$$\rightleftharpoonup{xx}$$
$$\longleftharp{xx}$$,
$$\longrightharp{xx}$$,
Assessing anchorage of bone to endosseous implant surfaces has been the focus of considerable attention, for which many mechanical testing methods have been described1,2. All such methods impose a force to disrupt the bone/implant model being employed, and can be broadly grouped into shear, generally presented as push-out or pull-out models3,4, reverse torque3,5, and tensile types6,7. Commonly in such tests, either bone8 or implant material (in the case of brittle glasses and ceramics9,10) is fractured and, assuming some form of anchorage has occurred, the bone/implant interface remains (at least partially) intact. Such experimental outcomes mean not only that the force required to cause the fracture (or disruption) of the model is not the force required to separate the bone/implant interface11,12, but also that the complex surface area of the created fracture plane can be refractory to accurate measurement. Nevertheless, such tests can be clinically relevant, since they provide a comparative gauge of the ability of implants of differing surface designs to be anchored in bone. However, it should also be noted that such comparisons are only valid within an experimental model, while comparisons between experimental models are fraught with difficulty since investigators use different animal species exhibiting either lamellar or woven bone; trabecular or cortical bone healing models, and different mechanical test geometries and conditions.
In an effort to derive a measurement of the tensile strength of the bone/implant interface, many investigators have used the nominal surface area of the implant to derive a "tensile strength" value, since tensile strength is measured as force per unit area. This is clearly an approximation given, as explained above, that the bone/implant interface remains intact in many of the disruption tests employed. In addition measuring the surface area of implants, particularly topographically complex surfaces, is limited by the resolution of the measurement technique as discussed by Ronald et al.13 However, as reviewed by Brunski et al.2, when the nominal surface area of an implant is taken into account, apparent differences in "tensile strength" associated with different implant surface designs are negated, suggesting that implant surfaces with higher surface area provide larger areas of bone/implant contact and thus require more force to fracture the model. The implication therefore is that more topographically complex surfaces can increase contact osteogenesis, which results in greater bone implant contact (BIC) and resultant higher disruption values in mechanical tests. Contact osteogenesis is the product of two distinct phenomena: osteoconduction and bone formation. Indeed, we have shown that increases in osteoconduction on topographically complex surfaces can be quantified by measuring the resultant BIC14, and that such surfaces also result in higher mechanical disruption values12.
However, it is salutary to note that peri-implant bone can form by two mechanisms. In contact osteogenesis cells of mesenchymal origin migrate to the implant surface (osteoconduction), differentiate into bone cells, and elaborate de novo bone matrix on the implant surface (bone formation). The first bony matrix elaborated is a mineralized cement line as seen in normal bone remodeling15 (there is much confusion in the literature concerning this mineralized biological structure that is sometimes thought to be un-mineralized1 or is syncretized with all interfaces in bone16 - for a full discussion on this topic see Davies and Hosseini17). Contact osteogenesis is an essential prerequisite for the phenomenon of bone-bonding, but is nonessential for bone ingrowth18. The mineralized cement line of bone is mechanically weaker than the mineralized collagen compartment of bone19. Thus, intuitively, if the interdigitation of cement line matrix with implant nano features is compared with bone tissue in growth into macro implant features then the mechanical force required to disrupt the former would, reasonably, be expected to be less than the latter, and we have recently demonstrated this experimentally12.
Peri-implant bone can also form by distance osteogenesis. In this case, bone is deposited on the old bone surface and gets progressively closer to the implant surface resulting in an interface comprising amorphous matrix and the remains of osteogenic cells20. In general, distance osteogenesis is associated with smooth, or machined, endosseous implant surfaces and is often seen in cortical bone healing, while microtopographically complex surfaces are associated with contact osteogenesis that is more typical of trabecular bone healing. Tensile test models using smooth implant surfaces and cortical bone healing have been able to test the adhesive properties of this amorphous biological matrix absent of the contact osteogenesis associated with topographically complex surfaces, and have shown that the so called “biochemical” bonding that occurs provides a minor component of the “tensile strength” values reported with topographically complex surfaces21. On the contrary, using a trabecular bone healing model, Wong et al.22 showed “an excellent correlation” between implant surface roughness and push-out failure load, and indicated that chemical bonding indeed played a negligible role in anchorage of bone to the implant surface. While it is probable that both contact and distance osteogenesis occur, to differing degrees, in all endosseous peri-implant healing compartments, microtopographically complex surfaces have shown themselves to be particularly advantageous in trabecular bony healing compartments23. The latter are classified as Class III or Class IV bone in the dental literature24.
Our purpose has been to focus on the mechanisms of contact osteogenesis and the resultant bone/implant anchorage that can ensue in a trabecular bone healing environment. This anchorage, which is dependent on the topography of the implant surface (see above), can occur at different scale-ranges. On the one hand, only submicron implant features are implicated in bone-bonding - as described by interdigitation of the bony cement line matrix with such surfaces, and seen on bioactive glasses, ceramics and reticulate metal oxides. On the other, bone tissue (sometimes complete with blood vasculature) can grow into multi-micron, or macro-scale, features of implant surfaces18. Both cases result in a form of bone anchorage to the implant surface, although the mechanisms are clearly different. However, a common failing of the majority of mechanical testing methods referenced above is to align the disruption force in an exactly perpendicular, or parallel plane to that of the implant surface (depending on whether tensile or shear mode is employed). We report herein a method that overcomes this limitation.