Interact Exercise 6

Imports

Put the standard imports for Matplotlib, Numpy and the IPython widgets in the following cell.



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%matplotlib inline
import matplotlib.pyplot as plt
import numpy as np



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from IPython.display import Image
from IPython.html.widgets import interact, interactive, fixed

Exploring the Fermi distribution

In quantum statistics, the Fermi-Dirac distribution is related to the probability that a particle will be in a quantum state with energy $\epsilon$. The equation for the distribution $F(\epsilon)$ is:



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Image('fermidist.png')









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In this equation:

$\epsilon$ is the single particle energy.
$\mu$ is the chemical potential, which is related to the total number of particles.
$k$ is the Boltzmann constant.
$T$ is the temperature in Kelvin.

In the cell below, typeset this equation using LaTeX:

YOUR ANSWER HERE

Define a function fermidist(energy, mu, kT) that computes the distribution function for a given value of energy, chemical potential mu and temperature kT. Note here, kT is a single variable with units of energy. Make sure your function works with an array and don't use any for or while loops in your code.



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def fermidist(energy, mu, kT):
    """Compute the Fermi distribution at energy, mu and kT."""
    # YOUR CODE HERE
    f=1/(np.exp((energy-mu)/kT)+1)
    return f









    Out[41]:





0.401312339887548



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assert np.allclose(fermidist(0.5, 1.0, 10.0), 0.51249739648421033)
assert np.allclose(fermidist(np.linspace(0.0,1.0,10), 1.0, 10.0),
    np.array([ 0.52497919,  0.5222076 ,  0.51943465,  0.5166605 ,  0.51388532,
               0.51110928,  0.50833256,  0.50555533,  0.50277775,  0.5       ]))

Write a function plot_fermidist(mu, kT) that plots the Fermi distribution $F(\epsilon)$ as a function of $\epsilon$ as a line plot for the parameters mu and kT.

Use enegies over the range $[0,10.0]$ and a suitable number of points.
Choose an appropriate x and y limit for your visualization.
Label your x and y axis and the overall visualization.
Customize your plot in 3 other ways to make it effective and beautiful.



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def plot_fermidist(mu, kT):
    # YOUR CODE HERE
    f=plt.figure(figsize=(9,6))
    energy=np.linspace(0,10,100)
    plt.plot(energy,fermidist(energy,mu,kT),'k')
    plt.xlim(0,10)
    plt.ylim(0,1)
    plt.tick_params(direction='out')
    plt.title('Fermi Dirac Distridution over a range of Energy Levels for Constant MU and kT')
    plt.ylabel('Fermi Distribution')
    plt.xlabel('Energy Range')

# energy=np.linspace(1,10,10)
# f=fermidist(4,1,energy) 
# f

# plt.plot(energy,f)



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plot_fermidist(4.0, 1.0)



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assert True # leave this for grading the plot_fermidist function

Use interact with plot_fermidist to explore the distribution:

For mu use a floating point slider over the range $[0.0,5.0]$.
for kT use a floating point slider over the range $[0.1,10.0]$.



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# YOUR CODE HERE
interact(plot_fermidist,mu=(0,5,0.1),kT=(0.1,10,0.1))

Provide complete sentence answers to the following questions in the cell below:

What happens when the temperature $kT$ is low?
What happens when the temperature $kT$ is high?
What is the effect of changing the chemical potential $\mu$?
The number of particles in the system are related to the area under this curve. How does the chemical potential affect the number of particles.

Use LaTeX to typeset any mathematical symbols in your answer.

When the temperature kT is low there is a dramatic change in the Fermi Distribution that occurs at the $\mu$ value.

When the kT value is high the Fermi Distribution gradually drops over a large energy range.

Changing the chemical potential, $\mu$ changes the Energy Range value at which the Fermi distribution has a dramatic change in value.

As the chemical potential, $\mu$ increases so does the number of particles in the system. Because the number of particles can be describes as $\int(F(\epsilon))$ and increasing $\mu$ pushes the system to the right, it increases the integral.



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