The priority of the heat production in a muscle twitch

When a muscle has been soaked in a moderately hypertonic solution its mechanical response to a shock is delayed, but its heat production is almost normal and starts considerably earlier than its shortening. After a more hypertonic solution the mechanical response is abolished, but a substantial part of the heat production remains. These effects are rapidly reversed by soaking in a normal isotonic solution. They strengthen the previous conclusion that chemical reactions triggered by a stimulus precede the mechanical response.

The ‘initial’ heat production of a non-medullated nerve ( Maia ) has been reinvestigated with more rapid recording equipment than was previously available. In a single impulse at 0° C a positive heat production was observed averaging about 9 x 10 -6 cal/g nerve: this is rapid and is probably associated with the active phase of the impulse. It is followed by a rather slower heat absorption averaging about 7 x 10 -6 cal/g nerve and lasting for about 300 ms. Previous methods were too slow to do more than record the difference between the two, the ‘net heat’, viz. about 2 x 10 -6 cal/g nerve: this is about one-third greater at 0°C than at 18° C. Maia nerves contain fibres from 20 to 0.3 µ in diameter, and about half the heat is probably derived from fibres less than 3.0 µ . The velocities of impulses in them at 0° C vary from 1.4 to 0.1 m/s, so impulses reach the recording thermojunctions throughout a long interval. Thus the observed course of the heat production is the resultant of positive and negative components in different fibres, and a substantial part of each is masked. The real positive and negative heats, therefore, are substantially greater than those observed: on the most likely estimate of velocity distribution, in a single impulse at 0° C they are about 14 x 10 -6 cal/g and — 12 x 10 -6 cal/g, respectively. Heat production, like ionic interchange, is probably proportional to fibre surface, which in 1 g of Maia nerve is estimated as 10 4 cm 2 . If the fibre surface is taken as 50 Å thick, the heats just calculated, if reckoned per gram of surface material, are 2.8 x 10 -3 cal and — 2.4 x 10 -3 cal, respectively. The former is about the same as the heat produced per gram in a muscle twitch. During the passage of an impulse there is known to be an interchange of Na and K ions between the axoplasm and the outside fluid. When isotonic solutions of NaCl and KCl are mixed there is a production of heat. A substantial part of the heat during an impulse may be derived from the interchange of Na and K. Another part may be associated with chemical reactions occurring in the excitable membrane during the cycle of permeability change accompanying the passage of an impulse. The negative heat production is discussed. It cannot be connected with ‘pumping back’ the Na and K ions; this is a much slower process and anyhow would probably involve a positive heat production. It may be a sign of endothermic chemical reactions, representing a first (anaerobic) stage in recovery, which occur in the surface membrane following the completion of the permeability cycle. The question is considered whether the positive and negative phases of the heat production could be due to the discharge and recharge, during the action potential, of the condenser residing in the excitable membrane. The heats so calculated are of the right order of size, but on present evidence the time relations seem to be quite wrong. The amount of K which escapes per impulse from Maia nerve during slow repetitive stimulation at 0° C was measured. It depends greatly on frequency of stimulation; at ‘zero frequency’ it was about 9 X 10 -8 mole/g x impulse.


The early heat production during the onset of a muscle twitch has been determined with the greatest precision possible for comparison with the mechanical response. When allowance is made for the time taken in propagation the heat is found to start off at its maximum rate. Its rate falls gradually to a constant value, while the muscle continues to shorten uniformly then decreases to zero as shortening draws to an end. The heat occurs in two separate processes, those of activation and shortening respectively. The heat of activation has well started before shortening is detected by ordinary methods. The heat of shortening runs parallel to the shortening. There is no sign of negative heat production at any stage of contraction. If endothermic processes occur they are exactly masked by exothermic ones. The latent period of the activation heat is about 10 msec. at 0°C in frog’s muscle, about 25 msec. in toad’s muscle. These, with an ordinary value of Q10, would correspond at 20°C to about 2 and 5 msec. respectively. Various physical methods are discussed of examining the rapid processes that occur during contraction. Chemical methods are inadequate in speed and sensitivity to give direct evidence of the nature and sequence of events occurring in a twitch. Theoretical con­clusions from experiments on muscle extracts, without critical comparison with the behaviour of living muscle, may lead to confusing results.


1979 ◽  
Vol 80 (1) ◽  
pp. 69-81 ◽  
Author(s):  
R. K. JOSEPHSON ◽  
D. YOUNG

1. Body temperatures during singing were measured in the cicada, Cystosoma saundersii Westwood, both in the field and in tethered animals indoors. 2. The temperature of the sound-producing tymbal muscle rises rapidly during singing to reach a plateau approximately 12°C above ambient. This produces a temperature gradient in the abdominal air sac which surrounds the muscle. When singing stops, the tymbal muscle cools exponentially. 3. Heat production during singing, estimated from the cooling curve, is 4.82 cal min−1 g muscle−1. Generation of the same temperature excess in the air sac by an artificial heat source yields an estimated heat production of 54.4 cal min−1 g muscle−1. This discrepancy may be caused by air mixing in the air sac during singing. 4. As temperature rises, tymbal muscle twitch contractions become faster and stronger. This and heat transfer to the thorax cause changes in the song pattern: a marked decrease in the interval between the two sound pulses produced by a single tymbal buckling and a lesser decrease in the interval between bucklings. The fundamental sound period remains unaltered. These effects are consistent with earlier data on sound production. Note: Present address: Department of Developmental and Cell Biology, University of California, Irvine, California 92717, U.S.A.


1987 ◽  
Vol 112 (1) ◽  
pp. 95-100 ◽  
Author(s):  
I. Lamprecht ◽  
B. Schaarschmidt ◽  
T. Plesser

1950 ◽  
Vol 137 (888) ◽  
pp. 330-331 ◽  

Under extreme loads a stimulated muscle neither shortens nor develops tension. The heat production in a twitch is then rather less than one-half of its value with maximal shortening. Under such conditions the heat of shortening and the mechanical work are nil. The remaining heat, therefore, is heat of activation alone. It is about the same in magnitude and onset as the heat of activation at ordinary lengths.


Author(s):  
Mythravaruni Pullela ◽  
Parag Ravindran

Aging of soft tissues occurs through various mechanisms, which involve biochemical reactions, like glycation, oxidation and calcification of proteins in the extracellular matrix of the soft tissue. Aging leads to changes in the microstructure of the soft tissues which results in changes in its mechanical behavior. In this paper, a mixture theory based model that is thermodynamically consistent and applicable for chemically reacting systems is developed. The tissue (elastin) is modeled as a viscoelastic material. The model is simulated for uni-axial loading to study the effect of chemical reactions occurring in the tissue (elastin) on its mechanical response.


2021 ◽  
Vol 118 (10) ◽  
pp. e2025717118
Author(s):  
Siyu Li ◽  
Daniel A. Matoz-Fernandez ◽  
Aaveg Aggarwal ◽  
Monica Olvera de la Cruz

Patterns and morphology develop in living systems such as embryos in response to chemical signals. To understand and exploit the interplay of chemical reactions with mechanical transformations, chemomechanical polymer systems have been synthesized by attaching chemicals into hydrogels. In this work, we design autonomous responsive elastic shells that undergo morphological changes induced by chemical reactions. We couple the local mechanical response of the gel with the chemical processes on the shell. This causes swelling and deswelling of the gel, generating diverse morphological changes, including periodic oscillations. We further introduce a mechanical instability and observe buckling–unbuckling dynamics with a response time delay. Moreover, we investigate the mechanical feedback on the chemical reaction and demonstrate the dynamic patterns triggered by an initial deformation. We show the chemical characteristics that account for the shell morphology and discuss the future designs for autonomous responsive materials.


2014 ◽  
Vol 06 (03) ◽  
pp. 1450023 ◽  
Author(s):  
A. D. DROZDOV

A model is developed for the mechanical response of hydrogels whose deformation is accompanied by swelling–shrinkage driven by the Belousov–Zhabotinsky reaction. A hydrogel is treated as a compressible network of flexible chains with a time-dependent reference (stress-free) state whose evolution is driven by oxidation of a catalyst pendent to chains. The model involves three components: stress–strain relations for deformation of a polymer network coupled with swelling, kinetic equations for chemical reactions with diffusing species, and relations connecting changes in the reference configuration with concentration of oxidized catalyst. Results of simulation confirm the ability of the model to describe autonomous oscillations of a hydrogel layer under constrained swelling. The effect of material parameters on amplitude and frequency of oscillations is studied numerically. In agreement with the available experimental data, it is shown that amplitude of oscillations decreases and their period increases when (i) elastic modulus of the polymer network grows, (ii) a good solvent is replaced with a poor one, (iii) concentration of a catalyst is reduced, (iv) size of a sample decreases, and (v) diffusivities of solvent and activator grow.


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