The gravitational field, f, at a distance r from a body with mass M is given by f=GM/rr; it is thus stronger for a more massive body at the same distance away; and weaker for the same body at a greater distance away.
This field is 'what is there' due to M and is independant of externals.
Should a second body of mass m now heave into view, there will be an attractive gravitational force, F, between them; this is given by the product of the field due to the first, f, and the mass of the second, m.
ie F=mf =m(GM/rr) =GMm/rr
It follows that the field can thus be thought of as the 'force per unit mass'
There is a direct correlation with the field due to an electric charge, Q, given by f=Q/4(pi)(Eo)rr and the force, F, exerted upon a second charge, q, which is given by F=qf =q(Q/4(pi)(Eo)rr) =qQ/4(pi)(Eo)rr
Since a force, (gravitational or electric), can only exist between two objects, (masses or charges), the field can be thought of as 'that which is there, due to the first, when there is no second to act upon'