Difference between revisions of "Team:TUDelft/DennisModel"

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             <h2>Overview</h2>
 
             <h2>Overview</h2>
             <p> Our modeling aimed to apply a control systems approach to achieve stability across bacterial species. To make expression host-independent, we proposed to include an incoherent feedforward loop in our design. Our analytical steady-state solution of this system showed that expression was completely independent of plasmid copy number and transcriptional and translational rates.  We verified this analytical solution by the implementation of a full Ordinary Differential Equation (ODE) model.     
+
             <p> With our modeling we aimed to apply a control systems approach to achieve stability across bacterial species. To make expression host-independent, we proposed to include an incoherent feedforward loop in our design. Our analytical steady-state solution of this loop showed that expression was completely independent of plasmid copy number and transcriptional and translational rates.  We verified this analytical solution by the implementation of a full kinetic model.     
 
                 <br>
 
                 <br>
 
                 <br>  
 
                 <br>  
  
                 Variables most often considered in the design of genetic circuits are plasmid copy number and transcriptional and translational rates. These variables play a major role in the steady-state levels of gene expression. However, when transferring genetic circuits between organisms, these variables change in unpredictable ways:
+
                 The key variables in the design of genetic circuits are plasmid copy number and transcriptional and translational rates. These variables play a major role in the steady-state levels of gene expression. However, when transferring genetic circuits between organisms, these variables change in unpredictable ways.
 
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                     <p>Promoters have different strengths in different organisms. Some promoters only work in a very narrow range of bacterial species (Yang, Liu et al. 2018). We, therefore, applied the concept of orthogonality, we approached the issue with the using T7 RNA polymerase. Although orthogonal transcription might not behave similarly when applied in varying biological contexts. We show through modeling that this won't influence gene expression levels when using our genetic circuit implementation of an iFFL. </p>
+
                     <p>Promoters have different strengths in different organisms. Some promoters only work in a very narrow range of bacterial species (Yang, Liu et al. 2018). In order to circumvent host related changes we made our system orthogonal to the host. We do this by using T7 RNA polymerase. Although orthogonal transcription might not behave similarly when applied in varying biological contexts. We show through modeling that this won't influence gene expression levels when using our genetic circuit implementation of an iFFL. </p>
 
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                     <p> Ribosome binding sites contain the Shine-Dalgarno sequence where the 16s rRNA of the ribosome binds. However, this sequence varies across species, and often ribosome binding sites are extremely inefficient when applied in phylogenetically distant species (Damilola Omotajo 2015). Our model shows that similar expression levels across organisms can be maintained when all genes in our genetic in the iFFL contain the same ribosome binding site. However, this is assuming translation elongation is similar in these species. Codon usage has been shown to influence translation elongation. We, therefore, developed a software tool that provides the user with a coding sequence similar in codon usage across different species. Similar codon usage minimizes any codon bias, which would cause translation elongation differences. </p>
+
                     <p> Ribosome binding sites contain the Shine-Dalgarno sequence where the 16s rRNA of the ribosome binds. However, this sequence varies across species, and often ribosome binding sites are extremely inefficient when applied in phylogenetically distant species (Salis, et al). Our model shows that similar expression levels across organisms can be maintained when all genes in our genetic circuit contain the same ribosome binding site. However, this is assuming translation elongation is similar in these species. However, translation elongation has been shown to be influenced by codon usage, which differs per organism. We, therefore, developed a software tool that determines a coding sequence similar in codon usage across different species. Similar codon usage minimizes any codon bias, which would cause translation elongation differences. </p>
 
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                    <img src = "https://static.igem.org/mediawiki/2019/1/19/T--TUDelft--ORI.png"  alt="Ori SOBL" style="width:90%;">
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                <img src = "https://static.igem.org/mediawiki/2019/1/19/T--TUDelft--ORI.png"  alt="Ori SOBL" style="width:90%;">
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                    <p>Genetic engineering makes extensive use of plasmids. However, not all plasmids work in every organism as they require a different origin of replication. Although origins of replication have been heavily studied, we still lack the ability to transfer plasmids between prokaryotes easily, and often they behave unpredictably (Jain and Srivastava 2013). Our system Sci-Phi29 makes use of the Phi29 replication system, which is fully orthogonal. However, this might still result in varying copy number when transferring between organisms. Through modeling,  we show that the steady-state level of the gene of interest is independent of copy number when our genetic implementation of an incoherent feedforward loop is used.  </p>
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            <div class="column right">
             <h2>The core of our model - Incoherent feed forward loop </h2>
+
                <p>Genetic engineering makes extensive use of plasmids. However, not all plasmids work in every organism as they require a different origin of replication. Although origins of replication have been heavily studied, we still lack the ability to transfer plasmids between prokaryotes easily, and often they behave unpredictably (Jain and Srivastava 2013). Our system Sci-Phi29 makes use of the Phi29 replication system, which is fully orthogonal to the host. However, an orthogonal replication system might still result in varying plasmid copy number when transferred between organisms. Through modeling,  we show that the steady-state level of the gene of interest is independent of copy number when our genetic implementation of an incoherent feedforward loop is used.  </p>
 +
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 +
           
 +
             <h2>The core of our design - Incoherent feed forward loop </h2>
 
             <p>
 
             <p>
                 We implemented an incoherent feedforward loop (iFFL) in a genetic circuit. In an iFFL, the input signal regulates both the activator and the repressor of the output of the system in the same way.  The iFFL results in perfect adaptation to the input when the negative regulation is fully uncooperative (Segall-Shapiro, Sontag et al. 2018).  
+
                 We implemented an incoherent feedforward loop (iFFL) in a genetic circuit. In an iFFL, the input signal regulates both the activator and the repressor of the output of the system in the same way.  The iFFL results in perfect adaptation to the input when the negative regulation is fully uncooperative (Segall, et al. 2018).  
                 The input in our case is the copy number of the DNA template, and the output is the steady-state expression of a gene of interest. In our system, we use a transcription activator-like effector (TALE) protein as a repressor. TALE proteins recognize DNA by a simple DNA-binding mechanism (Doyle 2013) and have been shown to bind fully uncooperative (Segall-Shapiro, Sontag et al. 2018). The promoter driving the gene of interest has been engineered to contain a binding site of a TALE protein. When the TALE protein is bound to the promoter, the expression of the gene of interest is repressed.  
+
                 The input in our case is the copy number of the DNA template, and the output is the steady-state expression of a gene of interest. In our system, we use a transcription activator-like effector (TALE) protein as a repressor. TALE proteins recognize DNA by a simple DNA-binding mechanism (Doyle 2013) and have been shown to bind fully uncooperative (Segall, et al. 2018). The promoter driving the gene of interest has been engineered to contain a binding site of a TALE protein. When the TALE protein is bound to the promoter, the expression of the gene of interest is repressed.  
 
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             </p>
 
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                         <p>  
 
                         <p>  
 
                         <h2>The kinetics</h2>
 
                         <h2>The kinetics</h2>
                         <p>In this section, we explain the kinetics of our system and derive a system of ordinary differential equations to describe the interactions within the genetic circuit. From this, we derive a steady-state solution step-wise, and describe the properties of the system. In the other sections, we use these properties to describe how we can utilize them to transfer genetic circuits between prokaryotes.  
+
                         <p>In this section, we explain the kinetics of our system and derive a system of ordinary differential equations to describe the interactions within the genetic circuit. We will step-wise derive a steady-state solution from the system of equations and describe the properties of the system. In the other sections, we use these properties to describe how we can utilize them to transfer genetic circuits between prokaryotes.  
 
                             The following scheme depicts all interactions considered in our system. </p>
 
                             The following scheme depicts all interactions considered in our system. </p>
  
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                             <img src="https://static.igem.org/mediawiki/2019/8/85/T--TUDelft--TALE_system.png"  style="width:70%" class="centermodel"
 
                             <img src="https://static.igem.org/mediawiki/2019/8/85/T--TUDelft--TALE_system.png"  style="width:70%" class="centermodel"
 
                                 alt="TALE system">
 
                                 alt="TALE system">
                             <figcaption class="centermodel"><br>Figure 2: Scheme of genetic circuit interactions developed by <cite><a href="https://www.nature.com/articles/nbt.4111"><i>(Sontag et al. (2018))</i></a></cite></figcaption>
+
                             <figcaption class="centermodel"><br>Figure 2: Scheme of genetic circuit interactions developed by <cite><a href="https://www.nature.com/articles/nbt.4111"><i>(Segall, et al. (2018))</i></a></cite></figcaption>
 
                         </figure>
 
                         </figure>
 
                         <br>
 
                         <br>
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                                 <td>$b_T$</td>
 
                                 <td>$b_T$</td>
 
                                 <td> 0.44 </td>
 
                                 <td> 0.44 </td>
                                 <td> (1/min) </td>
+
                                 <td> 1/min </td>
 
                                 <td>Translation rate TALE</td>
 
                                 <td>Translation rate TALE</td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>. </td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>. </td>
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                                 <td>$y_T$</td>
 
                                 <td>$y_T$</td>
 
                                 <td> 0.0347  </td>
 
                                 <td> 0.0347  </td>
                                 <td> (1/min) </td>
+
                                 <td> 1/min </td>
 
                                 <td>Degradation rate TALE</td>
 
                                 <td>Degradation rate TALE</td>
 
                                 <td> </td>
 
                                 <td> </td>
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                                 <td>$k_{on}$</td>
 
                                 <td>$k_{on}$</td>
 
                                 <td>9.85 </td>
 
                                 <td>9.85 </td>
                                 <td>(1/(nM*min)) </td>
+
                                 <td>1/(nM*min) </td>
 
                                 <td>Binding of TALE to promoter</td>
 
                                 <td>Binding of TALE to promoter</td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>.  </td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>.  </td>
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                                 <td>$k_{off}$</td>
 
                                 <td>$k_{off}$</td>
 
                                 <td>2.19</td>
 
                                 <td>2.19</td>
                                 <td>(1/(min))</td>
+
                                 <td>1/min</td>
 
                                 <td>Unbinding of TALE to promoter</td>
 
                                 <td>Unbinding of TALE to promoter</td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>.  </td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite>.  </td>
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                                 <td>$a_{Gmax}$</td>
 
                                 <td>$a_{Gmax}$</td>
 
                                 <td> 3.78 </td>
 
                                 <td> 3.78 </td>
                                 <td>(1/(nM*Min)) </td>
+
                                 <td>1/(nM*min) </td>
 
                                 <td>Maximum transcription of GFP</td>
 
                                 <td>Maximum transcription of GFP</td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite> </td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite> </td>
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                                 <td>$a_{Gmin}$</td>
 
                                 <td>$a_{Gmin}$</td>
 
                                 <td> 0 </td>
 
                                 <td> 0 </td>
                                 <td>  (1/(nM*Min)) </td>
+
                                 <td>  1/(nM*min) </td>
 
                                 <td>Maximum transcription of GFP</td>
 
                                 <td>Maximum transcription of GFP</td>
 
                                 <td><cite><a href="https://www.ncbi.nlm.nih.gov/pubmed/29553576"><i>Segall-Shapiro, Sontag et al.</i></a></cite></td>
 
                                 <td><cite><a href="https://www.ncbi.nlm.nih.gov/pubmed/29553576"><i>Segall-Shapiro, Sontag et al.</i></a></cite></td>
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                                 <td>$b_G$</td>
 
                                 <td>$b_G$</td>
 
                                 <td>3.65 </td>
 
                                 <td>3.65 </td>
                                 <td> (1/Min)</td>
+
                                 <td> 1/Min</td>
 
                                 <td>Translation rate GFP</td>
 
                                 <td>Translation rate GFP</td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite></td>
 
                                 <td><cite><a href="2018.igem.org/Team:Thessaloniki"><i>2018 iGEM Thessaloniki</i></a></cite></td>
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                                 <td> 1/min </td>
 
                                 <td> 1/min </td>
 
                                 <td>Degradation rate GFP</td>
 
                                 <td>Degradation rate GFP</td>
 +
                                <td> </td>
 +
                            </tr>
 +
                            <tr>
 +
                                <td>$c$</td>
 +
                                <td> variable </td>
 +
                                <td> Copy number of plasmid </td>
 +
                                <td> - </td>
 
                                 <td> </td>
 
                                 <td> </td>
 
                             </tr>
 
                             </tr>
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                         <br>
 
                         <br>
 
                         Using these assumptions, we can derive a steady-state solution for this system analytically. This derivation results in the following steady-state solution: <br> <br>
 
                         Using these assumptions, we can derive a steady-state solution for this system analytically. This derivation results in the following steady-state solution: <br> <br>
                         $$G = (\frac{c}{c^n}) (\frac{a_Gb_Gy_T^ny_m^n}{a_Tb_Ty_Gy_m})$$ <br>
+
                         $$G = \left((\frac{c}{c^n}) (\frac{a_Gb_Gy_T^ny_m^n}{a_Tb_Ty_Gy_m}\right)$$ <br>
 
                         <br>
 
                         <br>
  
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                             </div>
 
                             </div>
 
                         </li>
 
                         </li>
 
+
 
                    <br>
+
                        <br>
                    <p>According to our analytical solution, our genetic circuit is only dependent on copy number, and the ratio of transcription and translation rates of the genes in the circuit. In the next sections, we use this steady-state solution to demonstrate how it can be used to transfer genetic circuits between organisms. Furthermore, since this steady-state solution is based on assumptions, we solve the full system of ordinary differential equations in Matlab to validate our assumptions. In each segment, a link to our corresponding wetlab page is given. </p>
+
                        <p>According to our analytical solution, the level of the protein of interest only dependents on copy number, and the ratios of transcription and translation rates of the genes in the circuit. In the next sections, we use this steady-state solution to demonstrate how it can be used to transfer genetic circuits between organisms. Furthermore, since this steady-state solution is based on assumptions, we solve the full system of ordinary differential equations in Matlab to validate our assumptions. In each segment, a link to our corresponding wetlab page is given. </p>
                    <br>
+
                        <br>
                  </ul>
+
                    </ul>
 
                 </li>         
 
                 </li>         
  
         
+
 
 
                 <li>
 
                 <li>
 
                     <a class="toggle " href="javascript:void(0);" ><b>Copy number independence</b></a>
 
                     <a class="toggle " href="javascript:void(0);" ><b>Copy number independence</b></a>
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                         This formula is, however, based on a few assumptions. We, therefore, implemented the full system of ordinary differential equations to validate our assumptions. We vary both transcription parameters. We plot the resulting steady-state solutions as a function of these two variables. A line is plotted to indicate the steady-state solutions resulting from a constant ratio in transcription rates.   
 
                         This formula is, however, based on a few assumptions. We, therefore, implemented the full system of ordinary differential equations to validate our assumptions. We vary both transcription parameters. We plot the resulting steady-state solutions as a function of these two variables. A line is plotted to indicate the steady-state solutions resulting from a constant ratio in transcription rates.   
<img src="https://static.igem.org/mediawiki/2019/0/0f/T--TUDelft--transcription_variation.gif"  style="width:70%" class="centermodel"
+
                        <img src="https://static.igem.org/mediawiki/2019/0/0f/T--TUDelft--transcription_variation.gif"  style="width:70%" class="centermodel"
 
                             alt="TALE system">
 
                             alt="TALE system">
 
                         <figcaption class="centermodel">Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the transcription rate of both genes. </figcaption>
 
                         <figcaption class="centermodel">Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the transcription rate of both genes. </figcaption>
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                         <figcaption class="centermodel">Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the translation rate of both genes. </figcaption>
 
                         <figcaption class="centermodel">Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the translation rate of both genes. </figcaption>
  
                      <p> However, translation isn’t only dependent on initiation, translation elongation is dependent on codon usage. </p>
+
                        <p> However, translation isn’t only dependent on initiation, translation elongation is dependent on codon usage. </p>
  
 
                         [text from Osman here]
 
                         [text from Osman here]
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             </ul>
 
             </ul>
  
     
 
     
 
        <h3>References</h3>
 
        <ol>
 
            <li>
 
                <a id="RBS calculator" href="https://www.nature.com/articles/nbt.1568" target="_blank">
 
                  Salis, H. M., et al. (2009). "Automated design of synthetic ribosome binding sites to control protein expression." <u>Nature Biotechnology </u> 27(10): 946-950.
 
                </a>
 
            </li>
 
            <li>
 
                <a id="Segall-Shapiro" href="https://doi.org/10.1038/nbt.4111" target="_blank">
 
                    Segall-Shapiro, T. H., <i>et al.</i> (2018). "Engineered promoters enable constant gene expression at any copy number in bacteria." <u>Nature Biotechnology</u> 36: 352.
 
                </a>
 
            </li>
 
  
            <li>
 
                <a id="Doyle" href="https://lib.dr.iastate.edu/cgi/viewcontent.cgi?article=4139&context=etd" target="_blank">
 
                Doyle, E. L. (2013). Computational and experimental analysis of TALeffector-DNA binding. Plant Pathology and Microbiology, Iowa State University. <b>Dissertation.</b>
 
                </a>
 
            </li>
 
<li>
 
                <a id="Yang" href="https://www.ncbi.nlm.nih.gov/pubmed/29061047" target="_blank">
 
              Yang, S., et al. (2018). "Construction and Characterization of Broad-Spectrum Promoters for Synthetic Biology." <u> ACS Synthetic Biology </u> 7(1): 287-291.
 
                </a>
 
            </li>
 
  
<a id="Jain" href="https://academic.oup.com/femsle/article/348/2/87/731695" target="_blank">
+
            <h3>References</h3>
            Jain, A. and P. Srivastava (2013). "Broad host range plasmids." <u> FEMS Microbiology Letters </u>348(2): 87-96.
+
            <ol>
 +
                <li>
 +
                    <a id="RBS calculator" href="https://www.nature.com/articles/nbt.1568" target="_blank">
 +
                        Salis, H. M., et al. (2009). "Automated design of synthetic ribosome binding sites to control protein expression." <u>Nature Biotechnology </u> 27(10): 946-950.
 +
                    </a>
 +
                </li>
 +
                <li>
 +
                    <a id="Segall-Shapiro" href="https://doi.org/10.1038/nbt.4111" target="_blank">
 +
                        Segall-Shapiro, T. H., <i>et al.</i> (2018). "Engineered promoters enable constant gene expression at any copy number in bacteria." <u>Nature Biotechnology</u> 36: 352.
 +
                    </a>
 +
                </li>
 +
 
 +
                <li>
 +
                    <a id="Doyle" href="https://lib.dr.iastate.edu/cgi/viewcontent.cgi?article=4139&context=etd" target="_blank">
 +
                        Doyle, E. L. (2013). Computational and experimental analysis of TALeffector-DNA binding. Plant Pathology and Microbiology, Iowa State University. <b>Dissertation.</b>
 +
                    </a>
 +
                </li>
 +
                <li>
 +
                    <a id="Yang" href="https://www.ncbi.nlm.nih.gov/pubmed/29061047" target="_blank">
 +
                        Yang, S., et al. (2018). "Construction and Characterization of Broad-Spectrum Promoters for Synthetic Biology." <u> ACS Synthetic Biology </u> 7(1): 287-291.
 +
                    </a>
 +
                </li>
 +
 
 +
                <a id="Jain" href="https://academic.oup.com/femsle/article/348/2/87/731695" target="_blank">
 +
                    Jain, A. and P. Srivastava (2013). "Broad host range plasmids." <u> FEMS Microbiology Letters </u>348(2): 87-96.
 
                 </a>
 
                 </a>
            </li>
+
                </li>
  
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Revision as of 21:42, 16 October 2019

Sci-Phi 29

Overview

With our modeling we aimed to apply a control systems approach to achieve stability across bacterial species. To make expression host-independent, we proposed to include an incoherent feedforward loop in our design. Our analytical steady-state solution of this loop showed that expression was completely independent of plasmid copy number and transcriptional and translational rates. We verified this analytical solution by the implementation of a full kinetic model.

The key variables in the design of genetic circuits are plasmid copy number and transcriptional and translational rates. These variables play a major role in the steady-state levels of gene expression. However, when transferring genetic circuits between organisms, these variables change in unpredictable ways.

promoter SOBL

Promoters have different strengths in different organisms. Some promoters only work in a very narrow range of bacterial species (Yang, Liu et al. 2018). In order to circumvent host related changes we made our system orthogonal to the host. We do this by using T7 RNA polymerase. Although orthogonal transcription might not behave similarly when applied in varying biological contexts. We show through modeling that this won't influence gene expression levels when using our genetic circuit implementation of an iFFL.


RBS SOBL

Ribosome binding sites contain the Shine-Dalgarno sequence where the 16s rRNA of the ribosome binds. However, this sequence varies across species, and often ribosome binding sites are extremely inefficient when applied in phylogenetically distant species (Salis, et al). Our model shows that similar expression levels across organisms can be maintained when all genes in our genetic circuit contain the same ribosome binding site. However, this is assuming translation elongation is similar in these species. However, translation elongation has been shown to be influenced by codon usage, which differs per organism. We, therefore, developed a software tool that determines a coding sequence similar in codon usage across different species. Similar codon usage minimizes any codon bias, which would cause translation elongation differences.


The core of our design - Incoherent feed forward loop

We implemented an incoherent feedforward loop (iFFL) in a genetic circuit. In an iFFL, the input signal regulates both the activator and the repressor of the output of the system in the same way. The iFFL results in perfect adaptation to the input when the negative regulation is fully uncooperative (Segall, et al. 2018). The input in our case is the copy number of the DNA template, and the output is the steady-state expression of a gene of interest. In our system, we use a transcription activator-like effector (TALE) protein as a repressor. TALE proteins recognize DNA by a simple DNA-binding mechanism (Doyle 2013) and have been shown to bind fully uncooperative (Segall, et al. 2018). The promoter driving the gene of interest has been engineered to contain a binding site of a TALE protein. When the TALE protein is bound to the promoter, the expression of the gene of interest is repressed.

iFFL

Figure 1: Scheme of incoherent Feed Forward Loop.

We have extensively modeled the functioning of the genetic implementation of this system. An analytical steady-state solution of the system showed that the steady-state expression level of a gene of interest is completely independent of plasmid copy number and can be independent transcriptional and translational rates when the right design choices are made. After further verification through the implementation of a full ODE model, we designed experiments to test the independence on these variables. Key design choices were identified by modeling. These consist of:
  • The need for good insulation of the genes.
  • The promoter strength of the TALE protein and the gene of interest need to maintain the same ratio.
  • The ribosome binding site strength of the TALE protein and the gene of interest need to maintain the same ratio.

More detail on how we modeled the output of our system and determined it is independent of copy number, transcriptional and translational variations, and how we came to these design choices can be found in the sections below.


  • The kinetics

      The kinetics

      In this section, we explain the kinetics of our system and derive a system of ordinary differential equations to describe the interactions within the genetic circuit. We will step-wise derive a steady-state solution from the system of equations and describe the properties of the system. In the other sections, we use these properties to describe how we can utilize them to transfer genetic circuits between prokaryotes. The following scheme depicts all interactions considered in our system.

      TALE system

      Figure 2: Scheme of genetic circuit interactions developed by (Segall, et al. (2018))

      From these interactions we can derive the following system of ordinary differential equations:


        ${dm_T \over dt} = {c \cdot a_T - y_m \cdot m_T}$

        $\frac{dT}{dt} = b_T \cdot m_T - y_T \cdot T - n \cdot k_{on}\cdot T^n \cdot P_G + n \cdot k_{off} \cdot P_{G.T}$

        $\frac{dP_G}{dt} = k_{off} \cdot P_{G.T} - n \cdot k_{on} \cdot T^n \cdot P_G + n \cdot y_T \cdot P_{G.T}$

        $\frac{dP_{G.T}}{dt} = n \cdot k_{on} \cdot T^n \cdot P_G - k_{off} \cdot P_{G.T} - n \cdot y_T \cdot P_{G.T} $

        $\frac{dm_G}{dt} = a_{Gmax} \cdot P_G + a_{Gmin} \cdot P_{G.T} - y_m \cdot m_G $

        $\frac{dm_G}{dt} = b_G \cdot m_G - y_G \cdot G $


      Parameter Value Unit Explanation Source
      $a_T$ 1.03 (nM/min) Transcription rate TALE 2018 iGEM Thessaloniki
      $y_m$ log(2)/5 (1/min) degradation rate mRNA Kushwaha and Salis 2015
      $b_T$ 0.44 1/min Translation rate TALE 2018 iGEM Thessaloniki.
      $y_T$ 0.0347 1/min Degradation rate TALE
      n 1 - Cooperativity of binding Segall-Shapiro, Sontag et al.
      $k_{on}$ 9.85 1/(nM*min) Binding of TALE to promoter 2018 iGEM Thessaloniki.
      $k_{off}$ 2.19 1/min Unbinding of TALE to promoter 2018 iGEM Thessaloniki.
      $a_{Gmax}$ 3.78 1/(nM*min) Maximum transcription of GFP 2018 iGEM Thessaloniki
      $a_{Gmin}$ 0 1/(nM*min) Maximum transcription of GFP Segall-Shapiro, Sontag et al.
      $b_G$ 3.65 1/Min Translation rate GFP 2018 iGEM Thessaloniki
      $y_G$ 0.0347 1/min Degradation rate GFP
      $c$ variable Copy number of plasmid -

      Variable Explanation
      $m_T$ mRNA TALE
      T TALE
      $P_G$ Promoter GFP
      $P_G.T$ Promoter GFP with TALE bound
      $m_G$ mRNA GFP
      G GFP

      Simplification of the system

      This system can be simplified by making a few assumptions:

      1. Amount of TALE protein is much larger than binding sites for TALE
      2. TALE binding and unbinding occurs much more rapidly than protein production and degradation
      3. There is negligable expression when the promoter is repressed

      Using these assumptions, we can derive a steady-state solution for this system analytically. This derivation results in the following steady-state solution:

      $$G = \left((\frac{c}{c^n}) (\frac{a_Gb_Gy_T^ny_m^n}{a_Tb_Ty_Gy_m}\right)$$

    • Full derivation


    • According to our analytical solution, the level of the protein of interest only dependents on copy number, and the ratios of transcription and translation rates of the genes in the circuit. In the next sections, we use this steady-state solution to demonstrate how it can be used to transfer genetic circuits between organisms. Furthermore, since this steady-state solution is based on assumptions, we solve the full system of ordinary differential equations in Matlab to validate our assumptions. In each segment, a link to our corresponding wetlab page is given.


  • Copy number independence

      Copy number

      A big factor in every genetic circuit is the copy number of the DNA template. Broad host range plasmids are often used when using different hosts however, they do not guarantee the same copy number in every organism (Jain and Srivastava 2013). In some organisms, it is not common practice to use a plasmid but rather insert into the genome. The need for consistent expression at a wide range of copy number is thus a desirable feature of any synthetic circuit. Our model steady-state solution tells us that when our repressor binding is fully uncooperative, n = 1, we have complete independence of copy number:


      $$G = (\frac{c}{c^n}) (\frac{a_Gb_Gy_T^ny_m^n}{a_Tb_Ty_Gy_m})$$

      This formula is however based on a few assumptions. We, therefore, implemented the full system of ordinary differential equations to validate our assumptions.

      TALE system
      Steady-state GFP production for copy number 1 till 600 (genome integration till high copy number plasmid).
    • Wetlab

      We tested the prediction of copy number independence by implementing the iFFL system, where the output is GFP. We cloned the system in backbones containing different origins of replication. As a control, we also cloned GFP without repression into different backbones with different origins of replication. More info can be found here.

  • Transcriptional variation

      Every promoter might have a different strength when used in different organisms (Yang, Liu et al. 2018). Thus, when using the same promoter in different organisms, you can get unpredictable behavior. Our model steady-state solution tells us that the steady-state expression level of the gene of interest (GOI) is only dependent on the rate of transcription rates of the GOI and TALE.


      $$G = (\frac{c}{c^n}) (\frac{\color{red}a_\color{red}G \color{black} b_Gy_T^ny_m^n}{\color{red}a_\color{red}T \color{black} b_Ty_Gy_m})$$
      This formula is, however, based on a few assumptions. We, therefore, implemented the full system of ordinary differential equations to validate our assumptions. We vary both transcription parameters. We plot the resulting steady-state solutions as a function of these two variables. A line is plotted to indicate the steady-state solutions resulting from a constant ratio in transcription rates. TALE system
      Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the transcription rate of both genes.
    • Wetlab

      We tested the prediction of transcription rate independence when the same ratio in transcription is maintained. We made variations of the system where we change both promoters in the same way. As a control, we also cloned GFP without repression under the control of these same promoters. More info can be found here.

  • Translational variation

      Ribosome binding sites contain the Shine-Dalgarno sequence, where the 16s rRNA of the ribosome binds. However, this sequence varies across species, and often ribosome binding sites are extremely inefficient when applied in phylogenetically distant species (Salis, Mirsky et al. 2009). This adds unpredictability to the gene expression levels of your genetic circuit when used in a different organism. Similarly, as in transcription, our model steady-state solution tells us that the steady-state expression level of the gene of interest (GOI) is only dependent on the rate of translation rates of the GOI and TALE,


      $$G = (\frac{c}{c^n}) (\frac{a_G \color{red}b_\color{red}Gy_T^ny_m^n}{a_T \color{red}b_\color{red}Ty_Gy_m})$$

      To validate our assumptions, we implemented the full system of ordinary differential equations. We vary both translation parameters. We plot the resulting steady-state solutions as a function of these two variables. A line is plotted to indicate the steady-state solutions resulting from a constant ratio in translation rates.

      TALE system
      Steady-state GFP production while translation rates of both TALE and GFP are changed. The line indicates the same ratio in the translation rate of both genes.

      However, translation isn’t only dependent on initiation, translation elongation is dependent on codon usage.

      [text from Osman here]
    • Wetlab

      We tested the prediction of translational rate independence by implementing the iFFL system, where the output is GFP. We made variations of the system where we change both ribosome binding sites in the same way. As a control, we also cloned GFP without repression into under control of these ribosome binding sites. More info can be found here.

References

  1. Salis, H. M., et al. (2009). "Automated design of synthetic ribosome binding sites to control protein expression." Nature Biotechnology 27(10): 946-950.
  2. Segall-Shapiro, T. H., et al. (2018). "Engineered promoters enable constant gene expression at any copy number in bacteria." Nature Biotechnology 36: 352.
  3. Doyle, E. L. (2013). Computational and experimental analysis of TALeffector-DNA binding. Plant Pathology and Microbiology, Iowa State University. Dissertation.
  4. Yang, S., et al. (2018). "Construction and Characterization of Broad-Spectrum Promoters for Synthetic Biology." ACS Synthetic Biology 7(1): 287-291.
  5. Jain, A. and P. Srivastava (2013). "Broad host range plasmids." FEMS Microbiology Letters 348(2): 87-96.