Plasticity in smooth muscle, a hypothesis

1994 ◽  
Vol 72 (11) ◽  
pp. 1320-1324 ◽  
Author(s):  
Lincoln E. Ford ◽  
Chun Y. Seow ◽  
Victor R. Pratusevich
Keyword(s):  
Smooth Muscle ◽  
Preliminary Finding ◽  
Muscle Length ◽  
Shortening Velocity ◽  
Thin Filaments ◽  
Thick Filaments ◽  
Initial Hypothesis ◽  
In Series ◽  
Cross Bridges ◽  
Muscle Myosin

The controversial finding that the thick filaments of smooth muscle can be evanescent leads to the hypothesis that the large functional range of this muscle is accommodated by plastic rearrangements that place more thick filaments in series at longer lengths. Our preliminary finding that the shortening velocity and compliance of dog tracheal muscle were strongly dependent on adapted muscle length, while force was much less length dependent, supports this hypothesis (V.R. Pratusevich, C.Y. Seow, and L.E. Ford. Biophys. J. 66: A139, 1994). The hypothesis leads to two further corollaries. The first is that the lengthening of the thick filaments that must accompany their reformation will cause a series to parallel transition: fewer long filaments span the muscle length, but the longer filaments have more cross bridges acting in parallel. The second is that there is more than one activating mechanism in smooth muscle. It is known that myosin light chain phosphorylation activates the actomyosin ATPase, but this same phosphorylation also causes a structural change that facilitates filament formation. The consideration that the unaggregated, phosphorylated myosin must be prevented from competing with myosin in thick filaments and hydrolyzing ATP suggests that there must be a second mechanism that must allow the thin filaments to interact selectively with filamentous myosin. This need for a second activating mechanism may explain the presence of tropomyosin, calponin, and caldesmon on thin filaments. Although the two corollaries follow from the initial hypothesis, it should be emphasized that the three are not mutually dependent, and that the proof or disproof of any one of them would not prove or disprove the others.Key words: smooth muscle, myosin, thick filaments, contraction.

scholarly journals LOCALIZATION OF MYOSIN FILAMENTS IN SMOOTH MUSCLE

1968 ◽  
Vol 37 (1) ◽  
pp. 105-116 ◽  
Author(s):  
Robert E. Kelly ◽  
Robert V. Rice
Keyword(s):  
Smooth Muscle ◽  
Cross Section ◽  
Striated Muscle ◽  
Thick Filament ◽  
Longitudinal Axis ◽  
Thin Filaments ◽  
Chicken Gizzard ◽  
Thick Filaments ◽  
Myosin Filaments ◽  
Muscle Myosin

Thick myosin filaments, in addition to actin filaments, were found in sections of glycerinated chicken gizzard smooth muscle when fixed at a pH below 6.6. The thick filaments were often grouped into bundles and run in the longitudinal axis of the smooth muscle cell. Each thick filament was surrounded by a number of thin filaments, giving the filament arrangement a rosette appearance in cross-section. The exact ratio of thick filaments to thin filaments could not be determined since most arrays were not so regular as those commonly found in striated muscle. Some rosettes had seven or eight thin filaments surrounding a single thick filament. Homogenates of smooth muscle of chicken gizzard also showed both thick and thin filaments when the isolation was carried out at a pH below 6.6, but only thin filaments were found at pH 7.4. No Z or M lines were observed in chicken gizzard muscle containing both thick and thin filaments. The lack of these organizing structures may allow smooth muscle myosin to disaggregate readily at pH 7.4.

Models of contractile units and their assembly in smooth muscle

2005 ◽  
Vol 83 (10) ◽  
pp. 825-831 ◽  
Author(s):  
Farah Ali ◽  
Peter D Paré ◽  
Chun Y Seow
Keyword(s):  
Smooth Muscle ◽  
Striated Muscle ◽  
Dense Body ◽  
Unit Length ◽  
Muscle Length ◽  
Thick Filament ◽  
Contractile Apparatus ◽  
Thin Filaments ◽  
Dense Bodies ◽  
In Series

It is believed that the contractile filaments in smooth muscle are organized into arrays of contractile units (similar to the sarcomeric structure in striated muscle), and that such an organization is crucial for transforming the mechanical activities of actomyosin interaction into cell shortening and force generation. Details of the filament organization, however, are still poorly understood. Several models of contractile filament architecture are discussed here. To account for the linear relationship observed between the force generated by a smooth muscle and the muscle length at the plateau of an isotonic contraction, a model of contractile unit is proposed. The model consists of 2 dense bodies with actin (thin) filaments attached, and a myosin (thick) filament lying between the parallel thin filaments. In addition, the thick filament is assumed to span the whole contractile unit length, from dense body to dense body, so that when the contractile unit shortens, the amount of overlap between the thick and thin filaments (i.e., the distance between the dense bodies) decreases in exact proportion to the amount of shortening. Assembly of the contractile units into functional contractile apparatus is assumed to involve a group of cells that form a mechanical syncytium. The contractile apparatus is assumed malleable in that the number of contractile units in series and in parallel can be altered to accommodate strains on the muscle and to maintain the muscle's optimal mechanical function.Key words: contraction model, ultrastructure, length adaptation, plasticity.

scholarly journals Could an increase in airway smooth muscle shortening velocity cause airway hyperresponsiveness?

2011 ◽  
Vol 300 (1) ◽  
pp. L121-L131 ◽  
Author(s):  
Sharon R. Bullimore ◽  
Sana Siddiqui ◽  
Graham M. Donovan ◽  
James G. Martin ◽  
James Sneyd ◽  
...  
Keyword(s):  
Smooth Muscle ◽  
Airway Smooth Muscle ◽  
Airway Hyperresponsiveness ◽  
Isometric Force ◽  
Muscle Length ◽  
Shortening Velocity ◽  
Bridge Model ◽  
Generating Capacity ◽  
Cross Bridges

Airway hyperresponsiveness (AHR) is a characteristic feature of asthma. It has been proposed that an increase in the shortening velocity of airway smooth muscle (ASM) could contribute to AHR. To address this possibility, we tested whether an increase in the isotonic shortening velocity of ASM is associated with an increase in the rate and total amount of shortening when ASM is subjected to an oscillating load, as occurs during breathing. Experiments were performed in vitro using 27 rat tracheal ASM strips supramaximally stimulated with methacholine. Isotonic velocity at 20% isometric force (Fiso) was measured, and then the load on the muscle was varied sinusoidally (0.33 ± 0.25 Fiso, 1.2 Hz) for 20 min, while muscle length was measured. A large amplitude oscillation was applied every 4 min to simulate a deep breath. We found that: 1) ASM strips with a higher isotonic velocity shortened more quickly during the force oscillations, both initially ( P < 0.001) and after the simulated deep breaths ( P = 0.002); 2) ASM strips with a higher isotonic velocity exhibited a greater total shortening during the force oscillation protocol ( P < 0.005); and 3) the effect of an increase in isotonic velocity was at least comparable in magnitude to the effect of a proportional increase in ASM force-generating capacity. A cross-bridge model showed that an increase in the total amount of shortening with increased isotonic velocity could be explained by a change in either the cycling rate of phosphorylated cross bridges or the rate of myosin light chain phosphorylation. We conclude that, if asthma involves an increase in ASM velocity, this could be an important factor in the associated AHR.

Regulation of shortening velocity by cross-bridge phosphorylation in smooth muscle

1988 ◽  
Vol 255 (1) ◽  
pp. C86-C94 ◽  
Author(s):  
C. M. Hai ◽  
R. A. Murphy
Keyword(s):  
Smooth Muscle ◽  
Shortening Velocity ◽  
Internal Load ◽  
Cross Bridge ◽  
Bridge Model ◽  
The Family ◽  
Cross Bridges ◽  
Latch State ◽  
The Relationship ◽  
State Stress

We have proposed a model that incorporates a dephosphorylated "latch bridge" to explain the mechanics and energetics of smooth muscle. Cross-bridge phosphorylation is proposed as a prerequisite for cross-bridge attachment and rapid cycling. Features of the model are 1) myosin light chain kinase and phosphatase can act on both free and attached cross bridges, 2) dephosphorylation of an attached phosphorylated cross bridge produces a noncycling "latch bridge," and 3) latch bridges have a slow detachment rate. This model quantitatively predicts the latch state: stress maintenance with reduced phosphorylation, cross-bridge cycling rates, and ATP consumption. In this study, we adapted A. F. Huxley's formulation of crossbridge cycling (A. F. Huxley, Progr. Biophys. Mol. Biol. 7: 255-318, 1957) to the latch-bridge model to predict the relationship between isotonic shortening velocity and phosphorylation. The model successfully predicted the linear dependence of maximum shortening velocity at zero external load (V0) on phosphorylation, as well as the family of stress-velocity curves determined at different times during a contraction when phosphorylation values varied. The model implies that it is unnecessary to invoke an internal load or multiple regulatory mechanisms to explain regulation of V0 in smooth muscle.

scholarly journals Expression of smooth muscle myosin heavy chains and unloaded shortening in single smooth muscle cells

1997 ◽  
Vol 273 (4) ◽  
pp. C1259-C1266 ◽  
Author(s):  
Daniel P. Meer ◽  
Thomas J. Eddinger
Keyword(s):  
Smooth Muscle ◽  
Smooth Muscle Cells ◽  
Polymerase Chain Reaction Amplification ◽  
Mrna Level ◽  
Muscle Cells ◽  
Smooth Muscle Myosin ◽  
Minimum Length ◽  
Shortening Velocity ◽  
Variable Expression ◽  
Muscle Myosin

The functional significance of the variable expression of the smooth muscle myosin heavy chain (SM-MHC) tail isoforms, SM1 and SM2, was examined at the mRNA level (which correlates with the protein level) in individual permeabilized rabbit arterial smooth muscle cells (SMCs). The length of untethered single permeabilized SMCs was monitored during unloaded shortening in response to increased Ca2+ (pCa 6.0), histamine (1 μM), and phenylephrine (1 μM). Subsequent to contraction, the relative expression of SM1 and SM2 mRNAs from the same individual SMCs was determined by reverse transcription-polymerase chain reaction amplification and densitometric analysis. Correlational analyses between the SM2-to-SM1 ratio and unloaded shortening in saponin- and α-toxin-permeabilized SMCs ( n = 28) reveal no significant relationship between the SM-MHC tail isoform ratio and unloaded shortening velocity. The best correlations between SM2/SM1 and the contraction characteristics of untethered vascular SMCs were with the minimum length attained following contraction ( n = 20 and r = 0.72 for α-toxin, n = 8 and r = 0.78 for saponin). These results suggest that the primary effect of variable expression of the SM1 and SM2 SM-MHC tail isoforms is on the cell final length and not on shortening velocity.

Velocity-length-time relations in canine tracheal smooth muscle

1988 ◽  
Vol 64 (5) ◽  
pp. 2053-2057 ◽  
Author(s):  
C. Y. Seow ◽  
N. L. Stephens
Keyword(s):  
Smooth Muscle ◽  
Goodness Of Fit ◽  
Time Course ◽  
Muscle Length ◽  
Tracheal Smooth Muscle ◽  
Minimum Length ◽  
Shortening Velocity ◽  
Contracting Muscle ◽  
Parabolic Function ◽  
The Moment

Zero-load velocity (V0) as a function of the length of canine tracheal smooth muscle was obtained by applying zero-load clamps to isotonically contracting muscle under various loads. The load clamps were applied at a specific time after onset of contraction. The magnitude of the isotonic load therefore determines the length of the muscle at the moment of release or at the moment the unloaded shortening velocity was measured. A family of such V0-muscle length (L) curves was obtained at 1-s intervals in the time course of contraction. The V0-L curve was fitted by a parabolic function with satisfactory goodness of fit. The maximum shortening velocity at optimum muscle length varied with time, but the minimum length at which V0 diminished to zero was time independent.

scholarly journals Series-to-parallel transition in the filament lattice of airway smooth muscle

2000 ◽  
Vol 89 (3) ◽  
pp. 869-876 ◽  
Author(s):  
Chun Y. Seow ◽  
Victor R. Pratusevich ◽  
Lincoln E. Ford
Keyword(s):  
Smooth Muscle ◽  
Airway Smooth Muscle ◽  
Muscle Length ◽  
Thick Filament ◽  
Cycling Rate ◽  
Cross Bridge ◽  
Parallel Change ◽  
Force Velocity ◽  
Cross Bridges ◽  
Trachealis Muscle

Force-velocity curves measured at different times during tetani of sheep trachealis muscle were analyzed to assess whether velocity slowing could be explained by thick-filament lengthening. Such lengthening increases force by placing more cross bridges in parallel on longer filaments and decreases velocity by reducing the number of filaments spanning muscle length. From 2 s after the onset of stimulation, when force had achieved 42% of it final value, to 28 s, when force had been at its tetanic plateau for ∼15 s, velocity decreases were exactly matched by force increases when force was adjusted for changes in activation, as assessed from the maximum power value in the force-velocity curves. A twofold change in velocity could be quantitatively explained by a series-to-parallel change in the filament lattice without any need to postulate a change in cross-bridge cycling rate.

Vanadate oxidation activates contraction in skinned smooth muscle without myosin light chain phosphorylation

1997 ◽  
Vol 272 (1) ◽  
pp. C278-C288 ◽  
Author(s):  
M. J. Lalli ◽  
K. Obara ◽  
R. J. Paul
Keyword(s):  
Smooth Muscle ◽  
Light Chain ◽  
Muscle Activation ◽  
Isometric Force ◽  
Total Force ◽  
Shortening Velocity ◽  
Irreversible Damage ◽  
Initial Control ◽  
High Concentrations ◽  
Cross Bridges

Phosphorylation of the myosin regulatory light chain (LC20-P1) is the major route of smooth muscle activation. However, after prior exposure to vanadate, permeabilized guinea pig taenia coli smooth muscle contracts in the absence of LC20-P1. We characterized the vanadate-induced contraction and investigated the mechanism of this novel activation pathway. Addition of vanadate to a control contracture (6.6 microM Ca2+) inhibits force (effective dose for 50% response was approximately 100 microM). In contrast, preincubation with high concentrations of vanadate (threshold at 1-2 mM) elicited a contraction on subsequent transfer of the fiber to a vanadate-free, Ca(2+)-free solution. Maximum isometric force of approximately 60% of control was obtained in fibers preincubated in 4 mM vanadate for 10 min. Addition of Ca2+ to a vanadate-induced contracture increased force, but the total force never exceeded the initial control. After maximal thiophosphorylation of LC20 with adenosine 5'-O-(3-thiotriphosphate), treatment with vanadate did not increase force. Unloaded shortening velocity (Vmax) was similar in Ca2+ and vanadate contractures and was additive. After thiophosphorylation, preincubation in vanadate had no effect on Vmax, suggesting that vanadate affected the number of activated bridges and not cycle rate. Vanadate mechanisms likely involve oxidation, since preincubation with 4 mM vanadate and 25 mM dithiothreitol (DTT) did not produce force. DTT could reverse a vanadate-induced contracture in 30-60 min. Subsequently, fibers demonstrated control contraction/relaxation cycles. Thus vanadate treatment did not cause irreversible damage, such as the extraction of proteins. Potential oxidation sites are proteins at 17 kDa and between 30 and 40 kDa, which were not alkylated by N-ethylmaleimide if they were treated in the presence of vanadate or in the rigor state. Vanadate-induced contractures are likely mediated by a reversible oxidation that activates cross bridges similarly to that of LC20-Pi and may play an important role in oxidant injury.

scholarly journals Assembly of smooth muscle myosin into side-polar filaments.

1977 ◽  
Vol 75 (3) ◽  
pp. 990-996 ◽  
Author(s):  
R Craig ◽  
J Megerman
Keyword(s):  
Smooth Muscle ◽  
Opposite Polarity ◽  
Skeletal Muscle Myosin ◽  
Myosin Filaments ◽  
Skeletal Myosin ◽  
Cross Bridges ◽  
Bipolar Filament ◽  
Muscle Myosin

The in vitro assembly of myosin purified from calf aorta muscle has been studied by electron microscopy. Two types of filament are formed: short bipolar filament similar to those formed from skeletal muscle myosin, and longer "side-polar" filaments having cross bridges with a single polarity along the entire length of one side and the opposite polarity along the other side. Unlike the case with skeletal myosin filaments, antiparallel interactions between myosin molecules occur along the whole length of side-polar filaments. The side-polar structure may be related to the in vivo form of myosin in vertebrate smooth muscle.

scholarly journals Force: velocity relationship in single isolated toad stomach smooth muscle cells.

1987 ◽  
Vol 89 (5) ◽  
pp. 771-789 ◽  
Author(s):  
D M Warshaw
Keyword(s):  
Smooth Muscle ◽  
Smooth Muscle Cells ◽  
Striated Muscle ◽  
Muscle Cells ◽  
Length Change ◽  
Force Transducer ◽  
Cell Length ◽  
Shortening Velocity ◽  
Cross Sectional ◽  
Cross Bridges

The relationship between force and shortening velocity (F:V) in muscle is believed to reflect both the mechanics of the myosin cross-bridge and the kinetics of its interaction with actin. To date, the F:V for smooth muscle cells has been inferred from F:V data obtained in multicellular tissue preparations. Therefore, to determine F:V in an intact single smooth muscle cell, cells were isolated from the toad (Bufo marinus) stomach muscularis and attached to a force transducer and length displacement device. Cells were electrically stimulated at 20 degrees C and generated 143 mN/mm2 of active force per muscle cross-sectional area. At the peak of contraction, cells were subjected to sudden changes in force (dF = 0.10-0.90 Fmax) and then maintained at the new force level. The force change resulted in a length response in which the cell length (Lcell) rapidly decreased during the force step and then decreased monotonically with a time constant between 75 and 600 ms. The initial length change that coincided with the force step was analyzed and an active cellular compliance of 1.9% cell length was estimated. The maintained force and resultant shortening velocity (V) were fitted to the Hill hyperbola with constants a/Fmax of 0.268 and b of 0.163 Lcell/s. Vmax was also determined by a procedure in which the cell length was slackened and the time of unloaded shortening was recorded (slack test). From the slack test, Vmax was estimated as 0.583 Lcell/s, in agreement with the F:V data. The F:V data were analyzed within the framework of the Huxley model (Huxley. 1957. Progress in Biophysics and Biophysical Chemistry. 7:255-318) for contraction and interpreted to indicate that in smooth muscle, as compared with fast striated muscle, there may exist a greater percentage of attached force-generating cross-bridges.

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