than wet the surface [10][11][12][13][14][15][16][17][18][19][20][21][22][23] due to the high surface tension of water, the low surface energy of the substrate, and the minimal adhesion between water and the surface. The low surface energy and minimal adhesion can be attributed to multiscale features, ranging from micro to nano, [ 11 ] that trap air pockets between the surface and water, allowing the water droplet to only contact the peaks of the multiscale structures. The multiscale features can be highly patterned (homogeneous) or random (heterogeneous) but need to be multi-to nanoscale to trap air between the surface and fl uid. Such SH surfaces have been used for anti-fouling applications and drug delivery. [ 20,[24][25][26][27] When air is trapped between water and the surface, the surface is in the Cassie-Baxter regime, [ 10 ] and the water droplet's adhesion to the surface is poor. A droplet in the Cassie-Baxter regime can transition to the Wenzel regime (no air pockets and strong adhesion to the surface) [ 28 ] when the balance of forces is disrupted. [ 29 ] Pressure can disrupt this balance and change a water droplet from balancing on the peaks (Cassie) to sinking into the multiscale structures (Wenzel). [30][31][32][33] A water droplet can naturally transition from Cassie to Wenzel due to a change in internal droplet pressure, which can be quantifi ed bywhere γ is the surface tension of the fl uid, and R is the radius of the droplet. [ 30,34 ] Evaporation of a droplet can cause the Cassie to Wenzel transition due to the decrease in volume and increase in internal pressure. When a droplet of fl uid evaporates into the atmosphere, the balance of forces at the air-liquid interface constantly increases the droplet's surface tension and applies an inward force at the droplet's contact line (air-liquid-solid interface). [ 35 ] On a SH surface, the droplet's inward pulling force is greater than the droplet's adhesion to the surface, and the droplet's contact line continually moves inward, creating a smaller footprint and contact diameter (CD) for the droplet, [36][37][38][39][40][41] as shown in Figure 1 . Eventually, the droplet collapses to its fi nal footprint when the internal Laplace pressure overcomes the upward force from the air pockets, [ 30,31 ] and fl uid will stay pinned at this reduced contact area until evaporation is complete. This reduced contact area contains the content of the droplet with the molecules concentrated only on a small footprint.Protein in urine can be detected using a simple colorimetric output by evaporating droplets on a superhydrophobic (SH) surface. Evaporation on a SH surface allows fl uid to dramatically concentrate; the weak surface adhesion allows the droplet of fl uid to constantly decrease its footprint area and contact diameter. On a SH surface, pure water completely evaporates. Molecules in solution, however, are confi ned to a footprint that is 8.5 times smaller than the original and are greatly concentrated. By concentrating molecules, a 160 times improved detectio...