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Time-fractional diffusion with mass absorption under harmonic impact

  • Yuriy Povstenko EMAIL logo and Tamara Kyrylych
Published/Copyright: March 13, 2018

Abstract

Time-fractional diffusion equation with mass absorption and the harmonic source term is studied under zero initial conditions. The Caputo derivative of the order 0 < α ≤ 2 is used. Different formulation of the problem for integer values α = 1 and α = 2 are discussed. The integral transform technique is used. The results of numerical calculations are illustrated graphically.

References

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Appendix A

The inverse Laplace transforms (A.1)(A.4) are taken from [7], and Eqs. (A.5)(A.6) from [23]:

L11s+ps+q=eqteptpq.(A.1)
L11s2+p2s+q=1p2+q2eqtcospt+qpsinpt.(A.2)
L1expqs2+p2s2+p2=J0pt2q2,t>q>0,0,q>t>0,(A.3)

where J0(r) is the Bessel function of the first kind.

L1expqs2p2s2p2=I0pt2q2,t>q>0,0,q>t>0.(A.4)

Here I0(r) is the modified Bessel function of the first kind.

L1sμνsμ+p=tν1Eμ,νptμ,(A.5)

where Eμ, ν(z) is the Mittag-Leffler function in two parameters μ and ν:

Eμ,νz=k=0zkΓμk+ν,μ>0,ν>0,zC.(A.6)

Appendix B

The following integrals are taken from [7] and [30]:

01x2+p2cosqxdx=π2pepq,Rep>0,q>0.(B.1)
01x2p2cosqxdx=π2psinpq,p>0,q>0.(B.2)

The integral (B.2) is understood in the sense of Cauchy principal value.

0ea2x2x2+p2cosqxdx=π4pea2p2[epqerfcapq2a+epqerfcap+q2a],Rea>0,Rep>0,q>0,(B.3)

where erfc (z) is the complementary error function.

0epx2cosqxdx=π2pexpq24p,Rep>0,q>0.(B.4)
0cosax2+y2x2+p2cosqxdx=π2pepqcosay2p2,p>0,y>0,q>a>0.(B.5)
0sinax2+y2x2+p2x2+y2cosqxdx=π2pepqsinay2p2y2p2,p>0,y>0,q>a>0.(B.6)
Received: 2017-10-7
Published Online: 2018-3-13
Published in Print: 2018-2-23

© 2018 Diogenes Co., Sofia

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