Численные эксперименты с использованием модели ФитцХью-Нагумо (серия 01)
Приложение 02. Переход ревербератора
из режима гипоциклоиды в режим эпициклоиды
при e=0.2 и увеличении b
от 0.600 до 0.975 с шагом Db=0.010.
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| e=0.1 | e=0.2 | e=0.3 |
b=0.600 |
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b=0.610 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.620 |
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b=0.630 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.640 |
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b=0.650 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.660 |
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b=0.670 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.680 |
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b=0.690 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.700 |
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b=0.710 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.720 |
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b=0.730 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.740 |
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b=0.750 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.760 |
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b=0.770 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.780 |
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b=0.790 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.800 |
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b=0.810 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.820 |
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b=0.830 |
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| e=0.1 | e=0.2 | e=0.3 |
b=0.840 |
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b=0.850 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.860 |
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NONE |
b=0.870 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.880 |
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NONE |
b=0.890 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.900 |
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NONE |
b=0.910 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.920 |
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NONE |
b=0.930 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.940 |
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NONE |
b=0.945 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.950 |
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NONE |
b=0.955 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.960 |
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NONE |
b=0.965 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.970 |
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NONE |
b=0.975 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=0.980 |
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NONE |
b=0.990 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
b=1.000 |
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NONE |
| e=0.1 | e=0.2 | e=0.3 |
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