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* Department of Bioengineering, University of Washington, Seattle, Washington;
Department of Molecular Physiology and Biophysics, University of Vermont, Burlington, Vermont; and
Department of Biology and Molecular Biology Institute, San Diego State University, San Diego, California
Correspondence: Address reprint requests to Gerald H. Pollack, E-mail: ghp{at}u.washington.edu.
| ABSTRACT |
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| INTRODUCTION |
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During flight, the Drosophila thorax vibrates at its resonant frequency (
240 Hz), driving the wings to beat at the same frequency over a span of
170° with high efficiency (7
). Two sets of perpendicularly placed IFM work in tandem; when one set actively contracts, the other is stretched. Kinetic energy (stiffness times the square of the length change) is stored in elongated molecular "springs" consisting of connecting filaments and other elastic elements in the sarcomere, including thick filaments (8
). The stored energy is released to facilitate the wing beat stroke when the opposing set of IFM deactivates itself (5
). For fast vibrations, sarcomere-length changes cannot be large; therefore, small length changes (
3.5% in Drosophila melanogaster: (9
)) require high passive stiffness to store significant energy. The high tension generated from stretching connecting filaments is also thought to be a prerequisite for stretch activation (10
).
The high passive stiffness of IFM can be largely explained by short connecting filaments (C-filaments) that anchor the thick filaments to the Z-disk in the sarcomere (11
). In Drosophila IFM, C-filaments consist of the proteins projectin (12
) and kettin (13
,14
). Other proteins are thought to form cross-links between thick and thin filaments to further strengthen the sarcomere in Drosophila IFM, including troponin H (specifically, the C-terminal extension: (15
)), the myosin regulatory light chain (the N-terminal extension: (5
,6
)), and, possibly, flightin (3
). Weak actomyosin cross bridges have also been implicated (16
).
In this study, we examined the myofibril passive stiffness of two previously constructed lines of transgenic Drosophila that showed compromised flight ability compared to their positive controls. One group (hereafter referred to as hinge-switch lines) had the central portion of its endogenous S2 hinge (15a) in IFM replaced by the embryonic version (15b) (17
). As 15b is expressed in slower and presumably more compliant muscles than IFM, it is of great interest to investigate whether alternative hinge regions modulate sarcomere stiffness. In the other group (paramyosin mutants), one or more serines (putative phosphorylation sites) near the N-terminus of paramyosin's nonhelical region were replaced by alanines (18
). Previous muscle fiber mechanics studies on the paramyosin lines found a significant reduction in the passive, active, and rigor elastic modulus (18
). We designed this study to test whether similar differences in passive stiffness occur at the level of the myofibril, the smallest subdivision of muscle that retains the organized myofilament lattice.
A comparison of hinge-switch and paramyosin mutants at the myofibril and muscle fiber levels showed marked differences in passive stiffness. Although alternative hinge regions have different propensities for forming a coiled coil, the hinge mutants exhibit the same passive stiffness as the control. This result shows that swapping the S2 hinges does not affect passive sarcomeric stiffness. The paramyosin phosphorylation-site mutants, in contrast, have a significantly lower passive stiffness compared to control. The reduced stiffness suggests paramyosin interacts via phosphorylation with other sarcomeric proteins (probably projectin and/or kettin), which help maintain high passive stiffness in IFM myofibrils.
| MATERIALS AND METHODS |
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Single myofibril mechanics
A single myofibril, immersed in a physiological relaxing solution, was attached between the tips of a glass needle and a microfabricated cantilever working as a force transducer (stiffness, 12 pN/nm). The myofibril was then incrementally stretched by a total of
24%. Force and sarcomere length data were collected 12 min after each stretch increment. The slope of the linear fit to the force versus sarcomere length plot was taken as the sarcomere stiffness, which means the amount of tension (in nN) a single sarcomere develops per unit length (in nm) of stretch. Myofibril diameter was estimated from the width of the myofibril captured in CCD video images. Sarcomere length (SL) was the slope of the linear fit of A-band peak positions versus their index numbers. The experiments were performed at room temperature. The relaxing solution (pCa 8) was 20 mM BES, 15 mM creatine phosphate, 240 units/ml creatine phosphokinase, 1 mM DTT, 5 mM EGTA, 1 mM free Mg2+, 5 mM MgATP, and 8 mM Pi at pH 7.0 and an ionic strength of 200 mEq adjusted with sodium methane sulfate. Details of the method for preparing single myofibrils and measuring passive (resting) stiffness are given elsewhere (19
).
Elastic modulus (nN/µm2) of each tested myofibril was calculated from (stiffness/CSA) x SL0, in which SL0 means initial sarcomere length when tension is zero, and stiffness/CSA is sarcomere stiffness divided by cross-sectional area (CSA). The phase contrast imaging technique for measuring myofibril diameter underestimates the true values by roughly 24%, thereby producing an underestimate of true myofibril cross-sectional area by roughly 58% (19
). To account for this area underestimation, the uncorrected value of the elastic modulus was multiplied by 0.58 to obtain the corrected value.
Muscle fiber mechanics
A chemically skinned muscle fiber was secured at both ends with aluminum T-clips and mounted between a strain gauge force transducer and a piezo-motor. After measuring the initial length (L0) when the specimen was just taut, and the cross-sectional area (CSA), the fiber was prestretched incrementally to 1.05L0 in relaxing solution at 15°C. Sinusoidal perturbation of amplitude 0.125%L0 was applied at 47 frequencies (0.51000 Hz) and the tension (T) signal was recorded. The complex ratio (with both amplitude and phase) of stress (T/CSA) to strain (0.125%) was taken as the dynamic modulus of the passive muscle fiber, which was decomposed into elastic (in-phase) and viscous (out-of-phase) components. The relaxing solution (pCa 8) was the same as used for the myofibril mechanics. A detailed description of the preparation, experimental equipment, and method of sinusoidal analysis are given elsewhere (21
). Elastic modulus values obtained at the lowest oscillation frequency (0.5 Hz) are directly compared to the myofibril data since this slow oscillation best simulates the static methods used to determine the single myofibril stiffness. The frequency dependence of both elastic and viscous moduli was measured in the skinned fiber since phenotypical differences may only appear under dynamic conditions. Dynamic measurements with myofibrils were not feasible because of the technical difficulty in characterizing the high frequency viscoelastic properties of the attachments to the motor and strain gauge.
Transmission electron microscopy
After completion of muscle fiber mechanics, wild-type fibers were fixed for 2 h in Karnovsky's fixative (2.5% glutaraldehyde and 1.0% paraformaldehyde in 0.1 M Millonig's phosphate buffer, pH 7.2). After removal of their T-clips, fixed fibers were embedded in 2.5% SeaPrep Agarose, chilled for 15 min at 4°C, immersed in Karnovsky's fixative for 15 min at 4°C, and rinsed 3 times for 10 min each in Millonig's buffer. Samples were postfixed in 1% OsO4 for 45 min at 4°C, then washed 3 times for 5 min and subsequently stored for 24 h in 0.1 M Millonig's buffer at 4°C. Details of the dehydration, infiltration, embedding, sectioning, and imaging are given elsewhere (22
). Image analysis was performed using ImageJ software version 1.36b (National Institutes of Health, Bethesda, MD). Myofibril area per total fiber cross-sectional area, an important factor for making comparisons between myofibril and fiber studies, was calculated by darkening the myofibrils, thresholding the entire image, and calculating the percentage of total area covered by myofibrils in 18 x 18 µm fields.
COILS test
COILS is a program that predicts the probability of a sequence to form a coiled coil based on the similarity of the sequence in question with a database of known parallel two-stranded coiled-coils (23
). Amino acid sequences were fed to COILS version 2.2 program on line (http://www.ch.embnet.org/software/COILS_form.html). Default parameters were chosen whenever possible, i.e., matrix: MTIDK; no weighing on positions a and d, and window width: 21.
Statistical analysis
Statistical analysis was carried out with SPSS v.11 (SPSS, Chicago, IL). Test results were considered significant at the p < 0.05 level. For the myofibril data, one-way analysis of variance (ANOVA) tests were performed to determine the effects of different strains. If differences were found to be significant, the least significant difference (LSD) post hoc test was performed and used to determine which means differed. For the fiber data, since the elastic and viscous modulus were examined across various oscillation frequencies, a repeated-measures ANOVA with frequency as the repeated measure was performed first to determine the effects of the different transgenic and control strains. If a significant strain effect was found between subjects, then one-way ANOVAs were performed at each frequency to determine significant differences.
| RESULTS |
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Validation of positive controls
The positive controls, pwMhc2 for hinge-switch mutants and pm for paramyosin mutants, underwent the same transformation and genetic manipulations as their corresponding mutants, except that the wild-type versions of the protein supplied by the transgenes were crossed into the null mutant backgrounds. We compared myofibrils from the wild-type strain yw (19
) to the two positive controls (Table 1). The elastic moduli of the two positive controls and wild-type lines were similar, indicating the genetic transformations themselves did not alter the passive mechanical properties of the IFM. Interestingly, the myofibril diameter increased in both positive controls and the sarcomere stiffness was statistically higher in pwMhc2. These differences disappear, however, once the data are normalized for cross-sectional area, as shown by the stiffness/CSA and elastic modulus values.
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| DISCUSSION |
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Probing passive sarcomere stiffness
When a relaxed myofibril is stretched, most of its extension comes from the elongation of C- filaments that connect thick filaments to the Z-disk (11
). The C-filaments have recently been shown to consist of the long extensible proteins projectin (12
) and kettin (13
). Although thick and thin filaments are also extensible (24
27
), they are much stiffer than the C-filaments.
In the "stretch and hold" protocol from which the myofibril mechanics data were derived, each sarcomere was incrementally stretched by
100 nm (SL 3.6 µm x
3%). Because any possible cross-links (weakly attached myosin heads (16
), myosin regulatory light chain N-terminal extension (5
,6
), the myosin associated protein flightin (3
), and troponin-H isoform 34 (15
)) likely detach and reattach during the long-range stretch (instead of being elongated by 100 nm without breaking), it is unlikely that the cross-links contribute significantly to the stiffness of the myofibril. Thus, the passive compliance (1/stiffness) of the half sarcomere is equal to the sum of the thick and C-filament compliance, i.e.,
![]() | (1) |
A recent x-ray study of Drosophila flight muscle in vivo (8
) showed the thick filament backbone undergoes an
0.2% strain during each work-producing wing beat, as indexed by a strong 7.2-nm periodic reflection off the thick filament. Since the sarcomere length of Drosophila IFM changes by
3.5% during each wing beat (9
), the ratio of the two length changes suggests that the thick filament is
17x (= 3.5%/0.2%) stiffer than that of the C-filament. Therefore, we conclude that under passive conditions Drosophila IFM thick filaments are relatively inextensible compared to C-filaments.
Hinge-switch study
Drosophila has a single gene encoding the muscle myosin heavy chain; isoforms of the protein result from alternative splicing of the primary RNA transcript (28
). Alternative exons 15a and 15b encode the central 26 amino acids of the S2 hinge, which is the region located between the N-terminus of light meromyosin and the C-terminus of short S2 (29
) and may be part of the thick filament backbone. 15a and 15b hinges have different properties of charge, hydrophobicity, and propensities toward forming a coiled-coil (15a has a 59% probability; 15b, 91%).
In spite of the structural differences, we found no difference in elastic modulus between the two mutants and the positive (wild-type) control. Because passive sarcomere stiffness is determined primarily by C-filament stiffness, as noted above, the lack of a difference in resting stiffness between the hinge mutants and the control suggests that the alternative hinges do not interact (or do not vary significantly in their interaction) with the C-filaments (or other structures that may link thick and thin filaments). We conclude, therefore, that alternative hinges do not modulate passive sarcomere stiffness.
Although passive stiffness appears to be unaffected by the hinge substitutions, it is possible that hinge switches do affect sarcomere stiffness in active fibers. The thick filament is measurably extensible in working muscles (8
); thus, it is possible that differences in extensibility due to hinge differences may underlie the severely impaired flight ability seen previously in transgenic lines expressing an IFM myosin isoform with the "slow" hinge 15b compared to that with the native "fast" hinge 15a (17
). Clearly, a comparison of sarcomere stiffness in active, working IFM from the hinge mutants and controls is necessary to fully resolve the question whether hinge differences play a significant role in flight muscle stiffness.
Paramyosin phosphorylation study
Paramyosin, a major structural protein of invertebrate thick filaments, is a rod-like molecule with a central
-helical region and two nonhelical terminal domains (30
,31
). In vivo phosphorylation of paramyosin has been reported in Drosophila (32
) as well as in other species (33
,34
). In Drosophila IFM, paramyosin, despite its low concentration, is uniformly distributed along the core of the thick filament (35
,36
).
To test whether paramyosin phosphorylation in Drosophila plays an important role in muscle function, several transgenic lines were constructed in which one or more phosphorylatable serine residues near the N-terminus of paramyosin were replaced by alanines. Two of the resulting lines (pmS18A and pmS-A4) showed compromised flight ability, whereas the ultrastructure of their IFM was normal (18
).
In this study we examined the passive stiffness of Drosophila IFM myofibrils from the two mutant lines and their positive (wild-type) control. Myofibrils from the two transgenic lines with impaired flight ability had a 15% reduction in passive stiffness compared to control. The finding of reduced passive stiffness in the paramyosin mutants was surprising since, from Eq. 1, thick filament stiffness would have to diminish by 76% to accommodate a reduction in sarcomere stiffness of 15%, assuming an initial ratio of thick-filament to C-filament stiffness of
17. Thus, it is possible that the paramyosin molecule contributes directly and massively to thick filament stiffness, and that disruption of the phosphorylation sites directly affects thick filament stiffness. However, in light of the exceptionally large changes in thick filament stiffness that would have to occur, it is more likely that paramyosin plays a role in anchoring kettin and/or projectin to the thick filament, and that disruption of the phosphorylation sites disrupts the anchoring. It is worth noting that any anchoring model would have to accommodate the low molar ratio of paramyosin to myosin in Drosophila IFM (molar ratio,
1:34: (32)), and its putative location within the core of the thick filaments (37
).
Our myofibril measurements agree well with fiber measurements from a previous study (18
), which reported significant reductions in passive, active, and rigor elastic modulus of muscle fibers from the same paramyosin mutants. The authors of the previous study suggested that paramyosin phosphorylation most likely contributes to thick filament stiffness by interacting with myosin rods and/or stabilizing the thick filament's connection to the M-line. Because thick filament compliance cannot be neglected in the calculation of sarcomere stiffness under active or rigor conditions (25
,27
), Liu and colleagues propose, in essence, that thick filament stiffness is reduced in the phosphorylation site mutants, thereby accounting for the reduced elastic moduli observed in active and rigor fibers. Although this may be the case for active and rigor fibers, our analysis indicates that the reduction in passive stiffness of the sarcomere in the phosphorylation site mutants is most likely due to altered C-filament anchoring.
The fractional reduction in elasticity in active (and rigor) muscles is greater than that in passive muscle from the paramyosin phosphorylation site mutants (18
). Thus, it is likely that any weakened paramyosin interactions with C-filament proteins contributes to reduced active stiffness as well, consistent with notions advanced by previous research (10
,11
,16
). We propose that both mechanisms, altered anchoring and reduced thick filament stiffness, give rise to the reduced flight ability of the paramyosin phosphorylation site mutants.
Myofibril versus fiber mechanics
Our results show that the mutation-related trends of both lines were similar between myofibrils and fibers. The magnitudes of the myofibril and fiber elastic modulus were similar between controls and hinge-switch lines, but differences were observed between myofibrils and fibers in the magnitude of the changes observed in the paramyosin transgenic lines. The elastic modulus in the paramyosin transgenic lines compared to controls was reduced 1416% in myofibrils (using a 24% stretch) versus 2936% in fibers (using a 0.125% sinusoidal length perturbation at 0.5 Hz). Although this suggests a possible methodological difference (stretching versus sinusoidal perturbation), a previous fiber study showed a 2533% decrease in isometric tension for the paramyosin phosphorylation-site mutants (18
). Since similar magnitude decreases in performance are observed at the fiber level, independent of measurement technique, differences between myofibril and fiber data are most likely not due to methodological differences, but rather to the distinct structural architectures of the two systems.
| CONCLUSION |
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| ACKNOWLEDGEMENTS |
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Funding was provided by National Institutes of Health grants AR43396 to S.I.B. and R01049425 to D.W.M.
| FOOTNOTES |
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Hongjun Liu's present address is Cardiovascular Branch, National Heart, Lung, and Blood Institute, National Institutes of Health, Bldg. 10-CRC, Rm. 5-3288, 10 Center Dr., Bethesda, MD 20892.
Submitted on May 5, 2006; accepted for publication September 6, 2006.
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