It is thought that the large-scale solar-cycle magnetic field is gener
ated in a thin region at the interface of the radiative core (RC) and
solar convection zone (SCZ). We show that the bulk of the SCZ virogour
sly generates a small-scale turbulent magnetic field. Rotation, while
not essential, increases the generation rate of this field. Thus, full
y convective stars should have significant turbulent magnetic fields g
enerated in their lower convection zones. In these stars the absence o
f a radiative core, i.e., the absence of a region of weak buoyancy, pr
ecludes the generation of a large-scale magnetic field, and as a conse
quence the angular momentum loss is reduced. This is, in our opinion,
the explanation for the rapid rotation of the M-dwarfs in the Hyades c
luster. Adopting the Utrecht's group terminology, we argue that the re
sidual chromospheric emission should have three distinctive components
: the basal emission, the emission due to the large-scale field, and t
he emission due to the turbulent field, with the last component being
particularly strong for low mass stars. In the conventional dynamo equ
ations, the dynamo frequencies and the propagation of the dynamo wave
towards the equator are based on the highly questionable assumption of
a constant alpha. Furthermore, meridional motions, a necessary conseq
uence of the interaction of rotation with convection, are ignored. In
this context we discuss Stenflo's results about the global wave patter
n decomposition of the solar magnetic field and conclude that it canno
t be interpreted in the framework of the conventional dynamo equations
. We discuss solar dynamo theories and argue that the surface layers c
ould be essential for the generation of the poloidal field. If this is
the case an alpha-effect would not be needed at the RC-SCZ interface
(where the toroidal field is generated). The two central problems faci
ng solar dynamo theories may the transport of the surface poloidal fie
ld to the RC-SCZ interface and the uncertainty about the contributions
to the global magnetic field by the small-scale magnetic features.