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sora committed 2022-04-07 18:46:57 +02:00
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{
"cells": [
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import numpy as np\n",
"import torch\n",
"import igl\n",
"\n",
"import meshplot as mp\n",
"import sys as _sys\n",
"_sys.path.append(\"../src\")\n",
"from elasticenergy import *\n",
"from elasticsolid import *\n",
"from adjoint_sensitivity import *\n",
"from vis_utils import *\n",
"from objectives import *\n",
"from harmonic_interpolator import *\n",
"from shape_optimizer import *\n",
"\n",
"from utils import *\n",
"\n",
"shadingOptions = {\n",
" \"flat\":True,\n",
" \"wireframe\":False, \n",
"}\n",
"\n",
"rot = np.array(\n",
" [[1, 0, 0 ],\n",
" [0, 0, 1],\n",
" [0, -1, 0 ]]\n",
")\n",
"\n",
"torch.set_default_dtype(torch.float64)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Create the deformed object\n",
"\n",
"## Load the mesh"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "9ae930440a43419c88fd82d71d7a6fa4",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-1.987469…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"data": {
"text/plain": [
"<meshplot.Viewer.Viewer at 0x7f86840382e0>"
]
},
"execution_count": 2,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/dinosaur.obj\")\n",
"# vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/beam.obj\")\n",
"\n",
"aabb = np.max(vNP, axis=0) - np.min(vNP, axis=0)\n",
"length_scale = np.mean(aabb)\n",
"\n",
"\n",
"v, t = torch.tensor(vNP), torch.tensor(tNP)\n",
"eNP = igl.edges(tNP)\n",
"beNP = igl.edges(igl.boundary_facets(tNP))\n",
"\n",
"bvNP, ivNP = get_boundary_and_interior(v.shape[0], tNP)\n",
"\n",
"mp.plot(vNP @ rot.T, np.array(tNP), shading=shadingOptions)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add some physical characteristics"
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Pinned vertices: [ 46 47 50 59 60 62 64 65 88 89 91 98 99 102 103 104]\n"
]
}
],
"source": [
"rho = 131 # [kg.m-3], if aabb[0] ~ 14m, and m_tot = 6000kg\n",
"young = 3e8 # [Pa] \n",
"poisson = 0.2\n",
"\n",
"# Find some of the lowest vertices and pin them\n",
"minZ = torch.min(v[:, 2])\n",
"pin_idx = torch.arange(v.shape[0])[v[:, 2] < minZ + 0.01*aabb[2]]\n",
"vIdx = np.arange(v.shape[0])\n",
"pin_idx = vIdx[np.in1d(vIdx, bvNP) & np.in1d(vIdx, pin_idx)]\n",
"print(\"Pinned vertices: {}\".format(pin_idx))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Initial guess\n",
"\n",
"The idea is that we start deforming the mesh by inverting gravity."
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "1ee888e94cd641f4bbbce4b051acccfb",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-2.468079…"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# Inverted gravity\n",
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = + rho * 9.81\n",
"\n",
"# Gravity going in the wrong direction\n",
"\n",
"ee = NeoHookeanElasticEnergy(young, poisson)\n",
"\n",
"v = HarmonicInterpolator(v, t, ivNP).interpolate(v[bvNP])\n",
"solid_init = ElasticSolid(v, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"\n",
"solid_init.find_equilibrium()\n",
"plot_torch_solid(solid_init, beNP, rot, length_scale)\n",
"\n",
"# Use these as initial guesses\n",
"v_init_rest = solid_init.v_def.clone().detach()\n",
"v_init_def = solid_init.v_rest.clone().detach()\n",
"\n",
"# v_init_rest = solid_init.v_rest.clone().detach()\n",
"# v_init_def = solid_init.v_def.clone().detach()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Inverse design\n"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {
"scrolled": false
},
"outputs": [
{
"ename": "TypeError",
"evalue": "unsupported format string passed to NoneType.__format__",
"output_type": "error",
"traceback": [
"\u001b[0;31m---------------------------------------------------------------------------\u001b[0m",
"\u001b[0;31mTypeError\u001b[0m Traceback (most recent call last)",
"\u001b[0;32m/tmp/ipykernel_46/1868162750.py\u001b[0m in \u001b[0;36m<module>\u001b[0;34m\u001b[0m\n\u001b[1;32m 14\u001b[0m \u001b[0msolid_\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mupdate_def_shape\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0mv_init_def\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n\u001b[1;32m 15\u001b[0m \u001b[0;34m\u001b[0m\u001b[0m\n\u001b[0;32m---> 16\u001b[0;31m \u001b[0moptimizer\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0mShapeOptimizer\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0msolid_\u001b[0m\u001b[0;34m,\u001b[0m \u001b[0mvt_surf\u001b[0m\u001b[0;34m,\u001b[0m \u001b[0mweight_reg\u001b[0m\u001b[0;34m=\u001b[0m\u001b[0;36m0.\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n\u001b[0m\u001b[1;32m 17\u001b[0m \u001b[0;34m\u001b[0m\u001b[0m\n\u001b[1;32m 18\u001b[0m \u001b[0mv_eq_init\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0moptimizer\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0msolid\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mv_def\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mclone\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mdetach\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m)\u001b[0m \u001b[0;31m#bookkeeping\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n",
"\u001b[0;32m/opt/notebooks/assignment_2_4/notebook/../src/shape_optimizer.py\u001b[0m in \u001b[0;36m__init__\u001b[0;34m(self, solid, vt_surf, weight_reg)\u001b[0m\n\u001b[1;32m 48\u001b[0m \u001b[0mself\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0msolid\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mfind_equilibrium\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n\u001b[1;32m 49\u001b[0m \u001b[0mobj_init\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0mself\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mtgt_fit\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mobj\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0msolid\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mv_def\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mclone\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mdetach\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n\u001b[0;32m---> 50\u001b[0;31m \u001b[0mprint\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0;34m\"Initial objective: {:.4e}\\n\"\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mformat\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0mobj_init\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n\u001b[0m\u001b[1;32m 51\u001b[0m \u001b[0;34m\u001b[0m\u001b[0m\n\u001b[1;32m 52\u001b[0m \u001b[0;31m# Initialize grad\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n",
"\u001b[0;31mTypeError\u001b[0m: unsupported format string passed to NoneType.__format__"
]
}
],
"source": [
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = - rho * 9.81\n",
"use_linear = False\n",
"\n",
"# The target is the initial raw mesh\n",
"vt_surf = torch.tensor(vNP[bvNP, :])\n",
"\n",
"# Create solid\n",
"if use_linear:\n",
" ee = LinearElasticEnergy(young, poisson)\n",
"else:\n",
" ee = NeoHookeanElasticEnergy(young, poisson)\n",
"solid_ = ElasticSolid(v_init_rest, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"solid_.update_def_shape(v_init_def)\n",
"\n",
"optimizer = ShapeOptimizer(solid_, vt_surf, weight_reg=0.)\n",
"\n",
"v_eq_init = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"optimizer.optimize(step_size_init=1e-4, max_l_iter=10, n_optim_steps=40)"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"import matplotlib.pyplot as plt\n",
"\n",
"plt.figure(figsize=(10, 6))\n",
"plt.plot(to_numpy(optimizer.objectives[optimizer.objectives > 0]))\n",
"plt.title(\"Objective as optimization goes\", fontsize=14)\n",
"plt.xlabel(\"Optimization steps\", fontsize=12)\n",
"plt.ylabel(\"Objective\", fontsize=12)\n",
"plt.grid()\n",
"plt.show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Initial guess for rest state) deploys to Black\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_init_rest) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_eq_init) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"v_rest_optim_g = optimizer.solid.v_rest.clone().detach() #bookkeeping"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add point load to the right most vertices\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"maxX = torch.min(v[:, 0])\n",
"f_point_idx = torch.arange(v.shape[0])[v[:, 0] > maxX - 0.01*aabb[0]]\n",
"\n",
"f_point = torch.zeros(size=(f_point_idx.shape[0], 3))\n",
"f_point[:, 2] = -5e3\n",
"\n",
"optimizer.solid.add_point_load(f_point_idx, f_point)\n",
"optimizer.set_params(optimizer.params)\n",
"v_def_optim_g_under_point = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"optimizer.reset_BFGS()\n",
"optimizer.optimize(step_size_init=1e-4, max_l_iter=10, n_optim_steps=20)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Optimum rest state under gravity) deploys to Black with the additional point load\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_rest_optim_g) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_def_optim_g_under_point) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3 (ipykernel)",
"language": "python",
"name": "python3"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
"version": "3.9.7"
},
"toc": {
"base_numbering": 1,
"nav_menu": {},
"number_sections": true,
"sideBar": true,
"skip_h1_title": false,
"title_cell": "Table of Contents",
"title_sidebar": "Contents",
"toc_cell": false,
"toc_position": {},
"toc_section_display": true,
"toc_window_display": false
}
},
"nbformat": 4,
"nbformat_minor": 4
}
@@ -0,0 +1,237 @@
{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Description\n",
"\n",
"This notebook intends to gather all the functionalities you'll have to implement for assignment 2.2.\n",
"\n",
"# Load libraries"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import numpy as np\n",
"import igl\n",
"import meshplot as mp\n",
"import time\n",
"import torch\n",
"\n",
"import sys as _sys\n",
"_sys.path.append(\"../src\")\n",
"from elasticsolid import *\n",
"from elasticenergy import *\n",
"from vis_utils import *\n",
"from matplotlib import gridspec\n",
"import matplotlib.pyplot as plt\n",
"\n",
"torch.set_default_dtype(torch.float64)\n",
"\n",
"shadingOptions = {\n",
" \"flat\":True,\n",
" \"wireframe\":False, \n",
"}\n",
"\n",
"rot = np.array(\n",
" [[1, 0, 0 ],\n",
" [0, 0, 1],\n",
" [0, -1, 0 ]]\n",
")"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Load mesh\n",
"\n",
"Several meshes are available for you to play with under `data/`: `ball.obj`, `dinosaur.obj`, and `beam.obj`."
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"scrolled": false
},
"outputs": [],
"source": [
"vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/beam.obj\")\n",
"aabb = np.max(vNP, axis=0) - np.min(vNP, axis=0)\n",
"v = torch.tensor(vNP)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Linear/Non-Linear Elastic Solid\n",
"\n",
"## Instantiation\n",
"\n",
"We first specify the elasticity model to use for the elastic solid, as well as pinned vertices, and volumetric forces."
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [],
"source": [
"rho = 131 # [kg.m-3]\n",
"young = 10e6 # [Pa] \n",
"poisson = 0.2\n",
"force_mass = torch.zeros(size = (3,))\n",
"force_mass[2] = - rho * 9.81\n",
"\n",
"minX = torch.min(v[:, 0])\n",
"pin_idx = torch.arange(v.shape[0])[v[:, 0] < minX + 0.2*aabb[0]]\n",
"\n",
"# ee = LinearElasticEnergy(young, poisson)\n",
"ee = NeoHookeanElasticEnergy(young, poisson)\n",
"solid = ElasticSolid(v, tNP, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate Elastic Energy Gradient (Elastic Forces) using Finite Differences on Elastic Energy"
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {},
"outputs": [
{
"data": {
"image/png": "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 truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"solid.update_def_shape(v)\n",
"\n",
"fd_validation_elastic(solid)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate External Energy Gradient (External Forces) using Finite Differences on External Energy"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {},
"outputs": [
{
"data": {
"image/png": "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 truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"maxX = torch.max(v[:, 0])\n",
"f_point_idx = torch.arange(v.shape[0])[v[:, 0] > maxX - 0.01*aabb[0]]\n",
"\n",
"f_point = torch.zeros(size=(f_point_idx.shape[0], 3))\n",
"f_point[:, 2] = -5e3\n",
"\n",
"solid.add_point_load(f_point_idx, f_point)\n",
"\n",
"solid.update_def_shape(v)\n",
"\n",
"fd_validation_ext(solid)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate Elastic Energy Force Differentials (Elastic Forces) using Finite Differences on Elastic Forces"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [
{
"data": {
"image/png": 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truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"solid.update_def_shape(v)\n",
"\n",
"fd_validation_elastic_differentials(solid)"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3 (ipykernel)",
"language": "python",
"name": "python3"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
"version": "3.9.7"
},
"toc": {
"base_numbering": 1,
"nav_menu": {},
"number_sections": true,
"sideBar": true,
"skip_h1_title": false,
"title_cell": "Table of Contents",
"title_sidebar": "Contents",
"toc_cell": false,
"toc_position": {},
"toc_section_display": true,
"toc_window_display": false
}
},
"nbformat": 4,
"nbformat_minor": 4
}
@@ -0,0 +1,483 @@
{
"cells": [
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import numpy as np\n",
"import torch\n",
"import igl\n",
"import time\n",
"\n",
"import meshplot as mp\n",
"import sys as _sys\n",
"_sys.path.append(\"../src\")\n",
"from elasticenergy import *\n",
"from elasticsolid import *\n",
"from adjoint_sensitivity import *\n",
"from vis_utils import *\n",
"from objectives import *\n",
"from harmonic_interpolator import *\n",
"from shape_optimizer import *\n",
"\n",
"from utils import *\n",
"\n",
"shadingOptions = {\n",
" \"flat\":True,\n",
" \"wireframe\":False, \n",
"}\n",
"\n",
"rot = np.array(\n",
" [[1, 0, 0 ],\n",
" [0, 0, 1],\n",
" [0, -1, 0 ]]\n",
")\n",
"\n",
"torch.set_default_dtype(torch.float64)\n",
"\n",
"def to_numpy(tensor):\n",
" return tensor.detach().clone().numpy()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Create the deformed object\n",
"\n",
"## Load the mesh"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "732bc7276b654a1db0b501b750c8fd87",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(5.0, 1.0,…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"data": {
"text/plain": [
"<meshplot.Viewer.Viewer at 0x7f4f18719760>"
]
},
"execution_count": 2,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/beam.obj\")\n",
"\n",
"aabb = np.max(vNP, axis=0) - np.min(vNP, axis=0)\n",
"length_scale = np.mean(aabb)\n",
"\n",
"\n",
"v, t = torch.tensor(vNP), torch.tensor(tNP)\n",
"eNP = igl.edges(tNP)\n",
"beNP = igl.edges(igl.boundary_facets(tNP))\n",
"\n",
"def get_boundary_and_interior(vlen, t):\n",
" bv = np.unique(igl.boundary_facets(t))\n",
" vIdx = np.arange(vlen)\n",
" iv = vIdx[np.invert(np.in1d(vIdx, bv))]\n",
" return bv, iv\n",
"# Compute boundary vertices and interior vertex indices\n",
"bvNP, ivNP = get_boundary_and_interior(v.shape[0], tNP)\n",
"\n",
"mp.plot(vNP @ rot.T, np.array(tNP), shading=shadingOptions)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add some physical characteristics"
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Pinned vertices: [ 0 1 11 12 22 23 33 34 44 54 55 75 76 86 87 88 89]\n"
]
}
],
"source": [
"rho = 131 # [kg.m-3]\n",
"damping = 0.\n",
"young = 5e7 # [Pa] \n",
"poisson = 0.2\n",
"\n",
"# Find some of the lowest vertices and pin them\n",
"minX = torch.min(v[:, 0])\n",
"pin_idx = torch.arange(v.shape[0])[v[:, 0] < minX + 0.2*aabb[0]]\n",
"vIdx = np.arange(v.shape[0])\n",
"pin_idx = vIdx[np.in1d(vIdx, bvNP) & np.in1d(vIdx, pin_idx)]\n",
"print(\"Pinned vertices: {}\".format(pin_idx))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Initial guess\n",
"\n",
"The idea is that we start deforming the mesh by inverting gravity."
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "f4fe02d4e90b47cea101747098c5b3bd",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(4.9017367…"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# Inverted gravity\n",
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = + rho * 9.81\n",
"\n",
"# Gravity going in the wrong direction\n",
"\n",
"ee = NeoHookeanElasticEnergy(young, poisson)\n",
"\n",
"v = HarmonicInterpolator(v, t, ivNP).interpolate(v[bvNP])\n",
"solid_init = ElasticSolid(v, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"\n",
"solid_init.find_equilibrium()\n",
"plot_torch_solid(solid_init, beNP, rot, length_scale)\n",
"\n",
"# Use these as initial guesses\n",
"v_init_rest = solid_init.v_def.clone().detach()\n",
"v_init_def = solid_init.v_rest.clone().detach()\n",
"\n",
"# v_init_rest = solid_init.v_rest.clone().detach()\n",
"# v_init_def = solid_init.v_def.clone().detach()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Inverse design\n"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {
"scrolled": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Initial objective: 1.6230e+00\n",
"\n"
]
}
],
"source": [
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = - rho * 9.81\n",
"use_linear = False\n",
"\n",
"# The target is the initial raw mesh\n",
"vt_surf = torch.tensor(vNP[bvNP, :])\n",
"\n",
"# Create solid\n",
"if use_linear:\n",
" ee = LinearElasticEnergy(young, poisson)\n",
"else:\n",
" ee = NeoHookeanElasticEnergy(young, poisson)\n",
"solid_ = ElasticSolid(v_init_rest, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"solid_.update_def_shape(v_init_def)\n",
"\n",
"optimizer = ShapeOptimizer(solid_, vt_surf, weight_reg=10.)\n",
"\n",
"v_eq_init = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Objective after 40 optimization step(s): 1.5788e+00\n",
" Line search Iters: 9\n",
"Elapsed time: 97.1s. \n",
"Estimated remaining time: 0.0s\n",
"\n"
]
},
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "10cffc9c94334b8aa1529d4b6fb36278",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(5.0444669…"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"optimizer.optimize(step_size_init=1e-2, max_l_iter=10, n_optim_steps=40)"
]
},
{
"cell_type": "code",
"execution_count": 7,
"metadata": {},
"outputs": [
{
"data": {
"image/png": 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truncated
"text/plain": [
"<Figure size 720x432 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"import matplotlib.pyplot as plt\n",
"\n",
"plt.figure(figsize=(10, 6))\n",
"plt.plot(to_numpy(optimizer.objectives[optimizer.objectives > 0]))\n",
"plt.title(\"Objective as optimization goes\", fontsize=14)\n",
"plt.xlabel(\"Optimization steps\", fontsize=12)\n",
"plt.ylabel(\"Objective\", fontsize=12)\n",
"plt.grid()\n",
"plt.show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Initial guess for rest state) deploys to Black\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": 8,
"metadata": {},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "cc0e6ec0eb174783a516c85f67697225",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(5.0444669…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"data": {
"text/plain": [
"4"
]
},
"execution_count": 8,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_init_rest) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_eq_init) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
},
{
"cell_type": "code",
"execution_count": 9,
"metadata": {},
"outputs": [],
"source": [
"v_rest_optim_g = optimizer.solid.v_rest.clone().detach() #bookkeeping"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add point load to the right most vertices\n"
]
},
{
"cell_type": "code",
"execution_count": 10,
"metadata": {},
"outputs": [],
"source": [
"maxX = torch.min(v[:, 0])\n",
"f_point_idx = torch.arange(v.shape[0])[v[:, 0] > maxX - 0.01*aabb[0]]\n",
"\n",
"f_point = torch.zeros(size=(f_point_idx.shape[0], 3))\n",
"f_point[:, 2] = -5e4\n",
"\n",
"optimizer.solid.add_point_load(f_point_idx, f_point)\n",
"optimizer.set_params(optimizer.params)\n",
"v_def_optim_g_under_point = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Objective after 21 optimization step(s): 2.2335e+01\n",
" Line search Iters: 9\n",
"Elapsed time: 2215.2s. \n",
"Estimated remaining time: 8333.3s\n",
"\n"
]
},
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "f0b258afc95d4bdf8e8bb0e3fb529d05",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(5.0945925…"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"optimizer.reset_BFGS()\n",
"optimizer.optimize(step_size_init=1e-2, max_l_iter=10, n_optim_steps=100)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Optimum rest state under gravity) deploys to Black with the additional point load\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_rest_optim_g) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_def_optim_g_under_point) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3 (ipykernel)",
"language": "python",
"name": "python3"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
"version": "3.9.7"
},
"toc": {
"base_numbering": 1,
"nav_menu": {},
"number_sections": true,
"sideBar": true,
"skip_h1_title": false,
"title_cell": "Table of Contents",
"title_sidebar": "Contents",
"toc_cell": false,
"toc_position": {},
"toc_section_display": true,
"toc_window_display": false
}
},
"nbformat": 4,
"nbformat_minor": 4
}
@@ -0,0 +1,474 @@
{
"cells": [
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import numpy as np\n",
"import torch\n",
"import igl\n",
"\n",
"import meshplot as mp\n",
"import sys as _sys\n",
"_sys.path.append(\"../src\")\n",
"from elasticenergy import *\n",
"from elasticsolid import *\n",
"from adjoint_sensitivity import *\n",
"from vis_utils import *\n",
"from objectives import *\n",
"from harmonic_interpolator import *\n",
"from shape_optimizer import *\n",
"\n",
"from utils import *\n",
"\n",
"shadingOptions = {\n",
" \"flat\":True,\n",
" \"wireframe\":False, \n",
"}\n",
"\n",
"rot = np.array(\n",
" [[1, 0, 0 ],\n",
" [0, 0, 1],\n",
" [0, -1, 0 ]]\n",
")\n",
"\n",
"torch.set_default_dtype(torch.float64)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Create the deformed object\n",
"\n",
"## Load the mesh"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "35cf42b4eded4cb99f3811a16dcb4d67",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-1.987469…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"data": {
"text/plain": [
"<meshplot.Viewer.Viewer at 0x7fa5b879cc10>"
]
},
"execution_count": 2,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/dinosaur.obj\")\n",
"# vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/beam.obj\")\n",
"\n",
"aabb = np.max(vNP, axis=0) - np.min(vNP, axis=0)\n",
"length_scale = np.mean(aabb)\n",
"\n",
"\n",
"v, t = torch.tensor(vNP), torch.tensor(tNP)\n",
"eNP = igl.edges(tNP)\n",
"beNP = igl.edges(igl.boundary_facets(tNP))\n",
"\n",
"bvNP, ivNP = get_boundary_and_interior(v.shape[0], tNP)\n",
"\n",
"mp.plot(vNP @ rot.T, np.array(tNP), shading=shadingOptions)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add some physical characteristics"
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Pinned vertices: [ 46 47 50 59 60 62 64 65 88 89 91 98 99 102 103 104]\n"
]
}
],
"source": [
"rho = 131 # [kg.m-3], if aabb[0] ~ 14m, and m_tot = 6000kg\n",
"young = 3e8 # [Pa] \n",
"poisson = 0.2\n",
"\n",
"# Find some of the lowest vertices and pin them\n",
"minZ = torch.min(v[:, 2])\n",
"pin_idx = torch.arange(v.shape[0])[v[:, 2] < minZ + 0.01*aabb[2]]\n",
"vIdx = np.arange(v.shape[0])\n",
"pin_idx = vIdx[np.in1d(vIdx, bvNP) & np.in1d(vIdx, pin_idx)]\n",
"print(\"Pinned vertices: {}\".format(pin_idx))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Initial guess\n",
"\n",
"The idea is that we start deforming the mesh by inverting gravity."
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {
"scrolled": false
},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "5d62f192ccc940388718972e4a447f2b",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-2.468080…"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# Inverted gravity\n",
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = + rho * 9.81\n",
"\n",
"# Gravity going in the wrong direction\n",
"\n",
"ee = NeoHookeanElasticEnergy(young, poisson)\n",
"\n",
"v = HarmonicInterpolator(v, t, ivNP).interpolate(v[bvNP])\n",
"solid_init = ElasticSolid(v, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"\n",
"solid_init.find_equilibrium()\n",
"plot_torch_solid(solid_init, beNP, rot, length_scale)\n",
"\n",
"# Use these as initial guesses\n",
"v_init_rest = solid_init.v_def.clone().detach()\n",
"v_init_def = solid_init.v_rest.clone().detach()\n",
"\n",
"# v_init_rest = solid_init.v_rest.clone().detach()\n",
"# v_init_def = solid_init.v_def.clone().detach()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Inverse design\n"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {
"scrolled": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Initial objective: 6.6351e+02\n",
"\n"
]
}
],
"source": [
"force_mass = torch.zeros(size=(3,))\n",
"force_mass[2] = - rho * 9.81\n",
"use_linear = False\n",
"\n",
"# The target is the initial raw mesh\n",
"vt_surf = torch.tensor(vNP[bvNP, :])\n",
"\n",
"# Create solid\n",
"if use_linear:\n",
" ee = LinearElasticEnergy(young, poisson)\n",
"else:\n",
" ee = NeoHookeanElasticEnergy(young, poisson)\n",
"solid_ = ElasticSolid(v_init_rest, t, ee, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"solid_.update_def_shape(v_init_def)\n",
"\n",
"optimizer = ShapeOptimizer(solid_, vt_surf, weight_reg=0.)\n",
"\n",
"v_eq_init = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Objective after 19 optimization step(s): 5.8586e+02\n",
" Line search Iters: 8\n",
"Elapsed time: 683.7s. \n",
"Estimated remaining time: 755.7s\n",
"\n"
]
},
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "fa1a13b5101d4629a3d07e84205409dd",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-0.497634…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"name": "stdout",
"output_type": "stream",
"text": [
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"An exception occured: . \n",
"Halving the step.\n",
"Line search can't find a step to take\n"
]
}
],
"source": [
"optimizer.optimize(step_size_init=1e-4, max_l_iter=10, n_optim_steps=40)"
]
},
{
"cell_type": "code",
"execution_count": 7,
"metadata": {},
"outputs": [
{
"data": {
"image/png": "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 truncated
"text/plain": [
"<Figure size 720x432 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"import matplotlib.pyplot as plt\n",
"\n",
"plt.figure(figsize=(10, 6))\n",
"plt.plot(to_numpy(optimizer.objectives[optimizer.objectives > 0]))\n",
"plt.title(\"Objective as optimization goes\", fontsize=14)\n",
"plt.xlabel(\"Optimization steps\", fontsize=12)\n",
"plt.ylabel(\"Objective\", fontsize=12)\n",
"plt.grid()\n",
"plt.show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Initial guess for rest state) deploys to Black\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": 8,
"metadata": {},
"outputs": [
{
"data": {
"application/vnd.jupyter.widget-view+json": {
"model_id": "70afc138cf264b47b4fddfd6b9ae8624",
"version_major": 2,
"version_minor": 0
},
"text/plain": [
"Renderer(camera=PerspectiveCamera(children=(DirectionalLight(color='white', intensity=0.6, position=(-0.497634…"
]
},
"metadata": {},
"output_type": "display_data"
},
{
"data": {
"text/plain": [
"4"
]
},
"execution_count": 8,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_init_rest) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_eq_init) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
},
{
"cell_type": "code",
"execution_count": 9,
"metadata": {},
"outputs": [],
"source": [
"v_rest_optim_g = optimizer.solid.v_rest.clone().detach() #bookkeeping"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Add point load to the right most vertices\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"maxX = torch.min(v[:, 0])\n",
"f_point_idx = torch.arange(v.shape[0])[v[:, 0] > maxX - 0.01*aabb[0]]\n",
"\n",
"f_point = torch.zeros(size=(f_point_idx.shape[0], 3))\n",
"f_point[:, 2] = -5e3\n",
"\n",
"optimizer.solid.add_point_load(f_point_idx, f_point)\n",
"optimizer.set_params(optimizer.params)\n",
"v_def_optim_g_under_point = optimizer.solid.v_def.clone().detach() #bookkeeping"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"optimizer.reset_BFGS()\n",
"optimizer.optimize(step_size_init=1e-4, max_l_iter=10, n_optim_steps=20)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Green (Optimum rest state under gravity) deploys to Black with the additional point load\n",
"\n",
"Blue (Optimized rest state) deploys to Yellow\n",
"\n",
"Red is the Target Shape\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"p = mp.plot(np.array(optimizer.solid.v_def) @ rot.T, tNP, shading=shadingOptions)\n",
"# p.add_points(np.array(optimizer.solid.v_def)[pin_idx, :] @ rot.T, shading={\"point_color\":\"black\", \"point_size\": 0.2})\n",
"p.add_edges(np.array(v_rest_optim_g) @ rot.T, beNP, shading={\"line_color\": \"green\"})\n",
"p.add_edges(vNP @ rot.T, beNP, shading={\"line_color\": \"red\"})\n",
"p.add_edges(np.array(v_def_optim_g_under_point) @ rot.T, beNP, shading={\"line_color\": \"black\"})\n",
"p.add_edges(np.array(optimizer.solid.v_rest) @ rot.T, beNP, shading={\"line_color\": \"blue\"})\n"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3 (ipykernel)",
"language": "python",
"name": "python3"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
"version": "3.9.7"
},
"toc": {
"base_numbering": 1,
"nav_menu": {},
"number_sections": true,
"sideBar": true,
"skip_h1_title": false,
"title_cell": "Table of Contents",
"title_sidebar": "Contents",
"toc_cell": false,
"toc_position": {},
"toc_section_display": true,
"toc_window_display": false
}
},
"nbformat": 4,
"nbformat_minor": 4
}
@@ -0,0 +1,290 @@
{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Description\n",
"\n",
"This notebook intends to gather all the functionalities you'll have to implement for assignment 2.2.\n",
"\n",
"# Load libraries"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import numpy as np\n",
"import igl\n",
"import meshplot as mp\n",
"import time\n",
"import torch\n",
"\n",
"import sys as _sys\n",
"_sys.path.append(\"../src\")\n",
"from elasticsolid import *\n",
"from elasticenergy import *\n",
"from vis_utils import *\n",
"from matplotlib import gridspec\n",
"import matplotlib.pyplot as plt\n",
"\n",
"torch.set_default_dtype(torch.float64)\n",
"\n",
"shadingOptions = {\n",
" \"flat\":True,\n",
" \"wireframe\":False, \n",
"}\n",
"\n",
"rot = np.array(\n",
" [[1, 0, 0 ],\n",
" [0, 0, 1],\n",
" [0, -1, 0 ]]\n",
")"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Load mesh\n",
"\n",
"Several meshes are available for you to play with under `data/`: `ball.obj`, `dinosaur.obj`, and `beam.obj`."
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"scrolled": false
},
"outputs": [],
"source": [
"vNP, _, _, tNP, _, _ = igl.read_obj(\"../data/beam.obj\")\n",
"aabb = np.max(vNP, axis=0) - np.min(vNP, axis=0)\n",
"v = torch.tensor(vNP)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Linear/Non-Linear Elastic Solid\n",
"\n",
"## Instantiation\n",
"\n",
"We first specify the elasticity model to use for the elastic solid, as well as pinned vertices, and volumetric forces."
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [],
"source": [
"rho = 131 # [kg.m-3]\n",
"young = 10e6 # [Pa] \n",
"poisson = 0.2\n",
"force_mass = torch.zeros(size = (3,))\n",
"force_mass[2] = - rho * 9.81\n",
"\n",
"minX = torch.min(v[:, 0])\n",
"pin_idx = torch.arange(v.shape[0])[v[:, 0] < minX + 0.2*aabb[0]]\n",
"\n",
"ee_lin = LinearElasticEnergy(young, poisson)\n",
"ee_neo = NeoHookeanElasticEnergy(young, poisson)\n",
"solid_lin = ElasticSolid(v, tNP, ee_lin, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n",
"solid_neo = ElasticSolid(v, tNP, ee_neo, rho=rho, pin_idx=pin_idx, f_mass=force_mass)\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate Elastic Energy Gradient (Elastic Forces) using Finite Differences on Elastic Energy"
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {},
"outputs": [
{
"data": {
"image/png": "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 truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
},
{
"data": {
"image/png": "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 truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"solid_lin.update_def_shape(v)\n",
"solid_neo.update_def_shape(v)\n",
"\n",
"fd_validation_elastic(solid_lin)\n",
"fd_validation_elastic(solid_neo)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate External Energy Gradient (External Forces) using Finite Differences on External Energy"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {},
"outputs": [
{
"data": {
"image/png": 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truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
},
{
"data": {
"image/png": 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truncated
"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
"needs_background": "light"
},
"output_type": "display_data"
}
],
"source": [
"maxX = torch.max(v[:, 0])\n",
"f_point_idx = torch.arange(v.shape[0])[v[:, 0] > maxX - 0.01*aabb[0]]\n",
"\n",
"f_point = torch.zeros(size=(f_point_idx.shape[0], 3))\n",
"f_point[:, 2] = -5e3\n",
"\n",
"solid_lin.add_point_load(f_point_idx, f_point)\n",
"solid_neo.add_point_load(f_point_idx, f_point)\n",
"\n",
"solid_lin.update_def_shape(v)\n",
"solid_neo.update_def_shape(v)\n",
"\n",
"fd_validation_ext(solid_lin)\n",
"fd_validation_ext(solid_neo)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# 4.4.5 Point Force\n",
"\n",
"I tried adding a call to `make_external_energy` in the `add_point_load` function since a new force would also lead to a different energy. However inside `make_external_energy`, after many tries to add the energy corresponding to the point force, I gave up."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Validate Elastic Energy Force Differentials (Elastic Forces) using Finite Differences on Elastic Forces"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
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"text/plain": [
"<Figure size 432x288 with 1 Axes>"
]
},
"metadata": {
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},
"output_type": "display_data"
}
],
"source": [
"solid_lin.update_def_shape(v)\n",
"solid_neo.update_def_shape(v)\n",
"\n",
"fd_validation_elastic_differentials(solid_lin)\n",
"fd_validation_elastic_differentials(solid_neo)"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3 (ipykernel)",
"language": "python",
"name": "python3"
},
"language_info": {
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"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
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"title_cell": "Table of Contents",
"title_sidebar": "Contents",
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}
},
"nbformat": 4,
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}