and its rheological properties that control the mechanical properties of cells. [12,13] Examples of such large scale collective behaviors in synthetic active colloids have been experimentally demonstrated in electrically powered Quincke "rollers" [9,14] and metal-coated colloidal particles [8,15] or by magnetic colloids; [16,17] however it has been challenging to realize this in large volumes and at high density with artificial chemically active systems. Interesting material properties have been predicted for active colloids at high density, such as a reentrant phase behavior, dynamic pattern formation, and active turbulence that have the potential to form new active materials, but there have been very few suitable experimental systems that permit one to observe these phenomena. [18][19][20][21][22] Moreover, most of the conventional active colloidal systems are either confined to two dimensions or are operated at low densities, and hence are unable to drive changes in the bulk. Here, we show that inorganic chemically-active nanomotors can be used to prepare large volumes of an active medium, whose bulk viscosity can be controlled by the activity of its constituents. This is, to the best of our knowledge, a first demonstration of collective behavior of synthetic active matter giving rise to a tunable change in bulk material property.Inorganic chemically active colloids or nanomotors convert fuel available in the solvent to self-propel. Due to the asymmetric distribution of catalyst near the colloid, the reaction gives rise to a concentration gradient of product (and educt) molecules or ions across the particle. This causes fluid motion and a slip flow across the particle, and the propulsion of the particle in the opposite direction to the induced slip flows. While several model synthetic active systems are known, including catalytically active Janus particles, [23][24][25][26][27][28][29][30][31][32] it has thus far been difficult to obtain truly large numbers of chemical motors to form an active medium and operate them stably for an extended period of time. [23,33,34] The conventional approach to realize an asymmetric distribution of a catalyst on each colloid is to fabricate "Janus" particles, that have a reactive and nonreactive material on each of the particle's two faces. [12] Physical vapor deposition (PVD) and electro-chemical anodic aluminum oxide (AAO) templated synthesis are commonly used to fabricate Janus particles. [25,26,31,35] However, since both the processes are limited to a monolayer of particles, the overall yield is always low. In addition, pickering emulsion or biphasic electrochemistry based techniques had been used for the bulk synthesis of Janus colloids. [36][37][38][39] Here in this study, a simpler alternate strategy is employed to obtain large numbers of catalytically active self-propellingThe rheological properties of a colloidal suspension are a function of the concentration of the colloids and their interactions. While suspensions of passive colloids are well studied and have been s...