Volume 99, Issue 4, Pages (November 1999)

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Volume 99, Issue 4, Pages 421-431 (November 1999) Tomographic 3D Reconstruction of Quick-Frozen, Ca2+-Activated Contracting Insect Flight Muscle  Kenneth A Taylor, Holger Schmitz, Mary C Reedy, Yale E Goldman, Clara Franzini-Armstrong, Hiroyuki Sasaki, Richard T Tregear, Kate Poole, Carmen Lucaveche, Robert J Edwards, Li Fan Chen, Hanspeter Winkler, Michael K Reedy  Cell  Volume 99, Issue 4, Pages 421-431 (November 1999) DOI: 10.1016/S0092-8674(00)81528-7

Figure 1 Fiber Mechanics and EM of HST (A) Tension records during isometric contraction of the single IFM fiber used for the tomogram, up to the moment of freezing. The slow time base (at left) shows that flushing the relaxed fiber at A* with high Ca2+-activating solution gave a steep force rise. The resulting HST plateau persisted while freezing head was mounted on the guide rod. Faster time base (center and right) shows the absence of stretch activation in response to length pulses followed by sustained tension during the 170 ms drop. (B) Projection of the tomogram of a myac layer from the freeze-substituted HST fiber. Squares outline mask motifs that repeat every 116 nm. (C) Column averaging of the area in (B) enhances the 14.5 nm shelves of density on the thick filament (white lines) and the periodic distribution of crossbridges along the actin filament. Arrows point to troponin beads on the thin filament. Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 2 X-Ray Diffraction from IFM in HST Graphs compare intensity for three groups of crossbridge-associated reflections in five states, ordered left to right from relaxed through contraction to rigor. Data for non-HST states are from Tregear et al. 1998. HST values (fourth column) are nearer to rigor values than stretch activation (third column), suggesting more crossbridge attachment and consistent with the greater force in HST (340 μN/fiber) versus stretch activation (230 μN/fiber). (A) Axial dispersion or numerical depletion of relaxed myosin head array is shown by decrease in 14.5 and 7.2 nm meridionals. (B) Crossbridge attachment to target zones on thin filaments is signaled by rise of 10.12 versus decline of 10.6 intensity. (C) Overall crossbridge attachment on thin filaments is signaled by rise in two of three outer reflections on 38.7 nm layer line. For the location of the reflections within the diffraction pattern, and the theoretical basis of the deductions made in the present text, see Tregear et al. (1988). Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 3 Tomogram of HST (A) Surface rendering of ∼25% of one unaveraged tomogram (copper color). Some mask motifs are boxed in blue. (B) Column average (gold color) is superimposed in phase with the unaveraged reconstruction. m, myosin filament; a, actin filament; t, troponin. Z disk is at the bottom. Blue lines indicate crossbridge angle. Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 4 Rebuilt Fittings of the Acto-S1 Atomic Model into the Tomogram The color scheme in all fittings is as follows: actin strands are green and blue, unmodified rigor S1 is yellow, rebuilt S1 is red, and unmodified Holmes pre-stroke S1 is cyan. The rebuilt S1 is superimiposed on either rigor S1 or pre-stroke S1 as appropriate to LCD angle. Transverse views look toward the Z line. (A) Pair of ∼90° crossbridges and rebuilt S1 compared to the Rayment rigor model. (B) Transverse view of (A). In this 90° motif, the bridging density across the thin filament is less sigmoid than that in other 90° motifs. (C) Pair of “V-shaped” crossbridges with the LCD oriented at ∼110° compared to Holmes prestroke S1. (D) Transverse view of (C). Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 5 Acto-S1 Atomic Models Fitted to Partial Mask Motif (A) Partial mask motifs with rebuilt rigor S1 compared with either rigor or pre-stroke S1 models. M-ward and Z-ward denote bridge position relative to M and Z lines. (B) Transverse view of M-ward crossbridges. (C) Transverse view of Z-ward crossbridges. Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 6 Superposition of All 26 Rebuilt S1s (A) Longitudinal view; Z disk at bottom. (B) Transverse view, looking toward Z line. Myosin heavy chain is red, essential light chain is magenta, regulatory light chain is cyan, and unmodified rigor S1 is all yellow. Actin strands are green and blue. (C) Plot f axial tilt angles (βMD and βLCD) versus axial coordinate (ZLys-843) for the rebuilt S1s. Filled triangles (red) are βLCD, filled triangles (blue) are βMD for stage 1, and filled boxes (black) are βMD for stage 2. The origin for ZLys-843 is rigor. Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)

Figure 7 Possible Working Stroke Illustrated by a Sequence of Rebuilt S1s in HST The selected S1s encompass the range of structures found in HST. Other possible sequences illustrate different details but the same general trend. Each rebuilt S1 is shown in longitudinal view (Z disk toward the bottom) on the left and in transverse view on the right (toward the Z disk). The color scheme is the same as in Figure 6A and Figure 6B. (A) Initial actomyosin contact, probably weak binding. (B) MD rotation on actin, both azimuthally and axially, toward the rigor interface. (C) The MD is close to the rigor interface, and the LCD is angled at ∼124°. The MD is close to the azimuthal position of rigor S1. Tension may be developing. (D) The MD is in the rigor orientation on actin, and the light chain is angled at ∼100°. Many bridges are in this configuration in the fittings. (E) The LCD has tilted to a 71° rigor angle at the end of the working stroke. Cell 1999 99, 421-431DOI: (10.1016/S0092-8674(00)81528-7)