Department of Cardiology, Remin Hospital, Wuhan University, Wuhan, 430060, China.
Curr Med Sci. 2020 Dec;40(6):1191-1202. doi: 10.1007/s11596-020-2308-8. Epub 2021 Jan 11.
Lorenz-RR scatter plot has an obvious shortcoming in that it does not indicate the time when the scatter point happens. On the Lorenz RR scatter plot, one cannot know the time during which the cardiac rhythms take place. Since occurrence of cardiac rhythms is time-related, time should be introduced to such plots. In this study, time was used as abscissa and RR interval (the time interval between the previous RR wave and the R wave) as the ordinate and time was compressed into a visually observable length, and thereby a timed RR-interval scatter plot, or t-RR scatter plot, for short, was developed. On t-RR scatter plot, the patterns were band-shaped or were of linear type. On the t-RR plot, the sinus rhythm presented bands of various widths, with the spiculate or burred upper and lower boundaries, having diurnal variation. Premature beats showed separate layers ("stratification"), the layer number corresponding the number of RR-intervals. With simple premature beats, the layers were clearly separated. With parasystole rhythm, the upper and lower bands or layers might become thicker. With arial premature beats, the space or distance between layers varied. Ventricular premature beats presented equal space or distance between layers. With tachycardia, the lower layer became a "solid" layer. With atrial fibration, the "stratification" disappeared, presenting thicker or widened layers or bands, with neat lower boundary. With atrial flutter, the layers went parallel, with the layers being evenly separated or some distances being exact multiples of others. The second degree atrioventricular block displayed two layers, the lower and upper bands being equally away from the X-axis, presenting a straight line (pacing at a fixed rate) or a thicker or wider bands, with a neat upper boundary (the lowest pacing rate). When the scatter plot presented uncharacteristic patterns or had some scattered points, which rendered diagnosis difficult, a reverse technology could be used. Briefly, upon selection of scattered points, they were subjected to computerization, by regression, to reveal the piece of electrocardiogram (ECG) containing an R wave (QRS complex). Then ECG was analyzed to diagnose the cardiac rhythms. In conclusion, t-RR is a novel methodology which helps us understand heart rhythms from a new perspective.
洛伦兹-RR 散点图有一个明显的缺点,即它不能指示散点出现的时间。在洛伦兹 RR 散点图上,人们无法知道心律失常发生的时间。由于心律失常的发生与时间有关,因此应该在这些图中引入时间。在本研究中,我们使用时间作为横坐标,RR 间期(前一个 RR 波和 R 波之间的时间间隔)作为纵坐标,并将时间压缩到一个可观察的长度,从而得到一个时间 RR 间期散点图,简称 t-RR 散点图。在 t-RR 散点图上,图形呈带状或线性。在 t-RR 图上,窦性节律呈现出各种宽度的带,上下边界呈刺状或模糊状,具有昼夜变化。期前收缩显示出单独的层(“分层”),层的数量与 RR 间期的数量相对应。单纯期前收缩时,各层之间的分层明显。当出现并行节律时,上下带或层可能会变厚。房性期前收缩时,层间的空间或距离会发生变化。室性期前收缩时,各层之间的空间或距离相等。心动过速时,下层变为“实心”层。心房颤动时,“分层”消失,呈现出较厚或较宽的层或带,下界整齐。当心房扑动时,各层平行排列,各层之间的距离均匀或某些距离是其他距离的精确倍数。二度房室传导阻滞显示出两层,下带和上带与 X 轴等距,呈直线(以固定速率起搏)或带较厚或较宽,上界整齐(最低起搏率)。当散点图呈现出非特征性的模式或有一些散点,使得诊断困难时,可以使用反向技术。简要地说,在选择散点后,通过回归对其进行计算机化处理,以揭示包含 R 波(QRS 复合体)的心电图(ECG)片段。然后分析心电图以诊断心律失常。总之,t-RR 是一种新颖的方法学,可以帮助我们从新的角度理解心脏节律。