T h e cytoplasm of the ocular lens is a concentrated protein solution that normally remains transparent. T h e conditions for cytoplasmic transparency are described in a phase diagram that has been determined by two separate experimental methods.'.' Under normal physiological conditions the cytoplasm exists as a single transparent phase. A decrease in temperature below the phase separation temperature T, produces two coexisting phases and opacity.' :' Normally, T, is well below body temperature, but during cataract formation T, increases toward body temp e r a t~r e .~-'It is well known that the value of the cytoplasmic T, is determined by the molecular interactions between proteins and solvent constituents of lens cytoplasm that are responsible for transparent cytoplasmic structure.8 " T h e nature of these interactions has been investigated by measuring the effects of changes in ionic strength, pH, or other conditions on T,. In this report, the effects of H-bonding solvents were evaluated on the T,. of lens cells.We determined d T , / d C for several solvents with different H-bonding characteristics. T h e solvents, including methanol, D 2 0 , and several glycols, were selected on the basis of ( 1 ) the strength of the H bonds formed in solution, which were readily characterized by the value of the boiling points and heats of ( 2 ) previous work that has shown t h a t MeOH, D,O, and glycols change I , and ( 3 ) finding that these particular solvents were easily diffused into the calf lens. We observed that the change in T,, d T , / d C , was directly proportional to the boiling point and heat of vaporization of the solvents. While many factors may contribute to phase behavior of lens cytoplasm, these empirical findings indicate the importance of' hydrogen bonds. ( Woburn, M A ) . The solvents were diluted with phosphate buffer so that the final buffer concentration was 0.154 M , which maintained the p H at 7.0. Calf lenses were dissected out of fresh calf eyes a n d placed in 100 m L of each test solution to soak for approximately 16 h at 4°C until the Tc equilibrated t o a constant value. It should be noted that returning the lens to buffer solution without any solvent allowed T, t o return to normal. It was interpreted t h a t this decrease and increase in T, was due t o diffusion of medium into a n d out of the lens. In the case of D20, proton NMR spectroscopy was used to measure the diffusion of D 2 0 into lens c y t~p l a s m . '~ After soaking the lens in the solvent, each lens was placed in a cuvette filled with silicone oil (Dow Corning, Midland, M I ) . The cuvette was mounted in the path of a 5 mW He-Ne LASER ( Melles-Griot, San Marcos, CA) beam. T h e beam was directed through the center of the lens onto a PIN-1OD photodiode (United Detector Technologies, Culver City, CA) , which measured the transmitted intensity of the LASER beam. T h e photocurrent produced in the photodiode was measured using a Keithley multimeter ( Keithley Instrument?, Cleveland, OH) and recorded using a Houston Instruments c...