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Taida: March 3, 2015 Membrane Biophysics & Soft Matter Physics Huey W. Huang Rice University, Physics & Astronomy http://hwhuang.rice.edu The talk is about Proteins interacting with membranes. Physical process rather than


  1. Taida: March 3, 2015 Membrane Biophysics & Soft Matter Physics Huey W. Huang Rice University, Physics & Astronomy http://hwhuang.rice.edu

  2. The talk is about • Proteins interacting with membranes. • Physical process rather than chemical reactions. • Functions of proteins in membranes are well defined, in fact by phase transitions. • Unsolved problems.

  3. Subject • Membrane-active Antibiotics , often called antimicrobial peptides (AMPs). This talk is the story of how we found out how AMPs work. What is the significance of AMPs? What is the physics problem? • Unsolved membrane problems Recently a 2 nd kind of AMPs were discovered. Alzheimer’s disease, mad cow disease, type II diabetes and other neurodegenerative diseases could also be membrane problems.

  4. Cell Membranes target of membrane- active antibiotics target of conventional antibiotics The red part is a lipid bilayer. C. elegans

  5. Bacterial membranes E Coli Filament Stop Solution 77% Stop Solution 55% Stop Solution 32% Stop Solution 15% Stop Solution

  6. Cell membranes are not simple. - D P Bar=2.5um Live cell Dead cell Biophys J. 107, 2082 (2014)

  7. It is very difficult to know what happens when an antibiotic attacks a bacteria except that it kills. After Diffusion: LL-37 6uM+40% Stop Solution 5+0.5min 5+12.2min 5+8.8min 5+17.5min 5+20.7min 5+4.5min 5+12.4min

  8. Model membranes and This is the problem: AMP 5nm Soft! Vesicle A typical antibiotics or AMP (melittin) 1 nm X 2-3 nm

  9. Model membrane attacked by membrane-active antibiotics 30 m m Red - D P dye Green PNAS 110, 14243 (2013)

  10. Parallel Multilayers of Membranes side view top view Multilayers (smectics) Liposomes (vesicles)

  11. Neutron scattering in-plane scattering

  12. Using D 2 O to show the water pores perdeuterated lipid with H 2 O or D 2 O Natural lipid with D 2 O or H 2 O H 2 O D 2 O H 2 O D 2 O Biophys. J. 70,, 2659 (1996)

  13. Analysis of neutron scattering from fluid membranes 2 I  F ( q ) S ( q ) r r S ( r q ) 2 Pore size ~4.4 nm diameter F ( r q ) 4-7 melittin in the pore

  14. Phase transition by dehydration dehydration Biophys. J. 79, 2002 (2000)

  15. Diffraction by molecular crystalline Diffraction by soft matter crystals Same S ( q ), but Ex. 1D constant density In the unit cell q

  16. Anomalous Diffraction for centrosymmetric structures   q q r q r       n n F ( ) f exp( i ) ( f f ' if " ) exp( i ) k  j j j k  f ' if "   F F o 2 n f

  17. Multiwavelength Anomalous Diffraction (MAD) Method di18:0(9,10Br)PC f ' ' ~ 0 . 1 f '   JACS 128, 1340 (2006)

  18. Solving F 0 and F 2

  19. F 0 and F 2 Complete electron density Label only electron density

  20. Only one AMP forms pores of the (barrel-stave model) PNAS 105, 17379 (2008)

  21. All AMPs except one form pores of the (toroidal model) A topological question! PNAS 105, 17379 (2008) PNAS 110, 14243 (2013)

  22. Physics of pore formation in membranes • But why do the antibiotics make pores when D A/A exceeds ~4%? • Note that making pores when D A/A exceeds ~4% represents a concentration on-off switch. • All biological on-off switches are by concentrations!

  23. The biggest problem in membrane biophysics is: How to detect the physical state of proteins in membranes? Method 1: Oriented circular dichroism JCP 89, 2531 (1988) BJ 57, 797 (1990) We measured the orientation of helices as a function of antibiotic concentration. Method 2: Lamellar diffraction We measured the membrane thickness as a function of antibiotic concentration. BJ 68, 2361 (1995) Biochemistry 34, 16764 (1995); BJ 84, 3751 (2003)

  24. We detected a critical concentration.

  25. Physics of pore formation in a thin layer E o 2       2 R R R  /   E  R Litster, Phys. Rev. Lett. A35, 193 (1975) Taupin et al. Biochemistry 14, 4771 (1975)

  26. Phase transition as a function of P/L. E o      2  2 R R R P/L*  o  K ( A / A )( P / L ) a P L P/L<P/L* (for P/L>P/L*)    ( / )( ) / K A A P P L a P L I P/L>P/L*    R o P N 2 R  I p 2 2 3           2 ( 4 / 3 ) ( / ) E R R R N P  R o o p Phys. Rev. Lett. 92, 198304 (2004)

  27. With this understanding, we can now go back to the case of live cells. - D P Bar=2.5um Live cell Dead cell 5+0.5mi 5+8.8mi 5+12.2 5+17.5 5+20.7 5+4.5mi 5+12.4 n n min min min n min

  28. of pore formation story Although the pore-forming antibiotics have not yet been approved as drugs.

  29. The 2 nd kind of membrane-acting antibiotics (daptomycin) do not make pores. Daptomycin, Ca ++ Ca ++ dye 1.02 6 D A/A 1.01 4 1 2 0.99 0 Intensity 0.98 -2 control 0.97 -4 intensity 0.96 -6 dA/A 0.95 -8 0.94 -10 0.93 -12 No leakage 0 100 200 300 Time (s) Biochemistry 53, 5384 (2014)

  30. Amyloidoses (one of the most important medical problems) Alzheimer’s disease Type II diabetes Mad Cow disease Parkinson’s diesease other ~20 amyloidoses

  31. Common characteristics of amyloidoses • Each disease is strongly correlated with a protein. • The disease is associated with the presence of protein plagues. • But the fibrils and plagues do not harm cells.

  32. Characteristics II (somewhat controversial) • Protein-membrane interactions turn the proteins into the plaques. During this interaction something happens to the cell membranes. But how?

  33. We need experimental tools to study proteins in membranes.

  34. Acknowledgement Rice University : Collaborators : Glenn Olah (Los Alamos) Lin Yang (NSLS) Yili Wu Shuo Qian (ORNL) Ming-Tao Lee Ke He (Shell) (NSRRC) Steve Ludtke (Baylor MC) Wei-Chin Hung William Heller (ORNL) (Mil.Acad.tw) Thad Harroun (Brock U) Lin Yang (NSLS) SUPPORTED by : Thomas Weiss (SSRL) Lai Ding (Tuft) Wangchen Wang (Baylor MC) Shuo Qian (ORNL) Yen Sun (Harvard/Rice) Chang-Chun Lee (CGG) Tzu-Lin Sun

  35. Method of Oriented Circular Dichroism JCP 89, 2531 (1988) BJ 57, 797 (1990)

  36. Above a critical concentration (P/L)*, Peptide orientation changes with (P/L) All pore-forming peptides S studied showed critical orientation transitions. I BJ 82, 908 (2002)

  37. Membrane Thinning Effect Membrane thinning and peptide orientation change have the same critical concentration. BJ 68, 2361 (1995); Biochemistry 34, 16764 (1995); BJ 84, 3751 (2003)

  38. Peptide-induced pores are stable.   2  3 E R c R c R c R P/L* 1 2 3 P/L<P/L* 2    R o ( c 3 c ) ( c 3 c ) ( c / 3 c ) 2 3 2 3 1 3 P/L>P/L* c 1 =2  decreases with P/L . R o       c / 3 c 3 ( P / L ) 4 ( N / L ) 3 . 1 nm  2 p R o ~1-2nm Phys. Rev. Lett. 92, 198304 (2004)

  39. The diseases are each associated with the presence of plagues (fibrils) of one particular protein that misfolds.

  40. The disease is strongly correlated with the protein. b -cells co-secret insulin and amylin (an amyloid protein). Human amylin and rat amylin differ by a few amino acids. Human has diabetes; rat has not. But if the rat gene is modified to human gene, rat develops diabetes. Mad cow disease (bovine spongiform encephalopathy) can be transmitted to human beings by eating the animal protein.

  41. Penetratin binds to the membrane and comes out. Biophys. J. 98, 2236 (2010)

  42. Penetratin in membranes Peptide donformation change: CD vs. P/L

  43. A topological question.    2       H dA [ c c c c c ] 1 2 o 1 2 Helfrich (1973) 2 Gauss-Bonnet Theorem (for a closed surface)

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