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<?xml version="1.0" encoding="utf-8"?> | ||
<stdhw weight="1" tags=""> | ||
<title>Lennard-Jones Potential</title> | ||
<code>boltzmann = 8.617e-5 | ||
epsi = rRound(boltzmann * rand(900, 2000, 45)/10, 3) | ||
sig = rand(100, 500, 63)/100 | ||
mindist = 2^(1/6)*sig | ||
innerdist = 0.9*mindist | ||
outerdist = 1.1*mindist | ||
innerpot = 4*epsi*((sig/innerdist)^12-(sig/innerdist)^6) | ||
outerpot = 4*epsi*((sig/outerdist)^12-(sig/outerdist)^6) | ||
innerforce = -4*epsi*(-12*sig^12/innerdist^13 + 6*sig^6/innerdist^7)*1E10*1.602E-19 | ||
outerforce = -4*epsi*(-12*sig^12/outerdist^13 + 6*sig^6/outerdist^7)*1E10*1.602E-19 | ||
</code> | ||
<problemsetup> | ||
<p>As you have learned in class, the potential that an atom sees when it encounters another atom is defined by a combination of attractive forces and repulsive forces from the repulsion of the electron clouds due to the Pauli exclusion principle. Rather than explicitly solving the Schrödinger Equation, the <em>Lennard-Jones</em> potential provides a reasonable approximation for the case of neutral atoms or molecules that experience only van der Waals forces (or dispersion forces) for attraction.</p> | ||
<p>The Lennard-Jones potential is given by $V(r) = 4 \epsilon \left[ ( \frac{\sigma}{r} )^{12} - (\frac{\sigma}{r})^6 \right]$. Here, $r$ is the distance between atoms/molecules, $\epsilon$ is related to the depth of the potential, and $\sigma$ is related to the equilibrium bond length.</p> | ||
<p>This homework problem will illustrate the Lennard-Jones potential for you. Let $\epsilon = ${epsi} eV and $\sigma = ${sig} å.</p> | ||
</problemsetup> | ||
<question type="radio" feedbacktype="afterdeadline" weight="1"> | ||
<questionprompt> | ||
<p>Visualize the potential. Which of the two terms is due to the Pauli exclusion principle?</p> | ||
</questionprompt> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
<solution> | ||
<p>The Pauli exclusion principle governs the potential at small $r$, i.e., when the electron clouds overlap. When $r$ is small, $r^{12}$ is much smaller than $r^{6}$. Hence, $1/r^{12}$ is much larger than $1/r^6$ and dominates for small $r$.</p> | ||
</solution> | ||
<answerchoice iscorrect="true"> | ||
<text>The one proportional to $1/r^{12}$.</text> | ||
</answerchoice> | ||
<answerchoice iscorrect="false"> | ||
<text>The one proportional to $1/r^{6}$.</text> | ||
</answerchoice> | ||
<answerchoice iscorrect="false"> | ||
<text>No individual term. It is their combination.</text> | ||
</answerchoice> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p>At what point $r$ (besides infinity) does the potential vanish?</p> | ||
</questionprompt> | ||
<answer>{sig}</answer> | ||
<units>å</units> | ||
<correctFeedback> | ||
<p>Right answer !</p> | ||
</correctFeedback> | ||
<solution> | ||
<p>If you set $r = \sigma$, then you find that both terms inside become 1, so the attractive and repulsive forces cancel out.</p> | ||
</solution> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p>At what position $r_{\rm min}$ is $V(r)$ globally minimal?</p> | ||
</questionprompt> | ||
<answer>{mindist}</answer> | ||
<units>å</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
<help> | ||
<p>How do you find the minimum of a mathematical function?</p> | ||
</help> | ||
<solution> | ||
<p>$\frac{dV(r)}{dr} =4\epsilon\left[-12\frac{\sigma^{12}}{r^{13}} + 6\frac{\sigma^6}{r^7}\right]$</p> | ||
<p>Setting this to 0 gives you $r = 2^{1/6} \sigma$.</p> | ||
</solution> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p>What is the value of $V(r)$ at this minimum?</p> | ||
</questionprompt> | ||
<answer>-{epsi}</answer> | ||
<units>eV</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
<solution> | ||
<p>Just put $r$=$2^{1/6} \sigma$=$2^{1/6}\cdot $ {sigma} into $V(r)$, this gives $-\epsilon$.</p> | ||
</solution> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p>Now assume that an external force pushes two atoms closer together, such that $r$=$0.9\cdot r_{\rm min}$ ($r_{\rm min}$ as in Question 3). By how much does the potential energy increase?</p> | ||
</questionprompt> | ||
<answer>{innerpot}+{epsi}</answer> | ||
<units>eV</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p>How large is the increase in potential energy if the external force pulls the two atoms apart such that $r=1.1\cdot r_{\rm min}$?</p> | ||
</questionprompt> | ||
<answer>{outerpot}+{epsi}</answer> | ||
<units>eV</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">What is the value (and sign) of the force acting on the system at $r = 0.9 \cdot r_{\rm min}$?</span> | ||
</p> | ||
</questionprompt> | ||
<answer>{innerforce}</answer> | ||
<units>N</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
<solution> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">The force follows from $F(r)=-\frac{d}{dr}V(r)$.</span> | ||
</p> | ||
</solution> | ||
<feedback answer="-{innerforce}"> | ||
<message> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">Is the force equal to $\frac{dV}{dr}$? Draw some potentials out and think about what the sign of the force must be at different areas of the potential.</span> | ||
</p> | ||
</message> | ||
</feedback> | ||
</question> | ||
<question type="freeresponse" feedbacktype="immediate" weight="1"> | ||
<questionprompt> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">What is the value (and sign) of that force at $r = 1.1 \cdot r_{\rm min}$?</span> | ||
</p> | ||
</questionprompt> | ||
<answer>{outerforce}</answer> | ||
<units>N</units> | ||
<correctFeedback>Right answer !</correctFeedback> | ||
<solution> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">The force follows from $F(r)=-\frac{d}{dr}V(r)$.</span> | ||
</p> | ||
</solution> | ||
<feedback answer="-{outerforce}"> | ||
<message> | ||
<p> | ||
<span style="line-height: 20.7999992370605px;">Is the force equal to $\frac{dV}{dr}$? Draw some potentials out and think about what the sign of the force must be at different areas of the potential.</span> | ||
</p> | ||
</message> | ||
</feedback> | ||
</question> | ||
</stdhw> |
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