Originally, double network hydrogels were introduced in the form of two interpenetrating chemically crosslinked networks. [2] In these materials, high mechanical strength is obtained when the network has a definite structure, namely, when the first network is densely crosslinked and brittle, whereas the second network is loosely crosslinked and flexible. Under extreme deformation, sacrificial breakage of the chemical bonds in the first network and damping by the strands in the second network act synergistically and significantly increase the mechanical strength and reduce crack propagation. [1] However, the irreversible breakage of the chemical bonds limits their practical applicability. To overcome this limitation, novel double network hydrogels are developed based on physically crosslinked first networks, so that the sacrificial bonds can reform after deformation and the product can be reused. [3,4] Still, like the original double network hydrogels, the optimal elasticity and adaptability can be achieved only with specific structural features. [3-6] Despite this notion, most of the research in this field is devoted to the development of new hydrogels by combination of different types of polymers, [4,6-11] but general structure-property relationships for such materials are less developed as they are for single networks of pure chemical or pure physical crosslinks. Purely chemically crosslinked networks are generally prepared either by free radical copolymerization of monomers and crosslinker or by connecting pre-polymerized building blocks. [12] Either way, the reaction conditions strongly affect the structure of the gels obtained. [13] In turn, the properties of these gels, as-prepared or in swollen states, depend on the structure and the polymer-network homogeneity, and these are the two main tuning controls. [14,15] Accordingly, Sakai and coworkers have developed new hydrogels based on two complementary tetra-PEG building blocks, which offer a regular network mesh size and therefore a homogeneous structure to be formed that provides superior mechanical strength compared to the typical inhomogeneous hydrogels. [16] In contrast to such permanent chemical networks, purely physically crosslinked networks have a structure that evolves through time. [17-19] In this context, the dynamics of the reversible bonds determines the rate of structural development in response to external stimuli. Therefore, dynamic characteristics control the final properties of physical gels. Craig and coworkers [20] and Double network hydrogels are composed of chemical and physical bonds, whose influences on the macroscopic material properties are convoluted. To decouple these, a model dually crosslinked network with independently tunable permanent and reversible crosslinks is introduced. This is realized by interlinking linear and tetra-arm poly(ethylenegycol) (PEG) precursors with complementary reactive terminal groups. The former also carries a terpyridine ligand at each end, which forms reversible metallo-supramolecular bonds upon add...