The influence of heel pad confinement on heel pad mechanical properties

2021 ◽  
pp. 1-9
Author(s):  
Dan J. Gales ◽  
Samantha L. Winter ◽  
John H. Challis
1995 ◽  
Vol 28 (11) ◽  
pp. 1299-1308 ◽  
Author(s):  
P. Aerts ◽  
R.F Ker ◽  
D. De Clercq ◽  
D.W. Ilsley ◽  
R.McN. Alexander

2000 ◽  
Vol 17 (12) ◽  
pp. 854-859 ◽  
Author(s):  
T. -C. Hsu ◽  
C. -L. Wang ◽  
Y. -W. Shau ◽  
F. -T. Tang ◽  
K. -L. Li ◽  
...  

2017 ◽  
Vol 53 ◽  
pp. 191-195 ◽  
Author(s):  
Che-Yu Lin ◽  
Pei-Yu Chen ◽  
Yio-Wha Shau ◽  
Hao-Chih Tai ◽  
Chung-Li Wang

1998 ◽  
Vol 79 (9) ◽  
pp. 1101-1104 ◽  
Author(s):  
Tsz-Ching Hsu ◽  
Chung-Li Wang ◽  
Wen-Chung Tsai ◽  
Jung-Kun Kuo ◽  
Fuk-Tan Tang

2017 ◽  
Vol 38 (7) ◽  
pp. 779-784 ◽  
Author(s):  
Serkan Taş ◽  
Nilgün Bek ◽  
Mehmet Ruhi Onur ◽  
Feza Korkusuz

Background: Musculoskeletal foot disorders have a high incidence among overweight and obese individuals. One of the important factors causing this high incidence may be plantar fascia and heel pad (HP)–related mechanical changes occurring in these individuals. The aim of the present study was to investigate the plantar fascia and HP stiffness and thickness parameters in overweight and obese individuals and compare these values with those of normal-weight individuals. Methods: This study was carried out in 87 (52 female, 35 male) healthy sedentary individuals between the ages of 19 and 58 years (34 ± 11 years). Participants were subsequently categorized according to body mass index (BMI) as normal weight (18.5 kg/m2 < BMI < 25 kg/m2) or overweight and obese (BMI ≥25 kg/m2). Plantar fascia and HP thickness and stiffness were measured with an ultrasonography device using a linear ultrasonography probe. Results: Overweight and obese individuals had higher HP thickness ( P < .001), plantar fascia thickness ( P = .001), heel pad microchamber layer (MIC) stiffness ( P < .001), and heel pad macrochamber layer (MAC) stiffness ( P < .001), whereas they had lower plantar fascia stiffness ( P < .001) compared with the individuals with normal weight. BMI had a moderate correlation with HP thickness ( P < .001, r = 0.500), plantar fascia thickness ( P = .001, r = 0.536), MIC stiffness ( P < .001, r = 0.496), and MAC stiffness ( P < .001, r = 0.425). A negative and moderate correlation was found between BMI and plantar fascia stiffness ( P < .001, r = –0.439). Conclusion: Increased BMI causes a decrease in the stiffness of plantar fascia and an increase in the thickness of the plantar fascia as well as the thickness and stiffness of HP. Increased body mass could cause changes in the mechanical properties of HP and plantar fascia. Level of Evidence: Level 3, comparative study.


1999 ◽  
Vol 20 (10) ◽  
pp. 663-668 ◽  
Author(s):  
Wen-Chung Tsai ◽  
Chung-Li Wang ◽  
Tsz-Ching Hsu ◽  
Fon-Jou Hsieh ◽  
Fuk-Tan Tang

2017 ◽  
Vol 43 ◽  
pp. S89-S90 ◽  
Author(s):  
Chung-Li Wang ◽  
Che-Yu Lin ◽  
Pei-Yu Chen ◽  
Yio-Wha Shau ◽  
Hao-chih Tai

1996 ◽  
Vol 199 (7) ◽  
pp. 1501-1508 ◽  
Author(s):  
R F Ker

Previous measurements of the mechanical properties of the heel pad, especially of the energy loss during a cycle of compressive loading and unloading, have given contrasting values according to whether the investigators used isolated single impacts (e.g. pendulum tests; energy loss approximately 48%) or continuous oscillations (energy loss approximately 30%). To investigate this discrepancy, rest periods were inserted between single compressive cycles, giving intermittent loading as in locomotion. The energy loss, measured as the percentage area of the hysteresis loop, was found to change linearly with the logarithm of the rest time. It was approximately 33% when the rest time was 1 s. Each 10-fold increase in the rest time added approximately 3.7% to the energy loss. Thus, with rest times appropriate to locomotion, the pad is far from fully relaxed. The springy heel pad may help to reposition the foot during the transfer of load from the heel to the forefoot. Information is also included on the load-deformation curves for the heel pad and the way in which these change with rest time. This is presented as equations which may be useful in future models relating the mechanical properties of the heel to either its structure or its function.


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