Difference between revisions of "Team:Exeter/Collaborations"

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<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 $$ \lambda = \frac{Q}{4\pi[\Delta T\ \ln{(t)}$$Using this data a straight line of best fit was plotted using the least squares method. This was then used to calculate the average gradient of the graph. By using these value along with $$ \lambda = \frac{Q}{4\pi[T(t_{2})-T(t_{1})]}\ \log{\Big(\frac{t_{2}}{t_{1}}\Big)}$$ Where $Q$ is our power per unit length calculated by $Q = \frac{(I \times V)}{Length}$ , $T(t_\alpha)$ is the temperature at time $\alpha$ and $T(t_{2})-T(t_{1})$ is our gradient (Nagasaka and Nagashima, 1981).</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 $$ \lambda = \frac{Q}{4\pi\Delta T}\ \ln{(t)}$$Using this data a straight line of best fit was plotted using the least squares method. This was then used to calculate the average gradient of the graph. By using these value along with $$ \lambda = \frac{Q}{4\pi[T(t_{2})-T(t_{1})]}\ \log{\Big(\frac{t_{2}}{t_{1}}\Big)}$$ Where $Q$ is our power per unit length calculated by $Q = \frac{(I \times V)}{Length}$ , $T(t_\alpha)$ is the temperature at time $\alpha$ and $T(t_{2})-T(t_{1})$ is our gradient (Nagasaka and Nagashima, 1981).</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>
 
                 <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>

Revision as of 13:24, 19 October 2016