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УДК 517.9
A study on fractional order theory in thermoelastic half-space
under thermal loading
I.A. Abbas12
1 Department of Mathematics, Faculty of Science, Sohag University, Sohag, 82524, Egypt 2 Nonlinear Analysis and Applied Mathematics Research Group, Department of Mathematics, King Abdulaziz University, Jeddah, 21589, Saudi Arabia
In this study, the effect of fractional order derivative on a two-dimensional problem due to thermal shock with weak, normal and strong conductivity is established. The governing equations are taken in the context of Green and Naghdi of type III model (GNIII model) under fractional order derivative. Based on the Laplace and exponential Fourier transformations with eigenvalues approach, the analytical solutions has been obtained. For weak, normal and strong conductivity, the numerical computations for copper-like medium have been done and the results are shown numerically. The graphical results indicate that the effect of fractional order parameter has a major role on all physical quantities involved in the problem.
Keywords: eigenvalue approach, Green and Naghdi of type III model, fractional order generalized thermoelasticity
DOI 10.24411/1683-805X-2018-11008
Дробное исчисление и его применение для описания термоупругого полупространства в условиях тепловой нагрузки
I.A. Abbas1-2
1 Сохагский университет, Сохаг, 82524, Египет 2 Университет короля Абдулазиза, Джидда, 21589, Саудовская Аравия
В работе показано влияние производной дробного порядка на решение двумерной задачи о тепловой нагрузке с низкой, нормальной и высокой проводимостью. Определяющие соотношения выбраны в рамках модели Грина-Нагди типа III (GNIII) для производной дробного порядка. На основе преобразования Лапласа и экспоненциального преобразования Фурье с использованием метода собственных значений получены аналитические решения. Выполнены численные расчеты для среды со свойствами меди в случае низкой, нормальной и высокой проводимости. Показано, что параметр дробного порядка оказывает существенное влияние на расчет физических величин в задаче.
Ключевые слова: метод собственных значений, модель Грина-Нагди типа III, теория обобщенной термоупругости с производной дробного порядка
1. Introduction
Many existing models of physical processes have been modified successfully by using the fractional calculus. A series of integral theories and fractional derivatives was created in the last half of the last century. Various approaches and definitions of fractional derivatives have become the main object of numerous studies [1, 2]. Recently, to investigate the anomalous diffusion, a considerable research effort has been expended, which is characterized by the frac-
tional time equation of wave diffusion by Kimmich [3] as in the form below
pc = kl ac a, i = 1, 2, 3, (1)
where k is the diffusion conductivity, p is the mass density, c is the concentration and Ia is the fraction of Riemann-Liouville integral operator of order a. It introduced as a natural generalization ofthe well-known integral Ia f (t) repeated m times and wrote in the form of convolution type [4]
© Abbas I.A., 2018
Abbas I.A. / 0u3UHecKaM Me3OMexanuKa 21 1 (2018) 56-62
57
-J(t/(№ 0<a<2,
I af (t) = jr(a )J0V ' (2)
f (t), a = 0,
where r(a) is the Gamma function. The fractional order of weak, normal and strong heat conductivity under generalized thermoelastic theory was applied by Youssef [5] in the following form
dqt
q+To it"'
-KIa-1VT, 0 < a < 2.
(3)
By using Taylor expansion of time-fractional order, Ezzat and El-Karamany [6] proposed a new fractional order generalized thermoelasticity model, which developed by Ju-marie [7] as
q +
da
qt
-KVT, 0<a< 1.
(4)
r(a +1) dta
The fractional order study of generalized thermoelastic problems is an important branch in solid mechanics [812]. In addition, Abbas [13] studied the effects of fractional order and magnetic field in a thermoelastic medium due to moving heat source using the eigenvalue approach. Sherief and Abd El-Latief [14] studied the effect of the fractional order parameter and the variable thermal conductivity on a thermoelastic half-space. Due to thermal source, the effect of fractional order parameter on plane deformation in a thermoelastic medium was studied by Kumar et al. [15]. Abbas and Youssef [16] studied a two-dimensional thermoelastic porous material under fractional order theory. The fractional order influence in a functional graded thermoelastic material problem has been solved by Abbas [17]. Youssef and Abbas [18] studied the theory of generalized thermoelasticity with fractional order derivative in the case of variable thermal conductivity. Based upon the theory of two-temperature generalized thermoelasticity, Zenkour and Abouelregal [19] investigated the fractional heat conduction for an unbounded medium with a spherical cavity. Abbas [20] studied the solution of thermoelastic diffusion problem under fractional order theory in an infinite elastic medium with a spherical cavity.
In this work, the eigenvalue approach has been used to obtain the analytical solutions for temperature, displacement and the stress components. By employing an analytical-numerical technique based on the eigenvalues approach with Laplace and Fourier transformations, the nondimen-sional equations have been handled. Numerical computations for copper-like medium have been done for strong, normal and weak conductivity and the effect of the fractional order parameter has been estimated.
2. Basic equations
Let us consider a homogeneous, thermoelastic isotropic half-space y > 0 at initial uniform temperature T0. Cartesian coordinate system (x, y, z) has been used with y axis is taken perpendicular to the bounding plane (Fig. 1). The
displacement vector has the form u = (u, v, 0). The governing equations have the following form
^ . x d2u ^ x d2v d2u dT d2u _ (A + 2^)—+(A + ^)—- + -Y_ = p_ (5)
dx 2 d 2 v
dy
dxdy dy dx dt d2u d2v
dxdy ^ dx2
rdT dy
2
tfv dt2
(6)
T-a-1
K * + K — dt
J
d2T d2T
dt2
P ceT + YTo
dx2 + dy2
V J J
du dv
+
dx dy
(7)
J J
where the operator of fractional integral can be defined as the following [21]:
Ia f (9) =-FTtJ (a_1f (£)de,
I (a) 0
0 <a< 1 for weak conductivity, a = 1 for normal conductivity,
1 <a< 2 for strong conductivity,
a xx = (X + 2|) ^ + Xdv-Y (T - T0),
dx dy
:(X+2^) dv-Y (t - T0),
dy dx
(8)
yy
xy
du + dv dx dy
(9) (10) (11)
where X and | are the elastic parameters, T is the increment of temperature, p is the density of mass, axx, axy and ayy are the stress components, T0 is the body reference temperature, ce is the specific heat at constant strain, K is the thermal conductivity, y = (2X + 3|)at, and at is the linear thermal expansion coefficient. For convenience, the non-dimensional variables can be introduced on the following form:
c t - T
(U, v, x , y) = - (u, v, x, y), T' = 0 ,
- T0
1 C2
(a'xx > a'yy> a'xy ) =|(axx> ayy > axy X t = —t>
where c2 = (X + 2|)/p, - = K/(pce).
(12)
Fig. 1. Geometry of the problem
In terms of these nondimensional variables (12), Eqs. (5)—(11), after suppressing the primes, can be written as
P^-2 + (P-1)
ox
d v du dT „3 u -+ —2 -ra-= p—y,
dxdy dx2 dx dt
ad2v t2u d2v dT _32v
P—7 + (P-1)-+ —T-ra-= P-
dy dxdy dx dy
dt2
(13)
(14)
Ia-11 e, + —
I 1 dt
d Y 3 2T d 2T1
dx2' + 'dy2
d d2 1L ( du dv Y + xn—^ T + e.
3t 10 at2
■+ dx dy
, du )--
dx
dv d 2i,
J J
a xx = P—+ (P-2) — + —2-raT,
dy dx
ayy +(P-2) dx-raT,
a = du + dv x dy dx'
(15)
(16)
(17)
(18)
where P = (X + 2^)/ra = yT0/^, e1 = K*/(pc2ce), and e2 = Y/ (PCe).
3. Application
Now, we can assume the homogeneous initial conditions as
TV m dT(x, y, 0)
T(x, y, 0) =---= 0,
dt
u(x, y, 0) = 0,
dt
. 3v(x, y, 0)
v( x, y, 0) = v/ = 0. dt
(19)
The boundary conditions at y = 0 for the present problem are supposed as
T(x, 0, t) = TlH(a-|x|)H(t), (20)
where T is a constant, His the unit step function (Heaviside function). It is means that the thermal shock acts on a band of a width 2a centered around the x axis on the half-space surface (y = 0) and is zero elsewhere. On the boundary y = 0, we suppose that the body displacement v does not depend on y, which leads to dv(x, 0, t)
dy
- = 0.
(21)
Moreover, the medium is subjected to rigid foundation and rough enough to prevent the displacement u at any point of x and any time t, which leads to
u(x, 0, t) = 0. (22)
4. Laplace and Fourier transformations
Let us define the Laplace transformation for a function Q(x, y, t) by
Z[Q(x, y, t)] = Q(x, y, s) = J Q(x, y, t)e~stdt, (23)
0
s > 0,
where s is a parameter. Hence, the above equations will take the form:
„32u a2v a2u dT 2_
P—7 + (P-1)-+ —7 -ra— = Ps2u,
dx2 dxdy dy dx
2
,32 v
n" - /o n a2u a2 v dT 2_ PTT + (P-1)^- +TT-^ = Pi2 v,
dy2 dxdy dx2 dy
T + e2
a2t a2t sa-1 (^ tau av^
+- 2 -dx2 dy2 e + s^ v
â„ =Pdu +(P-2) ^ -raT,
ox oy
=P| +<P-2) I-raT"
+
dx dy
J J
T (x, 0, s) = dv (x, 0, s)
du dv dx
T1H (a-1 x |)
x dy dx'
(24)
(25)
(26)
(27)
(28)
(29)
(30)
dy
= 0, u (x, 0, s) = 0.
Now, the exponential Fourier transformation for the function Q(x, y, s) can be given by
Œ*(q, y, s) = J x, y, s)e lqxdx.
(31)
Hence, the above differential equations can assume the form: -q 2pu * + (P - 1)iq ^V- + ^TUT - iqraT * = ps 2- (32)
dy dy2
, d2 v*
dy2
dy
P^T- + iq(P-1)— + q2v* -ra— = Ps2v*, (33)
2 dy
2T * + d2T s a+1 ( -q T +
dy2 et + s
(
T +e,
iqu + ■
dv dy
■Y\
dv
= iqPu + (P-2)---raT ,
dy
, dv*
dy du " dy
â*yy = P—+ iq(P-2)u* -raT*,
axy = — +iqv >
T*(q,0, s) = TH 2-Sln(qa)
dv*(q, 0, s) dy
n qs
= 0, u *(q, 0, s) = 0.
(34)
(35)
(36)
(37)
(38)
By using the eigenvalue approach as made in Refs. [22, 23], let us now proceed to solve the coupled differential equations (32)—(34). In the form of vector-matrix differential equation, Eqs. (32)—(34) can be written as follows
d« = A«, dy where
and
(39)
* _* dv* du * dT * " T
v* u * T * - -
dy dy dy _
' 0 0 0 1 0 0
0 0 0 0 1 0
0 0 0 0 0 1
a41 0 0 0 a45 a46
0 a52 a53 a54 0 0
0 a62 a63 a64 0 0
A =
Thus, the matrix A has the characteristic equation in the form
- M^4 + M+ M3 = 0, (40)
where
M1 = a41 + a52 + a45a54 + a63 + a46'
M2 = a41a52 - a53a62 - a46a54a62 + a41a63 +
+ a52a63 + a45a54a63 + a46a52a64 - a45a53a64> M3 = a4ia53a62 — a4ia52a63-
The eigenvalues of matrix A are the roots of Eq. (40) in the form ±£2, ±£3. For the eigenvalue the corresponding eigenvector Y = [Y1, Y2, Y3, Y4, Y5, Y6] can be calculated as:
Y1 = -a45a54^+ a46^(a52 -
Y2 =-a46a54^2 + a53(a41 -^2)> (.,)
V — ( \p2 f.4 (41) Y3 = —a4ia52 + (a41 + a52 + a45a54— ^ ,
Y4 = \YA, Y5 =^Y2, Y6 = Y For further reference, the following notations can be used:
Y = [Y]ç=—çi, Y2 = [Y]ç=—ç2, Y3 = [Y]ç=—ç3, Y4 = [Y]ç=çi> Y5 = [Y]ç=Ç2, Y6 = [Y]|=ç3.
The solution of Eq. (39) can be given in the following form:
«(q, y, s) = E BJf^. (43)
i=1
Due to the regularity conditions of the solution, the exponential in the space variable x has been discarded at infinity. By using the problem boundary conditions, the constants B1, B2 and B3 have been calculated.
5. Double transformation inversion
The expression Q (q, y, s) in the domain of Fourier transformation can be expressed as
(42)
1
Q(q, y, s) = -= J Q*(q, y, s)eiqxdq.
V2n —J
(44)
Thus, the physical quantities can be given for x, y and s in the forms:
V(x, y, s) = _LEJ Bkvke-^y+qxdq, V2n k =1 —J
T(x, y, s) = * E J BkTke<ky+lqxdq, V2n k=1—J
1 3 j
5xx (x, y,s) = -¡= E J Bk ( m uk —
V2n k =1 —J
— iik (n —2) Vk —çTk )e~^ky+iqxdq,
1 3 J
5yy (x, y, s) = ^=E J Bk (—Iknvk —
V2n k=1 —J
— iq(n — 2) uk —çTk ) e"^ky+iqxd q,
1 3 J
5xy (x, y, s) =TÎ=E J BkKkuk +
V2n k=1—J
+ iqvk ) e"^ky+iqxdq,
(46)
(47)
(48)
(49)
(50)
T(x, y, s) = * E J Bkuke~^ky+iqxdq, V2n k =1—J
Fig. 2. Contour plots of the temperature distribution on the material for weak (a), normal (b) and strong conductivity (c) at t =0.12
where uk, vk and Tk are the components of the corresponding eigenvectors. We adopt a numerical inversion method based on the Stehfest algorithm [24]. In this method, the inverse g(x, y, t) of the Laplace transformation g(x, y, s) is approximated by the relation
ln2 * = f ln2
Q( x, y, t) =-E Vj Q
j=i
x, y,
t
-j
and V; takes the form
Vj = (-1)
(N/2+1) ,
min( i, N 2)
x E
k(N 2+1)(2k )!
(51)
(52)
k=(i+i)/2 (N/2-k)!k!(i-k)!(2k-1)! where N is the term number used in summation in Eq. (52) and should be optimized by trial and error.
6. Numerical results and discussion
In order to illustrate the theoretical results obtained in the previous section, we present some numerical values for the physical constants. We assume that the plate is made of an isotropic material (copper). The physical constants are listed below [25]:
p = 8954 kg m-3, X = 7.76 x 1010 N m
¡1 = 3.86 x 1010 N m-2, a t
1.78 x 10-5 K-1,
T0 = 293 K, ce = 383.1 J kg"1 K1. Here the graphs are plotted to display the variations of temperature, displacements and stresses for T1 = 1, a = 1 at t = 0.12. The results of the numerical evaluation of temperature distribution contours for weak, normal and strong conductivity are illustrated in Fig. 2. We can observed that the change of temperature area is limited within a finite area and the temperature does not change outside that area. In addition, we can find that the heat influence zone with weak conductivity gets greater than the heat influence area with normal conductivity which it is greater than the heat influence area with strong conductivity. Also, there are areas with a greater slope of the temperature of another zone. This means that heat conducts at a finite speed.
Figure 3 shows the variation of the nondimensional temperature, displacement components and stress components along the distance y for different fractional order parameter values a = 0.8, 1.0 and 1.2 at fixed time (t = 0.12) when x direction (x = 0.5) remains constant. The solid
I7X10"4
3 V l£
2 ■2\ v. l\
1
0
0.0 0.4 0.8 1.2 1.6 y
Fig. 3. The distribution of temperature T (a), horizontal u (b), vertical displacement v (c), a^ (d), a^ (e), and ayy f) stress components with respect to y for different values of a = 0.8 (1), 1.0 (2), 1.2 (3) when x = 0.5 at t = 0.12
3 2 1 0
-3-2-1 0 1 2 x ux
1 0 -1
-2
-3-2-1 0 1 2 x
vx 10~5
r1 A Id
4
3 2 1 ■ 3 ■■ \ // A
0 -1 J/ \V
5 -2 -1 0 1 2 x
Fig. 4 The distribution of temperature T (a), horizontal u (b), vertical displacement v (c) with respect to x for different values of a = 0.8 (1), 1.0 (2), 1.2 (3) when y = 0.5 at t = 0.12
line (1) refers to the weak conductivity, while the dotted line (3) refers to the normal conductivity and the dashed line (2) refers to the strong conductivity. Figure 3, a represents the variation of temperature with the distance y. It is observed that at the boundary y = 0, the magnitude of temperature is equal to one, which agrees with the imposed boundary condition. The magnitude of temperature starts from the maximum value and then continuously decreases to zero with increasing y, while it increases with decreasing the fractional parameter a. Figure 3, b represents the variation of the horizontal displacement with the distance y. The horizontal displacement starts from zero which obey the boundary condition, then gradually increases until it attains a peak value at a particular location after that gradually decreases to zero with increasing y. The horizontal displacement increases with decreasing the fractional parameter. Figure 3, c shows the variation of the vertical displacement with the distance y. The magnitude of vertical displacement starts from the maximum value and then continuously decreases to close zero with increasing y. Also, before the intersection of the three curves, the vertical displacement magnitude decreases as the value of the fractional order decreases.
Figures 3, d-f depict stress components axx, axy and ayy with respect to the distance y.The magnitude of stress components axx, axy and ayy decreases as the value of the fractional order decreases before the intersection of the three curves. However, after the intersection, all values increase as the fractional order decreases.
Figure 4 demonstrate the variation of the nondimensio-nal forms of temperature and the displacement components with the distance x for different fractional order parameter values a = 0.8, 1.0 and 1.2 at fixed time (t = 0.12) when the y direction (y = 0.5) remains constant. The solid line (1) refers to the weak conductivity, while the dotted line (3) refers to the normal conductivity and the dashed line (2) refers to the strong conductivity.
In Fig. 4, a the temperature distribution is plotted along the distance x for y = 0.5. At the length of the surface heated (-1 < x < 1), the temperature field has maximum values and begins to decrease near the edges (x = ±1) where it decreases smoothly and finally closes zero. Figure 4, b displays the distribution of the horizontal displacement along the distance x. The vertical displacement starts decreasing at the beginning and ending of the surface heated (-1 < x < < 1) and has a minimum value at the middle of the heated surface, after which it begins to increase and reaches a maximum close to the edges (x = ±1) and then decreases to zero. The variation of the vertical displacement with respect to x is shown in Fig. 4, c. The displacement magnitude has the maximum value along the length of the surface heated (-1 < x < 1), and it starts to decrease just near the edges (x = ±1), and then decreases to zero.
7. Conclusions
The effect of fractional order derivative on a two-dimensional problem due to thermal shock with weak, normal and strong conductivity has been investigated. The governing equations have been taken in the context of Green and Naghdi of type III model (GNIII model) under fractional order derivative. An analytical solutions has been obtained by employing the Laplace and exponential Fourier transformations in combination with the eigenvalues approach. For weak, normal and strong conductivity, some numerical computations for a copper-like medium have been carried out. The results demonstrate that the effect of fractional order parameter has a significant role for all physical quantities considered in the problem.
References
1. Oldham K.B., Spanier J. The Fractional Calculus. V. 111 // Mathematics in Science and Engineering. - New York-London: Academic Press, 1974.
2. Podlubny I. Fractional Differential Equations: An Introduction to Fractional Derivatives, Fractional Differential Equations, to Methods of Their Solution and Some of Their Applications. V. 198 // Mathematics in Science and Engineering. - San Diego: Academic Press, 1999.
3. Kimmich R. Strange kinetics, porous media, and NMR // Chem. Phys. -
2002. - V. 284. - No. 1-2. - P. 253-285.
lO"5
4. Mainardi F., Gorenflo R. On Mittag-Leffler-type functions in fractional evolution processes // J. Comput. Appl. Math. - 2000. - V. 118.-No. 1. - P. 283-299.
5. Youssef H.M. Theory of fractional order generalized thermoelasticity // J. Heat Trans. - 2010. - V. 132. - No. 6. - P. 1-7.
6. Ezzat M.A., El Karamany A.S. Theory of fractional order in electro-thermoelasticity // Eur. J. Mech. A. Solid. - 2011. - V. 30. - No.4.-P. 491-500.
7. Jumarie G. Derivation and solutions of some fractional black-scholes equations in coarse-grained space and time // Appl. Merton's Opt. Portfolio. Comput. Math. Appl. - 2010. - V. 59. - No. 3. - P. 11421164.
8. MashatD.S., Zenkour A.M., AbouelregalA.E. Fractional order thermo-
elasticity theory for a half-space subjected to an axisymmetric heat distribution // Mech. Adv. Mater. Struct. - 2015. - V. 22. - No. 11. -P. 925-932.
9. Sur A., Kanoria M. Fractional order generalized thermoelastic functionally graded solid with variable material properties // J. Solid Mech. - 2014. - V. 6. - No. 1. - P. 54-69.
10. Sarkar N., Lahiri A. The effect of fractional parameter on a perfect conducting elastic half-space in generalized magneto-thermoelasticity // Meccanica. - 2013. - V. 48. - No. 1. - P. 231-245.
11. Youssef H.M. Two-dimensional thermal shock problem of fractional order generalized thermoelasticity // Acta Mech. - 2012. - V. 223. -No. 6. - P. 1219-1231.
12. Ezzat M.A., El-Karamany A.S., Fayik M.A. Fractional ultrafast laser-induced thermo-elastic behavior in metal films // J. Thermal Stress. -2012. - V 35. - No. 7. - P. 637-651.
13. Abbas I.A. Eigenvalue approach to fractional order generalized mag-neto-thermoelastic medium subjected to moving heat source // J. Magnetism Magnet. Mater. - 2015. - V. 377. - P. 452-459.
14. Sherief H., Abd El-Latief A.M. Effect of variable thermal conductivity on a half-space under the fractional order theory of thermoelasticity // Int. J. Mech. Sci. - 2013. - V. 74. - P. 185-189.
15. Kumar R., Gupta V., Abbas I.A. Plane deformation due to thermal source in fractional order thermoelastic media // J. Comput. Theor. Nanosci. - 2013. - V. 10. - No. 10. - P. 2520-2525.
16. Abbas I.A., Youssef H.M. Two-dimensional fractional order generalized thermoelastic porous material // Latin Am. J. Solid. Struct. -2015.- V. 12. - No. 7. - P. 1415-1431.
17. Abbas I.A. A Problem on functional graded material under fractional order theory of thermoelasticity // Theor. Appl. Fract. Mech. - 2014. -V. 74. - P. 18-22.
18. Youssef H.M., Abbas I.A. Fractional order generalized thermoelasticity with variable thermal conductivity // J. Vibroeng. - 2014. - V. 16. -No. 8. - P. 4077-4087.
19. Zenkour A.M., Abouelregal A.E. State-space approach for an infinite medium with a spherical cavity based upon two-temperature generalized thermoelasticity theory and fractional heat conduction // Zeitsch. Angewandte Math. Phys. - 2014. - V. 65. - No. 1. - P. 149-164.
20. Abbas I.A. Eigenvalue approach for an unbounded medium with a spherical cavity based upon two-temperature generalized thermoelastic theory // J. Mech. Sci. Tech. - 2014. - V. 28. - No. 10. - P. 4193-4198.
21. Sur A., Kanoria M. Fractional heat conduction with finite wave speed in a thermo-visco-elastic spherical shell // Latin Am. J. Solid. Struct. -2014. - V 11. - No. 7. - P. 1132-1162.
22. Das N.C., Lahiri A., Giri R.R. Eigenvalue approach to generalized thermoelasticity // Ind. J. Pure Appl. Math. - 1997. - V. 28. - No. 12. -P. 1573-1594.
23. Abbas I.A. A Dual phase lag model on thermoelastic interaction in an infinite fiber-reinforced anisotropic medium with a circular hole // Mech. Based Design Struct. Machin. - 2015. - V. 43. - No. 4. -P. 501-513.
24. StehfestH. Algorithm 368: Numerical inversion of laplace transforms [D5] // Commun. ACM. - 1970. - V. 13. - No. 1. - P. 47-49.
25. Sherief H.H., El-Maghraby N.M. A mode-I crack problem for an infinite space in generalized thermoelasticity // J. Therm. Stress. -2005. - V 28. - No. 5. - P. 465-484.
Поступила в редакцию 14.03.2017 г.
Сведения об авторе
Ibrahim A. Abbas, Prof. Dr., Prof., Sohag University, Egypt, ibrabbas7@yahoo.com
