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FEED LINE BASICS                                                        319





















                Figure 6.6.10 a) Coaxial to TM01-mode transition, b) Rotary joint, c) Schematic drawing
                                              of rotary joint

            2.  According to the  Lorentz’s  equation introduced in  Chapter  1,  the E-field  nudges  the
               positively charged particles in the direction of the field. Evidently, the negatively charged
               particles move and accelerate in the opposite direction. If such interaction between the
               fields and particles lasts long enough (in term of speed of light), the kinetic energy of
               particles and their speed can be substantially increased. It’s imperative that the accelerated
               particles do not collide with gas molecules on their journey through the accelerator, so the
               particle beam is contained in an ultrahigh vacuum inside a metal pipe that is a natural WC.
               To maintain the particle acceleration, we must create in such tube the longitudinal force
               continuously  pushing particle forwards. TM01-mode  with its  z-component  meets this
               requirement perfectly well. We stop here since more detail discussion of power transfer
               efficiency during the accelerating process, and accelerator structure itself is far beyond the
               scope of this book.
            3.  One of the WC application is the industrial microwave material processing. The idea is
               trivial: a wide range of materials are more or less conductive. Then according to Ohms law,
               the E-field exerts the conductivity current and heats a material the same way as our home
               microwave oven warms up food. One of such “oven” for fruit drying is demonstrated in
                           17
               Figure 6.6.11a . Figure 6.6.11b illustrates the basic schematic of the heating process. Wet
               material is put on a conveyor belt that transports it inside the microwave heater. At room
               temperature and 1 atmosphere pressure, 1 kilowatt of microwave energy will evaporate
               approximately ~1.13 kg of water in 1 hour. As such, water vaporizes, and the dry material
               leaves the heater. TM01-mode in WC is one of the best candidates for such applications
               because it has the longitudinal component of E-field continuously heating material on its
               way inside the “oven.” The significant advantage of microwave heating is that the EM
               waves penetrate deeply into material drying it from inside out. Conventional processing is
               opposite and dries first the material surface and only then heats interior typically quite slow
               due to the commonly low thermal conductivity of materials. If so, the surface temperature
               could reach the  burning level  while its  interior  is still  unheated.  Microwave  heating
               overcomes those time and temperature limitations even when the materials are relatively
               thick.




            17  Public Domain Image, source: http://spanish.alibaba.com/product-gs/fruit-juice-industrial-microwave-
            tunnel-dryer-with-panasonic-magnetron-60300592430.html
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