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For modeling of our promoter-RBS combinations we used the given strength of the Anderson promoters (BBa_J23119,BBa_J23100 to BBa_J23110) and the strength of different RBS (BBa_J61100, BBa_B0030, BBa_B0031) to determine an estimate for their absolute strength. | For modeling of our promoter-RBS combinations we used the given strength of the Anderson promoters (BBa_J23119,BBa_J23100 to BBa_J23110) and the strength of different RBS (BBa_J61100, BBa_B0030, BBa_B0031) to determine an estimate for their absolute strength. | ||
<br>Promotor strength * RBS * 300(high value of our Measurment)<br> | <br>Promotor strength * RBS * 300(high value of our Measurment)<br> | ||
− | Prior to the experiments, we modeled the expression strength of different promoter and RBS combinations to create a database for our experiments. Therefore we used the given strength of the Anderson promoters and the strength of the different known RBS to determine and visualize their absolute strength shown in Fig.: | + | Prior to the experiments, we modeled the expression strength of different promoter and RBS combinations to create a database for our experiments. Therefore we used the given strength of the Anderson promoters and the strength of the different known RBS to determine and visualize their absolute strength shown in Fig.: 2. |
When generating these results, we do not only wanted to consider the use of different Anderson promoters, but also analyze the expression strength of different promoters in combinations with different RBS. Especially for our siRNA system, it was interesting to see the difference between inducible and constitutive promoters. | When generating these results, we do not only wanted to consider the use of different Anderson promoters, but also analyze the expression strength of different promoters in combinations with different RBS. Especially for our siRNA system, it was interesting to see the difference between inducible and constitutive promoters. | ||
In addition, we modeled other promoters of the parts registry. | In addition, we modeled other promoters of the parts registry. | ||
</article> | </article> | ||
+ | |||
+ | |||
+ | <figure role="group"> | ||
+ | <img class="figure hundred" src=""> | ||
+ | <figcaption> | ||
+ | <b>Figure 2:</b> Modeling of the Anderson promoter (BBa_J23119,BBa_J23100 to BBa_J23110)in combination with the RBS (BBa_J61100, BBa_B0030, BBa_B0031). | ||
+ | </figcaption> | ||
+ | </figure> | ||
+ | |||
+ | |||
+ | |||
+ | |||
<h2>Characterization</h2> | <h2>Characterization</h2> | ||
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<img class="figure hundred" src=""> | <img class="figure hundred" src=""> | ||
<figcaption> | <figcaption> | ||
− | <b>Figure | + | <b>Figure 3:</b> Possible applications of nanoparticles produced with ferritin. |
</figcaption> | </figcaption> | ||
</figure> | </figure> |
Revision as of 16:51, 17 October 2018
Part Collection
Short Summary
Design
Modeling
Promotor strength * RBS * 300(high value of our Measurment)
Prior to the experiments, we modeled the expression strength of different promoter and RBS combinations to create a database for our experiments. Therefore we used the given strength of the Anderson promoters and the strength of the different known RBS to determine and visualize their absolute strength shown in Fig.: 2. When generating these results, we do not only wanted to consider the use of different Anderson promoters, but also analyze the expression strength of different promoters in combinations with different RBS. Especially for our siRNA system, it was interesting to see the difference between inducible and constitutive promoters. In addition, we modeled other promoters of the parts registry.
Characterization
Results
Outlook
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Köker, T., Fernandez, A., & Pinaud, F. (2018). Characterization of Split Fluorescent Protein Variants and Quantitative Analyses of Their Self-Assembly Process. Scientific reports, 8(1), 5344.
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