The derivative of $F$ is $DF=[\nabla F_1,\cdots,\nabla F_k]^T$ ; let $a\in\mathbb{R}^n$, $b=F(a)$ and $V=F^{-1}(b)$. $V$ is the intersection of the $k$ hypersurfaces $F_i(x)=b_i$. The normal vector in $a$ to such a hypersurface is $\nabla F_i(a)\in \mathbb{R}^n$. Here $rank(DF_a)=k$, that is $W=span(\nabla F_1(a),\cdots,\nabla F_k(a))$ has dimension $k$. According to the implicit function theorem, in a neighborhhood of $a$, $V$ is a variety of dimension $n-k$, that is $V$ is $C^1$-isomorphic to an open subset of $\mathbb{R}^{n-k}$. Moreover the tangent space of $V$ in $a$ is the orthogonal of $W$.
For instance, let $n=3,k=2$. $V$ is the intersection of $2$ surfaces in the standard space. The normal vectors $u_1,u_2$ in $a$ are not parallel ; then $V$ is locally a line and the cross product $u_1\times u_2$ is tangent to this line.
EDIT 1. In other words, an approximation of the equation of $V$ is $DF_a(x-a)=0$, that is, for every $i\leq k$, $<\nabla F_i(a),x-a>=0$.
@ user36772 , I just read your last four lines ! You speak about the case when (in my instance) the $2$ previous normals are parallel. Then the surfaces are tangent in $a$ and we know nothing about the intersection. In other words, when the hypothesis of a theorem are not satisfied, then (is it surprising ?) the theorem does not work.
EDIT 2. (answer to user36772). A level set is a subvariety of codimension $1$, that is an hypersurface.
The tangent space to an hypersurface is the hyperplane that is orthogonal to a normal vector ; then the tangent space to $V$ is the intersection of these hyperplanes. From the geometrical point of view, to say that the $C^1$ functions are independent in a neighborhood of $a$ is equivalent to identify each hypersurface with its tangent hyperplane in $a$ and to say that the linear equations associated to these hyperplanes are linearly independent. This property is stable in the following sense: if we move slightly our hypersurfaces, then the intersection remains similar to the original one.
If these equations are not linearly independent, then the instability comes at a gallop. For instance, consider, in $\mathbb{R}^3$, $a=0, F_1=y-x^2,F_2=y-x^4$. Then, locally, the intersection of the surfaces is the line $Oz$. Yet, if you move one surface, then the intersection may be locally void.
Think also to the GPS ; we need $5$ satellites. Geometrically, the intersection of $3$ spheres suffice. Yet a fourth measure allows synchronization of clocks. Why the fifth ? Because if two among the satellites are "close", then the associated spheres are nearly tangent and the intersection is unstable.