Original Research ARTICLE
Spatiotemporal Changes of Cyanobacterial Bloom in Large Shallow Eutrophic Lake Taihu, China
- 1State Key Laboratory of Lake Science and Environment, Nanjing Institute of Geography and Limnology, Chinese Academy of Sciences, Nanjing, China
- 2School of Environment and Civil Engineering, Jiangnan University, Wuxi, China
- 3Chongqing Institute of Green and Intelligent Technology, Chinese Academy of Sciences, Chongqing, China
- 4Research Center of Poyang Lake, Jiangxi Academy of Sciences, Nanchang, China
Lake Taihu is a large shallow eutrophic lake with frequent recurrence of cyanobacterial bloom which has high variable distribution in space and time. Based on the field observations and remote sensing monitoring of cyanobacterial bloom occurrence, in conjunction with laboratory controlled experiments of mixing effects on large colony formation and colonies upward moving velocity measurements, it is found that the small or moderate wind-induced disturbance would increase the colonies size and enable it more easily to overcome the mixing and float to water surface rapidly during post-disturbance. The proposed mechanism of wind induced mixing on cyanobacterial colony enlargement is associated with the presence of the extracellular polysaccharide (EPS) which increased the size and buoyancy of cyanobacteria colonies and promote the colonies aggregate at the water surface to form bloom. Both the vertical movement and horizontal migration of cyanobacterial colonies were controlled by the wind induced hydrodynamics. Because of the high variation of wind and current coupling with the large cyanobacterial colony formation make the bloom occurrence as highly mutable in space and time. This physical factor determining cyanobacterial bloom formation in the large shallow lake differ from the previously documented light-mediated bloom formation dynamics.
(1) Use of various tools such as remote sensing, field in situ observation and laboratory controlled experiments to characterize the cyanobacterial bloom occurrence related to the hydrodynamic actions in this large shallow and eutrophic lake.
(2) Moderate or small disturbance will promote colony enlargement through cell/colony aggregation due to the presence of extracellular polysaccharide (EPS). Cells/colonies aggregation increase the colony buoyance and speed up the surface visible cyanobacterial bloom formation.
(3) The large variation of wind-induced disturbance interacting with the buoyant colony aggregation determine the high spatiotemporal heterogeneity of cyanobacterial bloom distribution in this large shallow and eutrophic lake.
Most fresh water lakes in China are shallow and generally polluted with nutrient over-enrichment (Liu and Yang, 2012). One direct consequence of eutrophication is an increase in the occurrence of cyanobacterial blooms (Huisman et al., 2005). The majority of bloom-forming algal species are toxic (Chorus and Bartram, 1999) hence threatening drinking water safety (Guo, 2007; Qin et al., 2010) and disrupting the food chain (Micheli, 1999). Furthermore, decaying blooms may cause anaerobic conditions, which adversely affect aquatic life (Diaz and Rosenberg, 2008), resulting in odorous “black water” conditons (Qin et al., 2015; Zhang et al., 2016), accompanied by biodiversity decreases (Vonlanthen et al., 2012).
The formation of a cyanobacterial bloom is determined by sufficient algal biomass, cellular buoyancy and hydrodynamic conditions (Reynolds, 2006). Cyanobacterial biomass is determined by nutrient concentration (Schindler, 1974; Smith et al., 1999), water temperatures (Paerl et al., 2011; Deng et al., 2014), underwater light (Foy et al., 1976; Oliver, 1994; Reynolds, 2006). The physical conditions such as mixing intensity affect the bloom spatiotemporal distribution (Cao et al., 2006; Hunter et al., 2008; Wu et al., 2013). With absence of disturbance, cellular buoyancy depends on the size, shape, and density according to Stokes’s law (Oliver, 1994). A positive buoyancy causes cyanobacteria to float upward and aggregate at the water surface, forming dense surface blooms when disturbance is weak or absent (Ibelings, 1996; Wallace and Hamilton, 1999; Paerl et al., 2011). The formation of blooms allows cyanobacteria to gain more access to light than other species of algae, thereby suppressing the growth of competing algal taxa (Moisander et al., 2002; Huisman et al., 2004; Paerl et al., 2011). In contrast, during strong mixing, turbulence can entrain cyanobacteria below the euphotic zone where they experience sub-optimal light conditions (Huisman and Weissing, 1994; Wallace and Hamilton, 1999; Paerl et al., 2011). In some lakes, such intensive mixing can cause the dominant algal species shift from cyanobacteria to green algae and diatoms (Reynolds et al., 1983; Moreno-Ostos et al., 2009; Visser et al., 2016).
But the cyanobacteria bloom occurrence in Lake Taihu is quite different. As a large shallow and eutrophic lake, the cyanobacteria bloom occurrence is characterized by rapid changes in situation and extent, which is likely coming and going without a trace. The duration of the cyanobacteria bloom often lasted a few hours (Supplementary Table S1 and Supplementary Figure S1), similar phenomenon was found in Lake Chao, the fifth largest freshwater lake in China (with area 825 km2 and mean depth ∼4 m) (Supplementary Table S2). It was, therefore, very difficult to monitor, track, simulate and predict. The bloom forming species in Lake Taihu is buoyant Microcystis which can account for 90% of total phytoplankton biomass during summer (Chen et al., 2003). Meanwhile, the cyanobacteria cells present in field in a form of large colonies (a number of cells stick together) which take an overall majority (Wu and Kong, 2009). It is supposed that the extracellular polysaccharide (EPS) supports aggregation of cells (Xu et al., 2013; Li et al., 2013). Because the large colonies have high buoyancy so as to sustain the colonies floating at water surface, the bloom forming cells/colonies are likely more susceptible to wind induced water movement. Here we hypothesized that the high spatiotemporal variation of cyanobacterial bloom in this large shallow lake are caused by wind-induced hydrodynamic mixture and advection associated with the presence of EPS. In this study, we examined the wind induced physical effects on the cyanobacterial bloom formation via field observations and laboratory controlled experiments. The purpose of this paper is to address the dynamics of bloom change in space and time in Lake Taihu, particularly the wind-induced mixing effects on the formation of cyanobacterial colonies and dense aggregation bloom at water surface.
Data and Methods
The Study Site
Lake Taihu, the third largest freshwater lake in China, is located in the Yangtze River Delta region. It’s area is 2338 km2, mean depth 2 m, and the maximum depth is no more than 3 m with flat-bottomed bathymetry. There is no persistent stratification during summertime. Its eutrophication began in the 1980s (Qin et al., 2007), and cyanobacteria bloom coverage has gradually extended from Meiliang Bay (Chen et al., 2003) to the entire northwest zone of the lake. The bloom-forming species is high buoyant Microcystis which account for overwhelming majority during summer (Chen et al., 2003). The nutrient enrichment combined with warm spring resulted in the earlier occurrecne of intensive cyanobacterial bloom which caused the drinking water crisis in late May 2007 (Qin et al., 2010). With a series of pollution control measures implemented since 2007 (Stone, 2011), the water quality has not further deteriorated, but the notorious harmful cyanobacterial blooms still persist and the bloom induced anaerobic “black water” recur throughout summer in this lake (Zhang et al., 2016).
In Situ Observation of Microcystis Colony Formation and Cyanobacterial Bloom Occurrence
To investigate the impact of wind-induced mixing on the cyanobacteria bloom occurrence, multi-parameter monitoring was conducted synchronously during both Typhoon Morakot (August 12–14, 2009) and Typhoon Soulik (July 12–13, 2013). Instruments to record wind velocity and direction, at a frequency of every 10 min, were moored at the pier end in Taihu Laboratory for Lake Ecosystem Research (TLLER), Chinese Academy of Sciences (CAS) nearby the Meiliang Bay in Lake Taihu (Figure 1). We were particularly interested in the vertical migration speed of Microcystis colonies, therefore, an Acoustic Doppler Current Profilers (ADCP) was deployed at the bottom of the water column near Wuguishan Islet to record three-dimensional current velocity (Figure 1). At the same site, multi-function water quality sensors (YSI6600) were deployed near the water surface (ca. 20 cm under surface) and the bottom (50 cm above bottom of lake). The sensors of water quality parameters, including pH, conductivity, turbidity, were recording with a 10 min resolution, while the chlorophyll-a concentration was recorded every 30 min by in vivo fluorescent light detectors which need to be adjusted before deploying.
FIGURE 1. Location of Lake Taihu, Taihu Laboratory for Lake Ecosystem Research (TLLER) and Wuguishan Islet for Acoustic Doppler Current Profiler (ADCP) and multi-parameter water quality instrument deploying.
Additionally, cyanobacteria colonies were sampled during typhoon Soulik at the end of pier in TLLER (Figure 1). Samples were taken at noon of July 12 and 13, 2013, followed by a period during which the sampling interval was 12 h from the midnight of July 13 to the noon of July 15, 2013. Samples were also collected around midnight of July 15 and in the morning of July 16, 2013. The depths of sampling included the bottom layer (0.1 m above sediments), middle layer (1.2 m above sediments) and surface layer (2 m above sediments). The colony size of Microcystis were counted from at least 30 colonies (>100 cells) with microscopy (Nikon E200). Microscopic examination showed that the dominant phytoplankton species were Microcystis aeruginosa, M. flos-aquae, and M. wesenbergii during observations, and the proportion of Microcystis accounted for more than 90% of total phytoplankton biomass. For convenience, we took the concentration of Chl a to represent Microcystis biomass.
In Situ Experiment of Mixing Induced by Wind-Wave on Colony Size of Microcystis in Lake Taihu
In order to examine whether the disturbance by wind is significant to promote the formation of Microcystis colony, an experiment was carried out under the pier in TLLER on September 23, 2017. Some M. aeruginosa and M. flos-aquae colonies separated from Meiliang Bay, Lake Taihu, were cultured with BG11 (TN = 50 mg/L, TP = 2.5 mg/L) for 2 months followed by extended 2 months culturing with modified BG11 (TN = 10 mg/L, TP = 0.5 mg/L); and a samples with single cell, unicells and small colonies of pure Microcystis were obtained. About 500 ml cultured pure M. aeruginosa (1.59 × 105 cells/mL) and M. flos-aquae (1.59 × 105 cells/mL) were transferred to pre-cleaned plastic bottle. Three 500 ml bottles were fixed to iron pile of the nearby as control of no wind induced disturbance; while the other three bottles as treatments, tethered to cement pile by rope, swing with the water movements induced by wind (Supplementary Figure S2). This experiment took 48 h. The wind speeds were measured every 1 h during experiment. Microcystis biomass, Microcystis colony size and EPS concentration in the bottles were measured at-beginning and at-end of experiment. The content of soluble extracellular polysaccharide (sEPS) and bound extracellular polysaccharide (bEPS) were quantified spectrophotometrically by the anthrone method (Herbert et al., 1971). Samples of M. aeruginosa (5 mL) and M. flos-aquae (5 mL) were preserved with Lugol’s iodine solution. After the M. aeruginosa and M. flos-aquae settled for 48 h, samples of M. aeruginosa (5 mL) and M. flos-aquae were concentrated (1 mL). Then M. aeruginosa and M. flos-aquae colony size was measured (400× magnification) with a Nikon E200 microscope and QCapture pro. software. The mean colony size of M. aeruginosa and M. flos-aquae were measured under microscopy with at least 50 colonies.
Effects of in Situ Simulated Mixing on Colony Size of Microcystis in the Lake Taihu
For further investigating the influence of disturbance on the formation of Microcystis colony, a simulated perturbation experiment was carried out in July in TLLER. Similarly, we took six big plastic barrels (three for control and three for treatment) and each barrel has 90 cm in diameter and 80 cm in height (Supplementary Figure S3). All barrels were filled with water containing Microcystis colonies taken from Meiliang Bay, Lake Taihu, to the depth of 60 cm. Total nitrogen (TN) and total phosphorus (TP) concentrations in barrels were adjusted with addition of NaNO3 and K2HPO4 3H2O to 5 mg/L for TN and 0.25 mg/L for TP which were almost two times of TN and TP concentration in Meiliang Bay, Lake Taihu. Six barrels were cultured in static condition during the first 5 days. During this period, samples were taken at 10:00 am every morning from two layers at the surface (50 cm above bottom) and the bottom (0 cm above bottom). From the 6th day, the treatments were imposed with wave produced by mini wave action generators (WP-60, Triopo Electric Co. Ltd.) which were deployed at 10 cm below the surface. The wave was produced with a frequency of 1 Hz and the maximum wave height was 5 cm (Supplementary Figure S3). Wave disturbances were lasting for 24 h. During the disturbance period, water samples were taken at 3, 6, 12, and 24 h after the beginning; and during the post-disturbance (wave generator stopped to work but the wave effects still existed), samples were taken at 3, 6, 12, 24, and 48 h. Sample analysis for Microcystis biomass and colony size and the concentrations of EPS were determined as described in Section “In Situ Experiment of Mixing Induced by Wind-Wave on Colony Size of Microcystis in Lake Taihu.” The concentrations of Chl a, TN and TP were determined by spectrophotometry. Microscopic examination showed that Microcystis was the overwhelming dominant species during experiment.
Effects of Simulated Mixing on the Colony Size of Microcystis in Laboratory
Single colony of M. aeruginosa and M. flos-aquae were isolated from lake water in Meiliang Bay (dominated by Microcystis bloom) in Lake Taihu and were cultured with BG-11 medium. Two months later, unialgal cultures of M. aeruginosa and M. flos-aquae were transferred to modified BG-11 medium (TN = 50 mg/L, TP = 2.5 mg/L), respectively. Until the beginning of experiment, M. aeruginosa and M. flos-aquae, present as single-cells, paired-cells and small colonies, were cultured in modified BG-11 media for 5 months. At the beginning of the experiment, 150 mL M. aeruginosa (4.83 × 106 cells/mL) and M. flos-aquae (1.78 × 106 cells/mL) were transferred to 500 mL Erlenmeyer flasks containing 200 mL modified BG-11 medium. Considering the velocities (0.005–0.077 m/s) of Lake Taihu (Zhou, 2016), five different mixing intensities were designed as following: 0, 50, 100, 200, and 400 rpm, which were corresponding to velocities of 0, 0.16, 0.32, 0.64, and 1.28 m/s (Camacho et al., 2007; Guadayol et al., 2009; Gallardo Rodríguez et al., 2009), respectively. The control had three 500 ml flasks with shaking intensity of 0 rpm. Each treatment also had three 500 ml flasks (triplicate) placed on shaking incubator. There were four shaking incubators with shaking intensities of 50, 100, 200, and 400 rpm. The shaking experiment lasted for 24 h at 25°C and cool/white fluorescent lights at an intensity of 40.5 mol m-2 s-1 with a light-dark cycle of 12:12 h. The total concentration of nitrogen and phosphorus in all treatments and control were maintained about 50 and 2.5 mg/L, respectively. Samples were taken before and after the experiment. The measurements of colony size, biomass of M. aeruginosa, concentrations of Chl a, EPS, TN, and TP were the same as described in Section “In Situ Experiment of Mixing Induced by Wind-Wave on Colony Size of Microcystis in Lake Taihu” above.
Measurements of Vertical Movement Velocity for Different Size Cyanobacteria Colonies
Large size colony has high buoyancy to overcome the mixing and gravity to float at water surface and form visible bloom. To measure the upward movement velocity of different size Microcystis colonies, the field samples of Microcystis were taken with net filtering (mesh sizes were 425, 100, 64, and 20 μm) to obtain five different size classes of Microcystis colonies (>425 μm, 100–425 μm, 64–100 μm, 20–64 μm, and <20 μm). For each colony size group, the cell numbers and proportion to all colonies were estimated before the experiment. A plexiglass column (1 m in height and 0.1 m in diameter) was used to measure the upward movement velocity of different size colonies. There was an inlet for injection at the column bottom and five sampling outlets distributed along the column every 0.2 m. The column was filled with distilled water. Different size colony samples were injected at the bottom. After 1 (>425 μm), 3 (100–425 μm), and 10 min (<100 μm), samples were taken from 5 sampling outlets simultaneously and the density of algae was counted with microscope. Five different size Microcystis colonies were injected into the columns separately. Each colony size experiment had triplicate.
The floating velocity of different size colonies was calculated as follows:
where Bt (the total biomass) equal to the product of injection density and injection volume, Bi (the biomass of each outlet) was calculated by the cell density of each outlet by 1/6 of the volume of plexiglass column, vi (floating velocity of each outlet) were calculated by the height of each sampling outlet divided by experimental time.
Remote Sensing Technique to Monitor Cyanobacteria Bloom Intensity Changes in Time and Space
Remote sensing about the cyanobacterial bloom area were used to investigate the cyanobacterial bloom changes in space. The lowest cyanobacteria biomass at which the bloom could be detected by satellite was equivalent to the Chl a concentration around ∼101 mg/m3. All the remote sensing images of cyanobacteria bloom were obtained from NASA1. The interpretation of MODIS images was according to the re-projection and geometric correction via ERDAS 9.1, and the information of blooms was retrieved by means of the ratio of near-infrared and red spectrum (Ma et al., 2008; Duan et al., 2009).
In Situ Field Monitoring of Cyanobacteria Bloom During Typhoon Morakot
Lake Taihu basin and delta of Changjiang River (Yangtze River) often experience typhoon during summer. These typhoons normally formed in the tropical or subtropical Pacific Ocean and moved westward or northwestward and influenced the eastern China coastal zone. Typhoon Morakot passed Lake Taihu during August 11–14, 2009. Its effects on the lake started in the early morning of August 11. The dominant wind directions were westerly and northwesterly and the maximum wind speed occurred in the evening of August 11 at 11.8 m s-1 (Figure 2A), then the wind speed gradually dropped until clam condition in the evening of August 12, while the wind direction shifted to east and northeast. During the typhoon, the near-surface vertical current velocity measured by Acoustic Doppler Current Meter (ADCP), was typically mixing with up and down movement and a maximum velocity was about 0.5 cm/s (Figure 2B) to correspond to the high wind speed. After the typhoon, the vertical direction current turned to be upward uniformly and the maximum velocity reached 1.0 cm/s (Figure 2B). Because of the measured vertical velocity representing the moving speed of particulate matter in the water column (Holdaway et al., 1999). Thus the measured vertical velocity actually indicated the cyanobacteria colonies moving speed in the water column. In situ observation after the typhoon showed that the algal cells/colonies generally ascended to the water surface, instead of sinking, representing that cyanobacteria cells or colonies moving upward was driven by the buoyancy.
FIGURE 2. Observations during Typhoon Morakot in August 12–13, 2009 in Lake Taihu. (A) The wind speed and wind direction. (B) Speed of suspended particulate matter (cyanobacterial colonies) moving up and down recorded by ADCP. (C) Chlorophyll-a concentration at the surface layer and the bottom layer.
Interestingly chlorophyll-a concentrations differed between the layers at near-bottom and near-surface during the post-typhoon. During the typhoon peak period (06:00 h 11 to 06:00 h of August 12), the chlorophyll-a concentrations was almost identical in the water column, suggesting well-mixed conditions during this period (Figure 2C). However, after the typhoon, the chlorophyll-a concentration at near-surface layer was increased and that near the bottom layer declined (Figure 2C), indicating that cyanobacteria cells/colonies in water column started to differentiate and aggregate at the water surface, which probably a precursor of the cyanobacteria bloom occurrence. Remote sensing images in the morning of August 12, 2009 (during Typhoon Morakot) showed the area of the bloom was only 92 km2 (Supplementary Figure S4A), which rapidly expanded to 391 km2 in the morning of August 13 (Supplementary Figure S4B).
Field Observation of Impact of Typhoon Soulik on Cyanobacteria Colony Formation
Typhoon Soulik affected Lake Taihu during July 12–17, 2013. The period could be divided into three stages according to the wind speed. The pre-typhoon period (00:00–22:00 of July 12), the wind speed increased gradually and average wind speed was 3.82 m s-1 (Figure 3A). During the typhoon period (from 22: 00 h, 12–18:00 h, July 15) when a high wind speed persisted with average of 6.63 m s-1 and a maximum speed of 13.8 m s-1 (at 18:00 h, July 13) (Figure 3A). The post-typhoon period (18:00 h, 15-00:00 h, July 17) had an average wind speed of 5.26 m s-1 which gradually reduced to 1 m s-1 near the end of the typhoon (Figure 3A). In situ measurements revealed that the mean size of Microcystis colonies in the water column increased from 32.8 to 69.4 μm within 48 h (Figure 3B).
FIGURE 3. Wind velocity (A) and average colony size of Microcystis spp. changes in the water column (B) before and after the Typhoon Soulik.
At the same time, remote sensing satellite images showed that little of the cyanobacteria blooms could be seen in the pelagic area of the lake during the Soulik Typhoon peak period from July 12 to July 14; however, around noon of July 17, after the typhoon, blooms occurred with coverage of 288 km2 (Supplementary Figure S5).
In Situ Experiment of Mixing Induced by Wind-Wave on Microcystis Colony Formation in Lake Taihu
During this experiment, the mean wind speed was 3.15 m/s (range 1.33–4.83 m/s) (Figure 4A). In the treatments (the bottles were not fixed), the colony size of M. aeruginosa and M. flos-aquae increased quickly after mixing induced by wind-wave for 48 h. The colony size of M. aeruginosa in controls (the bottles were fixed) and treatments were 23.6 (±1.2) and 59.0 (±1.8) μm, respectively (Figure 4B). The colony size of M. flos-aquae in controls and treatments were 25.5 (±1.1) and 40.8 (±1.7) μm, respectively (Figure 4C). ANOVA analysis showed that the difference of M. aeruginosa and M. flos-aquae colony sizes between control and treatment were significantly (p < 0.01) (Figures 4B,C). Also, ANOVA analysis showed that the EPS concentrations of M. aeruginosa and M. flos-aquae in treatments were significantly higher than that in controls (p < 0.01) (Figures 4D,E).
FIGURE 4. In situ experiments about mixing effect on colony size and EPS (extracellular polysaccharide (EPS)) concentrations, and colony size of Microcystis at the pier end of TLLER. (A) Wind speed during experiment. (B) Colony size of Microcystis aeruginosa in control and treatment. (C) Colony size of M. flos-aquae in control and treatment. (D) EPS concentration of M. aeruginosa in control and treatment. (E) EPS concentration of M. flos-aquae in control and treatment; error bars was indicated by ± SD ∗p < 0.05, ∗∗p < 0.01, n = 3).
Effects of in Situ Simulative Mixing on Colony Size of Microcystis in the Lake Taihu
Before the disturbance, the Microcystis spp. colony size in the control and treatment decreased gradually (Figure 5A). To the 6th day when the disturbance experiment started, the size of Microcystis in the control and treatment had reduced from 46.8 μm and 45.4 μm to 19.8 μm and 20.2 μm, respectively. During the disturbance experimental period, the mean Microcystis colony size decreased continuously in control while it increased rapidly to 68.4 μm after 24 h disturbance (Figure 5A). At the end of experiment (48 h after 24-h disturbance), the average colony size in treatment was 70.1 μm, while the mean colony size in control was 12.6 μm (Figure 5A). The colony size difference between control and treatment was significant (p < 0.01). After 24-h disturbance, the EPS concentration in the control and the treatment were 1.26 and 1.49 ng/cell, respectively, which was significantly different (p < 0.05) (Figure 5B). Before the experiment, the initial averaged Chl a concentration at the surface and the bottom in the experimental barrels were 36.8 and 33.4 μg/L (Figure 5C), respectively. There was no significant difference (p > 0.05). During the disturbance period, the surface concentration of Chl a decreased sharply to 51.2 μg/L while the Chl a concentration at bottom increased rapidly to 42.1 μg/L (Figure 5D), which was no significant difference (p > 0.05). At the end of the experiment (48 h after 24-h disturbance), the cyanobacterial colonies returned to water surface resulted in Chl a concentration of 102.6 μg/L at surface, which was higher than that in control (Figure 5D); while the Chl a near the bottom was only 28.6 μg/L which differed significantly from that at water surface (p < 0.05). The stratification recurred at the end of experiment in treatment (Figure 5D).
FIGURE 5. Simulation of mixing effect on Microcystis spp. colony size, EPS concentration and vertical distribution of Chl a in plastic barrels in TLLER. (A) Colony size in control and treatment (including 24-h disturbance during experiment) change with time. (B) EPS concentration in control and treatment (including 24-h disturbance during experiment) change with time. (C) Surface and bottom Chl a concentration in control change with time. (D) Surface and bottom Chl a concentration in treatment (including 24-h disturbance during experiment) change with time; error bars was indicated by ±SD (∗p < 0.05, ∗∗p < 0.01, n = 3).
Effects of Simulative Mixing on the Colony Size of Microcystis in Laboratory
In this experiment, the colony size of M. aeruginosa and M. flos-aquae in 50, 100, 200, and 400 rpm experiments were significantly larger than that in control (p < 0.05) (Figures 6A,C) after 24-h continuously mixing. The colony size of M. aeruginosa in control, 50, 100, 200, and 400 rpm experiments were 23.6 (±1.8), 50.1 (±8.6), 92.9 (±4.8), 67.8 (±10. 9), and 37.3 (±3.9) μm, respectively (Figure 6A and Supplementary Figure S6). The colony size of M. flos-aquae in control, 50, 100, 200, and 400 rpm were 10.6 (±0.6), 24.0 (±1.2), 33.0 (±1.2), 19.2 (±1.6), and 14.4 (±1.8) μm, respectively (Figure 6C). Both Microcystis species showed an increase firstly with the intensity of mixing followed by a decrease when the mixing intensity larger than 100 rpm (Figures 6A,C). In addition, ANOVA analysis indicated that the EPS concentration of M. aeruginosa and M. flos-aquae in all treatments were significantly higher than that in controls (p < 0.01) (Figures 6B,D).
FIGURE 6. Effects of different mixing intensity (four shaking intensity and control) on colony size and EPS of Microcystis. (A) Mean M. aeruginosa colony size of control and 50, 100, 200, and 400 rpm. (B) Mean M. aeruginosa EPS concentrations of control, 50, 100, 200, and 400 rpm. (C) Mean M. flos-aquae colony size of control and 50, 100, 200, and 400 rpm. (D) Mean M. flos-aquae EPS concentrations of control and 50, 100, 200, and 400 rpm; error bars was indicated by ±SD (∗p < 0.05, ∗∗p < 0.01, n = 3).
Vertical Migration Rate Measurement for Different Size of Cyanobacterial Colony
Experimental results showed that the large size colony (cell count of each colony > 100) accounted for an overwhelming majority in colony size distribution, which was consistent with our field observations (Figure 7), and floating rates increased with the colony size. The largest cell colony (>425 μm in diameter) had the floating rate of up to 0.77 ± 0.23 cm s-1 (Supplementary Table S3). The largest proportion of colony size occurred at colony diameters between 100 and 425 μm with a high floating rate of 0.30 ± 0.08 cm s-1 (Figure 7 and Supplementary Table S3), while colony sizes <20 μm were solitary cells or small colonies with floating rates about 0.0002 cm s-1 (Supplementary Table S3).
FIGURE 7. Proportion and floating rate of different Microcystis spp. colony sizes in the floating rate measurement experiment.
Our field observations and laboratory control experiments suggested that wind induced mixing increased the cyanobacterial colonies size resulted in the increase in colony buoyancy. With the mixing decrease, these large colonies floated upward to surface very quickly to form visible bloom. Lots of researches showed that a surface bloom development will occur only when the cyanobacterial colony buoyancy can overcome the mixing intensity (Denman and Gargett, 1983; Bormans and Condie, 1998; Visser et al., 2016). However, the relationship between the wind-induced hydrodynamic action and cyanobacterial bloom occurrence was not well addressed largely because this relation was simply assumed as a physical process, i.e., the interaction between mixing intensity and the buoyance of cyanobacterial colony. But our field observations and experiments found that the small and moderate physical disturbance will promote the large colony formation and increase the colony buoyance. It can explain why the algal aggregation move upward during the post-typhoons. Field in situ observations also found that the surface and bottom Chl a concentration were almost same during peak typhoon period indicating that the water column was fully mixed (Figure 2C). Meanwhile, the ADCP recorded near-surface vertical movement of colonies was bi-direction. During post-typhoon period, cyanobacterial colonies unifromly ascended to aggregate at water surface (Figure 2B) at speed about 0.5 cm/s near surface and 0.3 cm/s near bottom (Wu et al., 2013), which was much higher than previous reported about 10-4 m/s (Reynolds et al., 1987) and similar with Visser et al. (1997) documented as 0.7 cm/s for the colony diameter ∼400 μm. This higher vertical speed mainly caused by the buoyancy of large colones of Microcystis (Oliver, 1994; Wallace and Hamilton, 1999; Wu and Kong, 2009). According to our investigations in TLLER during July and October of 2013, the large colony (>96 μm) near the water surface took overwhelming majority ranging from 54.4 to 89.2% during different wind speed (Figure 8). By our experiment, the ascent rate of big colonies (100–425 μm) was about 1500 times of small colonies (<20 μm) (Figure 7 and Supplementary Table S3), which can explain why the cyanobacterial colonies in the field could congregate quickly at water surface within hours in lake Taihu (Supplementary Table S1 and Supplementary Figure S1). According to the Stoke’s law, the ascent rate of cyanobacterial colonies was determined by the spherical size (indicated as radius) and the density difference between water and Microcystis colony (Reynolds et al., 1987). For small colony (<20 μm) of Microcystis, almost all cells can get the same amount of light; for large colony (>100 μm) of Microcystis, light availability within colony is far less than at the surface of colony, the larger the colony size, the lower the light availability inside the colony, and the lower the colony density. Thus large Microcystis colony has low density and high buoyancy. As the large colonies of Microcystis have greater buoyancy and higher ascent velocity in the water column compared with solitary cells or small colonies (Xiao et al., 2012), large colonies could move to the water surface in a much shorter time, leading to the “outbreak” of Microcystis blooms.
FIGURE 8. Two in situ observations about the colony size composition vs. wind speed at the end of pier in TLLER in (A) July 2013 and (B) October 2013.
Traditionally, the cyanobacteria cells and colonies aggregation at the water surface results from its metabolism through the gas-vacuolate buoyance adjustment (Reynolds et al., 1987; Oliver, 1994). This accomplished by carbohydrates synthesized during the day increase the cell density to cause cells sink. Conversely carbohydrates are consumed at night, decreasing the cell density and providing positive buoyance to form blooms in the next morning (Visser et al., 1997). If the wind speed were greater than 3 m/s, wind-induced mixing would result the surface visible bloom vanishment (George and Edwards, 1976; Webster and Hutchinson, 1994; Brookes et al., 2003; Wu et al., 2013).
Previous studies already noted that the M. aeruginosa colony size can be affected by turbulence-induced aggregation (Naselli-Flores and Barone, 2003; O’Brien et al., 2004; Regel et al., 2004). Our laboratory experiments suggested that persistent and moderate hydrodynamic disturbance can cause aggregation of M. aeruginosa and M. flos-aquae, and small colonies become larger colonies. But disturbance will not take effect for the solitary cell or unicell on the formation of large colonies via collision (data not shown). This was attributed to the presence of extracellular polysaccharides (EPS) which played a critical role in the large colony formation via collision. EPS are mainly found in mucilage or the cell’s sheath. It can affect the ‘stickiness’ of the cell surface, and further influence large colony formation of Microcystis (Yang et al., 2008; Xu et al., 2013; Zhang et al., 2014; Zhu et al., 2014; Pannard et al., 2016). It was documented that the concentration of EPS was significantly higher in colony than in single cell (Li et al., 2013). Our observations suggested that EPS concentration in all mixing experiments were significantly higher than that in controls (Figures 4–6). Increasing of EPS after mixing may explain why colony size of Microcystis spp. enlarged in all treatments. The large colony formation in this large turbid lake, therefore, was caused by cell-colony or colony-colony aggregation, which was much faster than cell division and proliferation. The spatial distribution of EPS concentration in this lake was highly overlapping the bloom recurrence area (Liu et al., 2014), suggesting that turbulence induced colony aggregation maybe the primary reason for large colony formation and bloom recurrence. In addition, because Lake Taihu is a shallow lake, wind induced disturbance make the sediment resuspension frequently and lead to sharp decrease in light availability underwater, which further result in more gas vesicles of Microcystis cells (Walsby et al., 1991). Then Microcystis cells or colonies will ascend quickly after the wind halt. But intensive disturbance would disaggregate the large colonies (O’Brien et al., 2004) as it was shown in mixing simulation treatment with rotation rate larger than 100 r/min (Figures 6A,C).
For a large shallow lake, quiescent conditions rarely sustain for few hours, thus the cyanobacteria bloom coverage and distribution detected by the satellites or human visions were highly spatiotemporal changeable. The occurrence of cyanobacteria bloom, the location and extent, is the interaction result between colonies buoyancy, mixing intensity and horizontal migration by currents. The location and extent of the bloom, frequently present as a moving patchiness at the surface, can be highly variable. This high variability is originated from the wind-induced waves and currents. Our observation found that the wind speed and direction frequently varied (Supplementary Figure S7) because of the influence from rough ground surface, thermal contrast between water-land, etc. Correspondingly, the water current was showing similar variability to winds (Supplementary Figure S8). Because of the high variability of winds and water currents in this large shallow lake, it was concluded that the high variability of cyanobacteria blooms originated mostly from the highly changeable wind forcing. Thus the wind induced hydrodynamic actions in Lake Taihu not only determine the cyanobacteria colonies ascent to form surface visible bloom, but also determine the high spatiotemporal heterogeneity of cyanobacterial bloom, and enhance this heterogeneity through the influence on the large colony formation.
Based on the above observations and experiments, we proposed a four-stage of cyanobacteria bloom occurrence in this large shallow eutrophic lake. The first stage is the Microcystis cell division and proliferation. During this stage, the cyanobacterial unicells grow and divide, forming small colonies under favorable environmental conditions, such as high temperature, sufficient light and nutrient supply. Small colony will be formed with the secretion of tightly bound extracellular polysaccharides. The second stage is the formation of large cyanobacteria colonies. During this stage, the considerable cells and small-colonies in the water column will increase in size through aggregation. The presence of wind induced disturbance will produce large colonies or disaggregate large colonies. This aggregation and disaggregation process would alternatively happen in the water column until the wind speed declined and a great amount of large colonies formed. The third stage includes the cyanobacteria colonies ascending to form a visible bloom or scum at the water surface when the wind become weak. Moreover, a great amount of larger size colonies formed in water column by mixing and the enhanced buoyancy of larger size colonies allows them to fast aggregate at the water surface. The fourth stage is the onset of more persistent cyanobacteria blooms. In this stage, the blooms drift and aggregate driven by the surface currents and accumulate in the onshore zone, where downward migration is restricted by shallow depth. According to the wind speed measurement in Taihu Laboratory for Lake Ecosystem Research (TLLER), the frequency of calm weather condition (wind speed < 3 m s-1) occurs about one sixth of the time. Thus, the wind-induced physical factors such as turbulence may dominate during cyanobacterial bloom occurrence in this large shallow lake.
All authors listed have made a substantial, direct and intellectual contribution to the work, and approved it for publication.
This work was supported by the National Natural Science Foundation of China under Grants 41621002, 41230744, 41471021, and 41101053 and Chinese Academy of Sciences under Grants QYZDJ-SSW-DQC008. We acknowledge the TLLER for observation data obtained by the high frequency automatic online monitoring station which attributed to the International Collaborative Project GLEON, and additional support provided by Chinese Academy of Sciences Grant KZCX2-YW-419.
Conflict of Interest Statement
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
We thank Shixin Wang and Ronghua Ma for providing the remote sensing satellite images. We also thank Wenhao Ding for helping to draw the wind and current diagram, Dr. Feng Li, Prof. David Hamilton, and Prof. Hans Paerl for English editing and constructive suggestions, and the five reviewers for very helpful comments.
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fmicb.2018.00451/full#supplementary-material
FIGURE S1 | Variation in cyanobacteria bloom area in Lake Taihu by remote sensing detection at 10:04 h on June 13, 2009 (A) and 13:16 h on June 13, 2009 (B).
FIGURE S2 | The spot picture of in situ experiment of mixing induced by wind-wave on colony size of Microcystis in Lake Taihu.
FIGURE S3 | The spot picture of in situ simulative mixing on colony size of Microcystis in the Lake Taihu.
FIGURE S4 | The satellite image revealed the cyanobacterial bloom occurrence during post Morak Typhoon. (A) Little bloom with area 92 km2 was detected at 10:27 am, August 12, 2009, when the typhoon peak had passed. (B) Large bloom with area 391 km2 was detected at 11:09, August 13, 2009.
FIGURE S5 | The satellite images of cyanobacterial bloom during the Typhoon Soulik passed Lake Taihu in July 2013. The left: image of bloom at 13:10 h, July 12, 2013; the middle: image of bloom at 11:15 h, July 14, 2013; the right: image of bloom at 11:50 h, July 17, 2013.
FIGURE S6 | The colony pictures of M. aeruginosa in controls, 50, 100, 200, and 400 rpm groups after continuing mixing for 24 h in this experiment.
FIGURE S7 | The wind velocity and wind direction measurement at the lake center during July 14–August 17, 2015.
FIGURE S8 | The water current (about 200 cm above bottom) measurement at the lake center during July 14–August 17, 2015.
TABLE S1 | Satellite detected cyanobacterial bloom area changes in a short period in Lake Taihu.
TABLE S2 | Satellite detected cyanobacterial bloom area changes in a short period in Lake Chaohu.
TABLE S3 | Proportion and floating rate of different colony sizes of Microcystis.
Brookes, J. D., Regel, R. H., and Ganf, G. G. (2003). Changes in the photo-chemistry of Microcystis aeruginosa in response to light and mixing. New Phytol. 158, 151–164. doi: 10.1046/j.1469-8137.2003.00718.x
Camacho, F. G., Rodríguez, J. J. G., Mirón, A. S., García, M. C. C., Belarbi, E. H., and Grima, E. M. (2007). Determination of shear stress thresholds in toxic dinoflagellates cultured in shaken flasks: implications in bioprocess engineering. Process Biochem. 42, 1506–1515. doi: 10.1016/j.procbio.2007.08.001
Cao, H. S., Kong, F. X., Luo, L. C., Shi, X. L., Yang, Z., Zhang, X. F., et al. (2006). Effects of wind and wind-induced waves on vertical phytoplankton distribution and surface blooms of Microcystis aeruginosa in Lake Taihu. J. Freshw. Ecol. 21, 231–238. doi: 10.1080/02705060.2006.9664991
Chen, Y. W., Qin, B. Q., Dokulil, M. T., and Teubner, K. (2003). Long-term dynamics of phytoplankton assemblages: Microcystis-domination in Lake Taihu, a large shallow lake in China. J. Plankton Res. 25, 445–453. doi: 10.1093/plankt/25.4.445
Deng, J. M., Qin, B. Q., Paerl, H. W., Zhang, Y. L., Ma, J. R., and Chen, Y. R. (2014). Earlier and warmer springs increase cyanobacterial (Microcystis spp.) blooms in subtropical Lake Taihu, China. Freshw. Biol. 59, 1076–1085. doi: 10.1111/fwb.12330
Duan, H., Ma, R. H., Xu, X. F., Kong, F. X., Zhang, S. X., Kong, W. J., et al. (2009). Two-decade reconstruction of algal blooms in China’s Lake Taihu. Environ. Sci. Technol. 43, 3522–3528. doi: 10.1021/es8031852
Foy, R., Gibson, C., and Smith, R. (1976). The influence of daylength, light intensity and temperature on the growth rates of planktonic blue-green algae. Br. Phycol. J. 11, 151–163. doi: 10.1080/00071617600650181
Gallardo Rodríguez, J. J., Sánchez Mirón, A., García Camacho, F., Cerón García, M. C., Belarbi, E. H., Chisti, Y., et al. (2009). Causes of shear sensitivity of the toxic dinoflagellate Protoceratium reticulatum. Biotechnol. Prog. 25, 792–800. doi: 10.1002/btpr.161
George, D. G., and Edwards, R. W. (1976). The effect of wind on the distribution of chlorophyll a and crustacean zooplankton in a shallow eutrophic reservoir. J. Appl. Ecol. 13, 667–690. doi: 10.2307/2402246
Guadayol,Ò., Peters, F., Stiansen, J. E., Marrasé, C., and Lohrmann, A. (2009). Evaluation of oscillating grids and orbital shakers as means to generate isotropic and homogeneous small-scale turbulence in laboratory enclosures commonly used in plankton studies. Limnol. Oceanogr. Methods 7, 287–303. doi: 10.4319/lom.2009.7.287
Holdaway, G. P., Thorne, P., Flatt, D., Jones, S. E., and Prandle, D. (1999). Comparison between ADCP and transmissometer measurements of suspended sediment concentration. Cont. Shelf Res. 19, 421–441. doi: 10.1016/S0278-4343(98)00097-1
Huisman, J., Sharples, J., Stroom, J. M., Visser, P. M., Kardinaal, W. E. A., Verspagen, J. M. H., et al. (2004). Changes in turbulent mixing shift competition for light between phytoplankton species. Ecology 85, 2960–2970. doi: 10.1890/03-0763
Hunter, P., Tyler, A. N., Willby, N. J., and Gilvear, D. J. (2008). The spatial dynamics of vertical migration by Microcystis aeruginosa in a eutrophic shallow lake: a case study using high spatial resolution time-series airborne remote sensing. Limnol. Oceanogr. 53, 2391–2406. doi: 10.4319/lo.2008.53.6.2391
Ibelings, B. W. (1996). Changes in photosynthesis in response to combined irradiance and temperature stress in cyanobacterial surface water blooms. J. Phycol. 32, 549–557. doi: 10.1111/j.0022-3646.1996.00549.x
Li, M., Zhu, W., Gao, L., and Lu, L. (2013). Changes in extracellular polysaccharide content and morphology of Microcystis aeruginosa at different specific growth rates. J. Appl. Phycol. 25, 1023–1030. doi: 10.1007/s10811-012-9937-7
Liu, L. Z., Qin, B. Q., Zhu, G. W., Zhang, Y. L., Gao, G., Gong, Z. J., et al. (2014). Distribution of dissolved acidic polysaccharides (dAPS) during cyanobacteria blooms in northern Lake Taihu. Limnology 16, 21–29. doi: 10.1007/s10201-014-0435-2
Ma, R. H., Kong, F. X., Duan, H. T., Zhang, S. X., Kong, W. J., and Hao, J. Y. (2008). Spatio-temporal distribution of cyanobacteria blooms based on satellite imageries in Lake Taihu, China. J. Lake Sci. 20, 687–694. doi: 10.18307/2008.0605
Moreno-Ostos, E., Cruz-Pizarro, L., Basanta, A., and George, D. G. (2009). The influence of wind-induced mixing on the vertical distribution of buoyant and sinking phytoplankton species. Aquat. Ecol. 43, 271–284. doi: 10.1007/s10452-008-9167-x
Naselli-Flores, L., and Barone, R. (2003). Steady-state assemblages in a Mediterranean hypertrophic reservoir. The role of Microcystis ecomorphological variability in maintaining an apparent equilibrium. Hydrobiologia 502, 133–143. doi: 10.1023/B:HYDR.0000004276.11436.40
O’Brien, K. R., Meyer, D. L., Waite, A. M., Gregory, N. I., and Hamilton, D. P. (2004). Disaggregation of Microcystis aeruginosa colonies under turbulent mixing: laboratory experiments in a grid-stirred tank. Hydrobiologia 519, 143–152. doi: 10.1023/B:HYDR.0000026501.02125.cf
Paerl, H. W., Hall, N. S., and Calandrino, E. S. (2011). Controlling harmful cyanobacterial blooms in a world experiencing anthropogenic and climatic-induced change. Sci. Total Environ. 409, 1739–1745. doi: 10.1016/j.scitotenv.2011.02.001
Pannard, A., Pédrono, J., Bormans, M., Briand, E., Claquin, P., and Lagadeuc, Y. (2016). Production of exopolymers (EPS) by cyanobacteria: impact on the carbon-to-nutrient ratio of the particulate organic matter. Aquat. Ecol. 50, 29–44. doi: 10.1007/s10452-015-9550-3
Qin, B. Q., Li, W., Zhu, G. W., Wu, T. F., and Gao, G. (2015). Cyanobacterial bloom management through integrated monitoring and forecasting in large shallow eutrophic Lake Taihu (China). J. Hazard. Mater. 287, 356–363. doi: 10.1016/j.jhazmat.2015.01.047
Qin, B. Q., Zhu, G. W., Gao, G., Zhang, Y. L., Li, W., Paerl, H. W., et al. (2010). A drinking water crisis in Lake Taihu, China: linkage to climatic variability and lake management. Environ. Manage. 45, 105–112. doi: 10.1007/s00267-009-9393-6
Regel, R. H., Brookes, J. D., Ganf, G. G., and Griffiths, R. W. (2004). The influence of experimentally generated turbulence on the Mash01 unicellular Microcystis aeruginosa strain. Hydrobiologia 517, 107–120. doi: 10.1023/B:HYDR.0000027341.08433.32
Reynolds, C. S., Oliver, R. L., and Walsby, A. E. (1987). Cyanobacterial dominance: the role of buoyancy regulation in dynamic lake environments. N. Z. J. Mar. Freshw. Res. 21, 379–390. doi: 10.1080/00288330.1987.9516234
Reynolds, C. S., Wiseman, S. W., Godfrey, B. M., and Boutterwick, C. (1983). Some effects of artificial mixing on the dynamics of phytoplankton populations in large limnetic enclosures. J. Plankton Res. 5, 203–234. doi: 10.1093/plankt/5.2.203
Smith, V. H., Tilman, G. D., and Nekola, J. C. (1999). Eutrophication: impacts of excess nutrient inputs on freshwater, marine, and terrestrial ecosystems. Environ. Pollut. 100, 179–196. doi: 10.1016/S0269-7491(99)00091-3
Vonlanthen, P., Bittner, D., Hudson, A. G., Young, K. A., Müller, R., Lundsgaard-Hansen, B., et al. (2012). Eutrophication causes speciation reversal in whitefish adaptive radiations. Nature 482, 357–362. doi: 10.1038/nature10824
Walsby, A. E., Kinsman, R., Ibelings, B. W., and Reynolds, C. S. (1991). Highly buoyant colonies of the cyanobacterium Anabaena lemmermannii form persistent surface water blooms. Arch. Hydrobiol. 121, 261–280.
Wu, T. F., Qin, B. Q., Zhu, G. W., Luo, L. C., Ding, Y. Q., and Bian, G. Y. (2013). Dynamics of cyanobacterial bloom formation during short-term hydrodynamic fluctuation in a large shallow, eutrophic, and wind-exposed Lake Taihu, China. Environ. Sci. Pollut. Res. 20, 8546–8556. doi: 10.1007/s11356-013-1812-9
Wu, X., and Kong, F. X. (2009). Effects of light and wind speed on the vertical distribution of Microcystis aeruginosa colonies of different sizes during a summer bloom. Int. Rev. Hydrobiol. 94, 258–266. doi: 10.1002/iroh.200811141
Xiao, Y., Gan, N. Q., Liu, J., Zheng, L. L., and Song, L. R. (2012). Heterogeneity of buoyancy in response to light between two buoyant types of cyanobacterium Microcystis. Hydrobiologia 679, 297–311. doi: 10.1007/s10750-011-0894-y
Xu, H. C., Cai, H. Y., Yu, G. H., and Jiang, H. L. (2013). Insights into extracellular polymeric substances of cyanobacterium Microcystis aeruginosa using fractionation procedure and parallel factor analysis. Water Res. 47, 2005–2014. doi: 10.1016/j.watres.2013.01.019
Yang, Z., Kong, F., Shi, X., Zhang, M., Xing, P., and Cao, H. (2008). Changes in the morphology and polysaccharide content of Microcystis aeruginosa (Cyanobacteria) during flagellate grazing. J. Phycol. 44, 716–720. doi: 10.1111/j.1529-8817.2008.00502.x
Zhang, Y. L., Shi, K., Liu, J. J., Deng, J. M., and Qin, B. Q. (2016). Meteorological and hydrological conditions driving the formation and disappearance of black blooms, an ecological disaster phenomena of eutrophication and algal blooms. Sci. Total Environ. 569, 1517–1529. doi: 10.1016/j.scitotenv.2016.06.244
Keywords: hydrodynamics, cyanobacterial bloom, Microcystis colonies, turbulence, wind, Lake Taihu
Citation: Qin B, Yang G, Ma J, Wu T, Li W, Liu L, Deng J and Zhou J (2018) Spatiotemporal Changes of Cyanobacterial Bloom in Large Shallow Eutrophic Lake Taihu, China. Front. Microbiol. 9:451. doi: 10.3389/fmicb.2018.00451
Received: 26 September 2017; Accepted: 27 February 2018;
Published: 21 March 2018.
Edited by:Sandra M. F. O. Azevedo, Universidade Federal do Rio de Janeiro, Brazil
Reviewed by:Yonghong Bi, Institute of Hydrobiology (CAS), China
Klaus D. Joehnk, Commonwealth Scientific and Industrial Research Organisation (CSIRO), Australia
Myriam Bormans, Centre National de la Recherche Scientifique (CNRS), France
Copyright © 2018 Qin, Yang, Ma, Wu, Li, Liu, Deng and Zhou. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Boqiang Qin, firstname.lastname@example.org
†These authors have contributed equally to this work.