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The Dynamics of Intracellular Ca2+ Signals
Jianwei Shuai, Ohio University The Dynamics of Intracellular Ca2+ Signals Jianwei Shuai (帅建伟) Department of Physics Xiamen University GRC Nonlinear Science in Mt. Holyoke College
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Outline Introduction IP3R Ca2+ channel model
Ca2+ blips with single IP3R Ca2+ channel Ca2+ puffs with clustered Ca2+ channels Ca2+ waves at the global cell level Summary
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Fixed Ca2+ via Moving Ca2+
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Moving Calcium Ions In-between: Life beginning Life ending
A life and death signal in cells Life beginning Sperm Ca2+ Oscillation Cell Division Egg Life ending High Calcium Concentration protein-digesting enzymes Cell Death In-between: Brain memory Ca2+-related diseases: Cancer, Alzheimer’s Communication between cells, Communication among different organelles within a cell
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Cell Structure
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Ca2+ Release Dynamics Cytosol ER IP3R IP3 Membrane [Ca]Local>10mM
Pump IP3R ER Cell Membrane Pump
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Ca2+-induced Ca2+ release propagates Ca2+ waves
Cytosol Membrane ER Low [Ca] opens the IP3R channels: fast binding; High [Ca] inhibits the IP3R channels: slow binding.
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How does Ca2+ act as a cellular signal?
Ca2+ concepts Ca2+ Concentration Ca2+ Oscillation Spatiotemporal Ca2+ wave Cellular information is encoded by the spatiotemporal Ca2+ patterns (e.g. frequency and amplitude of oscillation). Ca2+ Signal
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Technique to Visualize Cytosolic Ca2+
Calcium Fluorescence dye Green light Blue light Blue light Blue light
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Ca2+ spreading wave Ian Parker, UC Irvine
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Lechleiter, Girard, Peralta and Clapham, Science, 1991
Ca2+ spiral wave Lechleiter, Girard, Peralta and Clapham, Science, 1991
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Fine structure underlying Ca2+ waves
Marchant & Parker, EMBO J. 1999
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Ca2+ waves consist of puffs
Ca2+ waves at higher [IP3] Local Ca2+ puffs at low [IP3] Marchant & Parker, EMBO J. 1999
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Jianwei Shuai, Ohio University
Puff is triggered by blip Blip Puff Temporal Profile Heather, Dargan, Shuai and Parker, Biophys J. 2006 GRC Nonlinear Science in Mt. Holyoke College
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Multi-scale Ca2+ Signals
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Single IP3R Channel Model
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- The IP3R channel model + +
Three independent and equivalent subunits. Each subunit IP3 + Ca - has 8 states: 110 IP3 + Ca The open subunit is Channel is open when 3 subunits are open DeYoung & Keizer, PNAS 1992
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Tetrameric Structure of IP3R
Hamada, et al, JBC 2003
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IP3R model with 4 Subunits
Each channel has four independent and equivalent subunits. IP3 Open Channel 3 active subunits 4 active subunits
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The IP3R model with conformational change
Shuai, et al, Biophys J. 2007
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Ca2+ Blips with Single IP3R Channel
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Model Design 6mm Mobile Buffer 6mm Immobile Buffer Free Ca2+ 6mm
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Markovian simulation of channel dynamics
Stochastic binding/unbinding dynamics: IP3 100 Random Number ? 110 a5[Ca]dt a2[Ca]dt 1 b1dt b1dt a2[Ca]dt a5[Ca]dt IP3 - Ca 101 IP3 + Ca 110 000 Shuai & Jung, Biophys J 2002
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[Ca2+] distribution around the channel mouth
400mM [Ca2+] mM 20mM [Ca2+]~400mM [Ca2+]~20mM 15nm Cytosol ER
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Effects of Ca2+ Buffers Shuai, et al, Biophys J. 2008
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Slower Decay of [Ca2+] due to Immobile Buffer
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Faster Decay of [Ca2+] with Mobile Buffer
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Ca2+ Puffs with Clustered IP3R channels
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Puff Model L L : Cluster width N : Total number of open
6mm 6mm L Immobile Buffer L : Cluster width N : Total number of open channels during a puff Free Ca2+ EGTA Fluo4 Dextran 6mm
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A Cluster of 9 IP3Rs
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Effects of Immobile Buffers
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Effects of Fast Mobile Buffer
[BAPTA] mM
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[Ca2+] in the Cluster Time (ms)
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Modified [Ca2+] by BAPTA
[BAPTA] mM Ruediger, Shuai, et al, Submitted
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Conclusion 1 Ca2+ Buffers function differently at single and clustered channel levels. The open probability for a single IP3R: increases with increasing immobile buffer has little change with the mobile buffer The open probability for a clustered IP3Rs: has little change with the immobile buffer shows a biphasic mode with the increase of fast mobile buffer (BAPTA).
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Ca2+ Waves at Global Cell Level
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Ca2+ wave model Cytosol ER Channel cluster Free Ca2+ Stationary Buffer
Mobile Buffer Channel cluster ER
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A stochastic Ca2+ model with clustered channels
y x Cluster distance 3 mm Each cluster 36 channels
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With low [IP3] stimulus ? [Ca2+] [IP3]
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What will happen if we change cluster distributions?
Cell size: Cluster distance 0.5 mm Each cluster 1 channel Cluster distance 3 mm Each cluster 36 channels Cluster distance 5 mm Each cluster 100 channels Total channels: 14,400 Fixed !!!
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No wave with low [IP3] at small cluster distance
Cluster distance 0.5 mm Each cluster 1 channel
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No wave with low [IP3] at large cluster distance
Cluster distance 5 mm Each cluster 100 channels
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At middle cluster distance Ca2+ waves generated with low [IP3]
Cluster distance 3 mm Each cluster 36 channels
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Noise-induced Ca2+ waves
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From Stochasticity To Periodicity at biologically realistic cluster distribution
Channel number per Cluster Characteristic time of self-correlation T Shuai and Jung, PNAS 2003
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With high [IP3] stimulus
? [Ca2+] [IP3]
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Puff-induced Ca2+ waves
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Bifurcation of calcium signal
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+ Interaction of channel noise and IP3 noise Channel noise only
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Restoration of Periodicity by Noise Suppressing Noise
Liao, Jung, Shuai, PRE (2009)
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The novel roles of molecular noise in Ca2+ system
Conclusion 2 The novel roles of molecular noise in Ca2+ system At resting state with low [IP3] concentration: The channel noise with clustered IP3Rs can generate the periodic Ca2+ waves At oscillatory state with high [IP3]: The channel noise will destroy the periodic Ca2+ oscillation The additional IP3 noise with certain strength can partly restore the periodicity of Ca2+ signals.
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Summary
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Thanks University of California, Irvine Prof. Ian Parker
Los Alamos National Lab John E. Pearson Ohio University Prof. Peter Jung NSF China ( ) NIH USA ( ) University of Pennsylvania Prof. J. Kevin Foskett Dr. Don-On Daniel Mak Humboldt-Univeristy at Berlin Dr. Sten Ruediger
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