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Eur J Appl Physiol (1995) 71:555-557 © Springer-Verlag 1995 S. F u k a s h i r o • M. I t o h • Y. Ichinose • Y. K a w a k a m i T. F u k u n a g a Ultrasonography gives directly but noninvasively elastic characteristic of human tendon in vivo Accepted: 30 August 1995 Abstract. To obtain an insight into tendon elasticity during human movement, a real-time ultrasonography was applied to the contracting tibialis anterior muscle. The insertion point of fascicles onto the aponeurosis was clearly visualized, and its position relative to a fixed marker on the skin moved proximally (/11) according to the increasing dorsiflexion force ( / I F ) with a fixed ankle joint. Notably, t h e / i l - / i F relationship in the tendon was found to be quadratic in nature ( / I F = c/i1 2., c = 1 . 4 8 " 2 . 2 4 , r=0.985--0.992, n-9) as has been reported in the isolated tendon, although the A F - / I 1 curves were slightly underestimated in comparison with the stiffness constant estimated from tendon architecture. This underestimation might be caused by changes in the height of the foot arch with the application of force. Key words: Human tendon elasticity • Ultrasonography • Tibialis anterior muscle • F-L curve Introduction According to Hill's classical model, the skeletal muscletendon complex consists of contractile and series elastic components (CC and SEC, respectively). The SEC demonstrates elastic behavior in most movement patterns and especially when the muscle is activated and simultaneously stretched prior to concentric action (Komi 1984). Although the elastic characteristics of SEC can be observed through t h e / I F - / l l relation, direct measurement of this relation has been impossible. For this reason, these characteristics have been indirectly estimated by special in vivo and in vitro methods (e.g. Huijing 1992; Poussen, et al. 1990). Because the major part of the SEC is located in the tendinuous tissues of a muscle, we can consider some fundamental characteristics of the SEC with regard to tendon (Huijing 1992). The displacement at a certain point in the human tendon can be directly but noninvasively observed in vivo by using ultrasonography (Kawakami, et a1.1993). We can then obtain the delta lengthening of the tendon with the force by measuring the distance traveled by a certain point on the tendon during an isometric contraction with increasing force. The purpose of this study was to determine the /1 F-/11 characteristics in a distal tendon of the human tibialis anterior muscle (TA) by ultrasonography. Methods Subjects were 3 healthy male volunteers (24-31 yr of age, 172-178 cm in body height, 62-73kg in body weight). Informed consent was obtained from each subject before the study began. As shown in Fig. 1, the subject lay supine on a bed and was requested to perform isometric dorsiflexion with gradually increasing force in each trial at three ankle joint angles (90, 105 and 120 deg) by using a special ergometer (MYORET, ASICS, JPN). The ultrasonic image of the TA during contraction was recorded on a videotape synchronized with a clock timer to record time in ms and dorsiflexion torque. The lengthening of the distal tendon of the TA was estimated with ultrasonic apparatus. The ultrasonic apparatus (SSD-2000, ALOKA, JPN) consists of an electronic linear array probe of 7.5MHz wave frequency. The scanning head is coated with a water-soluble transmission gel, which provide acoustic contact without depressing the dermal surface. The transducer was placed perpendicular to the tissue interface and parallel to the tibia located at a point 50% distal in the tibial bone length. The tester visually confirmed the echoes reflected from the aponeurosis and interspaces between fascicles in the TA. Frame-by-frame photos of ultrasonic images recorded on video tape were printed every 25ms onto image recording paper. The lengthening of distal tendon (1) was calculated from the displacement of ' z/' between two consecutive images. After the ultrasonic probe was firmly positioned, a specially-designed placement marker (K) was set between the body and the probe so that K did not move, which was confirmed by VTR. The cross-point (r/) between two echoes; one echo from the deep aponeuroses and the other from fascicles, was easily determined on the ultrasonogram as shown in Fig.l. The echoes have been confirmed to be from the aponeuroses and fascicles through a comparison of ultrasonic measurements with direct measures on cadavers, with a measurement error < 10(Kawakami et al. 1993). Therefore, the displacement (7/) is considered to indicate the lengthening of the distal tendon. Conversely, the torque measured by the ergometer was converted to the force at the distal end of the tibialis anterior muscle, according to the moment arm of TA (Rugg et al. 1990). 556 2a 800 A 90 deg 600- • 105 deg o 120 deg • q Z 400 .<1 200 0 i~Ai i 5 10 15 2b IOOO Estimated 750- 12o\\ . .... / . 120deg ................ 105deg z It- 25 (mm) A l degree 105 90 I 20 500- . . . . . . 90deg :.." ,,, z~- ' /,,5 •" 250- j 0 Torque & Angle 0 , ' I I I 5 10 15 20 Al(rnrn) F i g. 1. Example of an ultrasonic image of the anterior leg at a point 50% distal to the length of tibial bone. The subcutaneous adipose tissue, muscle (TA) and internal aponeurosis are visualized. The cross-point ;q was determined from the echoes of the deep aponeuroses and fascicles. Results and D i s c u s s i o n Fig. 2a shows a typical example of the / 1 F - / l l curves in each trial at three ankle angles. T h e / 1 F - / l l curve at 105 deg of ankle angle is shifted to the left compared to that at 90 deg of ankle angle. Also, a similar shift was observed among 120 and 105 deg in ankle angles. These shifts are probably due to the fact that the initial length of the muscle Fig. 2a: Force-Length relations of human tendon in three angles of ankle joint. 2b: Force-Length relations that were arranged on the length axis based upon the onset of the force generation. The estimated curve was calculated from tendon architecture. fibers would have been stretched by plantarflexion from 90 to 120 deg, but not the tendinuous tissue until acted upon by external and/or internal forces. In order to focus the elastic characteristics of the tendon itself, the three curves were arranged on the length axis based upon the onset of the force generation (Fig. 2b). Each curve in Fig. 2b fitted well to a quadratic regression. The correlation coefficients of these regression curves were high at three joint angles of all subjects (/1F=c/11 2; c=1.48"--2.24, r=0.985"--0.992, n=9). 557 These quadratic characteristics are quite similar to those isolated tendon (Woo 1981). Since the / 1 F - / l l curve in tendon mainly depends upon the cross-sectional area and length of tendon itself (Bobbert, et al. 1986), the stiffness constant and/or the compliance of each tendon is specific to its tissue. Therefore, we can estimate the curve from the tendon architecture that was conventionally used in the biomechanical analysis (Bobbert, et al. 1986). The curve measured in the present study agreed well with but slightly underestimated, the real values. This underestimation may be due to changes in the height of the arch of the foot with the application of force. Fukashiro et al. (1994) reported that the height of foot arch was changed by the external force body weight vector. The elastic characteristics of the SEC have usually been estimated using the following methods. Three methods used in the isolated preparation are: (i) the quick release method; (ii) a method using fast constant velocity releases; (iii) a method calculating compliance from the force-time curve of an isometric tetanic contraction. These methods have been briefly reported by Huijing (1992). Also, the compliance of SEC in elbow flexion was estimated using the quick release method by Poussen, et al. (1990). However, the elastic characteristics of human tendon can be directly but noninvasively measured using the technique presented in this paper. Then, the technique described in the present study would provide a powerful tool in determining in vivo characteristics of human tendon elasticity. It was concluded that the /1F-z~l curve of the human tendon can be directly but noninvasively obtained using the present method. References Bobbert MF, PA Huijing, GA van Ingen Schenau (1986) A model of the human triceps surae muscle-tendon complex applied to jumping. J.Biomech. 19:887-898 Fukashiro S and T Iraha (1994) How to prevent the navicular stress fracture by the increased training quantity i n long distance runner. Bulletin of the Physical Fitness Res Inst, 85:1-5 (in Japanese) Huijing PA (1992) Elastic potential of muscle. Strength and Power in Sport, B lackwell Sci.Pub. 151 - 168 Kawakami Y, T Abe and T Fukunaga (1993) Muscle-fiber pennation angles are greater in hypertrophied than in normal muscles. J Appl Physiol. 74:2740-2744 Komi PV (1984) Physiological and biomechanical correlates of muscle function: Effects of muscle structure and stretchshortening cycle on force and speed. In Terjung ed. Exer Sport Sci Review 12:81-121 Poussen M, JV Hoecke and F Goubel (1990) Changes in elastic characteristics of human muscle induced b y eccentric exercise. J Biomech. 23:343-348 Rugg S G, Gregor R J, Mandelbaum B R, Chiu L (1990) In vivo moment arm calculations at the ankle using magnetic resonance imaging (MRI). J Biomech 23:495-501 Woo SL-Y (1981) The effect of exercise on the biomechanical and biochemical properties of swine digital flexor tendons. J Biomech Engineering, 103:51-56