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Lateral dynamics of proteins with polybasic domain on anionic membranes: A dynamic Monte-Carlo study Vladimir Kiselev PhD student The University of Edinburgh CSBE seminar, Edinburgh, UK 18 November 2010

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Electrostatics in protein- membrane interactions 20-40% +++++ +++++ +++++ +++++ PA, PS (-1) PIP2 (-4)

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Example: proteins with polybasic domain c-Src MARCKS Murray D. et al. Structure (London, England : 1993) 5, no. 8 (August 1997): 985-9 Gambhir A. et al. Biophysical journal 86, no. 4 (April 2004): 2188-207

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Endocytosis Arf6 (+) ARNO PIP2 (-4) PLD PA (-1) PIP5K AP-2 Gundelfinger E. et al. Nature reviews. Molecular cell biology 4, no. 2 (March 2003): 127-39 •  Spatial dimension: ~100 nm •  Time: ~1 s •  Feedback loops (↑+,↑-) •  Electrostatics (+,-)

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Lipid gradients in endocytosis PLD Zeniou-Meyer M. et al. The Journal of biological chemistry 282, no. 30 (July 2007): 21746-57 PI4P PIP2 PIP5K ATP ADP Iman van den B. and Nullin Divecha. Journal of cell science 122, no. Pt 21 (November 2009): 3837-50 Free choline Water Membrane - - - - - - - - - + + -

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Model setup d=0.8nm

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PS (-1) is weakly sequestered by the peptide PS (-1) density At 25-35% PS the peptide is enriched with PS only by 1.3 No PIP2 Weak sequestration of PS lipids on binary membranes Exp

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PIP2 (-4) is strongly sequestered by the peptide PIP2 (-4) density At 1% PIP2 the peptide is enriched with PIP2 by 10 The peptide sequesters mainly PIP2 lipids, but not PS Exp

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PIP2 drastically changes electrostatic properties of peptide On binary PC/PS membranes the peptide is always positive Already at 0.2% PIP2 the peptide becomes negative Peptide total charge

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The peptide diffuses mainly with PIP2 lipids but not with PS Average association time of lipids bound to the peptide Exp

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Presence of PIP2 reduces the peptide diffusion rate Binary Ternary Exp Exp

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What happens if there is a lipid gradient on the membrane? Peptide charge Value of gradient Peptide diffusion coefficient PLD PLD

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Simulations are in agreement with analytical estimations Relevant biological conditions: V = 3 µm/s ~ 10 µm Cell Time Displacement

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Addition of PIP2 switches the effect PIP2

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Continuous model 30% t = 0.2 s 13.3 times •  Dimension: ~100 nm •  Time: ~1 s Endocytosis

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Conclusions •  Model predicts formation of a “lipid shell” in the vicinity of the PB •  PB domain sequesters mainly PIP2 lipids, but not PA or PS •  PB diffusion rate weakly depends on undisturbed membrane composition •  In the presence of lipid gradient PB drifts in the region of higher lipid density – spontaneous clustering

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Future work 1) Extending the continuous model by including: –  protein membrane-cytoplasmic shuttling –  local lipid production –  protein phosphorylation/dephosphorylation 2) Modelling of endocytic triggering and feedback loops

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Thank you Acknowledgements Dr. Andrew Goryachev CSBE, UoE Dr. Davide Marenduzzo School of Physics, UoE Prof. Sir Kenneth Murray The Darwin Trust of Edinburgh $

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Experimental evidence Golebiewska et al., Mol Biol Cell 19:1663-1669, 2008 Golebiewska et al., Biophys J 91:588-599, 2006 FCS Fluorescence quenching experiments