temporary point on the inner loop wrapper
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50
julia/test/inner_loop/find_closest.jl
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50
julia/test/inner_loop/find_closest.jl
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@testset "Find Closest" begin
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println("Testing NLP solver")
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using NLsolve, PlotlyJS
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# Initial Setup
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sc = Sc("test")
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a = rand(25000:1.:40000)
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e = rand(0.01:0.01:0.05)
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i = rand(0.01:0.01:π/6)
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T = 2π*√(a^3/μs["Earth"])
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prop_time = T
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n = 10
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# A simple orbit raising
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start = oe_to_xyz([ a, e, i, 0., 0., 0. ], μs["Earth"])
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Tx, Ty, Tz = conv_T(repeat([0.6], n), repeat([0.], n), repeat([0.], n),
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start,
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sc.mass,
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sc,
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prop_time,
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μs["Earth"])
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final = prop(hcat(Tx, Ty, Tz), start, sc, μs["Earth"], prop_time)[3]
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new_T = 2π*√(xyz_to_oe(final, μs["Earth"])[1]^3/μs["Earth"])
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# This should be close enough to 0.6 for convergence
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Tx, Ty, Tz = conv_T(repeat([0.59], n), repeat([0.01], n), repeat([0.], n),
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start,
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sc.mass,
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sc,
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prop_time,
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μs["Earth"])
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result = nlp_solve(start, final, sc, μs["Earth"], 0.0, prop_time, hcat(Tx, Ty, Tz))
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# Test and plot
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@test converged(result)
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path1 = prop(zeros((100,3)), start, sc, μs["Earth"], T)[1]
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path2, mass, calc_final = prop(tanh.(result.zero), start, sc, μs["Earth"], prop_time)
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path3 = prop(zeros((100,3)), calc_final, sc, μs["Earth"], new_T)[1]
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path4 = prop(zeros((100,3)), final, sc, μs["Earth"], new_T)[1]
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savefig(plot_orbits([path1, path2, path3, path4],
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labels=["initial", "transit", "after transit", "final"],
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colors=["#FFFFFF","#FF4444","#44FF44","#4444FF"]),
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"../plots/find_closest_test.html")
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if converged(result)
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@test norm(calc_final - final) < 1e-4
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end
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end
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13
julia/test/inner_loop/inner_loop.jl
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13
julia/test/inner_loop/inner_loop.jl
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@testset "Inner Loop" begin
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println("Testing Inner Loop")
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using Dates
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phase1 = Phase("Earth", "Mars", 3600*24*365*1.5, 5., 2.)
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phase2 = Phase("Mars", "Jupiter", 3600*24*365*3.5, 2., 0.1)
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inner_loop(DateTime(2024,3,5), 0.3, 0.4, [phase1, phase2])
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@test true
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end
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31
julia/test/inner_loop/laguerre-conway.jl
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31
julia/test/inner_loop/laguerre-conway.jl
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@testset "Laguerre-Conway" begin
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println("Testing LaGuerre-Conway")
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using Thesis: laguerre_conway
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# Test that the propagator produces good periodic orbits (forwards and backwards)
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for T in rand(3600*1.5:3600*4, (5))
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start = oe_to_xyz([ (μs["Earth"]*(T/(2π))^2)^(1/3), rand(0.01:0.01:0.5), rand(0.01:0.01:0.45π), 0., 0., 1. ], μs["Earth"])
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orbit = start
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for _ in 1:5
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i = 0.
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while i < T
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orbit = laguerre_conway(orbit, μs["Earth"], 1.)
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i += 1
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end
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@test i ≈ T
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@test norm(orbit - start) < 1e-2
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end
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for _ in 1:5
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i = 0.
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while i > -T
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orbit = laguerre_conway(orbit, μs["Earth"], -1.)
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i -= 1
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end
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@test i ≈ -T
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@test norm(orbit - start) < 1e-2
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end
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end
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end
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70
julia/test/inner_loop/monotonic_basin_hopping.jl
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julia/test/inner_loop/monotonic_basin_hopping.jl
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@testset "Monotonic Basin Hopping" begin
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println("Testing Monotonic Basin Hopper")
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# Initial Setup
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sc = Sc("test")
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a = rand(15000:1.:40000)
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e = rand(0.01:0.01:0.5)
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i = rand(0.01:0.01:π/6)
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T = 2π*√(a^3/μs["Earth"])
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prop_time = 0.75T
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n = 10
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# A simple orbit raising
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start = oe_to_xyz([ a, e, i, 0., 0., 0. ], μs["Earth"])
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# T_craft = hcat(repeat([0.6], n), repeat([0.], n), repeat([0.], n))
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Tx, Ty, Tz = conv_T(repeat([0.8], n), repeat([0.], n), repeat([0.], n),
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start,
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sc.mass,
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sc,
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prop_time,
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μs["Earth"])
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nominal_path, normal_mass, final = prop(hcat(Tx, Ty, Tz), start, sc, μs["Earth"], prop_time)
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new_T = 2π*√(xyz_to_oe(final, μs["Earth"])[1]^3/μs["Earth"])
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# Find the best solution
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best, archive = mbh(start,
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final,
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sc,
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μs["Earth"],
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0.0,
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prop_time,
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n,
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num_iters=5,
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patience_level=50,
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verbose=true)
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# Test and plot
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@test converged(best)
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transit, best_masses, calc_final = prop(tanh.(best.zero), start, sc, μs["Earth"], prop_time)
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initial_path = prop(zeros((100,3)), start, sc, μs["Earth"], T)[1]
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after_transit = prop(zeros((100,3)), calc_final, sc, μs["Earth"], new_T)[1]
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final_path = prop(zeros((100,3)), final, sc, μs["Earth"], new_T)[1]
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savefig(plot_orbits([initial_path, nominal_path, final_path],
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labels=["initial", "nominal transit", "final"],
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colors=["#FF4444","#44FF44","#4444FF"]),
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"../plots/mbh_nominal.html")
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savefig(plot_orbits([initial_path, transit, after_transit, final_path],
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labels=["initial", "transit", "after transit", "final"],
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colors=["#FFFFFF", "#FF4444","#44FF44","#4444FF"]),
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"../plots/mbh_best.html")
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i = 0
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best_mass = best_masses[end]
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nominal_mass = normal_mass[end]
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masses = []
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for candidate in archive
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@test converged(candidate)
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path2, cand_ms, calc_final = prop(tanh.(candidate.zero), start, sc, μs["Earth"], prop_time)
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push!(masses, cand_ms[end])
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@test norm(calc_final - final) < 1e-4
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end
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@test best_mass == maximum(masses)
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# This won't always work since the test is reduced in fidelity,
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# but hopefully will usually work:
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@test (sc.mass - best_mass) < 1.1 * (sc.mass - nominal_mass)
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@show best_mass
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@show nominal_mass
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end
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41
julia/test/inner_loop/propagator.jl
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41
julia/test/inner_loop/propagator.jl
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@testset "Propagator" begin
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println("Testing propagator")
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using Thesis: prop_one
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# Set up
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start = oe_to_xyz([ (μs["Earth"]*(rand(3600*1.5:0.01:3600*4)/(2π))^2)^(1/3),
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rand(0.01:0.01:0.5),
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rand(0.01:0.01:0.45π),
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0.,
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0.,
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1. ], μs["Earth"])
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stepsize = rand(100.0:0.01:500.0)
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# Test that Laguerre-Conway is the default propagator
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propped = prop_one([0., 0., 0.], start, 0., 0, 0., 1000., 0.1, μs["Earth"], stepsize)
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@test laguerre_conway(start, μs["Earth"], stepsize) ≈ propped[1]
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# Test that Laguerre-Conway is the default propagator for spacecrafts
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craft = Sc("no_thrust")
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start_mass = craft.mass
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state, craft = prop_one([0., 0., 0.], start, craft, μs["Earth"], stepsize)
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@test laguerre_conway(start, μs["Earth"], stepsize) ≈ state
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@test craft.mass == start_mass
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# Test that mass is reduced properly
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craft = Sc("test")
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start_mass = craft.mass
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state, craft = prop_one([1., 0., 0.], start, craft, μs["Earth"], stepsize)
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@test craft.mass == start_mass - craft.mass_flow_rate*stepsize
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# Test that a bad ΔV throws an error
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# craft = Sc("test")
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# start_mass = craft.mass
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# @test_throws ErrorException prop_one([1.5, 0., 0.], start, craft, μs["Earth"], stepsize)
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# Test that a full propagation doesn't take too long
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end
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