Week 3 - Solving second order ODEs
AIM: To write a program in MATLAB that will simulate the pendulum motion.
OBJECTIVE:
- To solve the given ODE that represents the equation of motion of a simple pendulum.

Where, g = gravity in m/s^2,
L = length of the pendulum in m,
M = mass of the ball in kg,
B = damping coefficient.
- From the results of ODE animate the motion of the pendulum.
GIVEN DATA:
L = 1 metre,
m = 1kg,
b = 0.05,
g = 9.81m/s^2
angular velocity = 3rad/sec at t = 0
time span = 0 – 20sec
THEORY AND CALCULATIONS:
In given equation,
Let us consider,
θ = θ1............(1)
dθ/dt = dθ1/dt = θ2............(2)
d^2θ/dt^2 = dθ2/dt..........(3)
By using above constants, the second order differential equation becomes,
dθ2/dt = -(b/m)θ2 – (g/l)sinθ
Writing above equation in form of matrix

Using the above equation and ode45 solver we can solve the equation and animate the simple pendulum in MATLAB
Note:
- Ode45 solver is an inbuilt solver in MATLAB. The ode45 solver requires simple differential equation to solve any kind of higher order differential equation.
- The given equation is of order 2 so i simplified it in simple ODE to use ode45 which is developed on basis of Runge-kutta method to solve higher order differential equation.
- Syntax of ode45 solver
[t,results]=Ode45(@(t,theta) ode_func(t,theta,b,g,l,m),t_span,theta_0)
MATLAB Code:
clear all
close all
clc
%inputs
b = 0.05;
g = 9.81;
l = 1;
m = 1;
% Initial Condition
% angular displacement is 0 and angular velocity is 3rad/sec
theta_0 = [0;3];
% time points
%pendulum oscillates between 0-20 seconds
t_span = linspace(0,20,200);
% solving ODE using ode45 function
[t,results] = ode45(@(t,theta) ode_func(t,theta,b,g,l,m),t_span,theta_0);
%plotting of angular velocity and displacement
figure(1)
plot(t,results(:,1))
hold on
plot(t,results(:,2))
title('motion of pendulum')
ylabel('displacement vs angular velocity')
xlabel('time')
legend('displacement','angular velocity')
grid on
% Starting loop to get animation
ct = 1;
for i = 1:length(t_span)
figure(2)
%fixed coordinates of one end of pendulum
x0 = 0;
y0 = 0;
%moving coordinates (bob)
x1 = l*sin(results(i,1));
y1 = -l*cos(results(i,1));
%plotting the animation
figure(2)
plot([x0 x1],[y0 y1],'linewidth',3,'Color','b')
hold on
plot(x1,y1,'o','markersize',15,'MarkerFaceColor','r')
plot([-3 3],[0 0],'LineWidth',2,'Color','g')
hold off
title('motion of pendulum')
axis([-3 3 -2 2])
grid on
M(ct) = getframe(gcf);
ct = ct+1;
end
% Animation of pendulum
movie(M)
videofile = VideoWriter('pendulum_animatin.avi');
open(videofile)
writeVideo(videofile,M)
close(videofile)
Function Code(ode_func):
function [dtheta_dt] = ode_func(t,theta,b,g,l,m)
theta1 = theta(1);
theta2 = theta(2);
dtheta1_dt = theta2;
dtheta2_dt = -(b/m)*theta2-(g/l)*sin(theta1);
dtheta_dt = [dtheta1_dt;dtheta2_dt];
end
OUTPUT:
the following plot obtained by the given data.

- The plot is drawn between angular acceleration and displacement of motion of simple pendulum
- The blue curve is displacement and red is angular velocity as shown in legend.
- At the end both velocity and diplacement becomes zero and pendulum comes in rest.
CONCLUSION:
we have animated the simple pendulum by the given data and ode45 solver.
ANIMATION LINK: