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This article is part of the supplement: Proceedings of the Australasian Podiatry Council Conference 2011

Open Access Invited speaker presentation

The heel fat pad: mechanical properties and clinical applications

Scott C Wearing12* and James E Smeathers3

Author Affiliations

1 Faculty of Health Sciences and Medicine, Bond University, Gold Coast, Qld, 4229, Australia

2 Centre of Excellence for Applied Sports Science Research, Queensland Academy Sport, Nathan, Qld, 4111, Australia

3 Institute of Health and Biomedical Innovation, Queensland University of Technology, Brisbane, Qld, 4059, Australia

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Journal of Foot and Ankle Research 2011, 4(Suppl 1):I14  doi:10.1186/1757-1146-4-S1-I14


The electronic version of this article is the complete one and can be found online at: http://www.jfootankleres.com/content/4/S1/I14


Published:20 May 2011

© 2011 Wearing and Smeathers; licensee BioMed Central Ltd.

This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Invited speaker presentation

The human heel pad is a highly specialised fibroadipose tissue that is hierarchically structured to dissipate the stress associated with weight–bearing activities. While the properties of the heel pad, as a whole, are believed to reflect those of the collagen– and elastin–rich septa which envelope adipocytes and confine their movement, the scientific literature provides little consensus on the properties of healthy heel pads. Experiments conducted in vitro typically yield stiffness and loss properties that differ by an order of magnitude to those performed in vivo. Such differences may, in part, reflect the difficulty in measuring heel pad mechanics in vivo. This paper reports the findings of a novel series of experiments in which a digital fluoroscope, synchronised with a pressure platform, was used to obtain force–deformation data of the heel pad during gait. Transient loading profiles associated with walking were observed to induce rapidly changing deformation rates in the heel pad and resulted in irregular load–deformation curves. Initial stiffness (32 N.mm-1) of the heel pad was an order of magnitude lower than its final stiffness (212 N.mm-1), which, in turn, was similar to that reported for cadaveric heel pads (296 N.mm-1) when impacted at comparable energies of 1.45 J. While the energy dissipating ratio of the heel pad (0.66 ± 0.12) fell between those commonly cited for mechanical tests of cadaveric heels and impact loading in vivo, peak deformation of the fat pad (10.3 mm) approached that predicted for the limit of pain tolerance (10.7 mm), suggesting that the heel pad operates near its physiological maximum, even at the relatively modest speeds encountered during walking. In plantar heel pain, the elastic properties of the heel pad remained unaltered. However, energy loss within the tissue was reduced in symptomatic limbs and was also correlated with the sonographic thickness of the plantar fascial enthesis. These findings suggest that viscosity, rather than elasticity, of the heel fat pad may play an important role in the severity of heel pain and provides a previously unidentified link between the mechanical behaviour of the plantar fat pad and plantar heel pain.