Page 179 - Book Hosokawa Nanoparticle Technology Handbook
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3.5 INTERACTIONS BETWEEN PARTICLES                                           FUNDAMENTALS



























                  Figure 3.5.27
                  Concept of two types of tensile tester.



















                  Figure 3.5.28
                  Concept of shear test using Jenike’s cell.



                    in the equation means   axial intercept of the line, it  Coulomb’s equation, and the flowability of powder is
                   C
                  is called the adhesion which shows the shearing  going bad with increment of n.
                  strength of adhesion power at    0. Generally, the
                  powder yield locus of fine powders such as nanoparti-  e) Flow factor
                  cles does not show the straight line, shows a convex  The powder yield locus changes with the pre-consol-
                  curve. In this case, the following Warren spring equa-  idation pressure or void fraction of the powder bed,
                  tion [10] can be used for the approximation of PYL  but as is indicated the powder flowability that does
                                                                 not depend on packing condition of the flow factor
                                 ⎛  	 ⎞  n                       was proposed by Jenike [11]. The flow factor means
                                 ⎜ ⎝  	 ⎠ ⎟     T    T  (3.5.64)  the maximum height of a self-sustaining powder with-
                                   c
                                                                 out collapse by the weight, and calculated from the
                                                                 shear test result.  As shown in Fig. 3.5.30, when
                  where    and    are the adhesion and the tensile  the Mohr’s stress circle is drawn, the flow factor F f
                         c
                               T
                  strength of the powder, respectively, and n is the shear  can be calculated from the maximum principal stress
                  index. For shear index n 1, the equation agrees with  of the Mohr’s stress circle or called the unconfined
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