Two series of self-assembled monolayers (SAMs) of -substituted alkanethiolates on gold were used to systematically examine the effects of varying substratum surface chemistry and energy on the attachment of two model organisms of interest to the study of marine biofouling, the bacterium Cobetia marina (formerly Halomonas marina) and zoospores of the alga Ulva linza (formerly Enteromorpha linza). SAMs were formed on gold-coated glass slides from solutions containing mixtures of methyl-and carboxylic acid-terminated alkanethiols and mixtures of methyl-and hydroxyl-terminated alkanethiols. C. marina attached in increasing numbers to SAMs with decreasing advancing water contact angles ( AW ), in accordance with equation-of-state models of colloidal attachment. Previous studies of Ulva zoospore attachment to a series of mixed methyl-and hydroxyl-terminated SAMs showed a similar correlation between substratum AW and zoospore attachment. When the hydrophilic component of the SAMs was changed to carboxylate, however, the profile of attachment of Ulva was significantly different, suggesting that a more complex model of interfacial energetics is required.Upon submersion in a nonsterile aqueous liquid, most surfaces become rapidly colonized by collections of bacteria and other microorganisms. These attached cells, along with extracellular material they produce and other organic compounds adsorbed to the surface, comprise a structure referred to as a biofilm (17). Biofilms are ubiquitous in natural aqueous milieus and are increasingly considered to represent a separate developmental form of microorganisms (29). Similarly, a number of macroorganisms, such as algae, exploit a unicellular form for attachment and colonization of surfaces. Surface coverage by both macro-and microorganisms, therefore, depends initially on the ability of single cells to adsorb and adhere to the attachment substratum.The tendency (driving force) for a microorganism to attach to a given surface is given by the free energy of adhesion (⌬G adh ), which can be expressed by the following equation as a thermodynamic energy balance between the interfacial energies between the substratum, the organism, and the surrounding liquid (1): ⌬G adh ϭ ␥ BS Ϫ ␥ BL Ϫ ␥ SL , where ␥ BS is the interfacial tension between the organism (e.g., a bacterium) and substratum, ␥ BL is the interfacial tension between the organism and the liquid, and ␥ SL is the interfacial tension between the substratum and the liquid.Experimental determination of the interfacial energy values for the above equation is controversial and has led to three different, yet complementary, models (8). All rely on estimation of interfacial energies by contact angles as indicated by Young's equation (2), which states that ␥ SV (the vapor interfacial tensions [surface tensions] of the substratum) is related to the contact angle () formed by a drop of liquid on the substratum such that ␥ SV ϭ ␥ SL ϩ ␥ LV cos, where ␥ SL is the interfacial tension between the surface and the liquid and ␥ LV is the interfac...