An asymptotic flow region refers to a part of a fluid flow where the behavior of the flow field approaches a predictable pattern as one moves away from a specific region or boundary. In this region, the effects of viscosity and other near-wall phenomena become negligible, allowing for simplified analysis, often characterized by inviscid or potential flow assumptions. This concept is commonly used in fluid dynamics to analyze flows around objects or in various engineering applications where the influence of boundaries diminishes at a distance.
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In a Geiger-Müller (GM) tube, there is a central anode and a "case" that is the cathode. A voltage is applied across these two elements, and an ionizing particle passing through the GM tube will cause current flow. But how much? Let's step through things and check it out. At low voltage, any electrons released by the cathode will eventually be collected by the anode, but there is no appreciable "current" per se in this, the ionization region. Things are still pretty "tame" in the GM tube through this range of voltages. By applying more voltage, an ionizing event will generate more current flow, and this current flow will be proportional to the voltage in what is (naturally) the proportional region. And as we apply more voltage, gas amplification, or Townsend avalanche, which appeared at the beginning of this region, is increasing across the area of the anode. As we apply even more voltage, it will only make for limited additional current flow in an ionizing event because the limits of the geometry of the GM tube and of the gas media to ionize and "conduct more" with the increasing voltage are being reached. This is the limited-proportional region. As voltage is increased even more, we enter the Geiger-Müller region. In this region, the current avalanche in an ionizing event is so great that is causes a "shield" of positive ions around the anode. The high current "sucks up" all the electrons and blankets the anode in a positive field that prevents additional current flow even with an increase in voltage. This is the Geiger plateau. It's the operating region where additional differential voltage will not cause higher current flow in an ionizing event.
A reverse-biased diode is typically operated in the reverse breakdown region of its current-voltage characteristic curve. In this region, the diode allows a small reverse current to flow, which is generally negligible until a certain breakdown voltage is reached. Beyond this breakdown voltage, the diode can conduct significant current, but in normal applications, it operates below this threshold to prevent damage. Thus, the diode primarily remains in the reverse bias region with minimal current flow.
Recombination in a diode is crucial because it facilitates the movement of charge carriers, enabling the diode to function effectively as a rectifier. In a p-n junction diode, when electrons from the n-type region recombine with holes in the p-type region, it creates a depletion region that allows current to flow in one direction while blocking it in the opposite direction. This process helps establish the diode's characteristic I-V curve, which is essential for controlling electrical current in circuits. Without recombination, the diode would not be able to regulate current flow properly.
A PN diode is a semiconductor device that allows current to flow primarily in one direction. It consists of a p-type region (with positive charge carriers, or holes) and an n-type region (with negative charge carriers, or electrons). When forward-biased, the diode conducts current, while in reverse bias, it blocks current flow. This property makes PN diodes essential for rectification, signal modulation, and various electronic applications.
N. D. Malmuth has written: 'Study of asymptotic theory of transonic wind tunnel wall interference' -- subject(s): Transonic wind tunnels, Perturbation theory, Transonic flow, Wind tunnel walls, Asymptotic series, Shock waves
Peter D. Miller has written: 'Applied asymptotic analysis' -- subject(s): Asymptotic theory, Differential equations, Integral equations, Approximation theory, Asymptotic expansions
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Edward Thomas Copson has written: 'Asymptotic expansions' -- subject(s): Asymptotic expansions
A curve may be both asymptotic and a line of curvature, in which case the curve is a line (such as the rulings of a ruled surface).
In mathematics, an asymptotic analysis is a method of describing limiting behaviour. The methodology has applications across science such as the analysis of algorithms.
Asymptotic
Musafumi Akahira has written: 'The structure of asymptotic deficiency of estimators' -- subject(s): Asymptotic efficiencies (Statistics), Estimation theory
A graph of y against x has an asymptote if, its y value approaches some value k but never actually attains it. The value k is called its asymptotic value. These are often "infinities" when a denominator in the function approaches 0. For example, y = 1/(x-2) has an asymptotic value of minus infinity when x approaches 2 from below and an asymptotic value of + infinity from above. But the asymptotic value need not be infinite - they could be a "normal number. For example y = 3-x + 2.5 has an asymptotic value of 2.5. y is always greater than 2.5 and as x increases, it comes closer and closer to 2.5 but never actually attains that value.
J. Lewowicz has written: 'Asymptotic directions of the solutions of linear differential equations' -- subject(s): Asymptotic theory, Linear Differential equations
This is much much stronger then BIBO & asymptotic.
F. H. Ruymgaart has written: 'Asymptotic theory of rank tests for independence' -- subject(s): Asymptotic theory, Statistical hypothesis testing