Rethinking Beetles Noise
 Noise in the larval class is damped by [math]\displaystyle{ \partial_L f_L }[/math] and grows proportional to its intrinsic variation and the contribution of other classes through their derivatives of [math]\displaystyle{ f_L }[/math], that is, [math]\displaystyle{ \partial_E f_l }[/math] as well as the sum of its intrinsic rates (essentially whichever is larger). Taking E dynamics to be fast we might reduce to a continous time LPA model:
 [math]\displaystyle{
\begin{align}
& \dot L = a_e \frac{bA  c_{ea} A  c_{el} L}{a_e + \mu_e}  a_l  \mu_l \\
& \dot P = a_l L  \mu_p P  a_p P \\
& \dot A = a_p P  \mu_a A
\end{align}
}[/math]
and the larval fluctuations are essentially:
 [math]\displaystyle{
\begin{align}
\sigma^2_L &= \frac{\nu + \beta_L}{2 \partial_L f_L} \\
\nu &= \frac{ 2(\partial_A f_L)^2 \sigma_A^2 }{\partial_L f_L + \partial_A f_A} \\
\partial_A L &= \frac{a_e (b  c_{ea} ) }{a_e + \mu_e}
\end{align}
}[/math]
where [math]\displaystyle{ \beta_i }[/math] is the intrinsic noise of the age class. Hence a class i which propagates large noise to another class j has a large [math]\displaystyle{ \partial_i f_j }[/math]. If this term is a linear transition [math]\displaystyle{ \lambda X_i }[/math], then the same term appears in [math]\displaystyle{ f_i }[/math] and hence damps the noise [math]\displaystyle{ \sigma_i^2 }[/math] and cancels out. Hence noise must propagate into a class through nonlinear transition rates OR through an asymmetry in the transition (i.e. the c_1, c_2 large noise example in the generalized crowley).
Compare to noise in Eggs:
 [math]\displaystyle{
\sigma^2_E = \frac{ \frac{ (\sigma_L^2 c_{el} +\sigma_A^2 c_{ea} )E^2 }{\mu_A + \mu_L + a_L}+ \beta_E/2}{\mu_E + c_{ea} A + c_{el} L + a_e}
}[/math]
Adding age delay to beetle dynamics
Current formulation has used exponential waiting times between stages. By subdividing the classes (increasing the system dimension size) and creating single jump withinstate transitions, these become gammadistributed waiting times. Adding ten steps to each phase and a little parameter fiddling introduces sustained oscillations. (Versionstable code).
beetle_pars < c(b=5, ue= 0, ul = 0.001, up = 0.00001, ua = 0.01, ae = 1.3, al = .1, ap = 1.5, cle = .2, cap = .1, cae = 5, V=100)
Xo[1] = 100
 Implementation still needs troubleshooting, variance dynamics don't seem to be being computed correctly. done
 Adult class doesn't need multiple stages. done
 Code should allow for a general k classes rather than a fixed 10 classes. done
and now we have noise in oscillatory, gammawaiting model:
Misc / Code notes
 Revolution parallelizes the variance dynamics calculation (perhaps the matrix multiplication step?) and is probably responsible for the openmp parallelization working.
 article on cloud computing vs grid. reminds me to include questions on cloud computing in the CSGF survey.
 Should also take a closer read of the recent: Kendall BE, Wittmann ME. A stochastic model for annual reproductive success. The American naturalist. 2010;175(4):4618. Available at: http://www.ncbi.nlm.nih.gov/pubmed/20163244.
