drag crisis

The drag crisis was observed in 1905{{cn|date=October 2019}} by Nikolay Zhukovsky, who guessed that this paradox can be explained by the detachment of streamlines at different points of the sphere at different velocities.{{cite book |last=Zhukovsky|first=N.Ye.|date=1938|title=Collected works of N.Ye.Zukovskii|url=http://books.e-heritage.ru/book/10075061|page=72}}

Later the paradox was independently discovered in experiments by Gustave Eiffel[https://vk.com/doc323168506_483174428?hash=e86399daab9927b560&dl=aa52a7d4992d20dfcd Eiffel G. Sur la résistance des sphères dans l'air en mouvement, 1912] and Charles Maurain.{{cite book |last=Toussaint|first=A.|date=1923|title=Lecture on Aerodynamics|url=https://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19930084658.pdf|publisher=NACA Technical Memorandum No. 227|page=20}}

Upon Eiffel's retirement, he built the first wind tunnel in a lab located at the base of the Eiffel Tower, to investigate wind loads on structures and early aircraft. In a series of tests he found that the force loading experienced an abrupt decline at a critical Reynolds number.

The paradox was explained from boundary-layer theory by German fluid dynamicist Ludwig Prandtl.{{cite journal |last1=Prandtl |first1=Ludwig |title=Der Luftwiderstand von Kugeln |journal=Nachrichten der Gesellschaft der Wissenschaften zu Göttingen |date=1914 |pages=177–190}} Reprinted in {{cite book |year=1961| last1=Tollmien |first1=Walter |last2=Schlichting |first2=Hermann |last3=Görtler |first3=Henry |last4=Riegels |first4=F. W. |title=Ludwig Prandtl Gesammelte Abhandlungen zur angewandten Mechanik, Hydro- und Aerodynamik |publisher=Springer Berlin Heidelberg |isbn=978-3-662-11836-8 | doi=10.1007/978-3-662-11836-8_45 }}

The drag crisis is associated with a transition from laminar to turbulent boundary layer flow adjacent to the object. For cylindrical structures, this transition is associated with a transition from well-organized vortex shedding to randomized shedding behavior for super-critical Reynolds numbers, eventually returning to well-organized shedding at a higher Reynolds number with a return to elevated drag force coefficients.

The super-critical behavior can be described semi-empirically using statistical means or by sophisticated computational fluid dynamics software (CFD) that takes into account the fluid-structure interaction for the given fluid conditions using Large Eddy Simulation (LES) that includes the dynamic displacements of the structure (DLES) [11]. These calculations also demonstrate the importance of the blockage ratio present for intrusive fittings in pipe flow and wind-tunnel tests.

The critical Reynolds number is a function of turbulence intensity, upstream velocity profile, and wall-effects (velocity gradients). The semi-empirical descriptions of the drag crisis are often described in terms of a Strouhal bandwidth and the vortex shedding is described by broad-band spectral content.

1. Fung, Y.C. (1960). "Fluctuating Lift and Drag Acting on a Cylinder in a Flow at Supercritical Reynolds Numbers," J. Aerospace Sci., 27 (11), pp. 801–814.
2. Roshko, A. (1961). "Experiments on the flow past a circular cylinder at very high Reynolds number," J. Fluid Mech., 10, pp. 345–356.
3. Jones, G.W. (1968). "Aerodynamic Forces on Stationary and Oscillating Circular Cylinder at High Reynolds Numbers," ASME Symposium on Unsteady Flow, Fluids Engineering Div. , pp. 1–30.
4. Jones, G.W., Cincotta, J.J., Walker, R.W. (1969). "Aerodynamic Forces on Stationary and Oscillating Circular Cylinder at High Reynolds Numbers," NASA Report TAR-300, pp. 1–66.
5. Achenbach, E. Heinecke, E. (1981). "On vortex shedding from smooth and rough cylinders in the range of Reynolds numbers 6x103 to 5x106," J. Fluid Mech. 109, pp. 239–251.
6. Schewe, G. (1983). "On the force fluctuations acting on a circular cylinder in crossflow from subcritical up to transcritical Raynolds numbers," J. Fluid Mech., 133, pp. 265–285.
7. Kawamura, T., Nakao, T., Takahashi, M., Hayashi, T., Murayama, K., Gotoh, N., (2003). "Synchronized Vibrations of a Circular Cylinder in Cross Flow at Supercritical Reynolds Numbers", ASME J. Press. Vessel Tech., 125, pp. 97–108, DOI:10.1115/1.1526855.
8. Zdravkovich, M.M. (1997). Flow Around Circular Cylinders, Vol.I, Oxford Univ. Press. Reprint 2007, p. 188.
9. Zdravkovich, M.M. (2003). Flow Around Circular Cylinders, Vol. II, Oxford Univ. Press. Reprint 2009, p. 761.
10. Bartran, D. (2015). "Support Flexibility and Natural Frequencies of Pipe Mounted Thermowells," ASME J. Press. Vess. Tech., 137, pp. 1–6, DOI:10.1115/1.4028863
11. Botterill, N. ( 2010). "Fluid structure interaction modelling of cables used in civil engineering structures," PhD dissertation (http://etheses.nottingham.ac.uk/11657/), University of Nottingham.
12. Bartran, D. (2018). "The Drag Crisis and Thermowell Design", J. Press. Ves. Tech. 140(4), 044501, Paper No: PVT-18-1002. DOI: 10.1115/1.4039882.

• {{cite web |url=https://repository.tudelft.nl/file/File_29722972-f288-47f6-a792-ba7ab7d21c0b?preview=1 |title= Simulating Drag Crisis for a Sphere Using Skin Friction Boundary Conditions |accessdate=2008-10-24}}
• {{cite web |url= http://home.iitk.ac.in/~smittal/publi_&_present/sm_journals/drag_crisis.pdf |title= Flow past a cylinder: Shear layer instability and drag crisis |accessdate=2008-10-24}}

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Category:Drag (physics)

Category:Fluid dynamics