deletions | additions       diff --git a/subsection_Varying_the_Polarization_time__.tex b/subsection_Varying_the_Polarization_time__.tex  index 2b4b2fb..a032761 100644  --- a/subsection_Varying_the_Polarization_time__.tex  +++ b/subsection_Varying_the_Polarization_time__.tex 
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In the equation above, $M_{\infty}$ represents the equilibrium Curie value (Eq. \ref{eq:curielaw}). The time constant $T_1$ is known as the spin-lattice relaxation time. In other words, $T_1$ is the time it takes for the magnetization to exponentially approach $M_{\infty}$. Eq. \ref{eq:growthrate} is used to describe the relationship between the voltage verses a changing polarization time. \\\\  The Curie law can derived using $M=n\mu$ $M=n\mu\left$  where $$ $\left$  represents the average value of $cos(\theta)$, measuring the alignment between the magnetic moment and the external field B, for all magnetic moments in the sample. The calculation of $$ using classical thermodynamics results in the Curie law. The Curie value can be calculated using the following equation: \begin{equation}  \label{eq:curielaw}  M_o=\frac{n\mu^2B}{3kT}