HZ Mawa, S. M. Rayhanul Islam, Md. Habibul Bashar, Md. Mamunur Roshid, Jahedul Islam, Sadia Akhter
{"title":"数学物理中BA模型和(3 + 1)维KP方程的高级展开格式的孤子解","authors":"HZ Mawa, S. M. Rayhanul Islam, Md. Habibul Bashar, Md. Mamunur Roshid, Jahedul Islam, Sadia Akhter","doi":"10.1155/2023/5564509","DOIUrl":null,"url":null,"abstract":"In this manuscript, the primary motivation is the implementation of the advanced <span><svg height=\"13.1353pt\" style=\"vertical-align:-3.429399pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.7059 57.5794 13.1353\" width=\"57.5794pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-102\"></use></g><g transform=\"matrix(.013,0,0,-0.013,5.525,0)\"><use xlink:href=\"#g190-121\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.661,0)\"><use xlink:href=\"#g190-113\"></use></g><g transform=\"matrix(.013,0,0,-0.013,18.542,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,23.04,0)\"><use xlink:href=\"#g117-33\"></use></g><g transform=\"matrix(.013,0,0,-0.013,30.671,0)\"><use xlink:href=\"#g113-243\"></use></g><g transform=\"matrix(.013,0,0,-0.013,38.018,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,42.516,0)\"><use xlink:href=\"#g113-236\"></use></g><g transform=\"matrix(.013,0,0,-0.013,48.341,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,52.839,0)\"><use xlink:href=\"#g113-42\"></use></g></svg>-</span>expansion method to construct the soliton solution, which contains some controlling parameters of two distinct equations via the Biswas–Arshed model and the (3 + 1)-dimensional Kadomtsev–Petviashvili equation. Here, the solutions’ behaviors are presented graphically under some conditions on those parameters. The height of the wave, wave direction, and angle of the obtained wave is formed by substituting the particular values of the considerations over showing figures with the control plot. With the collaboration of the advanced <span><svg height=\"13.1353pt\" style=\"vertical-align:-3.429399pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.7059 57.5794 13.1353\" width=\"57.5794pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-102\"></use></g><g transform=\"matrix(.013,0,0,-0.013,5.525,0)\"><use xlink:href=\"#g190-121\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.661,0)\"><use xlink:href=\"#g190-113\"></use></g><g transform=\"matrix(.013,0,0,-0.013,18.542,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,23.04,0)\"><use xlink:href=\"#g117-33\"></use></g><g transform=\"matrix(.013,0,0,-0.013,30.671,0)\"><use xlink:href=\"#g113-243\"></use></g><g transform=\"matrix(.013,0,0,-0.013,38.018,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,42.516,0)\"><use xlink:href=\"#g113-236\"></use></g><g transform=\"matrix(.013,0,0,-0.013,48.341,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,52.839,0)\"><use xlink:href=\"#g113-42\"></use></g></svg>-</span>expansion method, we construct entirely the solitary wave results as well as rogue type soliton, combined singular soliton, kink, singular kink, bright and dark soliton, periodic shape, double periodic shape soliton, etc. Therefore, it is remarkable to perceive that the advanced <span><svg height=\"13.1353pt\" style=\"vertical-align:-3.429399pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.7059 57.5794 13.1353\" width=\"57.5794pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g190-102\"></use></g><g transform=\"matrix(.013,0,0,-0.013,5.525,0)\"><use xlink:href=\"#g190-121\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.661,0)\"><use xlink:href=\"#g190-113\"></use></g><g transform=\"matrix(.013,0,0,-0.013,18.542,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,23.04,0)\"><use xlink:href=\"#g117-33\"></use></g><g transform=\"matrix(.013,0,0,-0.013,30.671,0)\"><use xlink:href=\"#g113-243\"></use></g><g transform=\"matrix(.013,0,0,-0.013,38.018,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,42.516,0)\"><use xlink:href=\"#g113-236\"></use></g><g transform=\"matrix(.013,0,0,-0.013,48.341,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,52.839,0)\"><use xlink:href=\"#g113-42\"></use></g></svg>-</span>expansion technique is a simple, viable, and numerical solid apparatus for clarifying careful outcomes to the other nonstraight equivalences.","PeriodicalId":18319,"journal":{"name":"Mathematical Problems in Engineering","volume":"22 2","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Soliton Solutions to the BA Model and (3 + 1)-Dimensional KP Equation Using Advanced -Expansion Scheme in Mathematical Physics\",\"authors\":\"HZ Mawa, S. 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Mamunur Roshid, Jahedul Islam, Sadia Akhter\",\"doi\":\"10.1155/2023/5564509\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this manuscript, the primary motivation is the implementation of the advanced <span><svg height=\\\"13.1353pt\\\" style=\\\"vertical-align:-3.429399pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.7059 57.5794 13.1353\\\" width=\\\"57.5794pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-102\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,5.525,0)\\\"><use xlink:href=\\\"#g190-121\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,11.661,0)\\\"><use xlink:href=\\\"#g190-113\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,18.542,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,23.04,0)\\\"><use xlink:href=\\\"#g117-33\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,30.671,0)\\\"><use xlink:href=\\\"#g113-243\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,38.018,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,42.516,0)\\\"><use xlink:href=\\\"#g113-236\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,48.341,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,52.839,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g></svg>-</span>expansion method to construct the soliton solution, which contains some controlling parameters of two distinct equations via the Biswas–Arshed model and the (3 + 1)-dimensional Kadomtsev–Petviashvili equation. Here, the solutions’ behaviors are presented graphically under some conditions on those parameters. The height of the wave, wave direction, and angle of the obtained wave is formed by substituting the particular values of the considerations over showing figures with the control plot. With the collaboration of the advanced <span><svg height=\\\"13.1353pt\\\" style=\\\"vertical-align:-3.429399pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.7059 57.5794 13.1353\\\" width=\\\"57.5794pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-102\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,5.525,0)\\\"><use xlink:href=\\\"#g190-121\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,11.661,0)\\\"><use xlink:href=\\\"#g190-113\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,18.542,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,23.04,0)\\\"><use xlink:href=\\\"#g117-33\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,30.671,0)\\\"><use xlink:href=\\\"#g113-243\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,38.018,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,42.516,0)\\\"><use xlink:href=\\\"#g113-236\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,48.341,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,52.839,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g></svg>-</span>expansion method, we construct entirely the solitary wave results as well as rogue type soliton, combined singular soliton, kink, singular kink, bright and dark soliton, periodic shape, double periodic shape soliton, etc. Therefore, it is remarkable to perceive that the advanced <span><svg height=\\\"13.1353pt\\\" style=\\\"vertical-align:-3.429399pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -9.7059 57.5794 13.1353\\\" width=\\\"57.5794pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g190-102\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,5.525,0)\\\"><use xlink:href=\\\"#g190-121\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,11.661,0)\\\"><use xlink:href=\\\"#g190-113\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,18.542,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,23.04,0)\\\"><use xlink:href=\\\"#g117-33\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,30.671,0)\\\"><use xlink:href=\\\"#g113-243\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,38.018,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,42.516,0)\\\"><use xlink:href=\\\"#g113-236\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,48.341,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,52.839,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g></svg>-</span>expansion technique is a simple, viable, and numerical solid apparatus for clarifying careful outcomes to the other nonstraight equivalences.\",\"PeriodicalId\":18319,\"journal\":{\"name\":\"Mathematical Problems in Engineering\",\"volume\":\"22 2\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-11-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Mathematical Problems in Engineering\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://doi.org/10.1155/2023/5564509\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Mathematics\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Mathematical Problems in Engineering","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1155/2023/5564509","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Mathematics","Score":null,"Total":0}
Soliton Solutions to the BA Model and (3 + 1)-Dimensional KP Equation Using Advanced -Expansion Scheme in Mathematical Physics
In this manuscript, the primary motivation is the implementation of the advanced -expansion method to construct the soliton solution, which contains some controlling parameters of two distinct equations via the Biswas–Arshed model and the (3 + 1)-dimensional Kadomtsev–Petviashvili equation. Here, the solutions’ behaviors are presented graphically under some conditions on those parameters. The height of the wave, wave direction, and angle of the obtained wave is formed by substituting the particular values of the considerations over showing figures with the control plot. With the collaboration of the advanced -expansion method, we construct entirely the solitary wave results as well as rogue type soliton, combined singular soliton, kink, singular kink, bright and dark soliton, periodic shape, double periodic shape soliton, etc. Therefore, it is remarkable to perceive that the advanced -expansion technique is a simple, viable, and numerical solid apparatus for clarifying careful outcomes to the other nonstraight equivalences.
期刊介绍:
Mathematical Problems in Engineering is a broad-based journal which publishes articles of interest in all engineering disciplines. Mathematical Problems in Engineering publishes results of rigorous engineering research carried out using mathematical tools. Contributions containing formulations or results related to applications are also encouraged. The primary aim of Mathematical Problems in Engineering is rapid publication and dissemination of important mathematical work which has relevance to engineering. All areas of engineering are within the scope of the journal. In particular, aerospace engineering, bioengineering, chemical engineering, computer engineering, electrical engineering, industrial engineering and manufacturing systems, and mechanical engineering are of interest. Mathematical work of interest includes, but is not limited to, ordinary and partial differential equations, stochastic processes, calculus of variations, and nonlinear analysis.