Difference between revisions of "Team:KU Leuven/Modeling/Toulouse"

 
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     <h2> Toulouse FBA Model </h2>
 
     <h2> Toulouse FBA Model </h2>
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  <p>We cooperated with Toulouse on the modeling. Here we describe the Flux-Balance-Analysis the Toulouse team generously
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  <p>We cooperated with Toulouse on the modeling. Here we describe the Flux Balance Analysis the Toulouse team generously
  performed for us. <br/>
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  performed for us. <br/> <br>
  Flux balance analysis is a widely used approach for studying the flow trough metabolic networks. In our
+
  Flux Balance Analysis is a widely used approach for studying the flow through metabolic networks. In our
  case we are interested in the Leucine and AHL production rates of the type A cells. To obtain these values
+
  case we are interested in the leucine and AHL production rates of the type A cells and their effect on the growth rate of the bacteria. This is very important because if cell A has a big metabolic burden and thus, a very low growth rate, cell B would overgrow it and our pattern formation system would not work. Therefore, it is very important to keep the growth rates of cells A and cells B as close as possible to each other. To check the effect of our system on the growth rate iGEM Toulouse ran a FB analysis. </p>
toulouse ran a FB analysis.  
+
   
  When a FBA is set up. The metabolic network of the organism in question is represented as a matrix $\mathbf{S}$  
+
<p> When a FBA is set up. The metabolic network of the organism in question is represented as a matrix $\mathbf{S}$  
  of size $m \times n$ is filled with the stoichiometric constants of each reaction. Each of the $m$ matrix
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  of size $m \times n$ . This matrix is filled with the stoichiometric constants of each reaction. Each of the $m$ matrix
 
  rows represents a unique compound. Similarly each of the n columns represents one unique reaction. Next  
 
  rows represents a unique compound. Similarly each of the n columns represents one unique reaction. Next  
  a vector $\mathbf{v}$ of length $n$ is defined which contains the flux trough each reaction. Finally the  
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  a vector $\mathbf{v}$ of length $n$ is defined which contains the flux through each reaction. Finally, the  
 
  vector $\mathbf{x}$ is defined to contain the concentrations of each metabolite. The steady state solution
 
  vector $\mathbf{x}$ is defined to contain the concentrations of each metabolite. The steady state solution
  in the insteresting one therefore:
+
  is the insteresting one, therefore:
 
  $$ \frac{dx}{dt} = \mathbf{Sv} = 0 $$
 
  $$ \frac{dx}{dt} = \mathbf{Sv} = 0 $$
  Which is the nullspace of $\mathbf{S}$. In this set of solutions a maximal or minimal value can be identified
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  Which is the nullspace of $\mathbf{S}$. In this set of solutions, a maximal or minimal value can be identified
 
  using numerical optimization. In order to run the optimization algorithm a cost function has to be defined.
 
  using numerical optimization. In order to run the optimization algorithm a cost function has to be defined.
 
  $$ f(x) = \mathbf{c}^{T}\mathbf{v} $$
 
  $$ f(x) = \mathbf{c}^{T}\mathbf{v} $$
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  From an optimization perspective the equation $\mathbf{Sv} = 0$ represents constraints, which guide the numerical
 
  From an optimization perspective the equation $\mathbf{Sv} = 0$ represents constraints, which guide the numerical
 
  solver to the right solution. <br/>
 
  solver to the right solution. <br/>
  In our case the $\mathbf{S}$ matrix comes from the in silico E. Coli model K12MG1665. The model is contained in an XML file.
+
  In our case the $\mathbf{S}$ matrix comes from the in silico <i>E. coli</i> model K-12 MG1665. The model is contained in an XML file.
 
  We told the Toulouse modelers our two reaction of interest:
 
  We told the Toulouse modelers our two reaction of interest:
 
  $$ \text{glutamate} + \text{aKIC} \rightarrow \text{aKG} + \text{Leucine} $$
 
  $$ \text{glutamate} + \text{aKIC} \rightarrow \text{aKG} + \text{Leucine} $$
  This reaction is interesting as Leucine serves as repellent in our scheme. The second reaction of interest is:
+
  This reaction is interesting as leucine serves as repellent in our scheme. The second reaction of interest is:
 
  $$ \text{acylACP} + \text{SAM} \rightarrow \text{ACP} + \text{MTA} + \text{AHL} $$
 
  $$ \text{acylACP} + \text{SAM} \rightarrow \text{ACP} + \text{MTA} + \text{AHL} $$
 +
This reaction is important because AHL serves as the key to the motility system of cell B. Without AHL, cell B is unable to move away from cell A and form patterns.
  
 
  Given this information the Toulouse team was able to locate the reactions of interest in the XML model file,
 
  Given this information the Toulouse team was able to locate the reactions of interest in the XML model file,
  and simulate the cell metabolism. The results are: <br/>
+
  and simulate the cell metabolism. The results are shown in figures 1 and 2. All of the graphs shown above are in $mmol \cdot gDW^{-1} \cdot h^{-1}$. In figure 1 the effect of AHL production on growthrate was plotted and in figure 2 the effect of leucine production. We can also deduce the maximum possible flux of AHL and leucine. This is the flux that corresponds to a growth rate of 0. In our case these maximum values are:</p> <br>
 +
      <p> For AHL: $ 150.71391 mmol \cdot gDW^{-1} \cdot h^{-1}$ <br>
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      <p> For leucine: $ 528.17774 mmol \cdot gDW^{-1} \cdot h^{-1}$ </p><br/>
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                     data-lightbox="AHL and Biomass production with maximal Leucine production rate."
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                     data-lightbox="AHL and Biomass production."
                     data-title="AHL and Biomass production with maximal Leucine production rate."
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                     data-title="Leucine and Biomass production."
                     href="https://static.igem.org/mediawiki/2015/4/47/KUL_Toulouse_AHL_effect_max_Leu.png"><img alt="AHL and Biomass production." class="example-image"
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                     href="https://static.igem.org/mediawiki/2015/3/30/KUL_Toulouse_Leucine_effect.png"><img alt="AHL and Biomass production." class="example-image"
 
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                     src="https://static.igem.org/mediawiki/2015/4/47/KUL_Toulouse_AHL_effect_max_Leu.png"
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                     src="https://static.igem.org/mediawiki/2015/3/30/KUL_Toulouse_Leucine_effect.png"
 
                     width="50%"></a>
 
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                 <h4>
 
                 <h4>
                   <div id=figure2>Figure 2</div>
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                   <div id=figure3>Figure 2</div>
                     AHL and Biomass production with maximal Leucine production rate.. Click to enlarge
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                     Leucine and Biomass production. Click to enlarge
 
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<p>Yet, we are interested in the combined effect of AHL and leucine production on the growth rate. This is why Toulouse also modeled the effect of one biomolecule, but with the constraint that the other biomolecule is produced at maximum rate. The results of these simulations are shown in figures 3 and 4. We see that the production values are way smaller in this simulation. This is logical, since more resources are being used. It is impossible to reach the maximum production rates, while producing two biomolecules. </p>
 
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                     data-lightbox="AHL and Biomass production."
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                     data-lightbox="AHL and Biomass production with maximal Leucine production rate."
                     data-title="Leucine and Biomass production."
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                     data-title="AHL and Biomass production with maximal Leucine production rate."
                     href="https://static.igem.org/mediawiki/2015/3/30/KUL_Toulouse_Leucine_effect.png"><img alt="AHL and Biomass production." class="example-image"
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                     href="https://static.igem.org/mediawiki/2015/4/47/KUL_Toulouse_AHL_effect_max_Leu.png"><img alt="AHL and Biomass production." class="example-image"
 
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                     src="https://static.igem.org/mediawiki/2015/3/30/KUL_Toulouse_Leucine_effect.png"
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                     src="https://static.igem.org/mediawiki/2015/4/47/KUL_Toulouse_AHL_effect_max_Leu.png"
 
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                 <h4>
 
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                   <div id=figure3>Figure 3</div>
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                   <div id=figure2>Figure 3</div>
                     Leucine and Biomass production. Click to enlarge
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                     AHL and Biomass production with maximal Leucine production rate. Click to enlarge
 
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                   <div id=figure4>Figure 4</div>
 
                   <div id=figure4>Figure 4</div>
                     Leucine and Biomass production at AHL maximum. Click to enlarge
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                     Leucine and Biomass production with maximal production rate. Click to enlarge
 
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      <p>In generally it follows from the analysis that the more AHL or leucine is produced the smaller the
 +
      biomass output becomes. It also shows that cell A can not operate at the maximum production rate, because the growth rate would then be so slow that cell B would overgrow it. This is something to keep in mind when we choose our promoters for the system. If our promoters are too strong, the growth rate of cell A will be too low and cell B will be able to overgrow cell A.
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        <a href="https://2015.igem.org/Team:KU_Leuven/Modeling" >
    <h2>Colony level</h2>
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    <img src="https://static.igem.org/mediawiki/2015/c/cb/KUL_Wiki_Button_-_Back.png" width="100%" >  
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    <h2>Hybrid model</h2>
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                                <a href="https://2015.igem.org/Team:KU_Leuven/Modeling/Top">
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                                    <h2>Colony level</h2>
            <div class="more"><p></p>
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                                    <p>
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                                        Our colony layer model relies on a Keller-Segel type system of differential
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                                        equations. These equations are simulated using finite differences.
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    <h2>Internal model</h2>
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                                    <h2>Hybrid</h2>
        <p>
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                                    <p> Our hybrid model merges both colony and internal level to define the cell-cell interactions of our pattern forming cells. </p>
          Coming soon <br/>
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    <b>Colony level</b>
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                                    <h2>Internal</h2>
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                                    <p>Our internal model aims to simulate the internal dynamics of every cell with a system of ordinary differential equations.</p>
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        <p>
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          Our colony layer model relies on a Keller-Segel type system of differential equations. These equations are simulated    using finite differences. <br/>
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    </a>
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  </div>
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<a href="https://2015.igem.org/Team:KU_Leuven/Modeling">
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    <div id="back">
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<img src="https://static.igem.org/mediawiki/2015/7/73/KUL_Wiki_Button_-_Read_more.png" 
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<div class="subimgrowm">
 
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+
                        <div class="subimgm">
    <b>Hybrid model</b>
+
                            <a href="https://2015.igem.org/Team:KU_Leuven/Modeling/Top">
<img src="https://static.igem.org/mediawiki/2015/9/98/HybridCover.png" width="100%">
+
                                <b>Colony</b>
</div>
+
                                <img
 +
                                    src="https://static.igem.org/mediawiki/2015/6/6a/KU_Leuven_Wiki_Button_-_Colony_level2.png"
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                                    width="100%"></a>
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+
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        <p>
+
                                <p>
          Coming soon <br/>
+
                                    Our colony layer model relies on a Keller-Segel type system of differential
        </p>
+
                                    equations. These equations are simulated using finite differences.
    </a>  
+
                                    <br/>
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                                </p>
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                            <a href="https://2015.igem.org/Team:KU_Leuven/Modeling/Hybrid">
 +
                            <b>Hybrid</b>
 +
                            <img
 +
                                src="https://static.igem.org/mediawiki/2015/0/02/KU_Leuven_Wiki_Button_-_Hybrid_model2.png"
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                                width="100%"></a>
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                        <div class="subtextm">
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                            <a href="https://2015.igem.org/Team:KU_Leuven/Modeling/Hybrid">
 +
                                <p> Our hybrid model merges both colony and internal level to define the cell-cell interactions of our pattern forming cells.
 +
                                </p>
 +
                            </a>
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                        </div>
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                            <a href="https://2015.igem.org/Team:KU_Leuven/Modeling/Internal">
 +
                            <b>Internal</b>
 +
                            <img
 +
                                src="https://static.igem.org/mediawiki/2015/4/47/KU_Leuven_Wiki_Button_-_Internal_model2.png"
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                                width="100%"></a>
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                        </div>
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                                <p>
 +
Our internal model aims to simulate the internal dynamics of every cell with a system of ordinary differential equations.
 +
                                </p>
 +
                            </a>
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<a href="https://2015.igem.org/Team:KU_Leuven/Modeling">
  <img src="https://static.igem.org/mediawiki/2015/d/dd/InternalCover.png" width="100%">
+
<b>Back</b>
 +
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</a>
 
</div>
 
</div>
  
<div class="whitespace">
+
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    <a href = "">
+
<a href="https://2015.igem.org/Team:KU_Leuven/Modeling">
        <p>
+
<p>Go back to the Modeling page.<br/></p>
          Coming soon <br/>
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<p style="font-size:1.3em; text-align: center">
 
<p style="font-size:1.3em; text-align: center">
 
Address: Celestijnenlaan 200G room 00.08 - 3001 Heverlee<br>
 
Address: Celestijnenlaan 200G room 00.08 - 3001 Heverlee<br>
Telephone : +32(0)16 32 73 19<br>
+
Telephone: +32(0)16 32 73 19<br>
Mail: igem@chem.kuleuven.be<br>   
+
Email: igem@chem.kuleuven.be<br>   
 
</p>
 
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       <a><img src="https://static.igem.org/mediawiki/2015/1/15/KUL_Ko-Lo_Instruments_logo_transparant.png" alt="Ko-Lo Instruments" width="95%"></a>
 
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       <a href="https://www.bioke.com/"><img src="https://static.igem.org/mediawiki/2015/e/e1/KUL_Biok%C3%A9_logo_transparant.png" alt="Bioké" width="95%"></a>
 
   </div>
 
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                <img src="https://static.igem.org/mediawiki/2015/e/e6/KU_Leuven_LOGO_LGC.png" alt="LGC Genomics" width="80%">
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      <a href="https://www.novolab.be/"><img src="https://static.igem.org/mediawiki/2015/4/4c/KU_Leuven_Novalab.png" alt="Novolab" height="95%"></a>
 
     </div>
 
     </div>
 
   </div>   
 
   </div>   

Latest revision as of 09:56, 20 October 2015

Toulouse FBA Model

We cooperated with Toulouse on the modeling. Here we describe the Flux Balance Analysis the Toulouse team generously performed for us.

Flux Balance Analysis is a widely used approach for studying the flow through metabolic networks. In our case we are interested in the leucine and AHL production rates of the type A cells and their effect on the growth rate of the bacteria. This is very important because if cell A has a big metabolic burden and thus, a very low growth rate, cell B would overgrow it and our pattern formation system would not work. Therefore, it is very important to keep the growth rates of cells A and cells B as close as possible to each other. To check the effect of our system on the growth rate iGEM Toulouse ran a FB analysis.

When a FBA is set up. The metabolic network of the organism in question is represented as a matrix $\mathbf{S}$ of size $m \times n$ . This matrix is filled with the stoichiometric constants of each reaction. Each of the $m$ matrix rows represents a unique compound. Similarly each of the n columns represents one unique reaction. Next a vector $\mathbf{v}$ of length $n$ is defined which contains the flux through each reaction. Finally, the vector $\mathbf{x}$ is defined to contain the concentrations of each metabolite. The steady state solution is the insteresting one, therefore: $$ \frac{dx}{dt} = \mathbf{Sv} = 0 $$ Which is the nullspace of $\mathbf{S}$. In this set of solutions, a maximal or minimal value can be identified using numerical optimization. In order to run the optimization algorithm a cost function has to be defined. $$ f(x) = \mathbf{c}^{T}\mathbf{v} $$ The equation above shows such a cost function. Here the vector $\mathbf{c}$ represents a weight vector. In practice it is used to choose the metabolite of interested by setting the corresponding entry to one and all others to zero. From an optimization perspective the equation $\mathbf{Sv} = 0$ represents constraints, which guide the numerical solver to the right solution.
In our case the $\mathbf{S}$ matrix comes from the in silico E. coli model K-12 MG1665. The model is contained in an XML file. We told the Toulouse modelers our two reaction of interest: $$ \text{glutamate} + \text{aKIC} \rightarrow \text{aKG} + \text{Leucine} $$ This reaction is interesting as leucine serves as repellent in our scheme. The second reaction of interest is: $$ \text{acylACP} + \text{SAM} \rightarrow \text{ACP} + \text{MTA} + \text{AHL} $$ This reaction is important because AHL serves as the key to the motility system of cell B. Without AHL, cell B is unable to move away from cell A and form patterns. Given this information the Toulouse team was able to locate the reactions of interest in the XML model file, and simulate the cell metabolism. The results are shown in figures 1 and 2. All of the graphs shown above are in $mmol \cdot gDW^{-1} \cdot h^{-1}$. In figure 1 the effect of AHL production on growthrate was plotted and in figure 2 the effect of leucine production. We can also deduce the maximum possible flux of AHL and leucine. This is the flux that corresponds to a growth rate of 0. In our case these maximum values are:


For AHL: $ 150.71391 mmol \cdot gDW^{-1} \cdot h^{-1}$

For leucine: $ 528.17774 mmol \cdot gDW^{-1} \cdot h^{-1}$



AHL and Biomass production.

Figure 1
AHL and Biomass production. Click to enlarge


AHL and Biomass production.

Figure 2
Leucine and Biomass production. Click to enlarge

Yet, we are interested in the combined effect of AHL and leucine production on the growth rate. This is why Toulouse also modeled the effect of one biomolecule, but with the constraint that the other biomolecule is produced at maximum rate. The results of these simulations are shown in figures 3 and 4. We see that the production values are way smaller in this simulation. This is logical, since more resources are being used. It is impossible to reach the maximum production rates, while producing two biomolecules.

AHL and Biomass production.

Figure 3
AHL and Biomass production with maximal Leucine production rate. Click to enlarge


AHL and Biomass production.

Figure 4
Leucine and Biomass production with maximal production rate. Click to enlarge

In generally it follows from the analysis that the more AHL or leucine is produced the smaller the biomass output becomes. It also shows that cell A can not operate at the maximum production rate, because the growth rate would then be so slow that cell B would overgrow it. This is something to keep in mind when we choose our promoters for the system. If our promoters are too strong, the growth rate of cell A will be too low and cell B will be able to overgrow cell A.



Contact

Address: Celestijnenlaan 200G room 00.08 - 3001 Heverlee
Telephone: +32(0)16 32 73 19
Email: igem@chem.kuleuven.be