Transcribed Text
Your team's task is to complete a MATLAB simulation of a square rigid body suspended within a ring by
one spring. The square is free to translate and rotate in the vertical plane, with gravity acting downward.
You do not need to worry about collisions between the square and the ring. Below is a diagram explaining
the setup of the system.
springAftechor Angle
o
Jg
os
=1
x
15


2
The system has already been set up for you in MATLAB. It involves four files that can be downloaded
from our Piazza course page resources area as hw09code.zip. The main file issimulate.square.starter. m.
When you first run it, this script will create the animation shown above right, except that the square will
move straight up from its starting location. Here are some things to know about this system:
The position of the center of the square is tracked through the variables x and y, both measured in m.
The velocity of the center is tracked through VX and vy, measured in m/s.
The angle of the square is tracked through the variable theta, measured in radians, with counterclock
wise positive. The object's angular velocity around the zaxis is omega, measured in rad/s.
The initial values for these states are set via variables such as xInitial.
The square's width is w, measured in m.
The square is made of sheet material that has a planar density of density, measured in kg/m²
The mass of the square is denoted n, measured in kg.
IG is the square's mass moment of inertia around the zaxis though the center of mass, which is located
at its geometric center. This parameter is measured in kgm2.
Gravity acts downward in the diagram, with gravitational acceleration having a magnitude of g, mea
sured in m/s².
The square is surrounded by a ring of radius R, measured in m. You don't need to worry about collisions
between the square and the ring.
A spring connects a stationary frictionless pivot on the ring to a frictionless pin on the square. The
square's pin is located at Dbll, byl] in the square's local frame.
The location of the spring anchor point on the ring is set through the variable springAnchorAngle.
This angle is measured in radians and is explained in the diagram above.
The spring has a rest length of springRestLength, measured in m, and it exerts forces in both
compression and extension. Its linear stiffness is springStiffness, measured in N/m.
In addition to experiencing forces from gravity and the spring, the square undergoes a translational
damping force as it moves through the simulation. This damping force is proportional to and in the
opposite direction as the velocity of the center of mass, and it acts at that point. The translational
damping coefficient is b, measured in N/(m/s).
The square feels a rotational damping moment as it moves through the simulation. This damping
moment is proportional to and in the opposite direction as the angular velocity that is occurring. The
rotational damping coefficient is beta, measured in Nm/(rad/s).
After completing these steps, make sure that your code still runs and produces a graph like the one shown
above, plus a plot of the system's energy over time. Fix any errors you encounter before proceeding.
1. Work out the dynamics of the square on a piece of paper or a whiteboard. Your analysis should include
a large freebody diagram of the square with all of the external forces and moments it is experiencing,
given its current state. Write out any additional equations you will need to formulate the NewtonEuler
equations of motion for this body, such as a vector expression for the viscous drag force. You do not
need to turn this in, but it will be useful when you're programming (I promise).
2. Complete the function compute.square.derivatives.m. This the main function that ode45 uses to
perform the entiresimulation It takes in the time t and the current state of the system Ug, ty,W/IT
Its job is to calculate the first derivative of the provided state vector: Performing
this calculation will require you to implement the dynamics you wrote out in the previous step. You
may want to use convert.local.positions.toglobal.positions, and you may also want to use the
builtin Matlab function cross, which computes cross products. Please comment your work. (4 points)
3.
Test your simulation for a wide range of initial conditions and parameter values. Use the provided
energy plot to check the physical correctness of your dynamics, and fix any problems that you uncover.
Try making the square very large or very small. Change the density of the material. Turn off the
spring by setting its stiffness to zero. Adjust the spring stiffness and the damping values. Move the
spring attachment point. Turn gravity off, then make it point upward. In all of these cases, make
sure your simulation behaves in a realistic way, and work at improving your intuition for planar rigid
body dynamics. After you've played with your simulation for about 30 minutes, configure it to your
favorite set of initial conditions and parameter values. Put a brief comment in the code near the initial
conditions to explain why you chose this configuration. (1 point)
These solutions may offer stepbystep problemsolving explanations or good writing examples that include modern styles of formatting and construction
of bibliographies out of text citations and references. Students may use these solutions for personal skillbuilding and practice.
Unethical use is strictly forbidden.