Modeling Overview
In light of our guiding principles (specificity, regulation and biocontainment), we modelled four different aspects of BeeT. The modelling work can inform and aid the improvement of wet-lab experiments. Another facet is to assess the optimal application strategy for BeeT in real world applications. We asked ourselves; what parts of our system can benefit the most from an interplay between modelling and experimental work? These considerations led us to ask the following questions:
- How can we assure optimal toxin production using quorum sensing and subpopulations?
- What are important parameters for the optogenetic killswitch to function optimally?
- Will BeeT be capable of surviving in sugar water?
- What is the best application strategy for BeeT?
Population Dynamics
For the final product, BeeT, we intend to use toxins produced by Bacillus thuringiensis, also called Cry toxins. However, these toxins are also harmful to our chassis, resulting in a reduction of toxin production when it is needed to kill the mites. To counteract this effect we envision the use of quorum sensing that activates Cry toxin production only when there is a large quantity of BeeT present. Ideally, BeeT is able to produce Cry toxin over a long period to improve its effectiveness against mites. However, if an entire population of BeeT is synchronized, we hypothesize that only a single burst of Cry toxin will take place before both the BeeT and mites are killed. Thus, this system will not be maximally effective over long time periods. To accomplish this we need multiple subpopulations of BeeT: some producing BeeT while others are recuperating. To help understand this complex system we use dynamic modelling.
What is Quorum Sensing?
Quorum sensing is a cell-cell communication system. The detection of chemical molecules allows the bacteria to sense the presence of other bacteria. In this way the bacteria control gene expression in response to changes in cell number 1,4. This process is achieved through the production and release of an Acylated Homoserine Lactone (AHL) autoinducer An autoinducer is a molecule that can diffuse through the cell membrane. . The AHL can diffuse from one cell to the other. There are many different types of autoinducers in quorum sensing systems. When sensed, the autoinducer can trigger other cells to produce more autoinducers.
Genetic circuit
The quorum sensing system consists of two proteins: LuxI and LuxR. LuxR is constitutively expressed, together with AHL it forms a complex which activates the transcription of a toxin. In our case we use the detection protein Green Fluorescence Protein (GFP) to follow the behaviour of the system 2. LuxI encodes an AHL synthase. AHL is a molecule that can diffuse freely through the cell membrane, and in this way travels from cell to cell. LuxR encodes for a protein and together they form a complex. In a natural system the LuxR-AHL complex controls transcription of LuxI, forming a positive feedback loop that increases the amount of AHL in the system 3. When there is more AHL in the system, AHL is more likely to bind to the LuxR protein. In Figure 1 you can see a schematic representation of the system.
According to the 2011 team from Davidson College and Missouri Western State University5, LuxR protein represses transcription of the luxR gene in the absence of AHL, establishing a negative feedback. We investigated whether this negative feedback can be used to create different populations. As you can see in Figure 2 different states of GFP responses can occur when the production rate of luxR and rate of complex formation are changed. However, when we remove the feedback in the system and change the same parameters, we get similar responses of the system as shown in Figure 3.
This shows that the feedback has a minimal influence on the system to create different subpopulations. Also when there is no negative feedback in the system, we found more parameter sets that give a high amount of GFP (see Figures 4 and 5).
The figures are simulated with the parameter sets obtained from the quorum sensing model. We are using the parameter sets that give the best response according to the confidence intervals (see Method section). In the presence and absence of negative feedback, the system behaves similarly by assuming the production rate of luxR and the formation rate of the complex are different in each cell. The quorum sensing system can simulate different responses with the same cells and different parameters, if we could control the LuxR production rate. However, we could not envision a method of doing this experimentally. We aim to make cells that are genetically identical but still can respond differently. Therefore, we designed another system that could help us create this response downstream of the quorum sensing mechanism. The two systems were tested in the lab parallel with the modeling.
Why include a subpopulation system?
Since the quorum sensing mechanism could not provide the subpopulations we desired using genetically identical cells, we created a system that could act downstream of quorum signalling to provide the response we needed. Population-wide Cry toxin overexpression if likely to kill all E. coli cells in the first moment of toxin expression. Since this would only affect one of the subpopulations, the second subpopulation would be able to initiate a new growth phase after death of the toxin-producing cells. The critical requirement for this is that cells respond at different times to the quorum stimuli despite being genetically identical. A small part of the population that acts differently from the rest of the population is called a subpopulation. The subpopulation system consist of two genes; the first encodes for the protein that inhibits the systems expression, the other encodes for the corresponding activation protein of the system. The 434-cI-LVA inactivates the λ-cI directly, or prevents the translation of the λ-cI protein. 434-cI-LVA has a higher turnover rate than λ-cI. This subpopulation system is based on a natural system for persister cell formation. 6.
As you can see in Figure 6, glucose has a suppressing function on the system. Arabinose has a activating function on the system. We used the model to predict what will happen when we add glucose in different amounts. The assumptions we made for the subpopulation system are the following; 434-cI-LVA degrades faster than λ-cI, cell division happens when the cell size has doubled, and two cell populations exist with one growing differently than another. We tested a number of parameter sets and picked the parameter set that gave the biggest RFP response based on the strength of glucose. To see how the model behaved when we changed the ratios of the initial amounts of λ-cI and 434-cI-LVA we investigated the effect of starting conditions on the outcome of the system. The initial conditions were varied between 1 and 10. Within the heat map you can see in which ratios the initial amounts of λ-cI and 434-cI-LVA in the system are needed to get high RFP production (here glucose and arabinose have a fixed concentration).
Shown in Figure 7 when λ-cI and 434-cI-LVA are present in similar amounts we have a subpopulation system. But if they are present in different amounts than there will be no subpopulations. This can be expected when you look at the subpopulation system. The system is inhibited by 434-cI-LVA, which represses the RFP production, and λ-cI activates the RFP production. In figure 4 you can see balance between the 434-cI-LVA and λ-cI amounts that are present for the output of RFP. This means that the initial conditions do not have much influence on the λ-cI and 434-cI-LVA. With this particular parameter set, we can conclude that the translation rates are more important for the RFP response than the initial conditions. For other parameter sets the initial conditions are important. To understand how changing the Ribosomal Binding Site (RBS) impacts RFP responses, we simulated the system for different combinations of transcription rates. From these simulations we found:
Lambda | 434-cl-LVA | RFP responses |
---|---|---|
1.94 | 135.6 | 7.00 |
1.94 | 108.8 | 8.51 |
1.94 | 942.5 | 1.48 |
1.94 | 726 | 1.77 |
1.94 | 628.6 | 1.962 |
1.94 | 577.1 | 2.09 |
1.94 | 529 | 2.23 |
1.94 | 40.3 | 20.1 |
1.94 | 384.9 | 2.87 |
1.94 | 268.5 | 3.87 |
1.94 | 257.8 | 4.01 |
1.94 | 256.7 | 4.02 |
1.94 | 73.2 | 12.1 |
1.94 | 100.9 | 9.09 |
To confirm that our model represents Biological behaviour we analysed the RBS library. We can conclude out of these results that the RFP quantitatively corresponds to the Figure 7.
Combined system
Based on the modeling we hypothesized the following: When there are more cells are present in the system, more AHL-LuxR complex is formed. The complex inhibits the subpopulation promoter. When the promoter is inhibited production of 434 will be suppressed and production of λ cl will be activated. At a certain time point λ-cl takes control over the system, because 434 has a higher turnover rate than λ-cl. In this case more λ-cl results in more RFP.
In a later stage, to get the desired response, the quorum sensing system and the subpopulation system were combined. As shown in Figure 8, you can see how we think to generate different cell populations. With this extended part we try to generate a system which predicts the behaviour of the subpopulations. In figure 9 you can see the increasing RFP over time after many cell divisions, indicating an increasing cell population.
Methods
During the research Matlab version R2016a has been used.
Because there was no data from the wet lab we assumed that all parameters exist within a biologically reasonable range numbers between 0 and 1. For the analyses we used 100.000 parameter sets, 10 cells, random initial conditions and 60 timesteps. Tuneable parameters are used, each parameter set can produce dramatically different population dynamics. To determine which of these parameters produce the best system response we used Latin Hypercube Latin hypercube is a statistical method to get random numbers from a box of x by n numbers. For example, if x = 4, where x is the number of divisions within the parameter value range, and n = 2, where n is number of parameters, you will obtain a box with 4 square times 2 square, giving you 24 random numbers. Within each division of the parameter space a single random number is chosen. sampling.
With the parameter numbers of the Latin Hypercube sampling we made parameter sets that are obtained from a lognormal distribution a lognormal distribution assigns probabilities to all positive values. However the distributions is skewed to favour smaller values. Biological reaction rates have been found to follow this distribution 8 with a parameter estimation based on Raue et al 7. Below you could see an example;
With these confidence intervals Equation for confidence interval used the best parameter sets could be chosen.
In conclusion
Quorum sensing ensures that the toxin is only produced when the density of bacteria is high enough, this standardizes the amount of toxin produced by the bacteria population.
The subpopulation system was coupled to the quorum sensing system. Together, quorum sensing and formation of non-producing subpopulations allow bacteria to produce waves of toxin.
With the results of the combined system we can conclude that waves of toxins are produced. Different parameters in the quorum sensing system elicit different GFP responses.
However, we can not expect to be able to make genetically identical cells with varying values for these parameters
with the subpopulation system we may be able to predict which RBSs of the library have the highest chance to successfully create subpopulations. The library in further research it could be tested in the lab.
Optogenetic Kill Switch Model
One important aspect of our project is the biocontainment of BeeT to the hive, preventing it from spreading into the environment. In collaboration with the wet-lab, we designed an optogenetic kill switch based on the blue light sensing pDusk and pDawn systems as described by Ohlendorf et al.1. The cell death is inflicted by the mazEF toxin-antitoxin (TA) system. The latter functions by the antitoxin (mazE) preventing the toxin (mazF) from cleaving mRNAs which ultimately kills the cell. With the underlying biology of the system in mind, we used synthetic bioengineering principles to mathematically describe our design and explore the dynamics of the system.
Our results show that we have a working mathematical model which describes the data of Ohlendorf et al.1. With this model, we now know where to look for the relative kinetic rates in the parameter space to give suggestions to the wet-lab on how to build a functioning optogenetic kill switch. Our differential equations of pDusk and pDawn can also be used by future iGEM teams to mathematically describe and build new optogenetic tools.
Light On
Modelling The Optogenetic Tool
For the first part of our analysis, we optimized the mathematical models of pDusk and pDawn using published data1. For now, we ignored the toxin-antitoxin system. This gave us the option to construct our scoring function to evaluate both systems simultaneously with a weighted means approach.
By constructing an accurate model of the optogenetic part of our overall kill switch system, we are confident that we are mathematically representing the behaviour of the microorganism in the lab. Results from the model can then be used as a reference point for building the toxin-antitoxin system into the kill switch model. We will search the parameter space to identify parameter sets which fit the data given in Figure 2a by Ohlendorf et al.1. In addition, we will select the best fit to data based on a scoring function as described by Raue et al.4. Lastly, we provide a mathematical model which can be used by future iGEM teams to build new optogenetic tools.
System Design
We first studied the pDusk system in more detail to derive simplified equations which can describe the system behaviour. The genetic switches are based on the interactions between the light sensing protein YF1 and the response regulator FixJ as described by Möglich et al.2. In darkness, YF1 phosphorylates FixJ, which in turn activates the promoter pFixK2. This activation leads to the expression of the desired genes. Under light conditions, YF1 enters an excited light-state, which inhibits the phosphorylation of FixJ. In addition, it prevents the activation of the pFixK2 promoter and thus represses the target genes in Figure 1 for pDusk.
The pDawn system functions in the same way as the pDusk system, with the addition of cIλ being expressed depending on the activity of the pFixK2 promoter. The protein form of cIλ inhibits the expression of the RFP reporter gene in Figure 1 for 1 pDawn.
Assumptions
To derive mathematical equations describing the above systems, we made some simplifying assumptions.
Wwe neglect the effects of dilution/ growth. We thus assume the cell’s volume to be constant over time.
Wwe assumed that the components in our system are not affected by and do not affect other cellular mechanisms.
Aas there is no additional information gained from modeling transcription and translation for the dark state of Yf1(yDD) and the inactive form of FixJ (ji) we lumped these processes and assumed that they can be described by a single parameter. This results in a less computationally expensive system.
We also assumed the rates of production, binding and degradation of mRNAs and proteins to be linear which resulted in a first order differential equations system
To model the influence of light on the system, we assumed light activation to occur similar to the model ofn phytochrome B dimerization described in Klose et al.3 (). In addition, we consider in our system the different stages of Yf1 (yDD, yDL/LD, and yLL) as described by Möglich et al.2. Translated to our system, this means that with increasing light intensities (N), the pool of activated Yf1 (yDL/LD and yLL) would deplete the dark state of Yf1 (yDD), which is responsible for the phosphorylation and thus activation from inactive FixJ (ji) to active FixJ (ja). As all stages of Yf1 form a dimer, we assumed dimerization to occur quicklyvery fast and be the dominant and relevant form for our system. Lastly, we assumed a quasi steady-state approximation (Michaelis-Menten kinetics) for the effect of activated FixJ (ja) on the expression downstream of the RFP (RFPm) reporter gene. A detailed system design is provided SOMEHWERE!?
Results
With our mathematical model we can describe the behaviour of both systems as tested in the lab by Ohlendorf et al.1.( See Figure 2). We can thus say that we built a simplified mathematical representation of the pDusk and pDawn system which can describe the systems’ behaviour.
Preliminary results from the lab show that the RFPp response after 17 hours incubation time is weak using the pDusk system. The experiment was conducted in darkness and under light intensity (see Table 2).
System | Dark | Light |
---|---|---|
pDusk | ||
pDawn |
The data from the lab suggests that there is not a high change in RFP for the pDusk system between dark and light conditions. When plotting the computed response of RFP for increasing light intensity in Figure 3 we see, however, that pDusk has a steep decline in RFP levels from complete darkness to very low light intensities. There could be two potential reasons for such a result. FirstThis could suggest that, despite all efforts in creating dark conditions, the experiment could have been was contaminated with low light intensities. This wcould explain why there is no significant change visible in the experimental data visible between different conditions. To confirm this, additional experiments would need to be conducted. Additionally, a more in-depth parameter sensitivity and robustness analysis could also reveal potential causes of the discrepancies in between model simulations and experiments conducted under darknesslow light conditions.
We also made the code for both systems available for future iGEM teams to build new optogenetic tools: Model.
Methods
After studying the pDusk and pDawn system, we constructed a parameter estimation procedure by picking random parameter sets based on the latin hypercube Latin hypercube is a statistical method to get random numbers from a box of x by n numbers. For example, if x = 4, where x is the number of divisions within the parameter value range, and n = 2, where n is the number of parameters. With the underlying sampling formula of (x!)^n-1 you will obtain 24 combinations. Within each division of the parameter space a single random number is chosen. sampling (LHS) method in Matlab 2015b (used for the whole study). We simulated 10, 000 parameter sets and assumed the initial conditions of only yDD and ja being in the on state, i.e. we assigned the value one. All other initial conditions were kept at 0. In addition we needed to transform those parameters to a more biologically feasible distribution as LHS generates uniformly distributed parameters. For those parameters where there was no information available, we assumed a widely biologically applicable lognormal distribution that is representative of measured biological rates7. We transformed the two parameters for which experimental data was available according to their known distribution (see Table 1 k2 and k3. We then loaded the RFP response data ± standard deviation from Ohlendorf et al.1 for both pDusk and pDawn and transformed the light intensities from to . For a more detailed explanation see the notebook.
We then simulated both systems according to our ordinary differential equations (ODEs) with the same parameter (sub)-sets and stored the response at 17 hours for later evaluation in the scoring function. We chose to simulate the system until 17 hours, as this is the duration Ohlendorf et al.1 used in their study. As a next step, we normalised the computed RFPp response with the measured response at the highest light intensity used bydata point of Figure 2a from Ohlendorf et al.1.
To evaluate how well a certain parameter set describes the response of the Ohlendorf et al.1 system, we used the sum of squared residuals to score each parameter set as described in Raue et al.4.
wWhere represents data points for each observable at time points . are the corresponding measurement errors and
To construct a corresponding score from the same parameter set for pDusk and pDawn we used the weighted means approach accordingly:
Where represents the score of a parameter set for pDusk and the corresponding score of the same parameter set for pDawn.
To put the equations and parameters into context, we created a more detailed graphical representation of the pDusk and pDawn system and provide the ordinary differential equations for both systems %!here.pdf.
Ordinary Differential Equations for pDusk
Ordinary Differential Equations for pDawn
For pDawn we used the same equations as for pDusk from yDD to ja and added the following differential equations.
Here we show the best parameter set obtained from the parameter estimation (see in Table 1). This parameter set was used as the basis for further analysis implementing the mazEF toxin-antitoxin system. To better put these numbers in context we provide a detailed graphical system representation of pDusk and pDawn in Figure_3.
Parameter | Value | Description |
---|---|---|
k1 | production rate of yDD | |
k2 | relaxation rate of yDL,LD and yLL. We assumed a search space for τ of 5900 ± 25 |
|
k3 | conversion cross-section σ of light intensity activated production rate of yDL,LD and yLL. The search space for this parameter was defined as 1000 ± 25034. | |
β1 | degradation rate of yDD | |
β2 | degradation rate of yDL,LD | |
β3 | degradation rate of yLL | k4 | production rate of ji |
k5 | de-phosphorylation rate of ja | |
β4 | degradation rate of ji | |
k6 | production rate of ja depending on the concentration of yDD and ji | |
β5 | degradation rate of ja | |
Vmax | Vmax of production rate of RFPm based on ja | |
KM | KM of production rate of RFPm based on ja | |
β6 | degradation rate of RFPm | |
k7 | translation rate from RFPm to RFPp | |
β7 | degradation rate of RFPp | |
β8 | degradation rate of lambda phage inhibitor RNAm | |
k8 | production rate of cIp depending on cIm | |
β9 | degradation rate of cIp | |
k9 | maximal production rate of RFPm | |
KD | dissociation constant of cIp at RFPm promoter. The Hill coefficient was chosen to be 2 as the cIp regulated promoter BBa_R0051 has 2 binding sites for cIp. |
Conclusion
With the above mentioned results, we conclude to have built a mathematical model of pDusk and pDawn which describes the system behaviour. We know now where in the parameter space we would need to zoom in to define relative kinetic rates in collaboration with experimentalists. Initial results from the lab, did not show a significant change in response for the pDusk system., However, the experimental results are in agreement with the computed data in the pDawn system. This leads us to suspect that either there was an irregularity with the dark conditions in the lab, or the model does not fully reflect the underlying biology of the system in the lower light intensity regions. We suggest that, in future,to further conduct a parameter sensitivity and robustness analysis could be conducted to find the most likely cause of the mismatch to data. With these results, we can nonetheless implement the equations for the mazEF mediated kill switch as we achieved a good fit to the more robust data given by Ohlendorf et al.1.
Light On, BeeT Off
Modeling The Optogenetic Kill Switch
After building the mathematical system for pDusk and pDawn, we were now able to simulate dark and light conditions. We have an understanding of how the optogenetic tool functions and can now explore the parameter space to find parameter sets which describe the wanted system behaviour and regulation of theincluding the toxin-antitoxin system. As there was no experimental data available in literature to score the combined system, we used conservative constraints which are known from literature5 6 to construct our model for the MazE and MazF kineticsoptogenetic kill switch.
Goals
- Parameter Estimation: Find sets of parameters which give a response within the conservative constraints and thus show us where in parameter space to search in further analysis (e.g. relative kinetic rates of promoters).
- System Selection: As the Biobrick BBa_K081007 is not only used in pDawn, but also in the quorum sensing system, we wanted to have a tool to decide whether we can also use the less favourableBased on data from Ohlendorf et al. (2012), pDusk shows a smaller change in RFPp ratio than pDawn. For the kill switch this translates into a smaller change in antitoxin over toxin (A/T) ratio and thus a smaller likelyhood to kill the cell effectively., but theoretically possible pDusk system in the kill switch design.
System Design
To build the kill switch we first studied the mazEF system and its functionality. The mazEF module is an antitoxin-toxin (TA) system native in E. coli. For the purpose of building a
mathematical model, we describe the relevant aspects of the system here. For more background on the mazEF system, please go to the
wet-lab part.
In the TA system, mazE represents the antitoxin which forms a dimer and binds two dimers of mazF to built an inactive complex under non-lethal conditions5.
The functionality of the system in nature is given by a fast degrading antitoxin and a slower degrading toxin. Once expression of the TA module is terminated, mazE will degrade faster and mazF
will start cleaving mRNAs which ultimately leads to cell death. For the kill switch, we will consider either “under"-production of mazE in pDusk or overproduction of mazF in pDawn both under light
inducing conditions (see Figure XY).
Constraints
For the parameter estimation of the optogenetic kill switch, all the assumptions mentioned in the above sections hold. Further, we assumed a lumped mazEF complex formation, where we disregard potential intermediatery stages of complex formation. In addition, we defined the following new constraints:
- As we have literature data supporting that mazF degrades faster than mazE5, we exploited this as a constraint in our parameter generation procedure.
- Another constraint was added to the system as the ratio of free A/T is assumed to be bigger than one6 under non- inducing conditions.
- Lastly, we added a logical constraint. Under the highest simulated light intensity, the A/T ratio has to be smaller than one
Results
We can show, that our parameter estimation procedure found two parameter sets, out of 1000 sampled sets, which satisfy these conservative constraints (see animated Figure 7 and Figure 8).
The two parameter sets give us an indication where in parameter space we will have to focus on for further analysis. These two sets also both describe a functioning pDusk and pDawn based optogenetic kill switch. Although, one might argue, that set number one (blue and red lines) is to be favoured as the change in mazE in pDusk compared to the change of mazE of set two (yellow and purple lines) in pDusk is higher and thus more likely to function and kill the cell. Future experiments on promoter strengths can be normalised to the model data. With such additional information, an indication can be given on which relative kinetic parameters are needed to make the system work.
When plotting the A/T ratio against the increasing light intensities, it becomes more evident that parameter set 1 has a higher change in the A/T ratio within pDusk between different light intensity conditions and is thus to be slightly favoured. To further evaluate these findings, more data from the lab is needed.
Methods
Looking at Figure_9 we can see that adding the mazEF module to the pDusk/ pDawn system requires another 10 parameters to describe the system. We constructed our parameter estimation similar to the parameter estimation of the previously described procedure and evaluated the system based on the constraints described above. It should be noticed here, that this is a qualitative evaluation and is not backed by statistical real world data. Nonetheless, it gives and indication about the real world situation.
We then took the best parameter set from the pDusk/ pDawn evaluation and added the equations describing the interactions with the MazEF systemnew parameters to the set of ODEs.
As we noticed that we have to discard around half of the parameter sets as they do not satisfy the constraint that mazE degrades faster than mazF, we built this constraint already into the parameter sampling procedure.
In addition, a mazEF deficient E. coli. strain was engineered in the lab to prevent any interaction between the native and the engineered mazEF system.
In Silico Kill Switch
After studying the optogenetic tools pDusk and pDawn as well as the integration of the mazEF toxin-antitoxin system, we can conclude, that we achieved a good fit in Figure 2 to the data available in literature by Ohlendorf et al.1. Further, preliminary data from our experiments shown in Table_2, can be explained by our model simulations.
We then studied the mazEF toxin-antitoxin integration to design our optogenetic kill switch. After analysis of this system, we found two parameter sets, which satisfy the constraints. These parameters give us an idea for how to search the parameter space for further analysis to select functioning kinetic rates in collaboration with the wet-lab.
In addition, future work could show the effect of parameter sensitivity (such as leaky promoters) we could give further suggestions to the wet lab using for example RBS libraries and their effect on the systemrelative expression rates to engineer the pDusk system, to adjusting it to suit ourfor the needs of our conditions for the optogenetic kill switch.
Lastly, we made the code available for future iGEM teams to design new optogenetic tools.
Metabolic Modeling
In order to assess the real world viability of BeeT, we evaluated the proposed system of application by making a model of the entire system. To do this we used Flux Balance Analysis (FBA) to model the chassis. The chassis The chassis-organism is the framework that is modified for use in synthetic biology experiments. of BeeT is a variant of Escherichia coli, for which it is known that it does not grow overnight in high osmotic pressure environments of 1 mol sucrose / liter or above. 1 Supplementing an Apis mellifera (honey bee) colony with sugar water is a well established practice amongst beekeepers. 4 This is usually done with about 1 kg of table sugar for each liter of table sugarChemically speaking this is pure sucrose: C12H22O11. After heating and stirring, this ends up as a concentration of 625 grams of sucrose per liter of water. This concentration can also be defined as 1.82 mol sucrose per liter, which is almost twice the threshold value at which E. coli would no longer grow. However, in this project we only need the E. coli to survive in the sugar water. This only needs to be as long as the worker bees require to pick the BeeT-cells up and bring them to where the Varroa destructor are. The question we try to answer is: does our chassis survive in the sugar water, and if so, for how long?
A model of E. coli survival
In order to make this model a technique called Flux Balance Analysis (FBA) was used to describe the relationship between the metabolism of the E. coli and the osmotic pressure of the sugar water. FBA is a mathematical method that can be used for predicting reaction fluxes and optimal growth rates of species using genome-scale reconstructions of their metabolic networks. In this case we used it to specifically predict the effect of water efflux on the total amount of ATP the cell has available for maintenance. The model used as a base for this analysis was iJO1366 3from the BIGG database.
The relationship between maximum ATP available for survival and water efflux is shown in Figure 1 the results from the metabolic model suggest that there is a linear relationship between ATP availability and water efflux. This implies that if no water is available for ATP used for maintenance, the cell will die. When the model runs without any modification, i.e. in an environment where it is in the exponential growth phase, an ATP Maintenance flux of 3.15 mmol⋅gram Dry Weight-1⋅hour-1 is given as output by the model.
We do not know the exact amount of ATP needed for survival in sugar water conditions, but because of the results from Figure 1 we can start looking at the relationship between survival time and water efflux.
In Figure 2 we can see not only the relationship of survival time against max ATP available for survival, but also how different thresholds of minimal cell-water tolerance would affect this relationship. The minimal cell-water tolerance threshold gives the value at which percentage of the remaining cell-water reaches a state that will cause cell-death. This has a drastic effect on survival time, changing 20 minutes of maximum survival time to a mere ~90 seconds in the worst case scenario.
Up to 90 minutes
Figure 1 shows us that osmotic pressure alone can indeed have an effect on cell regulation and cell death, and from Figure 2 it appears that the minimal water allowance threshold has a high impact on range of possible times. Our model is limited in that it predicts an infinite survival time beyond 90 minutes. This suggests that our model may be missing some form of regulation that allows for longer survival times. To understand this effect, we conducted an experiment to test this prediction. This experiment can be found here.
What we can say is that if the cells can survive for longer outside of this period, then they must have enough ATP available for basic maintenance. If cell death occurs, other processes than pure water-efflux must be the cause of that. This could be due to a combination of lacking nutrients and water-efflux, or over production of osmolytes to keep the balance.
Beehave
Due to regulatory and experimental hurdles it is difficult to test the effectiveness of BeeT in combating Varroa destructor. We would still like to be able to give advice to local beekeepers on the ideal application strategy of BeeT, based on several scenarios. To accomplish this, the previously published model BEEHAVE was adapted to include the effect of BeeT on Varroa mite and virus dynamics in simulated colonies. BEEHAVE is an open-source agent-based model, which can be used to examine the multifactorial causes of Colony Collapse Disorder
1
2
.
It consists of several modules which control aspects like foraging, Varroa mite dynamics, and colony growth (Figure 1), and was extensively tested for robustness and realism
1
.
BeeT can be transported to the hive by adding it in sugar water or bee bread. Both these sources have their advantages and disadvantages. In this project we have used Escherichia coli as our model chassis, which can be applied to sugar water [link to Ronald]. Sugar water is supplemented to support a colony during honey harvest before winter, as a substitute for nectar
3
4
.
Supplementing Apis mellifera,honey bee, with sugar water is a well established and familiar practice amongst beekeepers
3
. Alternatively, reconstructing the same system in Lactobacillus species would allow us to use BeeT in bee bread. Bee bread has an advantage over sugar water, as it is more frequently transported to larvae. Bee bread is a combination of pollen, regurgitated nectar, and glandular secretions. To protect against harmful micro-organisms honey bees also inoculate bee bread with fermenting bacteria.
5
. The fermentation process reduces the pH
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BeeT Module
BEEHAVE is an open-source GNU licensed agent-based model utilizing NetLogo, and consists of several interlocking modules which each model different aspects of the beehive. It models the wide variety of stresses affecting honey bees. 1 . As such, it is the ideal basis for our investigation into the effects of BeeT on Varroa mites and honey bee dynamics. BEEHAVE has several modules covering colony dynamics, foraging, and a Varroa mite model as depicted in Figure 1. Two viruses are also included in the model: deformed wing virus (DMV), and acute paralysis virus (APV), both for which Varroa mites are a vector. Our BeeT module, which runs parallel to BEEHAVE, is capable of modeling transport of BeeT into the hive using sugar water or bee bread. It also calculates how much BeeT is transported to larvae based on consumption of honey and pollen stores. The Varroa mite mortality is determined by the amount of BeeT near larvae when Varroa mites emerge from brood cells. This in turn affects Varroa mite population levels in the hive, reducing virus loads in the hive, and allowing colony survival.
Assumptions
Not everything is known about the BeeT model, and as such it was necessary to make certain assumptions. Some of these are related to BeeT in general, while others are specific to the sugar water or bee bread applications. We will first discuss general limitations of our model, and then address each of the applications separately.
General assumptions
Several properties of BeeT and its chassis are currently unknown. This includes the degradation rate of BeeT both inside and outside the hive. With both treatments BeeT encounters different environments while being transported to larvae. For sugar water, BeeT is exposed to the honey stomach of bees, honey stores, and brood cells, whereas bee bread encounters pollen and brood cells. We do not know the effects of these different environments on degradation rates of BeeT. For this reason we assumed that degradation rates are stable inside and outside the hive.
Another uncertainty is what the effect of BeeT is on Varroa mite mortality. We modelled this by using a saturating function. We also assumed that the effect of BeeT on Varroa mite mortality is entirely determined by the amount of BeeT present at larvae when a brood cell is capped.
Finally, the BEEHAVE model is only able to model a single virus: DMV or APV. We are unable to model the combined effects of both viruses on a bee colony. For all analyses we used the DWV virus, as it is more harmful to honey bee colony survival than APV
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Sugar water
We know that, based on the experimental results [hyperlink] obtained by metabolic modelling of E. coli, and it is able to survive in sugar water for at least 48 hours. Additionally, modeling predicts that if E. coli is capable of surviving 90 minutes, it can survive indefinitely[hyperlink].
Additionally, we estimate that in sugar water there are approximately 1 * 10^6 cells*ml-1. This estimate is based on the assumption that we add saturated medium (1 * 10 ^ 8 cells*ml-1) containing BeeT to sugar water and diluted this by a factor of 100. The dilution is performed to avoid rejection of sugar water by bees, as it would be too contaminated to consume.
We based the hourly uptake rate of sugar water on a paper by Avni et al.
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, but it is possible that this is not the maximal uptake rate of sugar water. In the measured period all of the sugar water was taken up by the colony, meaning a higher theoretical uptake rate.
Bee bread
We assume that the amount of Lactobacillus cells in bee bread is roughly equal to the number of CFU*ml-1 in yoghurt
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Artificial bee breads can be made using yoghurt, and are readily accepted by bees
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. Additionally, we assume that the removal rate of artificial bee bread is equal to 22.7 g*day-1
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Based on Avni et al. we know that the uptake rate depends on the manner in which bee bread is applied
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We chose to base the uptake rate of bee bread on Brodschneider et al., since their experimental setup is similar to Avni et al. 4
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Key results
The functionality of the BeeT module is primarily based on literature research, and as such requires a relatively low amount of parametrization. The main unknown quality is how BeeT will behave, namely degradation and its effectiveness at combating Varroa mites nearby larvae. We are interested in how BeeT can best be applied given certain assumptions [hyperlink previous section]. As such we are interested in the best period to apply BeeT, either before winter or during spring, so we can give recommendations to beekeepers. We also examine the difference in effectiveness between BeeT in sugar water and in bee bread for both periods. This can inform future work on whether it is beneficial to adapt BeeT for functionality in bee bread. There are three additional parameters related to BeeT that can be varied, and upon which effectiveness relies. These are: degradation of BeeT in the hive, outside the hive, and the effect of BeeT on Varroa mite mortality. Each is varied across a range of values. Additionally, for every combination we have five replicates to reduce the variance in our results. We divided the analyses into four treatments, each with the same three parameter ranges and five replicates per set of parameters. This can be seen in Table 1.
Period | Treatment | Range |
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1st April - 15th June | Sugar water | Varroa mite mortality, degradation in-hive and degradation outside-hive |
Bee bread | Varroa mite mortality, degradation in-hive and degradation outside-hive | |
1st September - 15 November | Sugar Water | Varroa mite mortality, degradation in-hive and degradation outside-hive |
Bee bread | Varroa Mite Mortality, degradation in-hive and degradation outside-hive |