In this paper we study the Brinkman system and the Darcy-Forchheimer-Brinkman system with the boundary condition of the Navier’s type $$ {\textbf{u}}_{{\mathbf {\mathcal {T}}}} = {\textbf{g}}_{{\mathbf {\mathcal {T}}}} $$
u
T
=
g
T
, $$\rho =h$$
ρ
=
h
on $$\partial \Omega $$
∂
Ω
for a bounded planar domain $$\Omega $$
Ω
with connected boundary. Solutions are looked for in the Sobolev spaces $$W^{s+1,q}(\Omega ,{\mathbb R}^2)\times W^{s,q}(\Omega )$$
W
s
+
1
,
q
(
Ω
,
R
2
)
×
W
s
,
q
(
Ω
)
and in the Besov spaces $$B_{s+1}^{p,r}(\Omega ,{\mathbb R}^2)\times B_s^{q,r}(\Omega )$$
B
s
+
1
p
,
r
(
Ω
,
R
2
)
×
B
s
q
,
r
(
Ω
)
. Classical solutions are from the spaces $${\mathcal C}^{k+1,\gamma }(\overline{\Omega },{\mathbb R}^2) \times {\mathcal C}^{k,\gamma }(\overline{\Omega })$$
C
k
+
1
,
γ
(
Ω
¯
,
R
2
)
×
C
k
,
γ
(
Ω
¯
)
. For the Brinkman system we show the unique solvability of the problem. Then we study the Navier problem for the Darcy-Forchheimer-Brinkman system and small boundary conditions.