Page 174 - Book Hosokawa Nanoparticle Technology Handbook
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FUNDAMENTALS                CH. 3 CHARACTERISTICS AND BEHAVIOR OF NANOPARTICLES AND ITS DISPERSION SYSTEMS


















                  Figure 3.5.22
                  Schematic drawing of the atomic force microscope.
                                                                 Figure 3.5.23
                                                                 Scanning electron microscope image of a colloid probe.
                  reasons, several other methods have been developed
                  to measure the interaction forces between the solid
                  surfaces of a wider variety of materials. Among them,  operate, the colloid probe method has recently been
                  the colloid probe method [1] using an atomic force  applied to a wider variety of research fields.
                  microscope (AFM) has recently become one of the  The details of the practical procedure of the AFM
                  most important methods in various research fields  colloid probe method are as follows. For the colloid
                  and has seemed to become as popular as the SFA  probe, spherical particles typically in the diameter
                  measurement or more.                           range of 1–30  m are used. A particle is attached to the
                    The AFM was originally designed to provide high-  probe with epoxy glue or hot-melt epoxy resin, using a
                  resolution topographic images of surfaces with a  micropositioning device such as a micromanipulator by
                  molecular (in the ideal case, atomic) order. Its princi-  observing with an optical microscope or a CCD
                  ple is shown in Fig. 3.5.22: a probe with a cantilever  camera. The probes for imaging are applicable to force
                  spring and a pyramidal-shaped sharp tip attached to  measurements and a large variety of probes are now
                  the end of the cantilever is brought in contact with a  available commercially. Thus, a probe can be chosen
                  sample surface mounted on a piezo scanner.  The   based on their spring constant, depending on the
                  tip scans over the surface by the movement of the  strength of the interaction force to be measured.
                  piezo scanner on which the sample is mounted. During  Typically, probes with a soft, triangular cantilever are
                  scanning, the displacement of the cantilever along the  used to measure repulsive forces, while those with a
                  undulation of the surface is measured with the laser  stiff, rectangular cantilever are used to measure strong
                  reflected onto the back of the cantilever. By mapping  attractive forces and/or adhension forces. Although
                  the displacement, a surface image can be obtained.  the nominal spring constant is usually provided by the
                    In order to apply the AFM to force measurements,  manufacturers, it is highly desirable to determine the
                  the sample surface is moved vertically (z direction) by  spring constant precisely to obtain the accurate value of
                  the expanding–shrinking of the piezo scanner to alter  the interaction force. To determine the spring constant,
                  the distance between the probe and the surface. The  various methods have been proposed thus far. The most
                  cantilever deflection by the interaction forces acting  popular and reliable method among them would be the
                  between the surfaces can be measured with the laser as  one developed by Cleveland et al. [2]. In this method,
                  is the case in imaging (most commercial AFMs have  the resonant frequency of the oscillating probe is meas-
                  an operation mode to conduct these procedures auto-  ured both by attaching and without attaching particles
                  matically).  The interaction forces are calculated by  of known mass to the cantilever, and the spring con-
                  Hooke’s law, multiplying the spring constant of the  stant is calculated from the shift in frequency.
                  cantilever by the cantilever deflection. The interaction  Figure 3.5.24(a) shows a schematic representation of
                  forces between macroscopic surfaces, which are a par-  the typical force data obtained by a force measurement
                  ticle and a flat surface, can also be measured by attach-  between symmetrically charged solid surfaces in an
                  ing a small particle onto the top of the cantilever   aqueous solution. This measurement cycle entails the
                  (Fig. 3.5.23), which is often called the “colloid probe”.  following procedure: approaching the probe to the flat
                  For the colloid probe, a wide variety of materials can  sample, making contact with both surfaces, and retract-
                  be used and the surface can also be modified with a  ing the probe from the flat sample. During the meas-
                  variety of molecules by adsorption from a solution or  urement, the photodetector output voltage  V that
                  chemical reaction. Due to its versatility and easiness to  indicates the deflection of the cantilever by the position

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