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Circulation. 2004;109:2976-2979
Published online before print June 7, 2004, doi: 10.1161/01.CIR.0000133322.19340.EF
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(Circulation. 2004;109:2976-2979.)
© 2004 American Heart Association, Inc.


Brief Rapid Communications

In Situ Measurements of Crossbridge Dynamics and Lattice Spacing in Rat Hearts by X-Ray Diffraction

Sensitivity to Regional Ischemia

James T. Pearson, PhD; Mikiyasu Shirai, MD, PhD; Haruo Ito, PhD; Noriyuki Tokunaga, MD; Hirotsugu Tsuchimochi, PhD; Naoki Nishiura; Daryl O. Schwenke, PhD; Hatsue Ishibashi-Ueda, MD; Ryuichi Akiyama, PhD; Hidezo Mori, MD, PhD; Kenji Kangawa, PhD; Hiroyuki Suga, MD, PhD; Naoto Yagi, PhD

From the National Cardiovascular Center Research Institute, Osaka, Japan (J.T.P., M.S., N.T., H.T., N.N., D.O.S., H.I.-U., H.M., K.K., H.S.); S-I Medico-Tech Co Ltd, Kashiwara, Osaka, Japan (H.I.); Muroran Institute of Technology, Muroran, Japan (R.A.); and SPring-8/JASRI, Sayo, Hyogo, Japan (N.Y.).

Correspondence to Dr James T. Pearson, Cardiac Physiology, National Cardiovascular Center Research Institute, 5-7-1 Fujishirodai, Suita, Osaka 565-8565 Japan. E-mail jpearson{at}ri.ncvc.go.jp

Received March 1, 2004; de novo received March 31, 2004; revision received May 6, 2004; accepted May 6, 2004.


*    Abstract
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Background— Synchrotron radiation has been used to analyze crossbridge dynamics in isolated papillary muscle and excised perfused hearts with the use of x-ray diffraction techniques. We showed that these techniques can detect regional changes in rat left ventricle contractility and myosin lattice spacing in in situ ejecting hearts in real time. Furthermore, we examined the sensitivity of these indexes to regional ischemia.

Methods and Results— The left ventricular free wall of spontaneously beating rat hearts (heart rate, 290 to 404 bpm) was directly exposed to brief high-flux, low-emittance x-ray beams provided at SPring-8. Myosin mass transfer to actin filaments was determined as the decrease in reflection intensity ratio (intensity of 1,0 plane over the 1,1 plane) between end-diastole and end-systole. The distance between 1,0 reflections was converted to a lattice spacing between myosin filaments. We found that mass transfer (mean, 1.71±0.09 SEM, n=13 hearts) preceded significant increases in lattice spacing (2 to 5 nm) during systole in nonischemic pericardium. Left coronary occlusion eliminated increases in lattice spacing and severely reduced mass transfer (P<0.01) in the ischemic region.

Conclusions— Our results suggest that x-ray diffraction techniques permit real-time in situ analysis of regional crossbridge dynamics at molecular and fiber levels that might also facilitate investigations of ventricular output regulation by the Frank-Starling mechanism.


Key Words: ischemia • myocardial contraction • myosin • radiography


*    Introduction
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*Introduction
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Despite the history of studies on crossbridge dynamics, lower photon counts and poorer quality of diffraction patterns obtained from cardiac muscle than skeletal and insect flight muscles1–3 have limited progress with cardiac muscle until recently.4,5 Some of us used third-generation synchrotron radiation (SPring-8, Japan Synchrotron Radiation Research Institute) to determine x-ray diffraction patterns in excised, perfused rat hearts while moving systematically across the left ventricular (LV) equator from the epicardium through to the ventricular cavity.6

X-ray diffraction patterns of cardiac muscle produce 2 equatorial-position reflections from the lattice-like arrangement of its protein elements.2 Mass transfer of myosin heads to actin during contraction is inferred from a decrease in the integrated 1,0 reflection intensity (I1,0, lattice plane containing only thick myosin filaments) and an increase in 1,1 reflection intensity (I1,1, plane with thick myosin and thin actin filaments).7 The myocardial intensity ratio (defined as I1,0/I1,1) is minimal in the rigor state and maximal in a quiescent state.1,2,6,8

Furthermore, the distance between 1,0 reflection peaks (d1,0 spacing) represents the myosin lattice spacing, which is inversely related to sarcomere length in isolated fibers5 as static myocytes maintain a constant cell volume. Whether decreases in myofilament spacing contribute to increasing Ca2+ sensitivity and increased probability of crossbridge formation at longer sarcomere lengths has been actively debated.9 However, it is still not known if lattice spacing is regulated to maintain constant lattice volume (ie, if lattice cross-sectional area decreases with increasing sarcomere length, then interfilament spacing must decrease) during dynamic contractions in vivo.

Recently, it was shown that the intensity ratio derived from x-ray diffraction patterns of isolated whole hearts decreased during isovolumic contractions with a similar time course throughout the LV,6 implying that crossbridge cycling in fibers of different myocardial layers is similar despite differences in fiber orientation and rate of shortening. However, it was not possible to follow dynamic lattice spacing changes. In the present study, we used a fine-focused x-ray beam to record diffraction patterns of a localized region of the LV of ejecting rat hearts in situ and then determined crossbridge cycling and myosin lattice spacing.


*    Methods
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Animals and Surgical Preparation
Anesthetized (50 mg/kg sodium pentobarbital IP) male Sprague-Dawley rats (Japan SLC, Hamamatsu, Japan), 9 to 10 weeks of age (350 to 400 g), were artificially ventilated and thoractomized. Procedures were performed according to SPring-8 guidelines for the care and welfare of experimental animals. The heart was continuously irrigated while the apex was raised by a manipulator paddle and restrained by 2 superficial sutures in the LV to minimize vertical movements. Pressure-volume loops were recorded from an apically inserted 1.4F micromanometer (SPR-671 Millar Instruments) and a 1.5F conductance catheter (S-I Medico-tech Co Ltd, Osaka)10 to determine the temporal sequence of cardiac events and heart rate (determined from end-diastole [ED] interval).

X-Ray Diffraction With Collimated Synchrotron Radiation
Measurements were conducted at the 40XU beamline of SPring-8.6 A collimated quasimonochromatic beam (wavelength, 0.08 nm) with a beam flux of {approx}1012 photons per second (15 keV; ring current, 60 to 100 mA) and dimensions 0.2 x 0.2 mm was focused at an oblique tangent to the myocardium ({approx}3 m from the detector). The ventilator was stopped at end-expiration to reduce heart movements during measurements ({approx}2.1 seconds). Images were digitally recorded at a 15-ms sampling interval with the use of an image intensifier and a fast CCD camera,6 simultaneous with pressure-volume analog signals (1000-Hz sampling frequency). The beam passed through the apical myocardium between the ends of the descending branch of the left coronary artery (LAD) and the posterior interventricular vein. Final burning of the recorded region (higher energy levels) confirmed that the beam only exposed fibers in the epicardium and part of the intermediate layer (histological inspection).

Acute Ischemia Treatment
Heart baseline recordings were established, permanent ligation of the proximal LAD was performed, and recordings were repeated 5 to 10 minutes later.

Intensity Ratio Calculations and Analyses
Integrated intensity of I1,0 and I1,1 was determined from the areas under the reflection peaks after background subtraction.6 Intensity ratio (I1,0/I1,1) was used rather than absolute reflection intensities of I1,0 and I1,1,, which are influenced by changes in the quantity of fibers sampled during contractions.3 Myosin mass transfer index was defined as the difference in intensity ratio between ED and end systole (ES).


*    Results
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Mass Transfer and Lattice Spacing in Nonischemic Hearts
Intensity ratio significantly decreased during systole (increase in LV pressure [LVP] and decrease in LV volume [LVV]) and conversely, increased during diastole under the baseline rhythm (Figure 1a). Averaging intensity ratio over multiple beats reduced variability during diastole in the otherwise sinusoidal patterns (black lines, Figure 1b). With regard to time, d1,0 spacing increased continuously during systole and then decreased during diastole, suggesting that considerable changes occur in the myofilament spacing (red line, Figure 1b).



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Figure 1. Relations between calculated intensity ratio, d1,0 spacing, LVP, and LVV obtained from an LV with the use of x-ray diffraction. a and c, Consecutive records (15-ms intervals) of intensity ratio, LVP, and LVV during the baseline (a) and after LAD occlusion (c) in the same heart. b and d, Average changes in intensity ratio (black lines), d1,0 spacing (red lines), LVP, and LVV over the cardiac cycle between the ED events (derived from a and c, respectively; bars indicate SEM).

Intensity ratio averaged 2.80±0.11 (SEM, n=13 hearts) at ED, and the average myosin mass transfer index was 1.71±0.09. In all hearts, the decrease in intensity ratio during crossbridge formation was completed before the full extent of the d1,0 spacing change (2 to 5 nm between hearts, Figure 2a). Furthermore, at any given LVV, the d1,0 spacing during systole was 1 to 2 nm larger than diastole (Figure 2b).



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Figure 2. a and b, Average loops formed between d1,0 spacing, LVV, and intensity ratio during consecutive cycles (shown in Figure 1) under baseline conditions (black symbols) and regional ischemia (red symbols). Systolic (s) and diastolic (d) trajectories are indicated for baseline. c, Mean intensity ratio at ED and ES during baseline (black columns) and regional ischemia (open columns; group mean±SEM). Ischemia versus baseline, paired t test *P<0.05, ***P<0.001.

Mass Transfer and Lattice Spacing During Regional Ischemia
LAD occlusion reduced the intensity ratio change and prevented normal lattice spacing increase, consistent with reduced contractility of the ischemic region (Figure 1, c and d). Occlusion significantly increased intensity ratios at both ED (P<0.05) and ES (P<0.001) in the same LV region (n=6, Figure 2c). Although mean heart rate was not depressed (341±16 bpm, 4% increase) and there was only a small decrease in mean LV ES pressure (–26.9±5.8 mm Hg SEM), regional ischemia severely depressed the mass transfer index (55% of baseline).


*    Discussion
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*Discussion
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Our data clearly demonstrate that current synchrotron technology can produce sufficient energy to obtain well-defined reflections from single exposures to enable calculation of intensity ratio and d1,0 spacing in in situ rat hearts (Figure 1). The mean ED intensity ratio of this study is similar to 2.96 obtained from LV in arrested rat hearts under normoxic perfusion.8 Furthermore, in rat papillary muscles, the resting ratio was 3.07.1,2 The results presented here were restricted to epicardial recordings (within 0.8-mm depth), consisting of helically orientated fibers, to minimize the contributions from fibers with orientations that vary at greater depth.11 Nevertheless, it was recently established that neither diastolic intensity ratio nor mass transfer varies with depth of x-ray beam penetration in beating, perfused hearts (paced at 2 Hz).6

In Situ Changes in Myofilament Spacing
We showed that significant lattice expansion occurs during contraction and that the relation between d1,0 spacing and intensity ratio is not linear but a loop in nonischemic hearts (black line, Figure 2a). The d1,0 spacing changes during contraction (2 to 5 nm) were larger than the 1-nm difference in d1,0 spacing reported between the epicardium and endocardium (at diastole).6 Therefore, the larger d1,0 spacing change found in ejecting hearts cannot be explained by shifts in the fiber layers exposed to the beam. The loop formed by these indexes might contain valuable information about how crossbridge axial and radial forces alter the dynamics of lattice spacing changes. Crossbridge projections from the myosin backbone produce radial force perpendicular to that of axial force in the filament direction.12 Release of isometric tension in intact skeletal myofibers during sarcomere shortening causes a brief and rapid lattice spacing increase, in excess of that predicted by fiber shortening in itself.12,13 We therefore conclude that lattice volume is not constant in the dynamic state because myosin lattice spacing is significantly larger (1 to 2 nm) during contraction than ventricular filling at the same LVV (d1,0 spacing during systole greater than diastole, Figure 2b). Crossbridge formation probably causes a brief lattice expansion in ejecting hearts mediated by radial forces.

Sensitivity of In Situ Indexes to Regional Ischemia
The relevance of our new findings is that although the intensity ratio of beating hearts in diastole was similar to that of relaxed papillary muscles, there is a very different response of the myocardium in beating hearts to ischemia in terms of crossbridge dynamics and lattice space changes. Higher intensity ratios and more variable intensity ratio changes during systole (Figure 1, c and d) occurred as the result of lower absolute I1,1 in systole and a lack of consistent increase in I1,1 when I1,0 decreased (data not shown). Thus, permanent regional ischemia severely attenuated mass transfer in the epicardium (Figure 2c). Furthermore, ischemia induced increases in ED intensity ratio in vivo, whereas other studies report maximal decreases in the intensity ratio under anoxic perfusion (isolated arrested hearts)8 or rigor.1,2 An increase in intensity ratio might be related to metabolite accumulation or pronounced passive stretching, because fiber shortening in infarcted regions progressively decreases until fibers eventually become passively stretched (bulging) by fiber shortening in the nonischemic region.14 In support of the bulging possibility, we found that d1,0 spacing no longer increases between ED and ES after occlusion.

The cellular basis of the Frank-Starling law of the heart involves increases in contractility caused by length-dependent increases in Ca2+ sensitivity associated with increased ventricular filling.9 However, it is still debated whether increased crossbridge activation results from increased probability of crossbridge formation with decreasing lattice spacing associated with fiber stretching (see review in Reference 9). In a future publication, we will examine how LV volume loading influences mass transfer in relation to myofilament spacing and length-dependent activation of contraction in situ.


*    Acknowledgments
 
This work was supported by the Promotion of Fundamental Studies in Health Sciences of the Organization for Pharmaceutical Safety and Research (OPSR) and Ministerial grants Nano-001 and a Grant-in-Aid for Scientific Research. The experiments were made with approval of the SPring-8 Program Review Committee. We thank Dr Keiji Umetani for access to the Medical Imaging Center.


*    References
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMethods
up arrowResults
up arrowDiscussion
*References
 

  1. Matsubara I, Kamiyama A, Suga H. X-ray diffraction study of contracting heart muscle. J Mol Biol. 1977; 111: 121–128.[CrossRef][Medline] [Order article via Infotrieve]
  2. Matsubara I, Suga H, Yagi N. An X-ray diffraction study of the cross-circulated canine heart. J Physiol (London). 1977; 270: 311–320.[Abstract/Free Full Text]
  3. Yagi N, Saeki Y, Ishikawa T, et al. Cross-bridge and calcium behavior in ferret papillary muscle in different thyroid states. Jpn J Physiol. 2001; 51: 319–326.[CrossRef][Medline] [Order article via Infotrieve]
  4. Konhilas JP, Irving TC, de Tombe PP. Myofilament calcium sensitivity in skinned rat cardiac trabeculae: role of interfilament spacing. Circ Res. 2002; 90: 59–65.[Abstract/Free Full Text]
  5. Irving TC, Konhilas J, Perry D, et al. Myofilament lattice spacing as a function of sarcomere length in isolated rat myocardium. Am J Physiol. 2000; 279: H2568–H2573.
  6. Yagi N, Shimizu J, Mohri S, et al. X-ray diffraction from a left ventricular wall of rat heart. Biophys J. 2004; 86: 2286–2294.[Abstract/Free Full Text]
  7. Huxley HE, Brown W. The low-angle x-ray diagram of vertebrate striated muscle and its behaviour during contraction and rigor. J Mol Biol. 1967; 30: 383–434.[Medline] [Order article via Infotrieve]
  8. Sowerby AJ, Harries J, Diakun GP, et al. X-ray diffraction studies of whole rat heart during anoxic perfusion. Biochem Biophys Res Commun. 1994; 202: 1244–1251.[CrossRef][Medline] [Order article via Infotrieve]
  9. Konhilas JP, Irving TC, de Tombe PP. Frank-Starling law of the heart and the cellular mechanisms of length-dependent activation. Pflugers Arch. 2002; 445: 305–310.[CrossRef][Medline] [Order article via Infotrieve]
  10. Ito H, Takaki M, Yamaguchi H, et al. Left ventricular volumetric conductance catheter for rats. Am J Physiol. 1996; 270: H1509–H1514.[Medline] [Order article via Infotrieve]
  11. Streeter DD Jr, Spotnitz HM, Patel DP, et al. Fiber orientation in the canine left ventricle during diastole and systole. Circ Res. 1969; 24: 339–347.[Abstract/Free Full Text]
  12. Cecchi G, Bagni MA, Griffiths PJ, et al. Detection of radial crossbridge force by lattice spacing changes in intact single muscle fibers. Science. 1990; 250: 1409–1411.[Abstract/Free Full Text]
  13. Bagni M, Cecchi G, Griffiths P, et al. Lattice spacing changes accompanying isometric tension development in intact single muscle fibers. Biophys J. 1994; 67: 1965–1975.[Abstract/Free Full Text]
  14. Lew WYW, Chen Z, Guth B, et al. Mechanisms of augmented segment shortening in nonischemic areas during acute ischemia of the canine left ventricle. Circ Res. 1985; 56: 351–358.[Abstract/Free Full Text]



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