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. 2014 Aug;13(4):801-12.
doi: 10.1007/s10237-013-0535-7. Epub 2013 Oct 22.

Dynamic permeability of the lacunar-canalicular system in human cortical bone

Affiliations

Dynamic permeability of the lacunar-canalicular system in human cortical bone

M Benalla et al. Biomech Model Mechanobiol. 2014 Aug.

Abstract

A new method for the experimental determination of the permeability of a small sample of a fluid-saturated hierarchically structured porous material is described and applied to the determination of the lacunar-canalicular permeability [Formula: see text] in bone. The interest in the permeability of the lacunar-canalicular pore system (LCS) is due to the fact that the LCS is considered to be the site of bone mechanotransduction due to the loading-driven fluid flow over cellular structures. The permeability of this space has been estimated to be anywhere from [Formula: see text] to [Formula: see text]. However, the vascular pore system and LCS are intertwined, rendering the permeability of the much smaller-dimensioned LCS challenging to measure. In this study, we report a combined experimental and analytical approach that allowed the accurate determination of the [Formula: see text] to be on the order of [Formula: see text] for human osteonal bone. It was found that the [Formula: see text] has a linear dependence on loading frequency, decreasing at a rate of [Formula: see text]/Hz from 1 to 100 Hz, and using the proposed model, the porosity alone was able to explain 86 % of the [Formula: see text] variability.

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Conflict of interest statement

Conflict of interest All authors state that they have no conflicts of interest.

Figures

Fig. 1
Fig. 1
a The loss tangent (mean ± SD) versus time for a period of 5 h. b The loss tangent (mean ± SD) versus time for a duration of 5 days (* p<0.05, nine loaded osteons in each analysis)
Fig. 2
Fig. 2
Curve fitting of the analytical model and experimental data of the loss tangent to evaluate the average lacunar–canalicular permeability, Krr = (2.34 ± 0.33) × 10−22m2(* p < 0.05, sixty loaded osteons)
Fig. 3
Fig. 3
Lacunar–canalicular permeability versus frequency, Krr = (3.27 − 0.02 f ) × 10−22m2(* p < 0.05, sixty loaded osteons) from inverse poroelastic model of Krr
Fig. 4
Fig. 4
Loss tangent, tan [δ(ω = 2π)], measured at 1 Hz cyclic loading of isolated human osteons versus lacunar–canalicular porosity, φLC (sixty loaded osteons)
Fig. 5
Fig. 5
Lacunar–canalicular permeability in the radial direction of isolated human osteons, Krr, versus lacunar–canalicular porosity, φLC (sixty loaded osteons)

References

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