scholarly journals Investigating two kinds of cellular alternans and corresponding TWA induced by impaired calcium cycling in myocardial ischemia

2021 ◽  
Vol 18 (6) ◽  
pp. 7648-7665
Author(s):  
Jiaqi Liu ◽  
◽  
Zhenyin Fu ◽  
Yinglan Gong ◽  
Ling Xia

<abstract> <sec><title>Background</title><p>The utility of T wave alternans (TWA) in identifying arrhythmia risk has been demonstrated. During myocardial ischemia (MI), TWA could be induced by cellular alternans. However, the relationship between cellular alternans patterns and TWA patterns in MI has not been investigated thoroughly.</p> </sec> <sec><title>Methods</title><p>We set MI conditions to simulate alternans. Either prolonging Ca<sup>2+</sup> release or increasing spark-induced sparks (secondary sparks) can give rise to different patterns of APD alternans and TWA. In addition, different ischemic zones and reduced conduction velocity are also considered in one dimensional simulation.</p> </sec> <sec><title>Results</title><p>Delay of Ca<sup>2+</sup> release can produce discordant Ca<sup>2+</sup>-driven alternans in single cell simulation. Increasing secondary sparks leads to concordant alternans. Correspondingly, morphology and magnitude of TWA vary in two different cellular alternans. Epi ischemia results in alternans concentrating in the first half of T wave. Endo and transmural ischemia lead to fluctuations in the second half of T wave. In addition, slowing conduction velocity has no effect on TWA magnitude.</p> </sec> <sec><title>Conclusion</title><p>Specific ionic channel dysfunction and ischemic zones affect TWA patterns.</p> </sec> </abstract>

2013 ◽  
Vol 767 ◽  
pp. 34-39 ◽  
Author(s):  
Shiro Kubota ◽  
Tei Saburi ◽  
Yuji Ogata ◽  
Kunihito Nagayama

The purpose of this study is to reconstruct the equation of state (EOS) whose parameters can be applied for high energetic material of arbitrary initial density without any modification. The simulation for detonation propagation in arbitrary initial density was proposed as the new method for obtaining the information of the EOS for detonation products of arbitrary initial density. At the same time, to collect the experimental data which verify the applicability of the numerical simulation, the detonation velocity for the system consisting of the pellet explosives and air gaps were conducted. The thickness of the 20 mm diameter pellet explosive was 10 mm, and air gaps were varied 0.5 mm to 2.0 mm. The relationship between detonation velocity and experimental condition was clarified for composition A5. The proposed one dimensional simulation was also conducted. The relationships between the pressure and the specific volume for detonation products were extracted from the proposed simulation


2015 ◽  
Vol 20 (1) ◽  
pp. 2-7
Author(s):  
Ozgur Surgit ◽  
Mehmet Erturk ◽  
Ozgur Akgul ◽  
Hamdi Pusuroglu ◽  
Ali Fuat Korkmaz ◽  
...  

Heart Rhythm ◽  
2012 ◽  
Vol 9 (3) ◽  
pp. e6-e7
Author(s):  
Violeta Monasterio ◽  
Pablo Laguna ◽  
Iwona Cygankiewicz ◽  
Rafael Vázquez ◽  
Antoni Bayés-Genís ◽  
...  

2015 ◽  
Vol 10 (9-10) ◽  
pp. 239-239
Author(s):  
Mislav Puljevic ◽  
Josko Bulum ◽  
Aleksander Ernst ◽  
Davor Milicic ◽  
Davor Puljevic

2018 ◽  
Vol 24 (2) ◽  
pp. e12610
Author(s):  
Mislav Puljevic ◽  
Ludmila Danilowicz-Szymanowicz ◽  
Giulio Molon ◽  
Davor Puljevic ◽  
Grzegorz Raczak ◽  
...  

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