Abstract
Convective heat transfer occurs in a wide range of engineering applications, from nuclear reactors to portable electronic devices. Accurate whole-field turbulence and flow measurements are crucial to understanding convective heat transfer in complex flow fields, thereby enabling optimal design of these devices. Particle image velocimetry (PIV) is the preferred whole-field flow measurement technique. However in many configurations the dynamic velocity range of conventional PIV is too limited to accurately resolve both high mean velocities and turbulence intensities in lower velocity regions. This paper employs high dynamic range (HDR) PIV with an advanced acquisition and processing technique based on multiple pulse separation (MPS) double-frame imaging. The methodology uses a conventional adaptive multi-grid algorithm for vector evaluation, and determines the optimal pulse separation in space and time in a post-processing routine. Two test cases are discussed: For an impinging synthetic jet flow (Case I), HDR PIV increases the dynamic velocity range 25-fold compared to conventional PIV. For an oscillatory buoyant plume from a pair of horizontal heated cylinders (Case II), the dynamic velocity range is increased 5.5 times. This technique has yielded new insights in synthetic jet heat transfer by correlating local surface heat transfer rates to near-wall turbulence intensity in a single whole-field measurement.
Highlights
1.4 Objectives Using high dynamic range (HDR) particle image velocimetry (PIV) based on multiple pulse separation (MPS) acquisition, this paper aims to obtain more accurate whole-field flow and turbulence measurements for use in experimental convective heat transfer studies
The wide velocity range makes this an ideal case to demonstrate the benefits of HDR PIV
The paper has demonstrated the benefits of high dynamic range (HDR) particle image velocimetry for two heat convection test cases, an impinging synthetic jet flow and natural convection from a pair of heated horizontal cylinders
Summary
The dynamic velocity range DRV is defined as the ratio of maximum to minimum resolvable velocity, or ܴܦ ൌ ܸ௫Ȁߪ ൌ ݏ௫Ȁߪ௦ where ߪ and ߪ௦ are minimum resolvable velocity and particle displacement, respectively (ߪ ൌ ߪܯ௦Ȁ߬, where M is the spatial pixel resolution and W is the pulse separation time). The minimum resolvable displacement Vs is determined by the overall displacement uncertainty and bias error. Accuracy and error refer to systematic bias between measured and true values, whereas precision and uncertainty refer to the repeatability of the measurement. As PIV evaluation methods have evolved over time, the dynamic velocity range has been steadily improved. For single-pass correlation algorithms, Keane and Adrian [1] proposed a quarter window rule (smax < 1⁄4dI) to avoid excessive loss of correlation strength, yielding ܴܦሺௌሻ ൌ
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