For a Fréchet differentiable map F:UEYF:U\subset E\to Y between real normed spaces, its linearization at uu is the operator DF(u)DF(u). The associated affine approximation is

F(u+h)=F(u)+DF(u)h+R(u,h),R(u,h)Y=o(hE).F(u+h)=F(u)+DF(u)h+R(u,h),\qquad \|R(u,h)\|_Y=o(\|h\|_E).

The controls all small increments in the stated source norm.

Linearized equations

To correct a residual F(u)F(u), one may first solve DF(u)h=F(u)DF(u)h=-F(u). This cancels the displayed constant and linear terms, leaving R(u,h)R(u,h). Invertibility and bounds for the inverse need separate proofs. Computing εF(u+εh)ε=0\left.\partial_\varepsilon F(u+\varepsilon h)\right|_{\varepsilon=0} in each direction gives a candidate linearization; directional derivatives alone do not establish Fréchet differentiability.