The First Quarter of This Century
The Middle of This Century
The 1970's Surge in Interest
After the Surge
Summary
The Pressure Theory
Superficial Observations
The Osmotic Pressure Hypothesis
Hydrostatic Pressure Measurements
Summary
The Proteolytic Enzyme Theory
The Earlier Studies
The Initial Enzyme Assays
Intrafollicular Injections of Proteases
Change in Follicular Distensibility
Efforts to Measure Collagenase
Summary
FUNCTIONAL ANATOMY OF THE OVARIAN FOLLICLE
General Morphology
Surface Epithelium
General Features
Cytoplasmic Granules
Polymorphous Nuclei
Scanning View of follicular Apex
Tunica Albuginea
General Features
The Collagen Matrix
Multivesicular Structures of Follicular Fibroblasts
Theca Externa
General Features
Thecal Fibroblasts
Ovulatory Changes in the Thecal Connective Tissue
Theca Interna
General Features
Steroid Synthesis
Vascular System
Granulosa Layer
General Features
Granulosa Gap Junctions
Other Anatomical Considerations
Follicular Fluid
Innervation of Ovarian Follicles
BIOCHEMICAL EVENTS IN OVULATION
Membrane Phenomena and Related Events
The Gonadotropin Surge
Gonadotropin Receptors
Cyclic AMP and Other Second Messengers
Protein Kinases
Mobilization of Membrane Phospholipids
RNA and Protein Synthesis
Vasoactive Agents and Related Substances
Histamine
Bradykinin
Angiotensin II
Prostaglandins
Lipoxygenase Products
Ovarian Steroids
Earlier Studies
Response to the Gonadotropin Surge
Sites of Steroid Synthesis
Importance of Steroids in Ovulation
Inhibitors of Steroidogenesis and Ovulation
Luteinized Unruptured Follicles
Other Considerations
Proteolytic Enzymes
Plasminogen Activator
Kallikrein and Kinin-Generating Activity
Collagenolytic Activity
Other Considerations
Follicular Inflammation
Fibroblast Proliferation
Growth Factors and Ovulation
Leukocytes and Ovulation
AN OVERVIEW OF THE OVULATORY PROCESS
INTRODUCTION
Mammalian ovulation is a distinct biological phenomenon that requires the rupture of healthy tissue at the surface of the ovary. In most mammals, the whole follicle protrudes markedly from the ovarian surface at the time of ovulation, and in many instances a thin translucent stigma, the macula pellucida, forms at the apex of the follicle as the final sign of impending rupture. This unique morphological change has left a striking impression on those who have actually observed it. Kelly (1) was so fascinated while observing a rabbit follicle near rupture he stated "as tension within the follicle increases, the transparent portion around the pole begins to bulge...It now stands out like the nipple on a breast." The moment of rupture sometimes appears as an explosive event, leading observers to compare it to a "volcano erupting" (2), or a "blister that bursts" (3).
Some years ago, Walton and Hammond (4) provided a detailed account of the macroscopic changes that can be observed in a laboratory animal like the rabbit. The changes that take place in the tissue at the site of rupture are pathophysiological in that they involve a fracture in the dense layers of collagenous tissue which encapsulates the follicle, and there is invariable hemorrhage in the vicinity of this ovarian lesion. However, the structural modifications are not limited only to the apically protruding stigma of the follicle. There is ample evidence that the ovulatory surge in gonadotropic hormones transforms the entire ovarian follicle into a highly secretory corpus luteum. In fact, there is reason to believe the primary action of the gonadotropins is luteinization, and that rupture of the follicular surface is somewhat of a fortuitous event that is contingent on the local softening of tissues and proliferation of fibroblasts that occur during the early stages of remodeling of the ovarian follicle into a corpus luteum (5).
This chapter provides a chronological account of the basic research on ovulation up to the 1970's, and then it concentrates on the information that has accumulated during the past several decades on the biochemical events of ovulation. The contents are not intended to be all-inclusive. For example, this chapter will not cover as many details about ovarian innervation and vascularity as the chapter on ovulation in the previous edition of these volumes (6).
Innumerable reviews on various aspects of ovulation have been written during the past 60 years. Some of these reviews are listed in the following sentences of this paragraph, while others are identified at more appropriate sites in this chapter. In 1932, Hartman (7) wrote the first comprehensive review of the work on ovulation, and his account provides many interesting insights into the early history of this subject. In addition, there are a number of other reviews of the earlier work on ovulation (3, 8-18). In more recent times, there has been an exponential growth in the number of studies on ovulation. Much of this more recent work has been described in detail in innumerable reviews that have appeared in the past 15 years. These include reviews of a comprehensive nature (19-26), on ovarian follicular development and ovulation (27, 28), on the structure and morphology of follicles (29-32), on the biochemistry of ovulation (33-36), on ovarian smooth muscle (37), on applications of the ovarian perfusion model (38), on ovulation and the immune system (39, 40), on the molecular aspects of ovulation (41-43), on signal transduction processes in ovulation (44), on ovulation as an inflammatory process (45, 46), and on ovulation in relation to the menstrual cycle (47, 48).
An initial note on terminology is also in order. It is common to use the expressions "preovulatory," "ovulatory," and "ovulation" all in reference to the entire gonadotropin-induced process. However, in this chapter, the adjective "ovulatory" will be applied to the entire process, while the term "preovulatory" will be used in reference to mature follicles that have not yet been stimulated to enter the ovulatory process. The term "ovulation" may indicate either the process, or the moment of egg release, but in instances where clear delineation of the latter phenomenon is of primary importance, then the term "follicular rupture" will be used for clarity.
HISTORICAL BACKGROUND
In the beginning, ovulation was studied mainly in vivo, simply with the naked eye. Observations of the follicular contents "oozing" or "bursting" from the ovary made a strong impression on the early investigators who managed to catch a glimpse of the phenomenon. The initial theories about the mechanism of ovulation keyed on the possible role of smooth muscle and the potential for such tissue to create intrafollicular pressures of sufficient magnitude to cause healthy follicular tissue to rupture. When light microscopy was first applied to studies of the microanatomy of visceral organs, the pioneering anatomists labeled much of the cellular component of the follicle as smooth muscle tissue. However, it is now clear that most of this tissue in and around mature ovarian follicles is collagenous connective tissue, which has arisen from resident fibroblasts. Nevertheless, the first 100 years of investigation into the mechanism of ovulation centered on the smooth muscle and the pressure theories. Therefore, the segments of this chapter that deal with the history of ovulation key on these two early theories and how they eventually gave way to the so-called "enzyme theory" of ovulation.
The Early Years
Ovarian follicles were first identified in 1672, when de Graaf examined human ovaries and observed vesicles on their surface which he mistakenly referred to as ova (49). Over a century later, Cruikshank (50) discovered ova in the fallopian tubes of rabbits, and eventually von Baer (28) realized that the mammalian oocyte was quite unlike the large avian and amphibian eggs, but instead was a relatively small cell within the follicular mass.
In the middle of the 19th century, von Kolliker (51) was the first to mention that smooth muscle was a structural constituent of the ovary. In 1858, Rouget (52) suggested that ovarian smooth muscle activity impaired venous return and caused congestion and "erection" of ovulatory follicles in a manner that increased intrafollicular pressure and caused rupture. That same year, von Luschka (53) concluded that the follicular fluid was derived primarily from secretions of the granulosa cells and secondarily from fluids transported to them from the blood vessels of the theca interna. A year later, Pfluger (54) observed the motion of frog ovaries and concluded that the "peristalsis" which they exhibited was responsible for ovulation, but he was apparently unaware of the fact that the amphibian ovary is in a state of constant movement even out of the sexual season (11). Two years later, Aeby (55) used acetic and nitric acid staining techniques to identify what he considered to be smooth muscle cells in the theca externa of avian and mammalian follicles, and he suggested that similar cells were responsible for the "peristaltic" contractions of the frog ovarian stroma. Several years later, Grohe (56) described the course of the muscle fibers in the ovary of the pig, and his observations led him to support the idea that congestion from impaired venous return caused rupture of mature follicles. In 1870, Waldeyer (57) agreed with Luschka's view of fluid formation, and he went on to hypothesize that a rapid hypertrophy of the theca interna increased intrafollicular pressure and caused rupture. There was little additional work on ovulation for the remainder of the 19th century, but the "smooth muscle" and "pressure" theories of ovulation were already firmly established by that time.
The Smooth Muscle Theory
The First Quarter of This Century
The smooth muscle theory of ovulation has been one of the most controversial issues in the field of reproductive physiology. The controversy has been perpetuated mainly by persistant reports that the dominant cell-type in the theca externa layer of the follicle wall is a typical smooth muscle cell. At the beginning of the present century, von Winiwarter and Sainmont (58) demonstrated what they called smooth muscle in the wall of the cat and human follicle, even though they were unable to demonstrate that either electrical or chemical stimuli could cause the follicle to rupture. In 1919, Thomson (59) carried out extensive histological studies and concluded that muscular contractions on an engorged follicle naturally increases the intrafollicular pressure and causes the follicle to rupture. In contrast, Corner (60) reported that same year his findings from an extensive study of the histology of the granulosa and thecal layers, and he concluded that the theca externa consisted of collagenous fibrils and long spindle-shaped "fibroblasts" that became mitotic just before rupture. Two years later, Guttmacher and Guttmacher (61) again reported histological evidence of thecal smooth muscle in the sow follicle, and they claimed that strips of these follicles contracted in response to solutions of HCl, barium chloride, and physostigmine sulfate. However, they also noted after 72 injections of ovarian and uterine arteries with saline, that "even though one braced himself against a wall and pushed the piston of the injection syringe with all the physical strength available," rupture did not occur in a single instance, although one could see the follicular vessels wash out clearly. In the end, they admitted that their experiments were so inconsistent that they were unable to conclude that muscle tissue had a role in the rupture of a follicle.
The Middle of This Century
Over a quarter of a century later, in 1947, Kraus (9) conducted an extensive study of ovulation in frogs, hens, and rabbits and found that attempts to induce contractility and ovulation with smooth muscle stimulants or electrical impulses invariably failed. That same year Claesson (62) attempted to resolve the smooth muscle issue by examining cow, swine, rabbit, guinea pig, and rat ovaries under a polarization microscope. By this method, he failed to find the high intrinsic birefringence that is characteristic of muscle, but instead found birefringence that is typical of connective tissue. The reliability of the method negated virtually all previous histological evidence, including Claesson's own, of smooth muscle in the follicle wall and threw doubt on the reliability of any physiological data. However, some years later, in 1960, Lipner and Maxwell (63) supported the smooth muscle theory by demonstrating visible muscle-like contractions in the follicles of ovarian tissue autotransplanted into the anterior chamber of the rabbit's eye. On the other hand, several years later, Espey (12) attempted to duplicate the earlier experiments by the Guttmachers. He found (i) that strips of sow follicles would contract only in response to HCl, (ii) that such contractions were tetanic in nature, (iii) that the tissue would relax only if it was exposed to alkaline solutions, and (iv) that such contractility could be attributed to collagen fibrils in the thecal layers of the follicle. Three years later, Espey (64) used transmission electron microscopy to confirm the distribution of collagenous connective tissue and fibroblasts in the theca externa of the follicle, and he conducted further studies to verify that follicular collagen contracts when it is exposed to acidic solutions (65).
The 1970's Surge in Interest
The smooth muscle controversy became more intense during the 1970's, when an avalanche of new reports claimed, on the basis of various kinds of evidence, that smooth muscle activity is an integral part of the ovulatory process. The reader is referred to an earlier review for enumeration of these reports (37). In brief, this review concluded that typical smooth muscle tissue is confined mainly to the hilar and medullary regions of the mammalian ovary. The numerous reports of myoid tissue in peri- and parafollicular areas are probably due to the overenthusiastic identification of "smooth muscle" tissue primarily on the observation of cytoplasmic filaments in the cells of the theca interna, without realizing that such structures are also a normal component of thecal fibroblasts (66-68). At the time of ovulation and especially during luteinization, there may be some differentiation of these thecal fibroblasts into myofibroblasts to facilitate wound healing and the removal of granulation tissue during luteolysis, but there is no convincing evidence that such tissue has an essential role in the mechanism of ovulation (37).
After the Surge
In spite of substantial evidence that ovarian contractions are not necessary for ovulation, there have been a number of more recent reports which continue to support the idea that smooth muscle is an important component in the mechanism of ovulation. Most of the effort to preserve the theory have come from Talbot, Martin, Schroeder, and collaborators (69-75), who continue to claim that there is a discrete layer of smooth muscle cells at least in the basal hemisphere of the follicle, and that such muscular tissue is necessary for extrusion of the oocyte. This lingering view is supported by further reports (i) that myocytes are present in the follicles of many mammals (76), (ii) that such cells are syncytially linked by several types of surface junctions (77), (iii) that these cells contain actin fibrils characteristic of smooth muscle cells (78), and (iv) that ovarian contractility and ovulation can be influenced by a wide range of agents that agonize and antagonize smooth muscle contractions (71, 79-82).
Also, Schroeder and Talbot (83) have reported that intrafollicular pressure changes during preovulatory contractility in the follicle. However, two decades earlier, Espey and Lipner (84) pointed out that such rhythmic fluctuations in intrafollicular pressure are rare and are not essential for ovulation. More recently, Kobayashi et al. (85) have also shown that perfused rabbit ovaries can ovulate in the absence of ovarian smooth muscle contractions, and Lofman et al. (86) have found that perfused rat ovaries can ovulate with no visible circumfollicular muscular activity.
Thus, there is still no convincing evidence that ovarian contractile activity is necessary for ovulation. Nevertheless, the existing data suggest that some kind of rhythmic motion is occasionally expressed by ovarian tissue near the time of ovulation, and the nature of this mechanical activity has not been adequately explained. Negligible attention has been given to the possibility that the rhythmic pulsations might be the consequence of vascular spasms in the blood vessels that enter the hilar region of the ovary (37). Also, it is possible that intraovarian pressure could fluctuate as a result of spasms in the tubo-uterine vasculature, because vessels of this origin anastomose with ovarian arteries (87). In considering this alternative explanation, it may be relevant to note that Markee (88) has observed that the uterine vasculature sometimes undergoes rhythmic spasms at 15-20 sec intervals, depending on the "hormonal" conditions of the tissue. Therefore, it is possible that an agent like prostaglandin F