American Institute of Aeronautics and Astronautics
1
Global Luminescent Oil-film Skin-Friction Meter
Generalized to Three-Dimensional Geometry and Applied to
FAITH Hill
Nicholas Husen
1
School of Aeronautics and Astronautics
Purdue University, West Lafayette, IN 47906
Sudesh Woodiga
2
, Tianshu Liu
3
Western Michigan University, Kalamazoo, MI 49008
and
John P. Sullivan
4
School of Aeronautics and Astronautics
Purdue University, West Lafayette, IN 47906
This paper further develops the global luminescent oil-film skin-friction meter by considering its
application to a three dimensional axisymmetric wall-mounted bump subjected to subsonic turbulent
boundary layer flow. The geometry gives rise to a necklace vortex and large scale separation on its lee
side. An oil-film is only usable by the global luminescent oil-film skin-friction meter if it meets certain
criteria. Most notably, it must be sufficiently thick to provide a good signal but not so thick that the
relationship between luminescent intensity and oil-film thickness becomes nonlinear. Different regions
on the model give rise to a usable oil-film at different times in an experiment. This paper proposes a
technique for the selection of which solutions from a sequence of “snapshot solutions” taken during the
run should be averaged for a particular region on the model. A relative skin-friction distribution
resulting from the techniques proposed herein is presented for each of four sections of the model: One
down the model’s centerline, and three across the model in the spanwise direction.
Nomenclature
y = height of model
H = total height of model
ℎ = thickness of oil film
r = radial distance from origin
ሺ
ଵ
,
ଶ
,
ଷ
ሻ = global coordinate system in object space
ሺ
ଵ
,
ଶ
,
ଷ
ሻ = coordinate system with 1-2 plane locally
tangent to surface
ሺ
ଵ
,
ଶ
,
ଷ
ሻ = coordinate system with 1-2 plane parallel
with image plane
S = function describing surface of model in
ሺ
ଵ
,
ଶ
,
ଷ
ሻ coordinates
= function describing surface of model in
ሺ
ଵ
,
ଶ
,
ଷ
ሻ coordinates
t = time
p = static pressure of external flow field
ߤ= dynamic viscosity of oil-film
= density of oil-film
1
Graduate Assistant, School of Aeronautics and Astronautics, 701 West Stadium Avenue. Student Member AIAA.
2
Graduate Assistant, Department of Mechanical and Aeronautical Engineering, Parkview Campus, MI 49008.
3
Professor, Department of Mechanical and Aeronautical Engineering, G-220, Parkview Campus, MI 49008, Senior Member
AIAA.
4
Professor, School of Aeronautics and Astronautics, 701 West StadiumAvenue. Fellow AIAA.
= -th component of gravity
= -th component of skin-friction
= change of coordinate matrix
I = Intensity of luminescent oil-film
ܫ
= Intensity of the excitation light incident
on the oil-film
= coefficient proportional to quantum
efficiency of luminescent molecules
= skin-friction
= equivelant skin-friction
= Lagrange multiplier
Downloaded by WESTERN MICHIGAN UNIVERSITY on March 15, 2015 | http://arc.aiaa.org | DOI: 10.2514/6.2014-1237
52nd Aerospace Sciences Meeting
13-17 January 2014, National Harbor, Maryland
AIAA 2014-1237
Copyright © 2014 by the American Institute of Aeronautics and Astronautics, Inc. All rights reserved.
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