The younger flagellum sets the beat for Chlamydomonas reinhardtii
Abstract
Eukaryotes swim with coordinated flagellar (ciliary) beating and steer by finetuning the coordination. The model organism for studying flagellate motility, Chlamydomonas reinhardtii, employs synchronous, breaststrokelike flagellar beating to swim, and it modulates the beating amplitudes differentially to steer. This strategy hinges on both inherent flagellar asymmetries (e.g. different response to chemical messengers) and such asymmetries being effectively coordinated in the synchronous beating. In C. reinhardtii, the synchrony of beating is known to be supported by a mechanical connection between flagella; however, how flagellar asymmetries persist in the synchrony remains elusive. For example, it has been speculated for decades that one flagellum leads the beating, as its dynamic properties (i.e. frequency, waveform, etc.) appear to be copied by the other one. In this study, we combine experiments, computations, and modeling efforts to elucidate the roles played by each flagellum in synchronous beating. With a noninvasive technique to selectively load each flagellum, we show that the coordinated beating essentially only responds to load exerted on the cis flagellum; and that such asymmetry in response derives from a unilateral coupling between the two flagella. Our results highlight a distinct role for each flagellum in coordination and have implication for biflagellates’ tactic behaviors.
Editor's evaluation
This important manuscript investigates how the two flagella of C. reinhardtii, which have inherently different dynamic properties, synchronize their beating. Through careful, noninvasive experiments, the authors help the field to understand the mechanisms responsible for this synchronization, arguing that these mechanisms are due to unilateral coupling between the two flagella. The data are convincing, and the conclusion about unilateral coupling has been strengthened by additional analysis during revision.
https://doi.org/10.7554/eLife.86102.sa0eLife digest
Many singlecell organisms use tiny hairlike structures called flagella to move around. To direct this movement, the flagella must work together and beat in a synchronous manner. In some organisms, coordination is achieved by each flagellum reacting to the flow generated by neighbouring flagella. In others, flagella are joined together by fiber connections between their bases, which allow movement to be coordinated through mechanical signals sent between flagella.
One such organism is Chlamydomonas reinhardtii, a type of algae frequently used to study flagellar coordination. Its two flagella – named trans and cis because of their positions relative to the cell’s eyespot – propel the cell through water using breaststrokelike movements. To steer, C. reinhardtii adjusts the strength of the strokes made by each flagellum. Despite this asymmetry, the flagella must continue to beat in synchrony to move efficiently.
To understand how the cell manages these differences, Wei et al. exposed each flagellum to carefully generated oscillations in water so that each was exposed to different forces and their separate responses could be measured. A combination of experiments, modelling and computer simulations were then used to work out how the two flagella coordinate to steer the cell.
Wei et al. found that only the cis flagellum coordinates the beating, with the trans flagellum simply copying the motion of the cis. A direct consequence of such oneway coupling is that only forces on the cis flagellum influence the coordinated beating dynamics of both flagella. These findings shed light on the unique roles of each flagellum in the coordinated movement in C. reinhardtii and have implications for how other organisms with mechanicallyconnected flagella navigate their environments.
Introduction
Swimming microorganisms ranging from bacteria (Berg and Brown, 1972; Smriga et al., 2016) to larger flagellates and ciliates (Hegemann and Berthold, 2009; Ueki et al., 2010; Stehnach et al., 2021) must be able to steer to swim towards desirable environments and away from hazardous ones. Such targeted navigation are known as tactic behaviors. For a specific organism, tactic behavior may be underpinned by distinct mechanisms. For example, bacteria modulate the tumbling rate (Berg and Brown, 1972) while flagellates and ciliates modulate the waveform (Brokaw et al., 1974; Gong et al., 2020; Gadêlha et al., 2020; Bennett and Golestanian, 2015), amplitude (Rüffer and Nultsch, 1991; Ueki and Wakabayashi, 2017) and frequency (Naitoh and Kaneko, 1972; Ueki et al., 2010) of their flagellar/ciliary beating. However, these active modulations of motility serve the same goal, that is, to generate a spatially asymmetric propulsive force so the cell can steer.
Chlamydomonas reinhardtii, the model organism for studies of flagellar motility, achieves tactic navigation by a finetuned differential modulation on its two flagella. Studying this organism offers great opportunities to look into how flagella coordinate with each other and how such coordination helps facilitate targeted steering. C. reinhardtii has a symmetric cell body and two nearidentical flagella inherited from the common ancestors of land plants and animals (Merchant et al., 2007). It swims by beating its two flagella synchronously and is capable of photo and chemotaxis (Rüffer and Nultsch, 1991; Choi et al., 2016). For this biflagellated organism, effective steering hinges on both flagellar asymmetry and flagellar coordination. On the one hand, the two flagella must be asymmetric to respond differentially to stimuli (Rüffer and Nultsch, 1990; Rüffer and Nultsch, 1991); on the other hand, the differential responses must be coordinated by the cell such that the beating would remain synchronized to guarantee effective swimming. Understanding this remarkable feat requires knowledge about both flagellar asymmetry and coordination.
The two flagella are known to be asymmetric in several, possibly associated, aspects. First of all, they differ in developmental age (Holmes and Dutcher, 1989; Dutcher and O’Toole, 2016). The flagellum closer to the eyespot, the cis(eyespot) flagellum, is always younger than the other one, the trans(eyespot) flagellum. This is because the cis is organized by a basal body (BB) that develops from a prematured one in the mother cell; and this younger BB also organizes the flagellar root (D4 rootlet) that dictates the eyespot formation (Mittelmeier et al., 2011). Second, the two flagella have asymmetric protein composition (Sakakibara et al., 1991; Mackinder et al., 2017; Yu et al., 2020). For example, the trans flagellum is richer in CAH6, a protein possibly involved in CO_{2} sensing (Choi et al., 2016; Mackinder et al., 2017). Finally, the flagella have different dynamic properties (Kamiya and Witman, 1984; Okita et al., 2005; Takada and Kamiya, 1997). When beating alone, the trans beats at a frequency 30–40% higher than the cis (Kamiya and Hasegawa, 1987; Rüffer and Nultsch, 1987; Okita et al., 2005; Wan et al., 2014); the trans also displays an attenuated waveform (Leptos et al., 2013) and a much stronger noise (Leptos et al., 2013; Wan, 2018). Additionally, their beating dynamics is modulated differentially by second messengers such as calcium (Kamiya and Witman, 1984; Okita et al., 2005) and cAMP (Saegusa and Yoshimura, 2015).
Remarkably, despite these inherent asymmetries, C. reinhardtii cells establish robust synchronization between the flagella. Such coordination enables the cells to swim and steer efficiently, and is mediated by the fibrous connections between flagellar bases (Quaranta et al., 2015; Wan and Goldstein, 2016). Intriguingly, in the coordinated beating, both flagella display dynamic properties, that is, flagellar waveform, beating frequency (~50 Hz), and frequency fluctuation, that are more similar to those of the cis flagellum (Rüffer and Nultsch, 1985; Kamiya and Hasegawa, 1987; Leptos et al., 2013; Wan et al., 2014; Wan, 2018). This has led to a longstanding hypothesis that ‘the cis somehow tunes the trans flagellum’ (Kamiya and Hasegawa, 1987). This implies that the symmetric flagellar beating (‘breaststroke’) observed is the result of interactions between two flagella playing differential roles in coordination. How does the basal coupling make this possible? Recent theoretical efforts show that the basal coupling can give rise to different synchronization modes (Klindt et al., 2017; Liu et al., 2018; Guo et al., 2021); and that flagellar dynamics, such as beating frequency, may simply emerge from the interplay between mechanics of basal coupling and bioactivity (Guo et al., 2021). Yet, most theoretical efforts examining flagellar synchronization have assumed two identical flagella, limiting the results’ implication for the realistic case. Moreover, very few experiments directly probe the flagella’s differential roles during synchronous beating (Wan and Goldstein, 2014). Therefore, flagellar coordination in this model organism remains unclear. To clarify the picture experimentally, one needs to selectively force each flagellum, and characterize the dynamics of the flagellar response.
In this study, we address this challenge and devise a noninvasive approach to apply external forces selectively on the cis or the trans flagellum. Oscillatory background flows are imposed along an angle with respect to the cell’s symmetry axis. Such flows result in controlled hydrodynamic forces, which are markedly different on the two flagella. With experiments, hydrodynamic computations, and modeling, we show definitively that the two flagella are unilaterally coupled, such that the younger flagellum (cis) coordinates the beating, whereas the elder one simply copies the dynamic properties of the younger. This also means that only external forces on the cis may mechanically finetune the coordination. We also study the effect of calcium in the cis’ leading role as calcium is deeply involved in flagellar asymmetry and hence phototactic steering. In addition, a wellknown mutant that lacks flagellar dominance (ptx1) (Horst and Witman, 1993; Okita et al., 2005) is examined. Results show that the coordinating role of cis does not need environmental free calcium, whereas it does require the genes lost or mutated in ptx1. Our results discern the differential roles of C. reinhardtii’s flagella, highlight an advanced function of the interflagellar mechanical coupling, and have implications for biflagellates’ tactic motility.
Methodology
We set out to establish a noninvasive experimental technique that exerts differential loads on the flagella of C. reinhardtii. Following Quaranta et al., 2015, we use external background flows to exert hydrodynamic forcing on captured cells. Hydrodynamic forces are generated by a relative motion between the captured cell and its surrounding fluid. While the cell is captured by a glass pipette fixed in the laboratory frame, the fluid moves with the flow chamber  which is fixed on an oscillating piezoelectric stage. By programming the sinusoidal oscillations of the stage, we generate flows of desired amplitude $U}_{0$ and frequency $f}_{0$ and impose these flows along different directions $\theta$ to differentially load the two flagella, see Figure 1A. For each recording, we extract the phase dynamics of flagellar beating from videography (Quaranta et al., 2015; Wei et al., 2019; Wei et al., 2021), Figure 1B. First, recordings are masked and thresholded to highlight the flagella. Then, we extract the mean pixel values over time within two sampling windows (Figure 1C), and convert the two signals into observableinvariant flagellar phases $\varphi}_{c,t$ (Kralemann et al., 2008), see Figure 1D. In all our experimental recordings, the cis and the trans flagella beat synchronously. Typical phase locking between them is represented in Figure 1D inset, where the phase difference $\mathrm{\Delta}={\varphi}_{c}{\varphi}_{t}$ fluctuates around 0. Therefore, $\varphi}_{c$ and $\varphi}_{t$ are equal and denoted as $\varphi$.
The response of the flagella to the external hydrodynamic loads is therefore characterized by the difference between the flagellar phase $\varphi (t)$ and the phase of the oscillating flow ${\varphi}_{0}=2\pi {f}_{0}t$. Hereafter, we refer to the synchronization of the flagellar beating with the imposed external flow as ‘flow entrainment’, in order to avoid confusion with the ‘synchronization’ between the cis and the trans flagella. In our experiments, the cis and trans flagella always beat synchronously, therefore flow entrainment always takes place for both flagella simultaneously, regardless of the flow’s direction.
Differential external loads are selectively exerted on the cis and the transflagellum by imposing oscillatory background flows at an angle with respect to the cell’s symmetry axis. We use numerical simulations to quantify the differential loads exerted by flows along different angles θ = 45° , 90°, and 135°, on the cis and the trans flagellum, see Figure 1A. For each experiment, we track both flagella for the entire duration of the recording, see Figure 1B. We use the tracked motion of the flagella together with the oscillatory background flow as the boundary conditions to solve the Stokes equations numerically. Our numerical approach uses boundary element methods (BEM) and slenderbody theory (SBT), from which we can directly deduce the total drag force $F$ on each flagellum as well as the associated power $P$ of the viscous forces on each flagellum. In the linear Stokes regime, the drag force $F$ is the sum of the contributions due to the motion of the flagella and the motion of external flow. Our simulations allow us to compute both contributions separately. We present the loads induced by the external flow $F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$ and $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$ (see Materials and methods for details). Our computations provide the loads on the flagella throughout the entire experiment, from the time the captured cell is gradually entrained by the external flow, see Appendix 1: Hydrodynamic computation for asymmetric loading for the entire time series. Figure 1E,F,G represent the loads on each flagellum for flows with θ = 45°, 90°, 135°, after the cell is fully entrained. The variations of the loads are presented for one period of the powerrecovery stroke, and have been obtained by phase averaging over N≈30 periods. Upper panels display the magnitude of the drag force ${F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}={\mathbf{\text{F}}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}$; while lower panels show associated power $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$. Each panel presents the forces and powers on the cis and the transflagellum in red and blue respectively. The force magnitudes are scaled by $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}=6\pi \mu R{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ = 9.9 pN; while the powers by ${P}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}={F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}=1.1$ fW. $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ is the Stokes drag on a typical freeswimming cell (radius $R=5$ μm, speed $\displaystyle {U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}=110$ μm/s, water viscosity $\mu =0.95$ mPa·s).
Along θ = 90°, the external flow loads both flagella symmetrically (Figure 1F). However, for flows with θ = 45°, the loads on the cisflagellum (red) are ~2 times stronger than those on the trans (blue)(Figure 1E, $F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}\approx 2{F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{t}$), whereas flows with θ = 135° do the opposite (Figure 1G). The selectivity also manifests in (the absolute values of) $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$. We do notice that flows along θ = 135° are able to entrain the flagella with $\displaystyle {P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}<0$, meaning that the flagella are working against the flows, and this shall be discussed in later sections. Our computations demonstrate that flows along θ = 45° impose stronger loads on the cis flagellum, and we will refer to these as cisflows, hereon forward. Likewise, flows on θ = 135° selectively load the trans and we denote these as transflows. Finally, the flows along θ = 90° that approach the cell from the front will be called frontalflows.
Results
Experimental results
Frontalflow entrains both the wt and ptx1 cells
We first study the cells’ response to symmetric hydrodynamic loads, i.e., frontalflows. Captured cells are subjected to flows of various amplitudes $U}_{0$ varying between 390 and 2340 µm/s, and frequencies $f}_{0$ varying between 40 and 75 Hz. The scanned range covers reported intrinsic frequencies of both the cis and trans flagellum (Kamiya and Witman, 1984; Kamiya and Hasegawa, 1987; Rüffer and Nultsch, 1987; Takada and Kamiya, 1997), while the amplitude reaches the maximum instantaneous speed of a beating flagellum (~ 2000 µm/s). Figure 2A displays representative variations of the phase difference $\mathrm{\Psi}(t)=\varphi (t){\varphi}_{0}(t)$ between the flagella and the flow, for different frequencies $f}_{0$ of the forcing (expressed in terms of the detuning $\displaystyle \nu ={f}_{0}f$, Pikovsky et al., 2001). Entrainment of the flagella by the flow is characterized by plateaus in the phase difference $\mathrm{\Psi}(t)$, marked in black on Figure 2A. This typical dynamics of the phase difference $\mathrm{\Psi}(t)$ between the flagella and the external periodic forcing is well captured by the Adler equation (Pikovsky et al., 2001; Polin et al., 2009; Friedrich, 2016):
with $\epsilon$ the flow’s effective forcing strength. $\epsilon$ describes the sensitivity of the flagellar phase to the external stimuli, and it thus depends on both the absolute strength of the flow as well as the biological susceptibility of the flagella. In this study, $\epsilon$ is experimentally measured from the phase dynamics to quantify the flow entrainment effectiveness. $\zeta$ represents a white noise that satisfies $\zeta ({t}^{\mathrm{\prime}}+t)\zeta ({t}^{\mathrm{\prime}})=2T\delta (t)$, with $T$ an effective temperature and $\delta (t)$ the Dirac delta function.
By definition, entrainment corresponds to a constant phase difference $\mathrm{\Psi}$ ($\dot{\mathrm{\Psi}}=0$). Solving Equation 1 under this condition, one sees that entrainment is only possible when the effective forcing strength is strong enough: $\left\epsilon \right>\left\nu \right$. Therefore, we can experimentally vary $\nu$ and measure $\epsilon$ directly by the frequency range where flow entrainment is established. The quality of entrainment is described by the entrained time fraction $\tau ={t}_{\mathrm{e}\mathrm{n}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{i}\mathrm{n}}$/$t}_{\mathrm{t}\mathrm{o}\mathrm{t}$, where $t}_{\mathrm{e}\mathrm{n}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{i}\mathrm{n}$ is the total time where the beating is entrained and $t}_{\mathrm{t}\mathrm{o}\mathrm{t}$ the flow’s duration, see Materials and methods.
In Figure 2A, the traces range from: no entrainment ($\tau$=0, i) and unstable entrainment ($\displaystyle 0<\tau <1$, iiiii), to stable entrainment ($\tau$=1, iv). In this study, the frequency range of $\nu$ for which $\tau \ge 0.5$ is considered as the region where entrainment is established, and is used as a measure for the flagellumflow coupling strength $\epsilon$ (see Figure 2A right panel). This method measures $\epsilon$ accurately when noises are low ($T\lesssim 2.5$ rad^{2}/s for typical values of frequencies and couplings used in this work). In this regime, this straightforward method is equivalent to previous methods based on multiparameter curve fitting (Wan et al., 2014; Quaranta et al., 2015) but is more robust (Appendix 1: Extracting coupling strength by fitting phase dynamics).
The flow entrainment landscape over the entire scanned ranges is presented in Figure 2B. Up until the strongest flow amplitude, the external forces cannot disrupt the synchronized flagellar beating. In addition, entrainment is never established around frequencies other than $f\approx 50$ Hz. Both phenomena indicate that the interflagellar coupling is much stronger than the flows’ maximum effective forcing ($\epsilon \sim 10$ Hz, see Appendix 1: MonteCarlo simulations).
We also examine the flagellar dominance mutant ptx1 whose two flagella are both putatively considered trans flagella (Horst and Witman, 1993; Rüffer and Nultsch, 1997; Rüffer and Nultsch, 1998; Okita et al., 2005; Leptos et al., 2013): they respond similarly to changes of calcium concentrations (Horst and Witman, 1993) and have similar beating frequencies when demembranated and reactivated (Okita et al., 2005). Ptx1 mutants have two modes of synchronous beating, namely, the inphase (IP) mode and the antiphase (AP) mode (Rüffer and Nultsch, 1998; Leptos et al., 2013). By applying frontalflows over the same ranges of frequencies and amplitudes, we find that the IP beating, which is in a similar breaststrokelike pattern to that of wt and is also around $f\approx 50$ Hz, is the only mode that can be flowentrained. We focus on this mode and report $\tau$ as $\tau ={t}_{\mathrm{e}\mathrm{n}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{i}\mathrm{n}}/{t}_{\mathrm{I}\mathrm{P}}$ for this mutant, where $t}_{\mathrm{I}\mathrm{P}$ is the total time of IPbeating under the applied flows, see Figure 2C. Albeit noisier, the Arnold tongue of ptx1 covers a slightly larger width compared to wt’s, meaning that the breaststroke beating of two trans flagella is similarly entrainable as that by one cis and one trans (Figure 2B–C right panels). This finding indicates that the trans flagellum is at least as susceptible to hydrodynamic loads as the cis.
Cisflow entrains wt cells more effectively than transflow
Next, we study how a cell is entrained by asymmetric flagellar loads. To each captured cell, we apply cisflows and transflows of a fixed amplitude ($\sim 7{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}$) but at varying detunings (see Materials and methods), and we compare the flows’ effective forcing $\epsilon$ to quantify the cells’ differential response.
We find that cisflows are the most effective in entraining the beating (Figure 3A). We illustrate this point with the entrainment profiles of an exemplary cell (Figure 3A inset). First, although both the cisflow (red) and the transflow (blue) can entrain the cell at small detunings ($\left\nu \right<0.5$ Hz), the cisflow entrainment is more robust and lasts over the entire duration of the experiment ($\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{cis}}\text{flow})$=1), while the transflow for a smaller time fraction ($\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{trans}}\text{flow})$ ≈0.85). This is due to phaseslips (steplike changes in $\mathrm{\Psi}$ in Figure 2A) between flagella and the flow, and means that the transflow entrainment is less stable. Additionally, for intermediate detuning ($0.5\text{}\mathrm{H}\mathrm{z}\left\nu \right4\text{}\mathrm{H}\mathrm{z}$), $\epsilon (\mathit{\text{cis}}\text{flow})=\epsilon (\mathit{\text{trans}}\text{flow})$ is always larger than $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{trans}}\text{flow})$. In some cases, the cisflow entrains the cell fully whereas the transflow fails completely (e.g. at $\nu =2$ Hz). Together, these results imply that a flow of given amplitude entrains flagellar beating more effectively if it selectively loads the cis flagellum.
We repeat the experiments with cells from multiple cultures, captured on different pipettes, and with different eyespot orientations (~50% heading rightward in the imaging plane) to rule out possible influence from the setup. The entrainment profile of N=11 wt cells tested in the TRISminimal medium (pH = 7.0) are displayed in Figure 3A (labeled as ‘TRIS’). On average, $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})$ = 2.9 Hz and is 70% larger than $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})$ = 1.7 Hz. It bears emphasis that for every single cell tested (11/11), the relation $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})>\epsilon (\mathit{\text{trans}}\text{flow})$ holds true. In Figure 3B, we show this by representing each cell as a point whose $x$ and $y$ coordinates are respectively its $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})$ and $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})$. A point being above the first bisector line ($y=x$) indicates that $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})>\epsilon (\mathit{\text{trans}}\text{flow})$ for this cell. All cells cluster clearly above the line. The entrainment asymmetry is very robust and is observed in almost all separate experiments for each cell and each flow condition. In Figure 3C, each point corresponds to the time fractions of the same cell entrained by the cisflow and the transflow at the same frequency. Most points (>90%) are above the first bisector line, meaning that $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{cis}}\text{flow})>\tau (\mathit{\text{trans}}\text{flow})$. Altogether, all results show that selectively loading the cis flagellum better enables flow entrainment, pointing to cis and trans flagella playing differential roles in the synchronous beating.
To highlight the differential roles, we resolve how the flows’ effective forcing strengths depend on the actual hydrodynamic loads on each flagellum, see Figure 3D. The loads are characterized by the beataveraged force, ${\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}={\int}_{0}^{2\pi}{F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}d\varphi /2\pi$, on each flagellum (see corresponding horizontal lines in Figure 1E–G). These loads are computed for the cisflow, transflow, and frontalflow. Experimental and computational data of flows along θ = 0° (circles, Appendix 1: Hydrodynamic computation for asymmetric loading) are also included to substantiate the results. From Figure 3D, we see that the effective forcing strength scales with the beataveraged drag on the cis, $\epsilon \sim {\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}$ while we find no such correlation between $\epsilon$ and $\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{t}$. Notably, the linear relation between $\epsilon$ and $\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}$ has an intercept near zero ($\epsilon {}_{{\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}=0}\approx 0$). Given the total forces on both flagella ($\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}+{\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{t}$) for these flows remains almost constant (0.74–0.79 $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$), the zerointercept implies that for a hypothetical flow that exerts no load on the cis but solely forces the trans, it will not entrain the cell at all. This suggests that the hydrodynamic loads on the trans flagellum do not significantly contribute to flow entrainment for wt cells. We will later discuss the implications of this result in the context of our earlier observation that the trans flagella of ptx1 are susceptible to entrainment by external hydrodynamic loads.
Depletion of environmental calcium does not affect the asymmetric flow response
We examine whether this newly observed cistrans asymmetry is affected by calcium depletion. Calcium is a critical second messenger for modulating flagellates’ motility and is deeply involved in phototaxis (Yoshimura, 2011). The depletion of the free environmental calcium is known to degrade flagellar synchronization and exacerbate flagellar asymmetry (Kamiya and Witman, 1984). Here, we focus on whether calcium depletion affects the asymmetry $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})>\epsilon (\mathit{\text{trans}}\text{flow})$. We deplete environmental calcium by EGTAchelation, following the protocol in Wakabayashi et al., 2009. Similar to previous reports (Kamiya and Witman, 1984; Pazour et al., 2005), the number of freely swimming cells drops significantly in EGTAcontaining medium. However, the remaining cells beat synchronously for hours after capture. For these beating cells, calcium depletion is first confirmed by characterizing their deflagellation behavior. Indeed, calcium depletion is reported to inhibit deflagellation (Wan et al., 2014; Quarmby and Hartzell, 1994). In experiments with standard calcium concentration, all cells deflagellated under pipette suction (20/20). For experiments conducted in calcium depleting EGTAcontaining medium, we observe deflagellation to occur in none but one cell (1/19).
After confirming the calcium depletion in our experiments, we perform the same sets of flow entrainment experiments. The dashed lines in Figure 3A show the median entrainment profiles for N=6 cells (labeled as ‘EGTA’). Clearly, the asymmetry $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})>\epsilon (\mathit{\text{trans}}\text{flow})$ is unaffected and it again applies for every single cell tested. The mere effect of calcium depletion appears to be a drop in the mean values of $\epsilon$ (Figure 3E). However, the difference between $\displaystyle \epsilon (\mathit{\text{cis}}\text{flow})=\epsilon (\mathit{\text{trans}}\text{flow})$ and $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})$ is not affected, see $\displaystyle \delta \epsilon =\epsilon (\mathit{\text{cis}}\text{flow}){\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})}$ for the two experimental conditions in Figure 3E inset.
ptx1 mutant loses the asymmetric flow response
Lastly, we examine the asymmetry in ptx1. The entrainment profiles of ptx1 are shown in Figure 4A. The median profiles are of similar width and height, indistinguishable from each other, and hence indicate a loss of asymmetric susceptibility to flow entrainment, which are in sharp contrast to the profiles of wt (Figure 3A). The loss is further confirmed by the extracted $\displaystyle \epsilon$ and $\displaystyle \tau$ presented in Figure 4BC, which are also significantly different from our results for wt cells (Figure 3BC). For ptx1, cells and entrainment attempts are distributed evenly across the first bisector lines: 7/14 cells are above $\epsilon (\mathit{\text{cis}}\text{flow})=\epsilon (\mathit{\text{trans}}\text{flow})$ in Figure 4B, and ~50% points are above $\tau (\mathit{\text{cis}}\text{flow})=\tau (\mathit{\text{trans}}\text{flow})$ in Figure 4C. Altogether, all results consistently show that the asymmetry is lost in ptx1.
In addition, it is noteworthy that the measured $\epsilon$ for both wt and ptx1 are within the same range (2–4 Hz), indicating that both strains are similarly susceptible to external flow. Furthermore, the transition to flow entrainment is sharper for wt cells, in Figure 3A, compared to ptx1 cells, in Figure 4A. For wt, the flow entrainment is robustly established for the entire length of the experiment and $\tau \approx 1$ for a range of $f}_{0$. For frequencies further away from the intrinsic flagellar beating frequency ($f$), the entrainment time sharply decreases to $\tau =0$ (Figure 3A). For ptx1 on the other hand, the transition is not as sharp (Figure 4A). This difference can be explained by a larger stochasticity in the beating of ptx1 compared to wt, which can be represented by a stronger noise $\zeta$ for ptx1 compared to wt in Equation 1.
Model
Model experimental findings by three coupled oscillators
To investigate the implications of our experimental results on the coupling between flagella and their dynamics, we develop a model for the system (Appendix 1: MonteCarlo simulations), representing flagella and external flows as oscillators with directional couplings:
${\varphi}_{0,c,t}(t)$ respectively represent the phase of the flow, the cis, and the trans flagellum. $f}_{0,c,t$ represents the (inherent) frequency of the flow, the cis, and the trans, respectively. The first equation represents the imposed periodic forcing, while the other equations represent the Langevin dynamics for the phases of the cis and trans flagella. The phase dynamics of each flagellum is influenced by the interactions with the other flagellum as well as the interactions with the periodic hydrodynamic forcing. Here, $\lambda}_{tc$ represents the forcing exerted by the trans on the cis and $\lambda}_{ct$, the forcing of the cis on the trans. $\u03f5}_{c$ is the hydrodynamic forcing on the cis and $\u03f5}_{t$ the one on the trans. In this simple model, we differentially vary $\u03f5}_{c$ and $\u03f5}_{t$ to match the values of the selective hydrodynamic loads ($\displaystyle {\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{c}/\phantom{\rule{thinmathspace}{0ex}}{\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{t}$) measured for each flow condition (Figure 1E–G). It bears emphasis that $\u03f5}_{c,t$ are input parameters of our model, whereas $\epsilon$ is measured from the phase dynamics to characterize the entrainment. In our simulations, $\epsilon$ is extracted following the same approach as in the experiments, see Figure 2A. Lastly, $\zeta}_{\mathrm{c},\mathrm{t}$ represent the uncorrelated white noises in the cis and trans flagellum respectively, whose strengths are ${\zeta}_{\mathrm{c},\mathrm{t}}({t}^{\mathrm{\prime}}+t){\zeta}_{\mathrm{c},\mathrm{t}}({t}^{\mathrm{\prime}})=2{T}_{\mathrm{c},\mathrm{t}}\delta (t)$. Figure 5A illustrates our model for flagellar beating subjected to cisflows. The direction and thickness of arrows represent the coupling direction and strength respectively.
Equation 2 can be combined and readily reduced to a single equation, which has the form of the Adler equation (Equation 1) in the asymptotic limit of $\varphi}_{c}\approx {\varphi}_{t$, see Appendix 1: MonteCarlo simulations for detail. From this equation, we can directly write the quantities $f$, $\epsilon$ and $T$ measured in our experiments as a function of the parameters from our model $f}_{c,t$, $\u03f5}_{c,t$, $\displaystyle {\lambda}_{ct,tc}$, and $\zeta}_{c,t$ as
with $\alpha ={\lambda}_{ct}\phantom{\rule{thinmathspace}{0ex}}/\left({\lambda}_{ct}+{\lambda}_{tc}\right)$. Remarkably, our experimental results are reproduced by the simple theoretical limit of $\alpha \approx 1$, for which the beating dynamics of the cell, frequency $f$ and noise $T$ become equal to those of the cis flagellum, and the flow entrainment strength $\epsilon$ only depends on the forcing strength on the cis $\u03f5}_{c$. $\alpha$ approaching unity corresponds to the limit when $\lambda}_{tc}\ll {\lambda}_{ct$ for which the beating of the cis sets the beating of the trans and is not influenced by the trans. It should be mentioned that our main observation about the measured entrainment strength $\epsilon$ only depending on the cisloading, can also be reproduced by assuming ${\u03f5}_{t}\approx 0$. This alternative limit implies that the trans flagellum has no susceptibility to hydrodynamic loads, which is inconsistent with our entrainment experiments of $ptx1$. In addition, $\alpha \approx 1$ is also necessary to explain the difference in noise and effective temperature between the wt and ptx1 experiments.
We perform MonteCarlo simulations to solve the stochastic Equation 2, and determine the parameters of our simulations that reproduce our experimental results.
Coordinated beating under symmetric forcing
The values of the parameters used in our simulations are summarized in Table 1. We first model the flow entrainment induced by frontalflow, for which the flagella are loaded symmetrically and $\u03f5}_{c}={\u03f5}_{t$. We take ${f}_{c}=45$ Hz and ${f}_{t}=65$ Hz following Kamiya and Hasegawa, 1987; Okita et al., 2005. We set $\u03f5}_{c,t$ as 2.4 Hz to match the measured $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\text{frontalflow})$ from Figure 3A. The noises for cis and trans flagellum are $\displaystyle {T}_{c}=1.57$ rad^{2}/s and ${T}_{t}=9.42$ rad^{2}/s respectively. At similar detunings as in the experimental results in Figure 2A, our MonteCarlo simulations reproduce the phase dynamics with: (i) no flow entrainment, (iiiii) unstable entrainment, and (iv) stable entrainment (Figure 5B). Repeating the simulations for varying forcing strengths $\u03f5}_{\mathrm{c},\mathrm{t}$ and frequencies $f}_{0$ yields Arnold tongue diagrams in agreement with those reported from our experiments. For wt, we assume asymmetric coupling strength, $\lambda}_{ct}=4{\lambda}_{tc$, while we assume a symmetric coupling strength $\lambda}_{ct}={\lambda}_{tc$ for ptx1. With these values, the Arnold Tongue for wt in Figure 2B and ptx1 in Figure 2C are reproduced with simulations shown in Figure 5C and D respectively. For wt, the asymmetry $\displaystyle {\lambda}_{ct}\gg {\lambda}_{tc}$ does not affect the overall shape of the Arnold tongue but leads to a low noise level, which is induced by the cis, and is much lower than the noise of ptx1.
Coordinated beating under selective loading
Next, we model flow entrainment by the cisflows and the transflows. The selective forcing ($\u03f5}_{\mathrm{c}}\ne {\u03f5}_{\mathrm{t}$) allows the effect of flagellar dominance ($\displaystyle {\lambda}_{ct}\ne {\lambda}_{tc}$) to manifest in the effective forcing strength $\epsilon$ and hence in the entrainment profiles $\tau (\nu )$, Figure 5E. We derive the ratio between $\u03f5}_{c$ and $\u03f5}_{t$ from our computations, see Figure 1E–G, such that ${\u03f5}_{c}:{\u03f5}_{t}=$ 2:1, 1:1, and 1:2 for the cisflows, the frontalflows, and the transflows respectively. With this setting, the model reproduces the experimental observations that the entrainment profile of cisflow is consistently broader than that of frontalflow (i.e. larger $\epsilon$), and the profile of transflow is always the narrowest (smallest $\epsilon$), see Figure 5E. Figure 5F shows how the asymmetry of interflagellar coupling ($\displaystyle {\lambda}_{ct}\text{}/\text{}{\lambda}_{tc}$) affects the asymmetry between the entrainment strength $\epsilon$ for the cisflows and the transflows. The open symbols represent $\epsilon$ measured from modeled entrainment profiles $\tau (\nu )$ and the lines represent Equation 3. The difference between $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})$ and $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})$ increases with $\displaystyle {\lambda}_{ct}\text{}/\text{}{\lambda}_{tc}$. At large $\displaystyle {\lambda}_{ct}\text{}/\text{}{\lambda}_{tc}$, the $\epsilon$ saturates to the forcing on the cis flagellum ($\u03f5}_{\mathrm{c}$, see the grey dashed lines in Figure 5F).
Our experimental results for wt cells under calcium depletion are reproduced with a lower total forcing strength (Figure 5G). $\u03f5}_{\mathrm{c}}+{\u03f5}_{\mathrm{t}$ is set to 4.08 Hz (15% lower) to reflect the 7% − 20% decrease in $\epsilon$ induced by calcium depletion (Figure 3E).
To reproduce the entrainment profiles of ptx1 in Figure 5H, both a stronger noise and a symmetric interflagellar coupling are needed: while the stronger noise lowers the maximal values of $\tau (\theta ,\nu )$, setting $\displaystyle {\lambda}_{ct}\text{}/\text{}{\lambda}_{tc}=4$ would still result in $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{cis}}\text{flow})>\tau (\mathit{\text{trans}}\text{flow})$ in the central range ($\left\nu \right\lesssim 2.4$ Hz). Finally, it is noteworthy that the noise in ptx1 increases not only because of a higher noise value for individual flagella, but also because the cistrans coupling has become symmetric. As shown by Equation 3, the unilateral coupling promotes not only the cisfrequency in the synchrony but also the cisnoise. Given $T}_{c}\ll {T}_{t$ and $\lambda}_{ct}=4{\lambda}_{tc$, we confirm with simulations that, for wt, the cis stabilizes the beating frequency of the trans. The simulations are in good agreement with experimental noise measurements, see Appendix 1: Noise in the beating of the ptx1 mutant for details.
Discussion
The two flagella of C. reinhardtii have long been known to have inherently different dynamic properties such as frequency, waveform, level of active noise, and responses to second messengers (Kamiya and Hasegawa, 1987; Okita et al., 2005; Leptos et al., 2013; Wan, 2018; Saegusa and Yoshimura, 2015). Intriguingly, when connected by basal fibers and beating synchronously, they both adopt the kinematics of the cis(eyespot) flagellum, which led to the assumption that the flagella may have differential roles in coordination. In this work, we test this hypothesis by employing oscillatory flows applied from an angle with respect to the cells’ symmetry axis and thus exert biased loads on one flagellum.
In all our experiments with wt cells, we robustly observe that cisflows, the ones that selectively load the cis flagellum, are always more effective in entraining the flagellar beating than the transflows. This is shown by the larger effective forcing strengths ($\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})>\epsilon (\mathit{\text{trans}}\text{flow})$, Figure 3B) and larger entrained time fractions ($\displaystyle \phantom{\rule{thinmathspace}{0ex}}\tau (\mathit{\text{cis}}\text{flow})>\tau (\mathit{\text{trans}}\text{flow})$, Figure 3C). Mapping $\epsilon (\theta )$ as a function of the loads, we find empirically that the flow entrainment strength scales with the hydrodynamic load on the cis, $\epsilon \propto {\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}$ (Figure 3D) and that transloads appear to matter negligibly. These observations all indicate that the cisloads determine whether an external forcing can entrain the cell. Moreover, this point is further highlighted by an unexpected finding: when transflows are applied, the trans flagellum always beats against the external flow ($\displaystyle {P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{t}}<0$) and the only stabilizing factor for flow entrainment is the cis flagellum working transiently along with the flow ($\displaystyle {P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}>0$) during the recovery stroke (Figure 1G lower panel). These observations definitively prove that the two flagella have differential roles in the coordination and interestingly imply that flagella are coupled to external flow only through the cis.
To elucidate the mechanisms at the origin of this asymmetry, we develop a reduced stochastic model for the system, see Equation 2. In the model, selective hydrodynamic loading and flagellar dominance in the coordinated beating are respectively represented by $\u03f5}_{\mathrm{c}}\ne {\u03f5}_{\mathrm{t}$ and $\lambda}_{ct}\ne {\lambda}_{tc$. Using this model, we express $f$ and $\epsilon$, which we can measure experimentally (Equation 3), as a function of $f}_{c,t$, $\u03f5}_{c,t$, $\lambda}_{ct$ and $\lambda}_{tc$ to illustrate how the flagellar dominance and selective loading affect the coordinated flagellar beating. Moreover, with MonteCarlo simulations, we clarify the interplay between flows and flagella (Appendix 1: MonteCarlo simulations), and reproduce all experimental observations. We show that a ‘dominance’ of the cis ($\lambda}_{ct}\gg {\lambda}_{tc$) is sufficient to explain the experimental phenomenology comprehensively. This dominance means that the cisphase is much less sensitive to the transphase than the other way around. We then reproduce the phase dynamics of flow entrainment at varying detunings (Figure 5B), amplitudes (Figure 5C), and noises (Figure 5D). Exploiting the observation that the coordination between flagella cannot be broken by external flows up to the strongest ones tested (${\epsilon}^{\mathrm{m}\mathrm{a}\mathrm{x}}\sim 10$ Hz, Figure 2B), we quantify the lower limit of the total basal coupling, $\lambda}_{ct}+{\lambda}_{tc$, to be approximately 40 Hz (deduced in Appendix 1: MonteCarlo simulations), which is an order magnitude larger than the hydrodynamic interflagellar coupling (Quaranta et al., 2015; Brumley et al., 2014; Klindt et al., 2016; Pellicciotta et al., 2020).
Dynamic modulation of flagellar dominance during synchronous beating is the basis of C. reinhardtii’s tactic motility (Kamiya and Witman, 1984; Horst and Witman, 1993; Pazour et al., 2005; Okita et al., 2005). Calcium has long been speculated to facilitates such dynamic modulation (Rüffer and Nultsch, 1997; Wan et al., 2014; Guo et al., 2021) because it is involved in switching the beating mode (Hayashi et al., 1998) and in tuning flagellar beating amplitude (Kamiya and Witman, 1984; Okita et al., 2005), and calcium influx comprises the initial step of the cell’s photo (Harz and Hegemann, 1991) and mechanoresponses (Yoshimura, 2011). We therefore investigate flagellar coupling in the context of tactic steering by depleting the environmental free calcium and hence inhibiting signals of calcium influxes. Cells are first acclimated to calcium depletion, and then tested with the directional flows. Our results show that the cis dominance in the synchronous beating does not require the involvement of free environmental calcium. Calcium depletion merely induces an overall drop in the forcing strength perceived by the cell $\epsilon (\theta )$ ($7\mathrm{\%}20\mathrm{\%}$), which is captured by reducing $\u03f5}_{\mathrm{c}}+{\u03f5}_{\mathrm{t}$ for 15% (mean drop) in the model (Figure 5G). In contrast to the speculation that calcium is involved in the dynamic modulation of ciliary dominance in synchronous beating (Rüffer and Nultsch, 1997; Wan et al., 2014; Guo et al., 2021), our results indicate that the leading role of cis (i.e., $\lambda}_{ct}\gg {\lambda}_{tc$) is an inherent property, which does not require active influx of external calcium, and possibly reflects an intrinsic mechanical asymmetry of the cellular mesh that anchors the two flagella into the cell body.
In ptx1 cells, a lack of flagellar dominance ($\lambda}_{ct}={\lambda}_{tc$) and a stronger noise level are necessary to reproduce our experimental observations. Previous studies suggested that both flagella of ptx1 are similar to the wildtype trans (Horst and Witman, 1993; Rüffer and Nultsch, 1997; Okita et al., 2005), and that the noise levels of this mutant’s synchronous beating are much greater than those of wt (Leptos et al., 2013) (see also Appendix 1: Noise in the beating of the ptx1 mutant). If both flagella and their anchoring roots indeed have the composition of the wildtype trans, such symmetry would predict $\lambda}_{ct}={\lambda}_{tc$. This symmetric coupling leads to a noise for ptx1 $T\approx {T}_{t}$ (Equation 3), which is about an order of magnitude larger than the noise of wt $T\approx {T}_{c}$.
The comparison between ptx1 and wt highlights an intriguing advantage of the observed unilateral coupling ($\lambda}_{ct}\gg {\lambda}_{tc$); that is, it strongly suppresses the high noise of the trans. Considering that the trans is richer in CAH6 protein and this protein’s possible role in inorganic carbon sensing (Mackinder et al., 2017; Choi et al., 2016), the trans may function as a more active sensor than the cis. Assuming the sensingrelated bioactivities is at the origin of trans’ strong noise, then because the unilateral coupling prevents the noise from disrupting the cell’s synchronous beating and effective swimming, it allows the cell to combine the benefit of having a stable cis as the driver and a noisy trans as a sensor.
Materials and methods
Cell culture
Request a detailed protocolC. reinhardtii wildtype (wt) strain cc125 (mt+) and flagellar dominance mutant ptx1 cc2894 (mt+), obtained from the Chlamydomonas Resource Center, are cultured in TRISminimal medium (pH = 7.0) with sterile air bubbling, in a 14 hr/10 hr daynight cycle. Experiments are performed on the fourth day after inoculating the liquid culture, when the culture is still in the exponential growth phase and has a concentration of ∼2 × 10^{5} cells/ml. Before experiments, cells are collected and resuspended in fresh TRISminimal (pH = 7.0).
Calcium depletion
Request a detailed protocolIn calcium depletion assays, cells are cultured in the same fashion as mentioned above but washed and resuspended in fresh TRISminimal medium +0.5 mM EGTA (pH = 7.0). Free calcium concentration is estimated to drop from 0.33 mM in the TRISminimal medium, to 0.01 µM in the altered medium (Wakabayashi et al., 2009). Experiments start at least one hour after the resuspension in order to acclimate the cells.
Experimental setup
Request a detailed protocolSingle cells of C. reinhardtii are studied following a protocol similar to the one described in Quaranta et al., 2015. Cell suspensions are filled into a customized flow chamber with an opening on one side. The airwater interface on that side is pinned on all edges and is sealed with silicone oil. A micropipette held by micromanipulator (SYSHS6, WPI) enters the chamber and captures single cells by aspiration. The manipulator and the captured cell remain stationary in the lab frame of reference, while the flow chamber and the fluid therein are oscillated by a piezoelectric stage (NanoDrive, Mad City Labs), such that external flows are applied to the cell. Frequencies and amplitudes of the oscillations are individually calibrated by tracking microbeads in the chamber. Bright field microscopy is performed on an inverted microscope (Nikon Eclipse TiU, 60× water immersion objective). Videos are recorded with a sCMOS camera (LaVision PCO.edge) at 600–1000 Hz.
Measurement scheme
Request a detailed protocolThe flagellar beating of each tested cell is recorded before, during, and after the application of the flows. We measure the cell’s average beating frequency $f$ over 2 s (~100 beats). For ptx1 cells, $f$ is reported for the inphase (IP) synchronous beating. Unless otherwise stated, directional flows (θ = 0°, 45°, 90°, 135°) are of the same amplitude (780±50 µm/s, mean±std), similar to those used in Quaranta et al., 2015. Flow frequencies $f}_{0$ are scanned over [$f7$, $f+7$] Hz for each group of directional flows.
Computation of the flagellar loads
Request a detailed protocolTo quantify the hydrodynamic forces on the flagella, we first track realistic flagellar deformation from videos wherein background flows are applied. Then we employ a hybrid method combining boundary element method (BEM) and slenderbody theory (Keller and Rubinow, 1976; Wei et al., 2021) to compute the drag forces exerted on each flagellum and the forces’ rates of work. In this approach, each flagellum is represented as a slenderbody (Keller and Rubinow, 1976) with 26 discrete points along its centerline and the timedependent velocities of each of the 26 points are calculated by the point’s displacement across frames. The cell body and the pipette used to capture the cell are represented as one entity with a completed double layer boundary integral equation (Power and Miranda, 1987). Stresslet are distributed on cellpipette’s surface; while stokeslets and rotlets of the completion flow are distributed along cellpipette’s centerline (Keaveny and Shelley, 2011). The noslip boundary condition on the cellpipette surface is satisfied at collocation points. Lastly, stokeslets are distributed along the centerlines of the flagella, so that noslip boundary conditions are met on their surfaces. Integrating the distribution of stokeslets $\mathbf{\text{f}}(s)$ over a flagellar shape, one obtains the total drag force $\mathbf{\text{F}}=\int \mathbf{\text{f}}(s)ds$. Similarly, the force’s rate of work is computed as $P=\int \mathbf{\text{f}}(s)\cdot \mathbf{\text{U}}(s)ds$, where $\mathbf{\text{U}}(s)$ is the velocity of the flagellum at the position $s$ along the centerline.
The computations shown in this study are based on videos of a representative cell which originally beats at ~50 Hz. The cell is fully entrained by flows along different directions (θ = 0°, 45°, 90°, 135°) at 49.2 Hz. In the computations, the applied flows are set to have an amplitude of 780 µm/s to reflect the experiments. Computations begin with the onset of the background flows (notified experimentally by a flashlight event), and last for ~30 beats (500 frames sampled at 801 fps). Additionally, we confirm the results of transflowentrainment, that both flagella spend large fractions of time beating against the flows, with other cells and with transflows at other frequencies.
Isolate loads of external flows
Request a detailed protocolThe total loads ($F$ and $P$) computed consist of two parts, one from the flow created by the two flagella themselves and the other from the flow imposed. In the low Reynolds number regime, the loads of the two parts add up directly (linearity): $\mathbf{\text{F}}={\mathbf{\text{F}}}_{\mathrm{S}\mathrm{e}\mathrm{l}\mathrm{f}}+{\mathbf{\text{F}}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}$, and $P={P}_{\mathrm{S}\mathrm{e}\mathrm{l}\mathrm{f}}+{P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}$. To isolate $\mathbf{\text{F}}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$ and $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$, we compute $\mathbf{\text{F}}}^{\mathrm{\prime}}={\mathbf{\text{F}}}_{\mathrm{S}\mathrm{e}\mathrm{l}\mathrm{f}$ and $P}^{\mathrm{\prime}}={P}_{\mathrm{S}\mathrm{e}\mathrm{l}\mathrm{f}$ by running the computation again but without the external flows, and obtain $\mathbf{\text{F}}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}=\mathbf{\text{F}}{\mathbf{\text{F}}}^{\mathrm{\prime}$ and $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}=P{P}^{\mathrm{\prime}$.
Compute time fraction of phaselocking
Request a detailed protocolIn practice, phaselocking is considered established if phase difference, either between the two flagella (Δ) or between the flow and flagella ($\mathrm{\Psi}$), varies slow enough over time. Here, we use $\mathrm{\Psi}$ to illustrate the process. We first break down an entire time series (${t}_{\mathrm{t}\mathrm{o}\mathrm{t}}\approx 10$ s) to segments of 0.1 s (~5 beats). A given segment is considered phaselocked if $\left\frac{d\mathrm{\Psi}}{dt}\right\le \pi$ rad/s. This particular threshold ($\pi$ rad/s) is equivalent to a frequency mismatch of 0.5 Hz, which is smaller than our frequency resolution in scanning the detuning (~0.8 Hz).
Modeling parameters
Request a detailed protocolWe assume the flagellar intrinsic frequencies $f}_{c$ and $f}_{t$ to be 45 Hz and 65 Hz respectively (Kamiya and Hasegawa, 1987; Okita et al., 2005; Wan et al., 2014). On this basis, $\lambda}_{ct}:{\lambda}_{tc$ is assumed to be 4:1 to account for the observed $f\sim 50$ Hz. $\u03f5}_{c}:{\u03f5}_{t$ is set as 2:1, 1:1, and 1:2 for the cisflows, the frontalflows, and the transflows respectively, see Figure 1E–G. The underlying assumptions are: the two flagella are equally susceptible to loads, and the effective coupling strength is linearly proportional to the hydrodynamic load. Additionally, $\u03f5}_{c}+{\u03f5}_{t$ is assumed to be constant to reflect the fact that $\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{c}}+{\overline{F}}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}}^{\mathrm{t}$ does not vary with flow directions (0.74–0.79 $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$). The noise levels for the cis and the trans flagella are taken as ${T}_{c},{T}_{t}=1.57,\phantom{\rule{thinmathspace}{0ex}}9.42$ rad^{2}/s. Under unilateral flagellar coupling, the collective noise level approximates to $T}_{c$ and the value corresponds to typical experimental observations (Quaranta et al., 2015). The sum of interflagellar coupling $\lambda ={\lambda}_{ct}+{\lambda}_{tc}$ is set to be large enough, i.e., $\lambda =3\left{f}_{t}{f}_{c}\right$, to account for the fact that: (1) the coordinated beating is approximated inphase, and (2) up until the strongest flow applied, the interflagellar synchronization cannot be broken (quantitative evaluation is detailed in Appendix 1: MonteCarlo simulations). To model wt cells under calcium depletion, we decrease $\u03f5}_{\mathrm{c}}+{\u03f5}_{\mathrm{t}$ by 15%  which is the mean decrease in the observed $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{cis}}\text{flow})$, $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\text{frontalflow})$, and $\displaystyle \phantom{\rule{thinmathspace}{0ex}}\epsilon (\mathit{\text{trans}}\text{flow})$(Figure 3E). For ptx1 cells, we assume a symmetric interflagellar coupling and set the noise level of both flagella to that of the trans, ${T}_{t}=9.42$ rad^{2}/s. The parameters are summarized in Table 1.
Appendix 1
Hydrodynamic computation for asymmetric loading
Here, we present the computation results for the flagellar loads under flows of different directions, see Appendix 1—figure 1. Realistic flagellar shapes are tracked from the video recordings. Background flows begin with a marked event (flash light) which defines the zero time (see the dashed lines at t=0). After several beats (shaded in blue), the cell becomes entrained by the flows, see the left panels Appendix 1—figure 1A1H1. Meanwhile, the right panels (A2H2) show the median and the interquartile range of $F}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$ and $P}_{\mathrm{F}\mathrm{l}\mathrm{o}\mathrm{w}$ over the flowentrained beats, respectively. Force magnitudes are scaled by $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}=6\pi \mu R{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ = 9.9 pN, which is the Stokes drag on a typical freeswimming cell (radius R=5 µm, swim velocity $U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ = 110 µm/s); while the viscous powers are scaled by $P}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}={F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}=6\pi \mu R{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}^{2$ = 1.1 fW. Here µ = 0.95 mPa·s is the dynamic viscosity of water at 22 °C. Panels A2F2 are presented and described in the main text. For the flow along 0°, the mean force is 0.37 $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ and 0.34 $F}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ (panel G2) while the mean power is –0.2 $P}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ and –0.4 $P}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}$ (H2), for the cis and the trans flagellum respectively.
Extracting coupling strength by fitting phase dynamics
In the main text, the flagellumflow forcing strength $\epsilon$ in wt cells is mainly extracted from the entrainment profile ($\tau (\nu )\ge$ 0.5). Meanwhile, in previous works (Polin et al., 2009; Quaranta et al., 2015), fitting the distribution of phase dynamics is employed to extract $\epsilon$. In the latter approach, the idea is that the phase locking during entrainment leads to a peaked probability distribution of $\mathrm{\Psi}$ (the difference between the flagellar phase and the flow’s phase), whose width is broadened by the noise. The distribution, $P(\mathrm{\Psi})$, can be derived from the Adler equation (Equation 1 in the main text) as:
Here $V(\mathrm{\Psi})=2\pi \nu \mathrm{\Psi}2\pi \epsilon \mathrm{cos}(\mathrm{\Psi})$ is a washboard potential, $T$ is the effective temperature in phase dynamics.
Here, we demonstrate that these two approaches are equivalent in extracting $\epsilon$. For all wt cells tested in the TRISminimal medium (N=11), their $\epsilon$ measured by the $\tau (\nu )$ width and extracted from fitting are plotted against each other, Appendix 1—figure 2. All points center around the identity line (y=x), showing the equivalence in obtaining $\epsilon$ by the two methods. For the ptx1 dataset displayed in the main text, $\epsilon$ are extracted from fitting the phase dynamics.
MonteCarlo simulations
Governing equations for the phase dynamics
The external flow and the two flagella are described by three coupled ordinary differential equations (ODEs), for the phase of the cis flagellum $\varphi}_{\mathrm{c}$, the phase of the trans flagellum $\varphi}_{\mathrm{t}$, and the phase of the external flow $\varphi}_{0$:
The phase dynamics $\varphi}_{0$, $\varphi}_{\mathrm{c}$ and $\varphi}_{\mathrm{t}$ depend on the intrinsic frequencies, with $f}_{0$ the frequency of the external flow, $f}_{\mathrm{c}$ and $f}_{\mathrm{t}$ the intrinsic beating frequencies of the cis and the trans flagellum respectively. $\lambda}_{tc$ represents the strength of the forcing exerted by the trans flagellum on the cis flagellum and $\lambda}_{ct$ the forcing exerted by the cis flagellum on the trans flagellum. Finally, $\u03f5}_{c$ represents the strength of the susceptibility of the cis flagellum to flow entrainment and $\u03f5}_{t$ the susceptibility of the trans flagellum to flow entrainment. The flow is assumed to be noise free (Equation 5), the cis and the transflagella are assumed to have noise levels $\zeta}_{c$ and $\zeta}_{t$ respectively. The noises are assumed to be Gaussian, such that ${\zeta}_{\mathrm{c},\mathrm{t}}(\tau +t){\zeta}_{\mathrm{c},\mathrm{t}}(\tau )$ = 2 ${T}_{c,t}\delta (t)$. In this study, the phase dynamics of these equations are examined using MonteCarlo simulation. The temporal resolution of the simulations ($dt$) is 1ms, which corresponds to the experimental frame rates (801 Hz). Hereafter, we derive analytical solutions to these equations in the limits of oscillatory steady states. For this, we rewrite the phase dynamics as functions of the interflagellar phase difference Δ and the average flagellar phase $\mathrm{\Phi}$ defined as:
Here, $\mathrm{\Psi}$ represents the difference between the average phase $\mathrm{\Phi}$ and the phase of the flow forcing $\varphi}_{0$. For a complete summary of the symbols used throughout this article, please see Appendix 1—table 1. Equation 5 can be rewritten as:
where $\nu}_{\mathrm{c}\mathrm{t}}={f}_{c}{f}_{t$, $\lambda ={\lambda}_{ct}+{\lambda}_{tc}$, $\nu ={f}_{0}f$, $\displaystyle f=\frac{{\lambda}_{ct}{f}_{\mathrm{c}}+{\lambda}_{tc}{f}_{\mathrm{t}}}{\lambda}$, $\displaystyle \zeta =\frac{{\lambda}_{ct}{\zeta}_{\mathrm{c}}+{\lambda}_{tc}{\zeta}_{\mathrm{t}}}{\lambda}$. The phases from both flagella can be easily recovered from the phase difference and the average phase, as: ${\varphi}_{c}=\mathrm{\Phi}+\mathrm{\Delta}/2$, ${\varphi}_{t}=\mathrm{\Phi}\mathrm{\Delta}/2$.
Flagellar synchronization
We first consider the synchronization between the cis and the trans flagella, in the absence of external flow, such that we assume: ${\u03f5}_{c}=0$ and ${\u03f5}_{t}=0$. When the flagella are synchronized to one another, $\dot{\mathrm{\Delta}}=0$, we can directly deduce from Equation 7 that the two flagella beat synchronously at the frequency:
In addition, from Equation 7 we can deduce the steadystate phase difference $\mathrm{\Delta}$, which satisfies:
It is therefore obvious that the two flagella can only synchronize (${\dot{\varphi}}_{\mathrm{c},\mathrm{t}}=f$) when $\left{\nu}_{\mathrm{c}\mathrm{t}}\phantom{\rule{thinmathspace}{0ex}}/\phantom{\rule{thinmathspace}{0ex}}\lambda \right\le 1$.
Interaction between three oscillators
We focus our discussion on the case when the cis and the trans flagella are synchronized in phase, as is observed in all of our experiments. Here, $\dot{\mathrm{\Delta}}=0$ and $\mathrm{\Delta}\approx 0$, which is realized for values of the parameters such that: $\lambda \gg {\u03f5}_{\mathrm{c},\mathrm{t}}\gg {\nu}_{\mathrm{c}\mathrm{t}}$. Equation 7 reduces to:
with $\epsilon =\left({\lambda}_{ct}{\u03f5}_{c}+{\lambda}_{tc}{\u03f5}_{t}\right)/\phantom{\rule{thinmathspace}{0ex}}\lambda$. For the sake of clarity, we recall here that $\nu ={f}_{0}f$, $f=\left({\lambda}_{ct}{f}_{\mathrm{c}}+{\lambda}_{tc}{f}_{\mathrm{t}}\right)/\phantom{\rule{thinmathspace}{0ex}}\lambda$, $\lambda ={\lambda}_{ct}+{\lambda}_{tc}$ and $\zeta =\left({\lambda}_{ct}{\zeta}_{\mathrm{c}}+{\lambda}_{tc}{\zeta}_{\mathrm{t}}\right)/\phantom{\rule{thinmathspace}{0ex}}\lambda$. It is noteworthy that Equation 10 is the same Adler equation as the one introduced in Equation 1 of the main text. This equation represents the phase dynamics of a single phase oscillator evolving under external periodic forcing (Pikovsky et al., 2001). In this strongcoupling limit, when interflagellar coupling strength $\lambda$ are much larger than flow’s effective forcing strength $\epsilon$, the coupled flagella simply work as one single oscillator of intrinsic frequency $f$. The phase dynamics is characterized by $f$, $\epsilon$ and $\zeta$, which are weighted averages of $f}_{\mathrm{c},\mathrm{t}$, $\epsilon}_{\mathrm{c},\mathrm{t}$ and $\zeta}_{\mathrm{c},\mathrm{t}$  the characteristics of the cis and trans flagella. Our main experimental observations can all be explained by the limit when the interflagellar forcing of the cis on the trans is much larger than that of the trans on the cis, such that $\lambda}_{ct}\gg {\lambda}_{tc$. In this case, $\epsilon \approx {\u03f5}_{c}$, which is consistent with the observation that flow entrainment is only a function of the hydrodynamic loads on the cis flagellum. Lastly, $\zeta \approx {\zeta}_{\mathrm{c}}$ is consistent with the observation that the noise in the phase dynamics when wt cells are entrained by the flow, is much smaller than the noise recorded for ptx1, which is putatively considered to have two trans flagella. In fact, when $\lambda}_{ct}\gg {\lambda}_{tc$, $\zeta \approx {\zeta}_{\mathrm{c}}$ satisfies even in the absence of imposed flows, which explains why the breaststroke beating (IP mode) of ptx1 is much noisier than that of wt (see the last section of Appendix 1).
Lower limit of interflagellar coupling
Lastly, we turn to the model’s behaviors when two flagella are not necessarily in synchrony, and we focus on the regime where $\lambda \left{\nu}_{\mathrm{c}\mathrm{t}}\right$ is comparable to $\u03f5}_{\mathrm{c},\mathrm{t}$. The primary question is: from the fact that even the strongest flow in our experiment could not disrupt interflagellar synchrony, can we infer a lower limit of λ? We assume $\left{\nu}_{\mathrm{c}\mathrm{t}}\right=20$ Hz (Kamiya and Hasegawa, 1987; Kamiya, 2000; Okita et al., 2005; Wan et al., 2014) and focus on the entrainment by the frontalflow. To further simplify the picture, coupling between cis and the trans are set as equal, $\lambda}_{ct}={\lambda}_{tc$.
The value $\left(\lambda \left{\nu}_{\mathrm{c}\mathrm{t}}\right\right)/\phantom{\rule{thinmathspace}{0ex}}\epsilon$ with $\epsilon ={\u03f5}_{c,t}$ determines if the flow can disrupt the synchrony between cis and trans. We plot the synchronization/entrainment profiles with increasing λ in Appendix 1—figure 3. When it satisfies $\left(\lambda \left{\nu}_{\mathrm{c}\mathrm{t}}\right\right)/\phantom{\rule{thinmathspace}{0ex}}\epsilon \ge 2$, external flows cease to affect the flagellar synchronization observably. As the strongest flow ($21{U}_{\mathrm{s}\mathrm{w}\mathrm{i}\mathrm{m}}$) applied experimentally corresponds to $\epsilon \approx 10$ Hz, altogether, we conclude that $\displaystyle \lambda \gtrsim \left{\nu}_{\mathrm{c}\mathrm{t}}\right+2{\epsilon}_{\mathrm{m}\mathrm{a}\mathrm{x}}=40$ Hz. In the main text, we set $\displaystyle \lambda =3\left{\nu}_{\mathrm{c}\mathrm{t}}\right=60$ Hz, which satisfies this relation and matches the observation that the phase lag between the flagella (Δ) is small.
Noise in the beating of the ptx1 mutant
Here, we show an asyet uncharacterized strong noise present in the synchronous beating of the mutant ptx1. The inphase (IP) mode of ptx1 cells and the breaststroke beating of the wt cells are similar in waveform and frequency (Horst and Witman, 1993; Rüffer and Nultsch, 1997; Leptos et al., 2013). However, the former has a much stronger noise.
The strong noises show obviously in fluctuations of IP beating frequencies (similar to data shown in Leptos et al., 2013). In Appendix 1—figure 4, we display the distribution of beating frequency of a representative wt cell (panel a) and four representative ptx1 cells (panels be). The broad peaks of the IP (purple) and AP (yellow) beating of ptx1 sharply contrast the narrow peak of wt. We quantify the frequency fluctuations of all the cells displayed in the main text (N=11 for wt and N=14 for ptx1) in Appendix 1—figure 4f. The cells are represented by their mean beating frequencies over time $f$ and the standard deviations $\sigma (f)$. Clearly, the breaststroke beating of wt, the IP, and the AP mode of ptx1 each forms a cluster. The wt cluster is at $(f,\sigma (f))=(50.5\pm 2.6,\text{}0.8\pm 0.3)$ Hz (mean±1 std. over cell population); and is less dispersed than both the IP and the AP modes of ptx1, which are at $(47.4\pm 3.1,\text{}3.4\pm 0.9)$ Hz and $(67.6\pm 2.1,\text{}1.9\pm 0.7)$ Hz, respectively. Under the assumption of a white (Gaussian) noise, $\sigma (f)$ is proportional to the amplitude of phase noise $\zeta$, and thus scales with $\sqrt{T}$. Considering that $\sigma (f)$ for ptx1 is three to fivefolds larger than that of wt, we conclude that the effective temperature of phase dynamics in ptx1 is an order of magnitude larger than wt, ${T}^{ptx1}/{T}^{wt}\sim \mathcal{O}(10)$.
The stronger noise in ptx1 can be attributed to two sources, namely, the loss of a stable cis and the loss of the unilateral coupling, Appendix 1—figure 5. We perform MonteCarlo simulations of the coupled beating of two flagella under three conditions (see the blue, yellow, and red data in Appendix 1—figure 5 respectively): (1) a cis coupled with a trans unilaterally ($\lambda}_{ct}=4{\lambda}_{tc$); (2) a cis coupled with a trans reciprocally ($\lambda}_{ct}={\lambda}_{tc$); and (3) two trans flagella coupled with each other reciprocally. We fix the noise level of the cis at $T}_{c}=1.57\text{}\mathrm{r}\mathrm{a}\mathrm{d}/{s}^{2$ and we vary the noise of the trans to compare how the increase in transnoise would destabilize the synchronous flagellar beating.
When a trans is unilaterally following the cis, increasing the transnoise over an order of magnitude only leads to a ~20% stronger frequency fluctuation (the blue line in Appendix 1—figure 5a). On the contrary, lacking either the unilateral coupling or the lownoised cis would increase the fluctuation for 200% (yellow line) or 300% (red line). Qualitatively, simulation results are in agreement with experimental measurements assuming that ${T}_{t}/{T}_{c}\sim \mathcal{O}(10)$, see the red and blue shaded areas in Appendix 1—figure 5a. Additionally, even when the cis and trans flagella exert equal forcing on one another ($\lambda}_{ct}={\lambda}_{tc$), having a lownoise cis flagellum already helps prevent phase slips from interrupting the interflagellar synchrony. This can be seen from Appendix 1—figure 5b: as long as a lownoise cis is present (yellow and blue data), slips will be sparse (< 0.01 Hz). Together, these simulation results highlight the stabilizing effect of a lownoise cis flagellum, and illustrate that a unilateral coupling further enhances the stabilization.
Data availability
The data and the code underlying this study is openly available at the 4TU. ResearchData repository: https://doi.org/10.4121/21972695. Codes for modeling and plotting, and the hydrodynamic computations' data are included.

4TU.ResearchDataDataset and codes underlying "The younger flagellum sets the beat for C. reinhardtii".https://doi.org/10.4121/21972695
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Article and author information
Author details
Funding
European Research Council (101042612)
 MarieEve AubinTam
European Research Council (716712)
 Daniel SW Tam
European Research Council (101045302)
 Daniel SW Tam
The funders had no role in study design, data collection and interpretation, or the decision to submit the work for publication.
Acknowledgements
The authors thank Roland Kieffer for technical support. DW thanks Ritsu Kamiya for helpful discussions. The authors acknowledge support by the European Research Council (ERC starting grants no. 716712 and no. 101042612, and ERC consolidator grant no. 101045302).
Version history
 Received: January 11, 2023
 Preprint posted: January 30, 2023 (view preprint)
 Accepted: April 3, 2024
 Version of Record published: May 16, 2024 (version 1)
Copyright
© 2024, Wei et al.
This article is distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use and redistribution provided that the original author and source are credited.
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