DyLab_3D_MOT/Coil_geometry_AHH/Untitled.ipynb

{
 "cells": [
  {
   "cell_type": "code",
   "execution_count": 13,
   "id": "672091c7",
   "metadata": {},
   "outputs": [],
   "source": [
    "# -*- coding: utf-8 -*-\n",
    "\"\"\"\n",
    "Created on Tue Aug 24 16:24:52 2021\n",
    "\n",
    "@author: Joschka\n",
    "\"\"\"\n",
    "\n",
    "import matplotlib.pyplot as plt\n",
    "import numpy as np\n",
    "import sys\n",
    "sys.path.insert(0,'..\\src')\n",
    "\n",
    "import coil_class_jupyter as BC\n",
    "\n",
    "#from IPython import get_ipython\n",
    "#get_ipython().run_line_magic('matplotlib', 'qt')\n",
    "#get_ipython().run_line_magic('matplotlib', 'inline')\n"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 14,
   "id": "d3a46f0f",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "HH = 1, Distance = 57.8 mm, z_min = 24.9 mm, z_max = 32.9 mm\n",
      "Radius = 45.29999999999999 mm, Radius_inner = 41.29999999999999 mm, Radius_outer = 49.30 mm\n",
      "layers = 1, windings = 1, wire_width = 8.0, wire_height = 8.0 mm \n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.47817553461759527 W\n",
      "B_z(0) = 13.37 G\n",
      "B_z_curvature(0) = 0.3775 G/cm^2\n",
      "current density = 1.2499999999999998 A/mm^2\n",
      "Power = 0.5193429647502357 W\n",
      "width = 0.2mm, height = 320.0mm\n",
      "B_z(0) = 1.81 G\n",
      "B_z_curvature(0) = 0.1083 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5188151771844329 W\n",
      "width = 0.30000000000000004mm, height = 213.33333333333331mm\n",
      "B_z(0) = 2.59 G\n",
      "B_z_curvature(0) = 0.1629 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5182873896186297 W\n",
      "width = 0.4000000000000001mm, height = 159.99999999999997mm\n",
      "B_z(0) = 3.32 G\n",
      "B_z_curvature(0) = 0.2160 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5177596020528267 W\n",
      "width = 0.5000000000000001mm, height = 127.99999999999997mm\n",
      "B_z(0) = 4.00 G\n",
      "B_z_curvature(0) = 0.2669 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5172318144870235 W\n",
      "width = 0.6000000000000001mm, height = 106.66666666666666mm\n",
      "B_z(0) = 4.63 G\n",
      "B_z_curvature(0) = 0.3147 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5167040269212204 W\n",
      "width = 0.7000000000000002mm, height = 91.4285714285714mm\n",
      "B_z(0) = 5.20 G\n",
      "B_z_curvature(0) = 0.3588 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5161762393554175 W\n",
      "width = 0.8000000000000003mm, height = 79.99999999999997mm\n",
      "B_z(0) = 5.74 G\n",
      "B_z_curvature(0) = 0.3987 G/cm^2\n",
      "current density = 1.25 A/mm^2\n",
      "Power = 0.5156484517896143 W\n",
      "width = 0.9000000000000001mm, height = 71.1111111111111mm\n",
      "B_z(0) = 6.22 G\n",
      "B_z_curvature(0) = 0.4344 G/cm^2\n"
     ]
    },
    {
     "data": {
      "image/png": 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\n",
      "text/plain": [
       "<Figure size 432x288 with 1 Axes>"
      ]
     },
     "metadata": {
      "needs_background": "light"
     },
     "output_type": "display_data"
    }
   ],
   "source": [
    "#set up axis\n",
    "x = np.linspace(-50, 50, 301)\n",
    "z = np.linspace(-50, 50, 301)\n",
    "\n",
    "#New coil\n",
    "HH_Coil = BC.BCoil(HH = 1, distance = 54 ,radius = 48 , layers = 4, windings = 4, wire_height = 1, wire_width = 1)\n",
    "\n",
    "#Compensation Coil\n",
    "HH_Coil_comp = BC.BCoil(HH = 1, distance = 54 ,radius = 37, layers = 4, windings = 4,wire_height = 1, wire_width = 1)\n",
    "\n",
    "\n",
    "\n",
    "#HH_Coil_44.Bz_plot_HH(I,x,z)\n"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "5eef49ab",
   "metadata": {},
   "outputs": [],
   "source": []
  }
 ],
 "metadata": {
  "kernelspec": {
   "display_name": "Python 3",
   "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": "3.8.8"
  }
 },
 "nbformat": 4,
 "nbformat_minor": 5
}