Abstract
Background and Aims
Excess salinity inhibits the metabolism of various systems and induces structural changes, especially in chloroplasts. Although the chloroplast body seems to swell under salinity stress as observed by conventional transmission electron microscopy, previous studies are limited to 2-D data and lack quantitative comparisons because specimens need to be sliced into ultrathin sections. This study shows three-dimensionally the structural changes in a whole mesophyll cell responding to salinity stress by serial sectioning with a focused ion beam scanning electron microscope (FIB-SEM) and compares the differences in chloroplast structures based on reconstructed models possessing accurate numerical voxel values.
Methods
Leaf blades of rice plants treated with 100 mm NaCl or without (control) for 4 d were fixed chemically and embedded in resin. The specimen blocks were sectioned and observed using the FIB-SEM, and then the sliced image stacks were reconstructed into 3-D models by image processing software.
Key Results
On the transverse sections of rice mesophyll cells, the chloroplasts in the control leaves appeared to be elongated meniscus lens shaped, while those in the salt-treated leaves appear to be expanded oval shaped. The 3-D models based on serial sectioning images showed that the chloroplasts in the control cells spread like sheets fitted to the shape of the cell wall and in close contact with the adjacent chloroplasts. In contrast, those in the salt-stressed cells curled up into a ball and fitted to cell protuberances without being in close contact with adjacent chloroplasts. Although the shapes of chloroplasts were clearly different between the two treatments, their volumes did not differ.
Conclusions
The 3-D reconstructed models of whole rice mesophyll cells indicated that chloroplasts under salt stress conditions were not swollen but became spherical without increasing their volume. This is in contrast to findings of previous studies based on 2-D images.
Keywords: Chloroplast, chloroplast protrusion, focused ion beam scanning electron microscope, mesophyll cell, Oryza sativa L, salt stress, three-dimensional reconstruction, ultrastructure, transmission electron microscope
INTRODUCTION
Salt accumulation in soil (soil salinization) is one of the most serious environmental factors limiting the growth and yield of crops (Hillel, 2000). Excess salinity inhibits various metabolisms, including photosynthesis (Parida and Das, 2005), and induces ultrastructural changes, especially in chloroplasts, which appear to be the most affected by salt stress (Rahman et al., 2000; Mitsuya et al., 2003a; Yamane et al., 2003, 2008, 2012).
Under severe salinity stress, swelling and degradation of thylakoids have been observed (Rahman et al., 2000; Mitsuya et al., 2003a; Yamane et al., 2003, 2004). These changes are induced by the accumulation of reactive oxygen species (ROS) derived from excess reductants (Yamane et al., 2004) when carbon fixation ability is reduced owing to stomatal closure in response to osmotic stress caused by high salinity in soil (Chaves et al., 2009). The destruction of the chloroplast envelope has also been observed and is considered to be caused by osmotic stress (Yamane et al., 2003). In addition, tubular projections of chloroplasts, termed stromules (Köhler and Hanson, 2000; Gray et al., 2012) or chloroplast protrusions (Bourett et al., 1999; Yamane et al., 2012), are formed under salt stress. It has been suggested that the formation of the chloroplast protrusion is followed by the ejection of a Rubisco-containing body (Chiba et al., 2003), which is isolated from the chloroplast body, and that this may be one of the pathways for chloroplast degradation under salt stress (Yamane et al., 2012; Ishida et al, 2014). In addition, the chloroplast body also seems to swell with salinity, not only under high salt concentrations or long-term treatment (Rahman et al., 2000) but also under mild concentrations (see fig. 3b in Yamane et al., 2008) or in the early stage of treatment (see fig. 3A in Yamane et al., 2003); however, the chloroplast volume has not been compared quantitatively.
As mentioned above, numerous studies on chloroplast structures under salinity stress have been reported; however, there are few studies showing their 3-D structural changes. Because the conventional transmission electron microscope (TEM) observations, which have been used in previous studies, require the specimens to be sliced into ultrathin sections (approx. 0.1 µm), it is difficult to comprehend the 3-D structure intuitively. There are also few studies that investigated changes in organelle volume in response to salinity stress. In addition, the TEM observation tends to focus attention on the region near the centre of the cell to take representative images of the cell. The peripheral regions of the cell have often been overlooked; however, it is important to observe a whole cell from the centre to the peripheral regions in order to understand the cell structure comprehensively.
Originally, sectional images are restricted to 2-D data; however, stacking the micrographs of serial sections provides 3-D volume data. Recently, several types of electron microscopy have been proposed for the reconstruction of 3-D structures from micrographs of serial sections (Hughes et al., 2014). One of the tools used to reconstruct the 3-D ultrastructure is a focused ion beam (FIB) scanning electron microscope (SEM) (FIB-SEM) (Knott et al., 2008). The FIB-SEM provides hundreds of sectioning images at correct intervals at the nanometre scale, and then image processing software can convert the image stacks into virtual cross-sections at every conceivable angle or depth and into the 3-D reconstructed models of cell components (Lucas et al., 2012).
Recently, we visualized the ultrastructure of a whole rice mesophyll cell by 3-D reconstruction based on serial sectioning 2-D images obtained with the FIB-SEM (Oi et al., 2017). The reconstructed models include 3-D information at the ultrastructural level with accurate values for volume and surface area. In our previous study, this method showed that unstressed rice mesophyll cells are discoid shaped with several lobes around the cell periphery, increasing the surface area to volume ratio, and the chloroplasts occupied half of the cell volume and spread as sheets along the cell lobes, covering most of the inner cell surface (Oi et al., 2017). It is considered that rice mesophyll cells with increased cell surface area and sheet-shaped chloroplasts enhance CO2 absorption (Sage and Sage, 2009; Oi et al., 2017).
In this study, we used the FIB-SEM followed by 3-D reconstruction to investigate ultrastructural changes in rice mesophyll cells, especially chloroplasts, associated with salinity stress. Here we discuss the 3-D morphological changes in chloroplasts based on reconstructed models with accurate numerical voxel values.
MATERIALS AND METHODS
Plant material and growth conditions
Caryopses of rice (Oryza sativa L. ‘Nipponbare’) were imbibed in a beaker containing distilled water in an incubation room at 30 ± 2 °C. After the white tip of the coleoptile appeared, the caryopses were sown on a mesh above a plastic bucket containing nutrient solution (Mae and Ohira, 1981). The seedlings were cultivated hydroponically in a growth chamber under a daily 14 h photoperiod at 500 μmol m−2 s−1 with 28/20 °C (day/night), for 21 d. Then, they were treated with 100 mm NaCl in the nutrient solution for 4 d. Control plants were grown in the nutrient solution without NaCl.
Specimen preparation
The uppermost fully expanded (fifth–seventh) leaves were chemically fixed and embedded in resin as described in Oi et al. (2017). Small segments (approx. 1 × 2 mm) excised from the middle portion of the leaf blades were vacuum-infiltrated for 5 min in Karnovsky’s fixative (mixture of 4 % paraformaldehyde and 5 % glutaraldehyde) in 50 mm sodium phosphate buffer (pH 7.2) and pre-fixed in the same solution for 5 h. After being rinsed in the buffer for 2 h, the segments were post-fixed in 2 % osmium tetroxide in the same buffer for 12 h. The segments were rinsed with the buffer and distilled water, dehydrated in a graded acetone series (30, 50, 70, 90, 99 and 100 %), treated with propylene oxide and then embedded in Spurr’s resin.
FIB-SEM observation
The leaf segments embedded in resin were serially cut and observed with a FIB-SEM according to Oi et al. (2017). Transverse section of the embedded leaf segments were exposed using a diamond knife on an ultramicrotome (EM UC6, Leica, Germany). The resin blocks were subsequently trimmed to a cuboid (approx. 3 × 3 × 2 mm) and glued to the standard specimen stage for FIB-SEM. The transverse section of the leaf faced the SEM column, and the leaf veins in the segment were placed vertically to the FIB column. The specimens were coated with a thin layer of evaporated carbon with a carbon coater (CADE-EMT, Meiwafosis, Japan) to prevent electron charging. Serial electron micrographs were obtained with a FIB-SEM (MI-4000L, Hitachi, Japan), in which the FIB and SEM columns were orthogonally arranged; the angle of the two columns was 90°. Specimen surfaces were exposed using the FIB, and then block-face images were captured with the SEM. Serial electron micrographs were obtained automatically by repetitive cutting with the FIB and image capturing with the SEM. The FIB was operated as follows: an accelerating voltage, 30 kV; a beam current for milling to prepare or to cut, repetitively, 1.6 or 1.2 nA, respectively; cutting interval, 50 nm. The SEM was operated as follows: accelerating voltage, 1.0 kV; working distance, 2 mm; dwell time, 30 µs per pixel; image size, 1000 × 1000 pixels; colour depth, 8-bit (256 grey scales); pixel size, 25 (or 20, only for NaCl-treated plant #3) nm per pixel; beam current, 10 pA (±10 %). Secondary electrons were detected by the upper detector in the SEM column. Backscattered electrons were also detected, but we did not use them for imaging in this study.
3-D reconstruction
The resultant image stacks from the block-face imaging were processed using the software ‘Fiji’ (http://fiji.sc/Fiji) (Schindelin et al., 2012); grey scale was inverted so that the SEM images resembled TEM images, brightness and contrast were adjusted and then the slices were aligned. The processed 2-D image stacks were then compiled into orthogonal slice images by volume rendering with the plugin ‘Volume Viewer’ of Fiji. The regions of cell walls and chloroplasts in all 2-D images (actual cross-sections) were also segmented using the software ‘PaintTool SAI’ (ver. 1, Systemax, Japan); each component was manually painted with a specified colour and saved in BMP format (colour depth: 24 bit). The colour-segmented image stacks were then reconstructed into 3-D models by surface rendering, using the software ‘Image-Pro Premier 3D’ (ver. 9.3, Media Cybernetics, USA). The 3-D rendered models were smoothed with the ‘Low-pass filter’ (3 × 3 × 3), and then their volume, surface area and sphericity were calculated with the function ‘3D Measure’ of Image-Pro Premier 3D.
Statistical analysis
The data were statistically analysed using Microsoft Excel with add-in software (Statcel 3, OMS Publishing Inc., Japan). Means were compared by Student’s t-test, and medians were compared by Mann–Whitney’s U-test (*P < 0.05, **P < 0.01). Other details regarding statistical parameters can be found in the figure legends.
RESULTS
The transverse sections at the centre of the rice mesophyll cells showed that the cells were lobed with several invaginations in both the control and NaCl-treated leaves (Figs 1A and 2A). In control leaves, the meniscus-lens-shaped chloroplasts were distributed along the lobed cell wall (Fig. 1A). Conversely, in NaCl-treated leaves, the chloroplasts expanded into an oval shape (Fig. 2A). The paradermal and longitudinal sections also showed meniscus-lens-shaped chloroplasts in the control leaves and expanded oval chloroplasts in the NaCl-treated leaves, even though the sections showed an oblong cell shape without deep invaginations (Figs 1B, C and 2B, C). Although the chloroplast envelope was partly distorted in the NaCl-treated cells (Fig. 2; white arrowheads), the swelling or degradation of thylakoids was not observed in either the control or NaCl-treated leaves (Figs 1 and 2). The sections in the NaCl-treated cells showed several protrusions and vesicles of chloroplast (Fig. 2: black arrowheads); however, they continuously connected with chloroplast bodies in serial image stacks. All slice data are shown in Supplementary data Videos 1–6.
The cell walls of mesophyll cells in the serial images were segmented and reconstructed into 3-D models (Fig. 3). Although there was some variation in the shape of these cells, they were generally bumpy discoid with lateral protuberances in both the control and NaCl-treated plants. Cell volume and surface area were calculated based on these 3-D models, and there were no significant differences between the control and NaCl-treated plants in terms of volume (P = 0.17) or surface area (P = 0.33) of the cells (Table 1).
Table 1.
Control | V (µm3) | S (µm2) | S/V (µm−1) | Salt stress | V (µm3) | S (µm2) | S/V (µm−1) |
---|---|---|---|---|---|---|---|
#1* | 1284 | 799 | 0.62 | #1 | 1165 | 812 | 0.70 |
#2 | 1644 | 995 | 0.61 | #2 | 1046 | 746 | 0.71 |
#3 | 1067 | 694 | 0.65 | #3 | 795 | 516 | 0.65 |
Mean | 1332 | 830 | 0.63 | Mean | 1002 | 691 | 0.69 |
± s.d. | 291 | 153 | 0.02 | ± s.d. | 189 | 155 | 0.03 |
Means were compared between the control and NaCl-treated plants by Student’s t-test; V (P = 0.17), S (P = 0.33), S/V (P = 0.03).
*The original serial sectioning images of control plant #1 were the same as the images used in Oi et al. (2017). The values of V and S in the previous study were calculated without smoothing the 3-D reconstructed model, and V of the previous model was similar (1280) to the present value; however, S of the previous model was higher (1213) than that of the present study.
The chloroplasts in the mesophyll cells were also reconstructed into 3-D models (Fig. 4A). They were distributed along the contour of the cells. The average number of chloroplasts contained in one mesophyll cell was 14.7 ± 2.1 (mean ± s.d.) in the control and 12.3 ± 2.3 (mean ± s.d.) in the NaCl-treated cells; there was no significant difference between the two treatments (P = 0.26). Chloroplasts varied in size, and surface area was positively correlated with volume in the control (R2 = 0.90) and NaCl-treated plants (R2 = 0.88) (Fig. 4B). The chloroplast volume did not differ between the control and NaCl-treated plants (P = 0.11) (Fig. 5A). However, the surface area (Fig. 5B, P < 0.05) and the ratio of surface area to volume (Fig. 5C, P < 0.01) were significantly lower in the NaCl-treated plants than in the control plants. There was also a clear difference in the shape of chloroplasts between the two treatments. The chloroplasts in the control cells spread like sheets fitted to the shape of the cell wall with the adjacent chloroplasts in close contact with each other (Fig. 5D). Conversely, those in the NaCl-treated cells curled up into a ball fitted to the cell protuberances without close contact with adjacent chloroplasts (Fig. 5E). To compare the structural changes in chloroplasts between the two treatments, the sphericity of each chloroplast was calculated (Fig. 5F). The sphericity indicates how closely the shape of the object approaches that of a perfect sphere (1.00). The sphericity of the chloroplasts in the NaCl-treated cells (median 0.77) was significantly higher than that in the control cells (median 0.67) (Fig. 5F).
DISCUSSION
The images of cross-sections obtained in this study showed that chloroplasts in salt-stressed mesophyll cells seemed to swell (Fig. 2), the same as found in the previous studies based on TEM observations (e.g. Rahman et al., 2000). However, the 3-D reconstructed models showed that the chloroplasts did not swell but became spherical without increasing in volume (Figs 4 and 5). Therefore, the view that chloroplast swelling (increasing volume) in response to osmotic pressure from salinity stress was based on misinterpretations of 2-D images. The use of 3-D data in the present study overturns the conventional view. Here we discuss the morphology of rice mesophyll cells based on these new 3-D images.
Mesophyll cells in rice leaf blades were a bumpy discoid shape with lateral protuberances (Fig. 3). The mesophyll cells were joined together by their lobes that vary in size and number (Chonan, 1967; Sage and Sage, 2009). The constrictions in the lobes were deep in the transverse (xy-) section, and the cell shapes generally seemed to be discoid (Fig. 3). One of the observed cells (Fig. 3C3) was not discoid but rather of an irregular shape; this cell was adjacent to a large epidermal cell on the abaxial leaf side. It seemed that the mesophyll cells in the exterior of the leaf tissue were more irregular in shape than those in the interior. Although cell shape was diverse, it is considered that the external form of the mesophyll cells was unaffected by salinity stress in this experiment (Fig. 3). The cell volume and surface area were not different between the control and salt-stressed cells (Table 1). In this study, we examined the leaves that had fully expanded before the treatments started and had not wilted by the end of the treatment; therefore, it is considered that the cells had not yet greatly dehydrated and shrunk.
Chloroplasts with various shapes were distributed along the complicated cell wall, and it is difficult to understand the difference in chloroplast shape between the two treatments from the perspective of a whole cell (Fig. 4). However, there are clear differences between the control and salt-stressed plants in terms of shape and location of the individual chloroplasts. The chloroplasts in control plants spread like sheets along the lobed cell wall and were in close contact with each other, as previously described (Oi et al., 2017) (Fig. 5D). Conversely, we observed that chloroplasts in the salt-stressed cells were significantly more spherical and were not in close contact with adjacent chloroplasts (Fig. 5E). Two possibilities are conceivable regarding the physiological significance of the morphological change under salt stress.
First, the sheet shape of the chloroplasts in the control leaves could be a response to CO2 concentrations in the intercellular space. For efficient CO2 absorption, chloroplasts would expand into a sheet shape, which increases the ratio of surface area to volume (Oi et al., 2017), and stick to the cell periphery, especially in the areas facing the intercellular space (Sage and Sage, 2009). However, salinity or osmotic stress causes stomatal closure and decreases CO2 concentration in the intercellular space of leaves. Then chloroplasts would become spherical by negatively responding to the low CO2 concentration. Alternatively, the spherical shape might simply be a result of damage caused by salt stress. It is known that chloroplasts under strong or weak light conditions move by chloroplast actin (cp-actin) filaments polymerized by Chloroplast Unusual Positioning 1 (CHUP1), which anchors the chloroplast outer membrane to the plasma membrane through unknown membrane proteins (Kadota et al., 2009; Wada and Kong, 2018). It is also considered that chloroplasts under conditions with moderate light actively maintain their intracellular position by anchoring with actin filaments (Takagi et al., 2009; Wada and Kong, 2018). Although the regulatory mechanism of chloroplast shape is not well understood, salt stress might disturb the anchoring of chloroplasts to the cell periphery, and the sheeted chloroplasts would passively change to a spherical shape. Further studies are required to reveal the cytoskeleton and membrane proteins involved in chloroplast shape regulation.
Conversely, this change to a spherical shape of chloroplasts might be the acclimation to salinity stress. Chloroplasts can change their intracellular positions; they move away from light to minimize photodamage under high-intensity light irradiation (Yamada et al., 2009; Wada and Kong, 2018) and drought or salinity stress (Yamada et al., 2009). In rice leaves, however, the mesophyll chloroplasts hardly changed their intracellular positions (Inoue and Shibata, 1974) (Fig. 4). Because the chloroplasts occupied half of the cell volume and covered most of the periphery in the rice mesophyll cell (Oi et al., 2017), they seemed to have less space to move inside the cell (Figs 4A and 5D). However, it is important for chloroplasts to dissipate excess light energy under salinity stress. Damage caused to chloroplasts, such as the swelling of thylakoids, under salinity is light dependent (Mitsuya et al., 2003b), and the damage is induced by excess hydrogen peroxide (H2O2) and H2O2-derived hydroxyl peroxide (Yamane et al., 2004). In the present study, however, thylakoids did not swell in all chloroplasts, suggesting that chloroplasts could dispose of excess light energy without changing their intracellular position. The spherical shape would reduce light absorption compared with the sheet-like shape with a higher ratio of surface area to volume (Fig. 5). The chloroplasts in rice leaves might actively change their shape to reduce light energy under salinity stress. However, the relationship between avoidance of photodamage and morphological changes (spherical shape) in chloroplasts has not been elucidated.
Overall, chloroplasts tend to become spherical under salt stress; however, they also form protrusions and pockets locally (Figs 2, 4A and 5E). The protruded bodies are in a sheet-like structure, and some chloroplasts construct pockets with a sheet structure that include cytoplasm, mitochondria or peroxisomes (Yamane et al., 2018). Since the protruded bodies of chloroplasts contribute to the re-assimilation of photorespired CO2 released from mitochondria (Busch et al., 2013), the construction of the sheet structure and pockets could compensate for the negative effects of reducing the CO2 absorption area by forming a spherical shape under salinity stress. Further studies are required to elucidate the relationship between the sub-structural changes in chloroplasts and photosynthesis.
In conclusion, chloroplasts became spherical under salinity stress without increasing in volume. Previous views of swelling in chloroplasts were misinterpretations based on 2-D observations, suggesting that the use of 3-D analysis would be useful for future studies to prevent similar misinterpretations. The physiological significance of this morphological change remains unclear and, therefore, the relationship between chloroplast ultrastructure and their functionality under salinity stress should be further investigated in the future.
SUPPLEMENTARY DATA
Supplementary data are available online at https://academic.oup.com/aob and consist of the following. Videos S1–S6: all actual transverse slices, virtual orthogonal slice and 3-D reconstructed models of chloroplasts in a whole rice mesophyll cell; S1, C1; S2, C2; S3, C3; S4, N1; S5, N2; and S6, N3 in Figs 3 and 4.
FUNDING
This work was supported by the Nagoya University microstructural characterization platform as a programme of the ‘Nanotechnology Platform’ of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan. In addition, this work was partially supported by the Japan Society for the Promotion of Science (JSPS) KAKENHI. Grant nos JP19K15823 (to T.O.), JP18K05603 (to K.Y.) and JP17H03757 (to M.T.).
ACKNOWLEDGEMENTS
We thank Mr Tsubasa Tanizawa for processing the image data, and Dr Hiroshi Miyake for reviewing the manuscript.
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