diff --git a/TeachingExamples/SuspendedObjects-exercise.ipynb b/TeachingExamples/SuspendedObjects-exercise.ipynb index 0e89554..f23613e 100644 --- a/TeachingExamples/SuspendedObjects-exercise.ipynb +++ b/TeachingExamples/SuspendedObjects-exercise.ipynb @@ -1,382 +1,279 @@ { "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "
\n", " WORK IN PROGRESS  This notebook is under development, please bear with us...\n", "
" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "
\n", "

Use case scenario
\n", " This notebook is made to be used by students as an assignment or exercise, in autonomy (at home or in an exercise session).

\n", "

Features
\n", " This notebook embeds auto-corrected quizzes to engage students with the virtual demonstration and uses different types of visualisations to help students understand the phenomena.
\n", " The example chosen is voluntarily simple so that anyone can understand what is illustrated and focus the pedagogical features of the example.

\n", "

More information on using notebooks for exercises or assignements.

\n", "
" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "# Suspended objects\n", "\n", "\n", "\n", "## The problem\n", "We consider a clothesline made of two poles and a cable.\n", "The cable is fixed on one pole. A pulley on the other pole allows to attach a counterweight to pull the cable taut.\n", "\n", "## Quiz 1" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "Execute the cell below to activate the interactive quiz." ] }, { "cell_type": "code", - "execution_count": 1, + "execution_count": null, "metadata": { "jupyter": { "source_hidden": true } }, - "outputs": [ - { - "data": { - "text/html": [ - "\n", - " \n", - " " - ], - "text/plain": [ - "" - ] - }, - "execution_count": 1, - "metadata": {}, - "output_type": "execute_result" - } - ], + "outputs": [], "source": [ "from IPython.display import IFrame\n", "IFrame('https://moodle.epfl.ch/mod/hvp/embed.php?id=1028285', 1024, 550)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Virtual lab\n", "\n", "The virtual demonstration below illustrates position of the clothesline for different counterweights. \n", "Execute the cell below to launch the virtual demonstration, then *answer the quiz 2 below*." ] }, { "cell_type": "code", - "execution_count": 2, + "execution_count": null, "metadata": { "jupyter": { "source_hidden": true } }, - "outputs": [ - { - "data": { - "application/vnd.jupyter.widget-view+json": { - "model_id": "50f0872e51ba49638b3627867d156cc1", - "version_major": 2, - "version_minor": 0 - }, - "text/plain": [ - "VBox(children=(HBox(children=(Label(value='Mass of the counterweight ($kg$):', layout=Layout(margin='5px 10px'…" - ] - }, - "metadata": {}, - "output_type": "display_data" - } - ], + "outputs": [], "source": [ "%matplotlib inline\n", "from lib.suspendedobjects import *\n", "SuspendedObjectsLab();" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Quiz 2\n", "\n", "Execute the cell below to activate the interactive quizz." ] }, { "cell_type": "code", - "execution_count": 3, + "execution_count": null, "metadata": {}, - "outputs": [ - { - "data": { - "text/html": [ - "\n", - " \n", - " " - ], - "text/plain": [ - "" - ] - }, - "execution_count": 3, - "metadata": {}, - "output_type": "execute_result" - } - ], + "outputs": [], "source": [ "from IPython.display import IFrame\n", "IFrame('https://h5p.org/h5p/embed/584119', 1024, 400)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "*If you wonder how the virtual lab works and would like to see the code, [you can have a look at it at the end of this notebook](#How-does-the-virtual-lab-work%3F).*\n", "\n", " " ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Analytic solution\n", "\n", "### Goal\n", "\n", "The question is which counterweight allows to suspend wet jeans (3kg) on the cable so that the cable is taut as shown on the diagram. \n", "We are therefore looking for the expression of the **mass of the counterweight $m_{cw}$ as a function of the other parameters of the problem**. \n", "\n", "### Method\n", "\n", "Given that the system is in static equilibrium, the sum of external forces exerted on the system will be zero, so using Newton's second law should be easy. The force that the counterweight exerts on the system will involve the mass of the counterweight so we should be able to rewrite Newton's second law to get an expression of the form $m_{cw} = ...$.\n", "\n", "### Hypotheses and simplifications\n", "\n", "We make the following assumptions and simplifications:\n", "* the jeans are considered as positioned exactly mid-way between the poles so the tension is equal on both sides of the cable\n", "* we represent the jeans by the point at which they are suspended\n", "* the cable is considered as rigid (not bended), with a negligible mass\n", "* the pulley is considered as perfect, without mass nor friction\n", "* we consider the static equilibrium obtained after changing the weight, once the system is stabilized\n", "\n", "### Resolution\n", "\n", "First, let's draw a diagram and represent the different forces involved.\n", "\n", "\n", "The *forces applied on the jeans* are:\n", "* the weight: $\\vec F_j = m_j \\vec g$ \n", "* the force exerted by the cable on each side of the jeans: assuming the jeans are suspended at the exact center of the cable, then the tension applied on each of the two sides is is equally distributed $\\vec T$, which combine into a vertical resulting tention $\\vec T_r = 2.\\vec T$\n", "\n", "From Newton's second law in a static equilibrium we can write: $\\sum \\vec F_j = \\vec 0$ \n", "With the forces on the jeans we get: $\\vec F_j + \\vec T_r = 0$ \n", "Using the fact that the tension is equal on both sides of the jeans we get: $\\vec F_j + 2.\\vec T = 0$\n", "\n", "If we project on $x$ and $y$ axes, we get: \n", "$\\left\\{\\begin{matrix} F_{jx} + 2.T_x = 0 \\\\ F_{jy} + 2.T_y = 0\\end{matrix}\\right. $\n", "\n", "Since the weight does not have a component on the x axis, it simplifies into: \n", "$\\left\\{\\begin{matrix} T_x = 0 \\\\ F_{jy} + 2.T_y = 0\\end{matrix}\\right. $\n", "\n", "The component of the weight on the y axis is $F_{jy} = - m_j.g$, which gives us: \n", "$\\left\\{\\begin{matrix} T_x = 0 \\\\ - m_j.g + 2.T_y = 0\\end{matrix}\\right. $\n", "\n", "Using the angle $\\alpha$ we can get the tension $T_y$ expressed as a function of T since $sin(\\alpha) = \\frac{T_y}{T}$, therefore $T_y = T.sin(\\alpha)$\n", "\n", "By replacing $T_y$ by this expression in the above equation we get: \n", "$\\left\\{\\begin{matrix} T_x = 0 \\\\ - m_j.g + 2.T.sin(\\alpha) = 0\\end{matrix}\\right. $\n", "\n", "From there we can get $T$, and this is equation number $(1)$: \n", "$T = \\frac{m_j.g}{2.sin(\\alpha)}$\n", "\n", " \n", "\n", "We now want to make the mass of the counterweight appear in this expression. \n", "So we will now look at the forces applied on the *counterweight*.\n", "\n", " \n", "\n", "The forces applied on the *counterweight* are:\n", "* the weight: $\\vec F_{cw} = m_{cw} \\vec g$ \n", "* the force exerted by the line: a simple pulley simply changes the direction of the tension so the tension applied on the counterweight is therefore $\\vec T$\n", "\n", "From Newton's second law in a static equilibrium we can write: $\\sum \\vec F_{cw} = \\vec 0$ \n", "With the forces involved in our problem : $\\vec F_{cw} + \\vec T = \\vec 0$ \n", "\n", "All forces being vertical, there is no need to project on $x$ so we get: $- F_{cw} + T = 0$ \n", "We replace the weight by its detailed expression: $-m_{cw}.g + T = 0$ \n", "Now we can express $T$ as a function of the other parameters, which is equation number $(2)$: $T = m_{cw}.g$ \n", "\n", " \n", "\n", "Let's now summarize what we have so far with equations $(1)$ and $(2)$: \n", "\n", "$\\left\\{\\begin{matrix}T = \\frac{m_j.g}{2.sin(\\alpha)} \\\\ T = m_{cw}.g\\end{matrix}\\right. $\n", "\n", "These two equations combined give us:\n", "\n", "$\\frac{m_j.g}{2.sin(\\alpha)} = m_{cw}.g$\n", "\n", "This allow us to find the mass of the counterweight as a function of the *mass of the jeans* and of the *angle that the line makes with the horizon*: \n", "\n", "$m_{cw} = \\frac{m_j}{2.sin(\\alpha)}$\n", "\n", " \n", "\n", "### Conclusion\n", "\n", "For the line to be taut as show on the figure, $\\alpha$ has to be really small i.e. close to zero. \n", "This means that $sin(\\alpha)$ will also be close to zero, which means in turn that $m_{cw}$ will be very big.\n", "Actually, **the more we want the line to be close to the horizon, the bigger $m_{cw}$ we will need!**\n", "In fact, it is impossible to get the line taut so that it is absolutely straight...\n", "\n", " \n", "\n", "### Application\n", "\n", "For a pair of wet jeans of $3 kg$ and an angle of $4^\\circ = \\frac{\\pi}{45}$, which is approximately like depicted on the figure, we need to put a counterweight of:" ] }, { "cell_type": "code", - "execution_count": 4, + "execution_count": null, "metadata": {}, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "21.503380539305514\n" - ] - } - ], + "outputs": [], "source": [ "mcw = 3 / (2 * np.sin(np.pi / 45))\n", "print(mcw)" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "You can **check that you get a similar result** with the virtual lab above!" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ " \n", "\n", "---\n", "# How does the virtual lab work?\n", "\n", "You can have a look at the code of the virtual lab by [opening this python file](lib/suspendedobjects.py).\n", "\n", "By executing the following cell, you will see the code of the function used to compute the angle that the line makes with the horizon depending on the masses of the object and the counterweight. " ] }, { "cell_type": "code", - "execution_count": 5, + "execution_count": null, "metadata": {}, - "outputs": [ - { - "data": { - "text/plain": [ - "\u001b[0;31mSignature:\u001b[0m \u001b[0mget_angle_from_masses\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0mm_object\u001b[0m\u001b[0;34m,\u001b[0m \u001b[0mm_counterweight\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n", - "\u001b[0;31mSource:\u001b[0m \n", - "\u001b[0;32mdef\u001b[0m \u001b[0mget_angle_from_masses\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0mm_object\u001b[0m\u001b[0;34m,\u001b[0m \u001b[0mm_counterweight\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m:\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;34m\"\"\"\u001b[0m\n", - "\u001b[0;34m Compute the angle that the cable makes with the horizon depending on the counterweight chosen\u001b[0m\n", - "\u001b[0;34m angle = arcsin(1/2 * m_object / m_counterweight)\u001b[0m\n", - "\u001b[0;34m \u001b[0m\n", - "\u001b[0;34m :m_object: mass of the object\u001b[0m\n", - "\u001b[0;34m :m_counterweight: mass of the counterweight\u001b[0m\n", - "\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m :returns: angle that the cable makes with the horizon \u001b[0m\n", - "\u001b[0;34m \"\"\"\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;31m# default angle value \u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0mangle\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0mnp\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0mpi\u001b[0m \u001b[0;34m/\u001b[0m \u001b[0;36m2\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;31m# let's check that there is actually a counterweight\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;32mif\u001b[0m \u001b[0mm_counterweight\u001b[0m \u001b[0;34m>\u001b[0m \u001b[0;36m0\u001b[0m\u001b[0;34m:\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;31m# then we compute the ratio of masses\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0mratio\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0;36m0.5\u001b[0m \u001b[0;34m*\u001b[0m \u001b[0mm_object\u001b[0m \u001b[0;34m/\u001b[0m \u001b[0mm_counterweight\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;31m# we check if the ratio of masses is in the domaine of validity of arcsin ([-1;1]) and compute the angle\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;32mif\u001b[0m \u001b[0mratio\u001b[0m \u001b[0;34m>=\u001b[0m \u001b[0;34m-\u001b[0m\u001b[0;36m1\u001b[0m \u001b[0;32mand\u001b[0m \u001b[0mratio\u001b[0m \u001b[0;34m<=\u001b[0m \u001b[0;36m1\u001b[0m\u001b[0;34m:\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0mangle\u001b[0m \u001b[0;34m=\u001b[0m \u001b[0mnp\u001b[0m\u001b[0;34m.\u001b[0m\u001b[0marcsin\u001b[0m\u001b[0;34m(\u001b[0m\u001b[0mratio\u001b[0m\u001b[0;34m)\u001b[0m\u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;34m\u001b[0m\n", - "\u001b[0;34m\u001b[0m \u001b[0;32mreturn\u001b[0m \u001b[0mangle\u001b[0m\u001b[0;34m\u001b[0m\u001b[0;34m\u001b[0m\u001b[0m\n", - "\u001b[0;31mFile:\u001b[0m ~/git/noto-poc-notebooks/TeachingExamples/lib/suspendedobjects.py\n", - "\u001b[0;31mType:\u001b[0m function\n" - ] - }, - "metadata": {}, - "output_type": "display_data" - } - ], + "outputs": [], "source": [ "get_angle_from_masses??" ] } ], "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": "3.6.8" } }, "nbformat": 4, "nbformat_minor": 4 } diff --git a/TeachingExamples/lib/suspendedobjects.py b/TeachingExamples/lib/suspendedobjects.py index a889e29..48052da 100644 --- a/TeachingExamples/lib/suspendedobjects.py +++ b/TeachingExamples/lib/suspendedobjects.py @@ -1,243 +1,250 @@ import numpy as np from ipywidgets import interact, interactive, fixed, interact_manual from ipywidgets import HBox, VBox, Label, Layout import ipywidgets as widgets from IPython.display import set_matplotlib_formats set_matplotlib_formats('svg') import matplotlib.pyplot as plt +import matplotlib.patches as pat plt.style.use('seaborn-whitegrid') # global style for plotting ###--- Functions depending on the problem parameters def get_angle_from_masses(m_object, m_counterweight): """ Compute the angle that the cable makes with the horizon depending on the counterweight chosen angle = arcsin(1/2 * m_object / m_counterweight) :m_object: mass of the object - :m_counterweight: mass of the counterweight + :m_counterweight: mass of the counterweight (has to be > 0) - :returns: angle that the cable makes with the horizon + :returns: angle that the cable makes with the horizon (in rad) """ # default angle value angle = np.pi / 2 # let's check that there is actually a counterweight if m_counterweight > 0: # then we compute the ratio of masses ratio = 0.5 * m_object / m_counterweight # we check if the ratio of masses is in the domaine of validity of arcsin ([-1;1]) and compute the angle if ratio >= -1 and ratio <= 1: angle = np.arcsin(ratio) return angle def get_object_coordinates(angle, x_origin, y_origin, distance, height): """ Computes the position of the object on the cable taking into account the angle determined by the counterweight and the dimensions of the hanging system. By default: - the object is supposed to be suspended exactly in the middle of the cable - the object is on considered the ground for all values of the angle :angle: angle that the cable makes with the horizon :x_origin: x coordinate of the bottom of the left pole (origin of the coordinate system) :y_origin: y coordinate of the bottom of the left pole (origin of the coordinate system) :distance: horizontal distance between the two poles :height: height of the poles (same height for both) :returns: coordinates of the point at which the object are hanged """ # the jean is midway between the poles x_object = x_origin + 0.5 * distance # default y value: the jean is on the ground y_object = y_origin # we check that the angle is comprised between horizontal (greater than 0) and vertical (smaller than pi/2) if angle > 0 and angle < (np.pi / 2): # we compute the delta between the horizon and the point given by the angle delta = (0.5 * distance * np.tan(angle)) # we check that the delta is smaller than the height of the poles (otherwise it just means the jean is on the ground) if delta <= height: y_object = y_origin + height - delta return [x_object, y_object] class SuspendedObjectsLab: """ This class embeds all the necessary code to create a virtual lab to study the static equilibrium of an object suspended on a clothesline with a counterweight. """ def __init__(self, m_object = 3, distance = 5, height = 1, x_origin = 0, y_origin = 0, get_angle_from_masses = get_angle_from_masses, get_object_coordinates = get_object_coordinates): ''' Initiates and displays the virtual lab on suspended objects. :m_object: mass of the suspended object :distance: horizontal distance between the two poles :height: height of the poles (same height for both) :x_origin: x coordinate of the bottom of the left pole (origin of the coordinate system) :y_origin: y coordinate of the bottom of the left pole (origin of the coordinate system) :get_angle_from_masses: function to compute the angle that the cable makes with the horizon, as a function of the respective masses of the object and the counterweight -- angle(m_object, m_counterweight) :get_object_coordinates: function to compute the coordinates of the point at which the object is suspended on the cable -- coord(angle, x_origin, y_origin, distance, height) ''' ###--- Parameters of the situation self.m_object = m_object # mass of the wet object, in kg self.distance = distance # distance between the poles, in m self.height = height # height of the poles, in m self.x_origin = x_origin # x coordinate of point of origin of the figure = x position of the left pole, in m self.y_origin = y_origin # y coordinate of point of origin of the figure = y position of the lower point (ground), in m # Functions to compute equations self.get_angle_from_masses = get_angle_from_masses self.get_object_coordinates = get_object_coordinates ###--- Then we define the elements of the ihm: # parameters for sliders self.m_counterweight_min = 0 self.m_counterweight_max = 100 self.m_counterweight = self.m_counterweight_min # initial mass of the counterweight (0 by default, no counterweight at the beginning) # IHM input elements input_layout=Layout(margin='5px 10px') self.m_counterweight_label = Label('Mass of the counterweight ($kg$):', layout=input_layout) self.m_counterweight_widget = widgets.FloatSlider(min=self.m_counterweight_min,max=self.m_counterweight_max,step=1,value=self.m_counterweight, layout=input_layout) self.m_counterweight_input = HBox([self.m_counterweight_label, self.m_counterweight_widget]) # IHM output elements self.y_object_output = widgets.Output(layout=input_layout) self.graph_output = widgets.Output(layout=input_layout) # Linking widgets to handlers self.m_counterweight_widget.observe(self.m_counterweight_event_handler, names='value') # Organize layout self.ihm = VBox([self.m_counterweight_input, self. y_object_output, self.graph_output]) ###--- Finally, we display the whole interface and we update it right away so that it plots the graph with current values display(self.ihm); self.update_lab() # Event handlers def m_counterweight_event_handler(self, change): self.m_counterweight = change.new self.update_lab() # Create visualisation def update_lab(self): # Clear outputs self.graph_output.clear_output(wait=True) self.y_object_output.clear_output(wait=True) # get angle of cable then coordinates of jean alpha = self.get_angle_from_masses(self.m_object, self.m_counterweight) + alpha_degrees = alpha*180/np.pi coord_object = self.get_object_coordinates(alpha, self.x_origin, self.y_origin, self.distance, self.height) # Create the figure fig = plt.figure(figsize=(14, 4)) ax1 = plt.subplot(131) ax2 = plt.subplot(132) ax3 = plt.subplot(133, sharex = ax2, sharey = ax1) ###--- First display the clothesline ax1.set_title('Clothesline') # Fix graph to problem boundaries ax1.set_ylim(bottom = self.y_origin) # limit bottom of y axis to ground - ax1.set_ylim(top = self.y_origin + self.height + .2) # limit top of y axis to values just above height + ax1.set_ylim(top = self.y_origin + self.height + .1) # limit top of y axis to values just above height # Customize graph style so that it doesn't look like a graph ax1.get_xaxis().set_visible(False) # hide the x axis ax1.set_ylabel("Height ($m$)") # add a label on the y axis ax1.grid(False) # hide the grid ax1.spines['top'].set_visible(False) # hide the frame except bottom line ax1.spines['right'].set_visible(False) ax1.spines['left'].set_visible(False) # Draw poles x_pole1 = np.array([self.x_origin, self.x_origin]) y_pole1 = np.array([self.y_origin, self.y_origin+self.height]) ax1.plot(x_pole1, y_pole1, "k-", linewidth=7) x_pole2 = np.array([self.x_origin+self.distance, self.x_origin+self.distance]) y_pole2 = np.array([self.y_origin, self.y_origin+self.height]) ax1.plot(x_pole2, y_pole2, "k-", linewidth=7) # Draw the hanging cable x = np.array([self.x_origin, coord_object[0], self.x_origin+self.distance]) y = np.array([self.y_origin+self.height, coord_object[1], self.y_origin+self.height]) - hangingcable = plt.Line2D(x, y, linewidth=3, linestyle = "-", color="green") - ax1.add_line(hangingcable) + ax1.plot(x, y, linewidth=3, linestyle = "-", color="green") # Draw the horizon line - horizonline = ax1.axhline(y=self.y_origin+self.height, color='gray', linestyle='-.', linewidth=1, zorder=1) + ax1.axhline(y=self.y_origin+self.height, color='gray', linestyle='-.', linewidth=1, zorder=1) - ### TODO draw the angle between hangingcable and horizonline + # Draw the angle between the hanging cable and horizonline + ellipse_radius = 0.2 + fig_ratio = self.height / self.distance + ax1.add_patch(pat.Arc(xy = (self.x_origin, self.y_origin+self.height), width = ellipse_radius/fig_ratio, height = ellipse_radius, theta1 = -1*alpha_degrees, theta2 = 0, color="gray", linestyle='-.')) + ax1.annotate(r'$\alpha$', xy=(self.x_origin+(.15/fig_ratio), self.y_origin+self.height-.05)) + #ax1.add_patch(pat.Arc(xy = (self.x_origin+self.distance, self.y_origin+self.height), width=ellipse_radius/fig_ratio, height=ellipse_radius, theta1 = 180, theta2 = 180 + alpha_degrees, color="gray", linestyle='-.')) + #ax1.annotate(r'$\alpha$', xy=(self.x_origin+self.distance-(.15/fig_ratio), self.y_origin+self.height-.05)) # Draw the point at which the object is suspended ax1.scatter(coord_object[0], coord_object[1], s=80, c="r", zorder=15) ax1.annotate('m = {} kg'.format(self.m_object), xy=(coord_object[0], coord_object[1]), xytext=(coord_object[0]+0.1, coord_object[1]-0.1)) ###--- Then display the angle and the height as functions from the mass of the counterweight - ax2.set_title('Angle of the cable vs. horizon ($^\circ$)') - ax3.set_title('Height of the suspension point ($m$)') + ax2.set_title(r'Angle $\alpha$ of the cable vs. horizon ($^\circ$)') + ax3.set_title(r'Height of the suspension point ($m$)') # Create all possible values of the mass of the counterweight m_cw = np.linspace(self.m_counterweight_min, self.m_counterweight_max, 100) # Compute the angle (in degrees) and height for all these values angle = [] height = [] for m in m_cw: a = self.get_angle_from_masses(self.m_object, m) angle.append(a*180/np.pi) c = self.get_object_coordinates(a, self.x_origin, self.y_origin, self.distance, self.height) height.append(c[1]) # Display the functions on the graphs ax2.set_xlabel('Mass of the counterweight (kg)') ax2.plot(m_cw, angle, "b") ax3.set_xlabel('Mass of the counterweight (kg)') ax3.plot(m_cw, height, "b") # Draw the horizon lines ax2.axhline(y=self.y_origin, color='gray', linestyle='-.', linewidth=1, zorder=1) ax3.axhline(y=self.y_origin+self.height, color='gray', linestyle='-.', linewidth=1, zorder=1) # Add the current angle from the counterweight selected by the user - ax2.scatter(self.m_counterweight, alpha*180/np.pi, s=80, c="r", zorder=15) + ax2.scatter(self.m_counterweight, alpha_degrees, s=80, c="r", zorder=15) # Add the current height from the counterweight selected by the user ax3.scatter(self.m_counterweight, coord_object[1], s=80, c="r", zorder=15) # Display height of object selected with self.y_object_output: print("Height of the point at which the object is hanged: {:.4f} m".format(coord_object[1])) # Display graph with self.graph_output: plt.show(); # EOF