Page 100 - Handbook of Adhesives and Sealants
P. 100

68   Chapter Two


            the radius and half the thickness of a thin, circular layer of liquid in
            contact with the solid; and   LV  is the surface tension of the liquid. If
            R is greater than R , then p will be greater than p . Hence, the two
                                                             1
                               2
             1
                                       2
            plates will be forced together because of the pressure difference p
                                                                          2
            p . From this equation it follows that many common liquids that spon-
             1
            taneously wet two such solid surfaces will hold them together.
              In reality, however, the assumptions stated above are never realized.
            Extremely close fitting, perfectly smooth, solid adherends would be
            very expensive to prepare. The absence of dust or other particles on
            the surface could be critically important in forming a strong joint. The
            resistance of the joint to stress is determined solely by the viscosity
            of the liquid film; hence, only if the viscosity is very great could the
            joint withstand practical loading pressures.
              Since real surfaces are not smooth or perfectly flat, it is necessary
            to understand the effects of surface roughness on joint strength. A
            viscous liquid can appear to spread over a solid surface and yet have
            many gas pockets or voids in small surface pores and crevices. Even
            if the liquid does spread spontaneously over the solid, there is no cer-
            tainty that it will have sufficient time to fill in all the voids and dis-
            place the air. The gap-filling mechanism is generally competing with
            the setting mechanism of the liquid.
              Problems occur when the liquid solidifies rapidly after being ap-
            plied. Two examples are fast curing epoxies and fast gelling hot melt
            adhesives. Very fast reacting epoxy adhesive systems generally do not
            have the high adhesion strength that slower curing epoxy systems
            have. One reason for this (there are others primarily related to the
            chemistry of these fast acting systems) is that the curing reaction does
            not provide sufficient time for the adhesive to fill the crevices on the
            substrate surface. Cyanoacrylate adhesives, on the other hand, are
            also very fast curing adhesives that provide exceptionally high bond
            strengths on many substrates. Although cyanoacrylate resins set rap-
            idly, their viscosity and wetting characteristics are such that they
            quickly permeate the crevices and valleys on a substrate surface.
            When a hot melt adhesive is applied in melt form to a cold metal
            surface, the adhesion is much weaker than if the hot melt was applied
            to a preheated metal surface and then allowed to cool at a slower rate
            along with the substrate. When the hot melt makes contact with the
            cold surface the adhesive gels immediately, and there is no time for
            the adhesive to fill-in the cavities on the surface.
              In certain cases, roughening of the surface may be undesirable—
            actually decreasing the resulting joint strength. There is a noticeable
            difference in measuring the contact angle of a liquid spreading over a
            clean dry surface,   , and the contact angle measured when the liquid
                              A
            recedes from a previously wet surface,   . When a difference is ob-
                                                   R
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