- #1
onanox
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I'm trying to solve question 4.12 from Cross and Greenside "pattern formation and dynamics in nonequilibrium systems".
the question is about the equation
[itex] \partial_t u = r u - (\partial_x ^2 +1)^2 u - g_2 u - u^3 [/itex]
Part A: with the ansatz [itex]u=\sum_{n=0}^\infty a_n cos(nx) [/itex] show that the bifurcation retains its pitchfork character and calculate [itex]a_1[/itex] to lowest order in [itex]r[/itex].
Part B: Find a condition on [itex]g_2[/itex] for the bifurcation to be supercritical
Background: The swift-hohenberg equation ([itex]g_2=0[/itex]) has a uniform solution for [itex]r<0[/itex] and undergoes a pitchfork bifurcation when [itex]r>0[/itex] to a stationary nonlinear striped state. The question is asking about generalizing this for [itex]g_2\neq 0[/itex].
Attempt at solution: I tried plugging in the ansatz into the equation and requiring that [itex]\partial_t=0[/itex] to find a stationary state, but got caught up in evaluating [itex]\left[\sum_{n=0}^\infty a_n cos(nx) \right]^2[/itex]. I tried looking back to see how the bifurcation was analyzed in the [itex]g_2=0[/itex] case, and there, we assume a single Fourier mode, find an amplitude equation and its easy to deduce that [itex]|A|\propto |r|^{1/2}[/itex] giving the pitchfork bifurcation.
I think I'm supposed to derive a similar relationship for [itex]a_1[/itex], but I don't know how to evaluate the square and cube of that infinite sum.
Any ideas?
the question is about the equation
[itex] \partial_t u = r u - (\partial_x ^2 +1)^2 u - g_2 u - u^3 [/itex]
Part A: with the ansatz [itex]u=\sum_{n=0}^\infty a_n cos(nx) [/itex] show that the bifurcation retains its pitchfork character and calculate [itex]a_1[/itex] to lowest order in [itex]r[/itex].
Part B: Find a condition on [itex]g_2[/itex] for the bifurcation to be supercritical
Background: The swift-hohenberg equation ([itex]g_2=0[/itex]) has a uniform solution for [itex]r<0[/itex] and undergoes a pitchfork bifurcation when [itex]r>0[/itex] to a stationary nonlinear striped state. The question is asking about generalizing this for [itex]g_2\neq 0[/itex].
Attempt at solution: I tried plugging in the ansatz into the equation and requiring that [itex]\partial_t=0[/itex] to find a stationary state, but got caught up in evaluating [itex]\left[\sum_{n=0}^\infty a_n cos(nx) \right]^2[/itex]. I tried looking back to see how the bifurcation was analyzed in the [itex]g_2=0[/itex] case, and there, we assume a single Fourier mode, find an amplitude equation and its easy to deduce that [itex]|A|\propto |r|^{1/2}[/itex] giving the pitchfork bifurcation.
I think I'm supposed to derive a similar relationship for [itex]a_1[/itex], but I don't know how to evaluate the square and cube of that infinite sum.
Any ideas?