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Hamilton's principle is employed to derive the corresponding higher order equations of motion for both nanotubes.
The higher order equations of type (1) have been studied in [11 13].
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The first order equation of Lagergren is generally expressed as follows (Lagergren 1898): frac{{{text{d}}q}}{{{text{d}}t}} = k_{1} (q_{text{e}} - q_{text{t}} ) (7 where k 1 is the rate constant of pseudo-first-order sorption (min−1).
This methodology uses the low-order equations of the Second-Moment (SM) method for the first two angular moments of the transport solution.
We consider the system of fractional-order equations of the form (1.1).
To this end a random generator for second-order equations of the type considered in this article is applied.
We investigate the existence of multiple solutions for perturbed nonlocal fourth-order equations of Kirchhoff type under Navier boundary conditions.
I will discuss related aspects of field theories with higher-derivative Lagrangians but second-order equations of motion, with a focus on the Lovelock and Horndeski classes that have found use in modifications to general relativity.
Here we have investigated the existence of multiple solutions for perturbed nonlocal fourth-order equations of Kirchhoff type under Navier boundary conditions.
where Z ( t ) ∈ R m for t ∈ R. The linear vector differential equation (3) can be written as an equivalent system of first-order equations of dimension mn.
We have given some new criteria for guaranteeing that the perturbed fourth-order equations of Kirchhoff type possess at least three weak solutions by using a variational method and some critical point theorems due to Ricceri.
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