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December 1, 2021 00:59
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ModelingToolkit.jl mechanical example.
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using ModelingToolkit, OrdinaryDiffEq | |
@variables t | |
D = Differential(t) | |
"The basic unit of the mechanical systems is a body with a position and a force" | |
@connector function Body(; name) | |
sts = @variables x(t) F(t) | |
ODESystem(Equation[], t, sts, []; name = name) | |
end | |
"The forces on connected bodies sum to zero. Bodies that are connected are in | |
the same place." | |
function ModelingToolkit.connect(::Type{Body}, ps...) | |
eqs = [0 ~ sum(p -> p.F, ps)] | |
for i = 1:(length(ps) - 1) | |
push!(eqs, ps[i].x ~ ps[i + 1].x) | |
end | |
eqs | |
end | |
"A body that never moves." | |
function Fixed(; name) | |
@named ground = Body() | |
eqs = [D(ground.x) ~ 0] | |
ODESystem(eqs, t, [], []; systems = [ground], name = name) | |
end | |
"A massive object obeys Newtons second law." | |
function Mass(; name, m = 1.0) | |
@named mass = Body() | |
val = [m] | |
ps = @parameters m | |
sts = @variables v(t) | |
eqs = [D(mass.x) ~ v, D(v) ~ mass.F / m] | |
ODESystem(eqs, t, sts, ps; systems = [mass], defaults = Dict(zip(ps, val)), name = name) | |
end | |
"The force applied by a linear spring is proportional to the distance between | |
its ends. This spring has zero length." | |
function Spring(; name, k = 1.0) | |
@named left = Body() | |
@named right = Body() | |
vals = [k] | |
ps = @parameters k | |
eqs = [left.F ~ -k * (right.x - left.x), 0 ~ right.F + left.F] | |
ODESystem( | |
eqs, | |
t, | |
[], | |
ps; | |
systems = [left, right], | |
defaults = Dict(zip(ps, vals)), | |
name = name, | |
) | |
end | |
"BOING!!!" | |
function simple_example() | |
@named g = Fixed() | |
@named s = Spring() | |
@named m = Mass() | |
eqs = [connect(g.ground, s.left)..., connect(s.right, m.mass)...] | |
@named oscillator = ODESystem(eqs, t, [], []; systems = [g, s, m]) | |
simplified_oscillator = structural_simplify(oscillator) | |
u0 = Dict(g.ground.x => 0.0, m.mass.x => 0.0, m.v => 1.0) | |
prob = ODEProblem(simplified_oscillator, u0, (0.0, 10.0)) | |
soln = solve(prob, Tsit5()) | |
@assert(all([abs(soln.u[j][2] - sin(soln.t[j])) < 5e-4 for j = 1:length(soln)])) | |
@assert(all([abs(soln.u[j][3] - cos(soln.t[j])) < 5e-4 for j = 1:length(soln)])) | |
soln | |
end | |
"The distance from the moving body to the fixed body must stay between min and max." | |
function Limits(; name, min = 0.0, max = 1.0, cor = 0) | |
@named fixed = Body() | |
@named moving = Body() | |
val = [min, max, cor] | |
ps = @parameters min max cor | |
sts = @variables v(t) | |
l = moving.x - fixed.x | |
eqs = [ | |
D(moving.x) ~ v, | |
# when against the stop, forces balance, otherwise zero | |
fixed.F ~ -moving.F * ((l == min) + (l == max)), | |
moving.F ~ -fixed.F * ((l == min) + (l == max)), | |
] | |
# Bounce off limits with coefficinet of restitution | |
continuous_events = [[0 ~ min - l, 0 ~ max - l] => [v ~ -cor * v]] | |
ODESystem( | |
eqs, | |
t, | |
sts, | |
ps; | |
systems = [fixed, moving], | |
defaults = Dict(zip(ps, val)), | |
continuous_events = continuous_events, | |
name = name, | |
) | |
end | |
function limit_example() | |
@named g = Fixed() | |
@named s = Spring(k=10) | |
@named m = Mass() | |
@named l = Limits(min = -0.5, max = 0.5) | |
eqs = [connect(g.ground, s.left, l.fixed)..., connect(s.right, m.mass, l.moving)...] | |
@named limited_oscillator = ODESystem(eqs, t, [], []; systems = [g, s, m, l]) | |
limited_oscillator = structural_simplify(limited_oscillator) | |
u0 = Dict( | |
g.ground.x => 0.0, | |
m.mass.x => 0.0, | |
m.v => 1.0, | |
l.moving.x => 0.0, | |
l.moving.F => 0.0, | |
) | |
prob = ODEProblem(limited_oscillator, u0, (0.0, 10.0)) | |
soln = solve(prob, Rodas5()) | |
limited_oscillator, prob, soln | |
end |
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