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Erschienen in: Experiments in Fluids 1/2015

01.01.2015 | Research Article

A direct measure of the frequency response of hot-wire anemometers: temporal resolution issues in wall-bounded turbulence

verfasst von: N. Hutchins, J. P. Monty, M. Hultmark, A. J. Smits

Erschienen in: Experiments in Fluids | Ausgabe 1/2015

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Abstract

Based on the need to characterise the accuracy of hot-wire anemometry (HWA) in high Reynolds number wall-bounded turbulence, we here propose a novel direct method for testing the frequency response of various systems to very high frequency velocity fluctuations (up to 50 kHz). A fully developed turbulent pipe flow is exploited to provide the input velocity perturbations. Utilising the unique capabilities of the Princeton Superpipe, it is possible to explore a variety of turbulent pipe flows at matched Reynolds numbers, but with turbulent energy in different frequency ranges. Assuming Reynolds number similarity, any differences between the appropriately scaled energy spectra for these flows should be indicative of measurement error. Having established the accuracy of this testing procedure, the response of several anemometer and probe combinations is tested. While these tests do not provide a direct or definitive comparison between different anemometers (owing to non-optimal tuning in each case), they do provide useful examples of potential frequency responses that could be encountered in HWA experiments. These results are subsequently used to predict error arising from HWA response for measurements in wall-bounded turbulent flows. For current technology, based on the results obtained here, the frequency response of under- or over-damped HWA systems can only be considered approximately flat up to 5–7 kHz. For flows with substantial turbulent energy in frequencies above this range, errors in measured turbulence quantities due to temporal resolution are increasingly likely.

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Fußnoten
1
It should be noted that the precise value of \(S\) is not crucial to these experiments. An estimate is good enough. Any error in \(S\) will only slightly alter the overall Reynolds number at which we conducted the experiments (along with the \(z^{+}\) and \(l^{+}\) values). More importantly, the estimate of \(S\) in no way influences how well matched the experiments are in terms of \(Re_\tau \), \(z^{+}\), \(l^{+}\) , etc.
 
2
The square-wave response is measured in situ, with the probe at the centreline of the pipe with the centreline velocity \(U_{0}\) matched to the measured mean at \(z^{+} = 79\) for experiment \(e5\). Since the pipe has a turbulent core, the measured square-wave response is extracted from the turbulent signal using a triggered/conditional averaging technique—see Appendix 2.
 
3
These average response curves are the mean of the \(\chi_e\) verses \(f_e\) profiles determined for experiments \(e = 1\rightarrow 4\).
 
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Metadaten
Titel
A direct measure of the frequency response of hot-wire anemometers: temporal resolution issues in wall-bounded turbulence
verfasst von
N. Hutchins
J. P. Monty
M. Hultmark
A. J. Smits
Publikationsdatum
01.01.2015
Verlag
Springer Berlin Heidelberg
Erschienen in
Experiments in Fluids / Ausgabe 1/2015
Print ISSN: 0723-4864
Elektronische ISSN: 1432-1114
DOI
https://doi.org/10.1007/s00348-014-1856-8

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