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Created May 16, 2014 19:21
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Least Action
{
"metadata": {
"name": ""
},
"nbformat": 3,
"nbformat_minor": 0,
"worksheets": [
{
"cells": [
{
"cell_type": "heading",
"level": 1,
"metadata": {},
"source": [
"Least Action"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Load modules"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"import numpy as np\n",
"import scipy.optimize \n",
"global g \n",
"g=9.8"
],
"language": "python",
"metadata": {},
"outputs": [],
"prompt_number": 1
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Following:\n",
"http://www.eftaylor.com/software/ActionApplets/LeastAction.html, we define the Action in one small segment of the free fall movement in one-dimension. \n",
" \n",
"For one segment of the action between $(t_1,x_1)$, and $(t_2,x_2)$, with $\\Delta t$ sifficiently small such that $L$ can be considered constant, we have\n",
"\\begin{eqnarray}\n",
"S_1&=&\\int_{t_1}^{t_2} L dt \\\\\n",
"&\\approx& \\left[\\frac12 m v^2-m g h \\right]\\Delta t\\\\\n",
"&\\approx& \\left[\\frac12 m\\left(\\frac{x_2-x_1}{t_2-t_1}\\right)^2-m g \\frac{x_2+x_1}{2} \\right](t_2-t_1)\n",
"\\end{eqnarray}\n",
"that corresponds to Eq. (11) of Am. J. Phys, Vol. 72(2004)478: http://www.eftaylor.com/pub/Symmetries&ConsLaws.pdf"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"from IPython.display import Image\n",
"Image(filename='leastaction.png')"
],
"language": "python",
"metadata": {},
"outputs": [
{
"metadata": {},
"output_type": "pyout",
"png": 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"prompt_number": 2,
"text": [
"<IPython.core.display.Image at 0x7f2fcd92fd10>"
]
}
],
"prompt_number": 2
},
{
"cell_type": "heading",
"level": 2,
"metadata": {},
"source": [
"Code implementation"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We define the Action $S$ such of an object of mass $m$ throw vertically upward from $x_{\\hbox{ini}}$, such that $t_{\\hbox{end}}$ seconds later the object return to a height $x_{\\hbox{end}}$, as\n",
"\\begin{eqnarray}\n",
"S&=&\\int_{t_{\\hbox{ini}}}^{t_{\\hbox{end}}} L dt \\\\\n",
"&=&\\sum_i S_i \\Delta t\n",
"\\end{eqnarray}"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"def S(x,t=3.,m=0.2,xini=0.,xend=0.):\n",
" t=float(t)\n",
" Dt=t/x[:-1].size\n",
" x=np.asarray(x)\n",
" #Fix initial and final point\n",
" x[0]=xini\n",
" x[-1]=xend\n",
" return ((0.5*m*(x[1:]-x[:-1])**2/Dt**2-0.5*m*g*(x[1:]+x[:-1]))*Dt).sum()"
],
"language": "python",
"metadata": {},
"outputs": [],
"prompt_number": 3
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Function to find the least Action by using `scipy.optimize.fmin_powell`. It start from $\\mathbf{x}=(x_{\\hbox{ini}},0,0,\\ldots,x_{\\hbox{end}})$ and find the least action"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"def xfit(n,t=3.,m=0.2,xini=0.,xend=0.,ftol=1E-8):\n",
" '''Find the array of n (odd) components that minimizes the action S(x)\n",
"\n",
" :Parameters:\n",
"\n",
" n: odd integer \n",
" dimension of the ndarray x that minimizes the action S(x,t,m)\n",
" t,m: numbers\n",
" optional parameters for the action\n",
" ftol: number\n",
" acceptable relative error in S(x) for convergence.\n",
"\n",
" :Returns: (x,xmax,Smin)\n",
" \n",
" x: ndarray\n",
" minimizer of the action S(x)\n",
" \n",
" xini:\n",
" \n",
" xend:\n",
"\n",
" xmax: number\n",
" Maximum height for the object\n",
"\n",
" Smin: number\n",
" value of function at minimum: Smin = S(x)\n",
" '''\n",
" t=float(t)\n",
" if n%2==0:\n",
" print 'x array must be odd'\n",
" sys.exit()\n",
" \n",
" x0=np.zeros(n)\n",
" a=scipy.optimize.fmin_powell(S,x0,args=(t,m,xini,xend),ftol=ftol,full_output=1)\n",
" x=a[0]\n",
" x[0]=xini;x[-1]=xend\n",
" xmax=np.sort(x)[-1]\n",
" Smin=a[1]\n",
" Dt=t/x[:-1].size\n",
" return x,xmax,Smin,Dt \n"
],
"language": "python",
"metadata": {},
"outputs": [],
"prompt_number": 4
},
{
"cell_type": "heading",
"level": 2,
"metadata": {},
"source": [
"Least Action calculation"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"_Problem_: Let an object of mass $m=0.2$ Kg throw vertically updward and returning back to the same hand after 3 s. Find the function of distance versus time of least Action. "
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Let us divide the intervals in 21 parts:"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"t=3.\n",
"m=0.2\n",
"y=xfit(21,t,m)\n",
"x=y[0]\n",
"Smin=y[2]\n",
"Dt=t/x[:-1].size\n",
"tx=np.arange(0,t+Dt,Dt)"
],
"language": "python",
"metadata": {},
"outputs": [
{
"output_type": "stream",
"stream": "stdout",
"text": [
"Optimization terminated successfully.\n",
" Current function value: -21.554977\n",
" Iterations: 28\n",
" Function evaluations: 5784\n"
]
}
],
"prompt_number": 5
},
{
"cell_type": "heading",
"level": 3,
"metadata": {},
"source": [
"Plot"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"plt.plot(tx,x,label='$S_{\\mathrm{min}}=$%.2f' %Smin)\n",
"plt.plot(tx,x,'ro')\n",
"plt.ylabel('HEIGHT meters')\n",
"plt.xlabel('TIME seconds')\n",
"plt.title('Worldline of least action')\n",
"plt.legend(loc='best')"
],
"language": "python",
"metadata": {},
"outputs": [
{
"metadata": {},
"output_type": "pyout",
"prompt_number": 6,
"text": [
"<matplotlib.legend.Legend at 0x7f2fcd92ff10>"
]
},
{
"metadata": {},
"output_type": "display_data",
"png": 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QPXv2BCApKYn+ciY0cewYvPSS2s5akoBwJr6+sGoV/OMfkJqqdTSOp8REEB0d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\ncpIIhBDCyUkiEEIIJyeJQAghnNz/Awr6aBJ1uQGmAAAAAElFTkSuQmCC\n",
"text": [
"<matplotlib.figure.Figure at 0x7f2fcc063050>"
]
}
],
"prompt_number": 6
},
{
"cell_type": "heading",
"level": 3,
"metadata": {},
"source": [
"Dynamics of the least action solution"
]
},
{
"cell_type": "heading",
"level": 4,
"metadata": {},
"source": [
"Velocity"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"v=(x[1:]-x[:-1])/Dt\n",
"Dt=t/v[:-1].size\n",
"tx=np.arange(0,t+Dt,Dt)\n",
"plt.plot(tx,v)\n",
"plt.plot(tx,v,'ro')\n",
"plt.xlabel('TIME seconds')\n",
"plt.ylabel('VELOCITY meter/seconds')"
],
"language": "python",
"metadata": {},
"outputs": [
{
"metadata": {},
"output_type": "pyout",
"prompt_number": 7,
"text": [
"<matplotlib.text.Text at 0x7f2fc01bdf90>"
]
},
{
"metadata": {},
"output_type": "display_data",
"png": 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yZViyBFJTYe5ciI+HTzdZ2JySgs+VKxQ0bMiQhATN7HYAFQoRcSuHDtmuLk4f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\nPKMtNg/kKQAAAABJRU5ErkJggg==\n",
"text": [
"<matplotlib.figure.Figure at 0x7f2fc0571150>"
]
}
],
"prompt_number": 7
},
{
"cell_type": "heading",
"level": 4,
"metadata": {},
"source": [
"Aceleration"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"Dt=t/x[:-1].size\n",
"a=(v[1:]-v[:-1])/Dt\n",
"pa=plt.hist(a)\n",
"plt.title('ACELERATION meter/second$^2$')"
],
"language": "python",
"metadata": {},
"outputs": [
{
"metadata": {},
"output_type": "pyout",
"prompt_number": 8,
"text": [
"<matplotlib.text.Text at 0x7f2fc03de5d0>"
]
},
{
"metadata": {},
"output_type": "display_data",
"png": "iVBORw0KGgoAAAANSUhEUgAAAYAAAAENCAYAAAAG6bK5AAAABHNCSVQICAgIfAhkiAAAAAlwSFlz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\no9566y1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"text": [
"<matplotlib.figure.Figure at 0x7f2fcc043b10>"
]
}
],
"prompt_number": 8
},
{
"cell_type": "heading",
"level": 4,
"metadata": {},
"source": [
"Energy"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"T=0.5*m*v**2\n",
"V=0.5*m*g*(x[1:]+x[:-1])\n",
"E=T+V\n",
"print np.round(E,2)"
],
"language": "python",
"metadata": {},
"outputs": [
{
"output_type": "stream",
"stream": "stdout",
"text": [
"[ 21.56 21.56 21.56 21.56 21.56 21.56 21.55 21.55 21.56 21.56\n",
" 21.56 21.56 21.56 21.56 21.56 21.55 21.55 21.56 21.56 21.55]\n"
]
}
],
"prompt_number": 9
},
{
"cell_type": "heading",
"level": 4,
"metadata": {},
"source": [
"Action"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"The Action is minimal in each interval!"
]
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"SS=(T-V)*Dt\n",
"SS"
],
"language": "python",
"metadata": {},
"outputs": [
{
"metadata": {},
"output_type": "pyout",
"prompt_number": 10,
"text": [
"array([ 2.61768077, 1.45086657, 0.41339493, -0.49446 , -1.2723905 ,\n",
" -1.92031546, -2.43943472, -2.8282667 , -3.0874324 , -3.21713113,\n",
" -3.21711687, -3.08747347, -2.82816487, -2.4388897 , -1.92039431,\n",
" -1.27224489, -0.49433123, 0.41338249, 1.45064066, 2.6171035 ])"
]
}
],
"prompt_number": 10
},
{
"cell_type": "code",
"collapsed": false,
"input": [
"print 'S_MINIMUM=%g Joules*second' %SS.sum()"
],
"language": "python",
"metadata": {},
"outputs": [
{
"output_type": "stream",
"stream": "stdout",
"text": [
"S_MINIMUM=-21.555 Joules*second\n"
]
}
],
"prompt_number": 11
}
],
"metadata": {}
}
]
}
@TalKachman
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I just came across this and have to say this is really helpful.
From playing around with the code though it is vey unstable for almost any other potential, even the solution for a simple harmonic oscillator or brachistochrone. Could this be the choice of the optimization you use ?

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