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C R Jacobs

Publications and source records attributed to C R Jacobs.

At least 37 records · Page 2Linked to original sources

Tension and bending, but not compression alone determine the functional adaptation of subchondral bone in incongruous joints.

In the present study, we tested the hypothesis that tension and bending, rather than compression alone, determine the functional adaptation of subchondral bone in incongruous joints. We investigated whether tensile stresses in the subchondral bone of the humero-ulnar articulation are affected by the direction of muscle and joint forces, and whether the tensile stresses are large enough to cause microstructural adaptation, specifically a preferential alignment of the trabeculae and the subchondral collagen fibres. Using a previously validated finite element model of the human humero-ulnar joint, we calculated the contact pressure, the principal compressive and tensile stresses, and the strain energy density in the subchondral bone for various flexion angles. A bicentric (ventro-dorsal) pressure distribution was found in the joint at 30 degrees to 120 degrees of flexion, with contact pressures of up to between 2.5 and 3 MPa in the ventral and dorsal aspects of the ulnar joint surface, but less than 0.5 MPa in the centre. The principal tensile stress in the subchondral bone of the trochlear notch quantitatively exceeded the principal compressive stress at low flexion angles (maximum 8.2 MPa), and the distribution of subchondral strain energy density differed substantially from that of the contact stress (r=-0.72 at 30 degrees and r=+0.58 at 90 degrees of flexion). No important tensile stress was computed in the trochlea humeri. On contact radiography, we found sagittally orientated subarticular trabeculae in the notch, running tangential to the surface. Furthermore, we observed sagittally orientated split lines in the subchondral bone of the notch of 20 cadaver joints, suggesting a ventro-dorsal orientation of the collagen fibres. The trochlea humeri, on the other hand, did not show a preferential direction of the subchondral split lines, these findings confirming the predictions of tensile stresses in the model. We conclude that, due to the important contribution of tension to subchondral bone stress, the distribution of subchondral density cannot be directly employed for assessing the long term distribution of joint pressure at the cartilage surface. The magnitude of the tensional stress varies considerably with the direction of the muscle and joint forces, and it appears large enough to cause functional adaptation of the subchondral bone on a microstructural level.

Adaptation, Physiological↗

NACOB presentation to ASB Young Scientist Award: Postdoctoral. The impact of boundary conditions and mesh size on the accuracy of cancellous bone tissue modulus determination using large-scale finite-element modeling. North American Congress on Biomechanics.

The apparent properties of cancellous bone are determined by a combination of both hard tissue properties and microstructural organization. A method is desired to extract the underlying hard tissue properties from simple mechanical tests, free from the complications of microstructure. It has been suggested that microCT voxel-based large-scale finite element models could be employed to accomplish this goal (van Rietbergen et al., 1995, Journal of Biomechanics, 28, 69-81). This approach has recently been implemented and it is becoming increasingly popular as finite element models increase in size and sophistication (Fyhrie et al., 1997, Proceedings of the 43rd Annual Meeting of the Orthopaedic Research Society, San Francisco, CA, p. 815; van Rietbergen et al., 1997, Proceedings of the 43rd Annual Meeting of the Orthopaedic Research Society, San Francisco, CA, p. 62). However, no direct quantitative measurements of the accuracy of this method applied to porous structures such as cancellous bone have been made. This project demonstrates the feasibility of this approach by quantifying its best-case accuracy in determining the trabecular hard tissue modulus of analogues fabricated of a material with known material properties determined independently by direct testing. In addition we were able to assess the impact of mesh size and boundary conditions on accuracy. We found that the assumption of a frictionless boundary condition in the parallel plate compression loading configuration was a significant source of error that could be overcome with the use of rigid end-caps similar to those used by Keaveny et al. (1997 Journal of Orthopaedic Research, 15(1), 101-110). In conclusion, we found that this approach is an effective method for determining the average trabecular hard tissue properties of human cancellous bone with an expected practical accuracy level better than 5%.

Awards and Prizes↗

Microcatheter adhesion of cyanoacrylates: comparison of normal butyl cyanoacrylate to 2-hexyl cyanoacrylate.

PURPOSE: To compare the catheter adhesion properties of 2-hexyl cyanoacrylate (Neuracryl M), a new agent, to those of normal butyl cyanoacrylate (Histoacryl), the most widely used liquid acrylic agent for microcatheter embolization. MATERIALS AND METHODS: 2-hexyl cyanoacrylate (Neuracryl M1) was tested in pure form and mixed with either a proprietary polymerization retardant/contrast agent (Neuracryl M2) or ethiodized oil (Ethiodol). Histoacryl was tested in pure form and mixed with Ethiodol. The cyanoacrylate mixtures were injected through microcatheters into wells partially filled with heparinized whole blood. The cyanoacrylates were allowed to polymerize around the microcatheter tips for 1-3 minutes. The microcatheters were then pulled at a constant rate until they were extracted from the polymerized cyanoacrylates. The peak forces required for extraction were recorded. RESULTS: The peak forces required to extract the microcatheters from either pure Histoacryl or Histoacryl mixed with 33% Ethiodol were significantly higher (P < .01; P < .05) than those for pure Neuracryl M1. When Neuracryl M1 and M2 were mixed together (as intended for clinical use), the force required for microcatheter extraction was significantly lower than that for either pure Histoacryl, Histoacryl mixed with 33% Ethiodol, or Neuracryl M1 alone (P < .01; P < .01; P < .01, respectively). The force required to extract microcatheters from the Neuracryl M1 and M2 mixture was not, however, significantly different from that of Histoacryl mixed with 50% Ethiodol. The force of extraction for the Neuracryl M1 and 50% Ethiodol mixture was below our ability to obtain precise measurements. CONCLUSION: When Neuracryl M1 was mixed with its proprietary polymerization retardant/contrast agent (Neuracryl M2), catheter adhesion was not significantly different from that of Histoacryl mixed with 50% Ethiodol, a mixture common in clinical use. When Neuracryl M1 was tested alone or mixed with Ethiodol (not intended by the manufacturer), catheter adhesion was significantly decreased relative to pure Histoacryl or equivalent mixtures of Histoacryl and Ethiodol.

Adhesiveness↗

Differential effect of steady versus oscillating flow on bone cells.

Loading induced fluid flow has recently been proposed as an important biophysical signal in bone mechanotransduction. Fluid flow resulting from activities which load the skeleton such as standing, locomotion, or postural muscle activity are predicted to be dynamic in nature and include a relatively small static component. However, in vitro fluid flow experiments with bone cells to date have been conducted using steady or pulsing flow profiles only. In this study we exposed osteoblast-like hFOB 1.19 cells (immortalized human fetal osteoblasts) to precisely controlled dynamic fluid flow profiles of saline supplemented with 2% fetal bovine serum while monitoring intracellular calcium concentration with the fluorescent dye fura-2. Applied flows included steady flow resulting in a wall shear stress of 2 N m(-2), oscillating flow (+/-2 Nm(-2)), and pulsing flow (0 to 2 N m(-2)). The dynamic flows were applied with sinusoidal profiles of 0.5, 1.0, and 2.0 Hz. We found that oscillating flow was a much less potent stimulator of bone cells than either steady or pulsing flow. Furthermore, a decrease in responsiveness with increasing frequency was observed for the dynamic flows. In both cases a reduction in responsiveness coincides with a reduction in the net fluid transport of the flow profile. Thus. these findings support the hypothesis that the response of bone cells to fluid flow is dependent on chemotransport effects.

Calcium Signaling↗

Plating techniques and plate orientation in repair of mandibular angle fractures: an in vitro study.

A biomechanical model utilizing polystyrene mandibles was devised to evaluate the fixation efficacy of various plating techniques for repair of mandibular angle fractures. A simple angle fracture was created in the mandible models at a standardized location and was repaired using five different plating techniques. Each experimental group consisted of 15 mandibles, with fracture site, plate placement, load application, and fracture displacement measurement standardized to ensure consistency among experimental groups. Measurement of fracture distraction under load application generated a load deformation curve and corresponding slope for each technique. Comparison of load deformation slopes allowed assessment of fixation stability. When applied with a subapical, medially placed monocortical tension band, bicortical compression plating demonstrated the most stable fracture fixation. The data show that biplanar plate placement in both monocortical noncompression and bicortical compression techniques yields a stronger fixation than monoplanar placement.

Biomechanical Phenomena↗

Computer simulation of subchondral bone adaptation to mechanical loading in an incongruous joint.

BACKGROUND: We hypothesized that the typically bicentric distribution of subchondral bone density (i.e., two maxima) in incongruous joints with deeper sockets could be predicted by a computer simulation employing a concavely incongruous finite-element model and current bone remodeling theory. Additional objectives were to assess the uniqueness of the solution with respect to assumed model parameters and initial conditions and to determine the relationship between contact areas, subchondral bone stress, and subchondral bone density patterns. METHODS: An idealized model of the humeroulnar joint was constructed with a quantitatively realistic representation of its natural incongruity. A currently accepted remodeling theory was implemented with a finite-element code using a node-based approach. RESULTS: The simulation predicted a dense subchondral bone plate after application of 3,000 daily load cycles for 300 days. The pronounced bicentric distribution of subchondral mineralization emerged. The solution was virtually independent of the initial density distribution and other assumed model parameters. Furthermore, the model predicted high tensile stresses in the subchondral bone, when the joint socket was spread apart during loading. Therefore, the locations of maximal strain energy density in the subchondral bone did not correspond with areas of joint contact. CONCLUSIONS: The results of the bone remodeling simulations are consistent with patterns of subchondral bone density determined experimentally. Furthermore, the solutions exhibited a high degree of uniqueness, were rather insensitive to changes in cartilage stiffness, moderately sensitive to number of applied loading cycles, and highly sensitive to loading magnitude. Tensile stresses seem to play a dominant role in subchondral bone remodeling due to bending in the subchondral bone plate. Thus, we conclude that, in the case of an incongruous joints with deeper sockets, the density of the subchondral bone cannot be regarded as a direct measure of the adjacent articular pressure.

Adaptation, Physiological↗

Adaptive bone remodeling incorporating simultaneous density and anisotropy considerations.

Over 100 years ago, Wolff hypothesized that cancellous bone altered both its apparent density and trabecular orientation in response to mechanical loads. A mathematical counterpart of this principle is derived by adding a remodeling rule for the rate-of-change of the full anisotropic stiffness tensor (all 21 independent terms) to the density rate-of-change rule adapted from an existing isotropic theory. As a result, anisotropy and density patterns develop such that the local stiffness tensor is optimal for the given series of applied loadings. The method does not rely on additional morphological measures of trabecular orientation. Furthermore, assumptions of material symmetry are not required, and any observed regions of orthotropy, transverse isotropy, or isotropy are a result entirely of the functional adaptation of the bone and not the consequence of a modeling assumption. This approach has been implemented with the finite element method and applied to a two-dimensional model of the proximal femur with encouraging results.

Anisotropy↗

Mechanobiological adaptation of subchondral bone as a function of joint incongruity and loading.

Computed tomography (CT) has been employed to determine non-invasively the distribution of subchondral bone density in joints and to evaluate their dominant loading pattern. The objective of this study was to investigate the relationship between subchondral bone adaptation, joint incongruity and loading, in order to determine to what extent the loading conditions and/or geometric configuration can be inferred from the distribution of subchondral density. Finite element models of joints with various degrees of incongruity were designed and a current remodeling theory implemented using the node-based approach. Appropriate combinations of joint incongruity and loading yielded subchondral bone density patterns consistent with experimental findings, specifically a bicentric distribution in the humero-ulnar joint and a monocentric distribution in the humero-radial joint. However, other combinations of incongruity and loading produced similar subchondral density patterns. Both the geometric joint configuration and the loading conditions influence the distribution of subchondral density in such a way that one of these factors must be known a priori to estimate the other. Since subchondral density can be assessed by CT and joint geometry by magnetic resonance imaging, the dominant loading pattern of joints may be potentially derived in the living using these non-invasive imaging methods.

Adaptation, Physiological↗

Evaluation of fracture predilection in the calcaneus after external fixator pin removal.

OBJECTIVES/HYPOTHESIS: External fixators have been advocated for the treatment of intra-articular fractures of the distal tibia, so-called "pilon" or "plafond" fractures. Current recommendations include placement of external fixator pins, which vary in diameters up to six millimeters, in the talus and calcaneus. Removal of a relatively large pin may create a large defect in the bone, theoretically increasing fracture predilection with weight bearing. The objective was to compare the compressive load at failure of intact and formerly instrumented calcanei. It was hypothesized that the pin hole defect would not lead to a clinically significant difference in compressive load at failure. STUDY DESIGN: A biomechanical evaluation of randomized matched pairs of cadaveric calcanei. METHODS: Fresh human calcanei were harvested, embedded in casting compound, and tested pairwise. Among pairs of calcanei, one served as the control, and the other was drilled with a 6.0-mm pin in the posterior portion. The pin was removed before biomechanical evaluation. Testing was performed in compression under displacement control on a hydraulic materials testing system. RESULTS: There was a 22% reduction in compressive load at failure (p = 0.021) of the drilled versus intact specimens. Compared with intact calcanei, defect calcanei had a compressive failure load much closer to forces that might be encountered with walking and running. CONCLUSIONS: The six-millimeter-pin defect is a significant stress riser, and protected, progressive weight bearing after pin removal should be recommended.

Aged↗

Effects of fluid flow on intracellular calcium in bovine articular chondrocytes.

Fluid flow-induced shear stress results in a variety of morphological and metabolic changes in cultured bovine articular chondrocytes (BAC). However, the mechanism by which the flow signal is transduced into a biological response is unknown. Therefore, we investigated the effects of fluid flow on intracellular Ca2+ concentration ([Ca2+]i) in BAC. Cells loaded with fura 2 were exposed to steady and pulsatile (0.5 Hz) flow at 9, 18, and 34 ml/min in a parallel-plate flow chamber. In response to flow, there was a significant and flow rate-dependent increase in the percentage of cells showing a rise in [Ca2+]i, but no effect on the [Ca2+]i response amplitude. There was no significant difference between the [Ca2+]i responses to steady and pulsatile flow. Mean intracellular Ca2+ response values ranged between 26.2 +/- 1.6 (9 ml/min) and 38.0 +/- 6.8 nM (34 ml/min) above basal [Ca2+]i (81.3 +/- 24.1 nM, n = 90). Removal of extracellular Ca2+ or addition of Gd3+ significantly reduced the percentage of cells responding, suggesting that influx of Ca2+, possibly through mechanosensitive channels, contributes to the rise in intracellular Ca2+. Our data suggest fluid flow-induced mobilization of intracellular Ca2+ may contribute to the mechanism by which mechanical loads are transduced by chondrocytes.

Animals↗

Different loads can produce similar bone density distributions.

Finite element models of a generic long bone and the proximal femur were used to identify important load characteristics and to determine whether small changes in load affect bone adaptation simulations. We also examined the effect of implants on the sensitivity of bone adaptation simulations to changes in loads. For each model, a primary load set was selected and incorporated in a bone adaptation simulation to generate a primary density distribution. A density-based load estimation method was used to determine a secondary set of loading conditions for each model. Each secondary load set was incorporated in a bone adaptation simulation and the resulting density distribution was compared to the corresponding primary density distribution. Nearly identical density distributions were produced for the natural generic long bone model (average nodal density difference 0.02 g/cm3). For the natural proximal femur model, the density distributions were very similar, but differences were apparent (average nodal density difference 0.07 g/cm3). The same primary and secondary load sets were used for bone adaptation simulations with implant models. For the proximal femur model, density distribution differences with the implant were very slightly less than those of the natural model. For the generic long bone model, the implant amplified differences between density distributions (average nodal density difference 0.14 g/cm3). Thus, variations in loading conditions may partially explain variations in long-term total joint outcome. The total equivalent stimulus load magnitudes for the two load sets for the generic long bone model were within 1%, and the stimulus-weighted average load directions were within 1 degree. The similarity of these parameters and the natural generic long bone density distributions indicate that the overall magnitude and average load direction are key factors affecting bone adaptation.

Adaptation, Physiological↗

Numerical instabilities in bone remodeling simulations: the advantages of a node-based finite element approach.

Long bone structure occurs in two distinct forms. The bone mass near the joint is primarily found in a distributed, porous trabecular structure, while in the diaphyses a tubular cortical structure is formed. It seems likely that these two observed morphologies come about, at least in part, as a mechanical adaptation to the different mechanical demands in the two regions. Mathematical formulations of this dependency have been proposed, thus facilitating numerical simulations of bone adaptation. Recently two types of discontinuities have been observed in these simulations. The first type (near-field) appears in areas near distributed load application and is characterized by a 'checkerboard' pattern of density wherein adjacent remodeled elements alternate between low and high density. The second type of discontinuity (far-field) appears remote from the load application and is characterized by strut or column-like regions of elements which become fully compact bone while adjacent regions are fully resorbed. In fact, the far-field discontinuity is an accurate representation of bone physiology and morphology since it is consistent with the appearance of cortical bone in the diaphysis. On the other hand, the near-field discontinuity, appears in a region where continuous distributions of intermediate apparent densities (trabecular bone) are expected. This finding may cause some to question whether a single continuum formulation of bone remodeling can predict both discontinuous far-field behavior and continuous near-field behavior. We describe a node-based implementation of current continuum bone remodeling theories which eliminates the spurious near-field discontinuities and preserves the anatomically correct far-field discontinuities, thus indicating that a single biological process may be at work in forming and maintaining both far-field and near-field morphologies.

Algorithms↗

Computational method for determination of bone and joint loads using bone density distributions.

Because bone structure is influenced by mechanical loading during ontogeny, the geometry and density distribution of bones contain information about their loading histories. Based on a mathematical theory relating stress history to bone remodeling, we have developed a method to determine dominant bone loading conditions using an optimization procedure. We applied this load determination method using a simplified two-dimensional bone-end finite element model, for which a standard density distribution had been calculated under a given set of loading conditions. With this density distribution, the optimization procedure was used to determine the original loads from a broad set of many plausible basic load distributions and locations. The optimization procedure adjusted the magnitude of each basic load to achieve the desired tissue level attractor stress stimulus throughout the model. The results show that the density-based bone load determination method yields accurate results for basic test cases and, thus, may have potential for estimating in vivo bone loads for both extant and extinct animals.

Animals↗

Biomechanical evaluation of the Ender's pins, the Harris nail, and the dynamic hip screw for the unstable intertrochanteric fracture.

While intramedullary fixation may have less operative morbidity than sliding plate systems, there also may be a loss of stability and strength of the fixation. In a biomechanical study with simulated unstable intertrochanteric fractures in cadaver femurs, multiple Ender's pins were 18% stronger than the single Harris nail. Compression hip screws were three times stronger than the Harris nail and two and one-half times stronger than Ender's pins. The compression hip screw was five times more rigid than either condylocephalic system.

Biomechanical Phenomena↗

Observations of convergence and uniqueness of node-based bone remodeling simulations.

Some investigators have indicated that mathematical theories and computational models of bone adaptation may not converge and that the density solutions from such simulations are dependent on the initial density distribution. In this study, two-dimensional finite element models were used to investigate the effect of initial density distribution on the final density distribution produced using a node-based bone remodeling simulation. The first model was a generic long bone, and the second was a proximal femur, For each model, we conducted time-dependent, node-based, linear rate-law bone remodeling simulations. Five initial density conditions were used with the generic long bone and three with the proximal femur. Remodeling simulations were performed, and the largest average nodal density differences at the end of the simulations were 0.000010 g/cm3 and 0.000006 g/cm3 for the generic long bone and proximal femur models, respectively. Results illustrate that, for a given set of loads and a given finite element model, the node-based bone adaptation algorithm can yield a unique density distribution. In conjunction with previous studies, this finding suggests that uniqueness of the density solution is dependent on both the mathematical theory and the computational implementation.

Algorithms↗

The role of loading memory in bone adaptation simulations.

The concept that bone responds to a time-averaged value of its current mechanical loading forms the basis for many computational bone adaptation algorithms. Some mathematical formulations have incorporated a quantification of the loading experienced during a single "average" day and thus implicitly assume that bone responds abruptly to changes in its loading history. To better reflect the time delays inherent in bone cell recruitment and activation processes, we included a fading memory of past loading. Implementing an exponentially fading memory with time constants of 5, 20, and 100 days, we simulated bone adaptations to abrupt and gradual changes in mechanical loading. Both an idealized single degree-of-freedom model and a finite element model of the proximal femur were studied. A time constant of 5 days produced time-dependent density changes that were negligibly different from those of the standard approach without memory. Models with higher time constants produced significant transient time lags (up to 8.1% difference) in the predicted short-term (3 months) bone density changes. A time constant of 100 days produced overshoots (by approximately 1%) of the eventual steady-state. All models predicted comparable long-term (after several years) steady-state adaptations. Future experimental analyses will be necessary to better determine appropriate fading memory time constants for bone under various loading conditions.

Adaptation, Physiological↗

The contribution of the ossific nucleus to the structural stiffness of the capital femoral epiphysis: a porcine model for DDH.

The preosseous femoral head is thought to be vulnerable to compressive ischemic injury during the treatment of developmental dysplasia of the hip. The ossific nucleus has been proposed to increase the mechanical strength of the capital femoral epiphysis (CFE) and to decrease the risk of avascular necrosis. Sixty mixed-breed fetal and postgestational femoral head specimens were evaluated for structural stiffness in relation to the size of the ossific nucleus within the CFE. The structural stiffness of the CFE in the porcine model was found to increase exponentially with the size of the ossific nucleus. A finite-element model revealed that the presence of an ossific nucleus occupying 40% of the epiphyseal volume reduced the compressive strain in the region of the posterior-superior branch of the medial circumflex artery by an average of 54%. The results of this study support the hypothesis that the presence of the ossific nucleus may protect the CFE from compressive ischemic injury in the treatment of DDH.

Animals↗

Effects of interference fit screw length on tibial tunnel fixation for anterior cruciate ligament reconstruction.

Graft-tunnel mismatch during arthroscopically assisted anterior cruciate ligament reconstruction using the central-third patellar tendon results in less than 20 mm of bone plug remaining in the tibial tunnel. We decided to evaluate the strength of bone plug fixation using interference fit screws that were less than 20 mm in length. Biomechanical testing was performed on 48 porcine hindquarters using 9-mm diameter interference fit screws that measured 12.5, 15, and 20 mm in length. No significant difference was noted between the different-length screws for insertion torque, divergence, stiffness, displacement, or load to failure. We believe, therefore, that comparable graft fixation can be achieved in the tibial tunnel using 9-mm diameter interference fit screws that are less than 20 mm long, and that these shorter screws may be useful in cases of graft-tunnel mismatch.

Analysis of Variance↗