AbstractThis note obtains a new regularity criterion for the three-dimensional magneto-micropolar fluid flows in terms of one velocity component and the gradient field of the magnetic field. The authors prove that the weak solution $(u,\omega,b)$
(
u
,
ω
,
b
)
to the magneto-micropolar fluid flows can be extended beyond time $t=T$
t
=
T
, provided if $u_{3}\in L^{\beta }(0,T;L^{\alpha }(R^{3}))$
u
3
∈
L
β
(
0
,
T
;
L
α
(
R
3
)
)
with $\frac{2}{\beta }+\frac{3}{\alpha }\leq \frac{3}{4}+\frac{1}{2\alpha },\alpha > \frac{10}{3}$
2
β
+
3
α
≤
3
4
+
1
2
α
,
α
>
10
3
and $\nabla b\in L^{\frac{4p}{3(p-2)}}(0,T;\dot{M}_{p,q}(R^{3}))$
∇
b
∈
L
4
p
3
(
p
−
2
)
(
0
,
T
;
M
˙
p
,
q
(
R
3
)
)
with $1< q\leq p<\infty $
1
<
q
≤
p
<
∞
and $p\geq 3$
p
≥
3
.