Team:Aalto-Helsinki/Modeling

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<h1>Modeling</h1>
<h1>Modeling</h1>
<p class="bigsplashtext">
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To test our theory and how well our test results fit, we did some modeling, too. $\int_0^\infty{xdx} = g0tH4X3D$
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Before bringing all the parts together in the lab, we built our switch in the mathematical world.
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</p>
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             <a href="#Math">
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             <a href="#Intro">
                 Scroll down to read more
                 Scroll down to read more
                 <img src="https://static.igem.org/mediawiki/2014/3/3e/Aalto_Helsinki_Nuoli.png" class="img-responsive center-block transp nuoli">
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<a href="#Math">Mathematical Model</a><br>
<a href="#Math">Mathematical Model</a><br>
         <a href="#Simulation">Simulation</a><br>
         <a href="#Simulation">Simulation</a><br>
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         <a href="#Accuracy">Accuracy</a><br>
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         <a href="#Discussion">Discussion</a><br>
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<!-- "The Mathematical Association of America (MAA) continues to support MathJax as a MathJax Supporter.
 
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The MAA is the largest professional society focused on mathematics accessible at the collegiate level. As an early adopter of the web, the MAA has led the way communicating mathematics online including resources such as MathDL, born-digital ebooks and journals. The MAA’s open-source homework system WeBWorK is used at over 500 institutions worldwide."
 
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Dear Lassi (programmer-in-charge, Aalto-Helsinki iGEM 2014),
 
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Based on the previous quote by the MathJax community, I hereby declare that, even if the scripts for displaying our math are located on another server, it doesn't matter. Should the support for MathJax ever cease to exist, the first victim would be the world wide mathematical community, not us.
 
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This is a safe method. We are using LaTeX. Period!
 
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Yours,
 
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Otto Lamminpää
 
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         <a id="Math-submenu" href="#Math">Mathematical Model</a>
         <a id="Math-submenu" href="#Math">Mathematical Model</a>
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<div class="link" id="Intro"></div>
<div class="link" id="Intro"></div>
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<h2>Introduction</h2>
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<h2 class="kakspaddingbottom">Introduction</h2>
<p>
<p>
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To get an idea of how our gene circuit would work on an ideal situation, we explored the structure and dynamics of our system by creating a mathematical model of the reaction kinetics and a real-time simulation. Wit the mathematical model, we started with no information ready whatsoever and derived differential equations to demonstrate how the use of blue light and the changes in phosphorylated YF1 and FixJ concentrations would control the production of our three target proteins. We labeled them simply A, B, and C, because the system is intended to be used with any user defined three genes coding different proteins.
+
To get an idea of how our gene circuit would work in an ideal situation, we explored the structure and dynamics of our system by creating a mathematical model of the reaction kinetics and a simulation that can be controlled in real time. We started working with the mathematical model without any detailed information about the system. We derived the differential equations to demonstrate how blue light and the changes in phosphorylated $YF1$ and $FixJ$ concentrations would affect the production of our three target proteins. We labeled them simply $A$, $B$ and $C$, because the system is intended to be used with any three genes encoding the proteins of choice.
</p>
</p>
<p>
<p>
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Using our equations we constructed a simulation showing the effects of red and blue light on our system in real time. The user can control the input of both lights to see how they affect the production of proteins A, B and C. We experimented with different values for all constants and with trial-and-error iteration we arrived to a visualized simulation that can be used to demonstrate the intended funcion of our system. All in all, this is an idealization. Based on present and future measurement data, the parameters can be adjusted to better match the real world.
+
Using our equations we constructed a simulation showing the effects of red and blue light on our system in real time. The user can control the input of both lights to see how they affect the production of proteins $A$, $B$ and $C$. We experimented with different values for all constants and via trial-and-error iteration we arrived to a visualized simulation that can be used to demonstrate the intended function of our system. This is an idealization. Based on present and future measurement data, the parameters can be adjusted to better the dynamics of our system.
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<div class="link" id="Math"></div>
<div class="link" id="Math"></div>
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<h2>Mathematical model</h2>
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<h2>Mathematical Model</h2>
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<h3>Overview </h3>
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<h3 class="kakspaddingtop">Assumptions</h3>
<p>
<p>
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Here, we will discuss the dynamics and interactions of different proteins and promoters introduced in the research section. We have developed a simplified mathematical model describing our system.
+
We assumed that the species identified in our gene circuit are the only ones that affect the overall concentrations inside the bacteria. We further assumed that binding of $CI$ to $O_R$ operator site does not impact the overall $CI$ concentration and that the amount of $CI$ bound to the $O_R$ sites was proportional to $CI$ concentration. The model is also strictly deterministic and doesn’t take any noise into account. The phosphorylation, decay, binding and production of proteins are assumed to be linear functions of concentration. We further assumed that the phosphorylation of $FixJ$ by phosphorylated $YF1$ would not involve phosphate transfer between the reacting molecules.
</p>
</p>
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<h3>Simplifications</h3>
 
<p>
<p>
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We assumed that the species identified from our gene circuit are the only ones that affect the overall concentrations in our bacterial culture. The bonding of CI to OR sites is assumed to be insignificant compared to the overall concentration. The model is also strictly deterministic and doesn’t take into account any noise. The phosphorylation, decay, bonding and production of proteins are assumed to be linear functions of concentration. We further assumed that the phsophorylation of FixJ by phosphorylated YF1 would not involve phosphor
+
The first model was constructed before our lab work had even begun and it contains many harsh simplifications. Our aim was to get a general picture of how the system could work in ideal conditions and how stable it was.
</p>
</p>
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<p>
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<h3>Equations for Dynamics</h3>
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The first model that was constructed before our lab work had even begun involves many harsh simplifications. Our aim was to get a general picture of how the system could work in ideal conditions and how stable it was.
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</p>
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<h3>Equations for dynamics</h3>
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<p>
<p>
Based on the assumptions made before, we arrived at following differential equations to describe the idealized dynamics of our system:
Based on the assumptions made before, we arrived at following differential equations to describe the idealized dynamics of our system:
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Differential equations describing our system
 
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<p class="modellatex">
\begin{eqnarray*}
\begin{eqnarray*}
-
& & \frac{d[YF1]}{dt} = P_1Rbs_1 + DP_1[YF1]_{phos} - (Deg_{YF1}+I_B)[YF1] \\ \quad \\
+
& & \frac{d[YF1]}{dt} = P_1Rbs_{YF1} + DP_1[YF1]_{phos} - (Deg_{YF1}+I_B)[YF1] \\ \quad \\
& & \frac{d[YF1]_{phos}}{dt} = I_B[YF1] - (Deg_{\text{YF1}} + DP_1)[YF1]_{phos} \\
& & \frac{d[YF1]_{phos}}{dt} = I_B[YF1] - (Deg_{\text{YF1}} + DP_1)[YF1]_{phos} \\
\
\
-
& & \frac{d[FixJ]}{dt} = P_1Rbs_1 + DP_2[FixJ]_{phos} - (C_{phos}[YF1]_{phos} + Deg_{FixJ})[FixJ] \\
+
& & \frac{d[FixJ]}{dt} = P_1Rbs_{FixJ} + DP_2[FixJ]_{phos} - (C_{phos}[YF1]_{phos} + Deg_{FixJ})[FixJ] \\
\\
\\
& & \frac{d[FixJ]_{phos}}{dt} = C_{phos}[YF1]_{phos}[FixJ] - (DP_2[FixJ]_{phos} + Deg_{FixJ}[FixJ]) \\
& & \frac{d[FixJ]_{phos}}{dt} = C_{phos}[YF1]_{phos}[FixJ] - (DP_2[FixJ]_{phos} + Deg_{FixJ}[FixJ]) \\
\\
\\
-
& & \frac{d[CI]}{dt} = P_2Rbs_1 - Deg_{CI}[CI] \\
+
& & \frac{d[CI]}{dt} = P_2Rbs_{CI} - Deg_{CI}[CI] \\
\\
\\
-
& & \frac{d[TetR]}{dt} = (P_A + P_B)Rbs_2 - Deg_{TetR}[TetR]
+
& & \frac{d[TetR]}{dt} = P_ARbs_{TetR_A} + P_BRbs_{TetR_B} - Deg_{TetR}[TetR]
\end{eqnarray*}
\end{eqnarray*}
</p>
</p>
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<h3>Legend</h3>
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    <div class="row row-eq-height">
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    <ul>
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      <div class="center-block">
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<li><strong>$[YF1]$</strong> = concentration of $YF1$ protein</li>
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        <ul>
-
<li><strong>$[YF1]_{phos}$</strong> = concentration of phosphorylated $YF1$ protein</li>
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        <h4 class="nopaddingtop">Legend</h4>
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<li><strong>$[FixJ]$</strong> = concentration of $FixJ$ protein</li>
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<li><strong>$[YF1]$</strong> = concentration of $YF1$ protein</li>
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<li><strong>$[FixJ]_{phos}$</strong> = concentration of phosphorylated $FixJ$ protein</li>
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<li><strong>$[YF1]_{phos}$</strong> = concentration of phosphorylated $YF1$ protein</li>
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<li><strong>$[CI]$</strong> = concentration of $CI$ protein</li>
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<li><strong>$[FixJ]$</strong> = concentration of $FixJ$ protein</li>
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<li><strong>$[TetR]$</strong> = concentration of $TetR$ protein</li>
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<li><strong>$[FixJ]_{phos}$</strong> = concentration of phosphorylated $FixJ$ protein</li>
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<li><strong>$P_1$</strong> = relative strength of the first promoter in gene circuit</li>
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<li><strong>$[CI]$</strong> = concentration of $CI$ protein</li>
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<li><strong>$P_2$</strong> = relative strength of the $FixK_2$ promoter</li>
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<li><strong>$[TetR]$</strong> = concentration of $TetR$ protein</li>
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<li><strong>$P_A$</strong> = relative strength of the $P_R$ promoter, codes gene A</li>
+
<li><strong>$P_1$</strong> = relative strength of the first promoter in gene circuit</li>
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<li><strong>$P_B$</strong> = relative strength of the $P_{RM}$ promoter, codes gene B</li>
+
<li><strong>$P_2$</strong> = relative strength of the $FixK_2$ promoter</li>
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<li><strong>$Rbs$</strong> = relative strengths of ribosome binding sites</li>
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<li><strong>$P_A$</strong> = relative strength of the $P_R$ promoter, codes gene $A$</li>
-
<li><strong>$Deg$</strong> = degradation coefficient</li>
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<li><strong>$P_B$</strong> = relative strength of the $P_{RM}$ promoter, codes gene $B$</li>
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<li><strong>$C_{phos}$</strong> = phosphorylation coefficient</li>
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<li><strong>$P_C$</strong> = relative strength of the promoter coding gene $C$
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<li><strong>$DP$</strong> = de-phosphorylation coefficient</li>
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<li><strong>$Rbs$</strong> = relative strengths of ribosome binding sites</li>
-
    </ul>
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<li><strong>$Deg$</strong> = degradation coefficient</li>
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<li><strong>$C_{phos}$</strong> = phosphorylation coefficient</li>
 +
<li><strong>$DP$</strong> = de-phosphorylation coefficient</li>
 +
    </ul>
 +
      </div>
 +
    </div>
 +
    <br><br>
<p>
<p>
-
These equations describe the essential proteins our system ($YF1$, $FixJ$, Phosphorylated $YF1$, Phosphorylated $FixJ$, $CI$, $TetR$). Proteins are produced with rates that depend on the strength of respective promoter and ribosome binding site, and also when phosphorylated protein (denoted with phos) is dephosphorylated back to its original form. The concentration of all proteins reduces by degradation, the rate of which depends on the concentration of protein in question.
+
These equations describe the essential proteins our system ($YF1$, $FixJ$, Phosphorylated $YF1$, Phosphorylated $FixJ$, $CI$, $TetR$). Proteins are produced with rates that depend on the strength of respective promoter and ribosome binding site, and also when phosphorylated protein (denoted with $phos$) is dephosphorylated back to its original form. The concentration of all proteins reduces by degradation and its depends on the concentration of protein in question.
</p>
</p>
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<h3>Dynamics' coefficients</h3>
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<h3>Rate Coefficients</h3>
 +
 
<p>
<p>
-
$P_1$, $P_2$, $P_A$ and $P_B$ denote the relative strengths of promoters and $Rbs_1$&$Rbs_2$ the relative strengths of ribosome binding sites, which both affect the protein synthesis linearly. Each protein has its own degradation coefficient (denoted $Deg$). $I_B$ is the combined effect of blue light that affects the phosphorylation of $YF1$. The phosphorylation of $FixJ$ is assumed to depend on phosphorylation coefficient $C_{phos}$ and the concentration of phosphorylated $YF1$. The dephosphorylation here depends on a respective dephosphorylation coefficient $DP$(1&2 for $YF1$ and $FixJ$).
+
$P_1$, $P_2$, $P_A$ and $P_B$ denote the relative strengths of the promoters. $Rbs$s are the relative strengths of ribosome binding sites, which both affect the mRNA translation rate linearly. Each protein has its own degradation coefficient (denoted $Deg$). $I_B$ is the combined effect of blue light that affects the phosphorylation of $YF1$. The phosphorylation of $FixJ$ is assumed to depend on phosphorylation coefficient $C_{phos}$ and the concentration of phosphorylated $YF1$. The dephosphorylation here depends on the respective dephosphorylation coefficient $DP$(1&2 for $YF1$ and $FixJ$). Later on, we found out that non-phosphorylated YF1 acts as a phosphatase on FixJ. However, these effects are not taken into account in our model.
</p>
</p>
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<h3>Equations for promoter activities</h3>
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<h3 class="nopaddingbottom">Equations for Promoter Activities</h3>
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Equations for promoter activities
 
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<p class="modellatex">
\begin{eqnarray*}
\begin{eqnarray*}
-
& & P_2  = C_{P_2}N[CI] \\
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& & P_2  = C_{P_2}N_1[CI] \\
\\
\\
& & P_A =
& & P_A =
\begin{cases}
\begin{cases}
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C_{P_A}N[CI] \quad \text{if} \quad N[CI] \leq 1 \\
+
C_{P_A}N_1[CI] \quad \text{if} \quad N_1[CI] \leq 1 \\
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0 \quad \text{if} \quad N[CI] > 1
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0 \quad \text{if} \quad N_1[CI] > 1
\end{cases} \\
\end{cases} \\
\\
\\
& & P_B =
& & P_B =
\begin{cases}
\begin{cases}
-
C_{P_B}N[CI] \quad \text{if} \quad N[CI] < 1 \\
+
C_{P_B}N[CI] \quad \text{if} \quad N_1[CI] < 1 \\
-
C_{P_B}(1-(N[CI] - 1)) \quad \text{if} \quad 1 \leq N[CI] < 2 \\
+
C_{P_B}(1-(N_1[CI] - 1)) \quad \text{if} \quad 1 \leq N_1[CI] < 2 \\
-
0 \quad \text{if} \quad N[CI] \geq 2
+
0 \quad \text{if} \quad N_1[CI] \geq 2
\end{cases} \\
\end{cases} \\
\\
\\
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\end{eqnarray*}
\end{eqnarray*}
</p>
</p>
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<h3>Promoters' coefficients</h3>
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<h3 class="nopaddingtop">Promoter Coefficients</h3>
<p>
<p>
-
Here, the $C_{P_n}$'s denote the respective promoter's maximum activity. The $N$ in front of $CI$ and $TetR$ concentrations is a normalization coefficient,
+
Here the $C_{P_n}$s denote the respective promoter's maximum activity. The $N_1$ and $N_2$ in front of $CI$ and $TetR$ concentrations are normalization coefficients, which are needed to map the values of $[CI]$ to the interval $(0,3)$ and values of $[TetR]$ to the interval $(0,1)$. This way, when multiplied by the promoters' maximum activity values, we get values in the interval $(0, C_{P_n})$  The functions definitions must also change so that they never take negative values, which would make no sense when it refers to promoter activity. We have simplified the model so that the promoters’ activity only depend on $[CI]$ and $[FixJ]$.
-
which is needed to map the fitting part of concentrations' values to the interval $(0,1)$. This way, when multiplied by the promoters' maximum activity values, we get values in the interval $(0, C_{P_n})$  The fuctions definitions must also change so that they never take negative values, which would make no sense when talking about promoter activities.
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<h2>Simulation</h2>
<h2>Simulation</h2>
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<h3>Overview </h3>
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<h3 class="kakspaddingtop">Overview </h3>
<p>
<p>
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Based on our mathematical model, we created an interactive simulation and a graphical user interface for it. This visualization, although idealized, is ideal for demonstrating the intended functioning of our gene circuit and gene switch system. We included two swithces, one for red and one for blue light. With these, the user can see the effect of light intensity to a bacterial coulture in real time. Here, proteins A, B and C are represented by GFP, RFP and BFP, so the bacteria change color in different circumstances. The original simulation was written in Python and later translated into Javascript, and it can be viewed on our web page by anyone. The source code can be found on our GitHub page.
+
Based on our mathematical model, we created an interactive simulation and a graphical user interface for it. This visualization, although idealized, is suitable for demonstrating the intended functioning of our gene circuit and the gene switch system. We included two sliders, one for red and one for blue light. With these, the user can see the effect of the light intensity to the simulated bacterial culture in real time. Proteins $A$, $B$ and $C$ are represented by GFP, RFP and BFP (green, red and blue fluorescent protein) and therefore the bacteria change color when lights’ intensities are changed.
<p/>
<p/>
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<p>
<p>
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In our system, the communication between user and the bacteria happens via illumination of blue light to the coulture. Blue light phosphorylates the $YF1$-protein, which is the key to controlling the overall protein production inside the bacterium. In the simulation, this is represented by change in the $I_B$ parameter from the mathematical model. This takes values between 0 and 1, and the rest of system behaves as described earlier.
+
In our system, the communication between user and the bacteria happens via illuminating the culture with blue and red light. Blue light phosphorylates the $YF1$-protein, which is the key to controlling the production of $A$, $B$ and $C$ proteins inside the bacteria. In the simulation, this is represented by change in the $I_B$ parameter from the mathematical model. This takes values between 0 and 1, and the rest of the system behaves as described previously.
</p>
</p>
<p>
<p>
-
Our original design had also an intensity switch, operated by red light. Due to time constraits, this wasn't yet implemented in our gene circuit. In the simulation, we added a second user controlled parameter in front of every promoter. This takes values between 0 and 1, representing the no production at all -state and the production at maximum promoter activity. With this, the user has control of all protein concentrations. The assumed mechanism is idealized and has a linear effect on the activity.
+
Our original design also had a transcription intensity switch, controlled by red light. Due to time constrains, this wasn't yet implemented in our gene circuit. In the simulation, we added a second user controlled parameter in front of every promoter. This takes values between 0 and 1, representing the zero production state and the production at maximum promoter activity. With this, the user has control of all desired protein concentrations. The assumed mechanism is idealized and has a linear effect on the activity.
</p>
</p>
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<h3>Runge-Kutta method </h3>
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<h3>Runge-Kutta Method </h3>
<p>
<p>
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The dynamics of our system were approximated using 4th order Runge-Kutta (RK4) method for the differential equations in our mathematical model. The point of this method is to approximate the function in question by it's derivatives without having to solve the function itself. The starting values of each concentrations are assumed to be zero, so y(0) = 0. With this, the simulation computes the next datapoint adding the derivative times a timestep (h) to previous concentrations. The method uses a mean value of different derivatives (the different k's below) during this timestep h to get a more accurate approximation.
+
The dynamics of our system were approximated and computed using 4th order Runge-Kutta method (RK4) for the differential equations in our mathematical model. The point of this method is to approximate the function in question by it's derivatives without having to solve the function itself. The starting values of each concentration are assumed to be zero, so $y(0) = 0$. The simulation computes the next datapoint adding the derivative times a timestep $h$ to previous concentrations. The method uses a mean value of different derivatives (the different k's below) during timestep $h$ to get a more accurate approximation.
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RK4 equations
 
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RK4 equations
 
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\begin{eqnarray*}
\begin{eqnarray*}
& & y' = f(t,y(t)), \quad y(t_0) = y_0 \\
& & y' = f(t,y(t)), \quad y(t_0) = y_0 \\
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<h3>Software implementation</h3>
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<h3 class="nopaddingtop">Software Implementation</h3>
<p>
<p>
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A computational model was created based on our mathematical model and the RK4 approximation. We made a real-time plotting function to illustrate the dynamics with each timestep. We added two light switches so that the user can have an impact on our simulation in real time. This all was then further developed into a presentable, user-friendly form that is accessible from our website. The simulation itself was created using Python and translated into Javascript for web implementation.
+
A computational model was created based on our mathematical model and the RK4 approximation. We made a real-time visualisation script to illustrate the dynamics in a simple and clear graphic UI. We added two light switches so that the user can have an impact on our simulation in real time. This all was then further developed into a presentable, user-friendly form that is accessible from our website. The simulation itself was created using Python and translated into Javascript for web implementation.
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<div class="img-center">
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<a href="http://igem-qsf.github.io/SimCircus/WebUI/"><img src="https://static.igem.org/mediawiki/2014/0/03/Aalto_Helsinki_Simulation.png" class="img-responsive"></a>
+
<a href="http://igem-qsf.github.io/SimCircus/WebUI/" target="_blank"><img src="https://static.igem.org/mediawiki/2014/0/03/Aalto_Helsinki_Simulation.png" class="img-responsive"></a>
<p class="kuvateksti">
<p class="kuvateksti">
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The UI of our simulation
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Here is a screenshot of the simulation. You can adjust the amount of the red and blue light and see how it affects the bacteria. You can also see how active each gene (A, B, C) is.
</p>
</p>
</div>
</div>
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<p>
<p>
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To demonstrate our work to the general public in an event called Summer of Startups Demo Day, we made a <a href="https://static.igem.org/mediawiki/2014/0/03/Aalto_Helsinki_Simulation.png">simulation</a> that shows our system in action. It shows an animated bacteria plate with adjustable light intensity sliders to remotely control the bacteria. The proteins the bacteria produce are colors, so you can see how the changes in light intensity correlate to the color of the colonies on the plate. The simulation also has a nice grap that shows the protein levels in one second intervals so you can see more clearly what's going on in the cell.
+
To demonstrate our work for the general public in an event, <a href="https://2014.igem.org/Team:Aalto-Helsinki/Business#Sos">Summer of Startups Demo Day</a>, we used the <a href="http://igem-qsf.github.io/SimCircus/WebUI/">simulation</a> to show our system in action. It can be accessed with a web browser and shows an animated bacterial plate with adjustable light intensity sliders to remotely control the bacteria. The proteins the bacteria produce in this simulation are colors, so you can see how the changes in light intensity correlate to the color of the colonies on the plate. The simulation also has a nice graph that shows the protein levels in real time so you can see more clearly what's going on in the cell.
</p>
</p>
<p>
<p>
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All of the code (including a more in-detail Python graph simulation) is available at the project's <a href="http://github.com/iGEM-QSF/SimCircus">GitHub page.</a>
+
All the code (including the Python simulation with more detailed graphs) is available at the project's <a href="http://github.com/iGEM-QSF/SimCircus">GitHub page.</a>
</p>
</p>
</article>
</article>
<div class="update Simulation"></div>
<div class="update Simulation"></div>
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<div class="update Accuracy"></div>
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<div class="update Discussion"></div>
<article>
<article>
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<div class="link" id="Accuracy"></div>
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<div class="link" id="Discussion"></div>
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<h2>Accuracy </h2>
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<h2 class="ykspaddingbottom">Discussion</h2>
<p>
<p>
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No noise was implemented in our simulation, so the results are over-idealized. This is generally very far from the truth in all biological systems, but having no noise gave us a pretty good idea of how things should work in a best case scenario.
+
Our model doesn’t take any noise into consideration. Therefore all interactions produce smooth, good-looking curves. On the other hand, the clear graphics generated by the simulation are easily interpretable, so even someone not familiar with science can clearly see what's going on in our system.
 +
</p>
 +
<p>
 +
So far we have also used arbitrary parameters, simplified reaction pathways and reaction equations. The parameters were acquired by estimation and empirical testing. Full experimental data wasn't available when the simulation was created, so derivation of differential equations by using the law of mass-action was not possible. All reaction mechanisms are our own estimations of what's going on inside the bacteria and the system.
 +
</p>
 +
 +
<p>
 +
Some unexpected observations were made after running the simulation several times. We noticed that when activating all the promoters while the $CI$ concentration was zero, both proteins $A$ and $C$ were produced simultaneously instead of just the anticipated $A$. When $TetR$ is further produced by the activation of $P_R$ promoter, $C$ production is repressed and the concentration drops back to zero. Secondly, when blue light intensity is set to a level that corresponds to the maximum concentration of either $A$ or $B$, the promoter activity adjustable using the red light and it should only affect the said concentration. Again, when lowering the activity enough, we noticed that a spike in production of protein $C$ appeared again. This seemed to be caused by the lowered concentration of $TetR$ that allowed a leak in $P_C$ promoter. We had no idea that a $C$ spike would appear based on the theoretical model of our gene circuit, so this phenomenon was discovered early thanks to our simulation.
 +
</p>
 +
 +
<p>
 +
We also noticed that going from directly producing the protein $A$ to protein $C$, or reversely, from $C$ to $A$ is virtually impossible without producing some protein $B$ along the way. We thus concluded that our Gene Switch is not entirely orthogonal between the three channels. The possible interactions with other products with protein $B$ are needed to be taken under consideration when designing applications that only use genes $A$ and $C$.
 +
</p>
 +
 +
<p>
 +
Upon later research, we found out the actual mechanism with which $FixJ$ was phosphorylated. In contrast to our model, the phosphate is actually transmitted from $YF1$ to $FixJ$. In their paper, Möglich et al. (2009, reference in research section) showed that in a two-step reaction, $FixL$ first undergoes autophosphorylation and then transfers the phosphate to its cognate, noncovalently bound, response regulator $FixJ$. The $YF1$ protein is a derivative of $FixL$ with different sensory domain, so it behaves the same way in this reaction. This wasn't however implemented in our model.
</p>
</p>
<p>
<p>
-
So far we have also used arbitrary parameters, simplified reaction pathways and reaction equations. In it's current state the simulation gives a good idea on how the system should work. Making it realistic and really accurate requires a lot of measurement of appropriate parameters and tuning. Still, this version is ideal for demonstration of our idea.
+
In it's current state the simulation gives a good idea on how the system should work. Making it realistic and accurate requires measuring the appropriate parameters, research on appropriate scientific publications, and tuning. Still, this version is ideal for demonstration of our idea, bringing the visual UI a significant marketing value.
</p>
</p>
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     $.each(tables, function(index, e){
     $.each(tables, function(index, e){
             var tableName = e.getAttribute("tab");
             var tableName = e.getAttribute("tab");
             if (!e.id){
             if (!e.id){
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                 e.setAttribute("id","figure"+(index+1));
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                 e.setAttribute("id","table"+(index+1));
             }
             }
             $.each($('a[tab="'+tableName+'"]'), function(j, e2){
             $.each($('a[tab="'+tableName+'"]'), function(j, e2){

Latest revision as of 15:14, 17 October 2014

Modeling

Before bringing all the parts together in the lab, we built our switch in the mathematical world.

Introduction

To get an idea of how our gene circuit would work in an ideal situation, we explored the structure and dynamics of our system by creating a mathematical model of the reaction kinetics and a simulation that can be controlled in real time. We started working with the mathematical model without any detailed information about the system. We derived the differential equations to demonstrate how blue light and the changes in phosphorylated $YF1$ and $FixJ$ concentrations would affect the production of our three target proteins. We labeled them simply $A$, $B$ and $C$, because the system is intended to be used with any three genes encoding the proteins of choice.

Using our equations we constructed a simulation showing the effects of red and blue light on our system in real time. The user can control the input of both lights to see how they affect the production of proteins $A$, $B$ and $C$. We experimented with different values for all constants and via trial-and-error iteration we arrived to a visualized simulation that can be used to demonstrate the intended function of our system. This is an idealization. Based on present and future measurement data, the parameters can be adjusted to better the dynamics of our system.

Mathematical Model

Assumptions

We assumed that the species identified in our gene circuit are the only ones that affect the overall concentrations inside the bacteria. We further assumed that binding of $CI$ to $O_R$ operator site does not impact the overall $CI$ concentration and that the amount of $CI$ bound to the $O_R$ sites was proportional to $CI$ concentration. The model is also strictly deterministic and doesn’t take any noise into account. The phosphorylation, decay, binding and production of proteins are assumed to be linear functions of concentration. We further assumed that the phosphorylation of $FixJ$ by phosphorylated $YF1$ would not involve phosphate transfer between the reacting molecules.

The first model was constructed before our lab work had even begun and it contains many harsh simplifications. Our aim was to get a general picture of how the system could work in ideal conditions and how stable it was.

Equations for Dynamics

Based on the assumptions made before, we arrived at following differential equations to describe the idealized dynamics of our system:

\begin{eqnarray*} & & \frac{d[YF1]}{dt} = P_1Rbs_{YF1} + DP_1[YF1]_{phos} - (Deg_{YF1}+I_B)[YF1] \\ \quad \\ & & \frac{d[YF1]_{phos}}{dt} = I_B[YF1] - (Deg_{\text{YF1}} + DP_1)[YF1]_{phos} \\ \ & & \frac{d[FixJ]}{dt} = P_1Rbs_{FixJ} + DP_2[FixJ]_{phos} - (C_{phos}[YF1]_{phos} + Deg_{FixJ})[FixJ] \\ \\ & & \frac{d[FixJ]_{phos}}{dt} = C_{phos}[YF1]_{phos}[FixJ] - (DP_2[FixJ]_{phos} + Deg_{FixJ}[FixJ]) \\ \\ & & \frac{d[CI]}{dt} = P_2Rbs_{CI} - Deg_{CI}[CI] \\ \\ & & \frac{d[TetR]}{dt} = P_ARbs_{TetR_A} + P_BRbs_{TetR_B} - Deg_{TetR}[TetR] \end{eqnarray*}

    Legend

  • $[YF1]$ = concentration of $YF1$ protein
  • $[YF1]_{phos}$ = concentration of phosphorylated $YF1$ protein
  • $[FixJ]$ = concentration of $FixJ$ protein
  • $[FixJ]_{phos}$ = concentration of phosphorylated $FixJ$ protein
  • $[CI]$ = concentration of $CI$ protein
  • $[TetR]$ = concentration of $TetR$ protein
  • $P_1$ = relative strength of the first promoter in gene circuit
  • $P_2$ = relative strength of the $FixK_2$ promoter
  • $P_A$ = relative strength of the $P_R$ promoter, codes gene $A$
  • $P_B$ = relative strength of the $P_{RM}$ promoter, codes gene $B$
  • $P_C$ = relative strength of the promoter coding gene $C$
  • $Rbs$ = relative strengths of ribosome binding sites
  • $Deg$ = degradation coefficient
  • $C_{phos}$ = phosphorylation coefficient
  • $DP$ = de-phosphorylation coefficient


These equations describe the essential proteins our system ($YF1$, $FixJ$, Phosphorylated $YF1$, Phosphorylated $FixJ$, $CI$, $TetR$). Proteins are produced with rates that depend on the strength of respective promoter and ribosome binding site, and also when phosphorylated protein (denoted with $phos$) is dephosphorylated back to its original form. The concentration of all proteins reduces by degradation and its depends on the concentration of protein in question.

Rate Coefficients

$P_1$, $P_2$, $P_A$ and $P_B$ denote the relative strengths of the promoters. $Rbs$s are the relative strengths of ribosome binding sites, which both affect the mRNA translation rate linearly. Each protein has its own degradation coefficient (denoted $Deg$). $I_B$ is the combined effect of blue light that affects the phosphorylation of $YF1$. The phosphorylation of $FixJ$ is assumed to depend on phosphorylation coefficient $C_{phos}$ and the concentration of phosphorylated $YF1$. The dephosphorylation here depends on the respective dephosphorylation coefficient $DP$(1&2 for $YF1$ and $FixJ$). Later on, we found out that non-phosphorylated YF1 acts as a phosphatase on FixJ. However, these effects are not taken into account in our model.

Equations for Promoter Activities

\begin{eqnarray*} & & P_2 = C_{P_2}N_1[CI] \\ \\ & & P_A = \begin{cases} C_{P_A}N_1[CI] \quad \text{if} \quad N_1[CI] \leq 1 \\ 0 \quad \text{if} \quad N_1[CI] > 1 \end{cases} \\ \\ & & P_B = \begin{cases} C_{P_B}N[CI] \quad \text{if} \quad N_1[CI] < 1 \\ C_{P_B}(1-(N_1[CI] - 1)) \quad \text{if} \quad 1 \leq N_1[CI] < 2 \\ 0 \quad \text{if} \quad N_1[CI] \geq 2 \end{cases} \\ \\ & & P_C = \begin{cases} C_{P_A}(1-N_2[TetR]) \quad \text{if} \quad N_2[TetR] \leq 1 \\ 0 \quad \text{if} \quad N_2[TetR] > 1 \end{cases} \end{eqnarray*}

Promoter Coefficients

Here the $C_{P_n}$s denote the respective promoter's maximum activity. The $N_1$ and $N_2$ in front of $CI$ and $TetR$ concentrations are normalization coefficients, which are needed to map the values of $[CI]$ to the interval $(0,3)$ and values of $[TetR]$ to the interval $(0,1)$. This way, when multiplied by the promoters' maximum activity values, we get values in the interval $(0, C_{P_n})$ The functions definitions must also change so that they never take negative values, which would make no sense when it refers to promoter activity. We have simplified the model so that the promoters’ activity only depend on $[CI]$ and $[FixJ]$.

Simulation

Overview

Based on our mathematical model, we created an interactive simulation and a graphical user interface for it. This visualization, although idealized, is suitable for demonstrating the intended functioning of our gene circuit and the gene switch system. We included two sliders, one for red and one for blue light. With these, the user can see the effect of the light intensity to the simulated bacterial culture in real time. Proteins $A$, $B$ and $C$ are represented by GFP, RFP and BFP (green, red and blue fluorescent protein) and therefore the bacteria change color when lights’ intensities are changed.

Lights

In our system, the communication between user and the bacteria happens via illuminating the culture with blue and red light. Blue light phosphorylates the $YF1$-protein, which is the key to controlling the production of $A$, $B$ and $C$ proteins inside the bacteria. In the simulation, this is represented by change in the $I_B$ parameter from the mathematical model. This takes values between 0 and 1, and the rest of the system behaves as described previously.

Our original design also had a transcription intensity switch, controlled by red light. Due to time constrains, this wasn't yet implemented in our gene circuit. In the simulation, we added a second user controlled parameter in front of every promoter. This takes values between 0 and 1, representing the zero production state and the production at maximum promoter activity. With this, the user has control of all desired protein concentrations. The assumed mechanism is idealized and has a linear effect on the activity.

Runge-Kutta Method

The dynamics of our system were approximated and computed using 4th order Runge-Kutta method (RK4) for the differential equations in our mathematical model. The point of this method is to approximate the function in question by it's derivatives without having to solve the function itself. The starting values of each concentration are assumed to be zero, so $y(0) = 0$. The simulation computes the next datapoint adding the derivative times a timestep $h$ to previous concentrations. The method uses a mean value of different derivatives (the different k's below) during timestep $h$ to get a more accurate approximation.

\begin{eqnarray*} & & y' = f(t,y(t)), \quad y(t_0) = y_0 \\ \\ \\ & & y_{n+1} = y_n + \frac{h}{6}(k_1 + 2k_2 + 2k_3 + k_4) \\ & & t_{n+1} = t_n + h \\ \\ & & k_1 = f(t_n,y_n) \\ & & k_2 = f(t_n +\frac{h}{2}, y_n + \frac{h}{2}k_1) \\ & & k_3 = f(t_n + \frac{h}{2}, y_n + \frac{h}{2}k_2) \\ & & k_4 = f(t_n + \frac{h}{2}, y_n +hk_3) \end{eqnarray*}

Software Implementation

A computational model was created based on our mathematical model and the RK4 approximation. We made a real-time visualisation script to illustrate the dynamics in a simple and clear graphic UI. We added two light switches so that the user can have an impact on our simulation in real time. This all was then further developed into a presentable, user-friendly form that is accessible from our website. The simulation itself was created using Python and translated into Javascript for web implementation.

Here is a screenshot of the simulation. You can adjust the amount of the red and blue light and see how it affects the bacteria. You can also see how active each gene (A, B, C) is.

To demonstrate our work for the general public in an event, Summer of Startups Demo Day, we used the simulation to show our system in action. It can be accessed with a web browser and shows an animated bacterial plate with adjustable light intensity sliders to remotely control the bacteria. The proteins the bacteria produce in this simulation are colors, so you can see how the changes in light intensity correlate to the color of the colonies on the plate. The simulation also has a nice graph that shows the protein levels in real time so you can see more clearly what's going on in the cell.

All the code (including the Python simulation with more detailed graphs) is available at the project's GitHub page.

Discussion

Our model doesn’t take any noise into consideration. Therefore all interactions produce smooth, good-looking curves. On the other hand, the clear graphics generated by the simulation are easily interpretable, so even someone not familiar with science can clearly see what's going on in our system.

So far we have also used arbitrary parameters, simplified reaction pathways and reaction equations. The parameters were acquired by estimation and empirical testing. Full experimental data wasn't available when the simulation was created, so derivation of differential equations by using the law of mass-action was not possible. All reaction mechanisms are our own estimations of what's going on inside the bacteria and the system.

Some unexpected observations were made after running the simulation several times. We noticed that when activating all the promoters while the $CI$ concentration was zero, both proteins $A$ and $C$ were produced simultaneously instead of just the anticipated $A$. When $TetR$ is further produced by the activation of $P_R$ promoter, $C$ production is repressed and the concentration drops back to zero. Secondly, when blue light intensity is set to a level that corresponds to the maximum concentration of either $A$ or $B$, the promoter activity adjustable using the red light and it should only affect the said concentration. Again, when lowering the activity enough, we noticed that a spike in production of protein $C$ appeared again. This seemed to be caused by the lowered concentration of $TetR$ that allowed a leak in $P_C$ promoter. We had no idea that a $C$ spike would appear based on the theoretical model of our gene circuit, so this phenomenon was discovered early thanks to our simulation.

We also noticed that going from directly producing the protein $A$ to protein $C$, or reversely, from $C$ to $A$ is virtually impossible without producing some protein $B$ along the way. We thus concluded that our Gene Switch is not entirely orthogonal between the three channels. The possible interactions with other products with protein $B$ are needed to be taken under consideration when designing applications that only use genes $A$ and $C$.

Upon later research, we found out the actual mechanism with which $FixJ$ was phosphorylated. In contrast to our model, the phosphate is actually transmitted from $YF1$ to $FixJ$. In their paper, Möglich et al. (2009, reference in research section) showed that in a two-step reaction, $FixL$ first undergoes autophosphorylation and then transfers the phosphate to its cognate, noncovalently bound, response regulator $FixJ$. The $YF1$ protein is a derivative of $FixL$ with different sensory domain, so it behaves the same way in this reaction. This wasn't however implemented in our model.

In it's current state the simulation gives a good idea on how the system should work. Making it realistic and accurate requires measuring the appropriate parameters, research on appropriate scientific publications, and tuning. Still, this version is ideal for demonstration of our idea, bringing the visual UI a significant marketing value.