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Louisiana State University, Baton Rouge, Louisiana 70803
* Author to whom correspondence should be addressed. Current address: Department of Biology, Colorado State University, Ft. Collins, CO 80523. E-mail: Skmedler{at}aol.com
| Abstract |
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| Introduction |
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Extensive research has been carried out to better understand bivalve pumping processes, and data on the rate of water pumping by various bivalves provide an important component needed to develop general models of the pumping process (Foster-Smith, 1976; Møhlenberg and Riisgård, 1979; Silvester and Sleigh, 1984; Meyhöfer, 1985; Jørgensen et al., 1986, 1990; Jørgensen and Riisgård, 1988; Kryger and Riisgård, 1988; Silvester, 1988; Jørgensen, 1989; Jones et al., 1992; Nielsen et al., 1993). There is general agreement that the lateral ciliated cells provide the driving force for water flow and that changes in valve gape and siphon dimension contribute to adjustments in pumping rate. However, little work has addressed the potential role of other system components in regulating pumping processes, and a detailed understanding of the overall control of pumping remains elusive. Debate continues as to whether pumping and feeding are regulated only in an on/off mode (Jørgensen et al., 1988; Jørgensen, 1996) or whether a more sophisticated physiological regulation of these processes is possible (Ward and Targett, 1989; Wildish and Saulnier, 1993; Navarro et al., 1994; Ward et al., 1997). Further refinement of bivalve pumping models requires more detailed knowledge of the gill itself.
Models of the bivalve pump have relied heavily on the principles of fluid mechanics to develop mathematical descriptions of pumping processes (Foster-Smith, 1976; Silvester and Sleigh, 1984; Jørgensen et al., 1986, 1988; Silvester, 1988; Grünbaum et al., 1998). This type of analysis requires a thorough knowledge of the animals morphology to accurately estimate pumping properties. For example, the length and width of water passageways are used to estimate pressure losses stemming from the frictional resistance to flow. These system components are generally approached as rigid structures, with models applying fixed estimates of gill geometry to calculate system characteristics (Foster-Smith, 1976; Silvester and Sleigh, 1984; Jørgensen et al., 1986, 1988; Silvester, 1988). Although this is a logical simplification for modeling purposes, a body of evidence indicates that smooth muscles are important in affecting the geometry of the passages that constitute the system (Setna, 1930; Elsey, 1935; Atkins, 1943; Gardiner et al., 1991; Medler and Silverman, 1997, 1998). Poiseuilles law describes fluid flow in a circular pipe as: Q = 
Pr4/8Lµ, where Q is flow rate,
P is pressure difference, r is pipe radius, L is pipe length, and µ is dynamic viscosity of the fluid (LaBarbera, 1990). One of the implications of Poiseuilles law is that relatively small changes in vessel radius result in significant alteration of fluid flow. Many organisms take advantage of this principle to regulate flow by contracting or relaxing smooth muscles or muscle-like cells that line the vessels. For example, vertebrates modify arteriole diameter to regulate blood flow into capillary beds (Eckert et al., 1988), sponges change water flow by contracting or relaxing porocytes and myocytes as water enters the animal (Bagby, 1964; Pearse et al., 1987), and bivalves adjust flow through the alteration of siphon dimensions (Foster-Smith, 1976; Jørgensen et al., 1986, 1988). In this study, we focus on the ability of the eulamellibranch gill to change the dimensions of water passageways by altering the tone of integral smooth muscles.
Bivalves possess several muscles that have the potential to affect water flow. The most widely recognized of these are the adductor muscles and muscles of the mantle edges and siphons that are important for controlling valve gape and siphon dimensions. The integral gill muscles are not as widely appreciated, but are also likely to play a role in basic pumping processes. Each of the individual conduits for water flow is closely associated with smooth muscle fibers that can alter the dimensions of these passageways (Setna, 1930; Elsey, 1935; Atkins, 1943; Gardiner et al., 1991; Medler and Silverman, 1997, 1998). In addition, extensive muscles in the gill axis lying dorsal to the suprabranchial chamber are important in shortening the gill (Setna, 1930; Atkins, 1943). Previous endoscopic studies have documented changes in interfilament width, ostial dimension, and water-tube dimension in living animals (Tankersley and Dimock, 1993; Ward et al., 1994; Tankersley, 1996). Although the exact mechanism of such movements has not been clearly defined, these are consistent with the types of movements observed after the contraction of smooth muscles in the gill (Setna, 1930; Elsey, 1935; Atkins, 1943; Gardiner et al., 1991; Medler and Silverman, 1997). Examination of gills in their fully relaxed and contracted states is useful for defining the extremes in a continuum of gill dimensions. We report here 2- to 6-fold differences between the dimensions of the water passages in fully relaxed and fully contracted gills.
| Materials and Methods |
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Solutions
Freshwater animals were maintained in aerated aquaria with artificial pondwater (APW) at 2224°C as described in Dietz et al. (1994). Specimens of M. mercenaria were held in aerated aquaria with artificial seawater (ASW) at 4°C as specified in Chambers and De Armendi (1979). Ringers solutions for the freshwater bivalves were prepared as described for D. polymorpha in Dietz et al. (1994), with differences in hemolymph osmolality between species being corrected by adding NaCl to the solutions as needed. For M. mercenaria, ASW was used in place of Ringers solution. Calcium-free solutions were prepared by omitting Ca++ from the solutions and adding 4 mM EDTA in its place (Medler et al., 1999). Neurotransmitters were added to Ringers solution or ASW at a concentration of 1 mM, a pharmacological dose that has been shown to elicit maximal contraction of these muscles (Medler and Silverman, 1997; Gainey et al., 1998). Acetylcholine is effective as an excitatory neurotransmitter in the gills of D. polymorpha (Medler and Silverman, 1997) and C. fluminea (Medler, unpub. obs.) and was used to stimulate contraction in these species. Serotonin acts as an excitatory neurotransmitter in the gill muscles of M. mercenaria (Gainey et al., 1998) and was used to stimulate contraction in this species.
Gill preparation
Gills were removed from animals by cutting along the dorsal connection to the body with surgical scissors and were placed in the appropriate Ringers solution or ASW. The gills from one side of an animal were placed in a solution containing Ca++ before exposing them to an excitatory neurotransmitter; those of the opposite side were placed in a Ca++-free solution. Interfilament width and internal ostial area were measured from live gills as described below.
Gills normally exhibit severe muscular contraction upon exposure to fixatives such as glutaraldehyde. This was not the case in the present study, since the gills with Ca++ available to trigger contraction were already contracted through exposure to excitatory neurotransmitter. In fact, any further contraction that occurred helped to ensure that the gill was in a fully contracted state. We have recently demonstrated that the removal of extracellular Ca++ blocks muscle contraction in the gills of D. polymorpha (Medler et al., 1999), and this effect is also evident for C. fluminea and M. mercenaria. Exposure of these relaxed gills to glutaraldehyde failed to initiate any muscular contraction during the fixation process.
Water-tube measurements were made from gill sections. Excised gills were fixed with a 2% glutaraldehyde solution in isosmotic phosphate buffer for the freshwater species and a 2% glutaraldehyde solution in ASW for M. mercenaria. Tissues were fixed for 1 h in glutaraldehyde, rinsed twice in either buffer or ASW, and postfixed for 1 h in 1% OsO4. After fixation, the gills were rinsed twice in deionized water and dehydrated in a graded ethanol series. Whole gills were embedded in LR White (London Resin Co.) medium-grade resin by first placing them in a 1:1 mixture of ethanol and resin for 24 h. They were then transferred to 100% resin for 12 h and embedded flat in fresh resin at 60°C for 2448 h.
Water-tube dimension
A small portion of the central region of relaxed and contracted gills (approximate midpoint along both the dorsoventral and anterioposterior axes) was cut from embedded, fixed gills and cross-sectioned. Sections were cut using a Reichert-Jung ultracut E ultramicrotome at 12 µm thickness and stained with toluidine blue. The sections were viewed with a Nikon Microphot FXA using bright field optics, and the cross-sectional area of the water tube was measured from digitized video images using Image-1 computer software (Universal Imaging Corp.). Because muscle contraction causes a shortening of the gill in an anterioposterior direction, it was necessary to account for this change in our water-tube measurements. This adjustment was made by standardizing water-tube area per unit length of gill (number of filaments spanning the anterioposterior direction). Thus, water-tube area is given as (µm2/filaments). This correction would be unnecessary if the total cross-sectional area of the gill were measured, but measurements were made from only a portion of the gill. Failing to correct for the shortening would overestimate the cross-sectional area in contracted gills. Water-tube dimensions from relaxed and contracted gills from individuals of each species were compared with paired t tests (n = 5).
Studies using fixed and dehydrated tissues are sometimes criticized for introducing artifacts due to shrinkage. Indeed, these procedures do lead to changes in gill dimensions that should be noted when an accurate measure of absolute dimensions is critical (Silverman et al., 1995). In the present study, we were interested only in comparing the relative differences between important dimensions in the fully relaxed and fully contracted states. When the gills were fixed for measurement of water-tube area, each gill pair came from an individual animal and was processed with the same fixatives, dehydration steps, and embedding. Thus, any shrinkage is expected to be proportional in the relaxed and contracted gills, leaving the relative change unaffected.
Interfilament width
Live gills were placed on microscopic slides in the appropriate solution and covered by coverslips elevated on posts of petroleum jelly to prevent the gills from being compressed. Gills were examined with differential interference contrast (DIC) optics on a Nikon Microphot FXA. Interfilament distances from digitized video images were measured as described above, and distances were calibrated with a stage micrometer. Interfilament widths from relaxed and contracted gills from individuals of each species were compared by paired t tests (n = 5).
Internal ostial area
Live gills were split into single lamellae and placed in an irrigation chamber as described in a previous study (Medler and Silverman, 1997). Gill lamellae were placed in Ca++-free solutions to completely relax their musculature before any measurements were made and remained in this solution when placed into the chamber. The internal water-channel epithelium was placed toward the bottom of the chamber so that the internal ostia could be observed using an inverted Nikon microscope with Hoffman modulation optics. After the relaxed gill ostia were measured, the chamber was irrigated with Ringers or ASW containing an excitatory neurotransmitter. The gill was observed and videotaped as it contracted; the ostia were remeasured once contraction was complete (about 1 min later). Ostial areas (µm2) were measured from digitized video images as described above and were calibrated with a stage micrometer in the experimental set-up. Ostial areas from relaxed and contracted gills from individuals of each species were compared with paired t tests (n = 5).
Scanning electron microscopy
Gills in contracted and relaxed states were fixed as described above. After dehydration, the gills were wrapped in lens paper, critical-point dried, and mounted on stubs. Dehydrated gills were either sectioned or split apart to reveal relevant regions of the gills. Specimens were sputter coated with a mixture of gold and palladium (20 nm) and viewed with a Cambridge S-260 scanning electron microscope. Digitized video images were enhanced for optimal brightness and contrast using Adobe Photoshop 5.0 software (Adobe Systems, Inc.).
Video endoscopy of live gills
An optical insertion tube (OIT) was inserted into the suprabranchial chamber of large specimens of L. anodontoides using the general approach described by Tankersley (1996). This species was selected because individuals tend to gape widely, allowing observations to be made without wedging the valves open. Animals were placed in an aerated container of APW (about 4 l) and fixed in position by means of a nylon bolt cemented to one valve. The OIT (1.7 mm diam. x 101 mm long; AEI North America) was attached to a 150 W halogen fiberoptic light source and inserted through the exhalent aperture into the suprabranchial chamber. A mirror sleeve was attached to the OIT to provide the 90° view needed for direct observation of the water tubes. The OIT was attached to a zoom adapter that provided a maximal magnification of about 150x. Maximum resolution was estimated to be approximately 5 µm at maximum magnification. The OIT and zoom adapter were coupled to a Costar color video camera (0.85 cm CCD model CV-730) mounted on a microscope stage. The microscope stage served as a micromanipulator, allowing movements in the X, Y, and Z planes. Observations were recorded on VHS videotape, and digitized video images of portions of these recordings were captured using Image-1 computer software. Images were adjusted for brightness and contrast using Adobe Photoshop 5.0 software.
No pharmacological agents were used during endoscopy. Animals were held in a darkened room, and once the endoscope was positioned, there was minimal disturbance to the animals. Changes in the geometry of the gills and suprabranchial chamber were spontaneous, not resulting from any discernible stimulus.
| Results |
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| Discussion |
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Jørgensen and colleagues have highlighted alteration of interfilament distance as a central control mechanism for regulating pumping activities (Jørgensen et al., 1986, 1988; Jørgensen and Riisgård, 1988; Jørgensen, 1989, 1990). There are several possible consequences of changes in interfilament distance, with the most obvious being that a change in distance will affect the resistance to water flow (Foster-Smith, 1976; Jørgensen et al., 1986). In addition, it has been suggested that as the filaments move toward one another, the lateral ciliated cells responsible for establishing water flow begin to interfere with one another (Jørgensen et al., 1988; Jørgensen, 1989, 1990). Recent mathematical modeling of gill dimensions has provided further insight into the specific consequences of a particular interfilament distance (Grünbaum et al., 1998). One of the predictions of this model is that the optimal interfilament width for maximizing water flow depends upon the pressure gradient producing the flow. At low pressure differences, a ciliary gap of near 20 µm is optimal; as pressure differences increase, the optimal gap decreases toward 510 µm (Grünbaum et al., 1998). This range corresponds well with the distances observed for each of the species in this study (Fig. 2a). When the gill muscles are relaxed, the interfilament width is close to 20 µm, but can quickly change to 10 µm or less as the muscles contract (Medler and Silverman, 1997; Fig. 2a). An environmental variable that may dictate adjustments of pump properties is water temperature, since water viscosity changes inversely with temperature and has direct effects on pumping activities (Jørgensen et al., 1990). It has also been suggested that changes in interfilament width may provide a mechanism to adjust feeding rate and efficiency (Ward et al., 1998). The data in this and previous studies provide evidence that interfilament distance is controlled directly by the activity of smooth muscles, allowing these animals to adjust interfilament distance as needed (Gardiner et al., 1991; Medler and Silverman, 1997).
Connecting the interfilament spaces with the suprabranchial chamber are the passages that constitute the "pipes" of the gill. As indicated by Grünbaum et al. (1998), the pressure drop across the gill filaments is dependent on filament geometry and upon the type of "piping system" to which the filaments are attached. In the eulamellibranch gill, these pipes include the water canals that lead to the central water channel (beginning with external ostia and emptying into the water channel via internal ostia) and the water tubes that lead to the suprabranchial chamber. Previous in vivo studies from several bivalve species indicate that the ostia are more open during active pumping (Foster-Smith, 1976; Tankersley, 1996), and Jørgensen and colleagues have emphasized a correlation between valve gape, ostial dimension, and rate of water pumping (Jørgensen et al., 1986, 1988; Jørgensen, 1990). Foster-Smith (1976) noted that changes in ostial dimension affect pumping activities, indicating that reductions in ostial size produce pressure losses across the gill. In this and a previous study, we have observed rapid and dramatic changes in internal ostial dimension in live gills (Fig. 3; Medler and Silverman, 1997). In addition, muscle contraction clearly leads to a reduction in the dimension of the water tubes (Figs. 4 and 5). Tankersley (1996) documented similar changes in water-tube dimension in another unionid bivalve, Pyganodon cataracta. Although no previous work has addressed the potential effects of such changes in water-tube dimension on pumping processes, Poiseuilles law predicts that as the internal diameter is halved, the flow rate decreases by a factor of 16. Other endoscopic studies have reported a rhythmic expansion and contraction of the gills that was believed to augment water flow through the water tubes (Tankersley and Dimock, 1993; Ward et al., 1994).
Bivalve pumping is a complex process that is dependent on ciliary motors as well as on the muscles that control valve gape, mantle and siphon posture, and gill dimension. The values provided by this study represent the extremes of a range of dimensions that the gills can adopt. It is likely that a continuum of ciliary activity and muscular tone are coordinated through the branchial nerves. Although it is well established that the nerves of the gill have control over ciliary activity (reviewed by Paparo, 1988), almost nothing is understood about the nervous control of the gill muscles. What is known is that the muscles respond to various neurotransmitters in vitro (Jørgensen, 1976; Gardiner et al., 1991; Medler and Silverman, 1997; Gainey et al., 1998), and that in a unionid bivalve, the neurotransmitter serotonin induces the gill muscles to relax while increasing the activity of the lateral ciliated cells (Gardiner et al., 1991). The apparent effect of serotonin in this species is to increase pumping rate by enhancing motor activity while simultaneously decreasing the resistance to water flow, but whether these processes are controlled by serotonergic neurons in vivo is unknown. Recent work by Gainey et al. (1999) reveals that peptides found in nerves in the gills of Mercenaria mercenaria have modulatory effects on ciliary activity and that these nerves are closely associated with the muscles of the gills. One of the conclusions drawn from that study is that the peptides are important for modulating both the ciliary and muscular activity involved in feeding activities (Gainey et al., 1999). Understanding the neural control over the muscles of the gill should be a productive focus of future research.
| Acknowledgments |
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| Footnotes |
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| Literature Cited |
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