Team:INSA Toulouse/contenu/project/modelling

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  <h1 class="title1">Modelling</h1>
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<h1 class="title1">Modelling</h1>
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The full adder was tailored taking into account the diffusion of the carry from the bit n to the bit n+1. Evidently, the molecule should reach the n+1 colony prior the calculation step! Therefore, we have modeled the diffusion of AHL through the agar plate. The model would then help us determine the spacing between the different <i>E. calculus</i> colonies and the time necessary between two bits counting.  
+
<p class="texte">The full adder was tailored taking into account the diffusion of the carry from the bit n to the bit n+1. Evidently, the molecule should reach the n+1 colony prior the calculation step! Therefore, we have modeled the diffusion of AHL through the agar plate. The model would then help us determine the spacing between the different <i>E. calculus</i> colonies and the time necessary between two bits counting.  
 +
<br>For the modelling, we used a strain of Chromobacterium violaceum deleted in the gene producing AHL. This strain can then only react to the external presence of AHL, coloring nicely with violacein, a violet pigment.</p>
<h2 class="title2"><i>N</i>-acetyl Homoserine lactone diffusion in agar medium</h2>
<h2 class="title2"><i>N</i>-acetyl Homoserine lactone diffusion in agar medium</h2>
 +
<p class="texte"><i>N</i>-acyl Homoserine Lactone (AHL), 3-oxohexanoyl-homoserine lactone was chosen as the biological messenger in our system.
 +
<!--/* Different models can be devised to implement the expression and diffusion of the AHL. */-->
 +
Let's imagine a simple system. A petri dish containing colonies equidistant from each other. The lights provide the information for the addition to perform, and the expression and diffusion of AHL from one colony to another allows the carry propagation.<br><br>
 +
This system seems quite simple but nevertheless raises a certain number of questions:
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  <p class="texte"><i>N</i>-acyl Homoserine Lactone (AHL), 3-oxohexanoyl-homoserine lactone was chosen as the biological messenger in our system.<br><br>
 
-
  </div>
 
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/* Different models can be devised to implement the expression and diffusion of the AHL. */<br><br>
 
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The system of Figure 1 operates as follows:<br>
 
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A petri dish containing colonies equidistant from each other. The lights provide the information for the addition to perform, and the expression & diffusion of AHL from one colony to another allows the carry propagation.<br><br>
 
-
This system seems quite simple but nevertheless raises a certain number of problems:
 
-
</p>
 
    
    
<div class="list">
<div class="list">
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<ol><li>Does a colony produce enough AHL to induce diffusion of the message?
+
<ol><li>Can a colony produce enough AHL to induce a response on the n+1 colony?
</li><li>Do the colonies have to be inoculated all at once or progressively during the calculation step?
</li><li>Do the colonies have to be inoculated all at once or progressively during the calculation step?
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</li><li>What is the ideal distance between the colonies? How can we avoid excessive AHL diffusion , for example from a colony n to colony n+2 rather than a colony n+1?
+
</li><li>What is the ideal distance between the colonies? How can we avoid excessive AHL diffusion that would reach the colony n+1 but also n+2, n+3 etc.</p>
</li>
</li>
</ol>
</ol>
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<h3 class="title3">Production of AHL</h3>
<h3 class="title3">Production of AHL</h3>
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   <p class="texte">To overcome the problem of the amount of AHL required for a rapid diffusion of the messenger, we can well imagine a system in which liquid precultures may be deposited. So we get a higher cell density and a greater production of AHL.
+
   <p class="texte">To overcome the problem of the amount of AHL required for a rapid diffusion of the messenger, we also imagined a system in which liquid precultures may be deposited. A higher cell density would be obtained as well as a greater production of AHL.
</p>
</p>
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<center><p class="textecaption"><i>Figure 2: Bacterial full adder system in wells.</i></p></center>
<center><p class="textecaption"><i>Figure 2: Bacterial full adder system in wells.</i></p></center>
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-
 
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<h3 class="title3">Inoculation of cultures</h3>
<h3 class="title3">Inoculation of cultures</h3>
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   <p class="texte">A gradual inoculation of wells during the addition process allows, first to avoid the direct interference between the wells. Secondly with this method we avoid also the problem of death cell (a death wouldn't be able to answer to the AHL messenger).
+
   <p class="texte">A gradual inoculation of wells during the addition process avoids the direct interference between the wells.
 +
  Furthermore, progressive inoculation would lower the problem of cells dying on the plate that could not respond anymore to the AHL messenger.  
</p>
</p>
 +
<h3 class="title3">The ideal distance between wells</h3>
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<h3 class="title3">The ideal distance between well</h3>
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   <p class="texte">In order to find the ideal distance between two colonies, we searched a model that would calculate how does AHL diffuse into the medium and how long does the diffusion process take place to pass from one colony to another.
-
 
+
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   <p class="texte">In order to find the ideal distance between two colonies we have searched a model which allow us to know: how does AHL diffuse into the medium and how long does the diffusion take to pass from one colony to another.
+
</p>
</p>
-
 
+
 
-
<h2 class="title2">Modelling steps</h2>
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-
 
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<h3 class="title3">Diffusion reminder</h3>
<h3 class="title3">Diffusion reminder</h3>
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<img src="https://static.igem.org/mediawiki/2013/2/26/Carry1_-_340px.png" class="imgcontentleft"/>
 
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<img src="https://static.igem.org/mediawiki/2013/b/b2/Carry2_-_340px.png" class="imgcontentright"/>
 
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<center><img style="width:400px" src="https://static.igem.org/mediawiki/2013/e/e3/Carry3.png" class="imgcontent"/></center>
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<img src="https://static.igem.org/mediawiki/2013/2/26/Carry1_-_340px.png" class="imgcontent"/></center>
<div class="clear"></div>
<div class="clear"></div>
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<img style="width:340px" src="https://static.igem.org/mediawiki/2013/b/b5/Carry4.png" class="imgcontentleft"/>
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<p class="texte">The graph above represents cylinder containing bacterias. Bacterias can produce AHL to send a message to another well. Here we can imagine that AHL diffuse into the medium. In order to introduce the theory of diffusion we can realize a simple model, with stationary state conditions.
 +
</p>
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<img style="width:340px" src="https://static.igem.org/mediawiki/2013/8/85/Carry5.png" class="imgcontentrightcaption"/>
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<img src="https://static.igem.org/mediawiki/2013/b/b2/Carry2_-_340px.png" class="imgcontent"/></center>
 +
<div class="clear"></div>
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<center><p class="textecaptionright"><i>Figure 3: Evolution of AHL concentration versus distance.</i></p></center>
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<p class="texte">In fact, we can establish a mass balance on AHL over a thickness of delta(r) :
 +
</p>
 +
<center><img style="width:400px" src="https://static.igem.org/mediawiki/2013/e/e3/Carry3.png" class="imgcontent"/></center>
<div class="clear"></div>
<div class="clear"></div>
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  <p class="texte">Figure 3 shows that the largest amount of AHL is between 2.5 and 20 mm. This information is important but we need to develop a model based on time.
 
-
</p>
 
-
 
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  <p class="texte"><span class="spantitle2">Two dimension model: </span></br>
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<p class="texte">Here we can introduce the Fick’s law for diffusion.
-
We realized many experiences in order to measure how AHL diffuse into agar medium. We used a particular bacteria, Chromobacterium violaceum, which is capable to detect presence of AHl by producing a purple pigment, the violacein.<br><br>
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Figure 4 shows petri dishes containing eight colonies of bacteria placed at 5, 10, 15, 20, 25, 30, 35 and 40 mm from the center of the box. With this experience we can track the diffusion of the AHL. Figure 5 represent the evolution of AHL diffusion versus time.
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</p>
</p>
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<center><img style="width:700px" src="https://static.igem.org/mediawiki/2013/9/90/Tri_boite.png" class="imgcontentcaption"/></center>
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<img style="width:340px" src="https://static.igem.org/mediawiki/2013/e/ea/Integration.png" class="imgcontentleft"/>
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<center><p class="textecaption"><i>Figure 4: Photographs at 25h of petri dishes containing each 8 Chromobacterium violaceum colonies from 5 mm to 40 mm.</i></p></center>
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<img style="width:340px" src="https://static.igem.org/mediawiki/2013/7/73/Concentration_profile.PNG" class="imgcontentrightcaption"/>
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<img style="width:500px" src="https://static.igem.org/mediawiki/2013/6/6b/Carry7.png" class="imgcontentcaption"/>
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<center><p class="textecaptionright"><i>Figure 3: Evolution of AHL concentration versus distance.</i></p></center>
-
<p class="textecaption"><i>Figure 5: Evolution of AHL diffusion into petri dish.</i></p>
+
<div class="clear"></div>
 +
  <p class="texte">With this equation we can establish the concentration profile (figure 3) of the diffusion of AHL. This equation is only valid in our case of well geometry. However, this model does not depend on time, that’s why we must try to develop a more complex system in order to model the diffusion of AHL into LBagar medium with time.
 +
</p>
-
 
+
<h1 class="title1">What modelling has tought us.</h1>
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  <p class="texte">We can see that the ideal distance between two wells is probably between 15 and 25 mm depending on the amount of AHL produced by the bacteria. Indeed, the AHL diffuses rapidly into the medium during the first 5 hours, then the concentration gradient decreases and the diffusion is slower. However, if the bacteria produce too AHL, the diffusion to colony n+1 will be in the first 5 hours but affect the colony n+2 after 24h. In the ideal case would have bacteria produce about 1 nmol per well of AHL.
+
<p class="texte">
 +
If you are not afraid of maths, you can go to the <a href="https://2013.igem.org/Team:INSA_Toulouse/contenu/lab_practice/results/carry" class="texte" style="display : list-item; list-style-image : url(https://static.igem.org/mediawiki/2013/8/84/Insa-toulouse2013-listpuce1.png);"> Modelling results  </a>
 +
Otherwise here is a brief summary of our main findings:
 +
<br> - the best model for diffusion is a system where the supply of AHL is not infinite and basically that will be the case in <i>E. calculus</i>. Two elements supports this theory : i) production of AHL is linked to growing. When cells growing will stop, production of AHL will stop too; ii )production of AHL is also linked to presence of the general inducer in the medium (which is not permanent)
 +
<br> - in order to avoid that AHL goes to n+1 and n+2 (and many other) colonies, AHL must be taken up and destroyed by the n+1 colony. That should also be the case as the n+1 colony will pump up AHL and destroy it. <br>
 +
So basically, the design would be OK provided that we could have extracted the right parameters for AHL diffusion starting from an <i>E. calculus</i> strain instead of pure AHL.  
 +
<br>Now that you have had the conclusions, you can go to the modelling results, there are very nice animated pictures at the end!!!
</p>
</p>
-
 
-
<img style="width:500px" src="https://static.igem.org/mediawiki/2013/a/a3/Carry8.png" class="imgcontentcaption"/>
 
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<p class="textecaption"><i>Figure 6: Radar graph of AHL diffusion into petri dish.</i></p>
 
-
 
-
 
</div>
</div>

Latest revision as of 03:16, 5 October 2013

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Modelling

The full adder was tailored taking into account the diffusion of the carry from the bit n to the bit n+1. Evidently, the molecule should reach the n+1 colony prior the calculation step! Therefore, we have modeled the diffusion of AHL through the agar plate. The model would then help us determine the spacing between the different E. calculus colonies and the time necessary between two bits counting.
For the modelling, we used a strain of Chromobacterium violaceum deleted in the gene producing AHL. This strain can then only react to the external presence of AHL, coloring nicely with violacein, a violet pigment.

N-acetyl Homoserine lactone diffusion in agar medium

N-acyl Homoserine Lactone (AHL), 3-oxohexanoyl-homoserine lactone was chosen as the biological messenger in our system. Let's imagine a simple system. A petri dish containing colonies equidistant from each other. The lights provide the information for the addition to perform, and the expression and diffusion of AHL from one colony to another allows the carry propagation.

This system seems quite simple but nevertheless raises a certain number of questions:

  1. Can a colony produce enough AHL to induce a response on the n+1 colony?
  2. Do the colonies have to be inoculated all at once or progressively during the calculation step?
  3. What is the ideal distance between the colonies? How can we avoid excessive AHL diffusion that would reach the colony n+1 but also n+2, n+3 etc.

Figure 1: Diffusion of AHL through colonies.

Production of AHL

To overcome the problem of the amount of AHL required for a rapid diffusion of the messenger, we also imagined a system in which liquid precultures may be deposited. A higher cell density would be obtained as well as a greater production of AHL.

Figure 2: Bacterial full adder system in wells.

Inoculation of cultures

A gradual inoculation of wells during the addition process avoids the direct interference between the wells. Furthermore, progressive inoculation would lower the problem of cells dying on the plate that could not respond anymore to the AHL messenger.

The ideal distance between wells

In order to find the ideal distance between two colonies, we searched a model that would calculate how does AHL diffuse into the medium and how long does the diffusion process take place to pass from one colony to another.

Diffusion reminder

The graph above represents cylinder containing bacterias. Bacterias can produce AHL to send a message to another well. Here we can imagine that AHL diffuse into the medium. In order to introduce the theory of diffusion we can realize a simple model, with stationary state conditions.

In fact, we can establish a mass balance on AHL over a thickness of delta(r) :

Here we can introduce the Fick’s law for diffusion.

Figure 3: Evolution of AHL concentration versus distance.

With this equation we can establish the concentration profile (figure 3) of the diffusion of AHL. This equation is only valid in our case of well geometry. However, this model does not depend on time, that’s why we must try to develop a more complex system in order to model the diffusion of AHL into LBagar medium with time.

What modelling has tought us.

If you are not afraid of maths, you can go to the Modelling results Otherwise here is a brief summary of our main findings:
- the best model for diffusion is a system where the supply of AHL is not infinite and basically that will be the case in E. calculus. Two elements supports this theory : i) production of AHL is linked to growing. When cells growing will stop, production of AHL will stop too; ii )production of AHL is also linked to presence of the general inducer in the medium (which is not permanent)
- in order to avoid that AHL goes to n+1 and n+2 (and many other) colonies, AHL must be taken up and destroyed by the n+1 colony. That should also be the case as the n+1 colony will pump up AHL and destroy it.
So basically, the design would be OK provided that we could have extracted the right parameters for AHL diffusion starting from an E. calculus strain instead of pure AHL.
Now that you have had the conclusions, you can go to the modelling results, there are very nice animated pictures at the end!!!