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Issue DateTitleAuthor(s)
2014-11-06Effect of bidirectional mechanoelectrical coupling on spontaneous oscillations and sensitivity in a model of hair cellsAmro, Rami; Neiman, Alexander
2017-12Characteristic of the equivalent impedance for an m×n RLC network with an arbitrary boundaryTan, Z Z; Zhu, H; Asad, J. H; Xu, C; Tang, H
2017Resistance formulae of a multipurpose n-step network and its application in LC networkTan, Z Z; Asad, J. H.; owaidat, M Q
2017Motion of a spherical particle in a rotating parabola using fractional lagrangian; Baleanu, D; Asad, J. H.; Alipour, M; Blaszczyk, T
2017-06The motion of a bead sliding on a wire in fractional sense; Baleanu, D; Jajarmi, A; Asad, J. H; Blaszczyk, T
2018-02Two-Point Resistance on the Centered-Triangular LatticeOwaidat, M Q; Al-Badawi, A.A; Asad, J. H; Al-Twiessi, M
2018-06New aspects of the motion of a particle in a circular cavityBaleanu, D; Asad, J. H.; Jajarmi, A
2018-09The fractional model of spring pendulum: New features within different kernelsBaleanu, D; Jajarmi, A; Asad, J. H
2019-03In this study, we consider two coupled pendulums (attached together with a spring) having the same length while the same masses are attached at their ends. After setting the system in motion we construct the classical Lagrangian, and as a result, we obtain the classical Euler-Lagrange equation. Then, we generalize the classical Lagrangian in order to derive the fractional Euler-Lagrange equation in the sense of two different fractional operators. Finally, we provide the numerical solution of the latter equation for some fractional orders and initial conditions. The method we used is based on the Euler method to discretize the convolution integral. Numerical simulations show that the proposed approach is efficient and demonstrate new aspects of the real-world phenomena.Owaidat, M Q; Asad, J. H.; Tan, Z Z
2019-03Electrical characteristics of the 2 ×n and □ × n circuit networkTan, Z; Tan, Z Z; Asad, J. H; owaidat, M Q

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