The intra- and extracellular fluid flow patterns, such as those represented in Figure 1A of our Point article are difficult to measure experimentally, because the extracellular space is very small and the intracellular water flow is thought to be very slow. From the model, we have predicted intracellular water flow velocity in the inner cortex to be ∼1.7 × 10−3 μm/s. The flow velocity in the extracellular compartment (which is approximately 400 times smaller than the intracellular compartment) would have to be 400 times faster to preserve the overall steady state lens volume.
Because the relative fluid flows in the intra- and extracellular spaces are vastly different, the movement of a tracer molecule in the lens would depend on whether it is localized extracellularly or whether (like the fluorescent dye referred to in Fig. 1 of the Counterpoint article) it is injected intracellularly. We predict that an intracellularly injected tracer molecule about the size of a Na+ ion, but which is uncharged, would be freely carried by convection through lens gap junction channels and would not be affected by voltage gradients within the lens. In this optimal circumstance, 1 hour after injection, the center of the diffusion pattern would be moved by the intracellular fluid flow only approximately 6 μm, or approximately three cell widths. Because dyes are larger than ions and most are charged, and because the effective mobility of a dye in moving between lens fibers is greatly reduced over that in free solution, an estimate of 6 μm in 100 hours is a more realistic estimate of their flow in the intracellular compartment. For well-coupled cells like lens fibers, the movement of a gap-junction–permeable dye from its site of intracellular injection into the surrounding cells is detectable within seconds. Thus, the relatively rapid spread of an intracellularly injected fluorescent tracer dye due to diffusion would mask any small shift due to water flow or voltage gradients. If one artificially created a large diffusion gradient for any permeant molecule, that molecule would diffuse down its gradient at a rate much faster than transfer at steady state by the lens circulation.
A similar argument pertains to NMR imaging of water flow in which an isolated lens is immersed in heavy water,
1 creating a large gradient for diffusion of heavy water into the lens. It is the small perturbations from equilibrium that create the lens circulation. It therefore follows that if one wants to study the lens circulation, large external perturbations must be avoided, and the steady state properties must be the focus. In modeling fluxes in the lens, we have invoked the circulation only in the steady state, when solutes and solvent are near equilibrium. Our measurements of standing voltage gradients, Na
+ concentration gradients, and Ca
2+ concentration gradients
2 and our more recent studies of hydrostatic pressure gradients (Mathias RT, et al.
IOVS 2010;51:ARVO E-Abstract 3459) and MRI-based water tensor measurements
3 were all conducted in the steady state lens.