Difference between revisions of "Team:Exeter/Collaborations"

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                 <p id="pp">A 0.65m insulated copper wire (cross-sectional area, 0.05m^2) was passed through the centre of a 50mL falcon tube containing the liquid medium to be measured, suspended in a water bath (Fig. 1b). Three thermocouples (Pico Technology TC-08) were attached, one to the wire in contact with the insulation using blue tack, one suspended in the liquid medium 5mm from the wire, and one in the water bath. Power was supplied to the wire at 5A, 1.8V for 600s, generating a small temperature increase of approximately 2&deg;C above room temperature (23 &plusmn; 1&deg;C) to avoid convection effects.</p>
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                 <p id="pp">A 0.65m insulated copper wire (cross-sectional area, 0.05m^2) was passed through the centre of a 50mL falcon tube containing the liquid medium to be measured, suspended in a water bath (Fig. 1b). Three thermocouples (Pico Technology TC-08) were attached, one to the wire in contact with the insulation using blue tack, one suspended in the liquid medium 5mm from the wire, and one in the water bath. Power was supplied to the wire at 5A, 1.8V for 600s, generating a small temperature increase of approximately 2&deg;C above room temperature (23 &plusmn; 1&deg;C) to avoid convection effects. Our experimental setup was calibrated to the thermal conductivity of <a href="http://www2.bren.ucsb.edu/~dturney/WebResources_13/WaterSteamIceProperties/PropOfWaterFrom0to100Celcius.pdf">water</a> at 20&deg;C, 598.4 $\frac{mW}{Km}\text{ }$. Measurements of two growth media, liquid broth (LB) and M9 were repeated at least in quintuple.</p>
  
 
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<p id="pp"By recording the difference in temperatures over a ten minute interval and repeating the experiment 5 times for reliability. We were able to use the first 50 seconds of data to produce the graph on the right.></p>
 
  
 
<img src="https://static.igem.org/mediawiki/2016/8/88/T--Exeter--Home_collab_cond.jpg" style="float:right; width:40vw; height:60vh;">
 
<img src="https://static.igem.org/mediawiki/2016/8/88/T--Exeter--Home_collab_cond.jpg" style="float:right; width:40vw; height:60vh;">
  
                 <p id="pp">Nagasaka and Nagashima noted that wire insulation has negligible impact on the measurement of the thermal conductivity of saline solutions (Nagasaka and Nagashima 1981) and thus can be described by the equation $$ \lambda = \frac{Q}{4\pi\Delta T}\ \ln{(t)}$$ where $Q$ is the power per unit length of the wire, $Q = \frac{(I \times V)}{Length}$, and $\Delta T$ is the change in temperature over time $t$, such that a linear fit of a $T$ vs. $ln(t)$ plot will yield the conductivity.</p>
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                 <p id="pp">Nagasaka and Nagashima noted that wire insulation has negligible impact on the measurement of the thermal conductivity of saline solutions (Nagasaka and Nagashima 1981) and thus can be described by the equation $$ \lambda = \frac{Q}{4\pi\Delta T}\ \ln{(t)}$$ where $Q$ is the power per unit length of the wire, $Q = \frac{(I \times V)}{Length}$, and $\Delta T$ is the change in temperature over time $t$, such that a linear fit of a $T$ vs. $ln(t)$ plot will yield the conductivity (Fig. 2).</p>
  
                 <p id="pp">As we used a plastic coated copper wire we had to apply a correction to the values to make them more accurate. This was done by calculating the conductivity of water using the insulated wire and comparing it to the given conductivities from  <a href="http://www2.bren.ucsb.edu/~dturney/WebResources_13/WaterSteamIceProperties/PropOfWaterFrom0to100Celcius.pdf">here</a>. We found that the conductivity value was roughly one fourth of the known value at any given temperature and the correction applied to the results of the lb and m9 media.Due to time constraints the lb experiment was repeated 6 times and 5 times for the m9 media with a water calibration being done each time and then the result averaged, errors were taken as the standard deviation of the measurements.Using the apparatus we had available we found the thermal conductivity of lb and M9 to be similar to that of water.The conductivity of water at room temperature is 598.4 $\frac{mW}{Km}\text{ }$(mili watt per metre kelvin). We found the conductivity to be (605 $\pm$ 20) $\frac{mW}{Km}\text{ }$ and (570 $\pm$ 30) $\frac{mW}{Km}\text{ }$ for LB and m9 respectively.</p>
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                 <p id="pp">We found the thermal conductivity of LB and M9 to be similar to that of water, at 605 $\pm$ 20 $\frac{mW}{Km}\text{ }$ and 570 $\pm$ 30 $\frac{mW}{Km}\text{ }$ respectively.</p>
  
                <p id="pp">These values were fairly reliable to what we experienced during the test. The lb media took the same time to cool down to equilibrium as the water control test and thus the conductivities should be the same. The m9 sample took longer than water to cool down which correlated with the fact the conductivity was lower.</p>
 
  
 
<h5>References</h5>
 
<h5>References</h5>

Revision as of 13:57, 19 October 2016