Difference between revisions of "Team:ShanghaiTech/Model NFBL"

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     <h2>Negative Feedback Loop</h2>
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     <h2>Negative feedback loop</h2>
 
     <br>
 
     <br>
  
 +
        <br>
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        <h3>Nomination</h3>
 +
        <br>
  
    <h3>Lux</h3>
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    <br>
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        <p>(Listed by the order of article)</p>
 +
        <figure><table class="table">
 +
        <thead>
 +
        <tr><th style='text-align:center;' >Variable</th><th style='text-align:center;' >Mean</th></tr></thead>
 +
        <tbody><tr><td style='text-align:center;' >$LuxR$</td><td style='text-align:center;' >The quantity (copy number) of LuxR gene</td></tr><tr><td style='text-align:center;' >$LuxProtein$</td><td style='text-align:center;' >The quantity (concentration) of LuxR  protein</td></tr><tr><td style='text-align:center;' >$AHL$</td><td style='text-align:center;' >The quantity (concentration) of AHL</td></tr><tr><td style='text-align:center;' >$LuxAHL$</td><td style='text-align:center;' >The quantity (concentration) of the combination  of LuxR protein and AHL</td></tr><tr><td style='text-align:center;' >$pLux$</td><td style='text-align:center;' >The quantity (copy number) of the pLux  gene</td></tr><tr><td style='text-align:center;' >$ActivepLux$</td><td style='text-align:center;' >The quantity (copy number) of pLux  promoter activated by the inducer LuxAHL</td></tr><tr><td style='text-align:center;' >$rate(pLux)$</td><td style='text-align:center;' >The expression rate of pLux</td></tr><tr><td style='text-align:center;' >$k_{pLux}$</td><td style='text-align:center;' >The rate coefficient of the expression  equation of pLux</td></tr><tr><td style='text-align:center;' >$K_{pLux}$</td><td style='text-align:center;' >A constant in the Hill function of pLux  combined with LuxAHL</td></tr><tr><td style='text-align:center;' >$n_LuxAHL$</td><td style='text-align:center;' >The Hill coefficient of the Hill function  of pLux combined with LuxAHL</td></tr><tr><td style='text-align:center;' >$[LuxAHL]$</td><td style='text-align:center;' >The instantaneous concentration of LuxAHL</td></tr><tr><td style='text-align:center;' >$[AHL]$</td><td style='text-align:center;' >The instantaneous concentration of AHL</td></tr><tr><td style='text-align:center;' >$k$</td><td style='text-align:center;' >A constant in the equation of producing  LuxAHL from AHL</td></tr><tr><td style='text-align:center;' >$TotalpLux$</td><td style='text-align:center;' >The total quantity (copy number) of pLux</td></tr><tr><td style='text-align:center;' >$n_{AHL}$</td><td style='text-align:center;' >The Hill coefficient of the Hill function  of the expression rate of pLux determined by AHL</td></tr><tr><td style='text-align:center;' >$rate(downstream)$</td><td style='text-align:center;' >The expression rate of downstream gene</td></tr><tr><td style='text-align:center;' >$k_{downstream}$</td><td style='text-align:center;' >A constant in the equation of activating  the downstream expression by the upstream product</td></tr><tr><td style='text-align:center;' >$ConnectionRatio$</td><td style='text-align:center;' >The connection ratio of the promoter with  the relative inducer</td></tr><tr><td style='text-align:center;' >$T$</td><td style='text-align:center;' >Total quantity (copy number) of the  promoter</td></tr><tr><td style='text-align:center;' >$upstream$</td><td style='text-align:center;' >The quantity (concentration) of upstream  product</td></tr><tr><td style='text-align:center;' >$n_{upstream}$</td><td style='text-align:center;' >The Hill coefficient of the Hill function  of the upstream product activating the downstream expression</td></tr><tr><td style='text-align:center;' >$K_{downstream}$</td><td style='text-align:center;' >A constant in the Hill function of the  upstream product activating the downstream expression</td></tr><tr><td style='text-align:center;' >$T’$</td><td style='text-align:center;' >A combined constant in the Hill function  of the upstream product activating the downstream expression</td></tr></tbody>
 +
        </table></figure>
 +
        <p> </p>
  
    <p>The Lux module is the input signal controller of our Negative Feedback Loop (NFBL) as the part A. In our project, we utilized quorum sensing systems sensing part as the signal sensor of the Module, this allows downstream gene expression to be able operated by external signal. We have examined four quorum sensing systems (Lux, Tra, Rhl, Rpa) and finally chose the Lux as our manipulate part of our module.</p>
 
    <p> <strong>Key Achievements</strong></p>
 
    <ul>
 
      <li><p>Construct Lux, Tra, Rhl, Rpa quorum sensing system</p></li>
 
      <li><p>Evaluation for each quorum sensing system</p></li>
 
    </ul>
 
    <h4>Overview</h4>
 
    <p>Quorum sensing is a natural occurring mechanism that certain strains of bacteria use to regulate gene expression in response to their population density. As quorum response proteins be translated, signaling molecules such as N-acyl homoserine lactones or AHLs could bind transcription factors and activate downstream gene expression as well the cell’s growth.</p>
 
    <p>In our project, quorum sensing response genes were connected to receptors from other modules, and associated AHLs were added to control downstream gene expression. We have examined four quorum sensing systems (Lux, Tra, Rhl, Rpa) to evaluate weather each quorum sensing system is suitable for our Negative Feedback Loop (NFBL) or not. </p>
 
    <p>Through experiments, Lux show advantages in its robustness and sensitivity, including:</p>
 
    <ul>
 
      <li><p>Lower background leakage: Downstream expression perform very low when associate AHL was note added.</p></li>
 
      <li><p>High sensitivity: Only very little amount of associate AHL were needed to activate downstream expression.</p></li>
 
      <li><p>Stable expression: Downstream gene expression performed stable even after 8 hours after adding associate AHL.</p></li>
 
    </ul>
 
    <p>According to Lux’s outstanding performance its sensitivity and robustness, we chose the Lux quorum system to control module A. </p>
 
    <p> </p>
 
    <h4>Our Approach</h4>
 
    <p>The first node of our three-node negative feedback loop, was controlled by the Lux quorum sensing system and the repressive RNA switch pT181 from module C, which was designed as “pCon(J23100) + pT181 Target + RBS(BBa_B0034) + LuxR + TER(BBa_B0015)”.</p>
 
    <p>We believe that, as pT181 RNA switch is open, the Lux transcriptional activator, LuxR, is translated. With the induction of exogenous AHL, LuxR will combine with AHL molecules and activate the Lux transcriptional promoter, pLux, and lead downstream gene expression.</p>
 
    <p>In the absence of AHL, the pLux promoter will not be activated, which means the system keeps off without input signal. When the concentration of AHLs changes, the Lux module start to work, activate the part B. Due to the nice input-output linearization of Lux, the input signal waveform will be well introduced to our system, without being changed.</p>
 
    <h4>Experimental design</h4>
 
    <p>Experiments were carriedout to determine which quorum sensing system should be chosen. We designed different plasmids whom have different Quorum resporter devices and add <em>Aequoria victoria</em> green fluorescent protein at the downstream of Quorum transcriptional promoters to detect the performance of different quorum sensing concentrations. </p>
 
    <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/9/9e/T--ShanghaiTech--lux_figure10.jpg' alt='lux_1'  /></p>
 
    <p class="text-center"><small>Fig.1 &quot;pCon(J23100) + RBS(BBa_B0034) + QuorumR + TER(BBa_B0015) + pQuorum + RBS(BBa_B0034) + GFP + TER(BBa_B0015)&quot;</small></p>
 
    <p> </p>
 
    <p>DH5-α cells whom contains plasmid of constructed resporter devices were cultured to Abs600 0.60 and then transferred to 96-well microplates where they were induced with appropriate AHL concentrations. By measuring the fluorescence output from each of the constructed devices by inducing cell cultures with various concentrations of AHL molecules. The induced cell cultures were grown in the microplates at 37°C and the fluorescence signal were monitored over time by using a microplate reader.</p>
 
    <p>We needed to characterize the response of the construct to different concentrations of AHL so that we could use the data in our model to predict how the system could function. The activation ranges were compared between the quorum sensing systems in order to determine their robustness, sensitivity, stability and if it is suitable to be used in our Negative Feedback Loop.</p>
 
    <h4>Results</h4>
 
    <p>Through experiments, concentration ranges of AHLs required for activation in each quorum sensing system were calculated to be 100nM-10uM for Rhl and 100pM-10nM for Lux, Tra, Rpa. Rhl were found to differ by a 1,000-fold sensitive difference than other quorum sensing systems, which meas Lux, Tra, Rpa has higher sensitivity.</p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 80%" src='https://static.igem.org/mediawiki/2018/7/79/T--ShanghaiTech--lux_figure11.jpg' alt='lux_2'  /></p>
 
    <p class="text-center"><small>Fig.2  LuxR-AHL Fluorescence 485-535 absorbance related to time.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 80%" src='https://static.igem.org/mediawiki/2018/8/8d/T--ShanghaiTech--lux_figure12.jpg' alt='lux_3'  /></p>
 
    <p class="text-center"><small>Fig.3  RpaR-AHL Fluorescence 485-535 absorbance related to time.</small></p>
 
    <p>Compared between different quorum sensing systems, the Lux quorum sensing systems has lower background leak, higher orthogonality and robustness and better expression stability. Therefore, we choose Lux quorum sensing systems as the input signal controller for module A.</p>
 
    <h3>STAR</h3>
 
    <br>
 
    <p>Small transcription activating RNA (STAR) is the part B of our feedback loop (NFBL), which works as a buffer in our three-node feedback loop. STAR is a significant switch which determines whether the gene of interest downstream could be expressed or not. With the presence of STAR, the target gene will be activated due to the combination of it with the terminator RNA upstream the gene of interest. While the target gene is inhibited without STAR. STAR is a good part as small RNA to construct synthetic gene networks that precisely control gene expression.</p>
 
    <p><strong>Key achievements</strong></p>
 
    <p>Characterization of STAR-mediated target gene activation over a period of time. </p>
 
    <h4>Overview</h4>
 
    <p>As the Three-node Negative Feedback Loop is needed for the precise control of the transcriptional level, a buffer is necessary to be the upstream of the target gene. STAR is chosen to play that role.</p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/6/62/T--ShanghaiTech--star.png' alt='STAR'  /></p>
 
    <p>The STAR contains a terminator and a STAR antisense. </p>
 
    <p>The terminator resides in the 5΄ untranslated region of the target gene. In the absence of the STAR antisense, the terminator will be allowed to form, which will prevent the transcription of the target gene.</p>
 
    <p>With STAR antisense present, it will anneal with the 5’ region of the terminator stem, which will prevent the formation of the terminator. In this way, the RNA polymerase is able to start transcribe.</p>
 
    <p>There are obvious advantages for introducing STAR into our system, including:</p>
 
    <ul>
 
      <li><p>Low metabolic burden: Compared to the universal protein-based regulatory systems, STAR dispense with translation step as a RNA regulator, which saves a great amount of resources.</p></li>
 
      <li><p>High efficiency: The presence of STAR produces an expression of the downstream gene whose activation is 100-fold compared with the condition when STAR is absent, which provides the efficiency and validity.</p></li>
 
      <li><p>Fast response: STAR acts quickly when receiving signal molecules and causes little delay in the circuit because of rapid RNA degradation.</p></li>
 
    </ul>
 
    <h4>Our approach</h4>
 
    <p>STAR is the part B in our negative feedback loop. With the existence of the part B, which works as a buffer in our system, our three-node feedback loop will show higher fidelity than the simple two-node feedback loop.</p>
 
    <p>STAR will be activated by part A, since it is regulated by the Lac I promoter. Meanwhile, STAR will upregulate the expression of part C since the terminator part of the STAR, which will be regulated by the STAR antisense is upstream the gene for part C. Consequently, the upregulation of part A caused by the input signal will indirectly activate part C with the help of the buffer - STAR. In this case, the whole system is ready to response change of the input signal.</p>
 
    <p>After the input is introduced into the system, we want the following parts response fast to the signal. Since STAR shows fast response due to the lack of translation step and rapid RNA degradation, it is the appropriate choice for the part B. </p>
 
    <p>In the absence of input signal, the system is expected to be shut down. However, the leak is inevitable in all the control systems. But it seems to be harmless as the STAR shows activation about 100-fold. It will also be reduced by the pT181 attenuator, which will be mentioned in the part C.</p>
 
    <p>When the input signal is introduced into the system by the part A, STAR will send it to both the regulator- the part C – and the output downstream it due to the fast response mentioned before. In this case, the high efficiency of the activation of STAR, the signal attenuation will be reduced at utmost.</p>
 
    <p>In brief, the STAR can help our system respond to the input with high-fidelity in a fast way.</p>
 
    <h4>Experimental design</h4>
 
    <p>The experiments on STAR can be generalized into two parts. Almost all the experience about STAR are operated under 20-25 degrees Celsius. Streptomycin medium has been used to cultivate bacteria in need. We mainly use plate reader and fluorescence microscope to get results of how STAR has been working. Massive data about corresponding bacterial density and fluorescence intensity have been detected every experience and have been compared(FL/ABS) in order to analyze the variation of fluorescence intensity of a single bacterium.</p>
 
    <p>We really appreciate the precious gift from SJTU, which is the STAR plasmid conduct by Imperial College in 2016 from SJTU. The plasmid consists of a STAR target upstream of a superfolderGFP with a RBS(BBa_B0034) and a terminator(t500) under control of a constitutive promoter (J23119). We transformed it into DH5-α <em>E.coli</em> cells.</p>
 
    <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/0/06/T--ShanghaiTech--star4.png' alt='star_4'  /></p>
 
    <p class="text-center"><small>Fig.4 STAR plasmid form Imperial College pCon(J23119) + STAR.Target1 + RBS(BBa_B0034) + superfolderGFP + Terminator(t500)</small></p>
 
    <p>Firstly, two different types of cells that contain different GFP (SFGFP as enhanced group and generic GFP as control group) were cultivated and examined using plate reader and fluorescence microscope, from this part of the experiment we wanted to verify the effectiveness of GFP in part B in order to make sure that it could express well in our system later. Additionally, by comparing the light intensity of different types of GFP, part B would be proved to be sensitive to embody its working status, which is helpful for our system to handle the upstream information, also convenient when manipulators want to analyze the situation of system. </p>
 
    <p>The second part was designed to measure the growth and green fluorescence of cells under time span, in order to coordinate with data and curve from other parts in our experiment, the graph we drew based on collected data would help us find out the characteristic and change of expression of STAR during a long period. Then FL/ABS is calculated likewise to give a clear expression of how the expression of a single bacterium varies from 0 to 15h.</p>
 
    <h4>Result</h4>
 
    <p>By analyzing these graphs below, the result shows that the GFP used in part B is an enhanced GFP which intensity is nearly 10 times as the control group, which proves to be greatly sensitive. Meanwhile, this experiment proved part B works and creates a brighter image when observing under fluorescence microscope.</p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/9/9f/T--ShanghaiTech--star5.png' alt='star_5'  /></p>
 
    <p class="text-center"><small>Fig.5 The quantity of four different types of GFP (enhanced, control) at 15 hours,
 
    which is shown to approach the same level.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/1/15/T--ShanghaiTech--star6.png' alt='star_6'  /></p>
 
    <p class="text-center"><small>Fig.6 The quantity of four different types of GFP (enhanced, control) at 15 hours,
 
    which is shown to approach the same level.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/c/c6/T--ShanghaiTech--star7.png' alt='star_7'  /></p>
 
    <p class="text-center"><small>Fig.7 The logarithmic form of fluorescence intensity divided by cell density respectively for STAR1, STAR2, Blank group at 15 hours.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 50%" src='https://static.igem.org/mediawiki/2018/6/6a/T--ShanghaiTech--star8.png' alt='star_8'  /></p>
 
    <p class="text-center"><small>Fig.8 100x image of STAR1 under fluorescence microscope.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 50%" src='https://static.igem.org/mediawiki/2018/3/35/T--ShanghaiTech--star9.png' alt='star_9'  /></p>
 
    <p class="text-center"><small>Fig.9 100x image of STAR1 under fluorescence microscope.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 50%" src='https://static.igem.org/mediawiki/2018/4/4e/T--ShanghaiTech--star10.png' alt='star_10'  /></p>
 
    <p class="text-center"><small>Fig.10 100x image of STAR1 under fluorescence microscope.</small></p>
 
    <p>Plus, how STAR works according to time can be seen from the graphs below.</p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/3/3e/T--ShanghaiTech--star11.png' alt='star_11'  /></p>
 
    <p class="text-center"><small>Fig.11 Bacterial density of STAR used in part B. The growth shows a steady increase from 0 to about 11h, then the numerical result fluctuates at approximately 1.04.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/b/b9/T--ShanghaiTech--star12.png' alt='star_12'  /></p>
 
    <p class="text-center"><small>Fig.12 The expression quantity of STAR varies with time and stabilizes at about 15 hours.</small></p>
 
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/4/40/T--ShanghaiTech--star13.png' alt='star_13'  /></p>
 
    <p class="text-center"><small>Fig.13 The ration of Fluorescence intensity divided by cell density. The curve first decreases sharply and then increases slowly, eventually stabilizes at about 15h.</small></p>
 
    <p> </p>
 
    <p><strong>Reference</strong>: A network of orthogonal ribosome·mRNA pairs, Oliver Rackham ; Jason W Chin, Nature Chemical Biology, 2005, Vol.1(3), p.159</p>
 
    <p>&nbsp;</p>
 
  
    <br>
 
    <h3>pT181</h3>
 
    <br>
 
  
    <p>The Repressive RNA Switch pT181 attenuator is the extra regulator of our Negative Feedback Loop (NFBL). We are utilizing pT181 attenuator – a dual control repressors – to regulate both gene transcription and translation in a fast and robust way. We have submitted it as our improved part since it increases repression from 84% to 98% compared with that of Kyoto 2013 submitted. As RNA transcriptional regulators are emerging as versatile components for genetic network construction, we believe that improving the part in this library is essential for advancing synthetic biology. We hope our improvement of pT181 attenuator to iGEM parts will encourage future teams to implement this versatile, highly orthogonal, and effective regulator in their circuits.  </p>
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        <br>
    <p><strong>Key achievements</strong></p>
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        <h3>Basic Assumptions</h3>
    <ul>
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        <br>
      <li><p>Characterization of pT181 attenuator  -mediated target gene activation in various conditions.</p></li>
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      <li><p>Improvement of a new sense target sequence of pT181 attenuator.</p></li>
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      <li><p>Update of the BioBrick Registry library by improving a RNA-logic toolset.</p></li>
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        <ol start='' >
    </ul>
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        <li>Our designed system is independent from other known and unknown factors. This means we can only focus on the properties of the target system to evaluate the features without the disturbance of other factors.</li>
    <h4>Overview</h4>
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        <li>Only the reactions of DNA transcripts to mRNA and mRNA translated to protein need time, the other reactions are regarded as fast reactions and will finish within no time. Among the reactions we care In <em>E. coli</em>, only the reactions of transcription and translation are chain reaction. Thus, all the other reactions finished in one step or few steps can be regarded as fast reactions and take no time to finish.</li>
    <p>Our engineered cells need a Three-Node Negative Feedback Loop to construct a more sensitive and high-fidelity control system. And pT181 attenuator is the part that plays the role of repressor in this loop.</p>
+
        </ol>
    <p>pT181 attenuator is a part composed of a sense target sequence and an antisense RNA that can regulate gene transcription and translation. Residing in the 5΄ untranslated region of the target gene, it can regulate the expression of a downstream gene at both transcriptional and translational levels.</p>
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    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/e/ed/T--ShanghaiTech--pt181.png' alt='pT181'  /></p>
+
 
    <p class="text-center"><small>Fig.14 A schematic representation of the pT181 attenuator in action</small></p>
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        <br>
    <p>At transcriptional level, the anti-terminator, which is a part of the sense target sequence will anneal with the 5’ region of the terminator stem without antisense RNA. In this case, the terminator could not format, which means the RNA polymerase can start transcribe. At translational level, in the absence of antisense RNA, a ribosome binding site (RBS) for the gene of interesting is exposed, so that the ribosome could bind to it to begin translation.</p>
+
        <h3>Transcription Layer</h3>
    <p>While the antisense RNA is present, the formation of terminator will be allowed as the anti-terminator is sequestered due to the kissing hairpin interaction between the antisense RNA and the sense target sequence. In this way, the downstream transcription will be prevented. As for the translational level, the occlusion of the RBS by the terminator hairpin will prevent the translation of the target gene. </p>
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        <br>
    <p>In conclusion, while antisense RNA is not present, the gene will express as normal, while antisense RNA is produced, the downstream target gene will be repressed effectively.</p>
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    <p>The RNA regulators show sufficient advantages over traditional protein-based regulatory systems, including:</p>
+
 
    <ul>
+
        <p><strong>Equations for transcription layer</strong></p>
      <li><p>Programmability: As Watson-Crick base pairing is predictable, the RNA-RNA interaction can be predicted by sophisticated software tools. In this way, a RNA switch can be designed artificially, which are difficult for proteins.</p></li>
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        <p>Our project started at dealing with the unexpected reaction of A bio-system. we knew that control theory could be a solution to this problem by intensive studies. As long as we inspired by this powerful theory in the field of mathematics and signal manipulation, we built the initial simple model to describe the system in <em>E. coli</em>. </p>
      <li><p>Lower metabolic cost: Compared with proteins, the RNA switches dispense with translation step, which saves a great amount of resources.</p></li>
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        <p>We studied the gene transcription in the loop, and found that Hill function was a best tool to describe the dynamic reactions in the system. For example, in part Lux, LuxR protein combines with AHL and reacts to LuxAHL. LuxAHL then connects to the promoter pLux as an inducer. After the inducer and the promoter have connected, the downstream expression starts. The expression rate of downstream gene is determined by the connection ratio of pLux and LuxAHL.</p>
      <li><p>Fast response: RNA switches could propagate signals faster than proteins considering the fast degradation rates of RNAs.</p></li>
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        <p> </p>
    </ul>
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        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/a/ac/T--ShanghaiTech--7_LuxR.png"/></p>
    <p>Despite these advantages, RNA regulators still suffer from incomplete repression in their OFF state, making the dynamic range less than that of the proteins. This leak can cause the network to function incorrectly. Therefore, we submit the dual-control pT181 attenuator, which can solve this problem. </p>
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        <p class="text-center"><small>LuxR mechanism</small></p>
    <p>The dual-control pT181 attenuator we submitted offers a significant advantage over previous iGEM parts that submitted in 2013:</p>
+
        <p>$$ LuxR \rightarrow LuxProtein\ \ \ (1)$$</p>
    <ul>
+
        <p>$$ LuxProtein + AHL \rightarrow LuxAHL\ \ \ (2)$$</p>
      <li><p>Reduce leak: As our pT181 attenuator could regulate both transcription and translation in a single compact RNA mechanism, which means it could provide stronger functions without increasing burden. This dual control repressor is able to increases repression from 85% to 98%.</p></li>
+
        <p>$$ LuxAHL + pLux \rightarrow ActivepLux\ \ \ (3)$$</p>
    </ul>
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        <p>$$ \frac{ActivepLux}{pLux+ActivepLux} = BondingRate$$</p>
    <p>&nbsp;</p>
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        <p>$$ rate(pLux)=k_{pLux}\cdot ActivepLux $$</p>
    <h4>Our approach</h4>
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        <p>$$ BongdingRate = \frac{LuxAHL^{n_{LuxAHL}}}{K_{pLux}+LuxAHL^{n_{LuxAHL}}} $$    (Hill function)</p>
    <p>pT181 attenuator is the part C in our negative feedback loop. As the regulator in our system, pT181 attenuator will be activated by part B, since we place part B’s target sequence upstream the gene for pT181 attenuator antisense. Meanwhile, pT181 attenuator will repress the part A due to the pT181 attenuator sense target upstream the gene for part A. Consequently, the upregulation of part B caused by the expression of part A will indirectly repress part A. In this case, the whole system is ready to response change of the input signal.</p>
+
        <p>The above equations describe the principle of the activation of pLux by LuxR and AHL. The first three equations ((1) and (2)) can be written in one total equation which is $LuxR + AHL \rightarrow LuxAHL$. Considering the quantity of LuxR in a mature <em>E. coli</em> is fixed, the quantity of active pLux only determined by the quantity of AHL when the total reaction is a fast reaction. Actually, compared to the rate of gene transcription, this reaction could be approximated as a fast reaction. Hence, we reach the equation $[LuxAHL]=k\cdot [AHL]$. Then, rewriting $pLux + ActivepLux = TotalpLux$, the Hill function describing part Lux can be derived (The coefficients has been integrated into the simplest form).</p>
    <p>In the absence of input signal, we hope that there is no expression of the output. However, due to the inevitable leak from the part A and part B, it seems to be impossible to avoid expression of the output. With pT181 attenuator in our system, we could avert it at utmost because of the efficient repression of it – just tiny quantity of pT181 attenuator will prevent most of the leak. This ensures the minimum expression of the output without input signal.</p>
+
        <p>$$rate(pLux)=TotalpLux\cdot \frac{AHL^{n_{AHL}}}{K_{pLux}+AHL^{n_{AHL}}}$$</p>
    <p>When the input signal is present, it will induce the expression of part A, which will upregulate the part B a lot. In this way, the output will be strongly expressed. But the upregulation of part B would cause the expression of pT181 attenuator, which will repress the part A. And this will cause the low expression of part A and indirect low expression of part B. Although the remains in the environment would keep the amount of output, the low quantity of each part of the system will prepare it for any change from the input signal. In this case, the output of the system would response to the change of the input in a very short time. This can also eliminate the possible superposition between outputs from different input signals.</p>
+
        <p>Now, it has been proved that for part Lux, the expression rate of downstream can be described by the Hill function of upstream product. In fact, because of the rate of downstream expression always determined by the connection ratio of inducer and promoter, the rate can mostly be described by the Hill function in the above form as long as the reaction of upstream expression is relatively a fast reaction. </p>
    <p>We used our model to predict whether the high repression effect of pT181 attenuator will cause the silence of the output, as it may cause the silence of part A. However, our model shows that the output will respond to the input perfectly, which support our experiment a lot.</p>
+
        <p>In our model, we assumed all the reaction of upstream expression are fast reactions, then all the expression rate in the transcription layer can be described as Hill function. It is necessary to notice that, if the downstream expression is repressed by the upstream, the rate of downstream expression equation is</p>
    <p>In conclusion, the presence of pT181 attenuator will reduce leak of our system at utmost, as well as allow it to rapidly respond to the changing signal.</p>
+
        <p>$$ rate(downstream)=k_{downstream}\cdot (1-ConnectionRatio) $$</p>
    <p> </p>
+
        <p>And we rewrite the downstream expression rate</p>
    <h4>Experimental design</h4>
+
        <p>$$ rate(downstream)=T\cdot(1-\frac{upstream^{n_{upstream}}}{K_{downstream}+upstream^{n_{upstream}}}) $$</p>
    <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/c/c1/T--ShanghaiTech--pt181_15.png' alt='pT181_15'  /></p>
+
        <p>$$ rate(downstream)=T'\cdot\frac{1}{K_{downstream}+upstream^{n_{upstream}}}$$</p>
    <p class="text-center"><small>Fig.15  A schematic representation of the experimental group plasmid. This has the basic
+
        <p>$$ T' = T\cdot K_{downstream} $$</p>
    pT181 attenuator Antisense under control of a constitutive promoter, as well as
+
        <p>Hence, the Hill function is a really great tool for transcription layer.</p>
    a GFP gene downstream of the pT181 attenuator sense target under the control of
+
        <p> </p>
    a constitutive promoter.</small></p>
+
        <p><strong>Choose a pattern</strong></p>
    <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/7/72/T--ShanghaiTech--pt181_16.png' alt='pT181_16'  /></p>
+
        <p>The result of the first model helped us to confirm our idea that control theory can be used to make the output what we want. Then we want to find out whether the first loop is the best one to have high fidelity. We use model to calculate the feature of three systems. The first system is a two-node feedback loop that the output is directly relative to the input signal and has a direct negative feedback to the start node. </p>
    <p class="text-center"><small>Fig.16  A schematic representation of the positive control plasmid with the GFP gene downstream of the pT181 attenuator sense target under the control of a constitutive promoter, without a pT181 attenuator Antisense on it.</small></p>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/7/75/T--ShanghaiTech--9_2Nodes-07.png"/></p>
    <p>We generated two plasmids, one is for experimental group, the other is for a positive control. The experimental plasmid, which is the pT181 attenuator in this experience, contains the antisense sequence downstream of a constitutive promoter and followed by a double terminator on a high-copy plasmid. Meanwhile, there are also a GFP gene with a ribosome binding site downstream of the pT181 attenuator sense target sequence. The GFP coding sequence is also downstream of a constitutive promoter and followed by a double terminator. The positive control plasmid, which is the blank in this experience, contains the same as the experimental plasmid except for the antisense sequence. </p>
+
        <p class="text-center"><small>system 2-1</small></p>
    <p>We did a group of pT181 attenuator expression experiments. First, as a part that needs to show strong inhibition, we should ensure that its inhibitory effect is obvious enough. Therefore, we compared experimental group and positive control group, which is transformed into a normal GFP plasmid. Depending on the GFP expression, we can prove that our work has a high credibility. Additionally, in the group above, three types of flora from Interlab are cultivated for contrast. The aim is to compare the statistics of pT181 attenuator and verified Interlab to find out which repressor level pT181 attenuator is in when put into practical application. </p>
+
        <p>The second system is a three-node feedback loop that the output is directly relative to the input signal and has an indirect negative feedback to the start node. </p>
    <p>For this group, we transform different plasmids into the <em>E. coli</em> in the tubes and cultivate for hours (37℃, 220RPM). Then we used ELISA plate to detect the change of fluorescence and OD600 over time. What should be noticed is that we set the original flora at OD600=0.05 to guarantee flora proliferating at the same concentration. As the repression of pT181 attenuator attenuator is so powerful that the fluorescence of the experimental group is hard to detect. As a result, to remove LB medium’s fluorescence background, we centrifuge fluid, take out supernatant, add PBS buffer and resuspend before detect.  </p>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/c/c8/T--ShanghaiTech--9_3Nodes-1.png"/></p>
    <h4>Result</h4>
+
        <p class="text-center"><small>system 3-1</small></p>
    <p>The form showed in figure 21 tells that the expression of GFP is greatly decreased in the presence of pT181 attenuator of 18 hours of culturing. The data from figure 19 shows that the pT181 attenuator is not harmful to the cells. The data suggests that pT181 attenuator is a promising tool for the regulator part in our Three-Node Feedback Loop.</p>
+
        <p>The third system is a three-node system that the output is indirectly relative to the input signal and has a direct negative feedback to the start node. </p>
    <p><img class="img-fluid mx-auto d-block" style="width: 50%" src='https://static.igem.org/mediawiki/2018/f/f5/T--ShanghaiTech--pt181_17.png' alt='pT181_17'  /></p>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/f/fc/T--ShanghaiTech--8_3Nodes-2-09.png"/></p>
    <p class="text-center"><small>Fig.17  400x image of positive control under fluorescence microscope.</small></p>
+
        <p class="text-center"><small>system 3-2</small></p>
    <p><img class="img-fluid mx-auto d-block" style="width: 50%" src='https://static.igem.org/mediawiki/2018/8/8b/T--ShanghaiTech--pt181_18.png' alt='pT181_18'  /></p>
+
        <p>Except for these three systems, there are other four three-node systems and one two-node system. However, they do not satisfy our requirement. We would like a system that input promotes the expression of output, and output represses the expression of input to keep the whole system stable. The remain two-node system and two of the remain three-node systems just have the opposite function. In these three systems, the output signal is repressed by the input signal. Because the output signal will only be produced under the active of input signal, and the input signal will negatively influence the producing output signal, the output will never raise up.</p>
    <p class="text-center"><small>Fig.18  400x image of experimental group under fluorescence microscope.</small></p>
+
        <p> </p>
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/1/14/T--ShanghaiTech--pt181_19.png' alt='pT181_19'  /></p>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/1/1f/T--ShanghaiTech--5_badsys-10.png"/></p>
    <p class="text-center"><small>Fig.19 Characterization of pT181 attenuator in DH5-α <em>E.coli</em> cells. OD600 monitored over time for cell lines
+
        <p class="text-center"><small>system 2-2</small></p>
    incorporating the pT181 attenuator in the absence or presence of the pT181 antisense. The result shows that the pT181 antisense is not harmful to the <em>E.coli</em>, which provides convenience for test for fluorescence as we do not need to normalize the OD600.</small></p>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/b/bf/T--ShanghaiTech--0_badsys-11.png"/></p>
    <div class="row">
+
        <p class="text-center"><small>system 3-3</small></p>
      <div class="col-4">
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/4/44/T--ShanghaiTech--7_badsys-12.png"/></p>
        <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/a/ae/T--ShanghaiTech--pt181_20A.png' alt='pT181_20A'  /></p>
+
        <p class="text-center"><small>system 3-4</small></p>
      </div>
+
        <p>The other two three-node systems are the systems that the regulator node is directly repressed by the upstream node. In these two patterns, the quantity of the regulator is also nearly zero for the same reason as the above three bad systems. Thus, these two systems will work like the two-node systems.</p>
      <div class="col-4">
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/c/c2/T--ShanghaiTech--8_badsys-13.png"/></p>
        <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/e/e3/T--ShanghaiTech--pt181_20B.png' alt='pT181_20B'  /></p>
+
        <p class="text-center"><small>system 3-5</small></p>
      </div>
+
        <p><img class="img-fluid mx-auto d-block" style="width: 50%" src="https://static.igem.org/mediawiki/2018/b/b4/T--ShanghaiTech--3_badsys-14.png"/></p>
      <div class="col-4">
+
        <p class="text-center"><small>system 3-6</small></p>
        <p><img class="img-fluid mx-auto d-block" src='https://static.igem.org/mediawiki/2018/3/3e/T--ShanghaiTech--pt181_20C.png' alt='pT181_20C'  /></p>
+
        <p>Now we can see that among the total 8 systems of two- or three- node, only three of them are valuable for our project. </p>
      </div>
+
        <p> </p>
    </div>
+
        <p>In order to evaluate the effectiveness of the valuable three systems, we used error function.</p>
    <p class="text-center"><small>Fig.20 Characterization of pT181 attenuator in DH5-α <em>E.coli</em> cells. The figures show the fluorescence for cells with or without pT181 antisense. (a) Fluorescence monitored over time for cell lines incorporating the pT181 system with pT181 antisense. It shows that the GFP can be expressed in the pT181-attenuator, and the expression level increases gradually. (b) Fluorescence monitored over time for cell lines incorporating
+
        <p>$$ Err = \sum_{i=1}^N([SystemOutputSequence]_i-[ExpectOutputSequnce]_i)^2 $$</p>
    the pT181 system without pT181 antisense. It matches the curve of how GFP’s expression increases without being repressed, which establishes foundation for measure the repression effect of pT181-attenuator. (c) The combination of (1) and (2). We could see the sharp difference in the fluorescence between the two
+
        <p>The <em>System Output Sequence</em> is the normalized output sequence of the given system, and the <em>Expect Output Sequence</em> is the normalized expected output. This equation calculates the difference sequence between these two sequences and get the quadratic sum of the difference sequence. The system will work better when the Err becomes smaller. </p>
    curves. This proves our pT181 could repress the expression of GFP as expected, which means our part C is able to produces repression effect as anticipated. This shows that the controller in our Three-Node Feedback Loop is constructed successfully.</small></p>
+
        <p>Then, we used ordinary differential equations (ODE) to get the output sequence of these systems. </p>
    <p><img class="img-fluid mx-auto d-block" style="width: 60%" src='https://static.igem.org/mediawiki/2018/5/54/T--ShanghaiTech--pt181_21.png' alt='pT181_21'  /></p>
+
        <p> </p>
    <p class="text-center"><small>Fig.21 Characterization of pT181 attenuator in DH5-α <em>E.coli</em> cells. endpoint fluorescence (18 hours) for cell lines in the absence or presence of Pt181. The data shows that our Pt181 attenuator could repress the target gene for 98%.</small></p>
+
        <p>For System 2</p>
    <p><strong>Reference</strong>: Achieving large dynamic range control of gene expression with a compact RNA transcription-translation regulator, Westbrook, Alexandra M ; Lucks, Julius B, Nucleic acids research, 19 May 2017, Vol.45(9), pp.5614-5624</p>
+
        <p>$$ \frac{dO}{dt} = C_{Input}\cdot \frac{I^{n_I}}{k_{Input}+I^{n_I}}-d_O\cdot O $$</p>
    <p>&nbsp;</p>
+
        <p>$$ \frac{dI}{dt}=C_{Inducer\cdot O}\cdot\frac{Inducer^{n_{Inducer}}}{k_{Inducer}+I^{n_{Inducer}}}\cdot \frac{1}{k_O+O^{n_O}} $$ </p>
    <p> </p>
+
        <p>For System 3-1</p>
 +
        <p>$$ \frac{dI}{dt}=C_{Inducer \cdot R}\cdot \frac{Inducer^{n_{Inducer}}}{k_{Inducer}+Inducer^{n_{Inducer}}} \cdot \frac{1}{k_{R}+R^{n_R}}-d_I \cdot I$$  </p>
 +
        <p>$$ \frac{dO}{dt}=C_{I} \cdot \frac{I^{n_I}}{k_I+I^{n_I}}-d_O \cdot O$$            </p>
 +
        <p>$$ \frac{dR}{dt}=C_O \cdot \frac{O^{n_O}}{k_O+O^{n_O}}-d_R \cdot R$$            </p>
 +
        <p>&nbsp;</p>
 +
        <p>For System 3-2</p>
 +
        <p>$$ \frac{dI}{dt}=C_{Inducer \cdot R}\cdot \frac{Inducer^{n_{Inducer}}}{k_{Inducer}+Inducer^{n_{Inducer}}} \cdot \frac{1}{k_{R}+R^{n_R}}-d_I \cdot I$$  </p>
 +
        <p>$$ \frac{dR}{dt}=C_{I} \cdot \frac{I^{n_I}}{k_I+I^{n_I}}-d_R \cdot R$$            </p>
 +
        <p>$$ \frac{dO}{dt}=C_R \cdot \frac{R^{n_R}}{k_R+R^{n_R}}-d_O \cdot O$$</p>
 +
        <p>                  </p>
 +
        <br>
 +
        <br>
 +
        <div class="row">
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/7/75/T--ShanghaiTech--9_2Nodes-07.png"/></p>
 +
            <p class="text-center"><small>system 2-1</small></p>
 +
          </div>
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/1/1b/T--ShanghaiTech--2_sys2.png"/></p>
 +
            <p class="text-center"><small>system 2-1 result</small></p>
 +
          </div>
 +
        </div>
 +
        <div class="row">
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/c/c8/T--ShanghaiTech--9_3Nodes-1.png"/></p>
 +
            <p class="text-center"><small>system 3-1</small></p>
 +
          </div>
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/3/37/T--ShanghaiTech--6_sys31.png"/></p>
 +
            <p class="text-center"><small>system 3-1 result</small></p>
 +
          </div>
 +
        </div>
 +
        <div class="row">
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/f/fc/T--ShanghaiTech--8_3Nodes-2-09.png"/></p>
 +
            <p class="text-center"><small>system 3-2</small></p>
 +
          </div>
 +
          <div class="col-6">
 +
            <p><img class="img-fluid mx-auto d-block" style="width: 90%" src="https://static.igem.org/mediawiki/2018/5/5a/T--ShanghaiTech--8_sys32.png"/></p>
 +
            <p class="text-center"><small>system 3-2 result</small></p>
 +
          </div>
 +
        </div>
 +
 
 +
        <p>These three figures indicate that three-node negative feedback loops (NFBL) are obviously better than the two-node feedback loop. For the two NFBL systems, we can see the $ Err$ of system 3-2 is much bigger than system 3-1. Thus, we chose system 3-1 as our target system. We use LuxR as the input node, STAR as the output node, and pT181 as the regular node. The system will be started by AHL activating LuxR. The output signal is adhesive to the STAR part.</p>
  
 
   </div>
 
   </div>

Revision as of 02:03, 18 October 2018

ShanghaiTech iGEM

Negative feedback loop



Nomination


(Listed by the order of article)

VariableMean
$LuxR$The quantity (copy number) of LuxR gene
$LuxProtein$The quantity (concentration) of LuxR protein
$AHL$The quantity (concentration) of AHL
$LuxAHL$The quantity (concentration) of the combination of LuxR protein and AHL
$pLux$The quantity (copy number) of the pLux gene
$ActivepLux$The quantity (copy number) of pLux promoter activated by the inducer LuxAHL
$rate(pLux)$The expression rate of pLux
$k_{pLux}$The rate coefficient of the expression equation of pLux
$K_{pLux}$A constant in the Hill function of pLux combined with LuxAHL
$n_LuxAHL$The Hill coefficient of the Hill function of pLux combined with LuxAHL
$[LuxAHL]$The instantaneous concentration of LuxAHL
$[AHL]$The instantaneous concentration of AHL
$k$A constant in the equation of producing LuxAHL from AHL
$TotalpLux$The total quantity (copy number) of pLux
$n_{AHL}$The Hill coefficient of the Hill function of the expression rate of pLux determined by AHL
$rate(downstream)$The expression rate of downstream gene
$k_{downstream}$A constant in the equation of activating the downstream expression by the upstream product
$ConnectionRatio$The connection ratio of the promoter with the relative inducer
$T$Total quantity (copy number) of the promoter
$upstream$The quantity (concentration) of upstream product
$n_{upstream}$The Hill coefficient of the Hill function of the upstream product activating the downstream expression
$K_{downstream}$A constant in the Hill function of the upstream product activating the downstream expression
$T’$A combined constant in the Hill function of the upstream product activating the downstream expression


Basic Assumptions


  1. Our designed system is independent from other known and unknown factors. This means we can only focus on the properties of the target system to evaluate the features without the disturbance of other factors.
  2. Only the reactions of DNA transcripts to mRNA and mRNA translated to protein need time, the other reactions are regarded as fast reactions and will finish within no time. Among the reactions we care In E. coli, only the reactions of transcription and translation are chain reaction. Thus, all the other reactions finished in one step or few steps can be regarded as fast reactions and take no time to finish.

Transcription Layer


Equations for transcription layer

Our project started at dealing with the unexpected reaction of A bio-system. we knew that control theory could be a solution to this problem by intensive studies. As long as we inspired by this powerful theory in the field of mathematics and signal manipulation, we built the initial simple model to describe the system in E. coli.

We studied the gene transcription in the loop, and found that Hill function was a best tool to describe the dynamic reactions in the system. For example, in part Lux, LuxR protein combines with AHL and reacts to LuxAHL. LuxAHL then connects to the promoter pLux as an inducer. After the inducer and the promoter have connected, the downstream expression starts. The expression rate of downstream gene is determined by the connection ratio of pLux and LuxAHL.

LuxR mechanism

$$ LuxR \rightarrow LuxProtein\ \ \ (1)$$

$$ LuxProtein + AHL \rightarrow LuxAHL\ \ \ (2)$$

$$ LuxAHL + pLux \rightarrow ActivepLux\ \ \ (3)$$

$$ \frac{ActivepLux}{pLux+ActivepLux} = BondingRate$$

$$ rate(pLux)=k_{pLux}\cdot ActivepLux $$

$$ BongdingRate = \frac{LuxAHL^{n_{LuxAHL}}}{K_{pLux}+LuxAHL^{n_{LuxAHL}}} $$ (Hill function)

The above equations describe the principle of the activation of pLux by LuxR and AHL. The first three equations ((1) and (2)) can be written in one total equation which is $LuxR + AHL \rightarrow LuxAHL$. Considering the quantity of LuxR in a mature E. coli is fixed, the quantity of active pLux only determined by the quantity of AHL when the total reaction is a fast reaction. Actually, compared to the rate of gene transcription, this reaction could be approximated as a fast reaction. Hence, we reach the equation $[LuxAHL]=k\cdot [AHL]$. Then, rewriting $pLux + ActivepLux = TotalpLux$, the Hill function describing part Lux can be derived (The coefficients has been integrated into the simplest form).

$$rate(pLux)=TotalpLux\cdot \frac{AHL^{n_{AHL}}}{K_{pLux}+AHL^{n_{AHL}}}$$

Now, it has been proved that for part Lux, the expression rate of downstream can be described by the Hill function of upstream product. In fact, because of the rate of downstream expression always determined by the connection ratio of inducer and promoter, the rate can mostly be described by the Hill function in the above form as long as the reaction of upstream expression is relatively a fast reaction.

In our model, we assumed all the reaction of upstream expression are fast reactions, then all the expression rate in the transcription layer can be described as Hill function. It is necessary to notice that, if the downstream expression is repressed by the upstream, the rate of downstream expression equation is

$$ rate(downstream)=k_{downstream}\cdot (1-ConnectionRatio) $$

And we rewrite the downstream expression rate

$$ rate(downstream)=T\cdot(1-\frac{upstream^{n_{upstream}}}{K_{downstream}+upstream^{n_{upstream}}}) $$

$$ rate(downstream)=T'\cdot\frac{1}{K_{downstream}+upstream^{n_{upstream}}}$$

$$ T' = T\cdot K_{downstream} $$

Hence, the Hill function is a really great tool for transcription layer.

Choose a pattern

The result of the first model helped us to confirm our idea that control theory can be used to make the output what we want. Then we want to find out whether the first loop is the best one to have high fidelity. We use model to calculate the feature of three systems. The first system is a two-node feedback loop that the output is directly relative to the input signal and has a direct negative feedback to the start node.

system 2-1

The second system is a three-node feedback loop that the output is directly relative to the input signal and has an indirect negative feedback to the start node.

system 3-1

The third system is a three-node system that the output is indirectly relative to the input signal and has a direct negative feedback to the start node.

system 3-2

Except for these three systems, there are other four three-node systems and one two-node system. However, they do not satisfy our requirement. We would like a system that input promotes the expression of output, and output represses the expression of input to keep the whole system stable. The remain two-node system and two of the remain three-node systems just have the opposite function. In these three systems, the output signal is repressed by the input signal. Because the output signal will only be produced under the active of input signal, and the input signal will negatively influence the producing output signal, the output will never raise up.

system 2-2

system 3-3

system 3-4

The other two three-node systems are the systems that the regulator node is directly repressed by the upstream node. In these two patterns, the quantity of the regulator is also nearly zero for the same reason as the above three bad systems. Thus, these two systems will work like the two-node systems.

system 3-5

system 3-6

Now we can see that among the total 8 systems of two- or three- node, only three of them are valuable for our project.

In order to evaluate the effectiveness of the valuable three systems, we used error function.

$$ Err = \sum_{i=1}^N([SystemOutputSequence]_i-[ExpectOutputSequnce]_i)^2 $$

The System Output Sequence is the normalized output sequence of the given system, and the Expect Output Sequence is the normalized expected output. This equation calculates the difference sequence between these two sequences and get the quadratic sum of the difference sequence. The system will work better when the Err becomes smaller.

Then, we used ordinary differential equations (ODE) to get the output sequence of these systems.

For System 2

$$ \frac{dO}{dt} = C_{Input}\cdot \frac{I^{n_I}}{k_{Input}+I^{n_I}}-d_O\cdot O $$

$$ \frac{dI}{dt}=C_{Inducer\cdot O}\cdot\frac{Inducer^{n_{Inducer}}}{k_{Inducer}+I^{n_{Inducer}}}\cdot \frac{1}{k_O+O^{n_O}} $$

For System 3-1

$$ \frac{dI}{dt}=C_{Inducer \cdot R}\cdot \frac{Inducer^{n_{Inducer}}}{k_{Inducer}+Inducer^{n_{Inducer}}} \cdot \frac{1}{k_{R}+R^{n_R}}-d_I \cdot I$$

$$ \frac{dO}{dt}=C_{I} \cdot \frac{I^{n_I}}{k_I+I^{n_I}}-d_O \cdot O$$

$$ \frac{dR}{dt}=C_O \cdot \frac{O^{n_O}}{k_O+O^{n_O}}-d_R \cdot R$$

 

For System 3-2

$$ \frac{dI}{dt}=C_{Inducer \cdot R}\cdot \frac{Inducer^{n_{Inducer}}}{k_{Inducer}+Inducer^{n_{Inducer}}} \cdot \frac{1}{k_{R}+R^{n_R}}-d_I \cdot I$$

$$ \frac{dR}{dt}=C_{I} \cdot \frac{I^{n_I}}{k_I+I^{n_I}}-d_R \cdot R$$

$$ \frac{dO}{dt}=C_R \cdot \frac{R^{n_R}}{k_R+R^{n_R}}-d_O \cdot O$$



system 2-1

system 2-1 result

system 3-1

system 3-1 result

system 3-2

system 3-2 result

These three figures indicate that three-node negative feedback loops (NFBL) are obviously better than the two-node feedback loop. For the two NFBL systems, we can see the $ Err$ of system 3-2 is much bigger than system 3-1. Thus, we chose system 3-1 as our target system. We use LuxR as the input node, STAR as the output node, and pT181 as the regular node. The system will be started by AHL activating LuxR. The output signal is adhesive to the STAR part.


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