Page 46 - Book Hosokawa Nanoparticle Technology Handbook
P. 46

1.7 COMPOSITE STRUCTURE                                                      FUNDAMENTALS
                    The values of t, r and r as a function of P/P can  [8] C. Orr Jr., J.M. DallaValle: Fine Particle Measurement,
                                                         s
                                  k
                                       p
                  be calculated by using a combination of equa-     Macmillan Inc., p. 271 (1959).
                  tions 1.6.8 and 1.6.9.                         [9] R.W. Craust, F.F.A. Inkley:  Advance in Catalysis 9,
                    Supposing total pore volume V , which is expressed as  Academic Press Inc., New York, p. 143 (1957).
                                           p
                  a liquid volume equivalent to adsorbed amount at P ,
                                                            s
                  and adsorbed amount  V at a pressure  P (also as an
                  equivalent liquid volume), V  V is considered as a total  1.7 Composite structure
                                        p
                  empty pore volume that is generated by evaporation tak-
                  ing place at pores having radius less than r while the
                                                    p
                  pressure is reduced from P to P. This is given by  1.7.1 Composite structure of nanoparticle
                                         s
                  the following equation:
                                                                 A peculiar characteristic of the nanoparticle appears by
                                                                 the effect of size that is the general structure factor of

                                             2
                             V   V   ∫   ( r   t L r dr  (1.6.10)  particle. For example, basic physical properties such as
                                                )
                                              (
                                            )
                                                                 melting point and boiling point drop by the super-
                              p
                                                                 miniaturization. Various functions such as activity of
                                     r p
                                                                 catalyst are also improved by the nanosize effect.
                  where L(r) is a total length of pore with radius r. V p  However, the cohesion of the nanoparticle remarkably
                  and V are obtained from adsorption data, and r and t  increases with increase in the surface energy of particle
                                                        p
                  can be determined with respect to P/P . However, L(r)  by the nanosize effect, and the strong cohesion
                                                s
                  has to be obtained for each r.                 decreases the handling character of the nanoparticle.
                    For this reason, Wheeler has analyzed L(r) with the  One useful method that improves handling character of
                  assumption that its distribution follows Maxwell’s or  nanoparticles is to apply the composite structure such
                  Gaussian distribution.                         as surface modification using nanoparticles. The com-
                    Thereafter, Barrett–Joyner–Halenda [6] have sug-  posite structural control such as surface modification
                  gested a method that uses numerical integration with-  will reduce the cohesive property of nanoparticels, and
                  out assuming any specific distribution, which is  the function of nanoparticles will appear smoothly. In
                  called BJH method. Since then this method has been  addition, the composite structure that is formed by
                  improved by Pierece [7], Orr-Dalla Vallue [8], and  some kinds of nanoparticles will be able to combine
                  Crauston-Inkley [9].                           some kinds of function, and it expects that new func-
                    The measurement of pore size distribution using the  tion will appear by the effect combined some kinds of
                  gas adsorption method would have a problem in appli-  function of nanoparticle. The composite structure can
                  cation of the Kelvin equation to pore radius less than  be roughly classified as follows: (1) the composite
                  1nm. Also, because measurement of relative pressure  structure using nanoparticles, (2) the composite struc-
                  around saturation level is difficult and making some  ture formed by agglomeration of nanoparticles, and (3)
                  assumptions cannot be avoided for analyzing data,  the composite body fabricated with nanoparticles.
                  pore size distribution only less than 30nm can be usu-  The size of the nanoparticle is defined from single
                  ally measured. Therefore, use of mercury intrusion  nano (less than 10nm) to about 100nm in the narrower
                  porosimetry in combination with the gas adsorption  sense, and also to a few 100nm in the wider sense. In
                  method is preferable for measuring a wide range of  this chapter, the composite structure is assumed to be
                  pore size distribution.
                                                                 classified by the wide-range definition (from single
                                                                 nano to few 100nm). Table 1.7.1 and Fig.1.7.1 show
                                   References
                                                                 Table 1.7.1
                  [1] The Society of Powder  Technology, Japan:  Funtai
                                                                 Classification of composite structure of nanoparticles.
                     Kogaku Binran, 2nd ed., Nikkan Kogyo Shimbun,
                     p. 355 (1998) (in Japanese).                Classification       Type of composite structure
                  [2] G. Jimbo: Funtai – Sono Kino to Oyo, Nihon Kikaku
                                                                 1) The composite     (a) core–shell, (b) internal
                     Kyokai, p. 111 (1988) (in Japanese).
                                                                 structure using      dispersion, (e) hollow,
                  [3] S.J. Gregg, K.S. Sing:  Adsorption Surface Area and
                                                                 nanoparticles.       (f) porous.
                     Porosity, Academic Press, Inc., New York (1982).
                                                                 2) The composite     (a) core–shell, (b) internal
                  [4] S. Kondo,  T. Ishikawa and I.  Abe:  Kyuchaku no
                                                                 structure formed from   dispersion, (c) agglomeration,
                     Kagaku, Maruzen, p. 52 (1991) (in Japanese).
                                                                 agglomeration        (d) coating (surface modifi-
                  [5] A. Wheeler: “Catalysis Vol. II ”, Reinhold Inc., p. 116
                                                                 of nanoparticles.    cation), (e) hollow (f) porous.
                     (1953).
                                                                 3) The composite     (g) nano dens body, (h) nano
                  [6] E.P. Barrett, L.G. Joyner and P.P. Halenda: J. Am. Chem.
                                                                 structure body fabricated   porous body, (i) nano thin
                     Soc., 73, 373 (2002).
                                                                 from nanoparticles.  film.
                  [7] C. Pierce: J. Phys. Chem., 57, 149 (1953).
                                                                                                         23
   41   42   43   44   45   46   47   48   49   50   51