Calculation of the stationary zone of the reaction with the flame H2+O2 as an example

1970 ◽  
Vol 19 (6) ◽  
pp. 1190-1196
Author(s):  
L. A. Lovachev ◽  
V. Ya. Basevich ◽  
A. M. Kogan ◽  
V. S. Posvyanskii
Keyword(s):  
Stationary Zone

Experimental Investigation of the Effect of the Machine Kinematic Behavior on the Surface Topography and Roughness in High Speed Ball end Milling of the AISI4142 Steel

2021 ◽  
Author(s):  
Sai Lotfi ◽  
Belguith Rami ◽  
Baili Maher ◽  
Desseins Gilles ◽  
Bouzid Wassila
Keyword(s):  
Surface Topography ◽  
High Speed ◽  
End Milling ◽  
Experimental Investigations ◽  
Ball End Milling ◽  
Tool Paths ◽  
Stationary Zone ◽  
Machining Errors ◽  
Kinematic Behavior ◽  
Milling Tool

Abstract The analysis of the surface topography in ball end milling is an objective studied by many researchers, several methods were used and many combinations of cutting conditions and machining errors are considered. In the milling tool paths the trajectories presents a points of changing direction where the tool decelerates before and accelerates after respecting the velocity profiles of the machine. In this paper, we propose experimental investigations of the effect of the kinematic behavior of the machine tool on the surface quality. A poor topography and roughness are remarked on the deceleration and the acceleration zones compared to the stationary zone.

Image Analysis of Particle Flow in Centrifugal Solar Particle Receiver

2021 ◽  
Author(s):  
Serdar Hicdurmaz ◽  
Reiner Buck ◽  
Bernhard Hoffschmidt
Keyword(s):  
Image Processing ◽  
Image Analysis ◽  
Numerical Model ◽  
Film Thickness ◽  
Flow Characteristics ◽  
Particle Flow ◽  
Flow Rates ◽  
Solar Particle ◽  
Stationary Zone ◽  
Mass Flow Rates

Abstract Particle solar receivers promise economical and operational advantages compared to the molten salt based solar receivers. In this study, an experiment is designed to observe the particle flow characteristics in the Centrifugal Solar Particle Receiver. A set of experiments for various receiver rotation speeds and particle mass flow rates is conducted, and experimentally obtained raw results are post-processed by means of an Image Processing Routine based on 4BestEstimate algorithm[1]. The axial advance of the particles in 1 turn, the particle film thickness and the ratio of the stationary zone to the receiver circumference are measured in order to be later used in the validation study of the Discrete Element Method based numerical model.

scholarly journals XX. On the comparative morphology of the leaf the vascular cryptogams and gymnosperms

1884 ◽  
Vol 175 ◽  
pp. 565-615 ◽  
Keyword(s):  
Leaf Development ◽  
External Surface ◽  
Comparative Morphology ◽  
Young Leaf ◽  
Deciduous Trees ◽  
Essential Difference ◽  
Text Book ◽  
Stationary Zone ◽  
History Of ◽  
The Mind

The origin of the tendency among the earlier morphologists to draw a sharp distinction between stem and leaf may most probably be traced to the fact that vegetable morphology was first pursued as a science in regions where deciduous trees prevail. Seeing the leaves of so many plants fall off as a whole, while the scar left was almost a direct continuation of the external surface of the stem, doubtless gave rise to the view that the two should be regarded as radically distinct members. As the science of morphology progressed it became necessary, if this distinction were to be maintained, to define more clearly how members belonging to these two categories differ one from another. Various attempts were made by authors to show in what the essential difference consisted, the most notable being that of Hofmeister, who brought forward a number of distinctions, based chiefly upon development. The most essential of these were adopted in that section of the Text Book of Sachs, which deals with the relations of leaves and leaf-forming axes. In the last paragraph (No. 8) of that section, he clearly lays down the principle that “the expressions stem and leaf denote only certain relationships of the parts of a whole— the shoot .” This principle is elaborated in his more recent lectures, in which he writes as follows:— “A typical shoot consists of the leaves and the axis, which however are not really to be regarded as different organs, but fundamentally as parts only of one organ . . . . . In their nature, and as shown by the history of their development, the leaves are fundamentally nothing more than processes, or outgrowths of the axis of the shoot. . . . . ” If we accept these propositions, and I do not see how we can do otherwise, the same method of morphological treatment should be applied to the leaf as is usual in studying the stem. On reading current morphological papers, however, it is very apparent that this is not done. Leaving out of account the use of that adhesive terminology, which constantly revives in the mind the older mode of viewing the leaf, it is still obvious that the treatment of the leaf by modern writers is different from that of the stem. Thus, to take as an example the best of the earlier works on leaf-development, viz., Eichler’s Dissertation on the Development of the Leaf; after defining the Primordial Leaf as the young leaf before internal differentiation, or distinction of external parts, the author goes on to describe (p. 7) how the primordial leaf becomes differentiated into “ two chief parts, which are common to the leaves of all Phanerogams, viz., a stationary zone, which takes no part in the further formation of the leaf, and a vegetative part which forms the lamina with its branches.” The former he names the foliar base (blattgrund), and the products of its development are the sheath and the stipules if present; the latter he designates the upper leaf (oberblatt), which gives rise to the simple or branched lamina. The petiole is also, according to Eichler (p. 8), derived from the upper leaf, though other more recent writers describe it as being intercalated between the two parts. This distinction first drawn by Eichler has recently been revived, and the terminology, with some slight modifications, adopted by Goebel. He has however imposed a very necessary limitation upon its application, viz.: that the two parts of the primordial leaf “are not sharply marked off from one another, but are only to be distinguished by the part which they play in the further growth of the young leaf. ” He has, on the other hand, extended it to the Monocotyledons and Gymnosperms, and occasionally also to certain Cryptogams, in which similar phenomena appear. Thus the distinction of the foliar base and upper leaf has become established in botanical terminology, and it is applied equally to both branched and unbranched leaves.

A simple and conservative unstructured sliding-mesh approach for rotor–fuselage aerodynamic interaction simulation

2016 ◽  
Vol 231 (1) ◽  
pp. 163-179 ◽  
Author(s):  
He-Yong Xu ◽  
Shi-Long Xing ◽  
Zheng-Yin Ye ◽  
Ming-Sheng Ma
Keyword(s):  
Interaction Model ◽  
Side Surface ◽  
Computational Domain ◽  
Sliding Mesh ◽  
Sliding Interface ◽  
Stationary Zone ◽  
Aerodynamic Interaction ◽  
On Line ◽  
Interaction Simulation ◽  
Institute Of Technology

A conservative unstructured sliding-mesh technique is developed for the rotor–fuselage aerodynamic interaction simulation. The computational domain is decomposed into a rotational zone and a stationary zone. The rotational zone contains the rotor blades that rotate with the zone, while the stationary zone contains the fuselage which keeps stationary during the simulation. The two zones are connected via a sliding interface, which is designed to be a cylindrical surface consisting of the top, bottom, and side surfaces. The top and bottom surfaces are paved with arbitrary triangles and the side surface is meshed by triangularizing equal-sized and right-angled quadrilaterals. The intersection information between the rotational and stationary sliding interface meshes, such as the number of intersection triangles and the area of each intersection polygon, is the key to the present conservative computation. For the top and bottom surfaces, the point-on-line cases are first identified and the point perturbation operation is carried out to eliminate the potential error due to the presence of a point-on-line case. The neighbor-to-neighbor searching algorithm is applied for efficient determination of the intersection triangles, and the intersection polygon areas are determined by enumerating all the possible intersection cases. For the side surface, the intersection relations and polygon areas can be easily determined based on the enumeration method due to the special triangularization. The present method is validated by simulating the GIT (Georgia Institute of Technology) rotor–fuselage interaction model, and comparing numerical results with experiment measurements. It is demonstrated that the present conservative sliding-mesh method is simple to implement, and is efficient for the prediction of complicated unsteady rotor–fuselage aerodynamic interaction.

scholarly journals IMAGE ANALYSIS OF PARTICLE FLOW IN CENTRIFUGAL SOLAR PARTICLE RECEIVER

2022 ◽  
pp. 1-10
Author(s):  
Serdar Hicdurmaz ◽  
Reiner Buck ◽  
Bernhard Hoffschmidt
Keyword(s):  
Image Processing ◽  
Image Analysis ◽  
Numerical Model ◽  
Film Thickness ◽  
Flow Characteristics ◽  
Particle Flow ◽  
Flow Rates ◽  
Solar Particle ◽  
Stationary Zone ◽  
Mass Flow Rates

Abstract Particle solar receivers promise economical and operational advantages compared to the molten salt based solar receivers. In this study, an experiment is designed to observe the particle flow characteristics in the Centrifugal Solar Particle Receiver. A set of experiments for various receiver rotation speeds and particle mass flow rates is conducted, and experimentally obtained raw results are post-processed by means of an Image Processing Routine based on 4BestEstimate algorithm[1]. The axial advance of the particles in one turn, the particle film thickness and the ratio of the stationary zone to the receiver circumference are measured in order to be later used in the validation study of the Discrete Element Method based numerical model.

Width of the stationary zone in detonation waves

1970 ◽  
Vol 6 (1) ◽  
pp. 102-106 ◽  
Author(s):  
V. N. Zubarev ◽  
N. V. Panov ◽  
G. S. Telegin
Keyword(s):  
Detonation Waves ◽  
Stationary Zone
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