OUTFLOW VII The Aqueous Circulation The aqueous humor is thought to be secreted by the epithelium of the ciliary body. That this may not be the only structure from which aqueous originates was suggested to me some years ago when I took care of a patient who had sustained blunt trauma to the globe of his right eye. When one looked at the eye with the slit lamp, one saw what appeared to be lens and iris lying under the nasal conjunctiva. The anterior chamber was deep and clear. The iris and lens were absent. The vitreous face was intact. On indirect ophthalmoscopy with scleral indentation one could see a temporal retinal detachment. Anterior to the ora serrata, no ciliary body structures could be identified. I inferred, therefore, that the ciliary body had been avulsed together with the lens and the iris. Initially the intraocular pressure was normal, but over a period of months the tension rose to the high thirties and proved, as a matter of fact, rather intractable to treatment. I concluded that in this patient, at least, the retina must have contributed significantly to the production of aqueous. Whatever its origin, the phenomenon of pupillary block leaves no question that the aqueous flows from the posterior into the anterior chamber. On occasion when one makes a laser iridotomy, one sees a jet of aqueous come forward carrying its particles of pigment. Particles of pigment or cells, whenever they can be identified in the anterior chamber aqueous, are seen to rise in the posterior part of the chamber and descend near its corneal boundary, indicating that the fluid in the chamber is in continuing motion. rising by convection as it is warmed by the iris, and similarly falling as it is cooled by the cornea. That the aqueous leaves the eye through structures in the anterior chamber angle may be inferred from the circumstance that in the great majority of eyes where gonioscopy shows the anterior angle to be closed, glaucoma supervenes, and the pressure rises. Gonioscopy also suggests that a substantial proportion of the outflow occurs in an area of the angle just posterior to Schwalbe's line. One may infer as much from the observation that angle closure does not provoke glaucoma until the anterior half of the ring that extends from the scleral spur to Schwalbes line is occluded, so that, if one can see scleral spur one may say with confidence that the filtering portion of the angle is not occluded. Occasionally when the intraocular pressure is low, one sees just anterior to the scleral spur a thin reddish band. This is thought to be blood in Schlemm's canal and quickly disappears if one increases the intraocular pressure as, for example, by pressing against the sclera with ones finger. On the surface of the globe one may on occasion be able to identify the aqueous veins that collect the aqueous once it has traversed the sclera in the collector channels. The pressure in the episcleral veins is approximately 9 mm Hg which corresponds to the pressure at the distal end of the capillary as it is cited in standard physiology texts. Thus the pressure gradient across the outflow channels of the eye ranges from two or three to perhaps 12 mm Hg, is 6mm, plus or minus 5 mm Hg. That is as much as one can observe through the slit lamp and with the ophthalmoscope. The simple operative maneuvre of paracentesis, where a narrow, oblique incision is made through the cornea into the anterior chamber with a thin, needle-like knife, serves to demonstrate, in the absence of pupillary block, that the anterior chamber is under the same pressure as the posterior chamber, and serve to demonstrate in the presence of pupillary block that the direction of flow is from the posterior chamber anterior through the pupil. Where resistance to flow is defined as that characteristic of a conduit which limits the flow that may be produced by any given pressure. Algebraically, one stipulates that resistance shall equal the pressure divided by the flow. In this equation, then, when pressure is treated as the independent variable, an increase in pressure is attributable either to an increase in resistance or to an increase in flow. Surely this is the case where the angle is grossly occluded as in angle closure and synechial glaucoma. The evidence that open angle glaucoma is also attributable to an increase in outflow resistance is almost as great. Hypersecretion glaucoma, if it occurs at all, must be very rare. What is in this context of greater importance is the interpretations of fluctuations in intraocular pressure, given the existence of glaucoma. The traditional explanation is that such fluctuations reflect not variations in the severity of the glaucoma, i.e., one assumes that the resistance to outflow remains constant, but that they reflect changes in the amount of aqueous produced. The evidence for this assumption is slight, for one cannot, in general, reproduce such pressure fluctuations by giving a patient a water load by mouth, concerning which one might infer wth some certainty that it enhances the production of aqueous. The salient issue here is whether or not, or to what extent, glaucoma represents a fixed anatomic deformation of the outflow channels and to what extent, if any it represents an impairment of a control mechanism that maintains the resistance to outflow at physiologic levels. Before addressing this question, we must take another look at the anatomy of thr outflow system, necessarily, through the microscope. The measurement of outflow resistance both in the laboratory by perfusion techniques and in the clinic by tonography leaves little room for doubt that the cause of increased pressure in the vast majority of glaucomas results from an increased resistance. * * * * *

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