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August 14, 2018 15:57
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Simple simulations with Python and NumPy
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{ | |
"cells": [ | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"# SAO Python Tutorial\n", | |
"7/14/2018\n", | |
"\n", | |
"Lehman Garrison ([email protected])" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"This notebook shows how to do simple simulations with Python and NumPy. It shows the \"naive\" way using Python `for` loops, then compares it to the fast solution using NumPy." | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"## Simulating events: coin flips" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"import numpy as np" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"Let's start simple by simulating a million coin flips and counting the number of heads.\n", | |
"\n", | |
"The naive (\"pure Python\") to do this is:" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"N = 2000000" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"#%%timeit\n", | |
"n_heads = 0\n", | |
"for i in range(N):\n", | |
" flip = np.random.randint(0,2)\n", | |
" if flip == 1:\n", | |
" n_heads += 1\n", | |
"print(n_heads)" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"You should try uncommenting the `%%timeit` command, which will run the cell multiple times to estimate the runtime." | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"The way to do this in Numpy is to generate the whole array of flips, then sum the array. This is much faster, because native Python \"`for`\" loops are very slow, while generating random numbers and summing arrays are fast in Numpy." | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"#%%timeit\n", | |
"flips = np.random.randint(0, 2, size=N)\n", | |
"n_heads = np.sum(flips)" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"Again, try uncommenting the `%%timeit` command to see how much faster this way is." | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"Let's look at the flips array, should be length `N` and filled with 0s and 1s:" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": { | |
"scrolled": true | |
}, | |
"outputs": [], | |
"source": [ | |
"flips" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"The fraction of heads should be close to 0.5:" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"np.sum(flips)/len(flips)" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"What about a weighted coin toss?" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"weighted_nheads = np.random.binomial(N, 0.75)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"weighted_nheads" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"## Advanced: computing $\\pi$ by generating random numbers" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"We can compute the value of $\\pi$ by generating random points in a 2D square and counting the number of points that fall inside a circumscribed circle. This gives us the area of the circle, from which we can compute $\\pi$. This general technique of computing area or volume by generating random points is known as \"Monte Carlo integration\"." | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"Here's the naive (slow) way to write such a simulation:" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"N = int(1e6) # Number of random points to use\n", | |
"R = 1.0 # Radius of circle" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"#%%timeit\n", | |
"N_inside = 0\n", | |
"for i in range(N):\n", | |
" point = np.random.rand(2)*2*R - R # (x,y) point between -R and R\n", | |
" \n", | |
" r = np.sqrt(point[0]**2 + point[1]**2)\n", | |
" \n", | |
" inside_circle = r < R\n", | |
" \n", | |
" if inside_circle:\n", | |
" N_inside += 1\n", | |
" \n", | |
"frac_in_circle = N_inside/N\n", | |
"area_of_square = (2*R)**2\n", | |
"pi_estimate = frac_in_circle*area_of_square/R**2\n", | |
"print(pi_estimate)\n", | |
"print((pi_estimate - np.pi)/np.pi)" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"### Exercise 1\n", | |
"\n", | |
"Can you re-write this simulation without a `for` loop? Remember how we avoided the `for` loop in the coin flip example: we created a big array with all the flips, and then summed it up, rather than checking each flip one at a time.\n", | |
"\n", | |
"#### Bonus:\n", | |
"What other tricks can you come up with to speed up this simulation?" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Your solution here" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"### Exercise 2\n", | |
"\n", | |
"Write a function that takes a parameter `n_trials` that executes the above code `n_trials` times. It's okay to use a `for` loop over the number of trials, since this will typically be small (~1000), while the number of points `N` will be more like 100000. Return an array of all the `pi_estimate` values (this array should be of length `n_trials`). Plot a histogram of this array.\n", | |
"\n", | |
"Also plot the true value of pi, and the mean value of all your trials." | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Your solution here" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"metadata": {}, | |
"source": [ | |
"### Exercise 3 (Bonus)\n", | |
"The trials have some built-in scatter due to the random nature of Monte Carlo integration. That's the spread of the histogram you just plotted. But you can see that the mean is a better estimate than any one trial.\n", | |
"\n", | |
"1. How much more precise do you expect the mean to be than the individual trials? If you're not sure, try the below experiment and then come back to this.\n", | |
"\n", | |
"1. Compute the standard deviation of the distribution of trials that you plotted above.\n", | |
"\n", | |
"1. Write a function that will repeat the above experiment of generating trials and taking the mean. Record the mean each time. Note: you can reduce the number of trials if you need this to run faster. You should finish with an array of mean values.\n", | |
"\n", | |
"1. Compute the standard deviation of this distribution of means.\n", | |
"\n", | |
"1. How much smaller is the standard deviation of the means than the standard devation of the samples?\n", | |
"\n", | |
"1. If you wanted your \"error bars\" (standard deviation of the mean) to shrink by a factor of two, how many more trials would you need to run?" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Your solution here" | |
] | |
} | |
], | |
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