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;">
 
<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 $t$, such that a linear fit of a $T$ vs. $ln(t)$ plot 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 14:15, 19 October 2016