As the global demand and consumption of clean and renewable electrical energy continues to grow, there is a complementary need for efficient energy storage technologies that charge rapidly. Currently, mesoporous metal nanoparticles, particularly Pd, are being examined for potential uses in hydrogen storage, electrochemistry (double-layer capacitors), and catalysis [1]. In all these applications, surface interactions control performance. An ideal structure would have a highlyconnected pore morphology, where any point in the structure is within a few atoms of a surface interface. Such a structure would exhibit rapid mass transport to the pore surface, faster reaction kinetics within the structure, and high capacitance in electrochemical double-layer capacitors. Palladium nanoparticles have been grown with interconnected ~3nm pores using a metal-surfactant paste, and it has been shown that the pore structure and morphology can be controlled by synthesis conditions [2, 3]. In order to synthesize porous Pd nanostructures with optimal pore morphology for hydrogen storage, the growth of Pd in the surfactant network must first be understood.Using in-situ STEM microscopy and a fluid stage by Hummingbird Scientific, the e-beam growth of Pd nanostructures can be recorded with nanometer spatial resolution. The in-situ fluid stage consists of 2 silicon nitride windows, each 50 nm thick. The chips are stacked, being separated by 50-70nm tall gold spacers, providing a channel for the liquid (Pd paste). Here we us this in-situ experimental setup on aqueous Pd salt solutions (control) and Pd-surfactant pastes. Figure 1 shows the progressive growth of Pd nanostructures from the Pd salt solution. Each image is taken ~10 seconds after the preceding image, providing an indication of the growth rate. The Pd growth consists of initial homogeneous nucleation of seed particles, followed by the coarsening and fusing of the small particles to grow large networks. Figure 2 shows the growth of Pd structure within the surfactant support. The initial nucleation of seed particles was not captured, but these images show the agglomeration and fusing of small particles, forming a larger porous Pd network. Diffusion and growth kinetics of Pd in the surfactant paste is much slower than in the aqueous solution. Far less nucleation of seed Pd particles occurs in the surfactant paste. Instead, growth of large networks is more dependent on the motion and agglomeration of existing Pd particles.[1] F.