Doubt in Coupled Ode
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I have written a code for coupled ode using ode45; however my results seems errornous when compared with analytical results:
%% Analytical
L=24;
A=9;
Iz=2.43;
J=21.18;
E=33.2e9;
EI=E*Iz;
rho=2.4e4;
volume=A*L;
m=(rho*A);
Fv=29.9e4;
theta=30*(pi/180);
R=L/theta;
v=40;
mu=0.2;
G=E/(2*(1+mu));
GJ=G*J;
g=10;
a1=(1/m)*(pi/L)^2*(EI*((pi/L)^2)+(GJ/(R^2)));
a2=(1/(m*R))*((pi/L)^2)*(EI+GJ);
b1=-(1/(rho*J))*((EI/R^2)+(GJ*((pi/L)^2)));
b2=-(1/(rho*J))*(1/R)*((pi/L)^2)*(EI+GJ);
wv=32.10; %% book formula provided in snip shot with constants
% factor_1=sqrt(((a1-b1)^2)+(4*a2*b2));
% wv=sqrt((a1+b1+factor_1)/2) ;% however I am getting different with my constants
g=10;
t=0.01:0.01:(L/v);
Sv=(pi*v)/(L*wv);
beta=(b1-(pi*v/L)^2)/(b1+a1-wv^2-(pi*v/L)^2);
xi=sin(pi*v*t/L)-(Sv*sin(wv*t));
u_deflect=-((2*Fv*g)/(m*L))*(1/wv^2)*(1/(1-Sv^2))*beta*xi;
figure();plot(t,u_deflect,'o-');title('Validation');
My code is:
%% Analysis using ode45
tspan_1=[0:0.001:0.6];%time range
y0_1=[0;0;0;0];%initial conditions f
[t1,y1]=ode45(@diffeqn11,tspan_1,y0_1);
%plot displacement
figure(1)
plot(t1, y1(:,1), 'r', 'LineWidth',2);title('Displacement of the beam');
hold on
plot(t1, y1(:,3), 'b', 'LineWidth',2);
%plot velocity_forced+free
figure(2)
plot(t1, y1(:,2), 'g', 'LineWidth',2);title('Velocity of the beam');
figure(3)
plot(t1, y1(:,4), 'r', 'LineWidth',2);
function f= diffeqn11(t,y)
L=24;
A=9;
Iz=2.43;
J=21.18;
E=33.2e9;
EI=E*Iz;
rho=2.4e4;
volume=A*L;
m=(rho*A);
Fv=29.9e4;
theta=30*(pi/180);
R=L/theta;
v=40;
mu=0.2;
G=E/(2*(1+mu));
GJ=G*J;
g=10;
a1=(1/m)*(pi/L)^2*(EI*((pi/L)^2)+(GJ/(R^2)));
a2=(1/(m*R))*((pi/L)^2)*(EI+GJ);
b1=-(1/(rho*J))*((EI/R^2)+(GJ*((pi/L)^2)));
b2=-(1/(rho*J))*(1/R)*((pi/L)^2)*(EI+GJ);
f=zeros(4,1);
f(1)=y(2);
f(2)=((2*Fv)/(m*L))*sin((pi*v*t)/L)-(a1*y(1))-(a2*y(3));
f(3)=y(4);
f(4)=-(b1*y(3))-(b2*y(1));
end
1 comentario
Torsten
el 16 de Nov. de 2023
Either the solution you took from the book is wrong or your differential equations are wrong.
Respuesta aceptada
Más respuestas (1)
Your 4th-order coupled system has two eigenvalues with positive real parts. Therefore, in theory, the state responses will diverge when the system is forced.
% parameters
a1 = 120.7217;
a2 = 1.3587e+06;
b1 = -4.4643e+06;
b2 = -1.2327e+05;
% state matrix
A = [ 0 1 0 0;
-a1 0 -a2 0;
0 0 0 1;
-b2 0 -b1 0];
% check eigenvalues
eig(A)
2 comentarios
Please note that in your beam-coupled system, there is typically no damping considered. However, in the real physical world, damping components exist. As a structural engineer, you can either incorporate other beams with stabilizing properties, or measure the deflections of existing beams and then counteract destabilizing vibration modes.
%% Analysis using ode45
tspan_1 = [0:0.001:4*pi]; % time range
y0_1 = [0; 0; 0; 0]; % initial conditions f
options = odeset('RelTol', 1e-8, 'AbsTol', 1e-8);
[t1, y1] = ode45(@diffeqn11, tspan_1, y0_1, options);
% plot displacement
figure(1)
plot(t1/pi, y1(:,1:2:3)); grid on,
title('Displacements of the beams'), xlabel('t/\pi')
legend('y_{1}', 'y_{3}', 'location', 'SE')
% A pair of Beam couples
function f = diffeqn11(t, y)
% parameters
a1 = 120.7217;
a2 = 1.3587e+06;
b1 = -4.4643e+06;
b2 = -1.2327e+05;
Constant= 0.1154;
% measure the deflections and velocities, and feed them back into the
% system in the same channel, where the sinusoidal force is injected.
k1 = 10562734.7949266;
k2 = 4596.24524333348;
k3 = 382536034.238245;
k4 = 181690.721406603;
K = [k1 k2 k3 k4];
f = zeros(4, 1);
u = Constant*sin(0.5*t) - K*y;
f(1) = 0*y(1) + 1*y(2) + 0*y(3) + 0*y(4);
f(2) = - a1*y(1) + 0*y(2) - a2*y(3) + 0*y(4) + u;
f(3) = 0*y(1) + 0*y(2) + 0*y(3) + 1*y(4);
f(4) = - b2*y(1) + 0*y(2) - b1*y(3) + 0*y(4);
end
Susmita Panda
el 16 de Nov. de 2023
Editada: Susmita Panda
el 16 de Nov. de 2023
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