We discuss the identification of untangled graph embeddings for finite planar and nonplanar graphs as well as infinite crystallographic nets. Two parallel approaches are discussed: explicit 3-space embeddings and reticulations of 2-manifolds. 2D and 3D energies are proposed that allow ranking of (un)tangled embedding graphs. §1. Introduction Graphs, G are topological objects, composed of a collection of vertices, v i (i ∈ {1, N}) and edges, e j , associated with vertex pairs, e j (v k , v l ). For simplicity, assume that G is simple (i.e. for any {k, l}, the number of associated edges is at most one). We are interested in embeddings of topological graphs in euclidean 3-space, G, motivated by the plethora of three-dimensional chemical structures, which can be idealised as embedded graphs. The vertices and edges of these graphs correspond to atoms and chemical bonds in covalent crystals or organic molecules; in the case of supra-molecular materials such as metal-organic frameworks (MOFs) or DNA assemblies) these coincide with molecular groups and polymeric ligands or H-bonds respectively. We are interested in the effects of the graph embedding on the behaviour of the material.These issues are relevant to the physical properties of materials. For example, the hardness of physical glasses can be correlated with the rigidity in the resulting bonding network, and is therefore critically dependent on the topology of the glass network. 22) The viscosity of polymers in solution is intimately associated with the entanglement of the polymer chains within the solution. 10) Here we explore aspects of ambient isotopy of graph embeddings. Define all embeddings G of a graph G that share a common ambient isotopy as equivalent isotopes. Distinct isotopeswhich are not ambient isotopic -differ in the relative entanglement of graph edges. Definition of entanglement requires elucidation of an unentangled 'ground state' isotope, G 0 , of a graph. We propose a definition for G 0 for generic G, including infinite graphs, later in this paper. For now, we assume G is 3-connected and planar (and simple), so that it is a polyhedral graph. 11) In this case, G 0 necessarily embeds in the sphere (S 2 ) without edge crossings. This is also sufficient to characterise G 0 , since Whitney's theorem ensures that the 2-cell embedding of G into S 2 -the isotope G 0 -is unique. 24) Downloaded from https://academic.oup.com/ptps/article-abstract