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Publisher: Springer-Verlag   (Total: 2281 journals)

 Showing 1201 - 1400 of 2281 Journals sorted alphabetically J. of Earth Science       (Followers: 6, SJR: 0.299, h-index: 11) J. of Earth System Science       (Followers: 24, SJR: 0.466, h-index: 27) J. of East Asian Linguistics       (Followers: 5, SJR: 0.669, h-index: 15) J. of Echocardiography       (Followers: 3, SJR: 0.136, h-index: 3) J. of Economic Growth       (Followers: 25, SJR: 5.251, h-index: 54) J. of Economic Interaction and Coordination       (SJR: 0.231, h-index: 11) J. of Economics       (Followers: 9, SJR: 0.463, h-index: 20) J. of Economics and Finance       (Followers: 7, SJR: 0.238, h-index: 15) J. of Educational Change       (Followers: 7, SJR: 0.694, h-index: 14) J. of Elasticity       (Followers: 4, SJR: 0.821, h-index: 38) J. of Electroceramics       (SJR: 0.566, h-index: 49) J. of Electronic Materials       (Followers: 2, SJR: 0.752, h-index: 68) J. of Electronic Testing       (Followers: 2, SJR: 0.241, h-index: 24) J. of Electronics (China)       (Followers: 3, SJR: 0.127, h-index: 7) J. of Elementary Science Education       (Followers: 8) J. of Engineering Mathematics       (SJR: 0.707, h-index: 32) J. of Engineering Physics and Thermophysics       (SJR: 0.132, h-index: 8) J. of Engineering Research J. of Engineering Thermophysics       (SJR: 0.294, h-index: 7) J. of Environmental Studies and Sciences       (Followers: 2) J. of Ethology       (Followers: 2, SJR: 0.484, h-index: 21) J. of Evolution Equations       (SJR: 1.312, h-index: 22) J. of Evolutionary Biochemistry and Physiology       (SJR: 0.127, h-index: 9) J. of Evolutionary Economics       (Followers: 8, SJR: 0.878, h-index: 42) J. of Experimental and Theoretical Physics       (Followers: 2, SJR: 0.565, h-index: 34) J. of Experimental Criminology       (Followers: 26, SJR: 1.587, h-index: 22) J. of Failure Analysis and Prevention       (Followers: 1, SJR: 0.256, h-index: 12) J. of Family and Economic Issues       (Followers: 6, SJR: 0.532, h-index: 27) J. of Family Violence       (Followers: 15, SJR: 0.552, h-index: 45) J. of Financial Services Research       (Followers: 16, SJR: 1.196, h-index: 29) J. of Fixed Point Theory and Applications       (SJR: 0.467, h-index: 10) J. of Fluorescence       (Followers: 4, SJR: 0.553, h-index: 47) J. of Food Measurement and Characterization       (SJR: 0.104, h-index: 1) J. of Food Science and Technology       (Followers: 5, SJR: 0.839, h-index: 21) J. of Forest Research       (Followers: 3, SJR: 0.578, h-index: 22) J. of Forestry Research       (Followers: 6, SJR: 0.271, h-index: 10) J. of Fourier Analysis and Applications       (Followers: 1, SJR: 1.248, h-index: 36) J. of Friction and Wear       (Followers: 6, SJR: 0.263, h-index: 6) J. of Fusion Energy       (Followers: 3, SJR: 0.389, h-index: 16) J. of Gambling Studies       (Followers: 3, SJR: 1.122, h-index: 50) J. of Gastroenterology       (Followers: 13, SJR: 1.724, h-index: 73) J. of Gastrointestinal Cancer       (Followers: 3, SJR: 0.371, h-index: 36) J. of Gastrointestinal Surgery       (Followers: 5, SJR: 1.632, h-index: 87) J. of General Internal Medicine       (Followers: 12, SJR: 2.379, h-index: 115) J. of General Plant Pathology       (SJR: 0.357, h-index: 17) J. of Genetic Counseling       (Followers: 4, SJR: 0.535, h-index: 32) J. of Genetics       (Followers: 4, SJR: 0.42, h-index: 24) J. of Geodesy       (Followers: 8, SJR: 4.049, h-index: 48) J. of Geographical Sciences       (Followers: 1, SJR: 0.58, h-index: 14) J. of Geographical Systems       (Followers: 2, SJR: 0.839, h-index: 32) J. of Geometric Analysis       (SJR: 1.496, h-index: 23) J. of Geometry       (Followers: 1, SJR: 0.349, h-index: 13) J. of Global Optimization       (Followers: 3, SJR: 0.919, h-index: 51) J. of Global Policy and Governance       (Followers: 8) J. of Grid Computing       (SJR: 0.727, h-index: 32) J. of Hand and Microsurgery       (Followers: 1) J. of Happiness Studies       (Followers: 14, SJR: 0.785, h-index: 30) J. of Hematopathology       (Followers: 3, SJR: 0.194, h-index: 11) J. of Heuristics       (Followers: 5, SJR: 1.718, h-index: 43) J. of High Energy Physics       (Followers: 4, SJR: 1.027, h-index: 139) J. of Homotopy and Related Structures       (SJR: 0.102, h-index: 1) J. of Housing and the Built Environment       (Followers: 6, SJR: 0.553, h-index: 21) J. of Huazhong University of Science and Technology [Medical Sciences]       (SJR: 0.317, h-index: 15) J. of Ichthyology       (Followers: 4, SJR: 0.28, h-index: 7) J. of Immigrant and Minority Health       (Followers: 8, SJR: 0.573, h-index: 29) J. of Inclusion Phenomena and Macrocyclic Chemistry       (Followers: 1, SJR: 0.459, h-index: 41) J. of Indian Philosophy       (Followers: 10, SJR: 0.179, h-index: 7) J. of Indian Prosthodontic Society       (SJR: 0.165, h-index: 5) J. of Industrial Microbiology and Biotechnology       (Followers: 10, SJR: 1.064, h-index: 68) J. of Industry, Competition and Trade       (Followers: 7, SJR: 0.411, h-index: 11) J. of Infection and Chemotherapy       (Followers: 1, SJR: 0.65, h-index: 39) J. of Infrared, Millimeter and Terahertz Waves       (Followers: 1, SJR: 0.902, h-index: 31) J. of Inherited Metabolic Disease       (Followers: 2, SJR: 1.182, h-index: 66) J. of Inorganic and Organometallic Polymers and Materials       (Followers: 6, SJR: 0.316, h-index: 27) J. of Insect Behavior       (Followers: 8, SJR: 0.537, h-index: 36) J. of Insect Conservation       (Followers: 9, SJR: 0.775, h-index: 36) J. of Intelligent and Robotic Systems       (Followers: 2, SJR: 0.501, h-index: 36) J. of Intelligent Information Systems       (Followers: 1, SJR: 0.427, h-index: 39) J. of Intelligent Manufacturing       (Followers: 4, SJR: 1.095, h-index: 44) J. of Interventional Cardiac Electrophysiology       (SJR: 1.073, h-index: 38) J. of Intl. Entrepreneurship       (Followers: 8, SJR: 0.489, h-index: 16) J. of Intl. Migration and Integration / Revue de l integration et de la migration internationale       (Followers: 12, SJR: 0.385, h-index: 9) J. of Labor Research       (Followers: 14, SJR: 0.228, h-index: 21) J. of Logic, Language and Information       (Followers: 5, SJR: 0.63, h-index: 20) J. of Low Temperature Physics       (Followers: 1, SJR: 0.773, h-index: 48) J. of Machinery Manufacture and Reliability       (Followers: 2, SJR: 0.194, h-index: 4) J. of Mammalian Evolution       (Followers: 5, SJR: 1.845, h-index: 32) J. of Mammary Gland Biology and Neoplasia       (Followers: 1, SJR: 3.22, h-index: 73) J. of Management and Governance       (Followers: 12, SJR: 0.383, h-index: 26) J. of Management Control       (Followers: 4, SJR: 0.134, h-index: 4) J. of Marine Science and Application       (Followers: 3, SJR: 0.343, h-index: 8) J. of Marine Science and Technology       (Followers: 3, SJR: 0.317, h-index: 22) J. of Maritime Archaeology       (Followers: 21, SJR: 0.19, h-index: 5) J. of Market-Focused Management       (Followers: 2) J. of Material Cycles and Waste Management       (Followers: 3, SJR: 0.392, h-index: 16) J. of Materials Engineering and Performance       (Followers: 24, SJR: 0.666, h-index: 31) J. of Materials Science       (Followers: 18, SJR: 1.006, h-index: 101) J. of Materials Science : Materials in Electronics       (Followers: 3, SJR: 0.697, h-index: 48) J. of Materials Science : Materials in Medicine       (Followers: 4, SJR: 0.926, h-index: 77) J. of Mathematical Biology       (Followers: 13, SJR: 1.183, h-index: 61) J. of Mathematical Chemistry       (Followers: 5, SJR: 0.407, h-index: 41) J. of Mathematical Fluid Mechanics       (Followers: 5, SJR: 1.709, h-index: 17) J. of Mathematical Imaging and Vision       (Followers: 3, SJR: 1.25, h-index: 44) J. of Mathematical Modelling and Algorithms       (Followers: 2, SJR: 0.358, h-index: 19) J. of Mathematical Sciences       (SJR: 0.32, h-index: 20) J. of Mathematics Teacher Education       (Followers: 13, SJR: 1.042, h-index: 14) J. of Maxillofacial and Oral Surgery       (Followers: 1) J. of Mechanical Science and Technology       (Followers: 4, SJR: 0.589, h-index: 20) J. of Medical and Biological Engineering       (SJR: 0.434, h-index: 13) J. of Medical Humanities       (Followers: 18, SJR: 0.251, h-index: 13) J. of Medical Systems       (Followers: 2, SJR: 0.604, h-index: 32) J. of Medical Toxicology       (Followers: 6, SJR: 0.765, h-index: 21) J. of Medical Ultrasonics       (Followers: 2, SJR: 0.209, h-index: 11) J. of Medicine and the Person J. of Membrane Biology       (Followers: 1, SJR: 0.971, h-index: 75) J. of Micro-Bio Robotics J. of Microbiology       (Followers: 7, SJR: 0.641, h-index: 35) J. of Mining Science       (Followers: 5, SJR: 0.296, h-index: 11) J. of Molecular Evolution       (Followers: 11, SJR: 1.07, h-index: 99) J. of Molecular Histology       (Followers: 2, SJR: 0.791, h-index: 43) J. of Molecular Medicine       (Followers: 15, SJR: 2.452, h-index: 100) J. of Molecular Modeling       (Followers: 4, SJR: 0.55, h-index: 42) J. of Molecular Neuroscience       (Followers: 8, SJR: 1.242, h-index: 61) J. of Mountain Science       (Followers: 3, SJR: 0.295, h-index: 11) J. of Muscle Research and Cell Motility       (SJR: 1.052, h-index: 51) J. of Nanoparticle Research       (Followers: 2, SJR: 0.777, h-index: 66) J. of Natural Medicines       (SJR: 0.586, h-index: 22) J. of Near-Death Studies       (Followers: 2) J. of Nephrology       (Followers: 5, SJR: 0.857, h-index: 48) J. of Network and Systems Management       (SJR: 0.331, h-index: 23) J. of Neural Transmission       (Followers: 2, SJR: 1.302, h-index: 77) J. of Neuro-Oncology       (Followers: 3, SJR: 1.342, h-index: 80) J. of Neuroimmune Pharmacology       (Followers: 1, SJR: 1.239, h-index: 36) J. of Neurology       (Followers: 13, SJR: 1.406, h-index: 91) J. of NeuroVirology       (Followers: 1, SJR: 1.367, h-index: 63) J. of Nondestructive Evaluation       (Followers: 7, SJR: 0.452, h-index: 22) J. of Nonlinear Science       (Followers: 1, SJR: 1.772, h-index: 36) J. of Nonverbal Behavior       (Followers: 3, SJR: 1.122, h-index: 38) J. of Nuclear Cardiology       (SJR: 1.456, h-index: 60) J. of Nutrition, Health and Aging       (Followers: 17, SJR: 0.886, h-index: 50) J. of Obstetrics and Gynecology of India       (Followers: 7, SJR: 0.174, h-index: 3) J. of Occupational Rehabilitation       (Followers: 11, SJR: 1.166, h-index: 43) J. of Ocean Engineering and Marine Energy       (Followers: 1) J. of Ocean University of China (English Edition)       (SJR: 0.144, h-index: 8) J. of Oceanography       (Followers: 7, SJR: 1.031, h-index: 46) J. of Ocular Biology, Diseases, and Informatics       (SJR: 0.228, h-index: 8) J. of Optical and Fiber Communications Reports       (Followers: 2, SJR: 0.831, h-index: 2) J. of Optics       (Followers: 4) J. of Optimization Theory and Applications       (Followers: 2, SJR: 0.928, h-index: 55) J. of Ornithology       (Followers: 20) J. of Orofacial Orthopedics / Fortschritte der Kieferorthopädie       (SJR: 0.667, h-index: 27) J. of Orthopaedic Science       (Followers: 5, SJR: 0.684, h-index: 42) J. of Paleolimnology       (Followers: 5, SJR: 1.284, h-index: 58) J. of Parasitic Diseases       (Followers: 2, SJR: 0.272, h-index: 5) J. of Pediatric Neuropsychology J. of Pest Science       (Followers: 2, SJR: 1.002, h-index: 21) J. of Pharmaceutical Health Care and Sciences J. of Pharmaceutical Innovation       (Followers: 7, SJR: 0.617, h-index: 14) J. of Pharmaceutical Investigation       (Followers: 1, SJR: 0.16, h-index: 2) J. of Pharmacokinetics and Pharmacodynamics       (Followers: 22, SJR: 0.567, h-index: 41) J. of Phase Equilibria and Diffusion       (Followers: 19, SJR: 0.367, h-index: 31) J. of Philosophical Logic       (Followers: 7, SJR: 0.94, h-index: 20) J. of Physiology and Biochemistry       (Followers: 3, SJR: 0.741, h-index: 30) J. of Plant Biochemistry and Biotechnology       (Followers: 5, SJR: 0.257, h-index: 17) J. of Plant Biology       (Followers: 9, SJR: 0.52, h-index: 16) J. of Plant Growth Regulation       (Followers: 1, SJR: 0.761, h-index: 47) J. of Plant Research       (Followers: 4, SJR: 1.055, h-index: 43) J. of Police and Criminal Psychology       (Followers: 414, SJR: 0.328, h-index: 10) J. of Polymer Research       (Followers: 6, SJR: 0.649, h-index: 27) J. of Polymers and the Environment       (Followers: 1, SJR: 0.618, h-index: 39) J. of Population Ageing       (Followers: 4, SJR: 0.357, h-index: 3) J. of Population Economics       (Followers: 16, SJR: 2.455, h-index: 42) J. of Population Research       (Followers: 1, SJR: 0.404, h-index: 10) J. of Porous Materials       (Followers: 3, SJR: 0.523, h-index: 34) J. of Primary Prevention       (Followers: 6, SJR: 0.816, h-index: 30) J. of Productivity Analysis       (Followers: 2, SJR: 0.825, h-index: 48) J. of Pseudo-Differential Operators and Applications       (SJR: 1.275, h-index: 5) J. of Psycholinguistic Research       (Followers: 9, SJR: 0.445, h-index: 37) J. of Psychology and Judaism       (Followers: 2) J. of Psychopathology and Behavioral Assessment       (Followers: 1, SJR: 0.949, h-index: 39) J. of Psychosocial Rehabilitation and Mental Health       (Followers: 3) J. of Public Health       (Followers: 23, SJR: 0.262, h-index: 17) J. of Quantitative Criminology       (Followers: 6, SJR: 2.481, h-index: 44) J. of Racial and Ethnic Health Disparities       (Followers: 1) J. of Radiation Oncology       (Followers: 1) J. of Radioanalytical and Nuclear Chemistry       (Followers: 5, SJR: 0.515, h-index: 44) J. of Radiosurgery       (Followers: 2) J. of Rational-Emotive & Cognitive-Behavior Therapy       (Followers: 1, SJR: 0.394, h-index: 19) J. of Real-Time Image Processing       (Followers: 6, SJR: 0.356, h-index: 16) J. of Regulatory Economics       (Followers: 7, SJR: 1.081, h-index: 35) J. of Religion and Health       (Followers: 10, SJR: 0.483, h-index: 18) J. of Religious Education       (Followers: 3) J. of Risk and Uncertainty       (Followers: 19, SJR: 2.34, h-index: 46) J. of Robotic Surgery       (SJR: 0.227, h-index: 11) J. of Russian Laser Research       (SJR: 0.326, h-index: 18) J. of Scheduling       (Followers: 2, SJR: 1.417, h-index: 38) J. of Science Education and Technology       (Followers: 16, SJR: 0.754, h-index: 30) J. of Science Teacher Education       (Followers: 17, SJR: 1.128, h-index: 22) J. of Scientific Computing       (Followers: 18, SJR: 1.771, h-index: 42) J. of Seismology       (Followers: 8, SJR: 0.855, h-index: 34)
 Experiments in Fluids   [SJR: 1.596]   [H-I: 69]   [7 followers]  Follow         Hybrid journal (It can contain Open Access articles)    ISSN (Print) 1432-1114 - ISSN (Online) 0723-4864    Published by Springer-Verlag  [2281 journals]
• Color gradient background-oriented schlieren imaging
• Abstract: Abstract Background-oriented schlieren is a method of visualizing refractive disturbances by comparing digital images with and without a refractive disturbance distorting a background pattern. Traditionally, backgrounds consist of random distributions of high-contrast color transitions or speckle patterns. To image a refractive disturbance, a digital image correlation algorithm is used to identify the location and magnitude of apparent pixel shifts in the background pattern between the two images. Here, a novel method of using color gradient backgrounds is explored as an alternative that eliminates the need to perform a complex image correlation between the digital images. A simple image subtraction can be used instead to identify the location, magnitude, and direction of the image distortions. Gradient backgrounds are demonstrated to provide quantitative data only limited by the camera’s pixel resolution, whereas speckle backgrounds limit resolution to the size of the random pattern features and image correlation window size. Quantitative measurement of density in a thermal boundary layer is presented. Two-dimensional gradient backgrounds using multiple colors are demonstrated to allow measurement of two-dimensional refractions. A computer screen is used as the background, which allows for rapid modification of the gradient to tune sensitivity for a particular application.
PubDate: 2016-05-17

• Dynamic mode decomposition for non-uniformly sampled data
• Abstract: Abstract We propose an original approach to estimate dynamic mode decomposition (DMD) modes from non-uniformly sampled data. The proposed strategy processes a time-resolved sequence of flow snapshots in three steps. First, a reduced-order modeling of the non-missing data is made by proper orthogonal decomposition to obtain a low-order description of the state space. Second, the missing data are determined with maximum likelihood by coupling a linear dynamical state-space model with the Expectation-Maximization algorithm. Third, the DMD modes are finally estimated on the reconstructed data with a multiple linear regression method called orthonormalized partial least squares regression. This methodology is assessed for the flow past a NACA0012 airfoil at 20° of angle of attack and a Reynolds number of 103. The flow measurements are obtained with time-resolved particle image velocimetry and artificially subsampled at different ratios of missing data. The results show that the proposed method can reproduce the dominant DMD modes and the main structures of the flow fields for 50 and 75 % of missing data.
PubDate: 2016-05-14

• Reattachment heating upstream of short compression ramps in hypersonic
flow
• Abstract: Abstract Hypersonic shock-wave/boundary-layer interactions with separation induce unsteady thermal loads of particularly high intensity in flow reattachment regions. Building on earlier semi-empirical correlations, the maximum heat transfer rates upstream of short compression ramp obstacles of angles $$15^{\circ }\leqslant \theta \leqslant 135^{\circ }$$ are here discretised based on time-dependent experimental measurements to develop insight into their transient nature ( $$M_{e}$$ = 8.2–12.3, $$Re_h= 0.17\times 10^{5}$$ – $$0.47\times 10^{5}$$ ). Interactions with an incoming laminar boundary layer experience transition at separation, with heat transfer oscillating between laminar and turbulent levels exceeding slightly those in fully turbulent interactions. Peak heat transfer rates are strongly influenced by the stagnation of the flow upon reattachment close ahead of obstacles and increase with ramp angle all the way up to $$\theta =135^{\circ }$$ , whereby rates well over two orders of magnitude above the undisturbed laminar levels are intermittently measured ( $$q'_\mathrm{max}>10^2q_{u,L}$$ ). Bearing in mind the varying degrees of strength in the competing effect between the inviscid and viscous terms—namely the square of the hypersonic similarity parameter $$(M\theta )^2$$ for strong interactions and the viscous interaction parameter $$\bar{\chi }$$ (primarily a function of Re and M)—the two physical factors that appear to most globally encompass the effects of peak heating for blunt ramps ( $$\theta \geqslant 45^{\circ }$$ ) are deflection angle and stagnation heat transfer, so that this may be fundamentally expressed as $$q'_\mathrm{max}\propto {q_{o,2D}}$$ $$\theta ^2$$ with further parameters in turn influencing the interaction to a lesser extent. The dominant effect of deflection angle is restricted to short obstacle heights, where the rapid expansion at the top edge of the obstacle influences the relaxation region just downstream of reattachment and leads to an upstream displacement of the separation front. The extreme heating rates result from the strengthening of the reattaching shear layer with the increase in separation length for higher deflection angle.
PubDate: 2016-05-12

• IR thermography for dynamic detection of laminar-turbulent transition
• Abstract: Abstract This work investigates the potential of infrared (IR) thermography for the dynamic detection of laminar-turbulent transition. The experiments are conducted on a flat plate at velocities of 8–14 m/s, and the transition of the laminar boundary layer to turbulence is forced by a disturbance source which is turned on and off with frequencies up to 10 Hz. Three different heating techniques are used to apply the required difference between fluid and structure temperature: a heated aluminum structure is used as an internal structure heating technique, a conductive paint acts as a surface bounded heater, while an IR heater serves as an example for an external heating technique. For comparison of all heating techniques, a normalization is introduced and the frequency response of the measured IR camera signal is analyzed. Finally, the different heating techniques are compared and consequences for the design of experiments on laminar-turbulent transition are discussed.
PubDate: 2016-05-12

• Flow topology and acoustic emissions of trailing edge serrations at
incidence
• Abstract: Abstract The flow past a NACA 0018 airfoil with sawtooth trailing edge serrations has been investigated using stereoscopic particle image velocimetry (PIV). The serration flap angle and airfoil incidence are varied in order to study the effect of secondary flow establishing between the suction and pressure sides of the serrations. The flow topology around the serrations is inferred from the analysis of time-averaged streamlines close to the airfoil surface and from the wall-normal flow velocity in between serrations. Additional PIV measurements with a plane in cross-flow highlight the formation of streamwise vortex pairs. The flow behavior is further characterized in terms of its turbulence statistics. Noise emissions are measured with an acoustic phased array in combination with beamforming. The serrations are found to be effective in reducing noise, and their application is studied for different degrees of airfoil incidence and serration flap angle.
PubDate: 2016-05-11

• Wall-drag measurements of smooth- and rough-wall turbulent boundary layers
using a floating element
• Abstract: Abstract The mean wall shear stress, $$\overline{\tau }_w$$ , is a fundamental variable for characterizing turbulent boundary layers. Ideally, $$\overline{\tau }_w$$ is measured by a direct means and the use of floating elements has long been proposed. However, previous such devices have proven to be problematic due to low signal-to-noise ratios. In this paper, we present new direct measurements of $$\overline{\tau }_w$$ where high signal-to-noise ratios are achieved using a new design of a large-scale floating element with a surface area of 3 m (streamwise) × 1 m (spanwise). These dimensions ensure a strong measurement signal, while any error associated with an integral measurement of $$\overline{\tau }_w$$ is negligible in Melbourne’s large-scale turbulent boundary layer facility. Wall-drag induced by both smooth- and rough-wall zero-pressure-gradient flows are considered. Results for the smooth-wall friction coefficient, $$C_f \equiv \overline{\tau }_w/q_{\infty }$$ , follow a Coles–Fernholz relation $$C_f = \left[ 1/\kappa \ln \left( Re_{\theta }\right) + C\right] ^{-2}$$ to within 3 % ( $$\kappa = 0.38$$ and $$C = 3.7$$ ) for a momentum thickness-based Reynolds number, $$Re_{\theta } > 15{,}000$$ . The agreement improves for higher Reynolds numbers to <1 % deviation for $$Re_{\theta } > 38{,}000$$ . This smooth-wall benchmark verification of the experimental apparatus is critical before attempting any rough-wall studies. For a rough-wall configuration with P36 grit sandpaper, measurements were performed for $$10{,}500< Re_{\theta } < 88{,}500$$ , for which the wall-drag indicates the anticipated trend from the transitionally to the fully rough regime .
PubDate: 2016-05-09

• Development and characterization of high-frequency resonance-enhanced
microjet actuators for control of high-speed jets
• Abstract: Abstract For flow control applications requiring high-frequency excitation, very few actuators have sufficient dynamic response and/or control authority to be useful in high-speed flows. Due to this reason, experiments involving high-frequency excitation, attempted in the past, have been limited to either low-frequency actuation with reasonable control authority or moderate-frequency actuation with limited control authority. The current work expands on the previous development of the resonance-enhanced microactuators to design actuators that are capable of producing high-amplitude pulses at much higher frequencies [ $$\mathcal {O}$$ (10 kHz)]. Using lumped element modeling, two actuators have been designed with nominal frequencies of 20 and 50 kHz. Extensive benchtop characterization using acoustic measurements as well as optical diagnostics using a high-resolution micro-schlieren setup is employed to characterize the dynamic response of these actuators. The actuators performed at a range of frequencies, 20.3–27.8 and 54.8–78.2 kHz, respectively. In addition to providing information on the actuator flow physics and performance at various operating conditions, this study serves to develop easy-to-integrate high-frequency actuators for active control of high-speed jets. Preliminary testing of these actuators is performed by implementing the 20-kHz actuator on a Mach 0.9 free jet flow field for noise reduction. Acoustic measurements in the jet near field demonstrate attenuation of radiated noise at all observation angles.
PubDate: 2016-05-07

• Technique for studying ablation-products transport in supersonic boundary
layers by using PLIF of naphthalene
• Abstract: Abstract A technique is developed that uses planar laser-induced fluorescence (PLIF) of sublimated gas-phase naphthalene to visualize the transport of ablation products in a high-speed turbulent boundary layer. The naphthalene is molded into a rectangular insert that is mounted flush with the floor of a Mach 5 wind tunnel, where the test gas is air. The naphthalene fluorescence is excited with 266 nm laser light, and broadband detection of the emitted light is used. Using spectroscopic data from a previous study and a first-order approximation for the mean temperature profile across the boundary layer, naphthalene PLIF images collected in a Mach 5 turbulent boundary layer are converted into two-dimensional fields of naphthalene mole fraction with an instantaneous uncertainty of ±20 %. These quantitative naphthalene PLIF images in the Mach 5 boundary layer reveal large-scale naphthalene vapor structures that are regularly ejected out to wall distances of approximately y/δ = 0.6 for a field of view that spans 3δ–5δ downstream of the trailing edge of the naphthalene insert. The magnitude of the calculated naphthalene mole fraction in these structures at y/δ = 0.2 ranges from approximately 1 to 6 % of the saturation mole fraction at the wind tunnel recovery temperature and static pressure. Mean mole fraction profiles taken at different streamwise locations collapse into one “universal” mole fraction profile when properly normalized and are in agreement with previous scalar dispersion measurements. The results indicate that PLIF of sublimating naphthalene can be an effective tool for studying scalar transport in supersonic and hypersonic flows.
PubDate: 2016-05-07

• Intensity-enhanced MART for tomographic PIV
• Abstract: Abstract A novel technique to shrink the elongated particles and suppress the ghost particles in particle reconstruction of tomographic particle image velocimetry is presented. This method, named as intensity-enhanced multiplicative algebraic reconstruction technique (IntE-MART), utilizes an inverse diffusion function and an intensity suppressing factor to improve the quality of particle reconstruction and consequently the precision of velocimetry. A numerical assessment about vortex ring motion with and without image noise is performed to evaluate the new algorithm in terms of reconstruction, particle elongation and velocimetry. The simulation is performed at seven different seeding densities. The comparison of spatial filter MART and IntE-MART on the probability density function of particle peak intensity suggests that one of the local minima of the distribution can be used to separate the ghosts and actual particles. Thus, ghost removal based on IntE-MART is also introduced. To verify the application of IntE-MART, a real plate turbulent boundary layer experiment is performed. The result indicates that ghost reduction can increase the accuracy of RMS of velocity field.
PubDate: 2016-05-06

• Experimental investigation of the Faraday instability on a patterned
surface
• Abstract: Abstract The effect of patterned substrates on the onset and behavior of the Faraday instability is studied experimentally. We show that the onset of Faraday standing waves in a vertically oscillating layer of liquid can be delayed due to the topography of the underlying two-dimensional patterned substrate. The magnitude of this stabilization effect can be predicted by existing linear stability theories, and we provide an additional physical explanation for the behavior. These observations suggest the feasibility of exploiting the Faraday instability in thin liquid layers in practical engineering systems.
PubDate: 2016-05-06

• POD-Galerkin advection model for convective flow: application to a
flapping rectangular supersonic jet
• Abstract: Abstract This article describes a model obtained by applying proper orthogonal decomposition to the advection equation. The resulting set of equations links the POD modes, their temporal and spatial derivatives and the flow convection velocity. It provides a technique to calculate the convection velocity of coherent structures. It follows, from the model, that a priori knowledge of the convection velocity suffices to construct a dynamical model of the flow. This is demonstrated using experimental data.
PubDate: 2016-05-05

• A synchronized particle image velocimetry and infrared thermography
technique applied to convective mass transfer in champagne glasses
• Abstract: Abstract In champagne glasses, it was recently suggested that ascending bubble-driven flow patterns should be involved in the release of gaseous carbon dioxide (CO2) and volatile organic compounds. A key assumption was that the higher the velocity of the upward bubble-driven flow patterns in the liquid phase, the higher the volume fluxes of gaseous CO2 desorbing from the supersaturated liquid phase. In the present work, simultaneous monitoring of bubble-driven flow patterns within champagne glasses and gaseous CO2 escaping above the champagne surface was performed, through particle image velocimetry and infrared thermography techniques. Two quite emblematic types of champagne drinking vessels were investigated, namely a long-stemmed flute and a wide coupe. The synchronized use of both techniques proved that the cloud of gaseous CO2 escaping above champagne glasses strongly depends on the mixing flow patterns found in the liquid phase below.
PubDate: 2016-05-05

• Delayed lubricant depletion on liquid-infused randomly rough surfaces
• Abstract: Abstract In this study, pressure drops on liquid-infused superhydrophobic surfaces were measured through a microchannel. A number of different superhydrophobic surfaces were prepared and tested. These surfaces included several PDMS surfaces containing precisely patterned microposts and microridges as well as a number of PTFE surfaces with random surface roughness created by sanding the PTFE with different sandpapers. Silicone oil was selected as the lubricant fluid and infused into the microstructures of the superhydrophobic surfaces. Several aqueous glycerin solutions with different viscosities were used as working fluids so that the viscosity ratio between the lubricant and the working fluid could be varied. The lubricant layer trapped within the precisely patterned superhydrophobic PDMS surfaces was found to be easily depleted over a short period of time even in limit of low flow rates and capillary numbers. On the other hand, the randomly rough superhydrophobic PTFE surfaces tested were found to maintain the layer of lubricant oil even at moderately high capillary numbers resulting in drag reduction that was found to increase with increasing viscosity ratio. The pressure drops on the liquid-infused PTFE surfaces were measured over time to determine the longevity of the lubricant layer. The pressure drops for the randomly rough PTFE surfaces were found to initially diminish with time before reaching a short-time plateau which is equivalent to maximum drag reduction. This minimum pressure drop was maintained for at least three hours in all cases regardless of feature size. However, as the depletion of the oil from the lubricant layer was initiated, the pressure drop was observed to grow slowly before reaching a second long-time asymptote which was equivalent to a Wenzel state.
PubDate: 2016-05-04

• Estimation of the measurement uncertainty in magnetic resonance
velocimetry based on statistical models
• Abstract: Abstract Velocity measurements with magnetic resonance velocimetry offer outstanding possibilities for experimental fluid mechanics. The purpose of this study was to provide practical guidelines for the estimation of the measurement uncertainty in such experiments. Based on various test cases, it is shown that the uncertainty estimate can vary substantially depending on how the uncertainty is obtained. The conventional approach to estimate the uncertainty from the noise in the artifact-free background can lead to wrong results. A deviation of up to $$-75\,\%$$ is observed with the presented experiments. In addition, a similarly high deviation is demonstrated with the data from other studies. As a more accurate approach, the uncertainty is estimated directly from the image region with the flow sample. Two possible estimation methods are presented.
PubDate: 2016-05-04

• Global surface pressure measurements of static and dynamic stall on a wind
turbine airfoil at low Reynolds number
• Abstract: Abstract Recognizing the need for global surface measurement techniques to characterize the time-varying, three-dimensional loading encountered on rotating wind turbine blades, fast-responding pressure-sensitive paint (PSP) has been evaluated for resolving unsteady aerodynamic effects in incompressible flow. Results of a study aimed at demonstrating the laser-based, single-shot PSP technique on a low Reynolds number wind turbine airfoil in static and dynamic stall are reported. PSP was applied to the suction side of a Delft DU97-W-300 airfoil (maximum thickness-to-chord ratio of 30 %) at a chord Reynolds number of 225,000 in the University of Wyoming open-return wind tunnel. Static and dynamic stall behaviors are presented using instantaneous and phase-averaged global pressure maps. In particular, a three-dimensional pressure topology driven by a stall cell pattern is detected near the maximum lift condition on the steady airfoil. Trends in the PSP-measured pressure topology on the steady airfoil were confirmed using surface oil visualization. The dynamic stall case was characterized by a sinusoidal pitching motion with mean angle of 15.7°, amplitude of 11.2°, and reduced frequency of 0.106 based on semichord. PSP images were acquired at selected phase positions, capturing the breakdown of nominally two-dimensional flow near lift stall, development of post-stall suction near the trailing edge, and a highly three-dimensional topology as the flow reattaches. Structural patterns in the surface pressure topologies are considered from the analysis of the individual PSP snapshots, enabled by a laser-based excitation system that achieves sufficient signal-to-noise ratio in the single-shot images. The PSP results are found to be in general agreement with observations about the steady and unsteady stall characteristics expected for the airfoil.
PubDate: 2016-05-04

• On the wake flow of asymmetrically beveled trailing edges
• Abstract: Abstract Trailing edge and wake flows are of interest for a wide range of applications. Small changes in the design of asymmetrically beveled or semi-rounded trailing edges can result in significant difference in flow features which are relevant for the aerodynamic performance, flow-induced structural vibration and aerodynamically generated sound. The present study describes in detail the flow field characteristics around a family of asymmetrically beveled trailing edges with an enclosed trailing-edge angle of $$25^\circ$$ and variable radius of curvature R. The flow fields over the beveled trailing edges are described using data obtained by particle image velocimetry (PIV) experiments. The flow topology for different trailing edges was found to be strongly dependent on the radius of curvature R, with flow separation occurring further downstream as R increases. This variation in the location of flow separation influences the aerodynamic force coefficients, which were evaluated from the PIV data using a control volume approach. Two-point correlations of the in-plane velocity components are considered to assess the structure in the flow field. The analysis shows large-scale coherent motions in the far wake, which are associated with vortex shedding. The wake thickness parameter $$y_{f}$$ is confirmed as an appropriate length scale to characterize this large-scale roll-up motion in the wake. The development in the very near wake was found to be critically dependent on R. In addition, high-speed PIV measurements provide insight into the spectral characteristics of the turbulent fluctuations. Based on the time-resolved flow field data, the frequency range associated with the shedding of coherent vortex pairs in the wake is identified. By means of time-correlation of the velocity components, turbulent structures are found to convect from the attached or separated shear layers without distinct separation point into the wake.
PubDate: 2016-05-03

• Tomographic PIV behind a prosthetic heart valve
• Abstract: Abstract The instantaneous three-dimensional velocity field past a bioprosthetic heart valve was measured using tomographic particle image velocimetry. Two digital cameras were used together with a mirror setup to record PIV images from four different angles. Measurements were conducted in a transparent silicone phantom with a simplified geometry of the aortic root. The refraction indices of the silicone phantom and the working fluid were matched to minimize optical distortion from the flow field to the cameras. The silicone phantom of the aorta was integrated in a flow loop driven by a piston pump. Measurements were conducted for steady and pulsatile flow conditions. Results of the instantaneous, ensemble and phase-averaged flow field are presented. The three-dimensional velocity field reveals a flow topology, which can be related to features of the aortic valve prosthesis.
PubDate: 2016-05-03

• Bursting process of large- and small-scale structures in turbulent
boundary layer perturbed by a cylinder roughness element
• Abstract: Abstract Hot-wire measurements on a turbulent boundary layer flow perturbed by a wall-mounted cylinder roughness element (CRE) are carried out in this study. The cylindrical element protrudes into the logarithmic layer, which is similar to those employed in turbulent boundary layers by Ryan et al. (AIAA J 49:2210–2220, 2011. doi:10.2514/1.j051012) and Zheng and Longmire (J Fluid Mech 748:368–398, 2014. doi:10.1017/jfm.2014.185) and in turbulent channel flow by Pathikonda and Christensen (AIAA J 53:1–10, 2014. doi:10.2514/1.j053407). The similar effects on both the mean velocity and Reynolds stress are observed downstream of the CRE perturbation. The series of hot-wire data are decomposed into large- and small-scale fluctuations, and the characteristics of large- and small-scale bursting process are observed, by comparing the bursting duration, period and frequency between CRE-perturbed case and unperturbed case. It is indicated that the CRE perturbation performs the significant impact on the large- and small-scale structures, but within the different impact scenario. Moreover, the large-scale bursting process imposes a modulation on the bursting events of small-scale fluctuations and the overall trend of modulation is not essentially sensitive to the present CRE perturbation, even the modulation extent is modified. The conditionally averaging fluctuations are also plotted, which further confirms the robustness of the bursting modulation in the present experiments.
PubDate: 2016-05-03

• Velocity field measurements on high-frequency, supersonic microactuators
• Abstract: Abstract The resonance-enhanced microjet actuator which was developed at the Advanced Aero-Propulsion Laboratory at Florida State University is a fluidic-based device that produces pulsed, supersonic microjets by utilizing a number of microscale, flow-acoustic resonance phenomena. The microactuator used in this study consists of an underexpanded source jet that flows into a cylindrical cavity with a single, 1-mm-diameter exhaust orifice through which an unsteady, supersonic jet issues at a resonant frequency of 7 kHz. The flowfields of a 1-mm underexpanded free jet and the microactuator are studied in detail using high-magnification, phase-locked flow visualizations (microschlieren) and two-component particle image velocimetry. These are the first direct measurements of the velocity fields produced by such actuators. Comparisons are made between the flow visualizations and the velocity field measurements. The results clearly show that the microactuator produces pulsed, supersonic jets with velocities exceeding 400 m/s for roughly 60 % of their cycles. With high unsteady momentum output, this type of microactuator has potential in a range of ow control applications.
PubDate: 2016-04-30

• Infrared thermography for detection of laminar–turbulent transition
in low-speed wind tunnel testing
• Abstract: Abstract This work presents the details of a system for experimentally identifying laminar-to-turbulent transition using infrared thermography applied to large, metal models in low-speed wind tunnel tests. Key elements of the transition detection system include infrared cameras with sensitivity in the 7.5- to 14.0-µm spectral range and a thin, insulating coat for the model. The fidelity of the system was validated through experiments on two wind-turbine blade airfoil sections tested at Reynolds numbers between Re = 1.5 × 106 and 3 × 106. Results compare well with measurements from surface pressure distributions and stethoscope observations. However, the infrared-based system provides data over a much broader range of conditions and locations on the model. This paper chronicles the design, implementation and validation of the infrared transition detection system, a subject which has not been widely detailed in the literature to date.
PubDate: 2016-04-30

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