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DIFFRACTION IMAGING OF THE MYOSIN
SUPERLATTICE OF VERTEBRATE MUSCLE

Rick Millane, David Wojtas, Chunhong Yoon* and John Squire+

        Department of Electrical and Computer Engineering
                    University of Canterbury

 *Department of Physics, University of Wisconsin - Milwaukee, USA

          +Department  of Physiology and Pharmacology
                  University of Bristol, Bristol, UK


           New Zealand Institute of Physics Conference
                Wellington, 17-19 October 2011

             Supported in part by the Marsden Fund

                                                                    1
Outline


•   Myosin lattice of vertebrate muscle
•   Electron microscopy and x-ray fibre diffraction
•   Image analysis
•   Disordered systems – frustration – statistical physics
•   X-ray diffraction
•   Conclusions




                                                             2
Imaging and diffraction imaging


Microscopy

  light

electrons



              specimen     FT lens         image

Diffraction Imaging
 x-rays
                                       computer
electrons


                                                   image
              specimen   diffraction
                          pattern
                                                           3
Myosin lattice




Muscle fibre




myofibril



sarcomere




                                4
Myosin lattice




Simple lattice                 Superlattice
                            Rotational disorder




                                                  5
Electron microscopy and image analysis




                                         Close up



Cross-section of sarcomere


                             Template
               Template      for
               for           rotations
               locations


                                                    6
Classification of orientations




                                 7
Distribution of orientations




                               8
Geometrically frustrated systems

A spin system, for example, for which as, a result of lattice topology,
the energy of each spin pair cannot be simultaneously minimised.

A very simple classical example is a triangular lattice with
antiferromagnetic interactions.

I.e. “unlike’ spins, or states, are energetically preferred.

It is not possible to satisfy the constraints on each elementary
plaquette of the lattice.

Leads to a large number of ground states.
                                                                   ?

This is the triangular Ising antiferromagnet – TIA.

Characterised using spin-pair correlations.



                                                                          9
TIA correlations



Different
temperatures




Partitioned into
two sublattices




                                      10
Spatial correlations – myosin lattice and TIA




           Observed – myosin lattice
           TIA by Monte Carlo simulation


                                                11
Myosin lattice disorder – measured and simulated




             Myosin lattice   TIA




                                                   12
X-ray fibre diffraction patterns from muscle




                                               13
Fibre diffraction pattern from relaxed frog muscle




         Iwamoto et al., Biophys. J., 85, 2492-2506 (2003).


                                                              14
Measured diffraction data – layer line amplitudes




                                                    15
Simulation of x-ray diffraction from the myosin array



   Develop methods to simulate x-ray
   diffraction from models of the
   myosin filament.

   Need to incorporate:

   The molecular structure and helical
   symmetry.

   The TIA disorder.

   Cylindrical averaging.




                                                    16
Calculated diffraction – ordered crystalline specimen




                                                    17
Calculated diffraction – completely disordered




                                                 18
Calculated diffraction – TIA disorder




                                        19
Summary

• The superlattice disorder observed in the myosin
  lattice of higher verebrate muscle is a manifestation of
  a frustrated system.
• The frustration is due to incompatible preferred
  interactions between the myosin filaments.
• This may have evolutionary significance for muscle
  function.
• Direct (electron microscopy) and diffraction (x-ray
  diffraction) imaging complement each other.
• Effects of disorder can be incorporated into diffraction
  calculations to allow rigorous analysis of diffraction
  data.
• Engineers and biophysicists can work productively
  together and have lots of fun!




                                                             20

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14.04 o14 r millane

  • 1. DIFFRACTION IMAGING OF THE MYOSIN SUPERLATTICE OF VERTEBRATE MUSCLE Rick Millane, David Wojtas, Chunhong Yoon* and John Squire+ Department of Electrical and Computer Engineering University of Canterbury *Department of Physics, University of Wisconsin - Milwaukee, USA +Department of Physiology and Pharmacology University of Bristol, Bristol, UK New Zealand Institute of Physics Conference Wellington, 17-19 October 2011 Supported in part by the Marsden Fund 1
  • 2. Outline • Myosin lattice of vertebrate muscle • Electron microscopy and x-ray fibre diffraction • Image analysis • Disordered systems – frustration – statistical physics • X-ray diffraction • Conclusions 2
  • 3. Imaging and diffraction imaging Microscopy light electrons specimen FT lens image Diffraction Imaging x-rays computer electrons image specimen diffraction pattern 3
  • 5. Myosin lattice Simple lattice Superlattice Rotational disorder 5
  • 6. Electron microscopy and image analysis Close up Cross-section of sarcomere Template Template for for rotations locations 6
  • 9. Geometrically frustrated systems A spin system, for example, for which as, a result of lattice topology, the energy of each spin pair cannot be simultaneously minimised. A very simple classical example is a triangular lattice with antiferromagnetic interactions. I.e. “unlike’ spins, or states, are energetically preferred. It is not possible to satisfy the constraints on each elementary plaquette of the lattice. Leads to a large number of ground states. ? This is the triangular Ising antiferromagnet – TIA. Characterised using spin-pair correlations. 9
  • 11. Spatial correlations – myosin lattice and TIA Observed – myosin lattice TIA by Monte Carlo simulation 11
  • 12. Myosin lattice disorder – measured and simulated Myosin lattice TIA 12
  • 13. X-ray fibre diffraction patterns from muscle 13
  • 14. Fibre diffraction pattern from relaxed frog muscle Iwamoto et al., Biophys. J., 85, 2492-2506 (2003). 14
  • 15. Measured diffraction data – layer line amplitudes 15
  • 16. Simulation of x-ray diffraction from the myosin array Develop methods to simulate x-ray diffraction from models of the myosin filament. Need to incorporate: The molecular structure and helical symmetry. The TIA disorder. Cylindrical averaging. 16
  • 17. Calculated diffraction – ordered crystalline specimen 17
  • 18. Calculated diffraction – completely disordered 18
  • 19. Calculated diffraction – TIA disorder 19
  • 20. Summary • The superlattice disorder observed in the myosin lattice of higher verebrate muscle is a manifestation of a frustrated system. • The frustration is due to incompatible preferred interactions between the myosin filaments. • This may have evolutionary significance for muscle function. • Direct (electron microscopy) and diffraction (x-ray diffraction) imaging complement each other. • Effects of disorder can be incorporated into diffraction calculations to allow rigorous analysis of diffraction data. • Engineers and biophysicists can work productively together and have lots of fun! 20