2.2.1 Load measuring instruments
The load measuring instruments consisted of two steel quadruped frames, each 400 mm high, 350 mm long and 350 mm wide, one with a 20 mm-thick polycarbonate resin top plate on the steel frame and the other with a scale on which the load was measured. The polycarbonate resin tabletop had a cross-hole to allow the ultrasound probe to image from the bottom [23].
In a preliminary experiment measurement of fast movements such as load-extraction movements, would be difficult to observe with ultrasound using the same technique as in the previous study because the PMP and the heel would separate at the time of ground release. Therefore, we created an original water tank using the PMP to enable the measurement of fast movements such as load-unloading movements. A water tank, 90 mm high, 350 mm long, and 155 mm wide, made of 5-mm-thick PMP plates was fixed at the position cut out for the cross-hole in the top panel, and water was filled to a height of 10 mm in the tank. Since the average foot axis angle during walking is considered to be approximately 7 degrees to the sagittal plane, the two evaluation platforms were placed so that they were open 7 degrees to the sagittal plane (Fig. 1).
2.2.2 Loading-unloading movement
The right foot, used as the measurement foot, was placed in the tank so that the second metatarsal and calcaneal ridge aligned with the straight line drawn on the PMP load measuring instrument. The subjects were made to stand shoulder-width apart, and the amount of load applied to the right foot was checked based on the scale readings. To prevent the heel from floating, the subjects were placed at eye level in the standing posture and kept their eyes on the marker during the measurement.
The loading and unloading movements were performed in accordance with previous studies [22]. The subject performed the loading and unloading movements on the PMP load measuring instrument at a frequency of 0.5 Hz on a metronome. The subject started with the toes grounded to a straight line drawn on a PMP tabletop to prevent the load axis from shifting, and the movements were performed three times in succession.
2.2.3 Thickness measurement of heel fat pad using ultrasonic method
The measurements were performed by a person with more than 6 years of experience observing heel fat pads. Measurements were taken using an ultrasound imaging system (ApplioαVerifia, Canon, JPN) with a 10 MHz high-frequency linear probe with the screen inverted vertically. The macrochamber layer was defined as the area from the inferior margin of the calcaneal ridge to the base of the fibroseptum, and the microchamber layer was defined as the area from the base of the fibroseptum to the skin. The macrochamber layer included the plantar tendon membrane, MASs, and fibroseptum, while the microchamber layer included the MICs and skin.
A set of three consecutive loading-unloading movements was performed, and changes in the microchamber and macrochamber layers of the heel fat pad were continuously imaged for a total of 6 seconds. The frame rate of the ultrasound imaging system was set at 30 images/second, which allowed clear observation of the internal structure of the heel fat pad. Six-second imaging was performed because the loading-unloading movements were performed at a frequency of 0.5 Hz, which required 1 second (30 fps) for loading, 1 second (30 fps) for unloading, and 2 seconds (60 fps) for loading-unloading movement. This is because the load was performed three times.
The following three points were identified during each loading movement (60 fps): the point where the heel contacted the PMP (initial contact), the point where the heel reached maximum load (the point where the thickness of the microchamber and macrochamber layers of heel fat pad no longer changed compared to the previous value) (maximal load), and the point where the heel left the PMP plate (unloading). The differences between the microchamber and macrochamber layers were compared. We also extracted 10 images from each of the 30 images measured between initial contact and maximal load and between maximal load and unloading, each of which was a multiple of 3, and evaluated the changes in the loading-unloading processes of the microchamber and macrochamber layers of the heel fat pad for each layer. The thicknesses of the microchamber and macrochamber layers of the heel fat pad between initial contact and maximal load and between maximal load and unloading were calculated, and the (1) amount of thickness change, (2) rate of thickness change, (3) ratio of thickness change of the microchamber and macrochamber layers to the entire heel fat body were calculated (Fig. 2). The calculation formulas are as follows.
Amount of change (mic) = Initial contact (mic) – Maximal load (mic)
or Amount of change (mac) = Initial contact (mac) – Maximal load (mac)・・(1)
Rate of change (mic) = \(\frac{Amount of change \left(mic\right)}{Initial contact \left(mic\right)}\)×100
or Rate of change (mic) = \(\frac{Amount of change \left(mac\right)}{Initial contact \left(mac\right)}\)×100・・(2)
Deformation proportion×100 (mic) = \(\frac{Amount of change \left(mic\right)}{Amount of change \left(mic\right)+Amount of change \left(mac\right)}\)×100
or Deformation proportion×100 (mic) = \(\frac{Amount of change \left(mic\right)}{Amount of change \left(mic\right)+Amount of change \left(mac\right)}\)×100・・(3)
One set of three loading-unloading movements was performed, and the average of the three was used as the measured value in this study.
2.3 Statistical Analysis
Statistical analysis was performed using SPSS software (SPSS Statistics28, IBM, USA). Sample size estimation was performed for each item.
A two-way analysis of variance was performed because normality was assumed after a Shapiro-Wilk test before performing a three-point comparison in the microchamber and macrochamber layers of the heel fat pad. If the test result of the difference in measurements was significant, the Bonferroni method was performed as a posteriori test.
The Shapiro-Wilk test was performed before comparing the loading-unloading processes in the microchamber and macrochamber layers of the heel fat pad at 10% intervals, and since normality was assumed, a corresponding t-test was performed. If the test result of the difference in measurements was significant, the Bonferroni method was performed as a posteriori test.
Before comparing the thickness change of the microchamber and macrochamber layers of the heel fat pad during the loading-unloading processes, the Shapiro-Wilk test was performed, and since normality was assumed, a paired t-test was used.
Pearson's correlation coefficients were used for the association between the thickness of the microchamber and macrochamber layers of heel fat pad and height and weight and the association between the percentage change in thickness of the microchamber and macrochamber layers of heel fat pad and height and weight. Multiple regression analysis was also performed using a stepwise method. The thickness and rate of thickness change of the microchamber and macrochamber layers of the heel fat pad were used as dependent variables, and height and weight were used as independent variables. Correlation results were categorized as follows: [0.00-0.20/-0.00–0.20 (poor correlation) / 0.21–0.40/-0.21–0.40 (fair correlation) / 0.41–0.60/-0.41–0.60 (moderate correlation) / 0.61–0.80/-0.61–0.80 (good correlation)/ 0.81-1.00/-0.81–1.00 (very good correlation)]. The significance level was set at less than 5%.