In [2]:
%matplotlib inline
import matplotlib.pyplot as plt
import seaborn as sns
import numpy as np
In [3]:
from scipy.interpolate import interp1d
The file trajectory.npz contains 3 Numpy arrays that describe a 2d trajectory of a particle as a function of time:
t which has discrete values of time t[i].x which has values of the x position at those times: x[i] = x(t[i]).x which has values of the y position at those times: y[i] = y(t[i]).Load those arrays into this notebook and save them as variables x, y and t:
In [4]:
# YOUR CODE HERE
#raise NotImplementedError()
with np.load('trajectory.npz') as data:
t = data['t']
x = data['x']
y = data['y']
In [5]:
assert isinstance(x, np.ndarray) and len(x)==40
assert isinstance(y, np.ndarray) and len(y)==40
assert isinstance(t, np.ndarray) and len(t)==40
Use these arrays to create interpolated functions $x(t)$ and $y(t)$. Then use those functions to create the following arrays:
newt which has 200 points between $\{t_{min},t_{max}\}$.newx which has the interpolated values of $x(t)$ at those times.newy which has the interpolated values of $y(t)$ at those times.
In [6]:
# YOUR CODE HERE
#raise NotImplementedError()
newt = np.linspace(min(t), max(t), 200)
#interpolates data with respect to t
w = interp1d(t, x, kind = 'cubic')
q = interp1d(t, y, kind = 'cubic')
#creates interpolated arrays like w and q
#has newt as t points
newx = w(newt)
newy = q(newt)
In [7]:
assert newt[0]==t.min()
assert newt[-1]==t.max()
assert len(newt)==200
assert len(newx)==200
assert len(newy)==200
Make a parametric plot of $\{x(t),y(t)\}$ that shows the interpolated values and the original points:
In [16]:
# YOUR CODE HERE
#raise NotImplementedError()
plt.plot(x,y, 'o', color = 'c', label ='origonal points')
plt.plot(newx, newy,color='k', label ='(new x, new y)')
plt.legend()
plt.title('Particle Trajectory')
plt.grid(False)
plt.ylabel('$y(t)$')
plt.xlabel('$x(t)$');
In [9]:
assert True # leave this to grade the trajectory plot