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Impedance matching network, 356 defined

Of course, care should be taken when comparing the experimental data and the modeling results the model is an approximation, and the experiment has its uncertainties. The most important approximation is that the model is one-dimensional. A main uncertainty of the experiment is the relation between source power and plasma power (see Section 1.3.2.3). The source power is defined as the power delivered by the power generator. In experiments, the source power is a discharge setting (Table IV). The plasma power is the power dissipated by the plasma. As a rule, this plasma power is smaller than the source power, due to losses in the matching network, which matches the plasma impedance to the impedance of the source power generator, viz., 50 [180]. From comparison of experimental data... [Pg.53]

In general, the input impedance will vary from point to point in the network because of variations in vessel sizes and properties. If the network has the same impedance at each point (perfect impedance matching), there will be no wave reflections. Such a network will transmit energy most efficiently. The reflection coefficient R, defined as the ratio of reflected to incident wave amplitude, is related to the relative characteristic impedance of the vessels at a junction. For a parent tube with characteristic impedance Zq branching into two daughter tubes with characteristic impedances Z and Z2, the reflection coefficient is given by... [Pg.979]


See other pages where Impedance matching network, 356 defined is mentioned: [Pg.41]    [Pg.290]   
See also in sourсe #XX -- [ Pg.414 ]




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