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85139770271
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note
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y/2).
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34
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85139759592
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note
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7 V/m).
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35
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0042646798
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note
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A number of energy extraction schemes were considered-ranging from insertion of a silicon wedge switch into a trapezoidal J-II gap, to resonant electro-elastic oscillation of the entire J-II gap region, to Faraday transformer induction coupling transient magnetic fields during J-II gap closure.
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37
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0003922284
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Beichner, R.J.2
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0041644933
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note
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If the piston were to scrape charge off the plates, then it might make a single pass through the channel, but since there can be no recharging of the plates (they are insulators), the piston would not cycle. This is an uninteresting case.
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39
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85139749204
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note
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y so piston dynamics are nonlinear, and even more so if the friction or load is a function of position or velocity.
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40
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0042646795
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The traveling piston can also be viewed as the material equivalent of an electrical pulse propagating through a resistive-capacitive transmission line.
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41
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0042646797
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note
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Reliable simulators of the full, time-dependent electromagnetic, thermodynamic, and transport equations appropriate for this system are not currently available.
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42
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0042646796
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note
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The small horizontal mirror asymmetry in the field can be traced to physical/geometric asymmetry between the device interior and exterior, above and below the gap. The vertical mirror asymmetry through the gap middle is due to the differences in physical properties of electrons and holes.
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43
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0041644932
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note
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The parameters for the standard device have not been optimized for power production or efficiency; they are meant to be merely representative.
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44
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0043147825
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Physical estimates indicate electron tunneling alone may be sufficient to support device operation in the absence of Ohmic current, but this is beyond the scope of this paper.
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85139776394
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c is commonly assumed for proposed micro-and nanoscale bearings.
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Quantum effects do not appear to preclude the challenge, but they are beyond the scope of this discussion.
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0042145815
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Almost no other common physical variable varies over as many orders of magnitude as electrical conductivity. Between copper and quartz it varies 24 orders of magnitude. This variability allows for wide tuning of the piston dynamics.
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0004006463
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Benjamin/ Cummings, Menlo Park, Chap. 1,20
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61
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0042145813
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The authors predict that a laboratory test will be feasible within 5 years.
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