A MODEL FOR THE ROLE OF INTEGRINS IN FLOW INDUCED MECHANOTRANSDUCTION IN OSTEOCYTES B METHODS: Our idealized structural model showing the suspension of a cell process in canalicular cross-sections with a local collagen hillock and its associated integrin complex is sketched in Fig. 2. Structurally, one conical collagen hillock, one integrin molecule and one integrin intracellular anchor protein complex locally replace one local transverse tethering element and its associated transmembrane molecule and crossfilament in the axisymmetric model in (5), in which only transverse tethering elements are present. The hydrodynamic loading on the transverse elements and the resulting deformation of the cell process is asymmetric because of the asymmetry of the local collagen hillock. Y Canalicular Wall B Transverse Element T6 T4 Cell Process Membrane T3 X Fimbrin Intracellular Anchor Protein Complex T6 T5 Actin Filament Transmembrane Molecule O A O’ O’’ Collagen Hillock T0 20 0 10 20 DISCUSSION: Although the precise mechanism by which bone cells sense mechanical signals still remains elusive, several candidate mechanotransducers, including the integrin-cytoskeleton structure, mechanically activated channels, G protein-dependent pathways and caveolin, have been proposed (9). Furthermore, links are emerging between integrins and other putative membrane mechanotransducers through the cytoskeleton or intermediate linkers (10). Therefore, mechanical consequences due to the integrin attachment could initiate other signaling pathways directly or indirectly and integrins would be the primary mediator in mechantransduction. β1 and β3 integrin subunits have been observed along the cell process (7). Results in Fig. 3A imply a rate of increase in T0 of approximately 20pN/s for a sinusoidal tissue loading of 20MPa at 1Hz. In this low applied loading rate limit, the typical force for detachment of a single α5β1 integrin-fibronectin pair would be 40-60pN (11), and that of a single β3 integrin roughly 20pN based on the measurements in (12, 13) and an analogy of the rupture force patterns between β1 and β3 integrins. Our model predicts that T0 is approximately 12pN at this tissue loading rate. Thus, the integrin attachment can resist rupture even if the focal attachment involves only a single integrin molecule. The large axial strains result from the large axial displacements of the free ends of the tethering elements about a fixed integrin site and fall into the range that could significantly excite bone cells in vitro (14). CONCLUSION: The prediction of our model provides a quantitatively feasible hypothesis that integrin attachments between the cell process membrane and the collagen hillocks could serve as mechanical transducer sites to directly or indirectly excite osteocytes via the flow induced tensions and strains in the vicinity of such sites. T2 T1 10 1 MPa 0 Frequency (Hz) Frequency (Hz) Fig.3. Mechanical consequences of the integrin attachment. A) The tensile force at integrin attachment site and B) the axial strain of the cell membrane around the integrin attachment site as a function of loading frequency with loading amplitude as a parameter. Fig.1. EM micrographs showing collagen hillocks with attachments and transverse tethering elements spanning the pericellular space between the cell process membrane and the canalicular wall. A) Longitudinal cross-section (bar=500nm). B) Transverse crosssection (bar=100nm). Pericellular Space Homogenous Elastic Cylinder 0 0 Collagen Hillock A Axial Strain (%) Transverse Tethering Element A Tensile Force (pN) *Wang, Y; *Weinbaum, S; **McNamara, LM; +**Schaffler, MB *Department of Biomedical Engineering, The City College of New York and CUNY Graduate Center, New York, NY; +**Leni and Peter W. May Department of Orthopedics, Mount Sinai School of Medicine, New York, NY [email protected] tethering filaments and their associated cross-filaments are assumed to INTRODUCTION: Osteocytes are generally believed to be the primary act in the same cross-sectional plane in treating the radial force balance mechanosensory cells in bone tissue (1). A growing body of theoretical shown in Fig. 2A. and experimental studies (2-5) suggests that the interstitial fluid flow in the lacunar-canalicular porosity provides stress-induced mechanical RESULTS: In Fig. 3, we plot the tensile force T0 acting at the integrin signals to excite osteocytes. However, the mechanoreceptors for the initial detection and the transduction of such extracellular mechanical attachment site and the axial strain εa of the cell membrane in the signals into intracellular biological signals remain to be determined. vicinity of the integrin attachment site as a function of loading frequency Integrins are ubiquitous transmembrane adhesion proteins that with tissue loading amplitude as a parameter. T0 increases as the couple the cytoskeleton to the extracellular matrix, and are essential for frequency or the amplitude of the tissue loading increases. Surprisingly, cellular responses to mechanical stimuli in many cell types (6). Recently, εa is approximately one order of magnitude larger than the radial strain it has been observed that conical collagen hillocks occasionally project of the cell membrane (data not shown) for the same tissue loading. T0 from the bony wall completely across the pericellular space to contact could reach 15pN, and εa 7%, for physiological tissue loading rates (8). the cell membrane of the osteocyte process as shown in Fig.1 and that A B such local asymmetric attachments are integrin-based (7). The primary 40 15 20 MPa goal of this study is to determine the mechanical consequence of such 30 attachments and its role in mechanotransduction. Of particular interest 10 10 MPa 20 are the tensile forces generated at the integrin attachment sites and the 5 MPa 5 resulting strains on the cell process membrane. 10 Cross Filament Integrin Molecule Fig.2. The idealized structural model showing the suspension of a cell process in canalicular cross-sections with a locally asymmetric collagen hillock and its associated integrin complex (solid line—before deformed; dash line—after deformed). A) Transverse cross-section. B) Longitudinal cross-section. To simplify the mechanical analysis of the cell process, two idealizations have been made. First, the central actin bundle in the core of the cell process is replaced by a homogenous elastic cylinder of the same size and overall radial elastic coefficient as the original cross-inked structure when dealing with the radial deformations due to the radial tensile forces. Second, the tensile forces on the integrin attachment, the ACKNOWLEDGMENTS: Funded by NIH AR41210 and AR48699. REFERENCES: 1) Burger, 1999, FASEB Journal; 13:S101; 2) Reich, 1991, Am. J. Physiol.; 261:C428; 3) Weinbaum, 1994; J. Biomech.; 27:339; 4) You, 2001, J. Biomech.; 34:1375; 5) Han, 2004, PNAS; 101:16689; 6) Katsumi, 2004, J Biol Chem.; 279:12001; 7) McNamara, 2006, ORS abstract; 8) Fritton, 2000, J. Biomech.; 33:317; 9) Rubin, 2006, Gene; 367:1; 10) Alenghat, 2002, Sci. 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