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. 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">A 0.65m insulated copper wire (cross-sectional area, 0.05m<sup>2</sup>) 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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<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 (Fig. 2).</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 $t$. A linear fit of a $T$ vs. $ln(t)$ plot following only the reading from the broth thermocouple will yield the conductivity (Fig. 2).</p>
  
 
                 <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">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>

Revision as of 14:20, 19 October 2016