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1 Multi-scale Cardiac Modelling Reveal Tachyarrhythmias Induced by Abrupt Rate Accelerations in Long QT Syndrome Jieyun Bai, Kuanquan Wang, Henggui Zhang School of Computer Science and Technology Harbin Institute of Technology, HIT Harbin, China Dec. 15, 2016, Shenzhen, China.

Multi-scale Cardiac Modelling Reveal Tachyarrhythmias ...qinsiw/fmbbs16/BIBM_2016_Bai.pdfcardiac arrhythmias. Part Ⅰ ... leading to genesis of reentrant excitations, but the reentry

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Page 1: Multi-scale Cardiac Modelling Reveal Tachyarrhythmias ...qinsiw/fmbbs16/BIBM_2016_Bai.pdfcardiac arrhythmias. Part Ⅰ ... leading to genesis of reentrant excitations, but the reentry

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Multi-scale Cardiac Modelling Reveal Tachyarrhythmias Induced by Abrupt

Rate Accelerations in Long QT Syndrome

Jieyun Bai, Kuanquan Wang, Henggui ZhangSchool of Computer Science and Technology

Harbin Institute of Technology, HITHarbin, China

Dec. 15, 2016, Shenzhen, China.

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Outline

Ⅰ. Background

Ⅱ. Methods

Ⅲ. Results

Ⅳ. Conclusion

Ⅴ. Acknowledgement

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Backgroundn Long QT syndrome (LQTS) is a rare congenital and inherited or

acquired heart condition which delayed repolarization of the heartfollowing a heartbeat increases the risk of episodes of ventriculararrhythmias

n The long-QT syndromes (LQTS) are characterized byq action potential (AP) prolongation in single cells.q a prolonged QT interval on the electrocardiography (ECG), and ventricular

arrhythmias in patients.

n Although molecular and genetic changes of the individual ionicchannels were addressed, it is relatively unclear for the exacttissue-level electrophysiological mechanism for arrhythmias as aresult from cellular disorder.

Part Ⅰ

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Backgroundn The mechanisms by which this

bradycardia-dependent phenomenoncontributes one to rapid arrhythmiasare worthy to be studied andimportant for preventing andmanaging sudden cardiac death.

n Multi-scale mathematical modelingprovides an alternative method forunderstanding the development ofcardiac arrhythmias.

Part Ⅰ

?Fig. 1 Early afterdepolarizationsEADs often occurred at slow heartrates and ventricular arrhythmiasare characterized by excessivelyhigh heart rates.

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Backgroundn Experimental studies in animal ventricle have suggested that

acceleration of heart rate can induce transient EAD activity(Burashnikov, et al. and Nuyens, et al.).

n This study sought to test the hypothesis that EADs induced byabrupt rate accelerations can occur and investigate how thisabrupt rate accelerations is related to the mechanisms of reentrantexcitations.

n A human ventricular cell was modified to model experimentalconditions in LQTS. Then, the normal and EADs cell modelswere incorporated into homogeneous multicellular 1D and 2Dtissue models to study the mechanism underlying the generationof reentrant events.

Part Ⅰ

Burashnikov,etal.(1998). Journal ofcardiovascular electrophysiology.9, 934-948.Nuyens,etal.(2001). Naturemedicine.7, 1021-1027.

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Methods n The TP06 model for the human

ventricular AP, which wassuggested that it can be used forventricular arrhythmias underpathological conditions, wasdeveloped by using the humanexperimental data.

n Thus, the TP06 model wasmodified to simulate EADs atthe cellular level based onexperimental data.

Part II

Fig. 2 A human ventricular model(upper) and ventricular arrhythmias(bottom) were studied by using the TP06model.

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Vandersickel,etal.(2014). PloSone.9, e84595.

§ The modified human ventricular cell model was govern as follows

where Cm, V, t, Istim and Iion are the membrane capacitance, the membrane potential, the

time and the stimulus current and the sum of transmembrane ionic current, respectively.

m ion stimC V t I I∂ ∂ = − +

1+ + ++ +ion Kr Ks K to Na bNa CaL bCa

NaK NaCa pCa pK NaL

I I I I I I I I II I I I I= + + + +

+ + +

Methods Part II

Parameters PercentageGKr 0.5fold (↓)GCaL 5 fold (↑)Tau 2 fold (↓)

Table 1. Changes of parameters for simulating EADsbased on experimental data (Vandersickel, et al. ).

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Methods n We constructed a 1.5cm cable (100 cell with cell length 0.015cm) with

an EADs region containing 10 cells (from 45 to 55) in the center of thefiber. The distance between the center of the EADs region and the fiberend is about ~7.5 mm, which is similar to that observed by Vijayakumaret al.

n For our 2D simulations, a square tissue of 15 mm×15 mm, whichcontains a 7.5 mm×7.5 mm EADs region (similar to ionicheterogeneity measured by Glukhovet et al., is developed to investigatethe dynamics of spiral waves.

Part II

0 10045-55

S1 Normalcells LQTCells Normalcells

Fig. 3 1D (left) and 2D(right) idealized human tissue model.

Vijayakumar et al.(2014). Circulation.130, 1936-1943.Glukhovet et al.(2010).Circulation research.106, 981-991.

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Methods

n Action potentials were simulated by changing pacing rate from 0.5Hz to2Hz, recording and analyzing ionic currents and concentrations changes.The stimulus strength is with the amplitude of -52pA/pF and theduration of 1 ms. APD90 was measured as the duration of APs at 90%repolarization.

n Dispersion of repolarization (DOR) was computed as the timedifference of repolarization time along the 1D tissue. APD spatialgradient was computed as rate of APD changes per unit length, whichprovides a measure of the extent to conduction block of cardiac tissue.

n The temporal vulnerable window (VW) was computed as the timewindow for unidirectional conduction block.

Part II

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§ During fast pacing (2Hz), the content ofSR calcium [Ca2+]SR increased from 3.64to 4.58 mM and spontaneous calciumrelease (Irel) occurred before completedrepolarization. EAD was triggered by asodium-calcium exchange current not theICaL.

Fig. 4. The development of EADs for abrupt rateaccelerations. The pacing rate was changed from0.5Hz to 2Hz and EAD was initiated byspontaneous calcium release (Irel) from SR and asodium-calcium exchange current (INCX),depolarizing inward current.

Results Part III

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§ Compared with the normal condition, DOR under LQTS conditionexcessively was increased by 473% (from 15ms to 86 ms) and causedby the EAD region. Prolonged APD in the EAD region was paralleledby an abrupt rise in DOR from 1ms/m to 63.3ms/mm, producingsteep spatial gradients of repolarization that was directly responsiblefor unidirectional conduction block.

Fig. 5.DOR under Normal and local LQT conditions.

Results Part III

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§ For the normal condition, bidirectional block (T=332 ms), unidirectionalconduction block (from T=333 to 333.5ms, 0.5ms) and bidirectionalconduction (T=333.6) were observed. But unidirectional conductionblock (from T=348 to 362ms) for the LQTS condition is 14 ms.Compared with the normal condition, a marked increase (from 0.5 ms to14 ms, 2800%) in VW demonstrated a notable increase in tissuesusceptibility to arrhythmogenesis.

Ai Aii Aiii

100 ms

Nor

mal

1.5 cm

0 cm

Loca

l LQ

T

1.5 cm

0 cm

AviT=332 ms T=333 ms T=333.5 ms T=333.6 ms

Bi Bii Biii BviT=347 ms T=348 ms T=362 ms T=363 ms

Fig. 6. Space-time plot of propagatingexcitation wave in response to apremature test stimulus at various timeinterval (T) between S1 and S2 stimulusunder normal (A) and LQTS (B)conditions.

Results Part III

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§ For the normal condition (Fig. 7, Normal), an abrupt pacing stimulusproduced bidirectional conduction leading to genesis of plane waveswithout breaking up. For the LQTS condition (Fig. 7, LQTS), anabrupt pacing stimulus produced unidirectional conduction blockleading to genesis of a reentrant excitation resulted from local planewaves block.

Ai Aii Aiii AivT=70 ms T=350 ms T=600 ms T=1000 ms

Bi Bii Biii BivT=70 ms T=350 ms T=600 ms T=1000 ms

Fig. 7. Simulation of spiral wavesin a 2D ventricular tissue undernormal and LQTS conditions.

Results Part III

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Conclusion§ Abrupt rate acceleration prolonged action potential duration, caused

premature beats and induced EADs in LQTS cells.

§ The changes in cellular electrophysiology modulated ventricularconduction and increased tissue temporal and spatial vulnerability. Thelocal LQT region increased spatial vulnerability and prolonged APD inlocal LQT cells increased temporal vulnerability, producing steep spatialrepolarization gradients that was directly responsible for unidirectionalconduction block.

§ An abrupt pacing stimulus produced unidirectional conduction blockleading to genesis of reentrant excitations, but the reentry wave for theLQTS condition was unstable and promoted self-termination inidealized 2D tissue. Local LQTS region with a longer wavelength isresponsible for self-termination of the reentry wave.

Part IV

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Conclusion§ Although EADs in LQTS classically occurred at slow heart rates, some

experimental studies suggested EADs may be induced at the fast heartrates, which provided a potential link between bradycardia-dependentAP prolongation and tachycardia-dependent ventricular arrhythmias.The present study provided direct evidences that support the hypothesisEADs induced by abrupt rate accelerations can transform intoventricular arrhythmias (EADs increased regional repolarizationdispersion that contributed to the genesis of tachyarrhythmias in LQTS).

Part IV

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Acknowledgement Part V

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Any questions ?