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A delay differential equation is an ODE which allows the use of
previous values. In this case, the function needs to be a JIT compiled
Julia function. It looks just like the ODE, except in this case there is
a function h(p,t)
which allows you to interpolate and grab
previous values.
We must provide a history function h(p,t)
that gives
values for u
before t0
. Here we assume that
the solution was constant before the initial time point. Additionally,
we pass constant_lags = c(20.0)
to tell the solver that
only constant-time lags were used and what the lag length was. This
helps improve the solver accuracy by accurately stepping at the points
of discontinuity. Together this is:
f <- JuliaCall::julia_eval("function f(du, u, h, p, t)
du[1] = 1.1/(1 + sqrt(10)*(h(p, t-20)[1])^(5/4)) - 10*u[1]/(1 + 40*u[2])
du[2] = 100*u[1]/(1 + 40*u[2]) - 2.43*u[2]
end")
h <- JuliaCall::julia_eval("function h(p, t)
[1.05767027/3, 1.030713491/3]
end")
u0 <- c(1.05767027/3, 1.030713491/3)
tspan <- c(0.0, 100.0)
constant_lags <- c(20.0)
JuliaCall::julia_assign("u0", u0)
JuliaCall::julia_assign("tspan", tspan)
JuliaCall::julia_assign("constant_lags", tspan)
prob <- JuliaCall::julia_eval("DDEProblem(f, u0, h, tspan, constant_lags = constant_lags)")
sol <- de$solve(prob,de$MethodOfSteps(de$Tsit5()))
udf <- as.data.frame(t(sapply(sol$u,identity)))
plotly::plot_ly(udf, x = sol$t, y = ~V1, type = 'scatter', mode = 'lines') %>% plotly::add_trace(y = ~V2)
Notice that the solver accurately is able to simulate the kink
(discontinuity) at t=20
due to the discontinuity of the
derivative at the initial time point! This is why declaring
discontinuities can enhance the solver accuracy.
These binaries (installable software) and packages are in development.
They may not be fully stable and should be used with caution. We make no claims about them.