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This is typically performed automatically by either your startup shell or the network services, described further below. All network operations such as receiving incoming connections, initiating outgoing connections or controlling open connections may be performed by manipulating files in the /net/ filesystem. Applications are, however, not restricted to this interface, and Inferno provides system calls through Limbo modules, which applications may invoke, rather than manipulating the /net/ filesystem manually.

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You can reduce the imperfections in your video file by choosing Filter Noise Dust & Scratches. The key to success with this filter is to find a good balance between the Radius and Threshold settings. Turning up the Radius setting while leaving the Threshold setting at zero quickly reduces the dust in your image, but just as quickly adds a blur to it. Increasing the Threshold setting maintains sharpness in the image and still reduces the imperfections (see Figure 14.21).

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The filters that have their own dialog boxes and can accept custom settings, such as Lens Correction, Smart Sharpen, and High Pass; used to optimize files for output The filters that don t have customizable settings, such as Despeckle, Sharpen Edges, Blur, and so forth; used to apply default settings for quick optimization Some of the filters are very memory hungry and can take considerable time to calculate and to apply settings, especially when the allocated RAM has been consumed and efficiency is well below 100% or you are working on large files in 16-Bits/Channel mode. In those circumstances, you can take some evasive measures before you apply a filter: purge clipboard, purge histories, close Bridge (and other applications and utilities not being used currently, such as a browser or e-mail client), increase the amount of available RAM, or reduce number of fonts and plug-ins. Decreasing or increasing the filter settings can also help. For instance, if you are using Palette Knife, decrease the Stroke Size or increase the Stroke Detail.

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FIGURE 41.1 Relations among the residuals { r M ( i ) ,f ~ ( i b ~ ( z ) }The boxes with question ), . marks indicate that we still need to develop a relation between { b ~ ( i 6 ,~ ( i ) }This relation turns ) . out to be a function of data structure. For example, if the regressors have shift structure, then the question marks will be replaced by pure delays, z-'. Other data structures would lead to other choices for the blocks with questions marks - see the derivation of Laguerre lattice filters in 16 of Sayed (2003).

The thruster plume is composed of ions and electrons of various energies and some neutral gas. The energetic beam ions accelerated by the thruster fields are the dominant ion species and the major source of thrust. The velocity and angular distributions of these ions can be measured in the laboratory and calculated by the thruster computer models discussed in previous chapters. For ion thrusters, where the accelerating voltages are a thousand volts or more, the weak plume electric fields have little influence on energetic ion trajectories. In this case, the challenge is usually determining the ion trajectories from the shaped-grid accelerator structure. However, for Hall thrusters, where the accelerating voltages are a few hundred volts, the plume electric fields can significantly broaden the energetic ion plume. The second source of ions is due to charge-exchange reactions between beam ions and neutral xenon gas. The neutral gas is due to un-ionized particles leaving both the thruster and the neutralizer (hollow cathode), and, in the case of laboratory measurements, background neutrals present in the vacuum chamber. Charge-exchange reactions have usually been associated with inelastic collisions processes yielding low-energy ions at large angles with respect to the main-beam direction. However, as thruster voltages increase to provide higher specific impulse (Isp), the energy of these scattered ions can become significant. The total plume plasma density, including all three ion components, is shown schematically in Fig. 8-2 for a 4-kW Hall thruster.

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