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Buhl-Strohmaier-Stiftung Viability Approach to Autoregulation of Cerebral Blood Flow in Preterm Infants Varvara Turova, Nikolai Botkin, Ana Alves-Pinto, Tobias Blumenstein, Esther Rieger-Fackeldey, Rene Lampe Clinic rechts der Isar


  1. Buhl-Strohmaier-Stiftung Viability Approach to Autoregulation of Cerebral Blood Flow in Preterm Infants Varvara Turova, Nikolai Botkin, Ana Alves-Pinto, Tobias Blumenstein, Esther Rieger-Fackeldey, Renée Lampe Clinic ‚rechts der Isar‘ & Mathematical Center Munich Technical University Workshop on Numerical Methods for Hamilton-Jacobi Equations in Optimal Control and Related Fields, November 21-25. 2016, Linz, Austria

  2. Motivation Incidence of intracranial hemorrhages Ultrasonic image showing in newborns weighting intraventricular bleeding in a less than 1500 gm dropped to 20% preterm newborn The cause of brain bleeding is the germinal matrix of the immature brain! 1

  3. Cerebral autoregulation Intact autoregulation Impaired autoregulation M. van de Bor, F.J. Walther. Cerebral blood fow velocity regulation in preterm infants. Biol. Neonate 59, 1991. H.C.Lou, N.A.Lassen, B. Friis-Hansen. Impaired autoregulationopf cerebral blood flow in the distressed 2 newborn infant. J. Pediatri. 94, 1979.

  4. Cerebral blood flow p a 1 10 the mean arterial pressure 2 the intracranial pressure (constant) the number of levels i the number of vessels at level the resistance of each vessel at level i+1 in the case of Poiseuille flow the length and radius of vessels at level M the reference radius S.K.Piechnik, P.A.Chiarelli, P. Jezzard, modifier due to the vascular volume change Modelling vascular reactivity to investigate the basis of the relationship between cerebral blood the reactivity and partial pressure volume and flow under CO2 manipulation. 3 NeuroImage 39, 2008.

  5. Micropolar field equations for incompressible viscous fluids the velocity field the micro-rotation field the hydrostatic pressure the classical viscosity coefficient the vortex viscosity coefficient the spin gradient viscosity coefficients 4 G. Lukaszewicz. Micropolar fluids: Theory and applications. Birkhäuser: Boston, 1999.

  6. Micropolar field equations in cylindrical coordinate system z Assumptions: p 1 q r L (1) p 2 r* (2) (Parameter s is a Boundary conditions: measure of suspension concentration ) + uniformity conditions on r=0 Solutions have the form: are the modified Bessel functions M.E.Erdoğan . Polar effects in apparent viscosity of a suspension. Rheol. Acta 9, 1970. 5

  7. Computation of solution using power-series expansion Note that Integrate equation (1) and express through to obtain Plug in equation (2) and denote : (set ) where Boundary conditions (set ) 6

  8. Computation of solution using power-series expansion 7

  9. , CBF and Resistance computed with Maple software 16 8

  10. Thus, we have in the case of a micropolar fluid: Here are computed as above with , where, as before, the reference radius of vessels at level modifier due to the vascular volume change the reactivity and partial pressure, respectively Finally, we have in both Newtonian and micropolar fluid cases: , where is a quickly computable function. 9

  11. Model equations Dynamic equations Additional dependencies Quasilinear regression model for arterial pressure (based on experimental data collected from premature babies (Newborns Intensive Station of the Children Clinic of the Technical University of Munich in the Women Clinic of the Clinic „rechts der Isar“) Constraints on control and disturbances State constraints 10

  12. Variables, constants, parameters - compliance (ability of vessels to distend with increasing pressure) State variables - partial carbon dioxide pressure - partial oxygen pressure - mean arterial pressure - vascular volume 1 = 5 mmHg - intracranial pressure 0.5 -0.5 0.5 M. Ursino, C.A. Lodi, A simple mathematical model of the interaction between 11 intracranial pressure and cerebral hemodynamics, J. Appl. Physiol. 82(4), 1997.

  13. Viability kernel Differential game Consider a family of state constraints: Find a function such that: 12

  14. Grid method for finding viability kernels Let be a time step, space sampling with Operator acting on grid functions: 13

  15. Let a sequence is chosen as: , . Denote Grid scheme Proposition. Let and , then as . (Botkin & T., Proc. Inst. Math. Mech 21(2), 2015) With , ( Botkin, Hoffmann, Mayer, & T., Analysis 31, 2011; Botkin &T., Mathematics 2, 2014) , we obtain that approximates if is large and is small. Criterion of the accuracy: 14

  16. Control design Feedback strategy of the first player Here is an interpolation operator. Feedback strategy of the second player 15

  17. Application to the blood flow model The space of state variables Blood is modeled as usual Newtonian fluid. The viability kernel is shown in different axes Compliance is replaced by cerebral blood flow Compliance is replaced by vascular volume 16

  18. The space of state variables Blood is modeled as a micropolar fluid. The viability kernel is shown in different axes (a) Compliance is replaced by cerebral blood flow Compliance is replaced by vascular volume 17

  19. Simulation of trajectories Optimal feedback control plays against step shaped disturbances Carbon Oxygen dioxide input input time time Control produced by the optimal feedback strategy time 18

  20. All state constraints are kept, but the chattering control is not physically implementable! Compliance Carbon dioxide pressure time time Cerebral blood flow Oxygen pressure time time 19

  21. A simple feedback strategy 1. Put this strategy into the model 2. Compute the viability kernel for the resulting system. In the case, the grid algorithm contains only maximizations over the disturbances. 3. If such a viability kernel is nonempty, the above control strategy is classified as acceptable. Result M.N.Kim et al. Noninvasive measurement of cerebral blood flow and blood oxygenation using near-infrared and diffuse correlation spectroscopies in critically brain-injured adults. Neurocrit. Care 12(2), 2010. 20

  22. The simple feedback control plays against step shaped disturbances Carbon Oxygen dioxide input input Control produced by the simple feedback strategy is acceptably bounded and smooth 21

  23. All state constraints are acceptably kept Compliance Carbon dioxide pressure Oxygen Cerebral blood flow pressure 22

  24. Computation details Grid parameters: : [0.1, 2] /100, : [20, 90]/140, : [20, 90]/120 Time-step width 0.0005, accuracy e = 10 -6 Linux SMP-computer with 8xQuad-Core AMD Opteron processors (Model 8384, 2.7 GHz) and shared 64 Gb memory. The programming language C with OpenMP (Open Multi-Processing) support. The efficiency of the parallelization is up to 80%. Computation time for viability set ca. 15 min 23

  25. Outlook • Evaluation of therapy strategies • Taking into account other factors • More realistic models of cerebral blood vessel system • More experimental data Project funded by Klaus Tschira-Stiftung just started: “Mathematical modelling of cerebral blood circulation in premature infants with accounting for germinal matrix” 24

  26. Acknowledgements We are grateful to Würth Stiftung Buhl-Strohmaier Stiftung Klaus Tschira Stiftung Thank you!

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