Team:UANL Mty-Mexico/Results
From 2013.igem.org
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<div class="col-md-6">Surprisingly, we obtained different behaviors in clones transformed with the same DNA (figure 4). We identified variations in plasmid copy number as the potential cause of phenotypic discrepancies among clones.</div> | <div class="col-md-6">Surprisingly, we obtained different behaviors in clones transformed with the same DNA (figure 4). We identified variations in plasmid copy number as the potential cause of phenotypic discrepancies among clones.</div> | ||
<div class="col-md-6"><figure><img src="https://static.igem.org/mediawiki/2013/1/1e/UANL13_37RNATchartClones.png" width=400px><figcaption><span class="text-muted"><font size="2"><br>Figure 3. Behavior of different clones transformed with this construction (M1, 2, 11 and 12). Relative fluorescence at 25, 30, 37 and 42 ºC. All measurements were performed at least in triplicate, the aritmethic mean is shown.</span></font> <br></figcaption> | <div class="col-md-6"><figure><img src="https://static.igem.org/mediawiki/2013/1/1e/UANL13_37RNATchartClones.png" width=400px><figcaption><span class="text-muted"><font size="2"><br>Figure 3. Behavior of different clones transformed with this construction (M1, 2, 11 and 12). Relative fluorescence at 25, 30, 37 and 42 ºC. All measurements were performed at least in triplicate, the aritmethic mean is shown.</span></font> <br></figcaption> | ||
+ | </figure></div> | ||
+ | </div> | ||
+ | <br> | ||
+ | <div class="row"> | ||
+ | <div class="col-md-6">Mathematically, we found that a simple gaussian function fits our data well, and it provides us a way to quantify the strength (amplitude), optimal value (horizontal shift), and definition or clearness (width) of our RNAT activity (figure 4). We believe positive slope is due to RNAT melting, while negative slope is due to increase in the overall protein degradation rate due to higher temperatures. This function also allows for comparisons between different RNAT, as well as being potentially predictive for non verified temperatures.</div> | ||
+ | <div class="col-md-6"><figure><img src="https://static.igem.org/mediawiki/2013/a/a9/GaussAllUANL13.png" width=400px><figcaption><span class="text-muted"><font size="2"><br>Figure 4. Gaussian Function fitting of the experimental data shown in figure 3.</span></font> <br></figcaption> | ||
</figure></div> | </figure></div> | ||
</div> | </div> |
Revision as of 00:18, 27 October 2013
At a glance
Figure 1 shows the predicted secondary structures of the two synthetic RNATs implemented in our project. So far, we detected fluorescence only with the 37ºC responsive RNAT, which controls mCherry's translation.
Figure 2 shows the visual appearance of cultures grown at 37ºC containing the 37ºC RNAT_mCherry construction (figure 2a), a non-fluorescent control (figure 2b), and a standard constitutively expressing RFP (figure 2c).
Fluorescence of cultures carrying our construction increases almost 4x from 31 to 37ºC (figure 3).
Surprisingly, we obtained different behaviors in clones transformed with the same DNA (figure 4). We identified variations in plasmid copy number as the potential cause of phenotypic discrepancies among clones.
Mathematically, we found that a simple gaussian function fits our data well, and it provides us a way to quantify the strength (amplitude), optimal value (horizontal shift), and definition or clearness (width) of our RNAT activity (figure 4). We believe positive slope is due to RNAT melting, while negative slope is due to increase in the overall protein degradation rate due to higher temperatures. This function also allows for comparisons between different RNAT, as well as being potentially predictive for non verified temperatures.