On the pressure magnitude at a spreading line

1993 ◽  
Vol 28 (2) ◽  
pp. 294-295
Author(s):  
G. I. Maikapar
2017 ◽  
Vol 63 (No. 7) ◽  
pp. 331-338
Author(s):  
Pecháček Jan ◽  
Vavříček Dušan ◽  
Kučera Aleš ◽  
Dundek Peter

The current revitalization of forest ecosystems in the Krušné Hory Mts. is carried out through: (i) spreading line windrows, (ii) chemical amelioration. The aim of this research consisted in: (i) assessing basic pedochemical characteristics of spread windrows, (ii) testing the effect of slow-release fertilizers from the Silvamix<sup>®</sup> series and dolomitic limestone on the root ball zone soil five years after application. The results of this study suggest that spread windrows are a suitable environment for forest species: with the only risk being extremely low P concentrations. Our results further show an increase in the amount of soil macrobioelements in the case of Silvamix<sup>®</sup> R and Silvamix<sup>®</sup> Forte, namely P over 125 and 85%; Mg<sup>2+</sup> over 84 and 108%; base saturation (BS) over 44 and 40.7%, respectively, compared with a control. Having applied dolomitic limestone, an increase of BS (by 88%), Mg<sup>2+</sup> (by 250%) and Ca<sup>2+</sup> (by 37%) was observed; there was a reduction in the level of mobile Al<sup>3+</sup> (by 25%) compared with the control. Stromfolixyl<sup>®</sup> application did not affect the chemistry of the soil environment.


Author(s):  
Wei Wang ◽  
Gang Li ◽  
Yong Huang

Cell damage due to the mechanical impact during laser-assisted cell direct writing has been observed and is a possible hurdle for broad applications of fragile cell direct writing. The objective of this study is to numerically investigate the bubble expansion-induced cell mechanical loading profile in laser-assisted cell direct writing. Some conclusions have been drawn as follows. The cell velocity increases initially and then smoothes out gradually with a constant ejection velocity. Both the cell acceleration and pressure can be very high at the beginning period of bubble expansion and then quickly approach zero in an oscillation manner. A high viscosity can lead to an observable velocity increment at the initial stage, but the ejection velocity decreases. The pressure magnitude decreases when the cell-bubble distance is large, and a larger initial pressure induces a larger cell pressure as expected. This study serves as a foundation to further investigate the cell damage mechanism in laser-assisted cell direct writing to improve the effectiveness and efficiency of cell direct writing techniques.


1971 ◽  
Vol 51 (5) ◽  
pp. 367-370
Author(s):  
D. H. HEINRICHS

Creeping-rooted alfalfa plants were studied for rate of spreading when planted in a grid spacing of 1.8 m. One year after planting, only three out of 15 lines displayed 100% creep in all five replicates on the basis of shoot formation. In the second year, all clones of all 15 plant lines had developed above-ground shoots. The range of spread varied from an average of 101 cm for the least spreading line to 176 cm for the strongest spreading line. By the third year they had expanded an additional 27% on the average. The stand density decreased as distance from the center of the plant increased. There were definite differences among creeping-rooted plant lines in rate of spreading ability. In three years most plants had spread horizontally to within each other’s peripheries.


Author(s):  
Michael W. Sracic ◽  
Jordan D. Petrie ◽  
Henry A. Moroder ◽  
Ryan T. Koniecko ◽  
Andrew R. Abramczyk ◽  
...  

Acoustic levitation is an advantageous particle positioning mechanism currently employed for applications of x-ray spectroscopy and micro-material manufacturing[1], [2]. By levitating a particle using only acoustic pressure waves, one eliminates the need for a container or other physical structure which may contaminate the specimen. Unfortunately, the pressure field generated by a standing acoustic wave is susceptible to periodic instabilities, and a particle that is levitated in this field tends to vibrate. The amplitude of the vibration is largest in the directions that are orthogonal to the axis in which the acoustic wave is generated. Therefore, by generating additional acoustic waves in each orthogonal axis, the vibration amplitude of the levitated particle is significantly reduced. The authors have shown this phenomenon to be true in a previous study[3]. In this paper, the authors explore the details of the pressure field that is generated with the device. A single degree-of-freedom relationship is developed between the acoustic field pressure, the location of the levitated particle, and the mechanical vibration needed to produce levitation. In order to levitate a 100 micrometer diameter water droplet at 55 kilohertz, the calculations suggest that the transducer must achieve an average surface vibration amplitude of at least 6.43 micrometers. This mechanical vibration must produce a root means-squared pressure amplitude of 933 Pascal. Under these conditions, the particle will levitate approximately 0.4 millimeters below a zero pressure node. To validate the use of the single degree of freedom relationships and to explore the acoustic field for one, two, and three-axis levitation, the authors designed and prototyped an acoustic levitator capable of generating standing waves in three orthogonal directions. Using a simple electrical control circuit, the acoustic wave transducers of each axis can be turned on individually or simultaneously. An experiment was developed to measure the pressure of the acoustic field using a microphone. Preliminary pressure magnitude results were measured for one-axis levitation along the center of the vertical axis of the levitator. The measurements suggest that the theoretical development provides a valid first approximation for the pressure magnitude and required mechanical vibration amplitude.


2018 ◽  
Vol 24 (C) ◽  
pp. 118
Author(s):  
Julio A. Lara-Hernández ◽  
Isabella Tan ◽  
Mark Butlin ◽  
Alberto P. Avolio

2017 ◽  
Vol 141 (1) ◽  
pp. 499-514 ◽  
Author(s):  
Douglas H. Keefe ◽  
M. Patrick Feeney ◽  
Lisa L. Hunter ◽  
Denis F. Fitzpatrick

1986 ◽  
Vol 49 (2) ◽  
pp. 102-111 ◽  
Author(s):  
Ted Catchpole ◽  
Neville de Mestre

2014 ◽  
Vol 104 (6) ◽  
pp. 622-632 ◽  
Author(s):  
Jolanta Pauk ◽  
Mikhail Ihnatouski ◽  
Bijan Najafi

Background Flatfoot, or pes planus, is one of the most common foot posture problems in children that may lead to lower-extremity pain owing to a potential increase in plantar pressure. First, we compared plantar pressure distribution between children with and without flatfoot. Second, we examined the reliability and accuracy of a simple metric for characterization of foot posture: the Clarke angle. Third, we proposed a mathematical model to predict plantar pressure magnitude under the medial arch using body mass and the Clarke angle. Methods Sixty children with flatfoot and 33 aged-matched controls were recruited. Measurements included in-shoe plantar pressure distribution, ground reaction force, Clarke angle, and radiography assessment. The measured Clarke angle was compared with radiographic measurements, and its test-retest reliability was determined. A mathematical model was fitted to predict plantar pressure distribution under the medial arch using easy-to-measure variables (body mass and the Clarke angle). Results A high correlation was observed between the Clarke angle and radiography measurements (r &gt; 0.9; P &lt; 10−6). Excellent between- and within-day test-retest reliability for Clarke angle measurement (intraclass correlation coefficient, &gt;0.9) was observed. Results also suggest that pressure magnitude under the medial arch can be estimated using the Clarke angle and body mass (R2 = 0.95; error, &lt;0.04 N/cm2 [2%]). Conclusions This study suggests that the Clarke angle is a practical, reliable, and sensitive metric for quantification of medial arch height in children and could be recommended for research and clinical applications. It can also be used to estimate plantar pressure under the medial arch, which, in turn, may assist in the timely intervention and prognosis of prospective problems associated with flatfoot posture.


2012 ◽  
Vol 23 (11) ◽  
pp. 2773-2781 ◽  
Author(s):  
Jae Young Jeong ◽  
So Hee Park ◽  
Ji Won Shin ◽  
Yun Gyeong Kang ◽  
Ki-Ho Han ◽  
...  

Author(s):  
H. M. Atassi ◽  
J. Fang ◽  
P. Ferrand

The rise of the unsteady pressure magnitude along the surface of a cascade blade in unsteady transonic flow is examined. It is shown that a similar rise in the unsteady pressure may occur for high subsonic flows where the mean flow is near sonic condition. For a subsonic cascade this unsteady pressure bulge is found to be associated with the cut-on of a new acoustic mode in the upstream direction. The level of the pressure bulge is significantly reduced as a downstream propagating mode cuts on. It is therefore proposed that this phenomenon is the result of the blockage of upstream propagating acoustic waves by the transonic mean flow. A transonic convergent-divergent nozzle is used as a model for investigating the acoustic blockage effect. Analytical and numerical computations using unsteady nonlinear Euler equations are then carried out to analyze and quantify the upstream and dowstream propagation of acoustic disturbances in the nozzle. The results confirm the sharp rise in the pressure of the upstream propagating disturbances at the nozzle throat as a result of the acoustic blockage.


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