Wave Pinning, Actin Waves, and LPA

51
Wave Pinning, Actin Waves, and LPA MCB 2012 William R. Holmes Monday, 14 May, 12

Transcript of Wave Pinning, Actin Waves, and LPA

Page 1: Wave Pinning, Actin Waves, and LPA

Wave Pinning, Actin Waves,

and LPA

MCB 2012William R. Holmes

Monday, 14 May, 12

Page 2: Wave Pinning, Actin Waves, and LPA

Intercellular Waves

• Dynamic Hem1 waves in neutrophils

Weiner et al., 2007, PLoS Biology

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Questions?

• How can such waves / pulses form?

• What molecular constituents play a role?

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FitzHugh Nagumo Idea

• Positive feedback induces a wave.

• Slower negative feedback yields a pulse.

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FitzHugh Nagumo

• Used to describe signal propagation in nerves.

• v = membrane voltage

• w = ion concentration

vt = v � v3 � w + I +Dv4v,

⌧wt = v � bw � a

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FitzHugh Nagumo

• Stable HSS leads to transient dynamics.

Stable HSS

v-nullcline

w-nullcline

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FitzHugh Nagumo

• Unstable HSS leads to a limit cycles and persistent dynamics

Unstable HSSw-nullcline

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FN Feature

• Stable HSS = transient excitable dynamics

• Unstable HSS = unstable persistent dynamics

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Relationship to cell dynamics

• Cells are not always all or nothing.

• Some cells exhibit dynamics even after a stimulus is removed.

• Some cells are excitable and persistent.

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FN Extionsion

• We will consider an augmentation of the standard FN framework.

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Hypothesis

• We still consider a basic ‘wave generator + refractory feedback’ model.

• Wave Generator = Actin Regulators

• Refractory feedback = Actin

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Hypothesis

• Polarity proteins such as GTPases or Phosphoinositides serve as a wave generator.

• Actin polymerization inactivates these proteins acting as a refractory feedback.

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Wave Generator

• Consider a wave pinning (WP) model indicative of GTPase function.

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Wave Generator : GTPases

• NPF = actin nucleating protein

• Exists in 2 forms.

• Only the active NPF nucleates F-Actin

Active NPFInactive NPF

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Model Features

• Primary features

• Slow Fast Diffusion

• Autocatalysis

• Conservation

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Wave Pinning: Equations

f(u, v) = v(k0 +�un

Kn + un)� �u

ut(x, t) = f(u, v) +Du4u

vt(x, t) = �f(u, v) +Dv4v

u

vDu ⌧ Dv

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LPA Reductionult(t) = f(ul, vg)

ugt (t) = f(ug, vg)

vgt (t) = �f(ug, vg)

ulug

vg

ug

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Conservation Reduction

• Assume the perturbation is highly localized.

Zu

g(t) + v

g(t) dx ⇡Z

u(x, t) + v(x, t) dx = C

• So vg(t) = T � ug(t)

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LPA System

ulug ug

ult(t) = f(ul, T � ug)

ugt (t) = f(ug, T � ug)

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Wave Pinning LPA

Local Branch

Well MixedBranch

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Wave Pinning: Stability

Stable HSS Stable HSS

Turing Unstable

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Wave Pinning: Stability

Stable HSS Stable HSS

Turing Unstable

Threshold

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Wave Pinning: Stability

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Wave Pinning

• + feedback yields a threshold response

• Conservation causes stalling.

• As the wave propagates, it depletes the inactive NPF

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Wave Pinning:Simulations

Wave Pinning+ Perturbation

Wave Pinning- Perturbation

TuringNoise

Active NPF

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Wave Pinning:Wave Generator

• We will assume this WP model acts as a wave generator.

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Refractory Feedback

• Polarity related proteins (GTPases) nucleate actin and initiate a wave.

• Growing actin ‘inactivates’ these proteins.

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Actin Wave Model

• Active NPF promotes F-Actin.

• Wave Generator

• F-Actin inactivates NPF

• Refractory feedback

NegativeFeedback

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Actin Wave ModelAt = f +DA4A,

It = �f +DI4I

f(A, I, F ) =

✓k0 +

�A3

A30 +A3

◆I � �

✓s1 + s2

F

F0 + F

◆A

Ft = ✏hh(A,F ) = knA� ksF

A

I

F

NPF Equations

F-Actin Equations

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Pulse Snapshot

• F-Actin wave trails NPF wave

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Spatio-TemporalBehaviour

• Kymograph = (x,t) plot

Pinned Wave Oscillating Wave

Reflecting Pulse

SinglePulse

PulseTrain Exotic

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Use LPA to map parameter space

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Actin Wave LP-System

Alt = f(Al, Ig, F l),

Agt = f(Ag, Ig, F g),

Igt = �f(Ag, Ig, F g),

F lt = ✏h(Al, F l),

F gt = ✏h(Ag, F g)

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Actin Wave LP-System

Alt = f(Al, Ig, F l),

Agt = f(Ag, Ig, F g),

Igt = �f(Ag, Ig, F g),

F lt = ✏h(Al, F l),

F gt = ✏h(Ag, F g)

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Actin Wave LPA

• Applying NPF conservation.

Alt = f(Al, C �Ag, F l),

Agt = f(Ag, C �Ag, F g),

F lt = ✏h(Al, F l),

F gt = ✏h(Ag, F g)

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Actin Wave LPA

H

H

H=Hopf Bifurcation • Branch Points are

retained from wave pinning.

• Hopf bifurcations are new and indicate oscillations.

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Actin Wave LPA

H

H

Oscillatory Instability

• Branch Points are retained from wave pinning.

• Hopf bifurcations are new and indicate oscillations.

Stable HSS

ExcitableOscillations

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Questions?

• How do the positive and negative feedback loops interact to initiate patterning?

• What role do they play in determining the resulting behaviour on a longer time scale?

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LPA + Simulation

• Curve = 2 parameter Hopf continuation.

• Points = values used for PDE simulations.

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LPA + Simulation

+ = Reflecting Waves

O = Reflecting Waves

* = Wave Trains

X = Single Wave

= Single Wave

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LPA + Simulation

• Inside the fish tail, patterning arises from instability.

• Outside, from excitability.

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Patterning Region

• Feedback is necessary for patterning, but to much suppresses it.

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Static to Dynamic Transition

• Increasing feedback yields a progression from static, to dynamic, to no patterning.

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Wave Trains

• Wave trains, indicative of target waves (in 2D), only occur inside the fish tail

(f)

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Conclusions

• GTPase like kinetics coupled with F-actin feedback is capable of producing a wealth of static and dynamic behaviours.

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Conclusions

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Conclusions

• The inclusion of a WP model (ie. conservation) as the ‘wave generator’ in the FitzHugh Nagumo framework yields substantially different behaviour.

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Conclusions

• The inclusion of a WP model (ie. conservation) as the ‘wave generator’ in the FitzHugh Nagumo framework yields substantially different behaviour.

• Static to dynamic transition.

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Conclusions

• The inclusion of a WP model (ie. conservation) as the ‘wave generator’ in the FitzHugh Nagumo framework yields substantially different behaviour.

• Static to dynamic transition.

• Reflecting waves vs wave trains.

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Conclusions

• The inclusion of a WP model (ie. conservation) as the ‘wave generator’ in the FitzHugh Nagumo framework yields substantially different behaviour.

• Static to dynamic transition.

• Reflecting waves vs wave trains.

• Persistent patterning in excitable regimes.

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Conclusions

• Increasing levels of feedback lead to a transition from static to dynamic behaviour and finally to the suppression of all patterning.

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