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- Ocean and Marine Division Technical Session 1
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- 2016 ASEE Annual Conference & Exposition
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Vukica M. Jovanovic, Old Dominion University; Petros J Katsioloudis, Old Dominion University; Mileta Tomovic, Old Dominion University; Thomas B. Stout, Tidewater Community College
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Ocean and Marine
with technology innovations, since computingcapabilities are driving advances in data management and cyber-physical system capabilities. 6 Acknowledgments The authors wish to acknowledge support from Office of Naval Research for grant βHigherEducation Pathways for Maritime Mechatronics Technicians (MechTech)β, Agency ProposalNumber N00014-15-1-2422.ReferencesArciszewski, H. F. R., de Greef, T. E., & van Delft, J. H. (2009). Adaptive Automation in a Naval Combat Management System. IEEE Transactions on Systems, Man & Cybernetics: Part A, 39(6), 1188-1199. doi: 10.1109/TSMCA.2009.2026428Arregi, B., Granados, S., Hascoet, J. Y., Hamilton, K., Alonso, M., & Ares, E
- Conference Session
- Ocean and Marine Division Technical Session 1
- Collection
- 2016 ASEE Annual Conference & Exposition
- Authors
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Lifford McLauchlan, Texas A&M University, Kingsville; Mehrube Mehrubeoglu, Texas A&M University, Corpus Christi
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Ocean and Marine
) π¦Μ = π sin(π) (1) πΜ = πThe position is x, y, U is the velocity and r is the input. This can then be extended to i vehicleswhich will move in a flocking behavior, a coordinated formation, with the same direction andvelocity. This can be accomplished using a local voting protocol [8] π₯Μ π = ππ cos(ππ ) π¦Μ π = ππ s ππ(ππ ) (2) πΜπ = π’πwhere in a given neighborhood Ni around vehicle i given π β π [8] πΜπ = βπβππ πππ (ππ β ππ
- Conference Session
- Ocean and Marine Division Technical Session 1
- Collection
- 2016 ASEE Annual Conference & Exposition
- Authors
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David Clippinger P.E., U.S. Coast Guard Academy; Ronald Adrezin, U.S. Coast Guard Academy; Mary Shalane Regan, U.S. Coast Guard Academy
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Ocean and Marine
) π΅π΅ππΜ M(t) Figure 1: Top View of Ship and the Associated Free Body Diagram (right)The ship has a mass moment of inertia about its vertical axis I, and is subject to a turningmoment M(t) from the shipβs rudder. The angle of the ship relative to the earthβs cardinal(inertial) directions is ΞΈ. The ship also experiences damping from the water, which here isapproximated as a linear function of the angular velocity ππΜ. The differential equation of motionfor such a system may be developed using appropriate techniques1, and is given as equation (1). πΌπΌππΜ + π΅π΅ππΜ = ππ(π‘π‘) (1)A transfer function relating the transformed input moment M(s) to the transformed