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L E Ford

Publications and source records attributed to L E Ford.

11 recordsLinked to original sources
PubMed1992

Contribution of damped passive recoil to the measured shortening velocity of skinned rabbit and sheep muscle fibres.

Maximum shortening velocities of skinned fibres from rabbit psoas and sheep extensor digitorum longus muscles were measured by the slack test and by extrapolating force-velocity curves to zero load. Both overall muscle velocity and sarcomere velocity were measured with each method. Maximum sarcomere velocity measured by the slack test was not significantly different from that assessed from the force-velocity curves (p greater than 0.1). Maximum overall muscle velocity measured from the slack test was significantly (p greater than 0.001) and substantially (62% rabbit, 83% sheep) greater than maximum sarcomere velocity. The difference is attributed to damped recoil of the series elastic elements contributing to the overall muscle velocity. The extent and time course of this damped recoil in isotonic steps was assessed from comparisons of overall muscle length and sarcomere length records during isotonic steps. When the records were shifted and scaled so that they superposed during the late stages of isotonic shortening, there was a substantial difference between the early parts of the records. This difference was reduced by about half in association with the step and the remaining half declined at a diminishing rate following the step, lasting longer with lower loads. This result is explained by about half of the series elastic element behaving as a viscoelastic element and half being undamped. With steps to the lowest isotonic loads, which averaged 6.7% of isometric force in sheep and 9.5% in rabbit, the total series elastic element recoil (both damped and undamped) averaged 3.4% and 2.7% of fibre segment length, respectively, in sheep and rabbit. The rapid series elastic element recoil at zero load, assessed from the slack test, was approximately 50% higher, indicating a substantial series compliance at low forces. The contribution of an additional, longer lasting, damped series elastic element recoil to the overall muscle velocity can explain the greater maximum velocity that is frequently found with the slack test.

Animals↗
PubMed1992

Changes in valvular resistance, power dissipation and myocardial reserve with aortic valvuloplasty.

Balloon aortic valvuloplasty results in small changes in valve area with great symptomatic improvement in some patients, while others have little relief with greater increases in valve area. Alternative indices to valve area may help explain this clinical discrepancy. A calculation of valve area does not provide a means of assessing the load imposed by a stenotic valve, while the complementary index valve resistance, defined as the quotient of mean pressure difference divided by flow, allows many other hemodynamic calculations and may provide an additional measure of the hemodynamic importance of valvular obstructions. To assess the value of these calculations, we studied hemodynamic changes in thirty elderly patients undergoing valvuloplasty for aortic stenosis. The valve area, as calculated by the Gorlin formula, increased by an average 67% (0.59 cm2 to 0.95 cm2), while hemodynamic resistance decreased by an average 52% (453 to 207 dyne.sec.cm5). The values of resistance were used to predict pressure gradients and work loads at different cardiac outputs. The increase in myocardial reserve with valvuloplasty was calculated as the increase in cardiac output that could be achieved at the pre-valvuloplasty value of either total ventricular pressure or ventricular work. These calculations assumed that valvular resistance did not change with cardiac output and that peripheral resistance varied inversely to cardiac output so as to maintain a constant aortic (systemic) pressure. The increase in myocardial reserve was 18% when ventricular work rate was the limiting factor, and 103% when pressure was limiting. The increase in reserve may be closer to the higher value since the myocardial work rate is probably not limited by myocardial energy in the absence of coronary artery disease. Four patients who did not do well clinically were characterized by small increases in reserve, either because of inadequate dilatation of the valve or because the original stenosis was not severe. Valve resistance, myocardial reserve, and ventricular work may be calculated using standard hemodynamic measurements. In conjunction with aortic valve area, these indices provide significant complimentary information and may further elucidate the hemodynamic consequences of valvular obstruction.

Aged↗
PubMed1991

Effect of osmotic compression on the force-velocity properties of glycerinated rabbit skeletal muscle cells.

The force-velocity relations of single glycerinated rabbit psoas muscle fibers at 5 degrees C were studied at maximum and half-maximum activation in the presence of 0 (control) and 39-145 g/liter dextran T-70. Resting fiber diameter decreased progressively to approximately 70% of the nondextran control as the dextran concentration was increased. Isometric force at full activation increased to a maximum of 136% of control at 111 g/liter dextran and then fell to 80% of control in 145 g/liter dextran. Maximum velocity, which fell to 49% of the control value in the highest concentration of dextran, was nearly constant at approximately 65% control over the range of 58-111 g/liter dextran. Relative maximum power, which gives an estimate of changes in intermediate velocity, was not significantly reduced by dextran concentrations up to 76 g/liter, but then fell progressively to 62% of control in the highest concentration of dextran. At half-maximum activation, maximum velocity and relative maximum power were not significantly different from the values at full activation. The results obtained at partial activation indicate that the decline of velocity seen in the presence of dextran is not due to a passive internal load and that the dextran does not cause a viscous resistance to shortening. The increased velocity in the absence of dextran can be explained by the reduced ability of cross-bridges to resist shortening, as proposed by Goldman (1987. Biophys. J. 51:57).

Animals↗
PubMed1991

Shortening velocity and power output of skinned muscle fibers from mammals having a 25,000-fold range of body mass.

The shortening velocities of single, skinned, fast and slow skeletal muscle fibers were measured at 5-6 degrees C in five animal species having a 25,000-fold range of body size (mouse, rat, rabbit, sheep, and cow). While fiber diameter and isometric force showed no dependence on animal body size, maximum shortening velocity in both fast and slow fibers and maximum power output in fast fibers were found to vary with the -1/8 power of body size. Maximum power output in slow fibers showed a slightly greater (-1/5 power) dependence on body size. The isometric force produced by the fibers was correlated (r = 0.74) inversely with fiber diameter. For all sizes of animal the average maximum velocity was 1.7 times faster in fast fibers than in slow fibers. The large difference in mechanical properties found between fibers from large and small animals suggests that properties of the contractile proteins vary in a systematic manner with the body size. These size-dependent changes can be used to study the correlations of structure and function of these proteins. Experimental results also suggest that the different metabolic rates observed in different sizes of animals could be accounted for, at least in part, by the difference in the properties of the contractile proteins.

Animals↗
PubMed1991

Effects of hypoxia and hypercapnia on the force-velocity relation of rabbit myocardium.

The separate effects of hypoxia and hypercapnia on the force-velocity relation of rabbit myocardium were compared in 10 papillary or trabecular muscles superfused using control (95% O2-5% CO2), hypoxic (18% O2), and hypercapnic (20% CO2) physiological salt solutions. This level of hypoxia did not irreversibly damage the muscles and reduced peak isometric force by 53 +/- 11%. The level of hypercapnia was chosen to match the force depression (50 +/- 12%) produced by hypoxia. Multiple force-velocity points were measured by applying critically damped isotonic force steps at 90% of the time to peak isometric force and at the time to 50% peak isometric force. These points defined the force-velocity relation and maximum velocity of shortening, the extrapolated isometric force, and the maximum power of nonpotentiated and postextrasytolic potentiated contractions. Hypoxia and hypercapnia reduced maximum force and maximum power nearly equally. Maximum velocity of shortening decreased more during hypoxia (21 +/- 12%) than during hypercapnia (12 +/- 9%) (p less than 0.01). Postextrasystolic potentiation completely reversed the reduction of maximum velocity of shortening during hypercapnia but not during hypoxia. A 6% internal load could account for the reduction in maximum velocity of shortening during hypercapnia and all but 9% of the reduction in maximum velocity of shortening during hypoxia. The relative time course of the force-velocity relation was not altered by either hypoxia or hypercapnia. We conclude that hypercapnia reduces the effect of activation because increased activation (by postextrasystolic potentiation) restored the force-velocity relation and maximum velocity of shortening to control values.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1978

A piezoelectric force transducer for single muscle cells.

A cantilevered piezoelectric force transducer is described. The cantilevered element has a 6-mm glass extension that can be projected into a horizontal muscle bath from above. By adjusting the length of the piezoelectric bar from 1 to 4 mm, the sensitivity of the device can be varied between 25 and 100 mV/mN (0.25--1.0 mV/mg) with its resonant frequency varying inversely between 8 and 15 kHz. Although moderately fragile, the sensing elements are inexpensive and easily made. The output of the sensing element is amplified by a small, unity-gain, high-input-resistance amplifier mounted on a support block with the element. Although the arrangement does not provide a DC output, its time constant of over 500 s is sufficiently long for measuring tension during muscle contractions lasting 1--2 s.

Muscle Contraction↗
PubMed1977

Tension responses to sudden length change in stimulated frog muscle fibres near slack length.

1. Apparatus for applying a step change of length to an isolated muscle fibre is described. The step was complete in about 0.2 ms.2. Effects of tendon compliance were eliminated by using a spot-follower device and by gripping the tendons with metal clips close to the fibre ends.3. The natural frequency of the force transducer was above 10 kHz.4. Steps of various amplitudes and in either direction were applied to isolated muscle fibres about 6 mm long from the anterior tibial muscle of Rana temporaria during tetanic stimulation. Initial sarcomere length was 2.0-2.2 mum, and temperature was 0-3 degrees C.5. The tension response to a step could be divided into four phases. The initial response was an apparently elastic change during the step itself (phase 1). After the step was completed there was a rapid partial recovery towards the original tension (phase 2, lasting 2-5 ms), followed by a slowing or reversal of recovery (phase 3, 10-50 ms), and finally a much slower return to the original tension (phase 4). Most of this paper is concerned with phases 1 and 2.6. The initial tension change (phase 1) occurred synchronously with the applied length change, indicating that the fibres possess a compliance which is almost linear and almost undamped. Its stiffness is such that an instantaneous shortening of about 4 nm per half-sarcomere would bring the tension to zero from its isometric value.7. The absence of detectable damping during phase 1 indicates that the viscosity of a stimulated fibre is substantially less than the apparent viscosity of a fibre at rest.8. The instantaneous force-extension curve approached the length axis at a sharp angle and a negative tension appeared at the force transducer when a very large step was applied. These observations suggest that the structures responsible for the stiffness of the fibre remain rigid when they are not under tension.9. During the few milliseconds after the step (phase 2) the tension recovered part of the way toward the level which existed before the step. In shortening steps the time course of this recovery was adequately fitted by the sum of four exponential terms, and was similar in steps of different amplitude but with a time scale shorter the larger the step. In stretches the slow components were relatively larger than in releases.10. The tension level, T(2), approached during phase 2 depended only on the total amplitude of the step and not on the time course of the length change, provided it was complete in 1-2 ms. The extreme tension reached during a step could thus vary widely without detectable change in T(2).11. With stretches and releases of up to about 3 nm per half-sarcomere this early recovery was almost complete, so that the curve of T(2) against step amplitude was nearly horizontal. With larger releases the line curved downwards, reaching zero in a release of about 14 nm per half-sarcomere.12. When the temperature was raised both the developed tension and the stiffness increased, but the relative increase was greater for tension than for stiffness. The amount of instantaneous shortening needed to bring tension to zero was therefore also increased.13. A set of empirical equations is given which describe adequately the first few milliseconds of the tension change in response to any imposed time course of shortening.14. The rapid elasticity and early tension recovery resemble the response of a combination of two elastic components and one viscous component. Reasons are given for preferring an interpretation in terms of an undamped compliance in series with a damped compliance (Voigt element) rather than an undamped elasticity in parallel with a series combination of viscous and elastic components (Maxwell element).15. The rapid compliance does not correspond to the ;series elastic component' of two-component theories of muscle contraction.

Animals↗
PubMed1976

Heart size.

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Animals↗