Research Article

Comparing Numerical Methods for Solving Time-Fractional Reaction-Diffusion Equations

Table 1

The operations of the GDTM.

Original functions Transformed functions

𝑢 ( 𝑥 , 𝑦 ) = 𝜈 ( 𝑥 , 𝑦 ) ± 𝑤 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = 𝑉 𝛼 , 𝛽 ( 𝑘 , ) ± 𝑊 𝛼 , 𝛽 ( 𝑘 , )
𝑢 ( 𝑥 , 𝑦 ) = 𝜆 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = 𝜆 𝑉 𝛼 , 𝛽 ( 𝑘 , )
𝑢 ( 𝑥 , 𝑦 ) = 𝐷 𝛼 𝑥 0 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = Γ ( 𝛼 ( 𝑘 + 1 ) + 1 ) 𝑉 Γ ( 𝛼 𝑘 + 1 ) 𝛼 , 𝛽 ( 𝑘 + 1 , ) ,   0 < 𝛼 1
𝑢 ( 𝑥 , 𝑦 ) = 𝐷 𝛽 𝑦 0 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = Γ ( 𝛽 ( + 1 ) + 1 ) 𝑉 Γ ( 𝛽 + 1 ) 𝛼 , 𝛽 ( 𝑘 , + 1 ) ,   0 < 𝛽 1
𝑢 ( 𝑥 , 𝑦 ) = 𝐷 𝛼 𝑥 0 𝐷 𝛽 𝑦 0 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = Γ ( 𝛼 ( 𝑘 + 1 ) + 1 ) Γ ( 𝛽 ( + 1 ) + 1 ) 𝑉 Γ ( 𝛼 𝑘 + 1 ) Γ ( 𝛽 + 1 ) 𝛼 , 𝛽 ( 𝑘 + 1 , + 1 ) ,   0 < 𝛼 , 𝛽 1
𝑢 ( 𝑥 , 𝑦 ) = 𝐷 𝛾 𝑥 0 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = Γ ( 𝛼 𝑘 + 𝛾 + 1 ) 𝑉 Γ ( 𝛼 𝑘 + 1 ) 𝛼 , 𝛽 𝛾 𝑘 + 𝛼 , ,   𝑚 1 < 𝛾 1
𝑢 ( 𝑥 , 𝑦 ) = 𝐷 𝛾 𝑥 0 𝐷 𝛿 𝑦 0 𝜈 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = Γ ( 𝛼 𝑘 + 𝛾 + 1 ) Γ ( 𝛽 + 𝛿 + 1 ) 𝑉 Γ ( 𝛼 𝑘 + 1 ) Γ ( 𝛽 + 1 ) 𝛼 , 𝛽 𝛾 𝑘 + 𝛼 𝛿 , + 𝛽
𝑢 ( 𝑥 , 𝑦 ) = ( 𝑥 𝑥 0 ) 𝑘 𝛼 ( 𝑥 𝑥 0 ) 𝛽 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = 𝛿 ( 𝑘 𝑛 ) 𝛿 ( 𝑚 )
𝑢 ( 𝑥 , 𝑦 ) = 𝜈 ( 𝑥 , 𝑦 ) 𝑤 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = 𝑘 𝑟 = 0 𝑠 = 0 𝑉 𝛼 , 𝛽 ( 𝑟 , 𝑠 ) 𝑊 𝛼 , 𝛽 ( 𝑘 𝑟 , 𝑠 )
𝑢 ( 𝑥 , 𝑦 ) = 𝜈 ( 𝑥 , 𝑦 ) 𝑤 ( 𝑥 , 𝑦 ) 𝑞 ( 𝑥 , 𝑦 ) 𝑈 𝛼 , 𝛽 ( 𝑘 , ) = 𝑘 𝑟 = 0 𝑘 𝑟 𝑡 = 0 𝑠 = 0 𝑠 𝑝 = 0 𝑉 𝛼 , 𝛽 ( 𝑟 , 𝑠 𝑝 ) 𝑊 𝛼 , 𝛽 ( 𝑡 , 𝑠 ) 𝑄 𝛼 , 𝛽 ( 𝑘 𝑟 𝑡 , 𝑝 )