Jeong Da Un, Lim Ki Moo
Computational Medicine Lab, Department of IT Convergence Engineering, Kumoh National Institute of Technology, Gumi, South Korea.
Front Physiol. 2018 Jul 31;9:926. doi: 10.3389/fphys.2018.00926. eCollection 2018.
The KCNQ1 S140G mutation, which is involved in I current, affects atrial fibrillation. However, little is known about its effect on the mechanical behavior of the heart. Therefore, we assessed the influence of the KCNQ1 S140G mutation on ventricular electrophysiological stability and mechanical pumping performance using a multi-scale model of cardiac electromechanics. An image-based electromechanical model was used to assess the effect on electrical propagation and arrhythmogenesis of the KCNQ1 S140G mutation. In addition, it was used to compare the mechanical response under the wild-type (WT) and S140G mutation conditions. The intracellular calcium transient obtained from the electrophysiological model was applied as an input parameter to a mechanical model to implement excitation-contraction coupling. The I current equation was modified to account for expression of the KCNQ1 S140G mutation, and it included a scaling factor (ϕ) for mutant expressivity. The WT and S140G mutation conditions were compared at the single-cell and three-dimensional (3D) tissue levels. The action potential duration (APD) was reduced by 60% by the augmented I current under the S140G mutation condition, which resulted in shorter QT interval. This reduced the 3D sinus rhythm wavelength by 60% and the sustained re-entry by 56%. However, pumping efficiency of mutant ventricles was superior in sinus rhythm condition. In addition, the shortened wavelength in cardiac tissue allowed a re-entrant circuit to form and increased the probability of sustaining ventricular tachycardia and ventricular fibrillation. In contrast, under the WT condition, a normal wavelength (20.8 cm) was unlikely to initiate and sustain re-entry in the cardiac tissue. Subsequently, the S140G mutant ventricles developed a higher dominant frequency distribution range (2.0-5.3 Hz) than the WT condition (2.8-3.7 Hz). In addition, stroke volume of mutant ventricles was reduced by 65% in sustained re-entry compared to the WT condition. In conclusion, signs of the S140G mutation might be difficult to identify in sinus rhythm even though the mutant ventricles show shortened QT interval. This suggests that the KCNQ1 S140G mutation increases the risk of death by sudden cardiac arrest. In addition, the KCNQ1 S140G mutation can induce ventricular arrhythmia and lessen ventricular contractility under re-entrant conditions.
参与I电流的KCNQ1 S140G突变会影响心房颤动。然而,其对心脏机械行为的影响却知之甚少。因此,我们使用心脏机电多尺度模型评估了KCNQ1 S140G突变对心室电生理稳定性和机械泵血性能的影响。基于图像的机电模型用于评估KCNQ1 S140G突变对电传播和心律失常发生的影响。此外,还用于比较野生型(WT)和S140G突变条件下的机械反应。从电生理模型获得的细胞内钙瞬变作为输入参数应用于机械模型以实现兴奋-收缩偶联。修改I电流方程以考虑KCNQ1 S140G突变的表达,并包括突变体表达率的比例因子(ϕ)。在单细胞和三维(3D)组织水平比较WT和S140G突变条件。在S140G突变条件下,增强的I电流使动作电位持续时间(APD)缩短了60%,导致QT间期缩短。这使3D窦性心律波长缩短了60%,持续折返缩短了56%。然而,在窦性心律条件下,突变型心室的泵血效率更高。此外,心脏组织中波长的缩短使折返回路形成,并增加了维持室性心动过速和心室颤动的可能性。相比之下,在WT条件下,正常波长(20.8厘米)不太可能在心脏组织中引发和维持折返。随后,S140G突变型心室的主导频率分布范围(2.0-5.3赫兹)高于WT条件(2.8-3.7赫兹)。此外,与WT条件相比,在持续折返中突变型心室的每搏量减少了65%。总之,即使突变型心室的QT间期缩短,在窦性心律中也可能难以识别S140G突变的迹象。这表明KCNQ1 S140G突变增加了心脏性猝死的风险。此外,KCNQ1 S140G突变可诱发室性心律失常,并在折返条件下降低心室收缩力。