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courses:lecture:pplec:pplecquantenergy 2011/08/09 11:10 courses:lecture:pplec:pplecquantenergy 2011/08/09 16:57 current
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=====Quantization of Energy in Mechanical Oscillators (15 minutes)===== =====Quantization of Energy in Mechanical Oscillators (15 minutes)=====
-  * Before beginning this lecture, ask the students to [[..:..:..:courses:activities:ppact:ppbound|Draw Some Bound States]].  This will help put students into the mindset of energies and bound states.+  * Before beginning this lecture, ask the students to [[..:..:..:courses:activities:ppact:ppbound|Draw Some Bound States]].
  * The most common bound state is the single mass on a spring, as seen below.   * The most common bound state is the single mass on a spring, as seen below.
Add image: pplecquanenergy1 Add image: pplecquanenergy1
-  * We can also extend this bound state premise to a system with multiple masses and springs as well.  Looking at the first normal mode for a five-mass system (if students have already performed the [[..:..:..:courses:activities:ppact:ppperiodiclab1|Monoatomic Chain Lab]], refer to this), if we keep the envelope function the same shape but increase the amplitude, the potential energy for the system changes with very similar behavior to the single mass system.+  * We can also extend this bound state premise to a system with multiple masses and springs as well.  Looking at the first normal mode for a five-mass system (if students have already performed the [[..:..:..:courses:activities:ppact:ppperiodiclab1|Monatomic Chain Lab]], refer to this), if we keep the envelope function the same shape but increase the amplitude, the potential energy for the system changes with very similar behavior to the single mass system.
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where $\hbar \omega_{mode}$ is the phonon energy and $n_{phonon}$ is called the phonon number.  $n_{phonon}$ increases with temperature and in whole steps (i.e. $n_{phonon}=0,1,2...$). where $\hbar \omega_{mode}$ is the phonon energy and $n_{phonon}$ is called the phonon number.  $n_{phonon}$ increases with temperature and in whole steps (i.e. $n_{phonon}=0,1,2...$).
-  * Unfortunately, use of the equipartition theorem for $U_{mode}$ breaks down if $n_{phonon} \sim 1$.  It turns out that we do not observe "fractional phonon numbers"; we find that a normal mode "freezes out" when $k_{B}T=\hbar \omega_{mode}$ for a system.+  * Unfortunately, use of the equipartition theorem for $U_{mode}$ breaks down if $n_{phonon} \sim 1$.  It turns out that we do not observe "fractional phonon numbers"; we find that a normal mode "freezes out" when $k_{B}T=\hbar \omega_{mode}$ for a system. This behavior is seen in the graph below. 
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 +Add image: pplecquanenergy3 
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 +Notice the abrupt drop off at the freeze out point.  It was later found that this "freeze out" range of temperatures can actually be modeled using the Real Bose-Einstein function 
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 +$$f(\omega)=\frac{1}{e^{\frac{\hbar \omega}{kT}}-1} \; \; . $$
  * So, the big question now is this: how do we determine the energy stored in a lattice once the temperature is in this "freeze out" zone?   * So, the big question now is this: how do we determine the energy stored in a lattice once the temperature is in this "freeze out" zone?

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