container ships by an al-ternative propulsion technique. In his pioneering work, Duckworth [1] proposed kite propulsion. Podeur et al. [2] confirmed the potential of this technique to achieve significant fuel savings. However, the assessment of the possible risk entailed in the towing of a ship by a kite has not been studied consistently. Existing literature ref-erences consider static equilibrium [3]. The dynamic in-teraction between a ship and a kite has been studied by Bigi [4]. The main objective of the present work is to pre-cise the dynamic effects on the ship and the kite operabil-ity for a realistic sea and wind environment. To achieve this, a unified seakeeping/manoeuvring numerical code is used by updating the equation of motions with the forces generated by the kite [5]. A zero mass model is used for the kite, assuming that the tethers are straight and inelastic. The aerodynamic lift coefficient and the lift-to-drag ratio are functions of the yaw turning rate of the kite. Two types of simulation are considered: firstly, the ship in calm water and, secondly, the ship subjected to regu-lar Airy wave for varying parameters such as wave ampli-tude, wind force, tether length and ship heading. The re-sults show that the kite is more affected by the dynamic motion than the ship (see figure). Indeed, a lock-in phe-nomenon between the wave frequency of encounter and the first harmonic of the kite is clearly demonstrated. A dimensional analysis is provided in order to identify this phenomenon prior to simulation.

ωk1kite first harmonic frequency, ∆σkkite wind load amplitude, ∆φsheel amplitude,Lttether length for a kite areaAw=500 m2, true wind speedUtw=12.5 m/s, wind direction βtw=45◦, a wave en-counter frequency ωe=0.285 rad/s.

References:

[1] D. Duckworth: The Application of Elevated Sails (Kites) for Fuel Saving Auxiliary Propulsion of Commercial Vessels. Journal of Wind Energy and Industrial Aerodynamics, n◦12, pp. 75-97 (1983) [2] V. Podeur, D. Merdrignac, M. Behrel, K. Roncin, C. Jochum, Y. Par-lier et P. Renaud: Simulation de voyage au long cours pour le cal-cul d’économies de carburant : Application á la propulsion par cerf-volant, in 15e Journèes de l’Hydrodynamique, Brest, France (2016) [3] J. Wellicome and S. Wilkinson: Ship Propulsive Kites: An Initial Study, University of Southampton (1984)

[4] N. Bigi: Investigation of The Dynamic Motions and Operability of a Ship Towed by Kite. PhD Thesis, University of Western Brittany, Brest (2017)

[5] N. Bigi, J.-B. Leroux, K. Roncin, A. Nême, C. Jochum, Y. Parlier: Ship Towed By Kite In Waves ś A Strongly Coupled System, The 4th International Conference on Innovation in High Performance Sail-ing Yachts, Lorient (2017)

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