Considering the following physical situation:
and writing the following code:
m := 1.52
g := 9.81
us := 0.15
uk := 0.10
k := 2.12
xi := 4.00
vi := 0.00
tmax := 10
P := m g
Fs := us P
Fk := uk P
Fe[t_] := -k x[t]
sol = NDSolve[{
Fe[t] - Sign[x'[t]] Fk == m x''[t],
x[0] == xi,
x'[0] == vi},
x, {t, 0, tmax}];
Plot[Evaluate[{
Sign[x'[t]] Fs,
Fe[t],
x[t]} /. sol],
{t, 0, tmax},
AxesLabel -> {"t", "fct[t]"},
PlotLegends -> {"-Fs", "Fe", "x"}]
you get the following graph:
which shows that oscillations are over for $t \approx 8\,s$ causes kinematic friction.
On the other hand, putting us = 0.40
you get this other graph:
which shows that oscillations are over for $t \approx 3\,s$ causes static friction.
Question: is it possible to automate all this by making the x(t)
graph plot until the motion stops?
Fk
inNDSolve
but plotFs
. Is this intended? Secondly, what exactly happens at 8s resp. 3s? I don't see anything significant at those times in the plots you provided. (Also,x[t]
seems nearly identical between the two plots, is this intended?) $\endgroup$