Protein aggregates are agglomerates of individual protein monomers, bound either through irreversible strong interparticle interactions or weak reversible interactions. Protein aggregates are implicated in the pathogenesis of several neurological disorders and are the main mechanism by which biopharmaceuticals, i.e. protein-based drugs, lose their stability during production, storage, and shipping [1,2]. The structure of protein aggregates varies widely depending on the protein type and the conditions under which the aggregate was formed and determines how they interact with biological systems. Conventional methods for determining protein structure include ensemble spectroscopy methods like NMR and x-ray scattering, and direct imaging approaches like negative-stain and cryo transmission electron microscopy (TEM). However, due to their electron beam sensitive nature and heterogeneous size and structure, none of these approaches are capable of determining the true structure of individual protein aggregates in their native hydrated state.We are currently working on in situ liquid cell electron microscopy (LCEM) methods for imaging protein aggregates in their near-native hydrated state with nanometer scale spatial resolution [3]. While this approach allows for direct imaging of nanoscale samples in a thin ( ) liquid layer [4], radiation damage quickly deteriorates the tertiary and quaternary structure of protein aggregates [5,6]. Radiation damage is due mainly to oxidizing radicals created from electron beam induced radiolysis in the liquid layer [7,8]. In this talk, I will outline our recently developed experimental approaches to mitigate radiation damage and enable damage-free imaging of protein aggregate structure and other beam sensitive soft materials. These approaches include (1) the addition of radical scavengers [8] to selectively eliminate oxidizing radicals and (2) the use of advanced electron beam control during imaging to reduce the overall production of damaging radicals.Protein aggregates of bovine serum albumin (BSA) were prepared either by heat-induced or agitationinduced denaturation and aggregation of a 30 mg/mL monomer solution. Protein aggregates had sizes on the order of 50 -500 nm, determined by dynamic light scattering. LCEM sample chips coated with positively charged poly-L-lysine were used to capture protein aggregates through attractive electrostatic interactions. For these experiments, we utilized Protochips microwell chips for protein aggregate imaging, as they enable creating very thin (~100 nm) liquid layer that enable high spatial resolution imaging (Figure 1a). In some cases, protein aggregates were positively stained with 0.1 wt% uranyl acetate stain to enhance contrast (Figure 1b). The aggregates were imaged in both bright field TEM and STEM imaging modes, keeping total dose exposures below . Solutions of unaggregated BSA protein were observed to aggregate with repeated imaging, likely due to oxidative protein damage (Figure 2). Imaging experiments utilizing radical scavengers common...