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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Copyright 2006, Ernst Jochen Meyer