By combining the experimental Gfd with the calculated humidified 𝜃 2 , we relate the degree of restructuring to the amount of aqueous condensate in Fig. . Like in Fig. , the points form two clusters: (1) TEG and (2) GA, AN, and SA. Here TEG shows the largest filling angle and the most significant decrease in Gfd. Despite its lowest hygroscopicity, TEG produced the most condensate under dry and humid conditions because of the relatively low contact angles of its neat liquid and aqueous solution. GA experienced a deliquescence transition at 85% RH, absorbing a larger than TEG amount of water, but producing less restructuring because at low RH it condensed in a smaller amount due to both a higher contact angle (Supplementary Table ) and a lower vapor saturation (Supplementary section 6). In the case of AN, the small initial volume increased significantly after humidification due the high hygroscopicity of this chemical, resulting in 𝜃 2 and Gfd comparable to those of GA. The filling angle of SA increased significantly during humidification because of its high hygroscopicity. Despite the small amount, SA caused comparable to GA restructuring upon humidification that may be related to the higher surface tension of SA, resulting in stronger capillary forces. Furthermore, SA condensed not only in the junctions but also over the entire particle surface. Hence, after humidification some of the aqueous SA condensate could be transported into the junctions, resulting in a larger filling angle than that predicted by our model. During this transport, the high contact angle of aqueous SA could have induced dynamic effects related to the condensate contact line pinning, producing larger momentary forces, which enhanced restructuring.