Law of motion through numerical aproximation
Show older comments
A ball of mass m=0.12 kg is a t rest at the origin of the X axis.
At the moment t0=0 a force parallel to the X axis begins to act upon the ball.
The force varies in time by the expression:
F(t)=6*sin(4*pi*t-pi/6)-0.5.
Numerically aproximate the law of motion x(t) of the ball and plot it for the time interval t=[0,10].
m=0.12
initial_time=0;
final_time=10;
N=1001;
t=linspace(initial_time,final_time,N);
dt=t(2)-t(1);
x(1)=0;
x(2)=0;
for i=2:N-1
x(i+1)=2*x(i)-x(i-1)+dt*dt*(6*sin(4*pi*t(i)-pi/6)-0.5);
end;
plot(t,x);
m=0.12 ;
initial_time=0;
final_time=10;
N=1001;
t=linspace(initial_time,final_time,N);
dt=t(2)-t(1);
The ball at t0 is at position 0 on the X axis, so x0=0
there is no initial speed so x1=x0=0
x(1)=0;
x(2)=0;
for i=2:N-1
x(i+1)=2*x(i)-x(i-1)+dt*dt*(6*sin(4*pi*t(i)-pi/6)-0.5)/m;
end
plot(t,x);
I do not think I got the correct solution to this problem, it seems a little bit weird that the ball is only moving in one direction, shouldn't it oscilate araound an center point given that the function is dependant of sin?
Accepted Answer
More Answers (1)
David Hill
on 9 Jan 2020
F=@(t)6*sin(4*pi*t-pi/6)-0.5;
t=0:.01:10;
a=F(t)/.12;
v=cumtrapz(a);
d=cumtrapz(v);
plot(t,d);
Categories
Find more on Earth and Planetary Science in Help Center and File Exchange
Community Treasure Hunt
Find the treasures in MATLAB Central and discover how the community can help you!
Start Hunting!