Unusual large magnetostrictions as well as anisotropy compensation have bee
n found in quaternary Sm0.9Pr0.1(Fe1-xCox)(2). The magnetostriction constan
ts lambda(111) and lambda(100) at room temperature are -4600 X 10(-6) and 5
600 X 10(-6), respectively, in Sm0.9Pr0.1(Fe0.4Co0.6)(2). The fact of \lamb
da(111)\ approximate to \lambda(100)\ can be understood in terms of the com
petition of different crystal distortion. The spin reorientation is also ob
served, which can be understood on the basis of a two-sublattice model. A p
hase diagram for the spin configurations of Sm0.9Pr0.1(Fe1-xCox)(2) (0 less
than or equal to x less than or equal to 1.0) is determined by analyzing t
he results of Mossbauer and magnetization measurements. The giant magnetost
riction is ascribed to the combined contribution of large magnetostrictive
praseodymium and of the filling of the 3d band due to the Co substitution f
or Fe.