Receptivity of Crossflow Instabilities to a Periodic Roughness Array on a Swept Cylinder: Investigation of the Roughness Size Influence

2008 ◽  
Author(s):  
Estelle Piot ◽  
Cedric Content ◽  
Gregoire Casalis
Keyword(s):  
Roughness Size

scholarly journals A Low-Cost, Non-hazardous Protocol for Surface Texturing of Glass Particles

2019 ◽  
Vol 67 (4) ◽  
Author(s):  
Anelechi Ibekwe ◽  
Yukie Tanino ◽  
Dubravka Pokrajac
Keyword(s):  
Low Cost ◽  
Packed Column ◽  
Surface Texturing ◽  
Nanometer Scale ◽  
Length Scale ◽  
Glass Spheres ◽  
Hard Particles ◽  
Microscope Images ◽  
Scanning Electron ◽  
Roughness Size

Abstract We present a cheap, efficient, and non-hazardous protocol for altering the roughness of hard particles at the nanometer-scale using a stone tumbler, a tool which is normally used for polishing stones. Six different textures were achieved by lining the tumbler with sandpaper of mean grit diameters $$d_{\mathrm{g}}=201$$dg=201, 58.5, 18.3, 12.6, and $$8.4\,\upmu \hbox {m}$$8.4μm. Two textures were created by tumbling a batch of glass spheres for 4 h and for 12 h with the $$12.6\,\upmu \hbox {m}$$12.6μm sandpaper; all other textures were established by tumbling for 12 h. Surface roughness was characterized by the integral length scale, $$\xi$$ξ, evaluated from 7 nm/pix resolution scanning electron microscope images. Roughness size increased from $$\xi = 24$$ξ=24 to 31 nm as the grit size decreased from $$d_{\mathrm{g}} = 201$$dg=201 to $$18.3\,\upmu \hbox {m}$$18.3μm, and then decreased to $$\xi = 6.4\,\hbox {nm}$$ξ=6.4nm at the smallest $$d_{\mathrm{g}}$$dg. The largest $$\xi \,(= 34\,\hbox {nm})$$ξ(=34nm) was achieved using a $$12.6\,\upmu \hbox {m}$$12.6μm sandpaper and the shorter tumbling time of 4 h. The permeability of a packed column of the particles broadly decreased with increasing $$\xi$$ξ, indicating that permeability decreases with increasing roughness size.

The Limitations of Using “Ra” to Describe Surface Roughness

2016 ◽  
Vol 138 (10) ◽  
Author(s):  
Martin N. Goodhand ◽  
Karl Walton ◽  
Liam Blunt ◽  
Hang W. Lung ◽  
Robert J. Miller ◽  
...  
Keyword(s):  
Surface Roughness ◽  
Reynolds Number ◽  
Skin Friction ◽  
Rough Surfaces ◽  
Leading Edge ◽  
Amplitude Parameter ◽  
Roughness Amplitude ◽  
The Relationship ◽  
Roughness Size

Current criteria used to determine whether rough surfaces affect skin friction typically rely on a single amplitude parameter to characterize the roughness. The most commonly used criteria relate the centerline averaged roughness, Ra, to an equivalent sandgrain roughness size, ks. This paper shows that such criteria are oversimplified and that Ra/ks is dependent on the roughness topography, namely, the roughness slope defined as the roughness amplitude normalized by the distance between roughness peaks, Ra/λ. To demonstrate the relationship, wake traverses were undertaken downstream of an aerofoil with various polished surfaces. The admissible roughness Reynolds number (ρ1u1Ra/μ1) at which the drag rose above the smooth blade case was determined. The results were used to demonstrate a 400% variation in Ra/ks over the roughness topographies tested. The relationship found held for all cases tested, except those where the roughness first initiated premature transition at the leading edge. In these cases, where the roughness was more typical of eroded aerofoils, the drag was found to rise earlier.

Tensiometric studies on wetting. I. Some effects of surface roughness (theoretical)

1981 ◽  
Vol 59 (13) ◽  
pp. 1954-1961 ◽  
Author(s):  
Erdal Bayramli ◽  
Theodore G. M. van de Ven ◽  
Stanley G. Mason
Keyword(s):  
Surface Roughness ◽  
Contact Angle ◽  
Contact Angle Hysteresis ◽  
Solid Surfaces ◽  
Surface Slopes ◽  
Receding Contact ◽  
Receding Contact Angle ◽  
Wetting Hysteresis ◽  
Non Equilibrium ◽  
Roughness Size

The effect of roughness on the wettability of an axisymmetric cylinder is investigated theoretically by making use of equilibrium meniscus shapes on solid surfaces analogously to previous studies for drops on horizontal surfaces. Employing circumferential sinusoidal and saw-toothed grooved structure, and using mechanistic arguments, one can explain wetting hysteresis, the formation of composite surfaces, and the presence of non-equilibrium jumps during contact line motion.On unidirectionally random surfaces the maximum surface slopes mainly determine the value of the advancing, and the minimum slopes of the receding contact angle. These effects of surface slopes diminish with decreasing roughness size. Diminishing roughness size also gives rise to numerous small non-equilibrium jumps imposed upon larger jumps during wetting. The contact angle hysteresis is found to show a nearly linear relationship with the spread in the distribution of solid surface slopes.

scholarly journals Characteristics of Trees Infested by the Invasive Primary Wood-Borer Aromia bungii (Coleoptera: Cerambycidae)

Insects ◽  
2022 ◽  
Vol 13 (1) ◽  
pp. 54
Author(s):  
Yuichi Yamamoto ◽  
Yosuke Ishikawa ◽  
Kazuhiko Uehara
Keyword(s):  
Mixed Models ◽  
Tree Damage ◽  
Explanatory Variables ◽  
Damage Response ◽  
Rosaceae Family ◽  
The Difference ◽  
Wood Borer ◽  
Future Work ◽  
Tree Characteristics ◽  
Roughness Size

The expanding distribution and tree damage of the invasive, primary wood-borer Aromia bungii (Coleoptera: Cerambycidae), which kills trees of the Rosaceae family, is a problem in intruded areas. However, the tree characteristics associated with infestation by A. bungii, which are useful for early detection or prioritizing preventive measures, are not well examined. We investigated the presence or absence of tree damage (response variable) in pre- and post- surveys along with tree characteristics (four explanatory variables; bark roughness, size, species, and vigor) on monitoring trees in uninvaded sites (survey for the first trees to be damaged) and already invaded sites (survey for the next trees to be damaged). We evaluated the variables using generalized linear mixed models for each site (i.e., a first trees model and a next trees model). Three tree characteristics (bark roughness, size, and vigor) were included as explanatory variables in both best models, indicating that trees with rough surface bark, large in size, and weakened conditions were more susceptible to A. bungii infestation. The reasons for the difference between the two models (species was only chosen in the next trees model) will be considered in our future work.

scholarly journals Stability and sensitivity of a cross-flow-dominated Falkner–Skan–Cooke boundary layer with discrete surface roughness

2017 ◽  
Vol 826 ◽  
pp. 830-850 ◽  
Author(s):  
Mattias Brynjell-Rahkola ◽  
Nima Shahriari ◽  
Philipp Schlatter ◽  
Ardeshir Hanifi ◽  
Dan S. Henningson
Keyword(s):  
Boundary Layer ◽  
Sensitivity Analysis ◽  
Surface Roughness ◽  
Energy Transport ◽  
Three Dimensional ◽  
Cross Flow ◽  
Domain Size ◽  
Great Sensitivity ◽  
Discrete Surface ◽  
Roughness Size

With the motivation of determining the critical roughness size, a global stability and sensitivity analysis of a three-dimensional Falkner–Skan–Cooke (FSC) boundary layer with a cylindrical surface roughness is performed. The roughness size is chosen such that breakdown to turbulence is initiated by a global version of traditional secondary instabilities of the cross-flow (CF) vortices instead of an immediate flow tripping at the roughness. The resulting global eigenvalue spectra of the systems are found to be very sensitive to numerical parameters and domain size. This sensitivity to numerical parameters is quantified using the $\unicode[STIX]{x1D700}$-pseudospectrum, and the dependency on the domain is analysed through an impulse response, structural sensitivity analysis and an energy budget. It is shown that while the frequencies remain relatively unchanged, the growth rates increase with domain size, which originates from the inclusion of stronger CF vortices in the baseflow. This is reflected in a change in the rate of advective energy transport by the baseflow. It is concluded that the onset of global instability in a FSC boundary layer as the roughness height is increased does not correspond to an immediate flow tripping behind the roughness, but occurs for lower roughness heights if sufficiently long domains are considered. However, the great sensitivity results in an inability to accurately pinpoint the exact parameter values for the bifurcation, and the large spatial growth of the disturbances in the long domains eventually becomes larger than can be resolved using finite-precision arithmetic.

Fine-Tuning of Superhydrophobicity Based on Monolayers of Well-defined Raspberry Nanoparticles with Variable Dual-roughness Size and Ratio

2014 ◽  
Vol 24 (36) ◽  
pp. 5745-5752 ◽  
Author(s):  
Camille C. M. C. Carcouët ◽  
A. Catarina C. Esteves ◽  
Marco M. R. M. Hendrix ◽  
Rolf A. T. M. van Benthem ◽  
Gijsbertus de With
Keyword(s):  
Fine Tuning ◽  
Roughness Size

scholarly journals Leading-Edge Roughness Affecting Diamond-Wing Aerodynamic Characteristics

Aerospace ◽  
2018 ◽  
Vol 5 (3) ◽  
pp. 98 ◽  
Author(s):  
Andrei Buzica ◽  
Lisa Debschütz ◽  
Florian Knoth ◽  
Christian Breitsamter
Keyword(s):  
Reynolds Number ◽  
Surface Pressure ◽  
Angle Of Attack ◽  
Leading Edge ◽  
Aerodynamic Characteristics ◽  
Aerodynamic Coefficients ◽  
Number Range ◽  
Edge Roughness ◽  
Vortex Separation ◽  
Roughness Size

Diamond wing configurations for low signature vehicles have been studied in recent years. Yet, despite numerous research on highly swept, sharp edged wings, little research on aerodynamics of semi-slender wings with blunt leading-edges exists. This paper reports on the stall characteristics of the AVT-183 diamond wing configuration with variation of leading-edge roughness size and Reynolds number. Wind tunnel testing applying force and surface pressure measurements are conducted and the results presented and analysed. For the investigated Reynolds number range of 2.1 × 10 6 ≤ R e ≤ 2.7 × 10 6 there is no significant influence on the aerodynamic coefficients. However, leading-edge roughness height influences the vortex separation location. Trip dots produced the most downstream located vortex separation onset. Increasing the roughness size shifts the separation onset upstream. Prior to stall, global aerodynamic coefficients are little influenced by leading-edge roughness. In contrast, maximum lift and maximum angle of attack is reduced with increasing disturbance height. Surface pressure fluctuations show dominant broadband frequency peaks, distinctive for moderate sweep vortex breakdown. The experimental work presented here provides insights into the aerodynamic characteristics of diamond wings in a wide parameter space including a relevant angle of attack range up to post-stall.

The Limitations of “Ra” to Describe Surface Roughness

2015 ◽  
Author(s):  
Martin N. Goodhand ◽  
Karl Walton ◽  
Liam Blunt ◽  
Hang W. Lung ◽  
Robert J. Miller ◽  
...  
Keyword(s):  
Surface Roughness ◽  
Reynolds Number ◽  
Skin Friction ◽  
Rough Surfaces ◽  
Leading Edge ◽  
Amplitude Parameter ◽  
Roughness Amplitude ◽  
The Relationship ◽  
Roughness Size

Current criteria used to determine whether rough surfaces affect skin friction typically rely on a single amplitude parameter to characterize the roughness. The most commonly used criteria relate the centreline averaged roughness, Ra, to an equivalent sandgrain roughness size, ks. This paper shows that such criteria are oversimplified and that Ra/ks is dependent on the roughness topography, namely the roughness slope defined as the roughness amplitude normalized by the distance between roughness peaks, Ra/λ. To demonstrate the relationship, wake traverses were undertaken downstream of an aerofoil with various polished surfaces. The admissible roughness Reynolds number (ρ1u1Ra/μ1) at which the drag rose above the smooth blade case, was determined. The results were used to demonstrate a 400% variation in Ra/ks over the roughness topographies tested. The relationship found held for all cases tested, except those where the roughness first initiated premature transition at the leading edge. In these cases, where the roughness was more typical of eroded aerofoils, the drag was found to rise earlier.

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