86 research outputs found
An Empirical Test of Harrod’s Model
After having illustrated in Chap. 13 the Harrod’s model and a chaotic specification of it, in this Chapter we are going to prove that (1) real data could be obtained by a suitable calibration of model’s parameters, (2) the calibrated model confirms theoretical predictions (Orlando and Della Rossa, Mathematics 7(6):524, 2019)
Optimal Regulation of Blood Glucose Level in Type I Diabetes using Insulin and Glucagon
The Glucose-Insulin-Glucagon nonlinear model [1-4] accurately describes how
the body responds to exogenously supplied insulin and glucagon in patients
affected by Type I diabetes. Based on this model, we design infusion rates of
either insulin (monotherapy) or insulin and glucagon (dual therapy) that can
optimally maintain the blood glucose level within desired limits after
consumption of a meal and prevent the onset of both hypoglycemia and
hyperglycemia. This problem is formulated as a nonlinear optimal control
problem, which we solve using the numerical optimal control package PSOPT.
Interestingly, in the case of monotherapy, we find the optimal solution is
close to the standard method of insulin based glucose regulation, which is to
assume a variable amount of insulin half an hour before each meal. We also find
that the optimal dual therapy (that uses both insulin and glucagon) is better
able to regulate glucose as compared to using insulin alone. We also propose an
ad-hoc rule for both the dosage and the time of delivery of insulin and
glucagon.Comment: Accepted for publication in PLOS ON
Numerical periodic normalization for codim 2 bifurcations of limit cycles : computational formulas, numerical implementation, and examples
Explicit computational formulas for the coefficients of the periodic normal forms for codimension 2 (codim 2) bifurcations of limit cycles in generic autonomous ODEs are derived. All cases (except the weak resonances) with no more than three Floquet multipliers on the unit circle are covered. The resulting formulas are independent of the dimension of the phase space and involve solutions of certain boundary-value problems on the interval [0, T], where T is the period of the critical cycle, as well as multilinear functions from the Taylor expansion of the ODE right-hand side near the cycle. The formulas allow one to distinguish between various bifurcation scenarios near codim 2 bifurcations of limit cycles. Our formulation makes it possible to use robust numerical boundary-value algorithms based on orthogonal collocation, rather than shooting techniques, which greatly expands its applicability. The implementation is described in detail with numerical examples, where numerous codim 2 bifurcations of limit cycles are analyzed for the first time
Qualitative resonance of feedback-controlled chaotic oscillators
The qualitative resonance of feedback-controlled chaotic oscillators is the ability of the control system to qualitatively synchronize with a reference signal similar to one of the unstable periodic orbits embedded in the open-loop attractor. This property, discovered by O. De Feo (2004a; 2004b) while studying Shilnikov-type attractors, was explained in terms of the random-like rephasing mechanism characterizing the oscillator's dynamics, so to guarantee the eventual in-phase looking with the reference forcing. We experimentally show that the phenomenon works more in general, even in the absence of a rephasing mechanism. Intuitively, the forcing by the target cycle, or by a qualitative approximation of it, is sufficient to bring in the in-phase condition. Our results can make chaos control more practicable than so far imagined, as a qualitative control can be achieved with no a-priori knowledge about the target solution
The Harrod Model
As mentioned in the Introduction, Sect. 1.2, the objective of this book is twofold: to provide a personal specification of a business cycle model within the Kaldor–Kalecki framework (see Chap. 16) and to choose a chaotic specification of the Harrod model (Sportelli and Celi (Metroeconomica 62:459–493, 2011)) to prove that (1) real data can be obtained by a suitable calibration of model’s parameters and (2) the calibrated model confirms theoretical predictions (Orlando and Della Rossa (Mathematics 7:524, 2019)).
In this chapter, we first explain the Domar model and the Harrod model separately, and then we describe the mathematical foundation to the Harrod’s instability principle that will be tested then in Chap. 18
Applied Spectral Analysis
In this chapter, we first explain what we mean by a signal, and then we describe some characteristics such as energy, frequency, phase, power spectrum, etc. We show how to analyse it by the means of spectral analysis and Fourier transform. Moreover, as the Fourier transform does not provide any information about the time at which each frequency appears, we explain how to deal with this problem with the Gabor and wavelet transform
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