Coupling Hair Follicle Cycles to Produce Traveling Waves

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Coupling Hair Follicle Cycles to Produce Traveling Waves Megan Jeans 1,2 and Dr. G. Bard Ermentrout 3 1 Bioengineering and Bioinformatics Summer Institute, Department of Computational Biology, University of Pittsburgh, PA 15261 2 Department of Bioengineering, Rice University, Houston, TX 77005 3 Department of Mathematics, University of Pittsburgh, Pittsburgh, PA 15261

Examples of Biological Synchronization Pacemaker cells in the heart Discharging of brain cells during epileptic seizures Women s s menstrual cycles Hair growth in rodents motivation for this study Suzuki, et al.

The Hair Follicle Cycle Begins with catagen apoptosis Telogen rest, exogen usually occurs in this phase Anagen growth, longest phase www.keratin.com/aa/aa008.shtml

Objectives Simulate the hair follicle cycle with two models. Activator/ inhibitor Substrate/ depletion Create networks of follicle oscillators via different modes of coupling To observe the effects of certain variables To produce synchronization.

The Activator/Inhibitor Model x autocatalytic activator y inhibitor

The Substrate/Depletion Model x product y - reactant Fall, et al.

Hopf Bifurcation Fixed point loses stability as the eigenvalues cross the imaginary axis of the complex plane Stable limit cycle

Perturbations and the Interaction d ω θ dt φ = ωt θ Function (H) = 2 π / T + βsin( ωt θ) 0 = 2 π /T Phase difference between oscillator and stimulator

Averaging Z(t) response function G(x) type of coupling Diffusive coupling x -x Bath coupling f((x+0.01*x,y),y)-f(x,y))/0.01 H(Φ) interaction function; coupling as a function of phase difference between oscillators

Diffusive coupling function via the activator Diffusive coupling function via the inhibitor

Network Equation 20 oscillators in the network Optional gradient (ε)( Coupling strength (a) must be weak gradient Neighbor influence

1-D D Arrays Kind of coupling Via x or y variable Via diffusive or bath coupling Coupling constant (a) Diffusion limit (number of neighbors) Heterogeneity (ε)(

Types of Coupling (ε = 0, 2 nearest neighbors) Activator Inhibitor Diffusive Coupling a = 1 Bath Coupling a = 5 Sine component is too small

Coupling Constant (ε = 0, 2 nearest neighbors, diffusive coupling) a = 1 a = 5 Activator Inhibitor

Diffusion Limit (a = 1, ε = 0, diffusive coupling via activator) 2 neighbors 4 neighbors 6 neighbors

Introducing Heterogeneity (a = 1, diffusive) eps = -1 eps = 1 eps = 5 Activator 2 nearest neighbors Inhibitor 4 nearest neighbors ( same phenomena for 6 neighbors)

2-D D Arrays Using Fourier approximation Simulates actual traveling waves in the mouse Suzuki, et al.

Activator 2-D Arrays Inhibitor Diffusive Bath

Types of Coupling (a=1, eps=0, 2 nearest neighbor) via product via reactant Diffusive coupling Bath coupling

Adding a gradient induces synchronization for bath coupling via product eps = 0 eps = 1 eps = 5

2-D D Arrays Diffusive coupling via Product Reactant Bath coupling did not produce any patterns.

Results Summary Types of Coupling Only 4 networks synchronized for both 1 and 2 D arrays.

Results Summary - Variables 1-D D Arrays The only coupling mode which never synchronized was bath coupling via the reactant. Changing the gradient can induce traveling waves, reverse wave direction and produce synchrony. The coupling constant and the diffusion limit are proportional to synchronization speed. 4 nearest neighbor coupling can initially produce unusual patterns. 2-D D Arrays

Conclusions The hair follicle cycle could be represented by either model. Most likely networks are those which synchronize for 1 and 2 D networks. Diffusive coupling via activator, product, and reactant Bath coupling via activator

Who cares??

Acknowledgments Dr. G. Bard Ermentrout,, advisor Judy Wieber and Rajan Munshi, coordinators BBSI participants BBSI Department of Computational Biology, Pittsburgh NIH/NSF

References Edelstein- Keshet,, Leah. Mathematical Models in Biology, 1 st ed. Boston: McGraw Hill, 1988. Ermentrout, G.B. and J. Rinzel. Beyond a pacemaker s entrainment limit: phase walk-through. through. Am J Physiol Regulatory Integrative Comp Physiol.. 246 (1984): 102-106. Fall, Christopher P., et. al., eds. Computational Cell Biology.. New York: Springer-Verlag Verlag,, 2002. Maini,, Philip K. How the mouse got its stripes. PNAS 100:17(2003): 9656-9657. 9657. Paus,, Ralf and Kerstin Foitzik. In search of the hair cycle clock : : a guided tour. Differentiation. 72(2004):489-511. Suzuki, Noboru, et al. Traveling strips on the skin of a mutant mouse. PNAS.. 100:17 (2003): 9680-9685. 9685.