Comments (2)
Because you can use it to save the branch while being computed. For example, in memory limited (GPU...) you cannot keep the branch with all eigenvectors in RAM whereas this info is needed to compute bifurcations. Hence, I propose saving this info on the disk every once in a while. This is set by ContinuationPar.saveToFile
.
Maybe I can increase the version in Project.toml
, it seems JLD2 has improved a lot.
from bifurcationkit.jl.
Yeap, have a look: https://discourse.julialang.org/t/ann-jld2-v0-2-0/45843
You can also use CompatHelper.jl to become aware of bound changes.
from bifurcationkit.jl.
Related Issues (20)
- typos HOT 3
- acceptSolution in DefCont() not used HOT 1
- continuation of periodic orbit from Hopf curve HOT 1
- Issue when implementing the KdV equation HOT 9
- Continuation of LPC from Bautin/GH point HOT 2
- Out of memory for 1D periodic non-linear system HOT 8
- Plotting with Makie HOT 3
- Getting print statements despite `verbosity=0` HOT 6
- BifurcationKit not working with ArrayPartitions ? HOT 1
- br.specialpoint[n].x different from getSolx(br, br.specialpoint[n].idx) HOT 1
- finaliseSolution not being called for codim2 fold point continuation HOT 3
- Move to `JuliaDynamics` org HOT 4
- Dependencies update HOT 15
- Is it possible to provide derivatives with respect to the parameter "p" ? + Minimal example with fold bifurcations that doesn't work HOT 8
- Convenient way to obtain the plotted elements HOT 22
- Reexport Setfield HOT 2
- Document what short names of bifurcations stand for HOT 11
- Use Julian style of code? HOT 8
- Continuation doesn't start when using Natural() and pMin = p0 HOT 1
- No way to set BifFunction's delta parameter HOT 2
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from bifurcationkit.jl.