Page 79 - Plastics Engineering
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62                                    Mechanical Behaviour of Plastics
                       to bear in mind that the manufacturing method may have introduced anisotropy
                       which will result in different thermal responses in different directions in the
                       material.
                         The coefficient of thermal expansion, UT, is given by

                                                                                    (2.17)


                       where SL  is the change in length in the material
                              L is the original length
                            AT  is the change in temperature.
                         There are standard procedures for determining UT (e.g.  ASTM  696) and
                       typical values for plastics are given in Table 1.2. It may be observed that the
                       coefficients of thermal expansion for plastics are higher than those for metals.
                       Thus if 50 mm lengths of polypropylene and stainless steel are each heated up
                       by 60°C the changes in length would be

                         (a)  polypropylene,  SZ = 100 x   x 50 x 60 = 0.3 mm
                         (b)  stainless steel,  SL = 10 x   x 50 x 60 = 0.03 mm

                       If  these changes in  length take place freely then  we  will have a  thermally
                       induced strain in the material (= 0.3 x 100/50 = 0.6% in the polypropylene)
                       but no stress. However, if the polypropylene was constrained in some way so
                       that the 0.3 mm expansion could not happen when it is heated by 6O"C, then
                       there would be a thermally induced stress in the material, i.e.
                                              stress = modulus x strain

                       If  the modulus of  the material is 1.2 GN/m2 at the final temperature, then the
                       stress in the material would be given by

                                      stress = 1.2 x io9 (;E) - = -7.2 MN/m2

                       Note  that  the  stress  is  compressive  because  the  material  is  effectively
                       compressed by 0.3 mm.
                         Example 2.6  The  bobbin  shown  in  Fig. 2.16 has  been  manufactured  by
                       sliding the acetal ring on to the steel inner and then placing the end-plate in
                       position. At 20°C there are no stresses in the acetal and the distance between
                       the  metal  end-plates is  equal to the length of  the  acetal ring.  If  the  whole
                       assembly is heated to lOO"C, calculate the axial stress in the acetal. It may be
                       assumed that there is no friction between the acetal and the steel. The coeffi-
                       cients of thermal expansion for the acetal and the steel are 80 x 10-6"C-' and
                        11 x 10-60C-1 respectively. The modulus of the acetal at 100°C is 1.5 GN/m*.
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