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                    FYS2160 - Termodynamikk og statistisk fysikk
                  
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       <!--startindex-->

       <!-- ------------------- main content ---------------------- --><!-- --- begin exercise --- -->
<h2 id="project-1-statistics-for-loaded-dice">Statistics for loaded dice</h2>

<p><a href="/studier/emner/matnat/fys/FYS2160/h25/lectures/lecture8/boltzmanndice_seminar_sol.pdf">Here is the solution to these problems</a></p>

<center><!-- FIGURE -->
<hr class="figure"/>
<center>
<p class="caption">Figure 1: Face loaded die that will be used in this project.</p>
</center>

<p><img align="bottom" alt="" src="/studier/emner/matnat/fys/FYS2160/h25/lectures/lecture8/figures/trick-dice.jpg" width="500" loading="lazy"/></p>
</center>

<div class="alert alert-block alert-block alert-text-normal"><b>The Boltzmann conjecture</b>

<p>&nbsp;</p>

<p>Particles with kinetic energy \( E_k \) move in a "landscape" of states \( i \) with potential energies \( E_i \). The probability of the particle to be in state \( i \) is</p>
$$ \begin{eqnarray} P_i&amp;=&amp;\frac{1}{Z}e^{-\beta E_i}\\ Z&amp;=&amp;\sum_{i=1}^Ne^{-\beta E_i}, \end{eqnarray} $$

<p>where \( \beta=\frac{\alpha}{E_k} \), \( \alpha \) is a positive proportionality constant and \( N \) is the number of states.</p>

<p>&nbsp;</p>
</div>

<p>The normalization factor \( Z \) ensures that the sum of the probabilities is \( \sum_iP_i=1 \).</p>

<div class="alert alert-block alert-block alert-text-normal"><b>Corollary to the Boltzmann conjecture</b>

<p>&nbsp;</p>

<p>The relative probability of two states is</p>
$$ \begin{equation} \frac{P_i}{P_j}=e^{-\beta(E_i-E_j)}. \label{_auto1} \end{equation} $$

<p>&nbsp;</p>
</div>

<p>When we throw a die that rolls many times along a flat surface it has a typical kinetic energy \( E_k \) just before settling with a given face up. When the die is lying still with a face \( i\in{1,6} \) up it is in a potential well with energy \( E_i \). A <b>homogeneous die</b> has the probability \( P_i=\frac{1}{6} \) and the same potential well depth \( E_i \) for all the 6 faces \( i\in{1,6} \). A <b>face loaded die</b> has one face that is heavier than the others. This will affect the probabilities \( P_i \).</p>

<div class="alert alert-block alert-block alert-text-normal"><b>Unstructured problem formulation</b>

<p>&nbsp;</p>

<p>Do face loaded dice follow the Boltzmann conjecture?</p>

<p>&nbsp;</p>
</div>
<!-- --- begin hint in exercise --- -->

<p><b>Hint.</b> We do not know which face \( i\in\{1\ldots 6\} \) is loaded. In order to have a naming convention that is the same for all cases we will define the loading in the following way:</p>

<p>As an example we can say that face 2 is loaded and then face 5 is opposite (the sum of opposite faces in a die is always 7). Let us give the positions of the die names according to which faces turns up:</p>

<ul>
	<li>\( d \): loaded face <font color="red">d</font>own, thus \( d=5 \)</li>
	<li>\( s \): loaded face to the <font color="red">s</font>ide, thus \( s=\{1,3,4,6\} \)</li>
	<li>\( u \): loaded face <font color="red">u</font>p, thus \( u=2 \)</li>
</ul>

<p>We will name the energy differences as follows:</p>

<p>$$ \begin{eqnarray} \Delta E_{ud}&amp;=&amp;E_u-E_d\\ \Delta E_{us}&amp;=&amp;E_u-E_s\\ \Delta E_{sd}&amp;=&amp;E_s-E_d \end{eqnarray} $$ <!-- --- end hint in exercise --- --> <!-- --- begin subexercise --- --></p>

<p><b>a)</b> Find expressions for the potential energy differences of the different faces of a loaded die.</p>
<!-- removed !bans ... !eans environment (because of the command-line option --without_answers)
 --><!-- removed !bsol ... !esol environment (because of the command-line option --without_solutions)
 --><!-- --- end subexercise --- --><!-- --- begin subexercise --- -->

<p><b>b)</b> What does the corollary to Boltzmanns conjecture predict for the relative probabilities of the different faces pointing up?</p>
<!-- removed !bans ... !eans environment (because of the command-line option --without_answers)
 --><!-- removed !bsol ... !esol environment (because of the command-line option --without_solutions)
 --><!-- --- end subexercise --- --><!-- --- begin subexercise --- -->

<p><b>c)</b> Find expressions for the normalization factor, \( Z \) of the die and for each probability.</p>
<!-- removed !bans ... !eans environment (because of the command-line option --without_answers)
 --><!-- removed !bsol ... !esol environment (because of the command-line option --without_solutions)
 --><!-- --- end subexercise --- --><!-- --- begin subexercise --- -->

<p><b>d)</b> Plan and execute an experiment with a loaded die to test if the Boltzmann conjecture is valid for face loaded dice.</p>
<!-- --- begin hint in exercise --- -->

<p><b>Hint.</b> Note the result every time you throw the die. In this way you conserve the maximum amount of data from your experiment and</p>

<ul>
	<li>you can reuse the data if you get new ideas for how to analyse it</li>
	<li>you can share and pool your data with that of others to get better statistics</li>
</ul>
<!-- --- end hint in exercise --- --><!-- removed !bsol ... !esol environment (because of the command-line option --without_solutions)
 --><!-- --- end subexercise --- --><!-- --- begin subexercise --- -->

<p><b>e)</b> Do face loaded dice follow the Boltzmann conjecture?</p>
<!-- removed !bans ... !eans environment (because of the command-line option --without_answers)
 --><!-- --- end subexercise --- --><!-- --- begin subexercise --- -->

<p><b>f)</b> Can the use of the Boltzmann conjecture improve estimation of the probabilities of landing on each side of a loaded die?</p>
<!-- removed !bans ... !eans environment (because of the command-line option --without_answers)
 --><!-- --- end subexercise --- --><!-- --- end exercise --- --><!-- ------------------- end of main content --------------- -->
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