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Isometric and isovelocity contractile performance of red musle fibres from the dogfish Scyliorhinus canicula

F. Lou1,*, N. A. Curtin1,{dagger} and R. C. Woledge2

1 Biological Structure and Function, Division of Biomedical Sciences, Faculty of Medicine, Sir Alexander Fleming Building, Imperial College of Science, Technology and Medicine, London SW7 2AZ
2 UCL Institute of Human Performance, Royal National Orthopaedic Hospital Trust, Brockley Hill, Stanmore, Middlesex HA7 4LP, UK
* Present address: Department of Biosciences, Faculty of Natural Sciences, University of Hertfordshire, College Lane, Hatfield, Hertfordshire AL10 9AB, UK



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Fig. 4. Sample recordings from the slack test measurements of V0, the unloaded velocity of shortening from a red muscle preparation. (A) Three superimposed recordings of tetanic force before and after the length steps ({Delta}L) shown in B. The fibre bundle was released by different distances from the same starting length. (C) Recordings of force from A shown on expanded scales and with regression lines fitted to the early part of the force redevelopment. The broken vertical lines marks the time of the release. The horizontal arrow marks {Delta}t, the time from the release to the regression intercept for the largest step. This is the time required to take up the slack following the length step. (D) Relationship between step size, {Delta}L, and {Delta}t. The slope of the regression line, 1.503±0.002 L0 s-1 (mean ± S.E.M., N=3), is V0 for this fibre bundle. The intercept on the {Delta}L axis, 0.053±0.0001L0 (mean ± S.E.M. N=3), is an estimate of the compliance of the series elastic component (SEC) of this fibre bundle. L0, the fibre length at which maximum isometric force was produced, was 8.7 mm.

 


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Fig. 7. (A) Example of a stress versus strain relationship for the series elastic component of a red fibre bundle. The points show observations from recordings such as those shown in Fig. 5. Stress is that produced at the end of the step change in length, and strain is the size of the step change in length. The fitted line was calculated as described in the text. Strain, Y, is the sum of a constant, k, a linear component, a(x), and a saturating component, b(x), where x is stress. Y=k+a(x)+b(x), where a(x)=mx; if x<c, then b(x)=nx; if x>=c, then b(x)=nc. The fitted values were k=-0.0498, m=0.0381, n=0.0625 and c=0.186. The total strain (black line) is the sum of k (broken line) and a(x) (red line) and b(x) (green line). (B) Corresponding strain versus stress relationship with points and black line as in A. {Delta}L, length change; L0, fibre length at which maximum isometric force was produced; P0, isometric force before shortening.

 


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Fig. 1. (A) Video image of a transverse cryo-section of a red fibre bundle after staining with Evans Blue. Intact fibres appear grey and damaged fibres pale. (B) Histogram of the numbers of fibres with different cross-sectional areas (CSA). The muscle preparation was the same as that shown in A.

 


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Fig. 2. Relationship between cross-sectional area of intact red fibres expressed as a fraction of total fibre area (intact+damaged) and the area of all fibres. The points are the observed values. The lines were calculated using the following equation on the assumption that damaged fibres were confined at a layer of either one (solid line) or two (broken line) fibres on the surface of the bundle and that the bundle is circular in cross section: l/A=[(4A/{pi})0.5-2d]2{pi}/(4A), where l is the area of intact fibres, A is the area of all fibres (intact+damaged) and d is the thickness of the layer of damaged fibres. The solid line was calculated using d=81.1 µm, which is the median fibre diameter measured here (see text), and the broken line assuming that the damaged layer is two fibres thick, i.e. d=162.2 µm.

 


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Fig. 3. Relationship between maximum tetanic force and cross-sectional area (CSA) of intact fibres in red (filled symbols) and white (open symbols) muscle preparations. Damaged fibres were removed as described in the text before CSA was measured. The slopes of the lines are the mean of the force/CSA values, 142.4±10.3 kN m-2 (N=35) for red fibres and 289.2±8.4 kN m-2 (means ± S.E.M., N=25) for white fibres.

 


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Fig. 5. (A) Three superimposed recordings of active force during tetanic stimulation of a red fibre bundle shortening at different velocities. (B,C) Force and length change ({Delta}L) on an expanded time scale. The horizontal lines in B show the forces that were measured during the period at the start of the ramp shortening when force was relatively constant. L0, the fibre length at which maximum isometric force was produced, was 6.6 mm.

 


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Fig. 6. (A) Summary of the force/velocity results for the seven red fibre bundles (different symbols for different bundles). Force is expressed relative to P0, the isometric force at L0, the fibre length at which maximum isometric force was produced, and velocity is expressed relative to maximum shortening velocity Vmax. Each fibre bundle's values are expressed relative to its own P0 and Vmax. Vmax was found for each fibre bundle by fitting a hyperbola to its force/velocity data as described in the text. The line is the mean of these fitted lines for the seven fibre bundles. (B) The relationship between power and velocity of shortening. The points are the products of the force and velocity values shown in A and the line is the mean of the calculated power curves for the seven fibre bundles. (C) The power for both stretch and shortening. The points are the products of the force and velocity values shown in A. The line for shortening is the same as in B. The line for stretch is a straight line fitted through the points and constrained to pass through the origin.

 


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Fig. 8. (A) Three superimposed recordings of active force during tetanic stimulation of a red fibre bundle with stretch at different velocities. (B,C) Force and length change ({Delta}L) on expanded scales. The horizontal lines in B show the forces that were measured during stretch. Results from the same fibre bundle as in Fig. 5. L0, the fibre length at which maximum isometric force was produced, was 6.6 mm.

 


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Fig. 9. Comparison of the force and power output by intact white (Curtin and Woledge, 1988Go) and red muscle fibres. Black lines (white fibres) and red lines (red fibres) were calculated from Hill's equation using the mean values of the fitted constants in Table 3A (means for seven white fibre preparations and seven red fibre preparations). (A) The relationship between relative force and relative velocity calculated from the following: P'={[B(P*+A)]/(V'+B)}-A, where P' is force expressed relative to P0, the maximum isometric force, V' is velocity expressed relative to Vmax, the maximum velocity of shortening, which is the intercept of the force/velocity curve on the velocity axis. Table 3A includes the values of the constants: for red fibres and 1.19±0.04 for white fibres; A=a/P0=0.269±0.024 for red fibres and 0.274±0.020 for white fibres; B=b/Vmax=0.225±0.024 for red fibres and 0.236±0.022 for white fibres. (B) The relationship between relative power and relative velocity calculated from the following: relative power=P'V', where P' and V' are defined as in A. (C,D) The corresponding relationships with force expressed in units of force per cross-sectional area and velocity expressed in units of L0 s-1, where L0 is the fibre length at which maximum isometric force, P0, was produced.

 





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