Page 353 - Book Hosokawa Nanoparticle Technology Handbook
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6.2 MECHANICAL PROPERTIES                                                    FUNDAMENTALS
                                                                  With the measurement of surface sound velocity, it
                                                                 can be applied to the measurement of elastic constants
                                               σ                 on thin films. It is reported that laser is used for gen-
                                                                 erating and measuring the surface wave, and the
                                                                 sound velocity on thin films can be measured [7].
                                                                  In nanomaterials, the elastic constants on the mate-
                                                         x       rials with two phases can be discussed. For the Young’s
                                                                 modulus of two phase materials, two models are
                                                                 reported for giving upper and lower limit of the value.
                                                                 The two phase with Young’s modulus of  E and  E ,
                                                                                                    1
                                                                                                          2
                                                                 with the volume fraction of V and V , the upper limit
                                                                                              2
                                                                                        1
                                                                 of the Young’s modulus of the mixed material, E is
                                                                                                       U
                                                                               E    V E   V E          (6.2.3)
                                                         L                      U    11   2  2
                                                                 and the lower limit, E becomes
                                                                                  L
                                                                                       EE
                                                                               E        12             (6.2.4)
                                                                                 L
                                                                                    VE   V E
                                                                                     12
                                                                                          2 1
                               y
                                                                 For discussing the mechanical vibration, dumping of
                                                                 the vibration is another point of interest in the materi-
                     s: tensile stress
                     L: original length                          als. Internal friction is a material parameter relating to
                                                                                                          1
                     x: strain parallel to stress                elastic constants [8, 9]. Internal friction,  Q ,
                     y: strain perpendicular to stress           expresses the energy loss on the vibration, or the delay
                                                                 of the vibration, and it is called loss tangent (tan  ),
                                                                 too. Internal friction can be determined with the
                     E  (Young’s modulus)   =   s / (x / L)
                     n  (Poisson’s ratio)   =   y / x            applied vibration energy, W, and the lost energy  W
                                                                 with one cycle of vibration.
                  Figure 6.2.8
                  Schematic figure on Young’s modulus, E, and Poisson’s          Q  1       W          (6.2.5)
                  ratio,  .                                                            2  W
                                   High frequency   Ultrasonic sound     Echo
                                   pulse generator                                 Amplifier



                                                                      Transducer



                                   Trigger
                                                                      Buffer rod      Signal


                                                             Specimen




                                   Trigger generator                                Oscilloscope
                                                             Synchronize

                  Figure 6.2.9
                  Example of the measurement system for ultrasonic sound velocity.

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