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Nonlinear method of angular boundary functions for singularly perturbed parabolic problems with cubic nonlinearities

https://doi.org/10.22405/2226-8383-2024-25-1-26-41

Abstract

In the rectangle Ω = {(𝑥, 𝑡) | 0 < 𝑥 < 1, 0 < 𝑡 < 𝑇} we consider an initial-boundary value problem for a singularly perturbed parabolic equation

$$
\varepsilon^2\left(a^2\frac{\partial^2 u}{\partial x^2}-\frac{\partial u}{\partial t}\right)=F(u,x,t,\varepsilon),   \quad  (x,t)\in \Omega,
$$
$$
u(x,0,\varepsilon)=\varphi(x),    \quad 0\le x\le 1,
$$
$$
u(0,t,\varepsilon)=\psi_1(t), \quad u(1,t,\varepsilon)=\psi_2(t), \quad 0\le t\le T.
$$

Research is carried out under the assumption that at the corner points (𝑘, 0) of the rectangle Ω, where 𝑘 = 0 or 1, the function 𝐹(𝑢) = 𝐹(𝑢, 𝑘, 0, 0) is cubic and has the form

$$
F(u)=(u-\alpha(k))(u-\beta(k))(u-\bar u_0(k)), \quad\mbox{где}\quad  \alpha(k)\leq\beta(k)<\bar u_0(k).
$$

The nonlinear method of angular boundary functions is used, which combines the (linear) method of angular boundary functions, the method of upper and lower solutions (barriers), and the method of differential inequalities. Under the condition 𝜙(𝑘) > ¯𝑢0(𝑘), a complete asymptotic expansion of the solution for 𝜀 → 0 is constructed and its uniformity in a closed rectangle is substantiated.
Previously, the following cases of cubic nonlinearities were considered:

$$
F(u)=u^3-\bar u^3_0, \quad\mbox{where}\quad \bar u_0=\bar u_0(k)>0,
$$ 

under the assumption that the boundary value 𝜙(𝑘) > ¯𝑢0(𝑘), as well as the case

$$
F(u)=u^3-\bar u^3_0, \quad\mbox{where}\quad \bar u_0=\bar u_0(k)< 0,
$$

under the assumption that the boundary value 𝜙(𝑘) is contained in the interval 

$$
\bar u_0<\varphi(k)<\frac{\bar u_0}{2}< 0.
$$

About the Authors

Alexey Igorevich Denisov
postgraduate student
Russian Federation

Tula State Lev Tolstoy Pedagogical University



Igor Vasil’evich Denisov
Tula State Lev Tolstoy Pedagogical University
Russian Federation

doctor of physical and mathematical sciences, professor



References

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8. Denisov, I. V. 2018, “Corner Boundary Layer in Boundary Value Problems for Singularly Perturbed Parabolic Equations with Monotonic Nonlinearity”, Computational Mathematics and Mathematical Physics, vol. 58, no. 4, pp. 562-571.

9. Denisov, I. V. 2009, “On some classes of functions”, Chebyshevskii Sbornik, vol. X, no. 2 (30). - Tula: Publishing house Tul. state ped. un-ta them. L. N. Tolstoy, pp. 79-108.

10. Denisov, A. I., Denisov, I. V. 2019, “Corner Boundary Layer in Boundary Value Problems for Singularly Perturbed Parabolic Equations with Nonlinearities”, Computational Mathematics and Mathematical Physics, vol. 59, no. 1, pp. 96-111.

11. Denisov, A. I., Denisov, I. V. 2019, “Corner Boundary Layer in Boundary Value Problems for Singularly Perturbed Parabolic Equations with Nonmonotonic Nonlinearities”, Computational Mathematics and Mathematical Physics, vol. 59, no. 9, pp. 1518–1527.

12. Denisov, I. V. 2021, “Corner Boundary Layer in Boundary Value Problems for Singularly Perturbed Parabolic Equations with Cubic Nonlinearities”, Computational Mathematics and Mathematical Physics, vol. 61, no. 2, pp. 242–253.

13. Denisov, I. V. 2021, “Corner Boundary Layer in Boundary Value Problems with Nonlinearities Having Stationary Points”, Computational Mathematics and Mathematical Physics, vol. 61, no. 11, pp. 1855-1863.

14. Denisov, A. I., Denisov, I. V. 2020, “Mathematical models of combustion processes”, Itogi Nauki i Tekhniki. Sovremennaya Matematika i Ee Prilozheniya. Tematicheskie Obzory, vol. 185. VINITI RAN, Moscow, pp. 82–88.

15. Denisov, A. I., Denisov, I.V. 2023, “Nonlinear method of angular boundary functions in problems with cubic nonlinearities”, Chebyshevskii Sbornik, vol. XXIV, no. 1 (88). - Tula: Publishing house Tul. state ped. un-ta them. L. N. Tolstoy, pp. 27-39.


Review

For citations:


Denisov A.I., Denisov I.V. Nonlinear method of angular boundary functions for singularly perturbed parabolic problems with cubic nonlinearities. Chebyshevskii Sbornik. 2024;25(1):26-41. (In Russ.) https://doi.org/10.22405/2226-8383-2024-25-1-26-41

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