The transverse velocity fluctuation in the wake of a circular cylinder was measured…

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Fluids & Continuum Physics · Data analysis and model fitting in the laboratory

Fluid Dynamics, Ch Transition to turbulence

Problem

The transverse velocity fluctuation in the wake of a circular cylinder was measured at several Reynolds numbers just above the onset of vortex shedding. The mean-square fluctuation v′2‾\overline{v'^2} (in mm2 s−2\mathrm{mm^2\,s^{-2}}) was recorded as: Data (ReRe, v′2‾\overline{v'^2} in mm2 s−2\mathrm{mm^2\,s^{-2}}): (50, 6.0)(50,\,6.0), (60, 24.0)(60,\,24.0), (70, 48.0)(70,\,48.0), (80, 66.0)(80,\,66.0). Close to a supercritical Hopf bifurcation at RecRe_c, the Landau equation predicts that the saturated mean-square amplitude should rise linearly with ReRe, v′2‾=m(Re−Rec)\overline{v'^2} = m(Re - Re_c), for some constant mm. ((a)) Fit a least-squares straight line v′2‾=m Re+c\overline{v'^2} = m\,Re + c to the four points, and give mm and cc. ((b)) Use the intercept to find RecRe_c, and compare it with the accepted value Rec≈47Re_c \approx 47 for a circular cylinder. ((c)) Compute the difference between each measured point and the fitted line, and use the size of these differences, relative to the range of v′2‾\overline{v'^2} spanned by the data, to decide whether the measurements are consistent with the square-root law of a supercritical Hopf bifurcation, or point instead to some other kind of onset.

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