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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.
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 Flow Transducer is also known as a flow senser. A flow senser is used to sense the flow rate a fluid flows or flow logger to record the flow of the fluids that run through them.
when the diode is applied forward bias voltage the width of depletion region gets reduced the barrier voltage decreases there by facilitating the easy exchange of holes and electrons. when the diode is reverse biased the width of depletion region increases there by hindering the flow or exchange of charge carriers.
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
west region
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.