A Fourier analysis of the linear and quadratic N + 1 and N + 2 Petrov-Gaterkin finite element methods applied to the one-dimensional transient convective-diffusion equation is performed. The results show that a priori optimization of the N + 1 method is not possible because dissipative errors are introduced as dispersive errors are reduced (any optimization is subjective). However, a priori optimization of the N + 2 Petrov-Galerkin method is possible because the reduction of dispersion errors can be accomplished without the addition of artificial dissipation. The Spectrally Weighted Average Phase Error Method (SWAPEM) for the optimization of the N + 2 Petrov-Galerkin method is introduced, in which the N + 2 weighting parameter is chosen at each time step to minimize the integral over wave number of the phase error of Fourier modes, weighted by the frequency content of the global solution at the previous time step (obtained via FFT). The method is dynamic, and general in that the dependence of the weighting parameter on the solution waveform is accounted for. Optimal values predicted by the method are in excellent agreement with those suggested by the numerical experimentation of others. Simulations of the pure convective transport of a Gaussian plume and a triangle wave are discussed to illustrate the effectiveness of the method.
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Liu, Zehui
Lu, Ming
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Lu, Ming
Li, Qing
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Li, Qing
Lv, Zhongbin
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Lv, Zhongbin
Chang, Afei
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Tech & Informat Ctr CPI Henan Co, Zhengzhou, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Chang, Afei
Pang, Kai
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
Pang, Kai
Zhao, Shujie
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State Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R ChinaState Grid Henan Elect Power Res Inst, Power Transmiss Line Galloping Prevent & Control, Zhengzhou 450052, Henan, Peoples R China
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Univ S Carolina, Dept Math, Columbia, SC 29208 USAUniv S Carolina, Dept Math, Columbia, SC 29208 USA
Wang, Hong
Yang, Danping
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E China Normal Univ, Dept Math, Shanghai 200241, Peoples R China
E China Normal Univ, Shanghai Key Lab Pure Math & Math Practice, Shanghai 200241, Peoples R ChinaUniv S Carolina, Dept Math, Columbia, SC 29208 USA
Yang, Danping
Zhu, Shengfeng
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E China Normal Univ, Dept Math, Shanghai 200241, Peoples R China
E China Normal Univ, Shanghai Key Lab Pure Math & Math Practice, Shanghai 200241, Peoples R ChinaUniv S Carolina, Dept Math, Columbia, SC 29208 USA