2023
DOI: 10.1016/j.enganabound.2022.10.015
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A polygonal element differential method for solving two-dimensional transient nonlinear heat conduction problems

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Cited by 7 publications
(6 citation statements)
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“…Mutually, boundary conditions are considered to be as Eq. (3)(4)(5)(6)(7). Considering a Sobolev space () HQ  ( 0   ) with the corresponding norm of () n HQ    and desired infinity domain…”
Section: Assuming the Temperature Filed ( )mentioning
confidence: 99%
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“…Mutually, boundary conditions are considered to be as Eq. (3)(4)(5)(6)(7). Considering a Sobolev space () HQ  ( 0   ) with the corresponding norm of () n HQ    and desired infinity domain…”
Section: Assuming the Temperature Filed ( )mentioning
confidence: 99%
“…Substituting the above approximations into Eq. (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16) in the Fourier space, we have…”
Section: Assuming the Temperature Filed ( )mentioning
confidence: 99%
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“…Unlike the above numerical methods, the element differential method (EDM) [18] is a strong-form technique to solve ordinary or partial differential equations. The most important feature of the EDM is that the derived spatial derivatives can be directly substituted into the governing equation and boundary conditions to form the final system of algebraic equations [19].…”
Section: Introductionmentioning
confidence: 99%