We provide a note on continuous-stage Runge-Kutta methods (csRK) for solving initial value problems of first-order ordinary differential equations. Such methods, as an interesting and creative extension of traditional...
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In this paper, we will develop new mathematical tools for mapping tissue microstructural properties via the use of space-time fractional calculus methods. We propose the following two new computational multi-term time...
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ISBN:
(数字)9781728134031
ISBN:
(纸本)9781728134048
In this paper, we will develop new mathematical tools for mapping tissue microstructural properties via the use of space-time fractional calculus methods. We propose the following two new computational multi-term time-space fractional diffusion models in three dimensions, which can be used to simulate multi-term time-space fractional Bloch-Torrey models in three dimensions: Model I: Finite element method for the multi-term time-space fractional diffusion model with Riesz fractional operator; Model II: Finite difference method for the multi-term time-space fractional diffusion equation with fractional Laplacian operator. Firstly, the three-dimensional multi-term time-space fractional Bloch-Torrey models are decoupled; the problem is then equivalent to solving the three-dimensional time-space fractional diffusion equations (Model I and Model II). Secondly, we propose the finite element method for Model I and finite difference method for Model II, respectively. These methods can be directly used to simulate three-dimensional multi-term time-space fractional Bloch-Torrey models. Finally, some numerical examples are given to demonstrate the versatility and application of the models.
In this paper, we study symmetric integrators for solving second-order ordinary differential equations on the basis of the notion of continuous-stage Runge-Kutta-Nyström methods. The construction of such methods ...
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This work presents the new exact solutions of nonlinear partial differential equations (PDEs). The solutions are acquired by using an effectual approach, the first integral method (FIM). The suggested technique is imp...
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Let F2m be a finite field of 2m elements, and R = F2m[u]/huki = 2m + u2m + . . . + uk-1F2m (uk = 0) where k is an integer satisfying k ≥ 2. For any odd positive integer n, an explicit representation for every self-du...
In this paper, we introduce two types of variational integrators, one originating from the discrete Hamilton’s principle while the other from Galerkin variational approach. It turns out that these variational integra...
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We develop Chebyshev symplectic methods based on Chebyshev orthogonal polynomials of the first and second kind separately in this paper. Such type of symplectic methods can be conveniently constructed with the newly-b...
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Many practical problems can be described by second-order system q¨ = −M∇U(q), in which people give special emphasis to some invariants with explicit physical meaning, such as energy, momentum, angular momentum, e...
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In this paper, we present continuous-stage partitioned Runge-Kutta (csPRK) methods for energy-preserving integration of Hamiltonian systems. A sufficient condition for the energy preservation of the csPRK methods is d...
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We develop continuous-stage Runge-Kutta-Nyström (csRKN) methods in this paper. By leading weight function into the formalism of csRKN methods and modifying the original pattern of continuous-stage methods, we est...
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