Obtaining of Four-Dimensional Nomograms Based on Similarity Theorem

2017 ◽  
Vol 5 (2) ◽  
pp. 69-74 ◽  
Author(s):  
Левкин ◽  
Yu. Levkin

In some performed experimental works there is no total characteristic of study processes with regard to their physical understanding. It’s possible to achieve such understanding by means of epure and graphic interdependency for parameters illustrating experiment process, and by means of geometrical images which testify regularity of their outline, and are characteristic of physical process. The use of epure multidimensional octant nomogram can promote the solution for a number of application-oriented problems. By means of two octant epure nomograms constructed on experimental tabular data with four or five parameters, the optimum choice of graphic execution and its implementation in the area of physical genesis is offered. This method’s justifications have been given in the paper. A basis for extension of new opportunities is certainly descriptive geometry that facilitates a solution to technical tasks on multidimensional geometry. At the heart of similarity of adjacent octant cells with general axis are plotted two octant axonometric nomograms creating interdependencies between parameters by means of communication lines. This method opens a possibility for physical processes’ nature understanding. In this paper have been presented two graphic models for two octant nomograms in which advantages of their creation and reading have been presented. Foundations on which derivations are built when constructing the nomograms are validated by the similarity theorem and the axiom of projected surface. Absolute values of parameters are actual ones, and presented from papers of journals, as well as from peer-reviewed scientific publications recommended by Higher Attestation Commission.

2017 ◽  
Vol 5 (4) ◽  
pp. 44-51 ◽  
Author(s):  
Ю. Левкин ◽  
Yu. Levkin

Multidimensional experimental tasks with interdependent physical quantities can't be characterized by use of flat two-dimensional plots. Nomograms of new type solve such tasks. In this paper have been presented the nomograms with systematized both axes and planes. At construction of such models it is required a clear separation of all parametrial variable on arguing and functional ones. Nearby axes of interdependent parameters should lie alongside. Each axonometric cell should have a resultant indicator in the form of full size’s geometrical image. For the optimum choice of graphic execution on tabular data with four or five parameters, in the present paper is offered a method of its realization by means of two-oktantal nomogram. Justifications for this method have been presented in the paper. The method itself is based on descriptive geometry’s opportunities expansion at the solution of technical tasks by means of multidimensional geometry. The main lever for the task implementation is, certainly, communication lines. Formerly known from descriptive geometry such concepts as plane of reference, horizontally projecting surface, on the one hand, and pointed measurement of all experimental parameters on the other hand, provides to the nomogram possibility of its understanding for genesis in physical processes. Based on similarity of adjacent oktantal cells having the general axis are plotting two oktantal axonometric nomograms, creating interdependence between parameters by means of communication lines. This method opens a possibility for understanding of physical processes transformation. In this paper have been presented two graphic models of two oktantal nomograms competing for the right to be used by force of theirs optimal advantages. Absolute values of parameters are the real ones, taken from papers in "News of Higher Educational Institutions. North Caucasus Region" journal. Technical Sciences. No. 3, pp. 77–83, and No. 2, pp. 112–119. 2016.


1974 ◽  
Vol 14 (01) ◽  
pp. 25-34 ◽  
Author(s):  
D.N. Sawyer ◽  
W.M. Cobb ◽  
F.I. Stalkup ◽  
P.H. Braun

Abstract This paper illustrates the application of a statistical experimental design technique (factorial design) to the study of a computer model of a physical process (the wet-combustion drive). physical process (the wet-combustion drive). Factorial design has been used successfully for many years in experimental work to allow investigators to study systematically and efficiently the interactions of important variables and their effects on physical processes. It can also be applied to great advantage processes. It can also be applied to great advantage to computer models of physical processes. The mathematical model in this illustration was programmed to simulate the wet-combustion process programmed to simulate the wet-combustion process in a previously waterflooded confined five-spot. The model couples basic energy and mass balance equations to approximate heat and fluid-flow phenomena. Application of the factorial design phenomena. Application of the factorial design technique to this computer model has allowed us to study individually and collectively, in a relatively short time, the effects that nine important variables exert on the economics of this process. These nine variables are measures of time, reservoir pressure, heat loss, oil burned as fuel, waterflooded residual oil, steam front sweep, oil bank sweep, air co st, and oil price. The final result is a simple equation containing these variables that can be used by the reservoir analyst quickly to screen reservoirs as candidates for the wet-combustion process and perform a sensitivity analysis to determine how perform a sensitivity analysis to determine how uncertainties in the variables will affect the economics. Introduction Since it is extremely difficult, if not impossible in most cases, to simulate reservoir performance in the laboratory, the oil production industry has been in the forefront of developing mathematical models of various recovery processes. As the models become more sophisticated, the computer run time per case -- and hence the cost of simulation - increases rapidly. Since it is desirable to minimize the number of computer runs, we very seldom simulate every field or make a completely general study of how the variables in our computer model (and their interactions) affect the process. The prohibitive cost of screening all fields with the computer simulator and then performing a complete sensitivity analysis involving a large number of variables often forces us to arbitrarily limit the scope of our study. For example we might first screen reservoirs by limiting our simulator runs tothose two or three fields in which we own the largest working interestthose that constitute our major sources of production, andthose that will very soon be production, andthose that will very soon be depleted by primary recovery or by waterflooding. The simulation is for the best-estimate set of conditions for each field. After picking the best prospects, we may run a sensitivity analysis, prospects, we may run a sensitivity analysis, possibly by choosing a few of the variables possibly by choosing a few of the variables considered to be most important and changing them, one variable at a time, about the best-estimate conditions. Factorial design is a statistical technique developed m assist experimentalists in dealing with some of the same problems faced by the users of reservoir simulators - namely, how to study systematically and efficiently the effects of a large number of variables on a complicated process and how to reduce the results to a reasonably simplified form. To our knowledge, factorial design has been used little, if at all, in reservoir analysis. We believe it can be valuable in reservoir simulation to obtain a simplified equation that can be used to screen reservoirs rapidly and to perform sensitivity analysis. The concepts and applications of factorial design and its variations, along with details of the calculations, are found in abundance in the literature and thus will not be presented in great detail here. Refs. 1 and 2 are particularly recommended for details on calculations Ref. 3 through 7 are recommended as practical examples of the use of the technique and as general reviews of As application. Likewise, the concepts of the wet-combustion process are well discussed in the literature. Details of our particular mathematical model (computer simulator) of the wet-combustion process can be found in Appendix A. In particular, process can be found in Appendix A. In particular, we will discuss only those details of factorial design and of the computer model that point out major advantages and major limitations of each. SPEJ P. 25


2020 ◽  
Vol 8 (6) ◽  
Author(s):  
Saeed Shahsavari ◽  
Mehran Moradi

When a physical process is performed, identifying the generated entropy can be used to investigate the irreversibility. But for this mean, from the perspective of the Boltzmann equation, both all microstates and macrostates must be studied. In fact, it is needed that all particles energy level to be investigated. Therefore, to investigate entropy in configurationally systems using the Boltzmann equation, a very large volume of calculations is required. In this study, we try to extract a way to investigate entropy production without the need to study all particles (or sub-structures). For this purpose, at first, a macroscopic energy structure equation “as an equation that shows the energy components of the system activated in the performed process as well as their dependence” is presented. As a study on the irreversibility (or entropy production) in physical systems, its structure and components are studied. Writing equations in the energy space of the system makes it possible to study the structure of irreversibility. Then using a new macroscopic quasi-statistical approach, the irreversibility and its structure in physical processes are investigated. Macro energy components of the system are used for this investigation and energy structure is studied base on them. Finally, a new macroscopic definition of the generated entropy is extracted using a new energy structure equation as well as dependent and independent macroscopic energy component concepts. Also, why and what entropy can be generated, from the perspective of the presented macroscopic energy structure equation are studied. In fact, this paper investigates the generated entropy structure in physical systems using macroscopic system energy components and takes a new approach to why and what irreversibility is occurred during the physical process. Therefore, presented equations can be used for investigating the irreversibility in configurationally physical systems without the need to study all its sub structures. Also, from the extracted equations, it can be concluded that entropy is generated because of the existence of the dependent energy components in the energy structure equation of the system, and this generated entropy depends on the variation of these components as well as the amount of the applied energy to the system and its conditions. Due to the kinematic theory of dissipated energy, these results are in the same line with the different formulations of the second law of thermodynamics.  


Akustika ◽  
2019 ◽  
Vol 32 ◽  
pp. 17-23
Author(s):  
Mikhail Fesina ◽  
Igor Deryabin ◽  
Gorina Larisa

This paper gives the results of experimental researches for producing physical processes of acoustic vibration beats, which are spread in a free and in a diffused field of enclosed air volumes in technical rooms of different types. There are defined general regularities and distinct features of forming the physical processes of acoustic vibration beats. A limited frequency range of beats production which includes two different frequency ranges of dynamic frequency interactions with close values of sound frequencies are found out. Sufficiency of frequency detuning of two independent sources of acoustic radiation which exclude physical process creation of sound frequency beats is defined.


2016 ◽  
Vol 5 (3) ◽  
pp. 179-183
Author(s):  
Dmitry Vladislavovich Popov

The article presents the research results of the formation model of students' professional experimental and research competences during performance of laboratory and experimental works. It explains the problem and solution of professional training of specialists in physical processes of oil and gas industry. It shows the meaning of laboratory and experimental works in competence paradigm of specialists in physical processes of oil and gas industry. Here author represents such concept as professional experimental and research competence and defines its functionality and content components. It points out the formation model of students' professional experimental and research competences during performance of laboratory and experimental works which is an algorithm and system navigator for developers and users of similar systems. The author notes descriptors of functionality and content components which use such as criterion of the formation level of students' professional experimental and research competence. The article points out the structure and content of the information and didactic basis based on the laboratory works complex in physical processes of oil and gas industry. The article represents the results of ascertaining and forming experiment. It determines the initial and final equation of formation in experimental and control groups. It shows the feasibility and effectiveness of using high innovative competence modular technology of laboratory and experimental works.


2019 ◽  
Vol 9 (22) ◽  
pp. 4732 ◽  
Author(s):  
Zhengguo Yang ◽  
Yuto Lim ◽  
Yasuo Tan

Accident models provide a conceptual representation of accident causation. They have been applied to environments that have been exposed to poisonous or dangerous substances that are hazardous in nature. The home environment refers to the indoor space with respect to the physical processes the of indoor climate, e.g., temperature change, which are not hazardous in general. However, it can be hazardous when the physical process is in some states, e.g., a state of temperature that can cause heat stroke. If directly applying accident models in such a case, the physical processes are missing. To overcome this problem, this paper proposes an accident model by extending the state-of-the-art accident model, i.e., Systems-Theoretic Accident Model and Process (STAMP) with considering physical processes. Then, to identify causes of abnormal system behaviors that result in physical process anomalies, a hazard analysis technique called System-Theoretic Process Analysis (STPA) is tailored and applied to a smart home system for indoor temperature adjustment. The analytical results are documented by a proposed landscape genealogical layout documentation. A comparison with results by applying the original STPA was made, which demonstrates the effectiveness of the tailored STPA to apply in identifying causes in our case.


2005 ◽  
Vol 44 (2) ◽  
pp. 241-255 ◽  
Author(s):  
Gyu Won Lee ◽  
Isztar Zawadzki

Abstract A systematic and intensive analysis is performed on 5 yr of reliable disdrometric data (over 20 000 one-minute drop size distributions, DSDs) to investigate the variability of DSDs in the Montreal, Quebec, Canada, area. The scale dependence (climatological scale, day to day, within a day, between physical processes, and within a physical process) of the DSD variability and its effect on rainfall intensity R estimation from radar reflectivity Z are explored in terms of bias and random errors. Detail error distributions are also provided. The use of a climatological R–Z relationship for rainfall—affected by all of the DSDs’ variability—leads on average to a random error of 41% in instantaneous rain-rate estimation. This error decreases with integration time, but the decrease becomes less pronounced for integration times longer than 2 h. Daily accumulations computed with the climatological R–Z relationship have a bias of 28% because of the day-to-day DSD variability. However, when daily R–Z relationships are used, a random error of 32% in instantaneous rain rate is still present because of the DSD variability within a day. This illustrates that most of the variability of DSDs has its origin within a storm or between storms within a day. Physical processes leading to the formation of DSDs are then classified according to the vertical structure of radar data as measured by a UHF profiler collocated with the disdrometer. The DSD variability among different physical processes is larger than the day-to-day variability. A bias of 41% in rain accumulations is due to the DSD variability between physical processes. Accurate rain-rate estimation (∼7%) can be achieved only after the proper underlying physical process is identified and the associated R–Z relationship is used.


1979 ◽  
Vol 44 ◽  
pp. 349-355
Author(s):  
R.W. Milkey

The focus of discussion in Working Group 3 was on the Thermodynamic Properties as determined spectroscopically, including the observational techniques and the theoretical modeling of physical processes responsible for the emission spectrum. Recent advances in observational techniques and theoretical concepts make this discussion particularly timely. It is wise to remember that the determination of thermodynamic parameters is not an end in itself and that these are interesting chiefly for what they can tell us about the energetics and mass transport in prominences.


Author(s):  
A. Baronnet ◽  
M. Amouric

The origin of mica polytypes has long been a challenging problem for crystal- lographers, mineralogists and petrologists. From the petrological point of view, interest in this field arose from the potential use of layer stacking data to furnish further informations about equilibrium and/or kinetic conditions prevailing during the crystallization of the widespread mica-bearing rocks. From the compilation of previous experimental works dealing with the occurrence domains of the various mica "polymorphs" (1Mr, 1M, 2M1, 2M2 and 3T) within water-pressure vs temperature fields, it became clear that most of these modifications should be considered as metastable for a fixed mica species. Furthermore, the natural occurrence of long-period (or complex) polytypes could not be accounted for by phase considerations. This highlighted the need of a more detailed kinetic approach of the problem and, in particular, of the role growth mechanisms of basal faces could play in this crystallographic phenomenon.


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