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Examination of the flow around a hot-wire probe using particle image velocimetry

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Abstract

Previous work has shown that the k 2 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 k 2 as calculated from the angle of deviation from the free stream.

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Abbreviations

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

α :

angle between free stream and degrees wire normal

δ :

angle through which flow is degrees deflected at working section of wire

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Graham, L.J.W., Soria, J. & Bremhorst, K. Examination of the flow around a hot-wire probe using particle image velocimetry. Experiments in Fluids 19, 379–382 (1995). https://doi.org/10.1007/BF00190254

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  • DOI: https://doi.org/10.1007/BF00190254

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