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to choose a level at which the normalization will bypass. Simply put, you might have sections of silence in your file. If you boost the gain in these sections, you might bring out unwanted frequencies (noise) that you could not hear previously. After you have scanned your selection you can use the RMS calculations to gauge what level to set the slider at.

Gas liquid mass transfer and kL a are described in 11. Dynamic absorption (usually of oxygen into aqueous liquids) has been a popular method for measuring kL a, although it suffers from the need for rapid response, robust dissolved oxygen probes, which although being available (the polarographic type with thin membrane and small electrolyte path length) were not always used. The probes are temperature sensitive, and their response lag must be deconvoluted from the overall response signal. More important, the dynamic methods are subject to gross errors with systems containing small bubbles, which become exhausted quickly in oxygen-lean zones then act as an extra oxygen sink in oxygen-rich zones (Heijnen et al., 1980). For these reasons, steady-state methods are preferred. Among the steady-state methods, the hydrogen peroxide catalase method of Hickman (1988a) is the most commonly used. It can be used at any scale with aqueous systems at pH around 7, but not with ionic solutes such as NaCl, KCl, or K2 SO4 (sometimes used to render the liquid noncoalescing). Air is the usual gas feed, and the liquid contains the enzyme catalase in excess. Hydrogen

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thruster in station keeping applications [13] is shown i Table 9-4 A schematic n of a generic Kaufman thruster was shown in 4, and a photograph of the T5 thruster is shown in Fig 9-5 The T5 thruster generates an 1100-V, 0329-A xenon ion beam that produces about 18 mN of thrust at a nominal Isp of 3200 s with a total efficiency of about 55% The RITA system uses a RIT-10 rf ion thruster originally developed [14] at the University of Giessen in Germany and manufactured [15] for Artemis by Astrium in Germany The performance of the RIT-10 thruster in the station keeping application [15] is shown in Table 9-5 A schematic of a generic rf thruster was shown in 4, and a photograph of the RIT-10 rf ion thruster from [16] is shown in Fig 9-6 The RIT-10 thruster generates a 1500-V, 0.

234-A xenon ion beam that produces 15 mN of thrust at an Isp of 3400 s and a total efficiency in excess of 5 1% The Institute of Space and Astronautical Science of the Japan Aerospace Exploration Agency (JAXA) launched four of the p10 ECR ion thrusters on the Hayabusa (formerly Muses-C) spacecraft [17] in 2003 These 10-cm griddiameter thrusters are successfully providing primary propulsion for an asteroid sample return mission that will return to Earth in 2010 The thruster [18,19] uses 42-GHz microwaves to produce the main plasma in the thruster and drive the electron neutralizer A schematic drawing of the thruster was shown in 4 The performance of the 10-cm ECR thruster is shown in Table 9-6, and a photograph of the thruster from Ref 20 is shown in Fig 9-7 The 10-cm ECR ion thruster generates a 1500-V, 0136-A xenon ion beam that produces 8.