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were not considered in detail in <strong>the</strong> literature [2, 29, 85, 104]. Starting point is <strong>the</strong> basic problem<br />

associated with <strong>the</strong> reproducible generation <strong>of</strong> sufficiently monodisperse liquid particles<br />

with an appropriate size, shape and density such that <strong>the</strong>y follow <strong>the</strong> macroscopic <strong>flow</strong> motion<br />

faithfully without disturbing <strong>the</strong> <strong>flow</strong> or fluid properties. In <strong>the</strong> past, very little attention has<br />

been paid to <strong>the</strong> observation that <strong>the</strong> particle size distribution generated may strongly deviate<br />

from <strong>the</strong> desired distribution if <strong>the</strong> liquid level in <strong>the</strong> aerosol generator changes, <strong>the</strong> pressure<br />

varies, or <strong>the</strong> nozzle holes are contaminated <strong>for</strong> any reason. This may cause serious problems<br />

as <strong>the</strong> accuracy <strong>of</strong> all tracer-based velocity measurement techniques, such as laser Doppler<br />

anemometry (LDA), particle image velocimetry (PIV) or Doppler global velocimetry (DGV),<br />

is ultimately determined by <strong>the</strong> particle dynamics [3]. Beside <strong>the</strong> fundamental problems associated<br />

with <strong>the</strong> generation <strong>of</strong> appropriate tracer particles, <strong>the</strong> registration, <strong>the</strong> storage and<br />

<strong>the</strong> read-out <strong>of</strong> <strong>the</strong> particle images will be investigated in detail in section 2.3. This process is<br />

ano<strong>the</strong>r key element in PIV as <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong> technique strongly depends on <strong>the</strong> precision<br />

with which <strong>the</strong> image displacement can be related to particle locations and <strong>the</strong>ir respective<br />

particle displacements [3]. Parts <strong>of</strong> <strong>the</strong> results have been already published in [39, 42, 47].<br />

Chapter 3 focuses on <strong>the</strong> stereoscopic PIV techniques because <strong>the</strong> conventional PIV system<br />

outlined in chapter 2 is not well suited to examine <strong>turbulent</strong> <strong>flow</strong>s <strong>for</strong> two reasons. First,<br />

only <strong>the</strong> projection <strong>of</strong> <strong>the</strong> three-dimensional <strong>flow</strong> velocity inside <strong>the</strong> measurement plane can<br />

be determined with <strong>the</strong> conventional PIV technique. Second, <strong>the</strong> two velocity components<br />

that can be measured are biased when <strong>the</strong> <strong>flow</strong> is three-dimensional because <strong>of</strong> <strong>the</strong> perspective<br />

error. In section 3.1 <strong>the</strong> advantages and drawbacks <strong>of</strong> various stereoscopic recording configurations<br />

will be compared and <strong>the</strong> basic principles <strong>of</strong> different evaluation schemes known<br />

as image warping, vector field warping and interrogation window warping will be discussed<br />

in section 3.2. Of primary interest is <strong>the</strong> investigation <strong>of</strong> <strong>the</strong> different image interpolation<br />

schemes which are required <strong>for</strong> <strong>the</strong> analysis <strong>of</strong> <strong>the</strong> image pairs, because <strong>the</strong> measurement error<br />

depends strongly on <strong>the</strong> interpolation algorithm applied. Ano<strong>the</strong>r systematic measurement<br />

error that was discovered by applying <strong>the</strong> stereoscopic PIV is investigated in section 3.3. As<br />

this error can be large relative to all o<strong>the</strong>r possible measurement errors a calibration validation<br />

technique is examined which has been developed to detect and compensate this error<br />

completely. <strong>The</strong> general material <strong>of</strong> this chapter is mainly based on [40, 42] and <strong>the</strong> section<br />

about <strong>the</strong> calibration validation method and <strong>the</strong> different evaluation schemes can be found<br />

partially in [39, 44].<br />

Chapter 4 describes <strong>the</strong> principles and properties <strong>of</strong> <strong>the</strong> multiplane stereo PIV technique.<br />

This technique was developed to obtain with high accuracy and spatial resolution in<strong>for</strong>mation<br />

about <strong>the</strong> spatio-temporal <strong>flow</strong> unsteadiness and to determine fundamentally important<br />

fluid-mechanical quantities which are presently not accessible with any o<strong>the</strong>r known measurement<br />

technique technique. First <strong>of</strong> all <strong>the</strong> principles and properties <strong>of</strong> <strong>the</strong> techniques will be<br />

outlined along with <strong>the</strong> required four pulse laser system. <strong>The</strong>reafter, <strong>the</strong> synchronisation and<br />

alignment <strong>of</strong> <strong>the</strong> system component will be discussed and different modes <strong>of</strong> operation will<br />

be outlined which have been applied <strong>for</strong> <strong>the</strong> fluid-mechanical investigations in chapter 6 and<br />

7. In section 4.6 and 4.7 polarisation effects and <strong>the</strong> effect <strong>of</strong> optical aberrations on <strong>the</strong> measurement<br />

precision will be studied. In particular, it will be shown how to reduce undesirable<br />

optical aberrations below <strong>the</strong> resolution <strong>of</strong> <strong>the</strong> recording medium and how to eliminate certain<br />

aberrations completely by accepting aberrations <strong>of</strong> o<strong>the</strong>r types which are <strong>of</strong> no harm in<br />

PIV. To examine <strong>the</strong> per<strong>for</strong>mance and reliability <strong>of</strong> <strong>the</strong> multiplane stereo PIV technique, <strong>the</strong><br />

acoustic receptivity <strong>of</strong> a laminar boundary layer along a flat plate with zero pressure gradient<br />

9

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