Pub Date : 2022-12-22DOI: 10.1016/j.exco.2022.100097
Valentino Smaldore
Minimal codes are being intensively studied in last years. -minimal linear codes are in bijection with strong blocking sets of size in and a lower bound for the size of strong blocking sets is given by . In this note we show that all strong blocking sets of length 9 in are the hyperbolic quadrics .
{"title":"All minimal [9,4]2-codes are hyperbolic quadrics","authors":"Valentino Smaldore","doi":"10.1016/j.exco.2022.100097","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100097","url":null,"abstract":"<div><p>Minimal codes are being intensively studied in last years. <span><math><msub><mrow><mrow><mo>[</mo><mi>n</mi><mo>,</mo><mi>k</mi><mo>]</mo></mrow></mrow><mrow><mi>q</mi></mrow></msub></math></span>-minimal linear codes are in bijection with strong blocking sets of size <span><math><mi>n</mi></math></span> in <span><math><mrow><mi>P</mi><mi>G</mi><mrow><mo>(</mo><mi>k</mi><mo>−</mo><mn>1</mn><mo>,</mo><mi>q</mi><mo>)</mo></mrow></mrow></math></span> and a lower bound for the size of strong blocking sets is given by <span><math><mrow><mrow><mo>(</mo><mi>k</mi><mo>−</mo><mn>1</mn><mo>)</mo></mrow><mrow><mo>(</mo><mi>q</mi><mo>+</mo><mn>1</mn><mo>)</mo></mrow><mo>≤</mo><mi>n</mi></mrow></math></span>. In this note we show that all strong blocking sets of length 9 in <span><math><mrow><mi>P</mi><mi>G</mi><mrow><mo>(</mo><mn>3</mn><mo>,</mo><mn>2</mn><mo>)</mo></mrow></mrow></math></span> are the hyperbolic quadrics <span><math><mrow><msup><mrow><mi>Q</mi></mrow><mrow><mo>+</mo></mrow></msup><mrow><mo>(</mo><mn>3</mn><mo>,</mo><mn>2</mn><mo>)</mo></mrow></mrow></math></span>.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"3 ","pages":"Article 100097"},"PeriodicalIF":0.0,"publicationDate":"2022-12-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"50203717","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-12-10DOI: 10.1016/j.exco.2022.100095
Guillermo Alesandroni
Let be a finite nonempty family of finite nonempty sets. We prove the following: (1) satisfies the condition of the title if and only if for every pair of distinct subfamilies , of , . (2) If satisfies the condition of the title, then the number of subsets of containing at least one set of is odd. We give two applications of these results, one to number theory and one to commutative algebra.
{"title":"Families of finite sets in which no set is covered by the union of the others","authors":"Guillermo Alesandroni","doi":"10.1016/j.exco.2022.100095","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100095","url":null,"abstract":"<div><p>Let <span><math><mi>ℱ</mi></math></span> be a finite nonempty family of finite nonempty sets. We prove the following: (1) <span><math><mi>ℱ</mi></math></span> satisfies the condition of the title if and only if for every pair of distinct subfamilies <span><math><mrow><mo>{</mo><msub><mrow><mi>A</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><mo>…</mo><mo>,</mo><msub><mrow><mi>A</mi></mrow><mrow><mi>r</mi></mrow></msub><mo>}</mo></mrow></math></span>, <span><math><mrow><mo>{</mo><msub><mrow><mi>B</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><mo>…</mo><mo>,</mo><msub><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>}</mo></mrow></math></span> of <span><math><mi>ℱ</mi></math></span>, <span><math><mrow><munderover><mrow><mo>⋃</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>r</mi></mrow></munderover><msub><mrow><mi>A</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>≠</mo><munderover><mrow><mo>⋃</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>s</mi></mrow></munderover><msub><mrow><mi>B</mi></mrow><mrow><mi>i</mi></mrow></msub></mrow></math></span>. (2) If <span><math><mi>ℱ</mi></math></span> satisfies the condition of the title, then the number of subsets of <span><math><mrow><munder><mrow><mo>⋃</mo></mrow><mrow><mi>A</mi><mo>∈</mo><mi>ℱ</mi></mrow></munder><mi>A</mi></mrow></math></span> containing at least one set of <span><math><mi>ℱ</mi></math></span> is odd. We give two applications of these results, one to number theory and one to commutative algebra.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"3 ","pages":"Article 100095"},"PeriodicalIF":0.0,"publicationDate":"2022-12-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"50203716","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-12-09DOI: 10.1016/j.exco.2022.100093
P. Priyadharshini, M. Vanitha Archana
An incompressible MHD nanofluid boundary layer flow over a vertical stretching permeable surface employing Buongiorno’s design investigated by considering the convective states. The Brownian motion and thermophoresis effects are used to implement the nanofluid model. Operating the similarity transmutations, to transform the governing partial differential equations into ordinary differential equations consisting of the momentum, energy, and concentration fields and later worked by using a program written together with the stiffness shifting in Wolfram Language. The consequences of various physical parameters on the velocity, temperature, and concentration fields are analyzed, such as magnetic parameter , Brownian motion parameter , thermophoresis parameter , Lewis number , temperature Biot number , concentration Biot number , and suction parameter . Furthermore, the Skin friction coefficient, local Nusselt, and local Sherwood numbers concerning magnetic parameter for various values of physical parameters (i.e. , ) are obtained graphically, then the outcome is validated with other recent works. Finally, introduced a new environment to employ machine learning by performing the sensitivity analysis based on the iterative method for predicting the Skin friction coefficient, reduced Nusselt number, and Sherwood number with respect to magnetic parameter for suction parameter and Brownian motion parameter. Machine learning algorithms provide a strong and quick data processing structure to enhance the actual research procedures and industrial application of fluid mechanics. These techniques have been upgraded and organized for fluid flow characteristics. The present optimization process has the potential for a new perspective on the metallurgical process, heat exchangers in electronics, and some medicinal applications.
{"title":"Augmentation of magnetohydrodynamic nanofluid flow through a permeable stretching sheet employing Machine learning algorithm","authors":"P. Priyadharshini, M. Vanitha Archana","doi":"10.1016/j.exco.2022.100093","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100093","url":null,"abstract":"<div><p>An incompressible MHD nanofluid boundary layer flow over a vertical stretching permeable surface employing Buongiorno’s design investigated by considering the convective states. The Brownian motion and thermophoresis effects are used to implement the nanofluid model. Operating the similarity transmutations, to transform the governing partial differential equations into ordinary differential equations consisting of the momentum, energy, and concentration fields and later worked by using a program written together with the stiffness shifting in Wolfram Language. The consequences of various physical parameters on the velocity, temperature, and concentration fields are analyzed, such as magnetic parameter <span><math><mi>M</mi></math></span>, Brownian motion parameter <span><math><mrow><mi>N</mi><mi>b</mi></mrow></math></span>, thermophoresis parameter <span><math><mrow><mi>N</mi><mi>t</mi></mrow></math></span>, Lewis number <span><math><mrow><mi>L</mi><mi>e</mi></mrow></math></span>, temperature Biot number <span><math><mrow><mi>B</mi><msub><mrow><mi>i</mi></mrow><mrow><mi>θ</mi></mrow></msub></mrow></math></span>, concentration Biot number <span><math><mrow><mi>B</mi><msub><mrow><mi>i</mi></mrow><mrow><mi>ϕ</mi></mrow></msub></mrow></math></span>, and suction parameter <span><math><msub><mrow><mi>f</mi></mrow><mrow><mi>w</mi></mrow></msub></math></span>. Furthermore, the Skin friction coefficient, local Nusselt, and local Sherwood numbers concerning magnetic parameter for various values of physical parameters (i.e. <span><math><msub><mrow><mi>f</mi></mrow><mrow><mi>w</mi></mrow></msub></math></span>, <span><math><mrow><mi>N</mi><mi>b</mi></mrow></math></span>) are obtained graphically, then the outcome is validated with other recent works. Finally, introduced a new environment to employ machine learning by performing the sensitivity analysis based on the iterative method for predicting the Skin friction coefficient, reduced Nusselt number, and Sherwood number with respect to magnetic parameter for suction parameter and Brownian motion parameter. Machine learning algorithms provide a strong and quick data processing structure to enhance the actual research procedures and industrial application of fluid mechanics. These techniques have been upgraded and organized for fluid flow characteristics. The present optimization process has the potential for a new perspective on the metallurgical process, heat exchangers in electronics, and some medicinal applications.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"3 ","pages":"Article 100093"},"PeriodicalIF":0.0,"publicationDate":"2022-12-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"50203719","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-12-07DOI: 10.1016/j.exco.2022.100094
Shyam Saurabh , Kishore Sinha
Some series of Group divisible designs using generalized Bhaskar Rao designs over Dihedral, Symmetric and Alternating groups are obtained.
利用二面体群、对称群和交替群上的广义Bhaskar-Rao设计,得到了一系列群可分设计。
{"title":"Algebraic constructions of group divisible designs","authors":"Shyam Saurabh , Kishore Sinha","doi":"10.1016/j.exco.2022.100094","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100094","url":null,"abstract":"<div><p>Some series of Group divisible designs using generalized Bhaskar Rao designs over Dihedral, Symmetric and Alternating groups are obtained.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"3 ","pages":"Article 100094"},"PeriodicalIF":0.0,"publicationDate":"2022-12-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"50203720","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100059
Claude Klöckl, Katharina Gruber, Peter Regner, Sebastian Wehrle, Johannes Schmidt
Rinne et al. (2018) conduct a detailed analysis of the impact of wind turbine technology and land-use on wind power potentials, which allows important insights into each factor’s contribution to overall potentials. The paper presents a detailed and very valuable model of site-specific wind turbine investment cost (i.e. road- and grid access costs), complemented by a model used to estimate site-independent costs.
However, the site-independent cost model is flawed in our opinion. This flaw most likely does not impact the results on cost supply-curves of wind power presented in the paper. However, we expect a considerable generalization error. Thus the application of the wind turbine cost model in other contexts may lead to unreasonable results. More generally, the derivation of the wind turbine cost model serves as an example of how applications of automated regression analysis can go wrong.
{"title":"The perils of automated fitting of datasets: The case of a wind turbine cost model","authors":"Claude Klöckl, Katharina Gruber, Peter Regner, Sebastian Wehrle, Johannes Schmidt","doi":"10.1016/j.exco.2022.100059","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100059","url":null,"abstract":"<div><p>Rinne et al. (2018) conduct a detailed analysis of the impact of wind turbine technology and land-use on wind power potentials, which allows important insights into each factor’s contribution to overall potentials. The paper presents a detailed and very valuable model of site-specific wind turbine investment cost (i.e. road- and grid access costs), complemented by a model used to estimate site-independent costs.</p><p>However, the site-independent cost model is flawed in our opinion. This flaw most likely does not impact the results on cost supply-curves of wind power presented in the paper. However, we expect a considerable generalization error. Thus the application of the wind turbine cost model in other contexts may lead to unreasonable results. More generally, the derivation of the wind turbine cost model serves as an example of how applications of automated regression analysis can go wrong.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100059"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000064/pdfft?md5=fdac94d105872fd1eb33da6ecfceea1a&pid=1-s2.0-S2666657X22000064-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828286","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100088
Navnit Jha
A high-resolution compact discretization scheme for the numerical approximation of two-point nonlinear fractal boundary value problems is presented to study the stationary anomalous diffusion process. Hausdorff derivative is applied to derive the models in fractal media. The proposed scheme solves the nonlinear fractal model and achieves an accuracy of order four by employing only three mesh points in a stencil and consumes short computing time. Numerical simulations with heat conduction in polar bear, convection–diffusion, boundary layer, Bessel’s and Burgers equation in a fractal medium are carried out to illustrate the utility of the scheme and their numerical rate of convergence.
{"title":"Numerical treatment of fractal boundary value problems for heat conduction in polar bear with spatial variation of thermal conductivity","authors":"Navnit Jha","doi":"10.1016/j.exco.2022.100088","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100088","url":null,"abstract":"<div><p>A high-resolution compact discretization scheme for the numerical approximation of two-point nonlinear fractal boundary value problems is presented to study the stationary anomalous diffusion process. Hausdorff derivative is applied to derive the models in fractal media. The proposed scheme solves the nonlinear fractal model and achieves an accuracy of order four by employing only three mesh points in a stencil and consumes short computing time. Numerical simulations with heat conduction in polar bear, convection–diffusion, boundary layer, Bessel’s and Burgers equation in a fractal medium are carried out to illustrate the utility of the scheme and their numerical rate of convergence.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100088"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000210/pdfft?md5=072080d010ecc5a7c70a88203588807f&pid=1-s2.0-S2666657X22000210-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828825","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100087
Fleurianne Bertrand , Maximilian Brodbeck , Tim Ricken
Finite element approximations of poroelastic materials are nowadays used within multiple applications. Due to wide variation of possible material parameters, robustness of the considered discretization is important. Within this contribution robust of discretization schemes, initially developed for Biot’s theory, will be applied within the Theory of Porous Media. Selected numerical test-cases, special attention will be paid to incompressible and impermeable regimes, are conducted.
{"title":"On robust discretization methods for poroelastic problems: Numerical examples and counter-examples","authors":"Fleurianne Bertrand , Maximilian Brodbeck , Tim Ricken","doi":"10.1016/j.exco.2022.100087","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100087","url":null,"abstract":"<div><p>Finite element approximations of poroelastic materials are nowadays used within multiple applications. Due to wide variation of possible material parameters, robustness of the considered discretization is important. Within this contribution robust of discretization schemes, initially developed for Biot’s theory, will be applied within the Theory of Porous Media. Selected numerical test-cases, special attention will be paid to incompressible and impermeable regimes, are conducted.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100087"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000209/pdfft?md5=34ba4d9728edf7f37992d4a62b749171&pid=1-s2.0-S2666657X22000209-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828819","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100090
Haresh P. Jani, Twinkle R. Singh
In this work, we solve partial differential equations using the Aboodh transform and the homotopy perturbation method (HPM). The Swift–Hohenberg equation accurately describes pattern development and evolution. The Swift–Hohenberg (S–H) model is linked to fluid dynamics, temperature, and thermal convection, and it can be used to describe how liquid surfaces with a horizontally well-conducting boundary form.
{"title":"Some examples of Swift–Hohenberg equation","authors":"Haresh P. Jani, Twinkle R. Singh","doi":"10.1016/j.exco.2022.100090","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100090","url":null,"abstract":"<div><p>In this work, we solve partial differential equations using the Aboodh transform and the homotopy perturbation method (HPM). The Swift–Hohenberg equation accurately describes pattern development and evolution. The Swift–Hohenberg (S–H) model is linked to fluid dynamics, temperature, and thermal convection, and it can be used to describe how liquid surfaces with a horizontally well-conducting boundary form.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100090"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000234/pdfft?md5=858850a7e53372b937f273f5a13392f6&pid=1-s2.0-S2666657X22000234-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828824","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100085
Alexander Yakovlevich Braginsky
The paper researches wind gusts that are caused by changes in pressure on a flat surface. To describe this phenomenon the equations of the state of a continuous medium are used. In the stationary case, these equations in the air are the equation of the decreasing exponent for the pressure gradient. Consequently, the volume force in the air cannot act permanently. It decreases at a distance of about a kilometer. This exponential damping solution is due to wind gusts. The paper concludes that the periodic dumping of volumetric forces leads to turbulence in the air. These disruptions or turbulence are also observed when the air rotates in cyclones and anticyclones. In the water, pressure fluctuation leads to periodic waves.
{"title":"Explanation of wind gusts induced by pressure changes. Turbulence in the air","authors":"Alexander Yakovlevich Braginsky","doi":"10.1016/j.exco.2022.100085","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100085","url":null,"abstract":"<div><p>The paper researches wind gusts that are caused by changes in pressure on a flat surface. To describe this phenomenon the equations of the state of a continuous medium are used. In the stationary case, these equations in the air are the equation of the decreasing exponent for the pressure gradient. Consequently, the volume force in the air cannot act permanently. It decreases at a distance of about a kilometer. This exponential damping solution is due to wind gusts. The paper concludes that the periodic dumping of volumetric forces leads to turbulence in the air. These disruptions or turbulence are also observed when the air rotates in cyclones and anticyclones. In the water, pressure fluctuation leads to periodic waves.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100085"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000192/pdfft?md5=e690703acae3c1787b38de1124d98d7b&pid=1-s2.0-S2666657X22000192-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828827","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2022-11-01DOI: 10.1016/j.exco.2022.100081
M.H.M. Moussa, Zidan M. Abd Al-Halim
Herein, the Painlevé analysis and Bäcklund transformation for the (3+1) dimensional Burger equation are presented. Using this analysis, it is shown that the equation under consideration non-integrable. But, it is under a constraint equation may be integrable. We construct the Bäcklund transformation for that equation. Similarity solutions for the mentioned equation have been obtained. Some of these solutions are completely new.
{"title":"Painlevé analysis, Bäcklund transformation and Exact solutions for the (3+1)-dimensional nonlinear partial differential equation represented by Burgers’ equation","authors":"M.H.M. Moussa, Zidan M. Abd Al-Halim","doi":"10.1016/j.exco.2022.100081","DOIUrl":"https://doi.org/10.1016/j.exco.2022.100081","url":null,"abstract":"<div><p>Herein, the Painlevé analysis and Bäcklund transformation for the (3+1) dimensional Burger equation are presented. Using this analysis, it is shown that the equation under consideration non-integrable. But, it is under a constraint equation may be integrable. We construct the Bäcklund transformation for that equation. Similarity solutions for the mentioned equation have been obtained. Some of these solutions are completely new.</p></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"2 ","pages":"Article 100081"},"PeriodicalIF":0.0,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666657X22000179/pdfft?md5=007e91f8e4bfa868782a7c5be15704e5&pid=1-s2.0-S2666657X22000179-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"71828828","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}