{ "metadata": { "name": "" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "code", "collapsed": true, "input": [ "from pylab import *\n", "%matplotlib inline\n", "from scipy.integrate import odeint\n", "\n", "# nastavitve za izris grafov (http://matplotlib.org/1.3.1/users/customizing.html)\n", "rc('text', usetex=True)\n", "rc('font', size=12, family='serif', serif=['Computer Modern'])\n", "rc('xtick', labelsize='small')\n", "rc('ytick', labelsize='small')\n", "rc('legend', fontsize='medium')\n", "rc('figure', figsize=(5, 3))\n", "rc('lines', linewidth=2.0)\n", "rc('axes', color_cycle=['k'])\n", "rc('contour', negative_linestyle='solid')" ], "language": "python", "metadata": {}, "outputs": [], "prompt_number": 2 }, { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Navadne diferencialne ena\u010dbe" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Pri re\u0161evanju diferencialne ena\u010dbe gre za dolo\u010ditev obna\u0161anja neke koli\u010dine, odvisne od ene ali ve\u010d spremenljivk, \n", "pri \u010demer v povezavi med iskano koli\u010dino $y$ in neodvisnimi spremenljivkami $x_i$ nastopajo tudi odvodi iskane koli\u010dine po neodvisnih spremenljivkah, npr. $\\frac{\\partial y}{\\partial x_i}$, $\\frac{\\partial^2 y}{\\partial x_i\\partial x_j},\\ldots$ \u010ce je neodvisna spremenljivka ena sama, govorimo o navadnih diferencialnih ena\u010dbah. \u010ce v diferencialni ena\u010dbi nastopajo samo prvi odvodi, govorimo o navadni diferencialni ena\u010dbi prveg reda. \u010ce poleg njih nastopijo tudi drugi odvodi, je to navadna diferencialna ena\u010dba drugega reda.\n", "\n", "Navadno diferencialno ena\u010dbo prvega reda lahko numeri\u010dno re\u0161imo tako, da odvod nadomestimo z diferen\u010dnim pribli\u017ekom: \n", "\n", "$$\\frac{\\mathrm{d}y(x)}{\\mathrm{d}x}=f\\left(y(x),x\\right)$$\n", "\n", "$$\\frac{y(x+\\Delta x)-y(x)}{\\Delta x}=f\\left(y(x),x\\right)$$\n", "\n", "$$y(x+\\Delta x)=y(x)+f\\left(y(x),x\\right)\\Delta x$$\n", "\n", "Na ta na\u010din lahko s poznavanjem za\u010detnega pogoja $y(0)$ z zaporedno uporabo zgornje zveze poi\u0161\u010demo vrednosti koli\u010dine $y$ pri poznej\u0161ih \u010dasih: \n", "\n", "$$y(0)\\rightarrow y(\\Delta x)\\rightarrow y(2\\Delta x)\\ldots$$\n", "\n", "Navadno diferencialno ena\u010dbo vi\u0161jega reda lahko z vpeljavo novih spremenljivk spremenimo v sistem navadnih diferencialnih ena\u010db prvega reda:\n", "\n", "$$\\frac{\\mathrm{d}^2y(x)}{\\mathrm{d}x^2}=f\\left(y(x),\\frac{\\mathrm{d}y(x)}{\\mathrm{d}x}, x\\right),$$\n", "\n", "$$\\frac{\\mathrm{d}y(x)}{\\mathrm{d}x}=u(x),$$\n", "\n", "$$\\frac{\\mathrm{d}u(x)}{\\mathrm{d}x}=f\\left(y(x),u(x),x\\right),$$\n", "\n", "ki ga nato numeri\u010dno re\u0161imo tako, kot smo se nau\u010dili pri navadni diferencialni ena\u010dbi prvega reda:\n", "\n", "$$y(x+\\Delta x)=y(x)+u(x)\\Delta x$$\n", "\n", "$$u(x+\\Delta x)=u(x)+f(y(x), u(x), x)\\Delta x$$\n", "\n", "Tu potrebujemo dva za\u010detna pogoja, vrednost iskane funkcije $y(0)$ in njenega odvoda $u(0)=\\left.\\frac{\\mathrm{d}y}{\\mathrm{d}x}\\right|_{x=0}$:\n", "\n", "$$\\left(y(0), u(0)\\right)\\rightarrow\\left(y(\\Delta x), u(\\Delta x)\\right)\\rightarrow\\left(y(2\\Delta x), u(2\\Delta x)\\right)\\ldots$$\n", "\n", "Algoritmi, ki jih za re\u0161evanje navadnih diferencialnih ena\u010db ponujajo profesionalna ra\u010dunalni\u0161ka orodja, so veliko bolj sofisticirani od zgoraj opisanjega. Z uporabo diferen\u010dnih pribli\u017ekov vi\u0161jega reda, spremenljivega koraka $\\Delta x$, ..., dose\u017eejo ve\u010djo stabilnost in hitrost iskanja re\u0161itve. " ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Kot primer si oglejmo izra\u010dun poti $s$ in hitrosti $\\frac{\\mathrm{d}s}{\\mathrm{d}t}$ telesa pri padanju le-tega v zemeljskem gravitacijskem polju. Na telo poleg gravitacijske sile deluje zaviralna sila, za katero velja kvadratni zakon upora. Zapi\u0161imo drugi Newtonov zakon:\n", "\n", "$$m\\frac{\\mathrm{d}^2s}{\\mathrm{d}t^2}=mg-c\\left(\\frac{\\mathrm{d}s}{\\mathrm{d}t}\\right)^2$$\n", "\n", "Za\u010detna pogoja sta $s(0)=0$ in $\\left.\\frac{\\mathrm{d}s}{\\mathrm{d}t}\\right|_{t=0}=0$." ] }, { "cell_type": "code", "collapsed": false, "input": [ "t=linspace(0, 10, 1000)\n", "m=1.0\n", "g=9.81\n", "c=0.01\n", "def deriv(y, t): \n", " return array([y[1], g - c / m * y[1] ** 2])\n", "\n", "y0=array([0, 0])\n", "y=odeint(deriv, y0, t)\n", "s=y[:, 0]\n", "v=y[:, 1]\n", "\n", "fig, (axa, axb) = subplots(2, 1, sharex='col', sharey='row', figsize=(5, 6))\n", "\n", "axa.plot(t, s);\n", "axa.set_ylabel(r'Pot (m)')\n", "axa.grid(alpha=0.5)\n", "axa.annotate('(a)', xy=(0.03, 0.92), xycoords='axes fraction')\n", "\n", "axb.plot(t, v);\n", "axb.set_ylabel(r'Hitrost (m/s)')\n", "axb.set_xlabel(r'\\v Cas (s)')\n", "axb.grid(alpha=0.5)\n", "axb.annotate('(b)', xy=(0.03, 0.92), xycoords='axes fraction')\n", "\n", "subplots_adjust(hspace=0.1)" ], "language": "python", "metadata": {}, "outputs": [ { "metadata": {}, "output_type": "display_data", "png": 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27FkANQujzZs3D6NGjYJCoRA5QkKkjXqcHqSlPaQrV64gLS0NPXr0wFtvvYWz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\ngJpLOWtPNoltx44dWLx4Mdq0aYN169a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"text": [ "" ] } ], "prompt_number": 9 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Naloge" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "
    \n", "
  1. Izra\u010dunaj in nari\u0161i, kako sta odklon iz ravnovesne lege in kotna hitrost matemati\u010dnega nihala odvisna od \u010dasa, \u010de ob \u010dasu $t=0$ nihalo miruje, odklon od ravnovesne lege pa je a) $30^\\circ$ in b) $150^\\circ$ (nihalo naj ima togo vrvico). Primerjaj z analiti\u010dnim rezultatom za majhne odklone iz ravnovesne lege. Kro\u017ena frekvenca nihala naj bo $1\\,$s$^{-1}$. \n", "\n", "
  2. Izra\u010dunaj in nari\u0161i tira Zemlje in Lune pri gibanju okoli Sonca. Podatki: $M_S=2\\times 10^{30}\\,$kg, $M_Z=6\\times 10^{24}\\,$kg, $M_L=7.35\\times 10^{22}\\,$kg, $d_{ZS}=1.5\\times 10^{8}\\,$km, $d_{LZ}=3.84\\times 10^5\\,$km, $T_Z=365.25\\,$dni in $T_L=29.53\\,$dni. Za\u010detni polo\u017eaj Zemlje naj bo $\\mathbf{r}_Z(0)=(d_{ZS}, 0)$, Lune pa $\\mathbf{r}_L(0)=(d_{ZS}, d_{LZ})$. \n", "Za\u010detna hitrost Zemlje naj bo $\\mathbf{v}_Z(0)=(0, 2\\pi d_{ZS}/T_Z)$, Lune pa $\\mathbf{v}_L(0)=(-2\\pi d_{LZ}/T_L, 2\\pi d_{ZS}/T_Z)$. Ker ima Sonce bistveno ve\u010djo maso od Zemlje in Lune, lahko predpostavi\u0161, da miruje v izhodi\u0161\u010du koordinatnega sistema.\n", "\n", "
" ] } ], "metadata": {} } ] }