“…In addition to the uncertainties associated with the droplet-size distribution, the sedimentation and evaporation processes of saliva droplets expelled from the mouth or nose are affected by a variety of different physical and chemical effects, which make modelling of airborne virus transmission even more complex. These effects include the evaporation-induced cooling of the droplet [ 28 , [44] , [45] , [46] ], airflows and ventilation effects for large droplets [ 21 , 25 , 47 ], finite evaporation-rate effects for small droplets [ 48 , 49 ], solar irradiation effect [ 50 , 51 ], and solute-induced effects, including water vapor-pressure lowering [ 52 , 53 ], local solute-concentration gradients [ [54] , [55] , [56] ], crust formation due to solute crystallization [ 54 , 57 , 58 ], liquid−liquid phase separation [ [59] , [60] , [61] ], and a possible solute-concentration dependence of the viscosity [ 62 , 63 ] and the water-diffusion coefficient [ 63 , 64 ] inside the droplet. These effects are themselves dominated by various parameters, such as the initial size of the droplet, the type and the initial volume fraction of solutes, the ambient temperature [ 47 , 50 , 65 , 66 ], the relative humidity [ 47 , 65 , [67] , [68] , [69] , [70] , [71] ], non-ideal effects due to inter-particle interactions inside the droplet [ 72 , 73 ], the internal morphology of droplets [ 59 , 74 , 75 ], and the initial height at which droplets are released into the air.…”