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Department of Medicine, Baylor College of Medicine, Houston, Texas 77030
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ABSTRACT |
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The role of extracellular elements on the mechanical properties of skeletal muscles is unknown. Merosin is an essential extracellular matrix protein that forms a mechanical junction between the sarcolemma and collagen. Therefore, it is possible that merosin plays a role in force transmission between muscle fibers and collagen. We hypothesized that deficiency in merosin may alter passive muscle stiffness, viscoelastic properties, and contractile muscle force in skeletal muscles. We used the dy/dy mouse, a merosin-deficient mouse model, to examine changes in passive and active muscle mechanics. After mice were anesthetized and the diaphragm or the biceps femoris hindlimb muscle was excised, passive length-tension relationships, stress-relaxation curves, or isometric contractile properties were determined with an in vitro biaxial mechanical testing apparatus. Compared with controls, extensibility was smaller in the muscle fiber direction and the transverse fiber direction of the mutant mice. The relaxed elastic modulus was smaller in merosin-deficient diaphragms compared with controls. Interestingly, maximal muscle tetanic stress was depressed in muscles from the mutant mice during uniaxial loading but not during biaxial loading. However, presence of transverse passive stretch increases maximal contractile stress in both the mutant and normal mice. Our data suggest that merosin contributes to muscle passive stiffness, viscoelasticity, and contractility and that the mechanism by which force is transmitted between adjacent myofibers via merosin possibly in shear.
muscular dystrophy; respiratory muscles; force transmission; extracellular matrix
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INTRODUCTION |
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MEROSIN IS AN
EXTRACELLULAR protein that is believed to transmit muscle force
between the sarcolemma and collagen fibers (17). Merosin
functions in cell attachment by providing pathways between the collagen
and the transmembrane proteins (20), and this occurs through two pathways. The first pathway involves merosin binding to
-dystroglycan of the dystrophin-glycoprotein complex. An alternate pathway involves merosin binding to
7
1-integrin of the integrin complex.
These pathways allow for interactions between collagen and neighboring
muscle fibers via merosin. Absence of merosin could create a disruption
in both pathways, thereby eliminating the communication between the
collagen and the transmembrane proteins.
Merosin deficiency causes congenital muscular dystrophy
(18), and this affects skeletal muscles as well as
peripheral nerves (22, 24, 26), so peripheral neuropathy
is found in a high percentage of affected persons (15).
Merosin-deficient congenital muscular dystrophy in humans is
characterized by several symptoms, including severe hypotonia, multiple
severe contractures, generalized weakness and atrophy, markedly delayed
motor development, and frequent severe respiratory insufficiency
(9). The disease results from an abnormality or absence of
one of the three merosin subunits, the
2-subunit, coded
for at chromosome 6 at the 6q2 position (29).
The dy/dy mouse lacks merosin in skeletal muscle and peripheral nerves and has severely defective basement membranes in the muscle (25, 32). The dy/dy mouse shares many of the hallmarks of the human form of congenital muscular dystrophy and therefore is a good mouse model for this disease (32, 33). The dy/dy mouse develops muscle weakness at ~3 wk of age (12), which progressively worsens, and by 8 wk of age the histological changes in muscles are significant. In the dy/dy mouse, the muscle initially appears normal, with normal fiber-type differentiation up to 2 wk of age, when the necrotic process starts. After 1 mo of age, there is marked variation in fiber size with necrotic and regenerating fibers (30). Interstitial fibrosis becomes evident as the disease progresses.
The role of the extracellular matrix protein merosin in force transmission in skeletal muscles is unknown. In this study, we investigated the mechanical properties of the diaphragm and biceps femoris hindlimb muscles in the dy/dy mouse. We tested the hypothesis that merosin deficiency alters muscle compliance, viscoelastic properties, and muscle contractile force production. To test this hypothesis, we determined the axial and transverse passive length-tension relationships in these muscles. We also examined the viscoelastic properties of the diaphragm in response to constant mechanical stretch in either the fiber or transverse to fiber direction. In addition, we determined the isometric contractile properties of the diaphragm during uniaxial and biaxial loading.
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MATERIALS AND METHODS |
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Measurements of passive mechanical properties.
We used eight C57BL/6J-Lama2dy-2J mice (weight: 13.4 ± 1.1 g; age: 55.7 ± 7.6 days) and eight normal C57BL/6J mice (weight: 20.5 ± 1.8 g; age: 50.7 ± 2.1 days) obtained from the
Jackson Laboratory for our experiments. All animal studies
were approved by the Baylor College of Medicine Advisory Committee for
Animal Use and conformed to the National Institutes of Health Guide for the Care and Use of Laboratory Animals. It is important to note that
the control mice used were either wild type or heterozygotes. At this
age, the effect of merosin deficiency is clearly observed in the
C57BL/6J-Lama2dy-2J through severe weakness of either one or both
hindlimbs (Fig. 1).
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Muscle mechanical testing.
After excision, either the diaphragm or biceps femoris was then placed
in an in vitro biaxial muscle testing apparatus. This apparatus has two
perpendicular axes, each driven by a micrometer. Four small identical
alligator clamps, one for each side of the muscle, were used to hold
the muscle during passive muscle lengthening and shortening maneuvers.
The diaphragm muscle was secured by fixing one clamp on the central
tendon and the opposing clamp on the muscle-tendonous junction at the
chest wall insertion with the rib cage intact. The biceps femoris
muscle was secured by fixing opposing clamps on the muscle near the
muscle-tendonous junction. The muscle was mounted so that the position
of these markers during stretching and shortening could be viewed with a black-and-white CCTV-type camera and recorded on a videocassette. Two
force transducers (World Precision Instruments, model FORT 100, ±50 g,
differential bridge type) were used to measure passive muscle force.
Each transducer has a resolution of 0.01% full scale, a sensitivity of
3 µV · V
1 · g
1,
and a hysteresis of 0.1% full scale. One transducer for each axis was
used to measure the forces applied to the muscle during passive
lengthening and forces released during passive muscle shortening. The
forces were then amplified and recorded with the use of LABVIEW
software version 6.0. The recorded video was digitally captured with a
video capture card by using a frame grabber at a sampling rate of 2 Hz.
The markers on the captured video were then digitized with Image Tool
V2.0 (www.ddsdx.uthscsa.edu), and the precise marker position was
determined on Cartesian coordinate axes, assuming that all markers lie
within the same plane.
Two-dimensional surface strains.
The mechanical strains were calculated according to Boriek et al.
(7) with some modifications. The region enclosed by the markers was divided into triangles, with the markers forming the apexes
of the triangles. The three points that define a triangle determine a
plane. The coordinates of these points in the plane at the reference
position were denoted as xi and
yi (i = 1, 2, 3). The
displacements in the local coordinate system of the markers from their
reference positions to their positions at a deformed state are denoted
by ui and vi. These are
assumed to be a linear function of position in the plane of the
triangle. For example, the following equation
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(1) |
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(2) |
x) and strains
transverse to the fibers (
y) that occurred during passive
lengthening and shortening of the muscles were computed according to
the following equations (4)
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(3) |
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(4) |
u and
v denote the marker's
displacement in the x (along fibers) and y
(transverse to fibers) directions, respectively. The values of
a2, a3, and so forth were
substituted in Eqs. 3 and 4 to obtain
u/
x,
u/
y, and
so forth. The values of
x and
y reflect
fractional changes in the direction along the muscle fibers and
transverse to the fibers, respectively. Calculations of strains were
made relative to the unstressed length of the muscle. Unstressed length
was defined as the length where the muscle was placed in the tissue
bath in the absence of applied mechanical forces. We computed the
extensibility ratio,
= 1 +
, where
is the
mechanical strain in either the fiber or transverse to the fiber direction.
We measured optimal length, Lo, by
determining the length at which the muscle produced maximal twitch
force in response to electric stimulation. Lo
was determined to correspond to a tension of ~5 g/cm for both normal
and dystrophic muscles. To establish a constant history of mechanical
loading, the muscle was preconditioned with five cycles of passive
lengthening to Lo and then passive shortening to
the unstressed length. Length-tension curves were then measured by
passively lengthening the muscle in the direction of the muscle fibers
from the unstressed length to a muscle length at tension of ~15 g/cm.
Then the muscle was passively shortened to the unstressed length.
Length-tension curves were also measured in the direction transverse to
the fibers. These curves were obtained by passively lengthening and
passively shortening the muscle in the direction transverse to the long
axis of the muscle fibers. We also conducted a biaxial mechanical
loading in which the muscle was first stretched by a tension of 5 g/cm
in the transverse direction and the muscle was kept at constant length
in the transverse fiber direction. The muscle was then passively
lengthened axially by a tension of ~15 g/cm, and then the muscle was
passively shortened to the shortest possible length in the presence of
a transverse load.
Measurements and modeling of viscoelastic properties. After producing the length-tension curves, we measured stress-relaxation curves in the same merosin-deficient and control mice. The behavior of the living tissue is sensitive to the history of muscle deformation; therefore, before uniaxial stress-relaxation maneuvers, we preconditioned the muscle by loading the muscle tissue to Lo for five cycles. In the axial direction, the muscle was stretched to Lo and kept at that length. In the transverse fiber direction, the muscle was stretched by a passive force equivalent to that applied in the axial direction and kept at that length. The muscle tension was allowed to relax symptotically until it essentially reached a plateau. Forces were collected at 10 Hz by using a force transducer.
Using nonlinear least-squares routines built in the MATLAB environment, we fitted the stress-relaxation data to the standard linear solid model of viscoelasticity (14). This simple model describes the muscle as a parallel combination of a dashpot with coefficient of viscosity
1 and a linear spring of spring constant µ1 with a second linear spring of spring constant
µ0 that is in parallel with the first spring and the
dashpot. The relaxation function based on this model has the form
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is
relaxation time for constant strain, and 
is the
relaxation time for constant stress. After obtaining the three
constants, ER, 
, and 
,
we then calculated the viscoelastic coefficients
1,
µ1, and µ2 based on the force-displacement
relationships of the model. The ratio
/µ is a relaxation time: it
characterizes the rate of relaxation of the dashpot. We reported the
ER and the dashpot relaxation time
(
1/µ1).
Measurement of isometric contractile properties of the diaphragm. Diaphragms from eight normal C57BL/6J mice (weight: 18.6 ± 1.9 g; age: 63.0 ± 4.0 days) and nine merosin-deficient C57BL/6J-Lama2dy-2J mice (weight: 16.9 ± 3.8 g; age: 81.6 ± 17.5 days) were used. After animals were anesthetized, we excised the left hemidiaphragms and immediately placed them in a muscle bath with continuously circulating oxygenated 95% O2-5% CO2 Krebs-Ringer solution. The muscle was clamped on both the central tendon and ribs, with one clamp being connected to a Cooper Instruments LQB 630 force transducer. After the muscle was positioned between two stainless steel mesh electrodes, it was stimulated by a Grass S88 stimulator. Lo was determined by twitch responses (0.1-ms stimulus duration, supramaximal voltage), and we tetanically stimulated the diaphragm muscle at 100 Hz preceded by twitches (supramaximal voltage, 0.5-ms pulses, tetanic train duration of 500 ms, 120-s recovery). The muscle was then clamped transverse to the long axis of the muscle fibers, with one clamp attached to a World Precision Instruments FORT250 force transducer and the other clamp attached to a force carriage. Tetanic stimulation sequences were repeated three times in the presence of either 1- or 2-g passive forces that were applied in the direction transverse to muscle fibers. These measurements were collected at room temperature (25°), which minimized temperature-dependent deterioration of the preparation. The contractile force data were collected at a sample rate of 300 Hz with the use of a data acquisition board (model Lab-PC-1200/AI, National Instruments) and LabVIEW software (version 4.0). The force data were stored in an ASCII file for postanalysis.
Contractile stress was computed as the ratio of applied passive tension to the unstressed thickness (stress = tension/thickness) [where stress is in N/cm2, tension is in N/cm (computed by the measured force in grams and divided by the clamp width), and thickness is in cm]. To obtain thickness, a digital image of muscle surface was obtained. The muscle was then gently blotted dry and weighed, and the surface area of the muscle sheet was determined by using Image Tool (version 2.0). Thickness was computed by using the measured surface area, mass, and muscle density. Twitch characteristics were analyzed with LabVIEW (version 5.2), and the MATLAB (version 5.0) program was used for analysis of maximal tetanic data.Immunolabelings. Muscles were frozen in isopentane precooled in liquid nitrogen. Transverse sections (5 µm thick) were preincubated for 20 min in phosphate-buffered saline (pH 7.2) containing 5% albumin. Serial sections were incubated overnight at 4°C with anti-collagen IV.
Statistical analysis. Differences between groups were assessed by ANOVA with use of the SAS Procedure "Mixed" Program (23). The model was a two-factor fixed or random effects model for two groups of mice (dy/dy null vs. controls) and two treatments (passive mechanics: uniaxial stretch along the muscle fibers vs. uniaxial stretch transverse to fibers; active mechanics: uniaxial loading vs. biaxial loading). A P value of 0.05 was chosen as the acceptable level of significance throughout the analysis of all data.
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RESULTS |
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Passive stiffness is increased in muscles from the dy/dy mice.
Data in Fig. 2 show representative
length-tension curves for the dy/dy and control mice. Both
loading (lengthening) and unloading (shortening) curves are shown. The
data demonstrate that, during lengthening, there is a slow and
continuous increase in tension over the range of imposed strains. Both
dy/dy and controls exhibited hysteresis; that is, at the
same tension, the muscle exhibited lower mechanical strain on
lengthening than on shortening. It appears that hysteresis is smaller
in the dy/dy muscles. Furthermore, the axial length-tension
curves of the normal diaphragm shifts to the right relative to the
transverse length-tension curve. This suggests that the muscle has
greater extensibility in the direction of muscle fibers than in the
transverse direction to the fibers. The length-tension curves of the
dy/dy diaphragm exhibit similar behavior. Extensibility
ratios (
) for all the dy/dy and control mice were
computed at a tension of 5 g/cm. In the direction along the fibers (AF)
of the diaphragm muscle,
is smaller in the dy/dy mice
compared with control mice (control:
= 1.35; dy/dy:
= 1.21). In the direction transverse to muscle fibers (TF),
is smaller in the dy/dy mice than in the control mice (control:
= 1.21; dy/dy:
= 1.17). At a
tension of 5 g/cm, the tensile strain in the direction of the fibers is
21 and 35% for dy/dy and control mice, respectively,
yielding a compliance ratio of 0.90. A compliance ratio that is less
than one implies that the muscle is less compliant compared with its
counterpart. The tensile strain at the same level of tension transverse
to the muscle fibers is 17 and 21%, respectively, yielding a
compliance ratio of 0.97. These data suggest that muscles lacking
merosin are less extensible and less compliant than those in normal
mice.
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of the
biceps femoris muscle from normal mice are greater than those of
merosin-deficient mice in the AF direction as well as in the TF
direction. At a tension of 5 g/cm, the
in the AF and TF directions
are higher in merosin-deficient mice compared with controls (AF:
control,
= 1.46; dy/dy,
= 1.11; TF:
control,
= 1.23; dy/dy,
= 1.17). At a tension of 5 g/cm, the tensile strain in the direction of the fibers is 11 and
46% for dy/dy and control mice, respectively, yielding a
compliance ratio of 0.76. Mechanical strain at the same level of
tension transverse to the muscle fibers is 17 and 23%, respectively,
yielding a compliance ratio of 0.95. The curves for the
merosin-deficient muscle in either direction are shifted to the left
compared with the normal muscles. These data suggest that biceps
femoris muscles lacking merosin are less extensible and less compliant
than those in controls.
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Merosin contributes to muscle viscoelasticity.
A linear spring instantaneously produces a deformation proportional to
the load, whereas a dashpot produces a velocity proportional to the
load at any instant. Furthermore, a dashpot represents a damping term
proportional to velocity. The dashpot relaxation time is the length of
time necessary for the dashpot, or shock-absorbing quality of muscle,
to be essentially relaxed, that is, at the completely relaxed point the
muscle is characterized as elastic. The dashpot relaxation times
(
) for merosin-deficient diaphragms compared with
controls are shown in Fig. 5. Because

is equivalent to the ratio of the dashpot to the
linear spring in series (
1µ1), an increase
in 
indicates that the dashpot component has a
greater effect than the linear spring in series for any given loading
condition. 
was significantly greater in
merosin-deficient diaphragms compared with normal muscle. This was true
during biaxial loading and during uniaxial loading (P < 0.05). These data suggest that the absence of merosin alters the
viscoelastic properties of the diaphragm muscle. In contrast to normal
muscles, differences between uniaxial loading and biaxial loading
vanished. That is, the effect of transverse load on the values of
ER is only apparent in normal muscles but not in
merosin-deficient muscles. These data suggest that the absence of
merosin alters the viscoelastic properties of the diaphragm muscle by
increasing the relaxation time, and this effect is more pronounced
during transverse loading as well as during biaxial loading.
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DISCUSSION |
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The mechanical properties of diaphragm muscle are dependent on the properties of the cells and the interconnections with the extracellular matrix. Merosin is considered one of the very essential extracellular elements that form this junction between the extracellular matrix and the muscle cytoskeleton. To date, no previous studies have investigated the mechanical properties of skeletal muscles in the dy/dy mouse. In this study, we measured length-tension curves, the viscous response, and maximal tetanic stress in the diaphragm from the dy/dy mouse, a mouse model of merosin deficiency. Our results demonstrate that muscle extensibility and compliance are decreased in the diaphragm and biceps femoris muscles of the dy/dy mouse. Furthermore, compared with controls, ER is greater in the deficient diaphragm muscle. Additionally, maximal tetanic force is depressed in the dy/dy mouse during uniaxial and biaxial loading.
Our data show that the normal diaphragm exhibits characteristics of viscoelastic response to mechanical loading. This is consistent with classic data on muscle viscoelasticity (14). Furthermore, recent studies from our laboratory (2, 5, 6) demonstrated that passive mechanical properties of diaphragm muscles in the AF direction are different from those in the TF direction. These studies showed that the diaphragm is less compliant in the TF direction compared with that in the AF direction. Most recently, our laboratory (21) has found two distinct signaling pathways of force transmission in the AF and TF directions. For both control and merosin-deficient mice, length tension curves in the TF direction are shifted to the left compared with those in the AF direction, indicating greater muscle extensibility along the muscle fibers. However, independent of the direction of passive stretch, merosin-deficient muscles demonstrate a leftward shift of the length-tension curves compared with controls. This suggests that merosin-deficient muscles are less extensible and that a greater tension is required to passively lengthen muscles from the mutant mice to the same muscle length as that of the normal mice. The length-tension curves of the biceps femoris, shown in Fig. 3, demonstrate that for the normal muscles the axial length-tension curves are shifted to the right of that in the transverse direction. In the dy/dy mouse, however, differences in length-tension curves between those in the axial direction and those in the transverse direction appear to be negligible. This indicates that the muscle sheet of the biceps femoris in the absence of merosin is nearly isotropic. That is, mechanical properties may be independent of the direction of mechanical stretch in merosin-deficient muscles. The data also demonstrate that the merosin-deficient muscle is essentially inextensible in either the fiber or the transverse to fiber direction. This is consistent with loss of muscle function in the hindlimb muscles of the dy/dy mice at this age. This is also consistent with upregulation of collagen IV in these muscles at that age.
In vivo, the diaphragm muscle unlike most other skeletal muscles of the hindlimb and forelimbs experiences loads in the AF direction as well as in the TF direction. Any muscle sheet that is loaded uniaxially in the AF direction would have different length-tension relationship than when the sheet is also loaded in the TF direction. Therefore, this complicates the use of uniaxial in vitro properties to analyze in vivo behavior of the diaphragm muscle. Conducting in vitro physiological experiments under biaxial loading of the diaphragm muscle is therefore critical to the understanding of diaphragm function. Therefore, the effect of biaxial loading or stresses applied in the two perpendicular directions of the muscle sheet of the diaphragm was investigated. The results show that length-tension curves during biaxial loading are much stiffer compared with axially loaded muscles. This is consistent with previous data on length-tension curves of the intact, pressurized loaded muscles and excised uniaxially loaded muscle sheets of the rat diaphragms (5). Furthermore, the data show that the merosin-deficient diaphragm is less extensible compared with controls when experiencing biaxial loading.
The dashpot relaxation time (
) is the time necessary
for the dashpot or shock-absorbing quality of the muscle to be essentially relaxed; that is, at this point the muscle is characterized as perfectly elastic. The 
was significantly greater
in the transverse plane of the muscle in merosin-deficient mice
compared with control mice. That is, in the absence of merosin, the
diaphragm muscle appears to require more time to reach the perfect
elastic state when loaded in the direction orthogonal to the long axis of the muscle fibers. ER provides a quantitative value for
the viscous response of the muscle, where an ER of 1.0 signifies a perfect elastic behavior. The results show that, compared
with controls, the merosin-deficient diaphragm has a smaller
ER value in the transverse plane. Both 
and ER data strongly suggest that the merosin-deficient
diaphragm is more viscous in the transverse plane compared with
controls. Therefore, these data suggest that, at least in the
transverse plane, merosin decreases the damping capacity of the muscle.
The effect of age and breeding constraints are important to the
understanding of the significance of the results of this study. The
contractile force capacity of merosin-deficient muscles is most likely
decreased with age, and this is because merosin deficiency causes
progressive muscle degeneration. It was impossible to conduct our
experiments on these mice in the prenecrotic stage because these mice
develop muscle necrosis shortly after birth. Merosin-deficient mice are
infertile, and, as such, heterozygotes must be mated to generate the
merosin-deficient mouse. However, genotyping studies on these mice are
inconclusive, and, as a result, distinguishing between controls and
knockouts must be made on the basis of phenotype. Merosin-deficient
mice can be easily phenotypically distinguished from normal mice on the
basis of gait, where these mice display an obvious paralysis of the
hindlimbs at ~40 days old. The mice reported in the present study are
of that age (~6-7 wk); therefore, muscles from these mice were
tested after the onset of the disease. In merosin-deficient mice, there
is an upregulation of
7
1-integrin in
skeletal muscles (19, 31), suggesting that integrin
engagement is needed to substitute for some of the loss of mechanical
integrity of the cells in the absence of merosin.
In earlier studies, we and our colleagues (3, 4, 8) investigated muscle fiber architecture and mechanism(s) of force transmission in the diaphragm of the dog. These studies demonstrated that muscle fiber architecture is complex and mostly discontinuous. That is, there are fibers that either span the entire length of the muscle or terminate by tapering before reaching either or both attachments. We reasoned that, when the diaphragm is submaximally activated, as during normal breathing and maximal inspiratory efforts, muscle force could be transmitted to the cell membrane and to the extracellular intramuscular connective tissues by shear linkage, presumably via structural transmembrane proteins. The results of our present study are consistent with merosin being a possible candidate protein that transmits muscle force from the cell membrane to collagen fibers. During submaximal activation, merosin could also transmit muscle force from the active muscle fibers of the diaphragm to the adjacent passive muscle fibers, and the mechanism of force transmission is most likely in shear.
Increased collagen and fibrosis are general features of muscular
dystrophy, and increased muscle stiffness has generally been attributed
to an increased proportion of collagen (1, 13, 16, 27,
28). However, some studies have demonstrated lack of correlation
between the increased amount of collagen and passive stiffness. In
particular, in soleus muscles of the rat, the changes in muscle
stiffness were not associated with increased collagen with aging. In
addition, Coirault et al. (11) found that muscle stiffness
was decreased in the diaphragm muscles from Syrian hamster, whereas
surface area of collagen was increased in these animals. On the basis
of these reports, muscle passive stiffness is not always correlated
with increase in the proportion of collagen. Therefore, the
increased stiffness in the merosin-deficient muscles is not necessarily
entirely due to the increase in collagen seen in the dy/dy
mice at ~2 mo of age (Fig. 9). Our experiments were conducted on
~50-day-old mice (after the onset of muscle necrosis); therefore, we
cannot rule out the likely possibility that merosin is a load-bearing
element in skeletal muscles. There are two possible pathways for force
transmission that include merosin at the sarcolemmal membrane and
through which forces are transmitted between the cytoskeleton and the
extracellular space (Fig. 10). Thus a
deficiency of merosin should alter the transmission of force in either
the axial or transverse plane of the muscle fibers. Lack of merosin disrupts both the transverse and longitudinal pathways of force transmission shown in Fig. 10, and such disruption in force
transmission could be responsible at least in part for the severe
phenotype and early death in the dy/dy mice. Disruption of
these pathways in the dy/dy mouse is consistent with our
results on the contractile properties of the merosin-deficient
diaphragm that indicate that, regardless of the presence or absence of
transverse passive muscle force, maximal muscle tetanic stress is
depressed in these mice compared with controls.
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Although the depression in muscle force production from dy/dy mice muscles may be attributable to merosin deficiency, the increase in collagen content must also be considered. Collagen fibers and connective tissue do not respond to electric stimulation. That is, these fibers do not display contractile properties. Thus, when merosin-deficient muscles are stimulated, they would be expected to generate a smaller force because of both deficiency of merosin and an increase in collagen content. This is consistent with our model that proposes that merosin is a key component in transmitting the forces both longitudinally and transversely to the muscle fibers.
In summary, our data demonstrate that the passive compliance of either hindlimb and diaphragm muscle is decreased in the absence of merosin. Furthermore, disruption of merosin appears to contribute to the viscous capacity of the diaphragm in response to mechanical loading, specifically, in the transverse plane of the muscle fibers of the diaphragm. Additionally, muscle force is depressed in the merosin-deficient muscles. Taken together, our results suggest that loss of merosin leads to altered muscle passive and active mechanical properties in both longitudinal and transverse pathways of force transmission.
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ACKNOWLEDGEMENTS |
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We thank Dr. Eva Engvall for conducting the immunocytochemical labeling analysis and discussion of the manuscript. We thank Dr. Michael B. Reid for discussions of the conceptual model of force transmission in skeletal muscles.
This work was supported by National Heart, Lung, and Blood Institute Grant HL-63134.
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FOOTNOTES |
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Address for reprint requests and other correspondence: A. M. Boriek, Baylor College of Medicine, One Baylor Plaza, Dept. of Medicine, Pulmonary Section, Suite 520B, Houston, TX 77030 (E-mail: boriek{at}bcm.tmc.edu).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
10.1152/japplphysiol.01078.2002
Received 25 November 2002; accepted in final form 11 March 2003.
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