Multiscale modeling of ocular physiology

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HAL Id: hal-02278863 https://hal.archives-ouvertes.fr/hal-02278863 Submitted on 6 Sep 2019 HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. Multiscale modeling of ocular physiology Lorenzo Sala, Riccardo Sacco, Giovanna Guidoboni To cite this version: Lorenzo Sala, Riccardo Sacco, Giovanna Guidoboni. Multiscale modeling of ocular physiology. Journal for Modeling in Ophthalmology, Kugler Publications, 2018, 2 (1), pp.12-18. hal-02278863

Transcript of Multiscale modeling of ocular physiology

Page 1: Multiscale modeling of ocular physiology

HAL Id: hal-02278863https://hal.archives-ouvertes.fr/hal-02278863

Submitted on 6 Sep 2019

HAL is a multi-disciplinary open accessarchive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come fromteaching and research institutions in France orabroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, estdestinée au dépôt et à la diffusion de documentsscientifiques de niveau recherche, publiés ou non,émanant des établissements d’enseignement et derecherche français ou étrangers, des laboratoirespublics ou privés.

Multiscale modeling of ocular physiologyLorenzo Sala, Riccardo Sacco, Giovanna Guidoboni

To cite this version:Lorenzo Sala, Riccardo Sacco, Giovanna Guidoboni. Multiscale modeling of ocular physiology. Journalfor Modeling in Ophthalmology, Kugler Publications, 2018, 2 (1), pp.12-18. �hal-02278863�

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Multiscale modeling of ocular physiology

Lorenzo Sala1, Riccardo Sacco2, and Giovanna Guidoboni3

1Universite de Strasbourg, CNRS, IRMA Unite Mixte deRecherche 7501, Strasbourg, France. [email protected]

2Department of Mathematics, Polytechnic University of Milan,Milan, Italy

3Department of Electrical Engineering and Computer Science,University of Missouri, Columbia, MO, USA

Keywords: Multiscale mathematical modelling, Ocular blood flow, Neurovas-cular coupling, Optic nerve head perfusion.

1 Background and Purpose

Our purpose is to devise mathematical models that can serve as synergistic com-plements to experimental and clinical studies and deepen the current knowledgeof ocular physiology in health and disease. One of the main challenges in devel-oping a mathematical description of ocular physiology stems from the inherentmultiscale nature of life in time and space. For example, the time scales ofcellular biochemical reactions, cardiac cycle, circadian rhythm and aging differby several orders of magnitude and yet they all matter when studying diseasessuch as glaucoma. Similarly, the length scales of ion channels, cells, tissuesand organs span from nanometers to centimeters and yet they all interact todetermine our body functions.

In this article, we highlight two recent contributions towards the multiscalemodeling of ocular physiology that our group presented at the 2017 AnnualMeeting of the Association for Research in Vision and Ophthalmology (7-11May, 2017, Baltimore, MD, USA). The first contribution presents a mathe-matical virtual simulator, henceforth indicated as model M1, to simulate thebiomechanics and the tissue perfusion of the lamina cribrosa (LC) [5]. ModelM1 may serve as a computational tool to visualize hemodynamic and biome-chanic parameters in the LC such as LC displacement, blood flow velocity andpressure, and predict their spatial and temporal variability. The aim of modelM1 is to leverage partial data available on some parts of the eye (e.g. bloodvelocity in the central retinal vessels and ocular geometry) to provide furtherinformation on other parts of the eye that are very important from a clinical

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OAfromInternal

CarotidArtery

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Figure 1: Mathematical virtual simulator multiscale scheme. Schematic repre-sentation of the ocular blood supply.

viewpoint but that may not be easily accessible with standard investigationinstruments.The second contribution presents a mathematical model, henceforth indicatedas model M2, to theoretically investigate the role of neural nitric oxide (nNO),jointly with 20-hydroxyeicosatetraeonic acid (20-HETE) and epoxyeicosatrienoicacid (EET), in the regulation of retinal neurovascular coupling [4]. The analysisis motivated by experimental data of flicker light-induced functional hyperemiain humans indicating that increased nitric oxide levels mediated by 20-HETEreduce vasodilation [3]. The aim of model M2 is to provide quantitative pre-dictions of the effect of increased levels of nNO on the vasodilation of retinalarterioles to theoretically investigate the conjecture that increased nitric oxidelevels may be responsible for suppressing flicker-evoked vasodilation in diabeticretinopathy [3].

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2 Methods

In both models M1 and M2, a deterministic multiscale approach is adopted, inwhich equations are derived by general physical principles, such as balance ofmass and linear momentum. In addition, both models M1 and M2 are designedso that their input data include quantities that can be determined in a clinicalsetting, such as systolic and diastolic blood pressure (SBP and DBP), intraocu-lar pressure (IOP) and ocular geometry. Model M1 employs a system of partialdifferential equations to provide a detailed spatial and temporal characterizationof the physical variables within the LC, combining a three-dimensional porous-media model for LC perfusion with a circuit-based model for blood flow in theretrobulbar and ocular posterior segments (Fig. 1). The whole coupled system issolved using advanced computational and visualization methods [6]. Model M2employs a system of ordinary differential equations to provide a systemic viewof retinal hemodynamics, combining an equivalent electrical circuit of resistiveand capacitive compartments for the retinal vasculature (Fig. 2b) with a cellu-lar scale chemomechanical description of neurovascular coupling as the resultinginteraction between vasoactive agents synthesized by active neurons, astrocytesand smooth muscle cell contraction/dilation (Fig. 2a). Kirchhoff current law issolved at each node of the equivalent electrical circuit to determine the timeevolution of nodal blood pressures and compartment diameters [2].

Retinal Microcirculation and Neurovascular Coupling 5

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vessel lumen

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Fig. 2 Multiscale structure of retinal vasculature, circulation and regulation. The picturegives a schematic view of the three principal scales that coexist in the system. Panel A:the macroscale. Panel B: the mesoscale. Panel C: the microscale. The image in panel Ahas been obtained via retinal oximetry [15,44]. The macroscale input sources are: Pin (in-put pressure of retinal vasculature), Pout (output pressure of retinal vasculature) and Pext

(pressure exerted by the eye on the retinal vasculature, a measure of which is given by theintraocular pressure). The microscale input sources are: nNO (nitric oxide synthesized byneurons in the vicinity of the astrocyte cells) and Glu (glutamate neurotransmitter syn-thesized by a post-synaptic terminal). Abbreviations: EthC: endothelial cell. SMC: smoothmuscle cell. Ast: astrocyte. NO: nitric oxide. EET: epoxyeicosatrienoic acid. 20-HETE: 20-hydroxyeicosatetraeonic acid. Glu: glutamate. v: blood velocity. ⌧sh: blood shear stress.{fig:scales}

represented in Fig. 2. The macroscale corresponds to the whole retinal vascu-lar network, as shown in Panel A, where the color scale represents the levelof oxygen saturation in the major retinal arteries and veins and it is obtainedusing retinal oximetry [15,44]. The mesoscale corresponds to one single vas-cular segment of the network surrounded by the glial environment, as shownin Panel B, where vessel lumen, endothelium layer, smooth muscle cell layerand astrocyte feet are reported in red, green, cyan and yellow, respectively.Each part of the scheme is assumed to be homogeneous and characterized byspecific constitutive parameters. The microscale corresponds to the cell levelin the vessel wall and the glia, as shown in Panel C. Each smooth musclecell (SMC) can alter its shape between undeformed (solid line) and deformed(dashed line) configurations as vasoactive agents are synthesized by endothe-lial cells (EthC) and astrocytes (Ast) in response to changes in blood shearstress (⌧sh), glutamate (Glu) and nitric oxide (NO).

The functional response of this multiscale system is driven by: (1) macroscaleinput sources, specifically the blood pressures Pin and Pout at the input andoutput of the retinal vasculature, respectively, and the external pressure ex-erted on the retinal vasculature by the eye, the so-called intraocular pressure(IOP); and (2) microscale input sources, specifically the amount of nitric ox-ide that is synthesized by neurons in the vicinity of the astrocyte cells (nNO)

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Figure 2: (a) Multiscale description of neurovascular coupling in the retina.The model inputs at the Macroscale (A) are the blood pressures at the inletand outlet of the retinal circulation, Pin and Pout. The Mesoscale (B) focusesarterioles, whose walls comprise endothelium and smooth muscle cells. TheMicroscale (C) entails the biochemistry at the cellular level that governs thechange in smooth muscle shape. (b) Macroscale, Mesoscale and Microscaleare effectively combined in a single model by means of appropriate equivalentresistances.

3 Results

Fig. 3a reports the M1 visualization of ocular geometry. Simulations performedusing the mathematical virtual simulator show that (i) LC displacement (Fig. 3f)

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Figure 3: Lamina cribrosa perfusion simulated using the mathematical virtualsimulator in the case of low, normal and high blood pressure, denoted by LBP,NBP and HBP, respectively. (a) Digitalized geometry of the eye. (b) Simu-lated discharge velocity. (c) Simulated blood velocity in the central retinal vein(CRV). (d) Simulated pressure distribution. (e) Simulated blood velocity in thecentral retinal artery (CRA). (f) Simulated lamina displacement. Only NBPdisplacement is shown because simulations in LBP and HBP conditions yieldsimilar results.

is not highly influenced by the presence of the CRA/CRV opening[7] and thevalues are comparable to those reported in experimental studies[9], (ii) LC bloodpressure distribution (Fig. 3d) is highly influenced by the values of SBP/DBPimposed at the inlet of the circuit model and attains realistic values[1], inparticular on the lateral boundary, (iii) LC perfusion (Fig. 3b) increases withSBP/DBP, particularly near the nasal area and (iv) CRA and CRV blood veloc-

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ities (Figs. 3c and 3e, respectively) are comparable to those obtained via directimaging modalities[8].

Figure 4: Neurovascular coupling simulations. (Top Left) Glutamate stimulus.(Bottom Left) Baseline (black) and elevated (red) levels of nNO. (Center) Simu-lated % change in MAD. Black circles: experimental data of[3]; green rectangle:data variation at the end of the GLU stimulus; dashed line: only one LA is NVA;dash-dotted line: network where only LA are NVA; solid black line: networkwhere both LA and SA are NVA. (Right) Simulated % change in MAD. Blackcircles: experimental data of[3]; solid black line: network where both LA andSA are NVA, nNO=nNOb; red black line: network where both LA and SA areNVA, nNO=nNO+.

Fig. 4 shows the results of model M2 in the simulation of functional hyper-emia (FH) in humans under flicker light stimulation (FLS)[3]. In the left panelFLS is modeled by a triangular glutamate (GLU) input signal of 0.07 µM for 20seconds. Simulations are performed for two different nNO levels (baseline value,nNOb, black line; increased value, nNO+ >nNOb, red line). In the central panelFH in humans is simulated with the triangular GLU signal, nNO=nNOb anddifferent neurovascularly active (NVA) segments. The y-axis is the % changein mean arterial diameter (MAD). Black circles indicate the experimental dataof[3]; the green rectangle highlights data variation at the end of the GLU stimu-lus; the dashed line shows model prediction using only one large arteriole (LA);the dash-dotted line is model prediction using the network of Fig. 2(b)b whereonly LA are assumed to be NVA; the solid black line shows model predictionusing the network of Fig. 2(b)b where both LA and small arterioles (SA) areassumed to be NVA. Results indicate that FH is correctly represented only ifboth LA and SA are assumed to be NVA. In the right panel we illustrate thesimulated effect on vasodilation due to the GLU signal and a 60s stimulus ofnNO=nNO+. Results indicate that elevated nNO may reduce vasodilation bya factor of 4.

4 Conclusions

Multiscale mathematical models may provide new ways to recover informationon ocular physiology in health and disease. In particular, model M1 may serveas an instrument to illustrate and estimate LC perfusion parameters whereasmodel M2 may serve as a virtual lab where hypothesized neurovascular coupling

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mechanisms can be tested and compared. The importance of the two proposedmathematical models is that, starting from general physical laws commonlyadopted in academic and industrial contexts, they may be able to describevarious aspects of ocular physiology. Moreover, after a severe validation processagainst experimental data, they can also be used as valid predictive instrumentsin a virtual laboratory serving as a complementary approach to experimentaland clinical investigation in Ophthalmology.

Acknowledgements

This work has been partially supported by the Ministere de l’Enseignementsuperieur et de la Recherche (France), NSF DMS-1224195, a grant from Re-search to Prevent Blindness (RPB, NY, USA), the Chair Gutenberg funds ofthe Cercle Gutenberg (France), the Labex IRMIA (University of Strasbourg,France) and Micron Semiconductor Italia S.r.l., statement of work #4505462139:”Modeling of tunneling and charging dynamics”, contractors: Micron Semicon-ductor Italia S.r.l.; Dipartimento di Matematica Politecnico di Milano, Italy.

References

[1] G. Guidoboni, A. Harris, S. Cassani, J. Arciero, B. Siesky, A. Amireskan-dari, L. Tobe, P. Egan, I. Januleviciene, and J. Park. Intraocular pres-sure, blood pressure, and retinal blood flow autoregulation: A mathemat-ical model to clarify their relationship and clinical relevanceeffects of iop,bp, and ar on retinal hemodynamics. Investigative ophthalmology & visualscience, 55(7):4105–4118, 2014.

[2] A. G. Mauri, R. Sacco, G. Guidoboni, A. Cardani, and A. Harris. Neurovas-cular coupling in the human retina: a multiscale mathematical model. Inpreparation, 2017.

[3] E. A. Newman. Functional hyperemia and mechanisms of neurovascularcoupling in the retinal vasculature. Journal of Cerebral Blood Flow &Metabolism, 33(11):1685–1695, 2013.

[4] R. Sacco, A. Mauri, A. Cardani, B. Siesky, G. Guidoboni, and A. Harris.Increased levels of nitric oxide may pathologically affect functional hyperemiain the retina: model and simulation. Annual Meeting of the Association forResearch in Vision and Ophthalmology, 2017. Posterboard Number 214 -B0245.

[5] L. Sala, , C. Prudhomme, D. Prada, F. Salerni, C. Trophime, V. Chabannes,M. Szopos, R. Repetto, S. Bertoluzza, R. Sacco, A.Harris, and G. Guidoboni.Patient-specific virtual simulator of tissue perfusion in the lamina cribrosa.Annual Meeting of the Association for Research in Vision and Ophthalmol-ogy, 2017. Posterboard Number 727 - B0474.

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[6] L. Sala, R. Hild, C. Prud’Homme, G. Guidoboni, R. Sacco, S. Bertoluzza,D. Prada, and M. Szopos. An implementation of hdg methods with feel++.application to problems with integral boundary condition. In preparation,2017.

[7] I. A. Sigal, J. G. Flanagan, I. Tertinegg, and C. R. Ethier. Finite elementmodeling of optic nerve head biomechanics. Investigative ophthalmology &visual science, 45(12):4378–4387, 2004.

[8] T. H. Williamson and A. Harris. Color doppler ultrasound imaging of theeyeand orbit. Survey of ophthalmology, 40(4):255–267, 1996.

[9] D. Yan, F. Coloma, A. Metheetrairut, G. Trope, J. Heathcote, and C. Ethier.Deformation of the lamina cribrosa by elevated intraocular pressure. BritishJournal of Ophthalmology, 78(8):643–648, 1994.

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