1. Introduction
In the last two decades, chaotic dynamics have been widely used in real-world applications such as biological systems [1], brain modeling [2], weather modeling [3], vibration modeling [4], mechanical and electrical engineering [5,6], control and synchronization [7,8,19], robotics [9,10], and more [12-15,20,21]. Currently, it is an active area of research by many in biology, physics, sociology, psychology, physiology, and engineering. However, this research is not only performed in natural sciences but also in the social sciences, including politics, economics, and the prediction of societal events composed of various addiction problems [12,18,19].
Addictions caused by tobacco, drugs, games, shopping, and the Internet are serious problems in our current society and many researchers are interested in treating and curing these addictions. Due to the different nature of each addiction, each symptom differs dramatically from one to the other. Therefore, it is not so easy to define encompassing symptoms for all the addictions mathematically [16]. Tobacco addiction has been subject to intense investigation by medical research groups. However, they mainly approach the tobacco addiction epidemiologically rather than mathematically. Therefore, it is necessary to develop a mathematical model of nonlinear phenomena in addiction of tobacco.
In this paper, we propose a dynamic model of tobacco addiction that originates from the dynamics of tobacco use, recovery, and relapse [17]. In order to make an addiction model of tobacco, we try to modify and rescale from the existing chaotic tobacco model and Lorenz model. By using this information, we derive a new tobacco addiction model mathematically. Finally, we obtain periodic and chaotic motion from the addiction model of tobacco. We say that periodic motion and quasi-periodic motion are related to the pre-addiction stage or recovery stage, respectively. Quasiperiodic and chaotic motion are related to the addiction stage and relapse stage, respectively.
2. Dynamic Model of Lorenz System
The mathematical models of the Lorenz system proposed by Edward L. Lorenz describe various dynamical models of weather systems. The formulation of the Lorenz system is given by the following Eq. (1).
where sigma is called the Prandtl number, which is the ratio of momentum diffusivity (kinematic viscosity) and thermal diffusivity; ρ is the Rayleigh number, which is determined by the heat transfer, primarily in the form of conduction or convection; and β is a geometric factor. The typical values of these three parameters are σ = 10, ρ = 28, β = 8/3; x is proportional to the intensity of convection motion; y is proportional to the temperature difference between the ascending and descending currents; and z is proportional to the distortion of the vertical temperature profile from linearity.
3. Dynamic Model of Tobacco Use, Recovery, and Relapse
Carlos Castillo-Garsow et al. [17] proposed mathematical models for the dynamics of tobacco use, recovery, and relapse.
They described the general model for drug abuse, vital dynamics, and nonlinear relapse. From these mathematical models, they found the parameter value by using stability theory.
3.1 General Mathematical Model for Drug Abuse
From the model proposed by Carlos Castillo-Garsow et al. [17], a general mathematical model for drug abuse is shown as Figure 1 and can be represented as s Eq. (2).
Figure 1.A general mathematical model for drug abuse.
where S is the total number of individuals in a given population that are susceptible to becoming regular drug users. D is a habitual drug user in that population, and R is the number of people recovered from habitual use. The parameters β, γ, and δ are per capita influence rate, recovery rate per habitual drug user per unit of time, and relapse rate per recovered individual per unit of time, respectively.
3.2 General Mathematical Model for Drug Abuse with Vital Dynamics
Because Eq. (2) assumes a constant population, we need to consider constant mortality rate, following as Eq. (3).
where μ is the constant mortality rate.
The previous two models did not provide the mechanism for the relapse process. We consider a similar peer pressure mechanism for relapse of recovered individuals. Eq. (4) represents relapse of recovered individuals.
3.3 Parameter Rescaling
In order to derive chaotic or nonlinear phenomena from Eqs. (2) and (3), we need to modify these equations. From Eqs. (2) and (3), we obtain a solution, which is shown in Figure 2 and 3. Figures 2 and 3 show time-series and a phase portrait for Eqs. (2)-(4), respectively. Here, we use N = 100, δ = 0.89, γ = 0.15, and β = 0.625 for Eq. (2), N = 100, μ = 0.1, δ = 0.89, α = 0.4, γ = 0.15, and β = 0.625 for Eq. (3), and N = 100, μ = 0.1, δ = 0.89, α = 0.4, γ = 0.15, and β = 0.625, R = 2.5 for Eq. (4). We recognize that there is no vibration or fluctuation because Eqs. (2) and (3) lack a nonlinear term.
Figure 2.Time series and phase protrait from Eq. (2).
Figure 3.Time series and phase portrait from Eq. (3).
Figure 4.Time series and phase portrait from Eq. (4).
To make a similar Lorenz equation such as Eq. (1) from Eq. (2), we need parameter rescaling and some substitution. To do this, we rescale each parameter x, y, and z, as described in Eqs. (5)-(7).
When we take derivatives of Eqs. (5)-(7), we obtain Eqs. (8)-(10).
We can set Eq. (1) equal to Eqs. (8)-(10). The new equation can be written as Eqs. (11)-(13).
From Eqs. (11)-(13), we can rearrange a new dynamic equation for tobacco use, recovery, and relapse, as shown in Eqs. (14)-(16).
In order to display nonlinear phenomena from Eqs. (14)–(16), we define each parameter in the previously shown equations to find periodic motion and chaotic motion.
3.4 Pre-addiction, Addiction Recovery, and Relapse Stages
From Eqs. (14)-(16), after assigning parameter values for α, γ, and δ, we varied σ, ρ, and β. As a result, we obtained various time series, phase portraits, and Poincaré for the pre-addiction stage of tobacco, as shown in Figure 5 and 6. The pre-addiction stage has a periodic motion, as with the following:
Figure 5.Time series, phase portrait, and Poincaré map of pre-addiction stage of tobacco model (periodic motion).
Figure 6.Time series, phase portrait, and Poincaré map of pre-addiction stage of tobacco model (periodic motion).
We obtain various time series, phase portraits, and Poincaré maps for the addiction stage of tobacco as the parameters vary. These are shown in Figures 7 and 8. These addiction stages show chaotic motions such as quasi-chaotic and chaotic attractor.
Figure 7.Time series, phase portrait, and Poincaré map of addiction stage (chaotic motion).
Figure 8.Time series, phase portrait, and Poincaré map of addiction stage (chaotic motion).
We also obtain another time series, phase portrait, and Poincaré map for the recovery stage of tobacco, as shown in Figure 9. The recovery stage has a quasi-periodic motion unlike the chaotic attractors of Figures 7 and 8. We also varied parameters of σ, ρ, and β, and obtained another phase portrait for the re-addiction stage of tobacco, as shown in Figure 10. The re-addiction stage displays chaotic motion well.
Figure 9.Time series, phase portrait, and Poincaré maps of recovery stage of tobacco model (quasi-periodic motion).
Figure 10.Time series, phase portrait, and Poincaré map of re-addiction stage of tobacco model (chaotic motion).
When we change the parameter valuesσ, ρ, and β accordingly, we obtain the relapse stage of the tobacco model, as shown in Figure 11. We obtain recovery and complete the recovery stage of tobacco, as shown in Figures 12 and 13, as we adjust more parameter values accordingly. Figures 12 and 13 represent periodic motion of the complete recovery stage for an addiction.
Figure 11.Time series, phase portrait, and Poincaré map of relapse stage of tobacco model (quasi-chaotic motion).
Figure 12.Time series, phase portrait, and Poincaré map of recovery stage of tobacco model (quasi-periodic motion).
Figure 13.Time series, phase portrait, and Poincaré map of complete recovery stage of the tobacco model (periodic motion).
4. Conclusions
We proposed a tobacco addiction model by rescaling parameters from the existing tobacco model and the Lorenz system. The mathematical addiction model of tobacco is organized by a third-order differential ordinary system. It is similar to the Lorenz system because it is derived from the system.
From the tobacco addiction model, we obtained periodic motion, quasi-periodic motion, quasi-chaotic motion, and chaotic motion. These motions correspond to pre-addiction or complete recovery, recovery or re-recovery, and the relapse and addiction stages, respectively.
In the future, we need to find detailed roles for each parameter in the addiction model of tobacco that we devised in order to control and treat the addiction status in humans.
참고문헌
- A. Garfinkel, M. Spano, W. Ditto, and J. Weiss, "Controlling cardiac chaos, " Science, vol. 257, no. 5074, pp. 1230-1235, Aug. 1992. http://dx.doi.org/10.1126/science.1519060
- P. Faure and H. Korn, "Is there chaos in the brain? I. Concepts of nonlinear dynamics and methods of investigation," Comptes Rendus de l'Academie des Sciences Serie III, Sciences de la vie, vol. 324, no. 9, pp. 773-793, Sep. 2001. https://doi.org/10.1016/S0764-4469(01)01377-4
- R. M. May, "Simple mathematical models with very complicated dynamics," Nature, vol. 261, no. 5560, pp. 459-467, Jun. 1976. http://dx.doi.org/10.1038/261459a0
- Y. C. Bae, "A study on chaotic phenomena in rolling mill bearing, " Journal of Korean Institute of Intelligent Systems, vol. 11, no. 4, pp. 315-319, Aug. 2001.
- Y. C. Bae, J. Kim, Y. Kim, and Y. W. Shon, "Secure communication using embedding drive synchronization," Journal of Korean Institute of Intelligent Systems, vol. 13, no. 3, pp. 310-315, Jun. 2003. https://doi.org/10.5391/JKIIS.2003.13.3.310
- Y. Bae, Y. G. Kim, and M. Tinduka, "A study on generalized synchronization in the state-controlled cellular neural network(SC-CNN)," International Journal of Fuzzy Logic and Intelligent Systems, vol. 5, no. 4, pp. 291-296, Dec. 2005. https://doi.org/10.5391/IJFIS.2005.5.4.291
- S. H. Yu, C. H. Hyun, and M. Park, "Backstepping control and synchronization for 4-D Lorenz-Stenflo chaotic system with single input," International Journal of Fuzzy Logic and Intelligent Systems, vol. 11, no. 3, pp. 143-148, Sep. 2011. http://dx.doi.org/10.5391/IJFIS.2011.11.3.143
- S. H. Yu, C. H. Hyun, and M. Park, "Control and synchronization of new hyperchaotic system using active backstepping design," International Journal of Fuzzy Logic and Intelligent Systems, vol. 11, no. 2, pp. 77-83, Jun. 2011. http://dx.doi.org/10.5391/IJFIS.2011.11.2.077
- Y. C. Bae, "Synchronization of dynamical happiness model," International Journal of Fuzzy Logic and Intelligent Systems, vol. 14, no. 2, pp. 91-97, Jun. 2014. http://dx.doi.org/10.5391/IJFIS.2014.14.2.91
- Y. C. Bae, Y. Kim, and Y. Koo, "The target searching method in the chaotic mobile robot embedding BVP model," Journal of Korean Institute of Intelligent Systems, vol. 17, no. 2, pp. 259-264, Apr. 2007. https://doi.org/10.5391/JKIIS.2007.17.2.259
- Y. C. Bae, "Chaotic phenomena in MEMS with duffing equation," The Journal of the Korea Institute of Electronic Communication Sciences, vol. 6, no. 5, pp. 709-716, Oct. 2011.
- Y. C. Bae, Y. Kim, and C. Kim, "Obstacle avoidance method in the chaotic unmanned aerial vehicle," Journal of Korean Institute of Intelligent Systems, vol. 14, no. 7, pp. 883-888, Dec. 2004 https://doi.org/10.5391/JKIIS.2004.14.7.883
- Y. C. Bae, "Chaotic phenomena in addiction model for digital leisure," International Journal of Fuzzy Logic and Intelligent Systems, vol. 13, no. 4, pp. 291-297, Dec. 2013. http://dx.doi.org/10.5391/IJFIS.2013.13.4.291
- J. C. Sprott, "Dynamical models of happiness," Nonlinear Dynamics, Psychology, and Life Sciences, vol. 9, no. 1, pp. 23-36, Jan. 2005.
- D. Satsangi and A. K. Sinha, "Dynamics of love and happiness: a mathematical analysis," International Journal of Modern Education and Computer Science, vol. 4, no. 5, pp. 31-37, Jun. 2012. http://dx.doi.org/10.5815/ijmecs.2012.05.05
- D. Lykken and A. Tellegen, "Happiness is a stochastic phenomenon," Psychological Science, vol. 7, no. 3, pp. 186-189, May 1996. http://dx.doi.org/10.1111/j.1467-9280.1996.tb00355.x
- S.W. Kim, S. K. Choi, Y. C. Bae, and Y. H. Park, "Chaotic phenomena in MEMS with duffing equation," Journal of the Korea Institute of Electronic Communication Sciences, vol. 9, no. 6, pp. 711-717, Jun. 2014. http://dx.doi.org/10.13067/JKIECS.2014.9.6.711
- Y. C. Bae, "Diagnosis of power supply by analysis of chaotic nonlinear dynamics," Journal of the Korea Institute of Electronic Communication Sciences, vol. 8, no. 1, pp. 113-119, Jan. 2013. http://dx.doi.org/10.13067/JKIECS.2013.8.1.113
- M. M. Kim and Y. C. Bae, "Mathematical modelling and chaotic behavior analysis of cyber addiction," Journal of Korean Institute of Intelligent Systems, vol. 24, no. 3, pp. 245-250, Jun. 2014. http://dx.doi.org/10.5391/JKIIS.2014.24.3.245
- C. ROSSI, "The role of dynamic modeling in drug abuse epidemiology," Bulletin on Narcotics, vol. 54, no. 1-2, pp. 33-44, 2002.
- C. Castillo-Garsow, G. Jordn-Salivia, and A. Rodriguez-Herrera, "Mathematical models for the dynamics of tobacco use, recovery, and relapse [BU-1505-M]," Available https://mtbi.asu.edu/research/archive/paper/mathematical-models-dynamics-tobacco-use-recoveryand-relapse
피인용 문헌
- Chaotic Behavior in a Dynamic Love Model with Different External Forces vol.15, pp.4, 2015, https://doi.org/10.5391/IJFIS.2015.15.4.283
- Analysis of Nonlinear Dynamics in Family Model vol.25, pp.4, 2015, https://doi.org/10.5391/JKIIS.2015.25.4.313
- Chaotic Behavior in Model with a Gaussian Function as External Force vol.16, pp.4, 2016, https://doi.org/10.5391/IJFIS.2016.16.4.262
- Analysis of Nonlinear Dynamics in Family Model including Parent-in-Law vol.26, pp.1, 2016, https://doi.org/10.5391/JKIIS.2016.26.1.037
- Periodic Doubling and Chaotic Attractor in the Love Model with a Fourier Series Function as External Force vol.17, pp.1, 2017, https://doi.org/10.5391/IJFIS.2017.17.1.17
- Analysis of Chaotic Behavior in a Novel Extended Love Model Considering Positive and Negative External Environment vol.20, pp.5, 2018, https://doi.org/10.3390/e20050365