Abstract
Microbial capsules are important virulence traits that mediate cell-host interactions and provide protection against host immune defense mechanisms. Cryptococcus neoformans is a yeast-like fungus that is capable of synthesizing a complex polysaccharide (PS) capsule that is required for causing disease. Microscopic visualization of capsule enlargement is difficult, because the capsule is a highly hydrated structure with an index of refraction that is very close to that of aqueous medium. In this study, we took advantage of the capsular reaction (“quellung” effect) produced by IgM monoclonal antibody (MAb) 13F1 to increase the refraction index difference between capsule and medium such that we visualized the capsule using differential interference contrast (DIC) microscopy. Time-lapse size measurements allowed us to quantify the growth rate of the capsule relative to that of the cell body. The increase in capsule volume per unit of time was consistent with a logistic variable slope model in which the capsule's final size was proportional to the rate of its growth. The rate of capsule growth (0.3 to 2.5 µm3/min) was at least 4-fold faster than the rate of cell body growth (0.1 to 0.3 µm3/min), and there was large cell-to-cell variation in the temporal kinetics of capsule and cellular growth. Previous to the first cellular replication event, both the capsule and cell body enlarged simultaneously, and their differences showed monotonic growth, which was affected only by its rate of volume increase per unit of time. Using these results, we provide an updated model for cryptococcal capsule biogenesis.
INTRODUCTION
Cryptococcus neoformans is a human-pathogenic fungus that has a distinctive capsule, which is a major virulence factor (1, 2). During an infection, C. neoformans is quickly stimulated to synthesize a thick polysaccharide (PS) capsule that reaches diameters larger than its cell body size (3). This mechanism of adaptation presents a significant problem to hosts, given the effectiveness of the capsule against immune defense strategies (i.e., phagocytosis and killing by macrophages) (4). The mechanisms involved in capsule growth remain poorly understood, in large part, because there are few tools to study the process of capsular enlargement.
In addition to its central role in fungus-host interaction, synthesis of a micrometer-size capsule (induced under nutrient-limited conditions) must represent both a substantial energy investment and a highly coordinated biosynthetic process. The major PS capsular component is glucuronoxylomannan (GXM), a very large (105 to 108 g/mol) and negatively charged heteropolymer formed by different repeating units (or structural reported groups [SRG]) (5). In serotype A strains (i.e., C. neoformans H99), the predominant SRG is a mannose triad with xylose and glucuronic acid substitutions (Man3Xyl2GlcA1). GXM is synthesized intracellularly in the Golgi apparatus and can be exported extracellularly via vesicles (3, 6–8), where it can incorporate on the cell wall surface. Anchoring of capsular GXM appears to involve PS-PS interactions, including cell-wall-derived PSs, such as α-glucans (9) and chitin-derived structures (10).
Capsule synthesis can be induced in vitro by growing the cells in various medium conditions, such as nutrient-limited conditions, mannitol, mammalian serum, carbon dioxide, alkaline pH, and low iron (11–15). Capsule formation is also increased by excess of calcium in minimal medium (16), suggesting the existence of a nonenzymatic process of enlargement involving ionic cross-linking and aggregation of PS molecules. Two not mutually exclusive models of capsule enlargement have been suggested: (i) proximal growth, in which addition of new PS is incorporated in the cell surface, displacing preexisting molecules to the outer edge (17); and (ii) distal growth, where addition of new PS is incorporated at the capsule edge (18). Regardless of the directionality of capsule growth or the assembly process, an increase in capsule size appears to result from the synthesis and incorporation of new PS molecules of increasing dimensions (19, 20).
Visual monitoring of capsule growth is challenging due to the capsule's high water content (∼99% [vol/vol]) (21), which contributes to a small refractive index difference in aqueous solutions that precludes observation by simple light microscopy. Furthermore, the hydration of the PS capsule makes it susceptible to dehydration procedures, which essentially precludes ultrastructural studies using electron microscopy (22). Scanning electron and confocal microscopy techniques can be used to visualize capsular material in whole cryptococcal yeast cells, with the latter exploiting fluorescently labeled antibodies (Abs) to GXM (10, 17, 23–26). In addition, capsule visualization can also be achieved by light microscopy (i) through negative staining of yeast cells by suspension in India ink or (ii) by the capsular reaction (“quellung” reaction) that follows binding of Abs to GXM (27–29). India ink particles allow visualization through their exclusion by the capsule, whereas the binding of capsular Abs allows visualization of the capsule by altering capsular optical properties such that the capsule can be distinguished from the surrounding aqueous medium.
In this study, we present the first temporal behavior analysis of capsule enlargement from 10 different C. neoformans H99 cells grown in vitro under capsule-inducing conditions. The capsule was labeled with monoclonal antibody (MAb) 13F1, an IgM that changes the optical properties of the capsule without significantly altering its elastic properties (30). This method allowed us to study capsule and cell body volume increase as a function of time, and the data provide new insight into the process of C. neoformans capsule synthesis, assembly, and architecture.
MATERIALS AND METHODS
C. neoformans serotype A strain H99 (ATCC 208821) cells from frozen stock were grown overnight in Sabouraud rich medium at 30°C under constant agitation. One milliliter of yeast cells was washed 3 times with phosphate-buffered saline (PBS) and enumerated using a hemocytometer. Approximately 104 cells were placed in a Lab-Tek chambered cover glass (Thermo Fisher Scientific, Rochester, NY) containing 200 μl of minimal medium containing 125 mM mannitol, 10 mM MgSO4, 29.3 mM KH2PO4, 13 mM glycine, and 3 μM thiamine-HCl (adjusted to pH 5.5 and 37°C) (12), supplemented with 20 μg/ml of IgM MAb 13F1 (31). This MAb was purified from hybridoma cell supernatant recovered after 14 days of growth using UltraLink immobilized-mannan binding protein (Pierce, Rockford, IL) chromatography.
The chamber slide was placed in a temperature-controlled microscope chamber adjusted to 37°C 2 h prior to recording. Image acquisition was done at 5-min intervals and different z-focus distances with a 63× differential interference contrast (DIC) objective in an Axiovert 200 M inverted microscope equipped with a Hamamatsu ORCA ER cooled charge-coupled device (CCD) camera and controlled by Axio Vision 4.6 software (Carl Zeiss Micro Imaging, New York, NY).
The whole-cell radius and cell body radius (rc and rb, respectively) were determined from time-lapse microscopy images using ImageJ software (National Institutes of Health, Bethesda, MD). For each cell, approximately 20 frames (20-min interval for a total of 400 min) were analyzed, with 3 line measurements (vertical, horizontal, and diagonal) across the whole cell (capsule included) and across cell body dimensions. The capsule average volume (Vcapsule) was calculated by subtracting the volume of the whole cell, Vcell (4/3 π rc3), from that of the cell body, Vbody (4/3 π rb3). Capsule and cell body growth curves (volume increase as a function of time) were fitted to different growth model equations (variable slope sigmoidal, Gompertz, logistic, and Weibull) using GraphPad Prism, version 5.0b (GraphPad Software, San Diego, CA). The Akaike's information criterion (AIC) method was used to determine the best model. Linear portions of curves were fitted to linear regression analysis to determine capsule and cell body growth rate (slope). Determination of capsule and cell body differences in radii, modeling, and calculations for the parameter alpha were done using MATLAB.
RESULTS
C. neoformans dimensions were recorded and measured over a period of 400 min for 10 individual cells. Both capsule enlargement and cell body enlargement could be simultaneously observed (see Movie S1 in the supplemental material). The halo depicting the outer edge of the PS capsule resulting from the “quellung” effect of MAb 13F1 (IgM) displaced away from the cell body as a function of time. Capsule growth appeared to be a continuous process with homogeneous circumferential enlargement. A cell was identified as dead by a quiescent cytoplasm devoid of any organelle motion. The dead cell manifested no capsule and/or cell growth and served as a negative control (see Movie S1).
Capsule growth as a function of time followed a nonlinear behavior, and we observed considerable cell-to-cell variation in the temporal kinetics of capsule and cell body growth (Fig. 1A). The growth curves were fitted to sigmoidal (4-parameter), Gompertz, Weibull, and logistic exponential equations, the latter being the most likely to be correct based on the Akaike's information criterion method (32) (Table 1). Capsules enlarged approximately from 3 to 15 times their initial volume sizes (ymax/ymin) and exhibited similar k values around 0.01 min (Table 2). Consistent with a logistic growth model, the final capsule size showed a positive and significant correlation with growth rate (slope of the curve, g) (Fig. 1A). The increase of cell body volume per unit of time did not show good fittings to a logistic growth model (Table 2), and the final cell body size did not correlate with the rate of its growth (Fig. 1B). These results suggest that the capsule and cell body follow distinct growth mechanisms and/or distinct time scales for their biosynthesis.
Table 1.
Cell | AIC value by equation |
|||
---|---|---|---|---|
Sigmoidalb | Gompertzc | Logisticd | Weibulle | |
1 | 4,686.4 | 6,339.5 | 3,246.9 | 3,519.1 |
2 | 4,526.3 | 3,777.8 | 2,370.2 | 2,909.5 |
3 | 10,780.9 | 5,052.5 | 3,235.6 | 6,507.5 |
4 | 3,065.8 | 4,005.6 | 2,744.9 | 2,138.5 |
5 | 10,110.5 | 6,818.3 | 3,864.3 | 6,527.1 |
6 | 13,366.4 | 7,068.9 | 3,764.9 | 9,256.2 |
7 | 14,473.0 | 3,745.8 | 3,130.7 | 16,689.4 |
8 | 18,695.9 | 72,989.9 | 14,740.3 | 2,043.3 |
9 | 3,385.3 | 6,818.3 | 3,864.3 | 6,527.1 |
10 | 7,006.7 | 7,124.1 | 4,653.7 | 4,845.9 |
For details, see reference 32. Based on the AIC model, the equation with the smallest AIC value (showed in italic type) is most likely to be correct.
The sigmoidal growth equation is , where ymax and ymin are the maximum and initial volumes, respectively, k is the value of x at halfway between ymin and ymax, and g is the slope.
The Gombertz growth equation is .
The logistic growth equation is .
The Weibull growth equation is .
Table 2.
Cell |
ymax (μm3) |
ymin (μm3) |
k (min) |
R2 |
||||
---|---|---|---|---|---|---|---|---|
Capsule | Body | Capsule | Body | Capsule | Body | Capsule | Body | |
1 | 976.3 ± 15.6 | 138.9 ± 9.3 | 64.6 ± 5.6 | 58.4 ± 2.1 | 0.015 ± 0.0006 | 0.006 ± 0.001 | 0.99 | 0.86 |
2 | 659.9 ± 9.6 | 112.8 ± 3.4 | 63.8 ± 5.5 | 38.4 ± 2.0 | 0.015 ± 0.0006 | 0.009 ± 0.001 | 0.98 | 0.93 |
3 | 539.3 ± 16.2 | 130.3 ± 9.9 | 66.1 ± 6.0 | 35.8 ± 2.0 | 0.012 ± 0.0008 | 0.007 ± 0.001 | 0.97 | 0.92 |
4 | 401.1 ± 10.5 | 116.6 ± 4.5 | 61.4 ± 6.9 | 25.3 ± 1.2 | 0.014 ± 0.0012 | 0.008 ± 0.001 | 0.93 | 0.97 |
5 | 558.1 ± 19.9 | 237.9 ± 39.9 | 61.9 ± 6.3 | 21.1 ± 1.7 | 0.012 ± 0.0008 | 0.007 ± 0.001 | 0.96 | 0.96 |
6 | 614.6 ± 20.3 | 176.5 ± 14.3 | 78.8 ± 5.4 | 14.3 ± 1.2 | 0.010 ± 0.0006 | 0.009 ± 0.001 | 0.98 | 0.97 |
7 | 371.5 ± 12.1 | 73.7 ± 3.6 | 94.4 ± 8.4 | 39.7 ± 1.8 | 0.011 ± 0.0012 | 0.007 ± 0.002 | 0.91 | 0.78 |
8 | 612.3 ± 106.4 | 92.8 ± 10.2 | 85.3 ± 6.4 | 3.9 ± 1.2 | 0.006 ± 0.0008 | 0.012 ± 0.002 | 0.94 | 0.91 |
9 | 186.6 ± 5.8 | 24.1 ± 0.8 | 62.6 ± 7.8 | 33.4 ± 2.8 | 0.015 ± 0.0025 | 0.019 ± 0.011 | 0.75 | 0.24 |
10 | 815.2 ± 20.7 | 93.8 ± 1.6 | 73.9 ± 11.2 | 55.6 ± 3.9 | 0.016 ± 0.0013 | 0.018 ± 0.004 | 0.95 | 0.63 |
Data were fitted using a logistic (3-parameter) nonlinear exponential equation.
On average, most of the capsule enlargement (∼70%) occurred prior to the first cellular replication event, when it switched from linear growth to a steady state (Fig. 1A). Some cells, however, continued to show some capsule growth during replication. The budding time varied between each replication event and among cells (Fig. 1A), consistent with previous reports (30). We noted that replication of C. neoformans cells occurred after attainment of a critical cell body size, ranging from 5 to 6 μm in diameter.
Linear regression analysis of exponential portions demonstrated that capsules always grew faster than the cell body (P = 0.004 based on paired t test), which is at least 4-fold faster (Table 3). The increase in capsule radius per unit of time was directly proportional and/or controlled by a single parameter (alpha), representing the relative growth rate of capsule to cell body. When the ratio is above 1/2, the capsule radius monotonically diverges from the cell boundaries. However, reduction of alpha below 1/2 results in an initial drop in the difference between the capsule and cell body radii followed by an exponential growth difference (Fig. 1C). The difference in radii of capsule and cell body for all cells demonstrated that the capsule envelope is monotonically increasing, or escaping the cellular boundaries, at least twice as fast the rate of cell body growth (Fig. 1D). Together, these results suggest that the size of growth of the capsule is dependent on the rate of its biosynthesis and suggest both a window of opportunity for capsule buildup preceding cellular replication and a minimum growth rate in order to escape the spherical volume boundaries of the cell body.
Table 3.
Cell | Increase in vol (µm3/min) of: |
Fold change (capsule/cell body) | |
---|---|---|---|
Capsule | Cell body | ||
1 | 2.51 ± 0.07 | 0.16 ± 0.01 | 15.7 |
2 | 1.63 ± 0.05 | 0.18 ± 0.01 | 9.1 |
3 | 1.25 ± 0.04 | 0.21 ± 0.01 | 6.0 |
4 | 0.87 ± 0.04 | 0.21 ± 0.01 | 4.1 |
5 | 1.27 ± 0.04 | 0.30 ± 0.01 | 4.2 |
6 | 1.30 ± 0.03 | 0.29 ± 0.01 | 4.5 |
7 | 0.70 ± 0.03 | 0.07 ± 0.01 | 10.0 |
8 | 0.80 ± 0.03 | 0.14 ± 0.01 | 5.7 |
9 | 0.28 ± 0.03 | ||
10 | 2.02 ± 0.09 | 0.06 ± 0.01 | 33.7 |
Growth rate (µm3/min) was determined by linear regression analysis of capsule or cell body radial length increase (μm3) as a function of time (min). Regression analysis was performed on the first 100 or 200 min of imaging, previous to the beginning of cellular replication.
DISCUSSION
Capsule synthesis is an important adaptation mechanism for several pathogens that cause infection and disease. In C. neoformans, capsular enlargement appears to be a survival strategy that occurs in response to predatory amoebae and during mammalian infection (4). Cryptococcal capsular enlargement implies an orchestrated array of biochemical processes and substantial energy investment, considering its complex composition and large dimensions.
The understanding of capsule construction is hampered by the capsule's complex molecular structure (4) and high water content (21) and the limited methodology for its study. Therefore, any effort at visualization and direct analysis of capsule growth has to overcome the capsule's fragility and dynamics. Furthermore, there is also the concern that any method used to visualize the capsule could affect the process of capsule growth.
In a prior study, we were able to identify the utility of MAb 13F1 for probing capsule enlargement. Although this MAb does change the refractive index of the capsule and allows visualization by light microscopy, it has little or no effect on the mechanical properties of the capsule (30). Consequently, MAb 13F1 labeling provides the first means to study capsule growth dynamics in real time. Here we report the first temporal analysis of H99 C. neoformans capsule and cell body enlargement using time-lapse microscopy and present an updated view for capsule synthesis, architecture, and assembly.
Our kinetic analysis revealed that capsule enlargement follows a logistic growth model. This type of exponential growth has been associated with autocatalytic reactions in which products can also act as reagents, resulting in spontaneous order and cooperativity. This finding is consistent with our prior observation that PS molecules carry structural information for capsule self-assembly (16, 33). In addition, the observed nonlinear growth demonstrates that the final capsule size is proportional to the rate of its growth (slope of curve). This suggests that the capsule dimensions are regulated by the rate of biosynthesis of its building blocks and the existence of a window of opportunity for capsule growth that may be related to the mitotic cycle.
The poor goodness of fit observed with the cell body volume increase per unit of time suggests that capsule and cell body enlargement follow distinct growth mechanisms and/or that they occur at different time scales. It is possible that this growth rate difference might reflect a metabolic priority toward the biosynthesis of capsular over cell wall building blocks. Alternatively, rather than focusing the anabolic activity toward a particular structure, the capsule could appear to grow faster as a consequence of the density and spatial organization between its components relative to the cell body structure.
We noted a relationship between capsule enlargement and cell division. For most cells, there was significant and simultaneous growth of the capsule and cell body previous to the first replication event. This relationship suggests that, like the cell body growth (34), capsule enlargement could represent a coordinated group of processes linked to the cell cycle. The observation that capsule enlargement was the first sign of metabolic activity demonstrates that C. neoformans prioritizes enlarging its capsule rather than its replication. Although the capsule is not required for C. neoformans viability, since acapsular mutants are viable (34, 35), the prioritization of capsule biosynthesis could reflect the importance of this surface modification for cryptococcal biology. In this regard, we note that the capsule is likely to serve a critical protective function during both mammalian infection and environmental survival, given that it protects against phagocytic cells and predators (36).
The rate and temporal behavior of capsule growth varied considerably among cells. This difference could account for the heterogeneity in capsule size observed in encapsulated cryptococcal samples. The rate of capsule enlargement was at least 4-fold faster than that of the cell body. It appears that the capsule must grow at least one-half as fast as the cell body to escape the boundaries depicted by the cell body envelope. Based on our measurement, C. neoformans cell body growth appears to occur approximately 100-fold slower than that reported for Saccharomyces cerevisiae (37).
The outward displacement of the capsule edge delineated by the “quellung” effect suggests a capsule growth model that includes proximal incorporation (at the cell body surface) of new PS molecules, displacing preexisting ones to the outer surface, as suggested previously (17). This, however, does not rule out the existence of simultaneous capsule growth by apical extension (18). A capsule in a growth model consisting solely of addition of new PS molecules at the capsule distal site (edge) would, in theory, be expected to exhibit a lower growth rate as a function of capsule size or, as the distance from the capsule edge to cell body increases, if the biosynthetic process was constant as a function of time and the density of capsular material was constant as a function of capsule radius. However, the density of capsular PS is known to decrease in the outer regions (24, 38), and the apical extension model could yield exponential growth if assembly of a less-dense outer capsule required less biosynthetic capacity than denser interior regions. Hence, nonlinear kinetics could be accommodated by either the proximal or apical extension models, and given that these are not mutually exclusive, we prefer a capsule growth model that includes PS addition at both distal and proximal capsule sites, since such a model would allow incorporation and reconciliation of all previous data (17, 18).
In summary, we provide the first cinematographic demonstration of capsular enlargement and cell body growth. Our results show great cell-to-cell variation in the temporal kinetics of capsule and cell body growth. Analysis of the rate of capsule growth can be reconciled with models of either proximal or apical growth. Overall, our results provide evidence that capsule growth follows an exponential growth pattern and is a highly regulated process that is linked to the timing of cell cycle progression.
Supplementary Material
ACKNOWLEDGMENTS
This work was supported by the National Institutes of Health grants AI033774, HL059842, and AI033142 to A.C. and R.J.B.C. R.J.B.C. was supported by grant T32 AI7506-15. R.J.B.C. is currently supported by CAPES/Programa Ciências sem Fronteiras.
We thank Nathan B. Viana for valuable discussion, all members of the A.C. lab who have worked on the problem of capsule growth visualization, and Antonio S. Nakouzi for purifying and providing MAb 13F1.
Footnotes
Published ahead of print 16 August 2013
Supplemental material for this article may be found at http://dx.doi.org/10.1128/EC.00163-13.
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