{"title":"拉普拉斯方程的合形导数与分数阶傅立叶级数解","authors":"R. Pashaei, M. Asgari, A. Pishkoo","doi":"10.21467/ias.9.1.1-7","DOIUrl":null,"url":null,"abstract":"In this paper the solution of conformable Laplace equation, \\frac{\\partial^{\\alpha}u(x,y)}{\\partial x^{\\alpha}}+ \\frac{\\partial^{\\alpha}u(x,y)}{\\partial y^{\\alpha}}=0, where 1 < α ≤ 2 has been deduced by using fractional fourier series and separation of variables method. For special cases α =2 (Laplace's equation), α=1.9, and α=1.8 conformable fractional fourier coefficients have been calculated. To calculate coefficients, integrals are of type \"conformable fractional integral\".","PeriodicalId":52800,"journal":{"name":"International Journal of Science Annals","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2019-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Conformable Derivatives in Laplace Equation and Fractional Fourier Series Solution\",\"authors\":\"R. Pashaei, M. Asgari, A. Pishkoo\",\"doi\":\"10.21467/ias.9.1.1-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this paper the solution of conformable Laplace equation, \\\\frac{\\\\partial^{\\\\alpha}u(x,y)}{\\\\partial x^{\\\\alpha}}+ \\\\frac{\\\\partial^{\\\\alpha}u(x,y)}{\\\\partial y^{\\\\alpha}}=0, where 1 < α ≤ 2 has been deduced by using fractional fourier series and separation of variables method. For special cases α =2 (Laplace's equation), α=1.9, and α=1.8 conformable fractional fourier coefficients have been calculated. To calculate coefficients, integrals are of type \\\"conformable fractional integral\\\".\",\"PeriodicalId\":52800,\"journal\":{\"name\":\"International Journal of Science Annals\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-11-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Science Annals\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21467/ias.9.1.1-7\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Science Annals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21467/ias.9.1.1-7","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Conformable Derivatives in Laplace Equation and Fractional Fourier Series Solution
In this paper the solution of conformable Laplace equation, \frac{\partial^{\alpha}u(x,y)}{\partial x^{\alpha}}+ \frac{\partial^{\alpha}u(x,y)}{\partial y^{\alpha}}=0, where 1 < α ≤ 2 has been deduced by using fractional fourier series and separation of variables method. For special cases α =2 (Laplace's equation), α=1.9, and α=1.8 conformable fractional fourier coefficients have been calculated. To calculate coefficients, integrals are of type "conformable fractional integral".