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               368                                                                         High-Pressure Synthesis (Chemistry)


























               FIGURE 1 Cross section of simple piston and cylinder appara-
               tus at high pressure. Original shape indicated by dashed lines.
               Distortions due to pressure are exaggerated.
                                                                 FIGURE 2 Cross section of “belt” high-pressure, high tempera-
                                                                 ture apparatus, split along the center line to show both (a) 1 atm
               pressure on the cylinder wall at the end of the piston im-  and (b) 6 GPa states.
               poses a high shear stress there. This, combined with the
               pinching effect on the inner cylinder between the high-
               pressure-chamber contents and the supporting rings, tends  is suitable for the synthesis of diamond and other high-
               to make the inner cylinder separate axially. The situation  pressure forms of matter. Special versions can reach pres-
               could be summed up by saying that all the free surfaces  sures of 15 GPa. Sometimes results must be interpreted
               tend to bulge and crack.                          with care because the chamber pressure can be affected
                 In order to generate pressures higher than the compres-  by local density changes resulting from heating or phase
               sive strength of the piston material, one recognizes that the  transformations. The compressible gasket, though indis-
               maximum stress gradients must be kept within limits. This  pensable, makes the determination of chamber pressure
               is best done by using a controlled reduction in stress from  more uncertain. Useful pressure calibration methods are
               the inner to the outer parts of the apparatus. This idea is  discussed later.
               embodied in all very high-pressure apparatus used above  Returning now to piston flank support, consider the
               about 4 GPa and can be seen in the cross section of the  ideal  tapered  piston  shown  in  Fig.  3,  a  truncated  cone
               “belt” apparatus shown in Fig. 2. The figure shows the sit-  of half angle α.If h is the slant height measured from
               uation at 1 atm and at 6 GPa. A composite conical gasket,  the projected apex of the cone, then at h = h 0 the work-
               consisting of a stone–steel–stone sandwich, seals the gap  ing face of the piston is exposed to a chamber pressure
               between piston and cylinder, permits the motion necessary
               for compressing the chamber contents, provides electrical
               and thermal insulation, and also supports the piston and
               cylinder surfaces with a monotonic fall in pressure from
               the tip of the piston to the atmosphere. Thus, the net stress
               on the piston falls smoothly, not abruptly, from the tip to
               the wide base. This point will be discussed more later.
                 The pressurized volume in this type of apparatus is rel-
               atively large, at least a few milliliters, and easily holds an
               electrically heated furnace. The pistons carry the heating
               current. Thermocouple or other sensing wires can be led
               out through the gaskets. Maximum steady temperatures
                                  ◦
               can be as high as 3000 C, depending on the thermal in-
               sulation used. Temperatures over 4000 C can be reached
                                              ◦
                                                                 FIGURE 3 Cross section of tapered piston with face pressure P 0
               in brief (millisecond) pulses. An apparatus of this type  and lateral support pressure P(h).
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