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This study explores the localization of cell division proteins, specifically DivIVA and its interaction with membranes in bacteria like Bacillus subtilis. We investigate potential mechanisms of protein binding to curved membranes, cell division proteins, and lipid species. Using advanced techniques like Biacore and Monte Carlo simulations, we analyze the affinity for membrane curvature and the structural implications of DivIVA oligomers. The findings offer insights into protein clustering, membrane interactions, and the underlying principles of bacterial cell division.
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How do proteins localize to cell poles ?(DivIVA as model system) DivIVA-GFP
(lack of) Information from secondary structure prediction 164 amino acids, mostly helical secondary structure prediction by PSIPRED coiled coil prediction by LUPAS multimerization via coiled coil regions
Possible mechanisms: 1) binding to another (cell division) protein 2) binding to a specific lipid species 3) affinity for curved membranes
20 % membrane vesicles 30 % 70 % Binding to another (membrane) protein? DG = DivIVA-GFP V = membrane vesicles Lip = liposomes D = DivIVA G = GFP
amphipathic helix of N-terminus (60 aa) Biacore (surface plasmon resonance) with L1-chip T = min
Possible mechanisms: 1) binding to another (cell division) protein 2) binding to a specific lipid species 3) affinity for curved membranes Edwards, 2000, EMBO
Cardiolipin Domains in Bacillus subtilis Kawai, 2003, J. Bac.
DivIVA localization in B. subtilis strains lacking certain lipids wt - PG -PE - CL
Possible mechanisms: 1) binding to another (cell division) protein 2) binding to a specific lipid species 3) affinity for curved membranes
Affinity for curvature = induces curvature ‘BAR domains as sensors or membrane curvature’ Peter et al., 2004, Science
Affinity for curvature = induces curvature ‘BAR domains as sensors or membrane curvature’ Peter et al., 2004, Science
DivIVA D D D D D D D D D liposomes Induction of curved membranes ? liposomes + DivIVA liposomes 200 nm
Possible mechanisms: 1) binding to another (cell division) protein 2) binding to a specific lipid species 3) affinity for curved membranes ?
Does curvature really not play a role? B. subtilis E. coli
E. coli division mutant MHD63
Possible mechanisms: 1) binding to another (cell division) protein 2) binding to a specific lipid species 3) affinity for curved membranes….., but not as we know it
Ø ~ 25 nm Higher order DivIVA structures ‘Doggy bones’ Stahlberg, 2004, Mol. Mic. ( Cryo-negative stain EM )
? ~ 25 nm ? Ø ~ 100 nm Conceptual simplification:
‘Molecular Bridging’ 1) self interaction (clustering) of subunits 2) subunits should be large (relative to curvature) 3) membrane interaction (weak) - no other proteins / lipids / or curved proteins necessary -
Monte Carlo simulation • Rules: • - cylinder 1 x 4 µm • - DivIVA oligomers (green) = spheres of 25 nm diameter • - curvature of membranes at transition from lateral wall to sides = diameter of 100 nm • - spheres can make max 8 contacts (doggy bone contains at least 8 DivIVA molecules) • 2 membrane contacts maximal (based on our EM data) • Epp and Epm in the range 1.5-6 k bT • (equivalent to 1-4 kcal/mol) ~in range of typical weak protein-protein attractions
- spheres can make 8 contacts - 2 membrane contacts maximal - spheres can make 4 contacts - no limitations in membrane contacts
d = 50 nm d =100 nm - No restrictions in nr. of interactions Epp = 2 k bT Epm = 6 k bT - 4 pp bonds - membrane contact = 1 pp contact Epp = 2.5 k bT Epm = 5.5 k bT
d = 50 nm d =100 nm • - max 4 pp bonds • - membrane contact • = 2 pp contact • Epp = 3 k bT • Emp = 5.5 k bT • max 6 pp bonds • membrane contact • = 3 pp contacts • Epp = 3.5 k bT • Epm = 5.5 k bT
Max 8 pp bonds • membrane contact • = 4 pp contacts • Epp = 3.5 k bT • Epm = 5.5 k bT d = 50 nm d =100 nm
CBCB - Newcastle University Rok Lenarcic Ling Wu Jeff Errington Sven Halbedel University of Oxford Wouter de Jong LoekVisser Michael Shaw University of Edinburgh Davide Marenduzzo