MATLAB code is given below in bold letters.
main MATLAB script file code:
clc;
close all;
clear all;
% define the Ode solver as given below
[t,y] = ode23(@vdp1,[0 20],[0 ; 0]);
% Plot the solutions for and against t.
figure;plot(t,y(:,1),'-o',t,y(:,2),'-o')
title('Solution with ODE23');grid;
xlabel('Time t');
ylabel('Solution');
legend('position','velocity');
functionn file code:
function dydt = vdp1(t,y,mu)
% define the parameters as follows
m = 1;
c = 1;
k = 3;
f = 10;
% define the first order state space differential
equations as given below
dydt = [y(2); 1/m*(-k*y(1)-c*y(2) + f)];
Result:
Problem Set A Problem 6. (20%) A ordinary differential equation for a mass-damper-spring system is following....
Consider a mass-spring-damper system (i.e., the plant) described by the following second-order differential equation where y represents the position displacement of the mass. Our goal is to design a controller so that y can track a reference position r. The tracking error signal is then et)(t). (a) Let there be a PID controller Derive the closed-loop system equation in forms of ODE (b) Draw the block diagram of the whole system using transfer function for the blocks of plant and...
a can be skipped Consider the following second-order ODE representing a spring-mass-damper system for zero initial conditions (forced response): 2x + 2x + x=u, x(0) = 0, *(0) = 0 where u is the Unit Step Function (of magnitude 1). a. Use MATLAB to obtain an analytical solution x(t) for the differential equation, using the Laplace Transforms approach (do not use DSOLVE). Obtain the analytical expression for x(t). Also obtain a plot of .x(t) (for a simulation of 14 seconds)...
Consider a mass-spring-damper system whose motion is described by the following system of differentiat equations [c1(f-k)+k,(f-х)-c2(x-9), f=f(t), y:' y(t) with x=x( t), where the function fit) is the input displacement function (known), while xit) and yt) are the two generalized coordinates (both unknown) of the mass-spring-damper systenm. 1. Identify the type of equations (e.g. H/NH, ODE/PDE, L/NL, order, type of coefficients, etc.J. 2. Express this system of differential equations in matrix form, assume f 0 and then determine its general...
6 (10) Spring Problems: (a) Find the displacement, y(t), (in arbitrary units) as a function of time for the mass in a mass-spring system described by the differential equatiorn Zy" 10y' + 8y = 100 cos 3t + 4et assuming that the mass is released from rest at the equilibrium position. (This forcing function is not very realistic.) (b) Assume the equation from part (a) describes a mass-spring-dashpot system with a dashpot containing honey. Imagine that the honey is changed...
a-d please 6 (10) Spring Problems: (a) Find the displacement, y(t), (in arbitrary units) as a function of time for the mass in a mass-spring system described by the differential equatiorn Zy" 10y' + 8y = 100 cos 3t + 4et assuming that the mass is released from rest at the equilibrium position. (This forcing function is not very realistic.) (b) Assume the equation from part (a) describes a mass-spring-dashpot system with a dashpot containing honey. Imagine that the honey...
matlab INSTRUCTIONS Consider the spring-mass damper that can be used to model many dynamic systems Applying Newton's Second Law to a free-body diagram of the mass m yields the following ODE m습+8 +kx=F(t) (1) dt2 Where F() is a forcing function, Consider the case where the forcing function itself is a damped oscillation: Where F F(t)-Ae-Bt COS(wt) (2) For this activity we'll see how we can formulate this ODE for a solution using MATLAB that could be used to study...
Solve it with matlab 25.16 The motion of a damped spring-mass system (Fig. P25.16) is described by the following ordinary differential equation: d’x dx ++ kx = 0 m dr dt where x = displacement from equilibrium position (m), t = time (s), m 20-kg mass, and c = the damping coefficient (N · s/m). The damping coefficient c takes on three values of 5 (under- damped), 40 (critically damped), and 200 (overdamped). The spring constant k = 20 N/m....
Problem #4. The convective heat transfer problem of cold oil flowing over a hot surface can be described by the following second-order ordinary differential equations. d'T dT +0.83x = 0 dx? dx T(0)=0 (1) T(5)=1 where T is the dimensionless temperature and x is the dimensionless similarity variable. This is a boundary-value problem with the two conditions given on the wall (x=0, T(O) = 0) and in the fluid far away from the wall (x = 5, T(5) = 1)....
Elementary Differential Equation Unit Step Function Problem Project 2 A Spring-Mass Event Problenm A mass of magnitude m is confined to one-dimensional motion between two springs on a frictionless horizontal surface, as shown in Figure 4.P.3. The mass, which is unattached to either spring, undergoes simple inertial motion whenever the distance from the origin of the center point of the mass, x, satisfies lxl < L. When x 2 L, the mass is in contact with the spring on the...
Problem 1 (Harmonic Oscillators) A mass-damper-spring system is a simple harmonic oscillator whose dynamics is governed by the equation of motion where m is the mass, c is the damping coefficient of the damper, k is the stiffness of the spring, F is the net force applied on the mass, and x is the displacement of the mass from its equilibrium point. In this problem, we focus on a mass-damper-spring system with m = 1 kg, c-4 kg/s, k-3 N/m,...