首页> 外文期刊>Computers & mathematics with applications >Dark breather waves, dark lump waves and lump wave-soliton interactions for a (3 + 1 )-dimensional generalized Kadomtsev-Petviashvili equation in a fluid
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Dark breather waves, dark lump waves and lump wave-soliton interactions for a (3 + 1 )-dimensional generalized Kadomtsev-Petviashvili equation in a fluid

机译:黑暗的呼吸波,暗块波和肿块波孤立孤独的A(3 + 1) - 百分比广义Kadomtsev-PetviaShvili方程在流体中

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Fluids are seen in a wide range of disciplines, including mechanical, civil, chemical and biomedical engineering, geophysics, astrophysics and biology. In this paper, we investigate a (3 + 1)-dimensional generalized Kadomtsev-Petviashvili equation for the long water waves and small-amplitude surface waves with the weak nonlinearity, weak dispersion and weak perturbation in a fluid. Breather-wave, lump-wave and lump wave-soliton solutions are derived under certain conditions via the Hirota method. With h(1)h(2)(-1) 0, where h(1) and h(2) represent the coefficients of dispersion and nonlinearity, respectively, we obtain the dark breather wave and lump wave. We observe the effects of h(1), h(2), h(4), h(6) and h(8) on the dark breather wave and lump wave, where h(6) is the perturbed effect, h(4) and h(8) stand for the disturbed wave velocity effects corresponding to they and z coordinates: h(1) and h(2) influence the amplitude of the dark breather wave: h(1), h(4) and h(8) influence the distance between the adjacent valleys of the dark breather wave; h(1), h(4), h(6) and h(8) influence the location of the dark breather wave; h(2), h(4), h(6) and h 8 influence the amplitude of the dark lump wave; h(1), h(4) and h(8) influence the width of the dark lump wave; h(4), h(6) and h(8) influence the location of the dark lump wave. When h(1)h(2)(-1) 0, we present the fusion between a bright lump wave and one bright soliton as well as fission of one bright soliton. We also observe the fusion between a dark lump wave and one dark soliton as well as fission of one dark soliton with h(1)h(2)(-1) 0. (C) 2019 Elsevier Ltd. All rights reserved.
机译:在各种学科中看到流体,包括机械,民用,化学和生物医学工程,地球物理,天体物理学和生物学。在本文中,我们研究了一种(3 + 1)的长尺寸广义Kadomtsev-PetviaShvili方程,具有弱的非线性,弱分散和液体扰动弱的小水波和小幅度表面波。通过HiROTA方法在某些条件下衍生出喘息波,块波和肿块波溶胶溶液。 H(1)H(2)( - 1)<0,其中H(1)和H(2)分别代表分散和非线性的系数,我们获得了黑暗的喘气波和块波。我们观察H(1),H(2),H(4),H(4),H(6)和H(8)对黑暗的喘息波和块波的影响,其中H(6)是扰动效果,H( 4)和H(8)用于对应于它们和Z坐标的干扰波速效应:H(1)和H(2)影响暗气波的幅度:h(1),h(4)和h (8)影响深呼吸波的相邻谷之间的距离; H(1),H(4),H(6)和H(8)影响黑暗喘气波的位置; H(2),H(4),H(6)和H 8影响暗块波的幅度; H(1),H(4)和H(8)影响暗块波的宽度; H(4),H(6)和H(8)影响暗块波的位置。当H(1)H(2)( - 1)> 0时,我们介绍了亮块波和一个明亮的孤子以及一个明亮孤子的裂缝之间的融合。我们还观察到暗块波和一个黑暗孤子之间的融合以及H(1)H(2)( - 1)> 0.(c)2019年Elsevier Ltd.保留所有权利。

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