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<title>BRINKMAN-FORCHHEIMER EQUATIONS IN HOMOGENEOUS SOBOLEV SPACES</title>
<link href="http://hdl.handle.net/123456789/1624" rel="alternate"/>
<subtitle/>
<id>http://hdl.handle.net/123456789/1624</id>
<updated>2026-04-20T07:19:53Z</updated>
<dc:date>2026-04-20T07:19:53Z</dc:date>
<entry>
<title>BRINKMAN-FORCHHEIMER EQUATIONS IN HOMOGENEOUS SOBOLEV SPACES</title>
<link href="http://hdl.handle.net/123456789/1625" rel="alternate"/>
<author>
<name>ADEYEMO, Kabiru Michael</name>
</author>
<id>http://hdl.handle.net/123456789/1625</id>
<updated>2022-03-02T14:27:38Z</updated>
<published>2021-01-01T00:00:00Z</published>
<summary type="text">BRINKMAN-FORCHHEIMER EQUATIONS IN HOMOGENEOUS SOBOLEV SPACES
ADEYEMO, Kabiru Michael
Brinkman-Forchheimer Equations (BFE) are used to describe non-Darcy be havior of  uid  ow in a saturated porous medium. Researchers in this area have&#13;
focused on the study of structural stability and long time behavior of solutions in&#13;
square integrable space L&#13;
2&#13;
. However, problems on existence of weak solutions in&#13;
the homogeneous Sobolev space H˙ s and stability of the system in the critical homo geneous Sobolev space H˙&#13;
1&#13;
2 remain relatively unresolved. This study was therefore&#13;
designed to obtain existence of weak solutions in H˙ s and stability of the system&#13;
with respect to initial data, ϕn in H˙&#13;
1&#13;
2 .&#13;
Galerkin method was employed to obtain weak solutions in H˙ s = {u ∈ S&#13;
0&#13;
(R&#13;
3&#13;
) :&#13;
||u||H˙ s(R3) &lt; +∞} where S&#13;
0&#13;
is dual space of tempered distribution and ||u|| is the&#13;
norm of u. BFE was approximated by  nite-dimensional problem when the damp ing term is continuous, continuously di erentiable and satis es Lipschitz condi tion. Cauchy-Schwarz inequality and Parseval identity were used to obtain uni form bounds on the Fourier transforms of some terms in L&#13;
2 appearing in the weak&#13;
formulation. The concept of pro le decomposition was employed to show that the&#13;
sequence of solutions of BFE associated with sequence of initial data was bounded&#13;
in E∞ = C&#13;
0&#13;
b&#13;
((R&#13;
+, H˙&#13;
1&#13;
2 (R&#13;
3&#13;
))∩L&#13;
2&#13;
(R&#13;
+, H˙&#13;
3&#13;
2 (R&#13;
3&#13;
))∩L&#13;
4&#13;
(R&#13;
+, L4&#13;
(R&#13;
3&#13;
)) where H˙&#13;
3&#13;
2 , is a space&#13;
of vector  elds whose  rst derivative is in H˙&#13;
1&#13;
2 , C&#13;
0&#13;
b&#13;
, is a space of bounded continuous&#13;
functions and L&#13;
4&#13;
is a space of four times integrable functions. By using the orthog onality property of sequence of scales and cores, (hj&#13;
, xn) in (R+ \ {0} × R&#13;
3&#13;
), the&#13;
sequence of solutions was decomposed into a sum of orthogonal pro les in E∞ to&#13;
generate a priori estimate. Finite time singularities of solutions was also obtained&#13;
with respect to singularity generating initial data by pro le decomposition.&#13;
The weak solution u(x, t) obtained belongs to L&#13;
∞((R+, H˙ s&#13;
(R3&#13;
))∩L&#13;
2&#13;
(R+, H˙ s+1(R3&#13;
))∩&#13;
L&#13;
r+1(R+, Lr+1(R3&#13;
)) for r ≥ 1 when the damping term is continuous and satis es&#13;
the estimate Sup0≤t≤T ||u||H˙ s(R3 +2λ&#13;
R T&#13;
0&#13;
||5u||2&#13;
H˙ s(R3)&#13;
dt+2β&#13;
R T&#13;
0&#13;
||u||r+1&#13;
Lr+1 dt ≤ ||u0||2&#13;
H˙ s&#13;
v&#13;
where λ and β are positive constants. Also for continuously di erentiable bi harmonic damping term, the solution is in L&#13;
∞((R+, L2&#13;
(R3&#13;
)) ∩ L&#13;
2&#13;
(R+, H˙ 1&#13;
(R3&#13;
)) ∩&#13;
L&#13;
2&#13;
(R+, H˙ 2&#13;
(R3&#13;
)) and satis es Sup0≤t≤T ||u||2&#13;
L2 + 2λ&#13;
R T&#13;
0&#13;
|| 5 u||2&#13;
L2 dt + 2β&#13;
R T&#13;
0&#13;
||u||2&#13;
H2 ≤&#13;
||u0||2&#13;
L2 . The damping term with Lipschitz condition satis es the estimate&#13;
Sup0≤t≤T ||u||2&#13;
H˙ s(R3)&#13;
+ 2λ&#13;
R T&#13;
0&#13;
|| 5 u||2&#13;
H˙ s(R3)&#13;
dt + 2β&#13;
R T&#13;
0&#13;
||u||r+1&#13;
Lr+1 ≤ ||u0||2&#13;
H˙ s(R3)&#13;
for u ∈&#13;
L&#13;
∞((R+, H˙ s&#13;
(R3&#13;
)) ∩ L&#13;
2&#13;
(R+, H˙ s+1(R3&#13;
)) ∩ L&#13;
r+1(R+, Lr+1(R3&#13;
)) and r ≥ 1 where L&#13;
∞&#13;
is a space of essentially bounded functions. The sequence of solutions, un obtained&#13;
was bounded in E∞. The boundedness of the sequence of solution was due to the&#13;
existence of a bound ||ϕn|| ≤ ρ on the sequence of initial data where ρ is any real&#13;
number in [0, CA&#13;
BF E]. Then a priori estimate ||BF E(ϕ)||E∞ ≤ B(||ϕ||&#13;
H˙&#13;
1&#13;
2 (R3)&#13;
, ||u||A)&#13;
was obtained where B, BF E(ϕn), A, C&#13;
A&#13;
BF E are non-decreasing function from&#13;
R&#13;
+ × [0, CA&#13;
BF E] to R&#13;
+, solution of BFE associated with initial data ϕ, admissi ble space, constant in R+ ∪ {+∞} respectively. Existence of singularity generating&#13;
initial data gave rise to  nite time singularities of solution that did not belong to&#13;
E∞.&#13;
The existence of weak solutions was obtained and the system was found to be&#13;
stable with respect to initial data in the homogeneous Sobolev space
</summary>
<dc:date>2021-01-01T00:00:00Z</dc:date>
</entry>
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