Chinese Journal of Computational Physics ›› 2023, Vol. 40 ›› Issue (1): 117-126.DOI: 10.19596/j.cnki.1001-246x.8552
• Research Reports • Previous Articles
Chengqian LI(), Furong GUAN, Minyi DENG*(
)
Received:
2022-04-28
Online:
2023-01-25
Published:
2023-07-04
Contact:
Minyi DENG
Chengqian LI, Furong GUAN, Minyi DENG. Effects of Conduction Block and Reentry on Evolution of Spiral Waves[J]. Chinese Journal of Computational Physics, 2023, 40(1): 117-126.
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URL: http://www.cjcp.org.cn/EN/10.19596/j.cnki.1001-246x.8552
Fig.1 Examples of the emergence of (a) conduction block and (b) reentry (The square frames and the figures represent cells and their state values, respectively.)
Fig.2 Patterns of stable spiral waves without CVR at t=30 000 and γ=2 (a)α=2 300, β=34;(b)α=1 400, β=40; (c)α=1 500, β=40; (d)α=2 600, β=36(The white, dark and gray represent the state of rest, excited and refractory, respectively. Deeper gray indicates smaller value of refractory state.)
Fig.3 The concave shape of spiral wave due to CVR and its relation with conduction block (a)~(c)spiral wave patterns; (d)~(f)local state distributions in concave region; (g)~(i)local state distributions in non-concave region (The square frames and figures in local state distributions are the same as in Fig. 1. Colors in patters represent the same as in Fig. 2. The cell with attention is signed with a circle. The end of arrow is at the point where electrical signal arrives, and beginning of the arrow is the source of electrical signal. Parameters are the same as in Fig. 2(a).)
Fig.4 Rhombic shape of spiral wave due to CVR and its relation with conduction block (a)~(c)spiral wave patterns; (d)~(f) local state distributions reflecting conduction blocks along the diagonal direction (Colors in patterns and signals in state distributions represent the same as in Fig. 3. Parameters are the same as in Fig. 2(b).)
Fig.5 Eckhaus instability due to CVR and its relation with conduction block and reentry (a) and (b) patterns during Eckhaus instability process; (c) and (d) local state distributions reflecting the conduction block; (e) and (f) local state distributions reflecting the reentry (Colors in patters and signals in state distributions represent the same as in Fig. 3. Parameters are the same as in Fig. 2(c).)
Fig.6 Doppler instability due to CVR and its relation with conduction block (a)~(d)patterns during Doppler instability process; (e)~(h)local state distributions reflecting the conduction block (Colors in patter and signals in state distributions represent the same as in Fig. 3. Parameters are the same as in Fig. 2(d).)
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
40 | 失败 | 成功 |
35 | 成功 | 失败 |
37 | 成功 | 失败 |
24 | 失败 | 失败 |
21 | 失败 | 失败 |
21 | 失败 | 成功 |
Table 1 Conduction time of a pulse from a cell at (69, 77) in Fig. 3 and excitation situation of its neighbors
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
40 | 失败 | 成功 |
35 | 成功 | 失败 |
37 | 成功 | 失败 |
24 | 失败 | 失败 |
21 | 失败 | 失败 |
21 | 失败 | 成功 |
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
27 | 成功 | 成功 |
27 | 成功 | 成功 |
29 | 成功 | 失败 |
30 | 成功 | 失败 |
30 | 成功 | 失败 |
28 | 成功 | 成功 |
Table 2 Conduction time of a pulse from a cell at (46, 84) in Fig. 3 and excitation situation of its neighbors
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
27 | 成功 | 成功 |
27 | 成功 | 成功 |
29 | 成功 | 失败 |
30 | 成功 | 失败 |
30 | 成功 | 失败 |
28 | 成功 | 成功 |
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
24 | 失败 | 失败 |
45 | 成功 | 成功 |
41 | 成功 | 失败 |
43 | 成功 | 失败 |
38 | 成功 | 失败 |
Table 3 Conduction time of a pulse from a cell at (75, 71) in Fig. 4 and excitation situation of its neighbors
单位距离传导时间 | 激发正向邻居 | 激发斜向邻居 |
24 | 失败 | 失败 |
45 | 成功 | 成功 |
41 | 成功 | 失败 |
43 | 成功 | 失败 |
38 | 成功 | 失败 |
Fig.7 Evolution types of spiral waves under different parameters as CVR is considered (〇, ▽and △ represent stable spiral waves, Eckhaus instability and Doppler instability, respectively.)
1 |
DOI |
2 |
|
3 |
DOI |
4 |
DOI |
5 |
|
6 |
DOI |
7 |
DOI |
8 |
DOI |
9 |
DOI |
10 |
DOI |
11 |
DOI |
12 |
|
13 |
董力耘, 陈立, 段晓茵. 基于教室人群疏散实验的行人流建模和模拟[J]. 物理学报, 2015, 64 (22): 220505.
DOI |
14 |
DOI |
15 |
|
16 |
DOI |
17 |
|
18 |
DOI |
19 |
|
20 |
DOI |
21 |
张学良, 谭惠丽, 白克钊, 等. 一种体现心肌细胞传导记忆的元胞自动机模型[J]. 广西师范大学学报(自然科学版), 2017, 35 (4): 1- 9.
|
22 |
DOI |
23 |
欧阳颀. 反应扩散系统中螺旋波的失稳[J]. 物理, 2001, 30 (1): 30- 36.
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