deletions | additions       diff --git a/specific heat.tex b/specific heat.tex  index d00104c..38881ad 100644  --- a/specific heat.tex  +++ b/specific heat.tex 
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The graph of $C_p$ vs temperature is shown in figure 10 and it shows that $C_p$ increases as the temperature approaches $T_{\lambda}$ . This makes sense since there is a $c_2^2$ in the denominator and it was shown in second sound that it approaches zero at $T_{\lambda}$ so this is a good confirmation that the data works.   \subsection{ Error in $C_p$}  The error in $C_p$ can be found by the equation   \[ \sqrt{\frac{2}{c_2^3} \frac{\rho_s}{\rho_n}) \sqrt{\left(\frac{2}{c_2^3} \frac{\rho_s}{\rho_n}  S^2 T^2)^2 T^2\right)^2  dc_2^2 + \frac{1}{c_2^2} \left(\frac{1}{c_2^2}  \frac{\rho_s}{\rho_n} S^2)^2 S^2\right)^2  dT^2} \]