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Various moving schemes of multiple vehicle travel including following, overtaking and side-by-side movements were considered.
The method is robust and accurately identifies every dynamic axle load for all moving schemes of vehicles.
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Hence, all educators in this study had moved schemes between two and four times.
By means of the above methods (Method 1 or Method 2) for constructing self-adaptive moving mesh schemes, we can also construct self-adaptive moving mesh schemes for the coupld SP equation and the complex SP equation.
Self-adaptive moving mesh schemes have exact solutions such as multi-soliton solutions and Lax pairs, thus those schemes are integrable.
Self-adaptive moving mesh schemes consist of two semi-discrete equations in which the time is continuous and the space is discrete.
We have shown several examples of numerical computations of the short pulse type equations by using self-adaptive moving mesh schemes.
Lax pairs of self-adaptive moving mesh schemes for short pulse type equations are constructed by discretization of Lax pairs of short pulse type equations.
Integrable self-adaptive moving mesh schemes for short pulse type equations (the short pulse equation, the coupled short pulse equation, and the complex short pulse equation) are investigated.
This paper investigates solution behaviors under the strong shock interaction for moving mesh schemes based on the one-dimensional Godunov and HLLC Riemann solvers.
Lax pairs of self-adaptive moving mesh schemes for short pulse type equations are obtained by discretization of Lax pairs of short pulse type equations, thus the existence of Lax pairs guarantees the integrability of self-adaptive moving mesh schemes for short pulse type equations.
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