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1 From the Departments of Ophthalmology and 3 Neurology, University of California, Los Angeles; and 2 Department of Ophthalmology, Okayama University Medical School, Okayama, Japan.
| Abstract |
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METHODS. Five human orbits, ages 33 weeks gestation to 93 years, were imaged intact by magnetic resonance (MRI), serially sectioned at 10 µm thickness, and stained for collagen, elastin, and smooth muscle (SM). With MRI used as a reference, digital images of sections were geometrically corrected for shrinkage and processing deformations, and normalized to standard normal adult globe diameter. EOM pulleys, interconnections, suspensory tissues, and entheses were quantitatively analyzed for collagen, elastin, and SM thickness and density.
RESULTS. Rectus and inferior oblique pulleys had uniform structural features in all specimens, comprising a dense EOM encirclement by collagen 1 to 2 mm thick. Elastin distribution varied, but was greatest in the orbital suspension of the medial rectus pulley and in a band from it to the inferior rectus pulley. This region corresponded to maximum SM density. Structural features of pulleys, intercouplings, and entheses were similar among specimens. The major mechanical couplings to the osseous orbit were near the medial and lateral rectus pulleys.
CONCLUSIONS. Quantitative analysis of structure and composition of EOM pulleys and their suspensions is consistent with in vivo MRI observations showing discrete inflections in EOM paths that shift predictably with gaze. Focal SM distributions in the suspensions suggest distinct roles in stiffening as well as shifting rectus pulleys.
| Introduction |
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Modern interest in orbital connective tissues was reawakened by the demands of biomechanical modeling of binocular alignment. Failures of initial attempts to compute ocular position based on static force equilibrium10 clarified the critical importance of EOM path determinants that had to be assumed arbitrarily in initial binocular models.11 The need for EOM path data motivated early radiographic studies in monkeys12 and humans,13 showing absence of obvious EOM sideslip over the globe during ocular rotations. A decade ago Miller14 used relatively low-resolution MRI with three-dimensional reconstruction to demonstrate the stability of rectus EOM belly paths throughout the oculomotor range. The further demonstration by MRI that EOM paths are little affected by large surgical transpositions of their tendons provided strong evidence for EOM path constraint by pulleys coupled to the orbit.15 16
Recent histologic studies have demonstrated that each rectus pulley consists of an encircling ring of collagen located near the globe equator in Tenon fascia,17 coupled to the orbital wall, adjacent EOMs, and equatorial Tenon fascia by slinglike bands containing densely woven collagen,18 elastin, and SM.17 19 Pulleys inflect rectus and inferior oblique (IO) EOM paths in the same manner that the trochlea inflects the path of the superior oblique (SO) tendon. The coronal plane location of each rectus pulley has been shown by MRI to be highly uniform in normal subjects.20 The global layer of each rectus EOM, containing about half of all EOM fibers,21 passes through the pulley and becomes contiguous with tendon to insert on the globe. The orbital layer, containing the remaining half of the EOM fibers, inserts on the pulley, not on the globe.21 22
The mechanical properties of pulleys are critical for ocular kinematics, the rotational properties of the eye. Rotations of any three-dimensional object are not mathematically commutativethat is, final eye orientation depends on the order of rotations.23 This vexing conundrum regarding the neural control of ocular motility is avoided if the ocular rotational axis shifts by half of the change in ocular orientation in relation to a primary position, for under these conditions the effect of noncommutativity becomes negligible.24 This half angle behavior is equivalent to Listings law of ocular torsion25 and is faithfully observed when the head is upright and stationary.26 Pulleys appear important to Listings law and commutativity.
Precise mechanical shifts in rectus pulley positions are consistent with commutativity22 and have been quantitatively confirmed in humans by MRI in tertiary gaze positions.27 The coordinated control postulate of the active pulley hypothesis states that, in an oculocentric coordinate system, rectus pulley location is maintained in a constant relationship with the EOMs scleral insertion, so that the distance from the pulley to globe center is equal to the distance from globe center to insertion. By this relationship, the velocity vector produced by contraction of the EOMs shifts by half of the change in ocular orientation from primary position. The IO muscle also has a pulley, mechanically coupled to the inferior rectus (IR) pulley,28 that moves anteroposteriorly by half the travel of the IR pulley to maintain an IR action perpendicular to the half-angle behavior of the rectus EOMs.29 30 During convergence, rectus pulleys may systematically shift in the coronal plane to meet visual demands, probably under the influence of the orbital layers of the oblique EOMs31 32 and SM in the medial orbit.19
These observations indicate a far greater degree of complexity in EOM function than previously suspected, with mutual mechanical interactions among EOMs in the periphery replacing the notion of a neural final common pathway.33 Interpretation of neural control of binocular coordination will require an accurate computational simulation of the mechanics of the EOMs and associated connective tissues. Although existing computational models of orbital biomechanics now incorporate pulleys,34 35 these are nonphysiologic regarding their essentially fixed orbital suspensions and absence of realistic gaze-related movements. Physiologic models of EOM action must incorporate a quantitative description of pulley structure. The present study was performed to determine quantitatively the composition and relative abundance of connective tissue components in the human EOM pulley system.
| Methods |
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Magnetic Resonance Imaging
The four fixed heads and the 93-year-old orbit were imaged by MRI, with dual 3-in. phased array surface coils in a 1.5-T scanner (Signa; General Electric, Milwaukee, WI). Multiple contiguous quasicoronal MRIs, 2 or 3 mm in thickness, were then obtained with a T1 pulse sequence encompassing a 256 x 256 matrix over a 4- or 5-cm2 field of view, providing a pixel resolution of 156 or 195 µm, respectively. To improve the signal-to-noise ratio at these high resolutions, four to nine excitations were performed. Digital MRIs were transferred to computers (Macintosh; Apple Computer, Cupertino, CA), converted into eight-bit tagged image file format (TIFF) by locally developed software, and quantified by NIH Image (W. Rasband, National Institutes of Health; available by file transfer protocol from zippy.nimh.nih.gov or on floppy disc from NTIS Springfield, VA; part number PB95500195GEI).
Histologic Processing
The four orbits fixed in situ were then removed in continuity with the eyelids and orbital bones. The orbital rims and walls were carefully thinned under magnification by using a high-speed drill and rongeurs before decalcification for 24 hours at room temperature in 0.003 M EDTA and 1.35 N HCl.22
Formalin-fixed tissues were dehydrated in graded solutions of alcohol and chloroform or xylenes, embedded in paraffin, and serially sectioned in the coronal plane at 10-µm thickness by disposable metal blades on a microtome (HM325; Carl Zeiss, Thornwood, NY), as previously described.17
19
22
This produced 2800 to 4800 sections per orbit, depending on the orbits size. Alternate sets of five contiguous sections were saved and mounted on 50 x 75 mm gelatin-coated glass slides. Masson trichrome stain was used to show muscle and collagen, and van Gieson stain to show elastin.36
As previously described,19
SM was confirmed using a monoclonal mouse antibody to human SM
-actin, which was visualized with an avidin-biotin complex (ABC) kit with blue chromogen (Alkaline Phosphatase Kit 3; Vector Laboratories, Burlingame, CA). To maximize chromatic uniformity, sections were stained with Masson trichrome and van Gieson stains in batches of 25 to 50 slides, and, for human SM
-actin, in batches of five slides, with fresh reagents used for each specimen.
Analysis
Whole stained histologic sections were imaged in color with one of two digital cameras equipped with a 50-mm fixed or variable macro lens (Nikon, Tokyo, Japan). One camera (Leaf Lumina; ScyTech, Bedford, MA) had a resolution of 3400 x 2800 pixels, and the other (D1X; Nikon) had a resolution of 3008 x 1960 pixels in 24-bit color. Images were spatially calibrated by imaging a 1-mm rectilinear grid affixed to a glass slide before and after each session of histologic imaging. Higher-power images were obtained by mounting either digital camera on a microscope (BH-2; Olympus, Lake Success, NY).
Coronal MRIs of each specimen were used as the spatial standard to correct histologic images for shrinkage and nonuniform distortions introduced by later processing. For this purpose, one coronal plane MRI was selected for each specimen from the level of the globe equator, so that it included the rectus EOMs and pulleys (Fig. 1 , top left).17 A more anterior MRI plane would have better intersected the densest pulley regions, but the flatness of EOM tendons and the density of connective tissue make it difficult to distinguish contours required to judge EOM or pulley position in the image plane.16 First, MRIs in NIH Image were absolutely scaled, based on the calibrated MRI field of view. Then, the MRI and histologic images (Fig. 1 , center left) were superimposed at partial transparency in image management software (Photoshop, ver. 5.5; Adobe Systems, San Jose, CA) and rotated to identical orientations (Fig. 1 , bottom left). To correct for shrinkage, the histologic images were then differentially scaled in the horizontal and vertical directions so that the orbital walls superimposed on the MRI (Fig. 1 , bottom left). This procedure assumes that dimensional distortion produced by shrinkage or stretching affects the entire section similarly in the same direction, but allows this distortion to be different in orthogonal directions. For example, sections tended to stretch in the dimension parallel to the motion of the microtome knife, but did not do so perpendicular to this direction. Specimens were not uniformly oriented in relation to the direction of knife travel, and shrinkage was therefore represented for the two arbitrary orthogonal directions required for superimposition of histologic images on MRIs. Shrinkage in orthogonal directions ranged from 30% x 40% (smaller x larger dimension) in the exenterated specimen to 10% x 15% in specimens processed with orbital bones intact, with mean (±SD) shrinkage of 20% ± 9% x 27% ± 7%. All dimensional measurements reported herein were performed with images individually corrected for bidirectional shrinkage distortions.
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Sections stained with Masson trichrome were used to measure collagen density and pulley thickness. Densitometry was performed digitally using the color range command in the image management software (Photoshop; Adobe). Collagen, constituting the most abundant and anatomically defining constituent of pulleys, stains blue with Masson trichrome. Most pulleys and connective tissue bands consist of laminae of collagen separated by voids that probably contain adipose tissue. The relative proportion of pulley or band thickness that contained collagen, as opposed to void, was considered to be collagen density. Collagen density was measured in the same sections stained with Masson trichrome and at the same low magnification used for measurement of pulley thickness. Density of the less-abundant microscopic elastin fibrils, which stain dark black with van Gieson elastin stain (Fig. 2B)
, was determined from high-power digital micrographs of adjacent sections. SM density was determined from high-power digital micrographs of adjacent sections immunostained with a blue chromogen for human SM
-actin, which is highly specific for SM (Fig. 2C)
. For each connective tissue constituent, the selected color was converted to grayscale. Grayscale images of specific tissue constituents were imported into NIH Image, and the density function was applied with the use of a consistent threshold. Density (percentage) was calculated as pixels exceeding threshold divided by grayscale pixels. Use of a threshold is unavoidable for quantitative analysis, because chromatic variation among specimens is inevitable, even with large-scale histologic processing techniques such as those used in the current study. Use of a threshold that appears reasonable in comparison with the original color images and is qualitatively consistent among specimens minimizes the effects of threshold selection. Identifiable blood vessels were excluded from areas of SM measurement, because vascular SM is not relevant to mechanical measurements. We estimated total connective tissue content to be the average density multiplied by average thickness of the structure under consideration.
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The anteroposterior extent of the MRIR SM band was measured in each specimen, as judged by the maintenance of the band structure in serial 10-µm-thick sections. Data on thickness and extent in each specimen were normalized to that specimens globe diameter compared with a normal globe diameter in vivo of 24.3 mm obtained by MRI.37 Enthesis dimensions were also measured. The SO pulleys (trochleas) in two specimens (57 and 93 years old) were not measured because of damage sustained during specimen preparation.
| Results |
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-actin (Figs. 2C
3H)
. The image plane in Figure 2
intersects a dense region of the orbital aspect of the MR pulley, showing a dense encirclement by collagen laminae having only sparse voids that presumably contained fat before elution in processing. More posterior sections demonstrated a thicker ring on the global aspect of the MR pulley, but the global aspect was not as thick as the orbital. Black elastin fibrils were embedded in the collagen of the pulley ring and in suspensory bands running superiorly and inferiorly (Figs. 2B
3)
. SM, appearing blue due to immunoreactivity for human SM
-actin, was abundant on the orbital surface of the MR pulley (Figs. 2C
3)
. The orbital layers of the rectus EOMs inserted into the collagen of each of their respective pulleys in every specimen. The morphology of the MR pulley was identical in all specimens except the fetal one.
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Quantitative analysis recognized that, because of the intersection of coronal histologic sections with the three-dimensional structure of the orbital connective tissues, the coronal histologic planes would not exactly coincide with the plane of each pulley ring. Total pulley thickness for each EOM was measured separately for the orbital and global portions, in each case from the coronal section showing the most complete development of that portion. The tissue bands interconnecting the pulleys were measured from sections showing maximal development of the two pulleys under consideration. In each case, measurements included all connective tissue constituents, plus intervening spaces that had presumably contained fat (Fig. 4) . The thickness, collagen, and elastin contents in the three specimens aged 17 months, 4 years, and 57 years were similar and were averaged to represent data from the predominant part of the postnatal human age range, whereas quantitative data from the fetal and 93-year-old specimens were considered separately. Pulley thickness tended to be greater on the orbital than the global aspect (Fig. 4) . For the midage-range specimens, mean pulley thickness of the orbital aspect ranged from 1.0 to 2.25 mm, whereas global aspect thickness ranged from 0.5 to 1.75 mm. Pulley thickness was modestly lower in the fetal and 93-year-old specimens. Interconnections among pulleys ranged in mean thickness from 1.25 mm for the MRSR band to 2.75 mm for the MRIR band. Similar to the thickness of the pulleys, interconnecting band thickness was generally lower in the fetal and 93-year-old specimens than in the other specimens. The SO sheaths were thinner than in the remaining EOMs.
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-actin. Recognizable blood vessels were avoided in the quantitative evaluations, but a few small vessels may have been included if their lumina could not be identified. There were two types of SM distributions (Fig. 3)
. Large SM bundles averaged 30 to 40 µm in diameter and were mainly located in a band from the superior border of the MR to the nasal border of the IR. These large bundles were apparently cut transversely by the coronal sections. Small SM bundles averaging 10 µm in diameter were located on the global surface of the large cell bundles, but formed a band having greater length, extending from the nasal border of the SR to the nasal border of the IR. The small SM bundles appeared to have been cut more tangentially, so that their long axes approximated the coronal plane. Because it formed a distinct structure (Figs. 3B
3E
3H)
, the SM band at the MR pulley was not included in the pulleys thickness, but the SM bundles at the MRIR band were included in the pulleys thickness, because the bundles were intrinsic within the band (Figs. 3C
3F
3I)
. For quantitative analysis, large and small SM bundle distributions were lumped together as a single structure. The normalized anteroposterior extent of the MRIR SM band of the five specimens averaged 4.74 ± 0.82 mm (±SE; range, 2.776.68 mm). The LRSR band, as well as other connective tissue bands, had few and widely scattered small SM cells. The MRSR band and the LRSR band had insufficient SM for quantitative measurement by
-actin immunoreactivity. The lateral levator aponeurosis (LLA) has been described to be a connective tissue condensation extending between the superior border of the LR pulley and the lateral border of the levator palpebral superioris (LPS).19 Careful examination of the our high-quality specimens suggested the need for revision of this description. More correctly, the LLA should be considered to be a lateral expansion of the LPS tendon, running inferolaterally and partially through the lacrimal gland to insert on the orbital bone at the lateral canthus. The muscular tissues of the LLA began superiorly as a lateral extension of striated muscle from the LPS in the medial half, contiguous with a particularly dense band of SM in the lateral half of the LLA. The SM in the LLA did not appear to be directly coupled to the oculorotary EOMs. However, another SM distribution, distinct from the LRSR band, extended from a lateral expanse of striated muscle fibers from the levator and continued laterally and inferiorly to the LR pulley. This distribution, forming part of what was described by Müller as the "peribulbar muscle,"39 40 was present anterior to the equator.
With both large and small bundles included, maximum SM thickness near the MR pulley or MRIR band ranged from 0.2 to 1.4 mm (Fig. 8) . Total SM content was taken to be the product of band thickness and SM density, thus having the dimension of mm (Fig. 9) . The SM content at the MR pulley in the region of the medial enthesis ranged from 0.01 to 0.13 mm.
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| Discussion |
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Earlier studies of orbital anatomy were hampered by difficulties in removing the delicate, elastic, soft tissues from the supporting orbital bones. Removal of the soft tissues by dissection almost inevitably results in damage, particularly to the entheses, where adhesion to bone is most secure. In the current study, we used specimens that, for the most part, had been processed in continuity with the orbital bones to clarify the relationship between the pulley system and its bony support, as depicted in the schematic frontal view in Figure 10 . This schematic depicts only the thick and presumably mechanically significant connective tissue structures, omitting the thinner anterior and posterior pulley slings. Figure 10 also depicts structures that generally do not all lie in the same plane. Contrary to the depiction in an earlier schematic, the IR and SR pulleys were found not to have direct mechanical coupling to an enthesis on the adjacent orbital bone. The rectus pulley system is mechanically coupled to the anterior orbital bones by heavy connective tissues nasally and temporally. The medial enthesis corresponds to the medial canthal tendon region where the lids are anchored nasally, whereas the lateral enthesis is several millimeters posterior to the lateral canthal tendon at the zygomatic tubercle. The absence of direct enthesis of the vertical rectus pulleys to the bone of the adjacent orbital rim regions is a necessary consequence of the mobility of the superior and inferior eyelids, which move through these regions within only loose connective tissues. The vertical rectus pulleys are thus indirectly coupled to the medial and lateral entheses by the intercouplings between the rectus pulleys. Further stability is provided by the SO tendon emerging from its rigid trochlea and by the sheath and belly of the IO muscle, which originates from anterior orbital bone.
Past descriptions suggested correctly that the orbital connective tissue system supports and protects the globe, but such descriptions emphasized a major role for the "check ligaments" in limiting and dampening ocular movements.38 The elasticity of the check ligaments was believed to be important in graduating the action of EOM contraction to ensure smooth ocular rotations without jolting the globe.38 The active-pulley hypothesis,22 32 as well as the current quantitative anatomic findings, support quite a different interpretation of the check ligamentselastic suspensions of the pulley system that actively regulates the direction of EOM force to control ocular kinematics. In view of the misleading functional connotation, the term check ligament should probably be abandoned.
The current report also makes a novel distinction between the LLA and the LRSR band. The LLA, connecting the lateral expansion of the LPS to the anterior bony orbit while partially traversing the lacrimal gland, appears to be mainly a suspension for the LPS in relationship to the Whitnall ligament. The LLA would only indirectly stabilize the SR pulley by mechanical coupling of the LPS and SR. The lateral half of the LLA contains abundant SM, whereas the medial half contains striated muscle contiguous with the LPS. In contrast, the LRSR band extends directly between the involved pulleys and contains only a small amount of SM in small bundles. The LRSR band is equivalent to the MRSR band in thickness and collagen content, but probably has lower stiffness, because the elastin content of the LRSR band is about one fourth of the MRSR band. Elastin has the property of reversible extensibility44 that probably confers elastic stiffness on pulley suspensory tissues.
The orbital aspect of each rectus pulley had more and thicker collagen than the global aspect. Elastin content in the orbital aspect was also richer than in the global aspect of each pulley. The more extensive and presumably stiffer structure of orbital aspects of rectus pulleys is likely to be related to concentration at those sites of stress associated with sharp EOM path inflections in secondary and tertiary gaze positions.27 37 Such inflections, which move in the anteroposterior direction during contraction of orbital layer fibers inserting on the pulleys,22 require support from pulley suspensions to the entheses to maintain their considerable resistance to sideslip in the coronal direction.
Although general features of pulleys were preserved in the 93-year-old specimen, there was also qualitative evidence of age-related degeneration. Elastin fibers in pulley showed clumping and shredding. The change may account for the observation that total elastin thickness in the 93-year-old specimen exceeded that of the other specimens (Fig. 6) . There also was obvious qualitative atrophy of collagen fibers in the 93-year-old specimen, associated with reduced total collagen thickness (Fig. 5) . Degenerative connective tissue changes in aging correlate with limited ocular ductions in the elderly,45 and with MRI evidence of downward displacement of horizontal rectus pulley positions.46 Asymmetrical occurrence of such changes in the two orbits may be expected to cause strabismus.46
SM has long been recognized in the orbital connective tissues,5 19 39 but its role has been unclear. Demer et al.19 described an intricate innervation pattern, including rich sympathetic, parasympathetic, and nitroxidergic innervation to pulley SM, suggesting the following possible roles for pulley SM: to maintain uniform stiffness in the pulley suspensions; to accomplish slow, adaptive adjustments in pulley locations as are necessary to maintain binocular alignment over a lifetime; and to fulfill a possible dynamic role in eye movements. The latter suggestion is consistent with new observations of excyclorotation of the four-rectus pulley array during convergence.31 The especially dense peribulbar SM between the IR and MR pulleys seems anatomically suited to accomplish the observed nasal shifting of the IR pulley in convergence.
Mathematical models of EOMs have led to much insight into EOM function, and have motivated significant new lines of inquiry.47 However, even the most comprehensive currently available models34 fail to account for important features such as large gaze-related shifts in rectus pulley positions.27 Quantitative data are now available for each of the four rectus EOMs, showing the number of global layer fibers inserting on the scleral tendon and the number of orbital layer fibers inserting on the pulley.21 More complete models may incorporate this and the current quantitative data on pulley structure and interconnections in computational implementations of these critical structures. The values for collagen and elastin content reported here provide a basis for reasonable estimates of relative stiffness of pulley suspensions and interconnections. Potential for pulley shift due to the actions of striated EOMs may be estimated from connective tissue and SM content in the specific structures described herein. A realistic computational model of EOM and orbital connective tissue mechanics would be of general value in understanding normal and pathologic behavior of ocular movements and binocular alignment.
| Acknowledgements |
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| Footnotes |
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Submitted for publication December 19, 2001; revised May 1, 2002; accepted May 23, 2002.
Commercial relationships policy: N.
The publication costs of this article were defrayed in part by page charge payment. This article must therefore be marked "advertisement" in accordance with 18 U.S.C.
1734 solely to indicate this fact.
Corresponding author: Joseph L. Demer, Jules Stein Eye Institute, 100 Stein Plaza, UCLA, Los Angeles, CA 90095-7002; jld{at}ucla.edu.
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