In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain. As a series of penalty problems, the existence of the solutions in the weak sense is proved by a limit process. The uniqueness of the solution is also proved.
Citation: Jia Li, Changchun Bi. Study of weak solutions of variational inequality systems with degenerate parabolic operators and quasilinear terms arising Americian option pricing problems[J]. AIMS Mathematics, 2022, 7(11): 19758-19769. doi: 10.3934/math.20221083
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In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain. As a series of penalty problems, the existence of the solutions in the weak sense is proved by a limit process. The uniqueness of the solution is also proved.
Let Ω⊂RN(N≥2) be a bounded simple connected domain, 0<T<∞ and QT=Ω×[0,T]. We study the following parabolic systems
{min{Liui−fi(x,t,u1,u2),ui−ui,0}=0,(x,t)∈QT,ui(0,x)=ui0(x),x∈Ω,ui(t,x)=0,(x,t)∈∂Ω×(0,T), | (1.1) |
with quasilinear degenerate parabolic operators, where
Liui=∂ui∂t−div(|∇ui|pi−2∇ui),i=1,2. |
The initial boundary value problem of variational inequalities arise in many application in pricing American options and their derivatives. Through the risk neutral strategy, the intrinsic value of many American options can ultimately be attributed to the solution of a variational inequality in the Black-Scholes models. The author refers to [1,2,3] and the references their in.
The nonexistence, existence and uniqueness theory for weak solutions of parabolic systems were studied by many existing works, see e.g., [4,5,6]. In particular, Hassnaoui and Idrissi [6] studied the existence and uniqueness of weak solutions for a nonlinear parabolic system with non-degenerate case of (1.1). Escher, Laurencot and Matioc in [7] proved the global existence of nonnegative weak solutions to a degenerate parabolic system without quasilinear terms in (1.1). Furthermore, the authors showed that these weak solutions converge at an exponential rate.
In recent years, there has been tremendous interest in developing existence and uniqueness theory for weak solutions of parabolic variational inequality (see, for example, [3,8,9,10,11,12,13,14] and the references therein). In 2014, the authors in [9] discussed the problem
{min{ut−Lu−F(u,x,t),u(x,t)−u0(x)}=0inQT,u(x,0)=u0(x)inΩ,u(x,t)=0on∂Ω, | (1.2) |
with second order degenerate elliptic operator
Lu=−udiv(a(u)|∇u|p(x,t)−2∇u)−γ|∇u|p(x,t). |
Under the assumptions about u0 and F, they proved the existence and uniqueness of the weak solution. When a(u)=1, and p(x,t)=2, the authors in [10,11] discussed the existence and numerical algorithm of solution. In [12], a new property of variable exponent Lebesgue and Sobolev spaces was examined. Using these properties, the authors proved the existence of the solution of some parabolic variational inequality.
To the best of our knowledge, the existence and uniqueness for multi-variable problem of parabolic variational inequalities (called variational inequality systems) were less studied. We cannot easily put the method in [10,11] to the multi-variable case since the systems are coupled with quasilinear terms.
The aim of this paper is to study the existence and uniqueness of solution for parabolic systems with quasilinear degenerate inequalities in a bounded domain. We mainly use comparison theorem and penalty method to construct a sequence of approximation solutions with the help of monotone iteration technique. Then we obtain the existence of solutions to the system (1.1) by a standard limiting process.
The paper is organized as follows. In Section 2, we present our main theorems. Section 3 gives some estimates about penalty problems to prove our main results. Section 4 analyses the existence and uniqueness of solutions to variational inequality system (1.1).
In spirit of [3] and [9], we introduce the following maximal monotone graph
G(x)={0,x>0,1,x=0. | (2.1) |
The purpose of the paper is to obtain the existence and uniqueness of weak solutions of (1.1), and the weak solution is defined as follows.
Definition 2.1. Function {(u1,ξ1),(u2,ξ2)} is called a generalized solution of the systems (1.1) if ui∈L∞(QT)∩L(0,T,W1,pi0(Ω)), ∂tui∈L2(ΩT), ξi∈L∞(0,T;L∞(Ω)), i=1,2, and satisfies (a) ui(x,t)≥ui0(x), (b) ui(x,0)=ui0(x), (c) ξi∈G(ui−ui0), (d) for every test-function φi∈C10(ˉQT)
∫∫QT(−ui⋅∂tφi+|∇ui|pi−2∇ui∇φi)dxdt−∫QTui0⋅φi(x,0)dx=∫∫QTfi(x,t,u1,u2)⋅φidxdt+∫t0∫Ωξi⋅φidxdt. | (2.2) |
Here C10(ˉΩT) is the space of all continuous and differentiable functions satisfying
φi(x,T)=0for(x,t)∈∂Ω×(0,T),i=1,2. |
Condition (d) of Definition 2.1 implies that
∫t0∫Ω(−ui⋅∂tφi+|∇ui|pi−2∇ui∇φi)dxdt+∫QTui(x,t)⋅φi(x,t)dx−∫ΩTui0⋅φi(x,0)dx=∫t0∫Ωfi(x,t,u1,u2)⋅φidxdt+∫t0∫Ωξi⋅φidxdt. | (2.3) |
We introduce the constrains to the nonlinear functions fi,i=1,2 involved in this paper as follows.
Definition 2.2. A function f=f(u1,u2) is quasimonotone nondecreasing (resp., nonincreasing) if for fixed u1 (or u2), f is nondecreasing (resp., nonincreasing) in u2 (or u1).
To study the problem (1.1), we make the following assumptions:
(H1) fi(x,t,u1,u2) is quasimonotonically nondecreasing for u1, u2, i=1,2.
(H2) fi(x,t,u1,u2)∈C(Ω×[0,T]×R2), and there exists a nonnegative function g(s)∈C1(R) such that
|fi(x,t,u1,u2)|≤min{g(u1),g(u2)}. |
Our main results are present as follows:
Theorem 2.1. Let (H1) and (H2) be satisfied, and ui0∈L∞(ΩT)∩W1,pi0(Ω), i=1,2. Then problem (1.1) has a solution u=(u1,u2) in the sense of Definition 2.2.
Theorem 2.2. Assume that f=(f1,f2) is Lipschitz continuous in (u1,u2), then the solution of problem (1.1) is unique.
To prove the theorem, we consider the following penalty problem
{Liεuiε=fi(x,t,u1ε,u2ε)−βε(uiε−ui0),(x,t)∈QT,uiε(x,0)=ui0ε(x)=ui0+ε,x∈Ω,uiε(x,t)=ε,(x,t)∈∂QT, | (3.1) |
where
Liεuiε=∂uiε∂t−div((|∇uiε|2+ε)pi−22∇uiε). |
Here, βε(⋅) is the penalty function satisfying
ε∈(0,1),βε(⋅)∈C2(R),βε(x)≤0,βε(0)=−1,β′ε(x)≥0,β″ε(x)≤0,limε→0+βε(x)={0,x>0,−1,x=0. | (3.2) |
It is worth noting that when ui>ui,0, Liui−fi(x,t,u1,u2)=0, and when ui=ui,0, one gets Liui≥fi(x,t,u1,u2) in (1.1). In (3.1), βε(uiε−ui0) plays a similar role. When uiε>ui0+ε,
Liεuiε−fi(x,t,u1ε,u2ε)=−βε(uiε−ui0)=0, |
and when ui0≤uiε≤ui0+ε, we have
Liεuiε−fi(x,t,u1ε,u2ε)=−βε(uiε−ui0)≥0. |
With a similar method as in [8], we can prove that regularized problem has a unique weak solution
ui∈L∞(QT)∩L(0,T,W1,pi0(Ω)),∂tui∈L2(QT),i=1,2, |
satisfying the following integral identities
∫Ω∂tui⋅φidx+∫Ω|∇ui|pi−2∇ui∇φidx+∫Ωβε(uiε−ui0)φidx=∫QTfi(x,t,u1,u2)⋅φidx | (3.3) |
with φi∈C1(ˉΩT) and t∈(0,T).
We start with two preliminary results that will be used several times henceforth.
Lemma 3.1. [[15], Lemma2.1.] Let M(s)=|s|p(x,t)−2s, then ∀ξ,η∈RN
(M(ξ)−M(η))⋅(ξ−η)≥{2−p|ξ−η|p,2≤p<∞,(p−1)|ξ−η|2(|ξ|p+|η|p)p−2p,1≤p<2. |
Lemma 3.2. (Comparison principle) Assume ui and vi are in Lpi(0,T;W1,pi(Ω)). If Liεui≥Liεvi in QT and ui(x,t)≤vi(x,t) on ∂QT, then ui(x,t)≤vi(x,t) in QT, i=1,2.
Proof. We argue by contradiction. Suppose ui(x,t) and vi(x,t) satisfy Liεui≥Liεvi in QT, and there is a δ>0 such that for some 0<τ≤T, wi=ui−vi>δ on the set
Ωδ=Ω∩{x:wi(x,t)>δ} |
and |Ωδ|>0, i=1,2. Let
Fε(ξ)={2⋅ε−12−2⋅ξ−12,ifξ>ε,0,ifξ≤ε, |
whereδ>ε>0. Since Fε(wi)≤0, we multiply Liεui≥Liεvi by Fε(wi) and integrate in Qτ to have
∫∫Qτ∂∂twi⋅Fε(wi)dxdt+∫∫Qτ[(|∇uiε|2+ε)pi−22∇uiε−(|∇viε|2+ε)pi−22∇viε]∇Fε(wi)dxdt≤0 |
or equivalently
J1+J2≤0, | (3.4) |
where Qτ,ε={(x,t)∈QT|w>ε},
J1=∫∫Qτ,ε∂∂twi⋅Fε(wi)dxdt, |
J2=12∫∫Qτ,εw−32i[(|∇uiε|2+ε)pi−22∇uiε−(|∇viε|2+ε)pi−22∇viε]∇widxdt. |
Now let t0=inf{t∈(0,τ]:w>ε}, then we estimate J1 as follows
J1=∫∫Qτ,θ∂∂twiFε(wi)dxdt=∫Ω(∫t00∂∂twiFε(wi)dt+∫t00∂∂twiFε(wi)dt)dx≥∫Ω∫wiεFε(s)dsdx≥∫Ωδ∫wiεFε(s)dsdx. | (3.5) |
Using δ>ε>0 and the function Fε(⋅) to (3.5), we have
J1≥∫Ωθ(wi−ε)Fε(s)dx≥(wi−ε)Fε(ε)|Ωδ|. | (3.6) |
By the virtue of the first inequality of Lemma 3.1, we use wi=ui−vi>δ to arrive at
J2≥2−(pi+1)∫∫Qτ,θw−32i|∇wi|pidxdt≥0. | (3.7) |
Since vi∈Lpi(0,T;W1,pi(Ω)), and we plug the above estimates (3.6) and (3.7) into (3.4) and drop the nonnegative terms, we arrive at
(δ−ε)ε−12|Ωδ|<˜C. |
Note that limε→0(δ−ε)ε−12|Ωδ|=+∞, we obtain a contradiction. This means that |Ωδ|=0 and wi≤0 a.e. in Qτ, i=1,2.
Lemma 3.3. Let be weak solutions of (3.1). Then
ui0ε≤uiε≤|ui0|∞+ε,i=1,2, | (3.8) |
uiε1≤uiε2forε1≤ε2,i=1,2, | (3.9) |
where |u0|=supx∈Ω|u0(x)|, for details, see [16,17].
Proof. First, we prove uiε≥ui0ε by contradiction. Assume uiε≤ui0ε in Q0T, i=1,2, Q0T⊂QT. Noting uiε≥ui0ε on ∂QT, we may assume that uiε=ui0ε on ∂Q0T. With (3.1) and letting t=0, it is easy to see that
Lui0,ε=−βε(ui0,ε−ui0,ε)=1,i=1,2, | (3.10) |
Luiε=−βε(uiε−ui0,ε)≤1,i=1,2. | (3.11) |
From Lemma 3.2, we have that
uiε(x,t)≥ui0,ε(x)forany(x,t)∈QT,i=1,2. | (3.12) |
Therefore, we obtain a contradiction.
Second, we pay attention to uiε(t,x)≤|ui0|∞+ε. Applying the definition of βε(⋅) gives
L(|ui0|∞+ε)=0, Luiε=−βε(uiε−ui0,ε)≥0, i=1,2. | (3.13) |
Using Lemma 3.2, (3.13) leads to
uiε(t,x)≤|ui0|∞+εon∂Ω×(0,T), |
uiε(t,x)≤|ui0|∞+εinΩ,i=1,2. | (3.14) |
Thus, combining (3.13) and (3.14) and repeating Lemma 3.2, we have
uiε(t,x)≤|ui0|∞+εinQT,i=1,2. | (3.15) |
Third, we aim to prove (3.9). From (3.1), it is easy to see that
Luiε1=βε1(uiε1−ui0,ε1),i=1,2. | (3.16) |
Luiε2=βε2(uiε2−ui0,ε2),i=1,2. | (3.17) |
It follows by ε1≤ε2 and the definition of βε(⋅) that
Lui0,ε2+βε1(uiε2−ui0,ε)=βε2(uiε2−ui0,ε)−βε1(uiε1−ui0,ε)=βε2(uiε2−ui0,ε)−βε1(uiε2−ui0,ε)≥0, | (3.18) |
i=1,2. Combining initial and boundary condition in (3.1), we obtain that the inequality (3.9) holds by Lemma 3.2.
Lemma 3.4. For any (x,t)∈ΩT, the solution of problem (3.1) satisfies the estimate
|∇uiε|Lpi(QT)≤∫∫QT(|∇uiε|2+ε)pi−22|∇uiε|2dxdt≤C, | (3.19) |
where C is a constant independent of ε.
Proof. Choosing φi=uiε in (3.3), we have
∫∫QT∂tuiε⋅uiε−div((|∇uiε|2+ε)pi−22∇uiε)⋅uiεdxdt=∫∫QTfi(x,t,u1ε,u2ε)uiε−βε(uiε−ui0)uiεdxdt, | (3.20) |
It is easy to see that
∫∫QT∂tuiε⋅uiεdxdt=12∫∫QT∂t(uiε)2dxdt=12∫QTuiε(⋅,T)−uiε(⋅,0)dx. | (3.21) |
Then we substitute (3.21) into (3.20) to arrive at
∫∫QT(|∇uiε|2+ε)pi−22|∇uiε|2dxdt=∫∫QTfi(x,t,u1ε,u2ε)uiε−βε(uiε−ui0)uiεdxdt−12∫QTuiε(⋅,T)−uiε(⋅,0)dx. |
By (3.8) and the property of fi,
|∫∫QTfi(x,t,u1ε,u2ε)uiεdxdt|≤C. | (3.22) |
Applying (3.2) and (3.8) obtains
∫∫QT−βε(uiε−ui0)uiεdxdt≤ε|Ω|T≤|Ω|T. | (3.23) |
Then Lemma 3.4 is proved by combining (3.21)–(3.23).
Lemma 3.5. The solution of problem (3.1) satisfies the estimate
‖∂tuiε‖L2(QT)≤C(pi,T,|Ω|),i=1,2. | (3.24) |
Proof. From (3.3), we have that
∫∫QT(∂tuiε)2dxdt=−∫∫QT(|∇uiε|2+ε)pi−22∇uiε∇∂tuiεdxdt+∫∫QT[fi(x,t,u1ε,u2ε)−βε(uiε−ui0)]⋅∂tuiεdxdt=−A1+A2, | (3.25) |
where
A1=∫∫QT(|∇uiε|2+ε)pi−22∇uiε∇∂tuiεdxdt, |
A2=∫∫QT[fi(x,t,u1ε,u2ε)−βε(uiε−ui0)]⋅∂tuiεdxdt. |
First, we pay attention to A1. Using some differential transform technique obtains
A1=−12∫∫QT(|∇uiε|2+ε)pi−22∂t(|∇uiε|2+ε)dxdt=−1pi∫∫QT∂t(|∇uiε|2+ε)pi2dxdt. |
Since ui0ε(x)=ui0+ε, then
A1≤−1pi∫∫QT∂t(|∇uiε|pi)dxdt≤∫Ω|∇ui0(⋅,0)|pidx. | (3.26) |
Applying Holder inequalities again, we have that
A2≤12∫∫QT[fi(x,t,u1ε,u2ε)−βε(uiε−ui0)]2dxdt+12∫∫QT(∂tuiε)2dxdt. | (3.27) |
Using (a+b)2≤2(a2+b2), the property of fi and (3.2), we arrive at
12∫∫QT[fi(x,t,u1ε,u2ε)−βε(uiε−ui0)]2dxdt≤∫∫QTfi(x,t,u1ε,u2ε)2dxdt+∫∫QTβε(uiε−ui0)2dxdt≤∫∫QTfi(x,t,u1ε,u2ε)2dxdt+T|Ω|≤C. | (3.28) |
Then, we obtain Lemma 3.5 by submitting (3.26)–(3.28) into (3.25).
In this section, we are ready to prove that the system (1.1) has a unique generalized solution. By (3.18), (3.19) and (3.24) and the uniqueness of the weak limits, we know that there are functions
ui∈L∞(QT)∩L(0,T,W1,pi0(Ω)), as ε→0, |
such that for some subsequence of (u1ε,u2ε), denoted again by (u1ε,u2ε),
uiε→ui,f(x,t,u1ε,u2ε)→f(x,t,u1,u2)a.e.inQT, | (4.1) |
∇uiεw→∇uiinLpi(QT), | (4.2) |
|∇uiε|pi−2∇uiεw→wiinLpipi−1(QT),forsomewi, | (4.3) |
∂tuiεw→∂tuiinL2(QT), | (4.4) |
where w→ stands for weak convergence, i=1,2.
Lemma 4.1. For any (x,t)∈ΩT, wi=|∇ui|pi−2∇ui, i=1,2.
Proof. Applying triangle inequality |a+b|≤|a|+|b|, (a,b∈R), it is easy to see that
∫∫QT||∇uiε|pi−2∇uiε−|∇ui|pi−2∇ui|dxdt≤∫∫QT||∇uiε|pi−2−|∇ui|pi−2|⋅|∇uiε|dxdt+∫∫QT|∇ui|pi−2⋅|∇uiε−∇ui|dxdt=I1+I2, |
where
I1=∫∫QT||∇uiε|pi−2−|∇ui|pi−2|⋅|∇uiε|dxdt, I2=∫∫QT|∇ui|pi−2⋅|∇uiε−∇ui|dxdt. |
By mean of the inequality |ar−br|≤|a−b|r, (r∈[0,1],a,b>0), we have
I1=∫∫QT|(|∇uiε|pi)pi−2pi−(|∇ui|pi)pi−2pi|⋅|∇uiε|dxdt≤∫∫QT||∇uiε|pi−|∇ui|pi|pi−2pi⋅|∇uiε|dxdt. |
Applying Holder inequality and (4.2), we have
I1≤(∫∫QT||∇uiε|pi−|∇ui|pi|dxdt)pi−2pi⋅(∫∫QT|∇uiε|pi2dxdt)2pi→0(ε→0). |
Now we pay our attention to I2. From (4.2), we know that ∇ui∈Lpi(QT1). By (4.1), we may conclude that
∇uiε→∇uia.e.inQT. |
If not, there exists a measurable domain OT satisfying
∫∫OT|∇uiε→∇ui|dxdt>0. |
Then, we obtain a contradiction with (4.2). Applying Holder inequality, we have
I2=(∫∫QT|∇ui|pidxdt)pi−2pi⋅(∫∫QT|∇uiε−∇ui|pi2dxdt)2pi→0(ε→0). |
Hence Lemma 4.1 is proved.
This proves that any weak convergence subsequence of |∇uiε|pi−2∂xluiε will have ∂xlwi as its weak limit and hence by a standard argument, and we have that as k→∞,
|∇uiε|∂xluiεw→|∇ui|pi−2∂xluiinLpipi−1(QT). | (4.5) |
Combining the above results, we have, in fact, proved that u=(u1,u2) is a generalized solution of (1.1).
Lemma 4.2. For any (x,t)∈ΩT, it hold that
βε(uε−u0)→ξ∈G(u−u0) as ε→0. | (4.6) |
Proof. Using (3.8) and the definition of βε, we have
βε(uε−u0)→ξasε→0. |
Now, we prove ξ∈G(u−u0). According to the definition of G(⋅), we only need to prove that if u(x0,t0)>u0(x0),
ξ(x0,t0)=0. |
In fact, if u(x0,t0)>u0(x0), there are a constant λ>0 and a δ-neighborhood Bδ(x0,t0) such that if ε is small enough, we have
uε(x,t)≥u0(x)+λ,∀(x,t)∈Bδ(x0,t0). |
Thus, if ε is small enough, we have
0≥βε(uε−u0)≥βε(λ)=0,∀(x,t)∈Bδ(x0,t0). |
Furthermore, it follows by ε→0 that
ξ(x,t)=0,∀(x,t)∈Bδ(x0,t0). |
Hence, (4.6) holds, and the proof of Lemma 4.3 completes.
The proof of Theorem 2.1. Applying (3.8), (3.9), and Lemma 4.3, it is clear that
u(x,t)≤u0(x),in ΩT, u(x,0)=u0(x),in Ω, ξ∈G(u−u0), |
thus (a), (b), and (c) of Definition 1.1 hold. The rest arguments of existence part are the same as those of Theorem 2.1 in [8] by a standard limiting process. Thus, we omit the details.
The proof of Theorem 2.2. The following is the uniqueness result to the solution of the system. Assume that {(u1,ξ1),(u2,ξ2)} and {(v1,ζ1),(v2,ζ2)} are two solutions of (1.1). Let φi=ui−vi in Definition 2.1, i=1,2, then by (2.3),
∫t0∫Ω−ui∂tφi+|∇ui|pi−2∇ui∇φidxdt+∫Ωui(x,t)φi(x,t)dx−∫Ωui(x,0)φi(x,0)dx=∫t0∫Ωfi(x,t,u1,u2)φidxdt+∫t0∫Ωξi⋅φidxdt,a.e.t∈(0,T), |
∫t0∫Ω−vi∂tφi+|∇vi|pi−2∇vi∇φidxdt+∫Ωvi(x,t)φi(x,t)dx−∫Ωvi(x,0)φi(x,0)dx=∫t0∫Ωfi(x,t,v1,v2)φidxdt+∫t0∫Ωζi⋅φidxdt,a.e.t∈(0,T), |
i=1,2. Subtracting the 2 equations, we get
12∫Ωφi2dx=∫t0∫Ω(|∇ui|pi−2∇ui−|∇vi|pi−2∇vi)⋅∇φidxdt+∫t0∫Ω(fi(x,t,u1,u2)−fi(x,t,v1,v2))⋅φidxdt−∫t0∫Ω(ξi−ζi)⋅φidxdt. |
Now we prove
(ξi−ζi)⋅φi≤0,|(ξi−ζi)⋅φi|≤φi. | (4.7) |
On one hand, if ui(x,t)>vi(x,t), then using Lemma2.1 yields
ui(x,t)>ui0(x). |
From (2.1) and above inequality, it is easy to see that
ξi=0≤ζi. | (4.8) |
Combining (2.1) and (4.8),
(ξi−ζi)⋅φi=(ξi−ζi)⋅(ui−vi)≤0,(ξi−ζi)⋅φi≥−φi. | (4.9) |
On the other hand, if ui(x,t)<vi(x,t), it is easy to have thatξi≥0=ζi.In this case,
(ξi−ζi)⋅φi=(ξi−ζi)⋅(ui−vi)≤0,(ξi−ζi)⋅φi≥φi. | (4.10) |
Combining (4.9) and (4.10), (4.7) still holds.
Using the previous inequality and the Lipschitz condition, a simple calculation shows that
∫Ω|u1−v1|2+|u2−v2|2dx≤2K∫t0∫Ω(|u1−v1|+|u2−v2|)2dxdt+∫t0∫Ω|u1−v1|+|u2−v2|dxdt. |
Furthermore, it follows by (a+b)2≤2(a2+b2) and Holder inequalities that
∫Ω|u1−v1|2+|u2−v2|2dx≤(2K+12T|Ω|)∫t0∫Ω|u1−v1|2+|u2−v2|2dxdt. |
Setting F(t)=∫t0∫Ω|u1−v1|2+|u2−v2|2dxdt, then the above inequality can be written as
ddtF(t)≤(2K+12T|Ω|)⋅F(t). |
A standard argument show that F(t)=0 since F(0)=0, and hence ui=vi,i=1,2. The proof is complete.
In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain
{min{Liui−fi(x,t,u1,u2),ui−ui,0}=0,(x,t)∈QT,ui(0,x)=ui0(x),x∈Ω,ui(t,x)=0,(x,t)∈∂Ω×(0,T), |
with quasilinear degenerate parabolic inequalities, where
Liui=∂ui∂t−div(|∇ui|pi−2∇ui),i=1,2. |
The existence and uniqueness of the solutions in the weak sense are proved by using the penalty method and the reduction method with assumptions that p1 and p2 are constants satisfying pi>2. However, there are some problems that have not been solved: when 1<pi<2, pi>2 or pi is x-functions, i=1,2, we cannot use Lemmas 3.1 and 3.2 to prove Lemmas 3.3–3.5. We will continue to study this problem in future.
The author sincerely thanks the editors and anonymous reviewers for their insightful comments and constructive suggestions, which greatly improved the quality of the paper. This work was supported by the Supply and demand docking education employment practice base project of education ministry (No. 20220106223) and the Supply and demand docking education oriented talent training project of education ministry (No. 20220104747).
The authors declare no conflict of interest.
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