|
222 | 222 | \\end{aligned} |
223 | 223 | ``` |
224 | 224 |
|
225 | | -The Hénon–Heiles system [1] was introduced as a simplification of the motion |
| 225 | +The Hénon–Heiles system [1] is a conservative dynamical system and was introduced as a simplification of the motion |
226 | 226 | of a star around a galactic center. It was originally intended to study the |
227 | 227 | existence of a "third integral of motion" (which would make this 4D system integrable). |
228 | 228 | In that search, the authors encountered chaos, as the third integral existed |
|
283 | 283 | """ |
284 | 284 | qbh([u0]; A=1.0, B=0.55, D=0.4) |
285 | 285 |
|
| 286 | +A conservative dynamical system with rule |
286 | 287 | ```math |
287 | 288 | \\begin{aligned} |
288 | 289 | \\dot{q}_0 &= A p_0 \\\\ |
@@ -533,7 +534,7 @@ labyrinth(u0 = [1.0, 0, 0]) |
533 | 534 | \\begin{aligned} |
534 | 535 | \\dot{x} &= \\sin(y) \\\\ |
535 | 536 | \\dot{y} &= \\sin(z) \\\\ |
536 | | -\\dot{V} &= \\sin(x) |
| 537 | +\\dot{z} &= \\sin(x) |
537 | 538 | \\end{aligned} |
538 | 539 | ``` |
539 | 540 | Three dimensional conservative continuous system, whose evolution in 3D space |
@@ -590,8 +591,6 @@ normalized such that for energy value of 1 it is a circle of diameter ``d0``. |
590 | 591 | The magnetic field is also normalized such that for value `B=1` the cyclotron |
591 | 592 | diameter is 1. |
592 | 593 |
|
593 | | -Fo more details see [1]. |
594 | | -
|
595 | 594 | [1] : G. Datseris *et al*, [New Journal of Physics 2019](https://iopscience.iop.org/article/10.1088/1367-2630/ab19cc/meta) |
596 | 595 | """ |
597 | 596 | function antidots(u0 = [0.5, 0.5, rand(2)...]; |
@@ -740,3 +739,21 @@ function magnetic_pendulum(u = [sincos(rand()*2π)..., 0, 0]; |
740 | 739 | p = [γ, d, α, ω] |
741 | 740 | ds = ContinuousDynamicalSystem(m, u, p) |
742 | 741 | end |
| 742 | + |
| 743 | +""" |
| 744 | + fitzhugh_nagumo(u = 0.5ones(2); I = 1.0) |
| 745 | +Famous excitable system which emulates the firing of a neuron, with equations |
| 746 | +```math |
| 747 | +\\begin{aligned} |
| 748 | +\\dot{v} &= v - v^3/3 - w + I \\\\ |
| 749 | +\\ddot{y} &= 0.08(v + 0.7 - 0.8w) |
| 750 | +\\end{aligned} |
| 751 | +``` |
| 752 | +
|
| 753 | +More details in the [Scholarpedia](http://www.scholarpedia.org/article/FitzHugh-Nagumo_model) entry. |
| 754 | +""" |
| 755 | +function fitzhugh_nagumo(u = 0.5ones(2); I = 1.0) |
| 756 | + ds = ContinuousDynamicalSystem(fitzhugh_nagumo_eom, u, [I]) |
| 757 | +end |
| 758 | +fitzhugh_nagumo_eom(u, p, t) = |
| 759 | +SVector(u[1] - u[1]^3/3 - u[2] + p[1], 0.08(u[1] + 0.7 - 0.8u[2])) |
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