Examination of the flow around a hot-wire probe using particle image velocimetry |
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Authors: | L. J. W. Graham J. Soria K. Bremhorst |
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Affiliation: | (1) CSIRO Division of Building, Construction and Engineering, PO Box 56, 3190 Highett, Victoria, Australia;(2) Department of Mechanical Engineering, Monash University, 3168 Clayton, Victoria, Australia;(3) Department of Mechanical Engineering, The University of Queensland, 4072 Brisbane, Qld, Australia |
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Abstract: | Previous work has shown that the k2 term in the effective cooling velocity equation for inclined hot-wires can become negative under certain probe configurations and wire length-to-diameter ratios. It was hypothesised that this was due to a downwash component of velocity along the wire when prong interference effects were expected to be minimal. Direct measurements of the flow around a typical hot-wire probe using digital particle image velocimetry have shown that this downwash velocity component does exist, leading to negative values of k2 as calculated from the angle of deviation from the free stream.List of symbols d diameter of hot-wire mm - k factor in equation for effective dimensionless velocity for inclined hot-wire - l length of hot-wire mm - Q effective velocity mm/s - U free stream velocity mm/s - angle between free stream and degrees wire normal - angle through which flow is degrees deflected at working section of wire |
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