{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "Homework Assignment 1\n", "=====================\n", "\n", "\n", "**Note**: This is a computable IPython notebook who's source code can be downloaded [here](https://raw.githubusercontent.com/johnfoster-pge-utexas/PGE383-AdvGeomechanics/master/files/assignment1_solution.ipynb).\n", "\n", "## Problem 1\n", " \n", "The motion of a certain continuous medium is defined by the equations\n", " \n", "\\begin{align}\n", " x_1 &= \\frac{1}{2} \\left( X_1 + X_2 \\right) e^t + \\frac{1}{2} \\left( X_1-X_2 \\right) e^{-t}, \\notag \\\\\n", " x_2 &= \\frac{1}{2} \\left( X_1 + X_2 \\right) e^t - \\frac{1}{2} \\left( X_1-X_2 \\right) e^{-t}, \\notag \\\\\n", " x_3 &= X_3 \\notag\n", "\\end{align}\n", "\n", "1. Compute the following\n", "\n", " 1. The Green-Lagrange strain tensor $E$\n", " \n", " 1. The linear (small) strain tensor $\\varepsilon$\n", "\n", " Plot the $11$, $22$, and $12$ components of $E$ and $\\varepsilon$ on the same figure\n", " from time $t=0$ to $t=0.05$.\n", " \n", "\n", "1. Compute the following\n", "\n", " 1. The rate-of-deformation tensor $D$\n", " \n", " 1. The rate-of-change of the small strain tensor $\\dot{\\varepsilon} = \\frac{d\\varepsilon}{dt}$\n", "\n", " Plot the $11$, $22$, and $12$ components of $D$ and $\\dot{\\varepsilon}$ on the same figure\n", " from time $t=0$ to $t=0.05$.\n", " \n", " \n", "**Solution**" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "This cell loads some important packages from sympy, numpy, and matplotlib that I will use the perform calculations and display the results neatly. In order to run this notebook, you will have to have these packages installed in your Python distribution." ] }, { "cell_type": "code", "execution_count": 1, "metadata": { "collapsed": false }, "outputs": [], "source": [ "from sympy import *\n", "from sympy.matrices import *\n", "import sympy.mpmath\n", "from sympy.utilities.lambdify import lambdify\n", "init_printing()\n", "\n", "import numpy\n", "\n", "%matplotlib inline\n", "import matplotlib.pyplot as plt\n", "#plt.style.available\n", "#plt.style.use('bmh')" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Defining which variables will be \"symbolic\" in nature, i.e., they will not take on numerical values." ] }, { "cell_type": "code", "execution_count": 2, "metadata": { "collapsed": false }, "outputs": [], "source": [ "t, X1, X2, X3 = symbols('t, X_1, X_2, X_3')" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "This defines the deformation mapping as in the problem statement." ] }, { "cell_type": "code", "execution_count": 3, "metadata": { "collapsed": false }, "outputs": [], "source": [ "x1 = Rational(1, 2) * (X1 + X2) * exp(t) + Rational(1, 2) * (X1 - X2) * exp(-t)\n", "x2 = Rational(1, 2) * (X1 + X2) * exp(t) - Rational(1, 2) * (X1 - X2) * exp(-t)\n", "x3 = X3" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Now we compute the deformation gradient." ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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"text/latex": [ "$$\\left[\\begin{matrix}\\cosh{\\left (t \\right )} & \\sinh{\\left (t \\right )} & 0\\\\\\sinh{\\left (t \\right )} & \\cosh{\\left (t \\right )} & 0\\\\0 & 0 & 1\\end{matrix}\\right]$$" ], "text/plain": [ "⎡cosh(t) sinh(t) 0⎤\n", "⎢ ⎥\n", "⎢sinh(t) cosh(t) 0⎥\n", "⎢ ⎥\n", "⎣ 0 0 1⎦" ] }, "execution_count": 4, "metadata": {}, "output_type": "execute_result" } ], "source": [ "F = simplify(Matrix([[diff(x1, X1), diff(x1, X2), diff(x1, X3)],\n", " [diff(x2, X1), diff(x2, X2), diff(x2, X3)],\n", " [diff(x3, X1), diff(x3, X2), diff(x3, X3)]])); F" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "And the Green-Lagrange strain" ] }, { "cell_type": "code", "execution_count": 5, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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"text/latex": [ "$$\\left[\\begin{matrix}\\sinh^{2}{\\left (t \\right )} & \\frac{1}{2} \\sinh{\\left (2 t \\right )} & 0\\\\\\frac{1}{2} \\sinh{\\left (2 t \\right )} & \\sinh^{2}{\\left (t \\right )} & 0\\\\0 & 0 & 0\\end{matrix}\\right]$$" ], "text/plain": [ "⎡ 2 sinh(2⋅t) ⎤\n", "⎢sinh (t) ───────── 0⎥\n", "⎢ 2 ⎥\n", "⎢ ⎥\n", "⎢sinh(2⋅t) 2 ⎥\n", "⎢───────── sinh (t) 0⎥\n", "⎢ 2 ⎥\n", "⎢ ⎥\n", "⎣ 0 0 0⎦" ] }, "execution_count": 5, "metadata": {}, "output_type": "execute_result" } ], "source": [ "E = Rational(1, 2) * (F.T * F - eye(3)); simplify(E)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "We can immediatelly evaluate the linear \"small\" strain as well, directly with the deformation gradient." ] }, { "cell_type": "code", "execution_count": 6, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAARAAAABLCAMAAACP6iinAAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\nRU5ErkJggg==\n", "text/latex": [ "$$\\left[\\begin{matrix}\\cosh{\\left (t \\right )} - 1 & \\sinh{\\left (t \\right )} & 0\\\\\\sinh{\\left (t \\right )} & \\cosh{\\left (t \\right )} - 1 & 0\\\\0 & 0 & 0\\end{matrix}\\right]$$" ], "text/plain": [ "⎡cosh(t) - 1 sinh(t) 0⎤\n", "⎢ ⎥\n", "⎢ sinh(t) cosh(t) - 1 0⎥\n", "⎢ ⎥\n", "⎣ 0 0 0⎦" ] }, "execution_count": 6, "metadata": {}, "output_type": "execute_result" } ], "source": [ "epsilon = simplify(Rational(1,2) * (F.T + F) - eye(3)); simplify(epsilon)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "This turns our symbolic output into actual functions of $t$ that we can evaluate and plot" ] }, { "cell_type": "code", "execution_count": 7, "metadata": { "collapsed": false }, "outputs": [], "source": [ "E11_function = lambdify(t, E[0,0], \"numpy\")\n", "epsilon11_function = lambdify(t, epsilon[0,0], \"numpy\")\n", "\n", "E22_function = lambdify(t, E[1,1], \"numpy\")\n", "epsilon22_function = lambdify(t, epsilon[1,1], \"numpy\")\n", "\n", "E12_function = lambdify(t, E[0,1], \"numpy\")\n", "epsilon12_function = lambdify(t, epsilon[0,1], \"numpy\")" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Evaluating the functions" ] }, { "cell_type": "code", "execution_count": 9, "metadata": { "collapsed": false }, "outputs": [], "source": [ "t0 = numpy.linspace(0.0,0.05)\n", "\n", "E11 = E11_function(t0)\n", "epsilon11 = epsilon11_function(t0)\n", "\n", "E22 = E22_function(t0)\n", "epsilon22 = epsilon22_function(t0)\n", "\n", "E12 = E12_function(t0)\n", "epsilon12 = epsilon12_function(t0)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Plotting the results" ] }, { "cell_type": "code", "execution_count": 10, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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"text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure(1)\n", "ax = fig.add_subplot(111,xlabel='$t$', ylabel='$\\epsilon$')\n", "ax.plot(t0, E22,'k-', t0, epsilon22, 'k--',\n", " t0, E12,'b-', t0, epsilon12, 'b--');\n", "plt.grid()\n", "ax.annotate('$E_{11}, E_{22}$', xy=(0.04, 0.001), xycoords='data',\n", " xytext=(0.03, 0.01), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=0,armA=20,angleB=80,armB=10,rad=10\"),\n", " fontsize='15'\n", " )\n", "ax.annotate('$\\epsilon_{11}, \\epsilon_{22}$', xy=(0.05, 0.0008), xycoords='data',\n", " xytext=(0.042, 0.011), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=0,armA=20,angleB=80,armB=10,rad=10\"),\n", " fontsize='15'\n", " )\n", "ax.annotate('$E_{12}, \\epsilon_{12}$', xy=(0.03, 0.03), xycoords='data',\n", " xytext=(0.035, 0.02), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=90,armA=20,angleB=-80,armB=10,rad=10\"),\n", " fontsize='15'\n", " );\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Now compute the rate-of-deformation tensor, i.e. the symmetric part of the velocity gradient" ] }, { "cell_type": "code", "execution_count": 11, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAFgAAABLCAMAAADDCbAzAAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\nBUsqL0RiPGE+T4rlBUuM4Qdc7inlXZCnqwAAAABJRU5ErkJggg==\n", "text/latex": [ "$$\\left[\\begin{matrix}0 & 1 & 0\\\\1 & 0 & 0\\\\0 & 0 & 0\\end{matrix}\\right]$$" ], "text/plain": [ "⎡0 1 0⎤\n", "⎢ ⎥\n", "⎢1 0 0⎥\n", "⎢ ⎥\n", "⎣0 0 0⎦" ] }, "execution_count": 11, "metadata": {}, "output_type": "execute_result" } ], "source": [ "Fdot = F.diff(t);\n", "\n", "L = expand(Fdot * F.inv());\n", "\n", "D = simplify(Rational(1,2) * (L.T + L)); D" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "And the linear \"small\" strain-rate, $\\dot{\\epsilon}$" ] }, { "cell_type": "code", "execution_count": 12, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAMgAAABLCAMAAAACojjaAAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\nRU5ErkJggg==\n", "text/latex": [ "$$\\left[\\begin{matrix}\\sinh{\\left (t \\right )} & \\cosh{\\left (t \\right )} & 0\\\\\\cosh{\\left (t \\right )} & \\sinh{\\left (t \\right )} & 0\\\\0 & 0 & 0\\end{matrix}\\right]$$" ], "text/plain": [ "⎡sinh(t) cosh(t) 0⎤\n", "⎢ ⎥\n", "⎢cosh(t) sinh(t) 0⎥\n", "⎢ ⎥\n", "⎣ 0 0 0⎦" ] }, "execution_count": 12, "metadata": {}, "output_type": "execute_result" } ], "source": [ "epsilon_dot = epsilon.diff(t); epsilon_dot" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Now we will turn the symbolic small strain components into functions that we can evaluate in time. It's not necassary to perform this operation on the rate-of-deformation tensor because it has constant components" ] }, { "cell_type": "code", "execution_count": 13, "metadata": { "collapsed": true }, "outputs": [], "source": [ "epsilon11_dot_function = lambdify(t, epsilon_dot[0,0], \"numpy\")\n", "\n", "epsilon22_dot_function = lambdify(t, epsilon_dot[1,1], \"numpy\")\n", "\n", "epsilon12_dot_function = lambdify(t, epsilon_dot[0,1], \"numpy\")" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Evaluating the functions" ] }, { "cell_type": "code", "execution_count": 14, "metadata": { "collapsed": false }, "outputs": [], "source": [ "D11 = numpy.zeros_like(t0)\n", "epsilon11_dot = epsilon11_dot_function(t0)\n", "\n", "D22 = D11\n", "epsilon22_dot = epsilon22_dot_function(t0)\n", "\n", "D12 = numpy.ones_like(t0)\n", "epsilon12_dot = epsilon12_dot_function(t0)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Plotting the results" ] }, { "cell_type": "code", "execution_count": 15, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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"text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure(2)\n", "ax = fig.add_subplot(111,xlabel='$t$', ylabel='$\\dot{\\epsilon}$')\n", "ax.plot(t0, D11,'k-', t0, epsilon11_dot, 'k--',\n", " t0, D12,'b-', t0, epsilon12_dot, 'b--');\n", "plt.grid()\n", "ax.annotate('$D_{11}, D_{22}$', xy=(0.04, 0.0), xycoords='data',\n", " xytext=(0.025, 0.15), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=0,armA=20,angleB=80,armB=10,rad=10\"),\n", " fontsize='15'\n", " )\n", "ax.annotate('$\\dot{\\epsilon}_{11}, \\dot{\\epsilon}_{22}$', xy=(0.05, 0.03), xycoords='data',\n", " xytext=(0.04, 0.15), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=0,armA=20,angleB=80,armB=10,rad=10\"),\n", " fontsize='15'\n", " )\n", "ax.annotate('$D_{12}, \\dot{\\epsilon}_{12}$', xy=(0.04, 1.0), xycoords='data',\n", " xytext=(0.035, 0.75), textcoords='data',\n", " arrowprops=dict(arrowstyle=\"->\", connectionstyle=\"arc,angleA=90,armA=20,angleB=-80,armB=10,rad=10\"),\n", " fontsize='15'\n", " );\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Problem 2\n", "\n", "\n", "Given the following stress tensor\n", "$$\n", "\\sigma =\n", "\\begin{bmatrix}\n", " 36 & 27 & 0 \\\\\n", " 27 & -36 & 0 \\\\\n", " 0 & 0 & 18 \n", "\\end{bmatrix}\n", "$$\n", "\n", "Find:\n", "\n", "1. the components of the traction vector acting on a plane with unit normal\n", " vector $\\hat{n}^T = \\left[ 2/3, -2/3, 1/3 \\right]$\n", "\n", "1. the magnitude of the traction vector found in (a)\n", "\n", "1. its component in the direction of the normal\n", "\n", "1. a. the angle between the traction vector and the normal\n", "\n", "**Solution**" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Defining the stress tensor and normal vector" ] }, { "cell_type": "code", "execution_count": 16, "metadata": { "collapsed": false }, "outputs": [], "source": [ "sigma = Matrix([[36, 27, 0],[27, -36, 0],[0, 0, 18]])\n", "n = Matrix([Rational(2, 3), Rational(-2, 3), Rational(1, 3)])" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The traction vector is then $\\vec{t} = \\sigma^{T} \\hat{n}$ according to the Cauchy stress equation." ] }, { "cell_type": "code", "execution_count": 17, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAACUAAABLCAMAAADAvr4bAAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\n0BxNNyqMcgAAAABJRU5ErkJggg==\n", "text/latex": [ "$$\\left[\\begin{matrix}6\\\\42\\\\6\\end{matrix}\\right]$$" ], "text/plain": [ "⎡6 ⎤\n", "⎢ ⎥\n", "⎢42⎥\n", "⎢ ⎥\n", "⎣6 ⎦" ] }, "execution_count": 17, "metadata": {}, "output_type": "execute_result" } ], "source": [ "t = sigma.T * n; t" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Computing the magnitude" ] }, { "cell_type": "code", "execution_count": 18, "metadata": { "collapsed": false }, "outputs": [ { "data": { "text/plain": [ "42.8485705712571" ] }, "execution_count": 18, "metadata": {}, "output_type": "execute_result" } ], "source": [ "sympy.mpmath.mp.pretty = True\n", "magnitude = sympy.mpmath.norm(t,2); magnitude" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "And the projection in the direction of the normal." ] }, { "cell_type": "code", "execution_count": 19, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAC4AAAAZBAMAAAC86AERAAAALVBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAADAOrOgAAAADnRSTlMAu90iEM0ymauJRO92VEnJ\nOWQAAACrSURBVCgVYxBSMmBAB1xKmgwK6IJgvgUx4uaFYgwMYIIBWT1LA8O8BWCCAUWcw4GBewOY\nQBXnVmDgeAYmUMVZnwDFwQSqONCBTE+gBLK9QKF1E6AEmrgiUJgBRIDEWYKUgEA1gYGBXQAoBCZQ\n1Z8ACjOACRRx3gIGYwYwgeIvhnQGhsMQAkWcWXNmhQKYQHU/67t37xTABKo4yFIYQLEXJgikB05c\nCWv60QAAIbIqR7bpCM0AAAAASUVORK5CYII=\n", "text/latex": [ "$$\\left[\\begin{matrix}-22\\end{matrix}\\right]$$" ], "text/plain": [ "[-22]" ] }, "execution_count": 19, "metadata": {}, "output_type": "execute_result" } ], "source": [ "t.T * n" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The angle between the normal and the traction vector (in radians)" ] }, { "cell_type": "code", "execution_count": 20, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAJ8AAAAPBAMAAAAIUwCQAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nYII=\n", "text/latex": [ "$$2.10998044394962$$" ], "text/plain": [ "2.10998044394962" ] }, "execution_count": 20, "metadata": {}, "output_type": "execute_result" } ], "source": [ "acos(((t / magnitude).T * n)[0])" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "or in degree" ] }, { "cell_type": "code", "execution_count": 21, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAJ8AAAAPBAMAAAAIUwCQAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA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\nTkSuQmCC\n", "text/latex": [ "$$120.892974293453$$" ], "text/plain": [ "120.892974293453" ] }, "execution_count": 21, "metadata": {}, "output_type": "execute_result" } ], "source": [ "_ * 180. / numpy.pi" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Problem 3\n", "\n", "Given the following stress tensor\n", "$$\n", "\\sigma =\n", "\\begin{bmatrix}\n", " 18 & 0 & 24 \\\\\n", " 0 & -50 & 0 \\\\\n", " 24 & 0 & 32\n", "\\end{bmatrix}\n", "$$\n", " \n", "Find:\n", "\n", "1. the principle stresses $\\sigma_{I}, \\sigma_{II}, \\sigma_{III}$\n", "\n", "1. the three invariants $I_{1}, I_{2}, I_{3}$\n", "\n", "1. the deviatoric stress\n", "\n", "1. the two nonzero invariants of the deviatoric stress, i.e. $J_{2}, J_{3}$\n", "\n", "**Solution**" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Defining the stress tensor" ] }, { "cell_type": "code", "execution_count": 22, "metadata": { "collapsed": false }, "outputs": [], "source": [ "sigma = Matrix([[18, 0, 24],[0, -50, 0],[24, 0, 32]])" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Here we use sympy to diagonalize (or find the eigenvalues, they are shown on the diagonal of the matrix. We then define $\\sigma_I > \\sigma_{II} > \\sigma_{III}$ accordingly." ] }, { "cell_type": "code", "execution_count": 23, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAH0AAABLCAMAAABqfXinAAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\nJ4TqG0mnMdrmk+pNAAAAAElFTkSuQmCC\n", "text/latex": [ "$$\\left[\\begin{matrix}-50 & 0 & 0\\\\0 & 0 & 0\\\\0 & 0 & 50\\end{matrix}\\right]$$" ], "text/plain": [ "⎡-50 0 0 ⎤\n", "⎢ ⎥\n", "⎢ 0 0 0 ⎥\n", "⎢ ⎥\n", "⎣ 0 0 50⎦" ] }, "execution_count": 23, "metadata": {}, "output_type": "execute_result" } ], "source": [ "_, D = sigma.diagonalize();\n", "sigma1 = D[2,2];sigma2 = D[1,1]; sigma3 = D[0,0]; D" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The first, second, and third invariants" ] }, { "cell_type": "code", "execution_count": 24, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAAoAAAAOBAMAAADkjZCYAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAv3aB7AAAAD3RSTlMAEJmJdjLNVN0iZu+7\nq0QgoRR7AAAAVklEQVQIHWNgEDJRZWBgSGeQmMDAtYGBOYGB5wID+0cG/gsMfN8Z5BUY+L4wzDdg\nYP0MJeUNQCL8Cgzs3xk4DjBwfWRg2cDAlMDA0M4gHcDAIOxylQEA9FISlFfRJtkAAAAASUVORK5C\nYII=\n", "text/latex": [ "$$0$$" ], "text/plain": [ "0" ] }, "execution_count": 24, "metadata": {}, "output_type": "execute_result" } ], "source": [ "I1 = sigma1 + sigma2 + sigma3; I1" ] }, { "cell_type": "code", "execution_count": 25, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAADcAAAAOBAMAAAB5gJkQAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAv3aB7AAAAD3RSTlMAEM3dMiKZu6uJRO92\nVGZ6zyUAAAAA80lEQVQYGU3Qv0oDMQCA8S/XBqsWCU4+gHtBkY7eG1gRnIuDUpcWHHS0FVwrgmKh\noG9QUDt1uRssBZebXPsAgh2EYruc+WPjZfhI8ksIBP6GPD4PCeL8KaI2DF0WxgbLc1bTNCJIxI6L\nxyYMCB7e4BNuXTy+QDssmOUFjJWNx5Ja4A/0EhuPerKrCl/DUEw1xiZRBldmLCk5lzPYuzO5yWCu\nYRZnWVzfNmNTb5/Yg/V9fakXm0R2w6Z4CS14fNLPjRObf/xAVp6hrsowcfGYr1KsVGGLdzhy8XjQ\nub/ikLU+uUS8ungspek3snatEN2R/niTX7UxUXc+k3IOAAAAAElFTkSuQmCC\n", "text/latex": [ "$$-2500$$" ], "text/plain": [ "-2500" ] }, "execution_count": 25, "metadata": {}, "output_type": "execute_result" } ], "source": [ "I2 = sigma1 * sigma2 + sigma1 * sigma3 + sigma2 * sigma3; I2" ] }, { "cell_type": "code", "execution_count": 26, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAAoAAAAOBAMAAADkjZCYAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAv3aB7AAAAD3RSTlMAEJmJdjLNVN0iZu+7\nq0QgoRR7AAAAVklEQVQIHWNgEDJRZWBgSGeQmMDAtYGBOYGB5wID+0cG/gsMfN8Z5BUY+L4wzDdg\nYP0MJeUNQCL8Cgzs3xk4DjBwfWRg2cDAlMDA0M4gHcDAIOxylQEA9FISlFfRJtkAAAAASUVORK5C\nYII=\n", "text/latex": [ "$$0$$" ], "text/plain": [ "0" ] }, "execution_count": 26, "metadata": {}, "output_type": "execute_result" } ], "source": [ "I3 = sigma1 * sigma2 * sigma3; I3" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "The deviatoric stress" ] }, { "cell_type": "code", "execution_count": 27, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAIgAAABLCAMAAACcGD96AAAAPFBMVEX///8AAAAAAAAAAAAAAAAA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\ngg==\n", "text/latex": [ "$$\\left[\\begin{matrix}18 & 0 & 24\\\\0 & -50 & 0\\\\24 & 0 & 32\\end{matrix}\\right]$$" ], "text/plain": [ "⎡18 0 24⎤\n", "⎢ ⎥\n", "⎢0 -50 0 ⎥\n", "⎢ ⎥\n", "⎣24 0 32⎦" ] }, "execution_count": 27, "metadata": {}, "output_type": "execute_result" } ], "source": [ "Sij = sigma - 1. / 3. * I1 * eye(3); Sij" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Here we perform the same procedure on the deviatoric stress and compute the invariants." ] }, { "cell_type": "code", "execution_count": 28, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAADcAAAAOBAMAAAB5gJkQAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAv3aB7AAAAD3RSTlMAEM3dMiKZu6uJRO92\nVGZ6zyUAAAAA80lEQVQYGU3Qv0oDMQCA8S/XBqsWCU4+gHtBkY7eG1gRnIuDUpcWHHS0FVwrgmKh\noG9QUDt1uRssBZebXPsAgh2EYruc+WPjZfhI8ksIBP6GPD4PCeL8KaI2DF0WxgbLc1bTNCJIxI6L\nxyYMCB7e4BNuXTy+QDssmOUFjJWNx5Ja4A/0EhuPerKrCl/DUEw1xiZRBldmLCk5lzPYuzO5yWCu\nYRZnWVzfNmNTb5/Yg/V9fakXm0R2w6Z4CS14fNLPjRObf/xAVp6hrsowcfGYr1KsVGGLdzhy8XjQ\nub/ikLU+uUS8ungspek3snatEN2R/niTX7UxUXc+k3IOAAAAAElFTkSuQmCC\n", "text/latex": [ "$$-2500$$" ], "text/plain": [ "-2500" ] }, "execution_count": 28, "metadata": {}, "output_type": "execute_result" } ], "source": [ "_, D = Sij.diagonalize();\n", "Sij1 = D[2,2]; Sij2 = D[1,1]; Sij3 = D[0,0]; \n", "\n", "J2 = Sij1 * Sij2 + Sij1 * Sij3 + Sij2 * Sij3; J2" ] }, { "cell_type": "code", "execution_count": 29, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": "iVBORw0KGgoAAAANSUhEUgAAAAoAAAAOBAMAAADkjZCYAAAAMFBMVEX///8AAAAAAAAAAAAAAAAA\nAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAv3aB7AAAAD3RSTlMAEJmJdjLNVN0iZu+7\nq0QgoRR7AAAAVklEQVQIHWNgEDJRZWBgSGeQmMDAtYGBOYGB5wID+0cG/gsMfN8Z5BUY+L4wzDdg\nYP0MJeUNQCL8Cgzs3xk4DjBwfWRg2cDAlMDA0M4gHcDAIOxylQEA9FISlFfRJtkAAAAASUVORK5C\nYII=\n", "text/latex": [ "$$0$$" ], "text/plain": [ "0" ] }, "execution_count": 29, "metadata": {}, "output_type": "execute_result" } ], "source": [ "J3 = Sij1 * Sij2 * Sij3; J3" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Problem 4\n", "\n", "Show that\n", "$$\n", " \\frac{\\partial J_2}{\\partial \\sigma_{ij}} = S_{ij}\n", "$$\n", "where $J_2$ is the second invariant of the deviatoric stress tensor, $S_{ij}$.\n", " \n", "\n", "**Solution**\n", "\n", "\\begin{align}\n", "\\frac{\\partial J_2}{\\partial \\sigma_{ij}} &= \\frac{\\partial}{\\partial \\sigma_{ij}}\\left(J_2\\right) \\\\\n", " &= \\frac{\\partial}{\\partial \\sigma_{ij}}\\left(\\frac{1}{2}S_{kl}S_{kl}\\right) \\\\\n", " &= \\frac{1}{2} \\left(\\frac{\\partial}{\\partial \\sigma_{ij}}\\left(S_{kl}\\right)S_{kl} + S_{kl}\\frac{\\partial}{\\partial \\sigma_{ij}}\\left(S_{kl}\\right) \\right) \\\\ \n", " &= S_{kl}\\frac{\\partial}{\\partial \\sigma_{ij}}\\left(S_{kl}\\right) \\\\\n", " &= S_{kl}\\frac{\\partial}{\\partial \\sigma_{ij}}\\left(\\sigma_{kl} - \\frac{1}{3} \\sigma_{mm}\\delta_{kl}\\right) \\\\\n", " &= S_{kl}\\left(\\delta_{il}\\delta_{kj} - \\frac{1}{3} \\delta_{im}\\delta_{jm}\\delta_{kl}\\right) \\\\\n", " &= S_{kl}\\left(\\delta_{il}\\delta_{kj} - \\frac{1}{3} \\delta_{ij}\\delta_{kl}\\right) \\\\\n", " &= S_{ij} - \\frac{1}{3} S_{kk} \\delta_{ij} \\\\\n", " &= S_{ij}\n", "\\end{align} \n", "\n", "because\n", "\n", "$$\n", "S_{kk} =0\n", "$$\n", "\n", "by definition of $S$ being a deviatoric tensor." ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Problem 5\n", " \n", "For each of the following stress states (values not given are zero), plot the three Mohr's circles and\n", "determine the maximum shear stress.\n", " \n", "1. Uniaxial tension $\\sigma_{11} = 40$\n", "\n", "1. Biaxial stress $\\sigma_{11} = -10, \\sigma_{22} = 30$\n", "\n", "1. Hydrostatic tension of magnitude 100 psi\n", " \n", "1. $\\sigma_{11} = -60, \\sigma_{22} = 100, \\sigma_{33} = 40$\n", "\n", "1. $\\sigma_{11} = 10, \\sigma_{22} = 40, \\sigma_{21} = \\sigma_{12} = 20$\n", "\n", "\n", "**Solution**" ] }, { "cell_type": "code", "execution_count": 30, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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ypnLbtsF777ltktu0gQUL3MCGjz+Gc8+14demYlYjCaFcrpFUVbxP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\nAAAASUVORK5CYII=\n", "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure()\n", "ax = fig.add_subplot(111,xlabel='$\\sigma_n$', ylabel='$\\sigma_t$',title='Uniaxial tension, $\\sigma_{11}=40$')\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)\n", "ax.axhline(0, color='black', lw=2)\n", "ax.axvline(0, color='black', lw=2)\n", "ax.annotate('$\\sigma_{II},\\sigma_{III}$', xy=(0.04, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{I}$', xy=(40, 1.0), xycoords='data', fontsize='15');\n", "circ = plt.Circle((0.5*(40-0), 0), radius=20, fill=False, color='b')\n", "ax.add_patch(circ)\n", "plt.axis('equal')\n", "plt.grid()\n", "plt.show()" ] }, { "cell_type": "code", "execution_count": 31, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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w4cMB/rpfVpVQx0iSEZHrgD9U9e74cl7ESP7801rpLl1qWSZVYelSa8f7wAOw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\nSSwWo6CgAFXz3777LrRtW/X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"text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure()\n", "ax = fig.add_subplot(111,xlabel='$\\sigma_n$', ylabel='$\\sigma_t$',title='Biaxial stress, $\\sigma_{11}=-10, \\sigma_{22}=30$')\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)\n", "ax.axhline(0, color='black', lw=2)\n", "ax.axvline(0, color='black', lw=2)\n", "ax.annotate('$\\sigma_{III}$', xy=(-10, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{II}$', xy=(0.04, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{I}$', xy=(30, 1.0), xycoords='data', fontsize='15');\n", "circ1 = plt.Circle((0.5*(30+(-10)), 0), radius=20, fill=False, color='b')\n", "circ2 = plt.Circle((0.5*(30+(0)), 0), radius=15, fill=False, color='b')\n", "circ3 = plt.Circle((-5, 0), radius=5, fill=False, color='b')\n", "ax.add_patch(circ1)\n", "ax.add_patch(circ2)\n", "ax.add_patch(circ3)\n", "plt.axis('equal')\n", "plt.grid()\n", "plt.show()" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "**For the hydostatic tension case, there are no Mohr's circles to draw because $\\sigma_I = \\sigma_{II} = \\sigma_{III}$**" ] }, { "cell_type": "code", "execution_count": 32, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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gZMs0WevDELuSHwXmxJVFjFHAObH35wCvZlq2sPDZZ+a7GDfO7LGuLKJLu3aW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\nbKj6wQfJP//lF9W6dVVXrcq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"text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure()\n", "ax = fig.add_subplot(111,xlabel='$\\sigma_n$', ylabel='$\\sigma_t$',\n", " title='$\\sigma_{11} = -60, \\sigma_{22} = 100, \\sigma_{33} = 40$')\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)\n", "ax.axhline(0, color='black', lw=2)\n", "ax.axvline(0, color='black', lw=2)\n", "ax.annotate('$\\sigma_{III}$', xy=(-60, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{II}$', xy=(40, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{I}$', xy=(100, 1.0), xycoords='data', fontsize='15');\n", "circ1 = plt.Circle((0.5*(100+(-60)), 0), radius=80, fill=False, color='b')\n", "circ2 = plt.Circle((70, 0), radius=30, fill=False, color='b')\n", "circ3 = plt.Circle((-10, 0), radius=50, fill=False, color='b')\n", "ax.add_patch(circ1)\n", "ax.add_patch(circ2)\n", "ax.add_patch(circ3)\n", "plt.axis('equal')\n", "plt.grid()\n", "plt.show()" ] }, { "cell_type": "code", "execution_count": 33, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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"text/latex": [ "$$\\left[\\begin{matrix}0 & 0 & 0\\\\0 & 0 & 0\\\\0 & 0 & 50\\end{matrix}\\right]$$" ], "text/plain": [ "⎡0 0 0 ⎤\n", "⎢ ⎥\n", "⎢0 0 0 ⎥\n", "⎢ ⎥\n", "⎣0 0 50⎦" ] }, "execution_count": 33, "metadata": {}, "output_type": "execute_result" } ], "source": [ "sigma = Matrix([[10,20,0],[20,40,0],[0,0,0]])\n", "_, D = sigma.diagonalize(); D" ] }, { "cell_type": "code", "execution_count": 34, "metadata": { "collapsed": false }, "outputs": [ { "data": { "image/png": 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ZE/3KV+DQQ+G22+K8forjpEz5i5HruutgyJDm709xrFLMVIxkC8lqdARm5yzP\nBraIlKWmDRkCN9wQrusgkrLXXw/XHjnmmNhJ6tM6MV/czMYC7Zu463x3H1XAt2qyGTJ48GA6d+4M\nQNu2benRowe9e/cGVvwlUO/LWU3d7w4bbdSbJ56AVq0qmy+7Lvb4FDJeWo73/l1wQQN9+8L666/+\n8bnZypmnmpYbGhq4LTP1kP28LFSyzfYsMxsP/CTbbDezoQDufmVm+VHgEnd/ttHz1GzPQ3PN9qxb\nboHRo2HEiEqmEsnf55/DVlvBs8+GZruUptaa7blyf6iRwLFm1srMtga6As/FiVW4xn8Zpe7448NJ\nHN9+u7Kvm+I4KVP+Kpnrnntgjz3WXERSHKsUMxUj2UJiZkeY2b+AvYDRZvYIgLtPBe4FpgKPAEO0\n6VE+G24IP/gBXHZZ7CQiq1q8GH75S/jpT2MnqW/JT20VS1Nb+VnT1BbA/PnhUrxPPw3bbVepZCJr\ndv318NBD8NhjsZPUjmKmtlRI6lw+hQTg6qvDHPT991cilcia/ec/4Q+c0aOhZ8/YaWpHLfdIaka1\nzomeeWYoJM8+u+bHtoQUx0mZ8leJXMOGwf77519EUhyrFDMVI+ruv1I9WreGSy6BoUNh3LhwlmCR\nWD78MBSSCRNiJxHQ1Fbdy3dqC2Dp0nBN99/9Dg46qNzJRJr3k5+E3X6vvz52ktqjHkkOFZL8FFJI\nIPRILr8cJk6EtTQxKhG8806YznrllXBuLWlZ6pFUgWqfEz3ySFhnnbDvfjmlOE7KlL9y5rrkEjjt\ntMKLSIpjlWKmYqhHIgUxC3PT3/52mN5q1y52IqknTz4JTzwRtkYkHZraqnOFTm1lnXMOzJ0Ld91V\njlQiq/r0U9h559AXOfjg2Glql3okOVRI8lNsIfnsM+jRA666Co44ohzJRFb2wx+GI9lvvTV2ktqm\nHkkVqJU50Q02gOHD4fTTw2V5W1qK46RM+WvpXE8+CQ8/DL/5TfHfI8WxSjFTMVRIpGj77APHHhsO\nVhQpl08/he9/H26+Gdq2jZ1GmqKprTpX7NRWlqa4pNw0pVVZ6pHkUCHJT6mFBOAf/4Cjj4YpU7QX\nl7SsJ5+EwYPD75a2RipDPZIqUCtzormyU1wnn9xyl+VNcZyUKX8tkev99+Gkk1puSivFsUoxUzFU\nSKRFXHFFOP/RpZfGTiK1YPHicKzSd7+rXX2rgaa26lxLTG1lzZsXrlT361+HqS6RYrjDqaeGLZIH\nHtCpeCrgy57IAAAP90lEQVStmKktHdkuLWbzzcO13fv1gy5ddI0IKc7118Mzz8A//6kiUi30NlVY\nrcyJNqdnT7juOjj88LCFUqwUx0mZ8ldsrnHjwmWdR46ENm3SyFROKWYqhgqJtLhjjoHvfQ+OOirM\ndYvk48034fjjw2l3ttkmdhophHokda4leyS5li8PZwredFO45RZdCEtW79NPYe+9wzEjp58eO019\n03EkOVRI8lOuQgLhw+HrX4cTToCf/7zFv73UiMWLw1Rop05w0036oyM2HUdSBWplTjQfbdrAI4+E\nD4c//KGw56Y4TsqUv3xzLVkSjkFq1Sr01spZRFIcqxQzFUN7bUlZdeoUGqj77w/rrw+nnBI7kaRi\n2bLQS1u4EB58ENZdN3YiKZamtupcOae2cs2cCX36hMv0DhpU1peSKrBsWTgTwr/+Fc7q27p17ESS\npeNIJFldu8LYsXDAAWFOXFsm9Wvp0nD+rHffVRGpFeqRVFitzIkWY/vtoaEhHCfwxz+u/rEpjpMy\n5a+5XIsXw3HHwQcfwOjRsOGG8TPFlGKmYmiLRCqqa1d46ino2zecgv5nP9NeOvVi4cJwjBGEAw7X\nWy9uHmk56pHUuUr1SBqbPRsOOgj22w9+//uw147UrjlzwvVqvvY1uO02vd8pq6ndf83sGjObZmYv\nmdkDZvblnPvOM7OZZjbdzPrFzCnF6dQpnEtpzpzQN/ngg9iJpFyeey6czHPgQPjrX1VEalGyhQR4\nHNjB3XcBZgDnAZhZd+A7QHegP3C9maX8c6ykVuZEW8KXvhRO8rjffrD77vDSSyvuS3GclCl/2Vx3\n3gmHHhpOxHj++XGnMVMcqxQzFSPZD2B3H+vu2cskPQt0ynw9ELjb3Ze4+yzgdWCPCBGlBay1Vtgl\n+Morw5bJ/ffHTiQtYdkyOPdc+MUvYPx4GDAgdiIpp6rokZjZKELxuMvM/gBMcPe/Zu77E/CIu9/f\n6DnqkeQhVo+kKZMmhXn0k06Ciy/WKcSr1YIF4eSLixbBvffq8svVpup6JGY21symNHE7LOcxFwCL\n3f2u1Xyr+J+CUrJevcJ8+tix4cJY8+fHTiSFeuUV2GuvcD2aRx9VEakXUXf/dfcDV3e/mQ0GDgH6\n5qx+F9gyZ7lTZt0qBg8eTOfOnQFo27YtPXr0oHfv3sCKuclKL2fXxXr9pvLEfP2mlseNgwMPHEa3\nbj0YPrw3hx6aRr7Jkydz9tlnRx+f3OXsuth5nnyygbvugpEje3PNNbBgwTD+8Y/4/9/0/q15uaGh\ngdtuuw3gi8/Lgrl7kjdCI/1VYNNG67sDk4FWwNbAG2Sm6Bo9zlM0fvz42BFWQtiaix1jFePHj/eG\nBvdttnH/3vfcP/44dqL03jv3NDJNmeLeq5d7v37ub78d1qWQqzFlyk/m86Cgz+tkeyRmNpNQLD7O\nrPqnuw/J3Hc+cBKwFDjL3R9r4vme6s+WkpR6JE35739h6NBwUr8bbwx7AEkali6Fq66CYcPgiivC\nubN0cGn10/VIcqiQ5Cf1QpL11FOhCb/vvuGDa+ONYyeqb6+8Es6Xtckm8Kc/wVZbxU4kLaXqmu31\nqHFvQprWeJz23x9efjkce7LTTmE34UrXvhTfu0pn+vzzcK60Pn3g1FPhsceaLiIaq/ykmKkYKiRS\nNTbcMFwg669/DR9me+8dTgIp5bd0abhkcteuMHly2FX7lFM0lSWBprbqXLVMbTW2fDnccw9ceCFs\nuy386lfQs2fsVLXHHR54AC64ADp0CAeO7rln7FRSTuqR5FAhyU+1FpKsxYvh5pvD0fF9+oQtla99\nLXaq2jBuXNjRYenS0Ezv109bIPVAPZIqUCtzouWW7zi1agVnnBGuwLj99uGv5dNPh/fei5epksqR\nadKkUDR+8AM45xyYODGcqbmQIlIvY1WqFDMVQ4VEasJGG8FFF8G0aaG4dO8eLqD09NOVb8pXo0WL\n4K67wl5xAwfC4YfD1Klw7LE6VY2smaa26ly1T201Z8ECuP32cNbZVq1gyBA44QRo0yZ2srS8/Tbc\ndBPcemvYG27IkHCCxXV0ybu6paktkYy2beGss2D69HDcyRNPwFe/Gqa9Xnkldrq4li8P58EaMAB2\n3TVcqfKpp8IYHXmkiogUToWkwmplTrTcWmqczMJlfe+/PxyHsummYf4/e2XGt96qfKaWlG+m5cvD\nCTEvvBC6dYPzzguF5J13QqHdbrs4uSpJmcpHhUTqRqdOcOmlYTrnpz8Nx0PsuWeY0rngAnj22fCB\nWys+/xwefjg0zbfYAgYNgiVLwnE4L7wA3/9+ODZHpFTqkdS5Wu2R5GvZslBARo2CkSPho4/gsMPC\nrW/f6vugnTsXRo8OP8+4cWHqasCA8PN07Ro7nVQDHUeSQ4UkP/VeSBp7/fUVReXZZ8N1NXr1gt12\nC//usgu0bh07ZfDRR2FX3UmTwi66kyaFnQz69QvF4+CDdT0QKZwKSY5UC0lDQ8MX1wRIQaqFJIVx\nWrQIpkxZ8WHd0NDA7Nm9vyguvXrBDjtAx47hVo49wtxDwZgzB2bPDte1zxaN+fNh660b6Nu39xfF\nrkuXNHbXTeH9a0yZ8lNMIdH+GSLNWG+98OG8225huaEhnN8rt7jce284+DF7AGTHjuFUItl/O3QI\nDf511w23ddYJN/dwxPjSpaFvsWgRzJsXCsZ77634d+7ccIxM9nvuvDN8+9vhSPMuXeDvf4fEPoek\nDmmLpM6lukVSjT79dNVCMGdO2KLILRpLloSthnXWWVFcWrWCzTdftRC1bw/rrx/7J5N6oqmtHCok\n+VEhEZFcOiCxCtTKfuPlluI4KVP+UsylTOWjQiIiIiXR1Fad09SWiOTS1JaIiFScCkmF1cqcaLml\nOE7KlL8UcylT+aiQiIhISdQjqXPqkYhILvVIRESk4lRIKqxW5kTLLcVxUqb8pZhLmcpHhUREREqi\nHkmdU49ERHKpRyIiIhWXbCExs8vM7CUzm2xmT5rZljn3nWdmM81supn1i5mzULUyJ1puKY6TMuUv\nxVzKVD7JFhLganffxd17ACOASwDMrDvwHaA70B+43sxS/jlWMnny5NgRqkKK46RM+UsxlzKVT7If\nwO7+ac7iRsCHma8HAne7+xJ3nwW8DuxR4XhFW7BgQewIVSHFcVKm/KWYS5nKJ+krJJrZ5cB3gc9Z\nUSw6AhNyHjYb2KLC0UREJCPqFomZjTWzKU3cDgNw9wvcfStgODBsNd+qanY5mjVrVuwIVSHFcVKm\n/KWYS5nKpyp2/zWzrYAx7r6jmQ0FcPcrM/c9Clzi7s82ek76P5iISIIK3f032aktM+vq7jMziwOB\nFzNfjwTuMrNrCVNaXYHnGj+/0IEQEZHiJFtIgCvMbFtgGfAG8EMAd59qZvcCU4GlwBAdeSgiEk9V\nTG2JiEi6kt39t1hmdo2ZTcsczPiAmX05574oBzKa2dFm9qqZLTOzXRvdF+3gSjPrn3ndmWb280q+\ndqMcfzazeWY2JWfdJpmdMWaY2eNm1rbCmbY0s/GZ9+0VM/tR7Fxmtr6ZPZs5SHeqmV0RO1NOtrXN\n7EUzG5VCJjObZWYvZzI9l0imtmZ2X+bzaaqZ7ZlApm0zY5S9fWJmPyo0V80VEuBxYAd33wWYAZwH\n0Q9knAIcAfw9d2XMTGa2NvDHzOt2B44zs+0r8dpNGJ7JkWsoMNbduwFPZpYraQnwY3ffAdgLOD0z\nPtFyuftCoE/mIN2dgT5mtm/MTDnOIkw3Z6c4YmdyoLe793T37KEDsTP9jrDT0PaE92967Ezu/lpm\njHoCvYDPgAcLzuXuNXsjfHj/JfP1ecDPc+57FNirwnnGA7vmLEfLBOwNPJqzPBQYGvG96gxMyVme\nDmye+bo9MD3y79II4IBUcgEbAM8DO8TOBHQCngD6AKNSeP+At4B2jdZFywR8GXizifVJ/D5lXr8f\n8HQxuWpxiyTXScCYzNcdCQcvZqVwIGPMTFsA/4r02vnY3N3nZb6eB2weK4iZdQZ6As8SOZeZrWVm\nkzOvPd7dX42dCfgt8DNgec662JkceMLMJprZKQlk2hr4wMyGm9kLZnaLmW0YOVNjxwJ3Z74uKFfK\ne201y8zGEqpkY+e7e3aO9gJgsbvftZpv1WJ7GuSTKU+V2vuhavaycHePdVyQmW0E3A+c5e6fmq3Y\nqzxGLndfDvTI9P4eM7M+je6vaCYzOxR4391fNLPeTT0m0vu3j7u/Z2abAWPNbHrkTOsAuwJnuPvz\nZjaMRtNFkX/PWwGHAav0SvPJVZWFxN0PXN39ZjYYOATom7P6XWDLnOVOmXUVydSMsmYq8LW3ZOWt\no9jmmVl7d59rZh2A9ysdwMzWJRSRO919RCq5ANz9EzMbTZjXjpnp68AAMzsEWB/4kpndGTkT7v5e\n5t8PzOxBwimWYmaaDcx29+czy/cRprbnpvD7BBwMTHL3DzLLBY1VzU1tmVl/wmb2QA/NyayRwLFm\n1srMtqaZAxkrETGRTBOBrmbWOfPXyHcyeVIxEhiU+XoQoUdRMRY2PW4Fprp77ul5ouUys02ze8+Y\nWWvgQMKButEyufv57r6lu29NmBoZ5+7fjZnJzDYwszaZrzckzP1PiZnJ3ecC/zKzbplVBwCvAqNi\nZWrkOFZMa0GhYxWrsVPGhtFM4G3Cf7AXgetz7jufcLbg6cBBFcx0BKEf8TkwF3gkdqbMax8MvJZ5\n/fMivmd3A3OAxZlxOhHYhNDAnUHYE69thTPtS5jzn5zzu9Q/Zi5gJ+CFTKaXgZ9l1kcdq5x8+wMj\nY2ci9CMmZ26vZH+3Y48TsAthB4mXgAcIDfjo7x2wIeHs6m1y1hWUSwckiohISWpuaktERCpLhURE\nREqiQiIiIiVRIRERkZKokIiISElUSEREpCQqJCIiUhIVEhERKYkKiUiZmNlOZvZQ5mJBy5u4DYid\nUaQlqJCIlEHmJIYTCCfHHEQ40+ti4EbCeZb2Z8UlDkSqWlWe/VckZWbWFbgXONvdb8lZvz2wvbuP\nixZOpAy0RSLS8q4gXO3xlkbrP6Dpa9aIVDUVEpEWlDnN+wDg9ibu7kY4M7VITVEhEWlZ2xKmjFe6\nrkzmuhh9gAdjhBIpJxUSkZY1P/Pvfxqt/yHhmivDKxtHpPxUSERakLvPAJ4h7JkFgJntD5wOHOnu\ni2NlEykXXdhKpIWZ2VeA3xOuOrcOsBS41FdcDzv7uE0IV4Pcl9Cg3xloA2zh7j+taGiREqiQiERi\nZicTmvJTCIXmHjP7EvCuu7eJm04kf5raEonn/4BNgQ3d/Z7Mul7AtHiRRAqnQiISibv/m9BLeTJn\n9dFAdstEpCqokIjE9UUhMTMjFJK/Ad+PGUqkECokInF1AcYCeGhYTgD6AU/HDCVSCDXbRUSkJNoi\nERGRkqiQiIhISVRIRESkJCokIiJSEhUSEREpiQqJiIiURIVERERKokIiIiIlUSEREZGS/H8HPGhD\nj9YSYQAAAABJRU5ErkJggg==\n", "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "fig = plt.figure()\n", "ax = fig.add_subplot(111,xlabel='$\\sigma_n$', ylabel='$\\sigma_t$',\n", " title='$\\sigma_{11} = 10, \\sigma_{22} = 40, \\sigma_{21} = \\sigma_{12} = 20$')\n", "ax.xaxis.label.set_size(20)\n", "ax.yaxis.label.set_size(20)\n", "ax.axhline(0, color='black', lw=2)\n", "ax.axvline(0, color='black', lw=2)\n", "ax.annotate('$\\sigma_{II},\\sigma_{III}$', xy=(0.04, 1.0), xycoords='data', fontsize='15');\n", "ax.annotate('$\\sigma_{I}$', xy=(50, 1.0), xycoords='data', fontsize='15');\n", "circ = plt.Circle((0.5*(50-0), 0), radius=25, fill=False, color='b')\n", "ax.add_patch(circ)\n", "plt.axis('equal')\n", "plt.grid()\n", "plt.show()" ] } ], "metadata": { "kernelspec": { "display_name": "Python 2", "language": "python", "name": "python2" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 2 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", "version": "2.7.10" } }, "nbformat": 4, "nbformat_minor": 0 }