HOW TO: Using each step result in subsequent step during integration via ODE

조회 수: 8 (최근 30일)
Presley
Presley 2023년 7월 31일
댓글: Torsten 2023년 10월 7일
Hello, I am trying to solve these equation of motion using ode45. The implementation process in Matrix format is presented below.
x0=zeros(16,1);
opts=odeset('RelTol',1e-6);
% Freq = linspace(1,4000,50);
ti = 0; % initial time step
tf = 1; % final time step
dt = 0.001 ; % size of the time step
nt = fix((tf-ti)/dt)+1; % number of time steps
tau = 0:dt:tf;
W = 4000
[t, Xx] = ode45(@gearCH, tau, x0, opts, W);
function Xx=gearCH(t,x0,W)
m1 = 2.8;
i1 = 0.003655;
j1 = 0.00731;
m2 = m1;
i2 = i1;
j2 = j1;
kby1 = 5e9;
kbz1 = 4e8;
kb0 = 3.23e6;
kby2 = kby1;
kbz2 = kbz1;
r1 = 70e-3;
r2 = r1;
beta=deg2rad(25.232);
e5= .01e-6;
torload = 450; % Output Torque (lb-in, N-m)
et = e5 * sin(W * t);
M = blkdiag(m1, m1, i1/(r1^2), j1/(r1^2), m2, m2, i2/(r2^2), j2/(r2^2)); %mass
Kb = blkdiag (kby1, kbz1, kb0/(r1^2), 0, kby2, kbz2, kb0/(r2^2), 0); %bearing stiff
Q = [cos(beta) -sin(beta) sin(beta) cos(beta) -cos(beta) sin(beta) sin(beta) cos(beta)]'; %Q
Kt = 3.6e8; %%use as time invariant here
Km = Kt *( Q* Q');
Fb = [0 0 0 torload/r1 0 0 0 torload/r2]';
Fc = (Kt*et)*Q;
cma = (2*0.03) * sqrt(Kt /((1/r1) + (1/r2)));
cG = cma*( Q* Q'); %gear estimated damping
cB = 2.5e-5*Kb; %bearing estimated damping
K = Kb + Km; %stiffness matrix
C = cG + cB; %damping matrix
P = Fb + Fc; %force
Xx=[x0(9:16);inv(M)*(P-C*x0(9:16)-K*x0(1:8))];
end
As can be seen, this is done using ode45 and also, I have not use p(t) and p(t) dot, to multiply K and C as required. How can I get the displacements X, for each time so I can calulate p(t), multiply it by K and C for the next integration during the whole process? It seems I have to implement Rung-Kutta manually, maybe not. But how can I achieve that given this 8 second order odes? Thank you

답변 (3개)

Joe
Joe 2023년 7월 31일
I am not sure this is doable using matlab. The equations are not common, at least to me. Try SciPy maybe

Torsten
Torsten 2023년 7월 31일
편집: Torsten 2023년 7월 31일
All variables needed to compute p(t) are part of the solution vector x which is input to "gearCH". So I don't see the problem to compute p(t) from them.
  댓글 수: 7
Torsten
Torsten 2023년 10월 7일
You will get exact solutions also with a low order code if you strengthen the tolerances in the options setting. So I suggest using ODE45 with smaller values for RelTol and/or AbsTol.

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Sam Chak
Sam Chak 2023년 10월 7일
From your provided formula, both and can be directly computed from the ode45 solution vector x. Could you please verify if they have been plotted correctly?
% Freq = linspace(1, 4000, 50);
ti = 0; % initial time step
tf = 0.02; % final time step
dt = 1/20000; % size of the time step
% nt = fix((tf-ti)/dt)+1; % number of time steps
% call ode45 solver
tspan = 0:dt:tf;
x0 = zeros(16, 1);
opts = odeset('RelTol', 1e-6);
W = 4000;
[t, x] = ode45(@gearCH, tspan, x0, opts, W);
% plot pt and dp/dt
beta = deg2rad(25.232);
e5 = .01e-6;
et = e5*sin(W*t);
pt = (x(:,1) - x(:,5) + x(:,4) + x(:,8))*cos(beta) + (- x(:,2) + x(:,6) + x(:,3) + x(:,7))*sin(beta) - et;
dpdt = (x(:,9) - x(:,13) + x(:,12) + x(:,16))*cos(beta) + (- x(:,10) + x(:,14) + x(:,11) + x(:,15))*sin(beta) - e5*W*cos(W*t);
figure(1)
subplot(211)
plot(t, pt), grid on, xlabel('t'), ylabel('p_{t}')
subplot(212)
plot(t, dpdt), grid on, xlabel('t'), ylabel('dp/dt')
% plot solution
figure(2)
for j = 1:16
subplot(4,4,j)
plot(t, x(:,j)), grid on
title("x"+string(j));
end
% Equations of Motion
function dxdt = gearCH(t, x, W)
% parameters
m1 = 2.8;
i1 = 0.003655;
j1 = 0.00731;
m2 = m1;
i2 = i1;
j2 = j1;
kby1 = 5e9;
kbz1 = 4e8;
kb0 = 3.23e6;
kby2 = kby1;
kbz2 = kbz1;
r1 = 70e-3;
r2 = r1;
beta = deg2rad(25.232);
e5 = .01e-6;
torload = 450; % Output Torque (lb-in, N-m)
et = e5*sin(W*t);
pt = (x(1) - x(5) + x(4) + x(8))*cos(beta) + (- x(2) + x(6) + x(3) + x(7))*sin(beta) - et;
dpdt = (x(9) - x(13) + x(12) + x(16))*cos(beta) + (- x(10) + x(14) + x(11) + x(15))*sin(beta) - e5*W*cos(W*t);
% Mass matrix
M = blkdiag(m1, m1, i1/(r1^2), j1/(r1^2), m2, m2, i2/(r2^2), j2/(r2^2));
% Bearing stiffness matrix
Kb = blkdiag (kby1, kbz1, kb0/(r1^2), 0, kby2, kbz2, kb0/(r2^2), 0);
% Q array
Q = [cos(beta) -sin(beta) sin(beta) cos(beta) -cos(beta) sin(beta) sin(beta) cos(beta)]';
% unnamed parameter used in the computation of Km
Kt = 3.6e8; % used as time invariant here
% untitled Q-based square matrix
Km = pt*Kt*(Q*Q'); % <-- pt is injected here
% untitled b-force
Fb = [0 0 0 torload/r1 0 0 0 torload/r2]';
% untitled c-force
Fc = (Kt*et)*Q;
% unnamed parameter used in the computation of cG
cma = 2*0.03*sqrt(Kt/(1/r1 + 1/r2));
% gear-estimated damping marix
cG = dpdt*cma*(Q*Q'); % <-- dp/dt is injected here
% bearing-estimated damping matrix
cB = (2.5e-5)*Kb;
% True stiffness matrix
K = Kb + Km;
% True damping matrix
C = cG + cB;
% Total force
F = Fb + Fc;
% Equations of Motion
dxdt = zeros(16, 1);
dxdt(1:8) = x(9:16); % kinematics
dxdt(9:16) = M\(F - C*x(9:16) - K*x(1:8)); % dynamics
end
  댓글 수: 1
Presley
Presley 2023년 10월 7일
Thanks for the response, however, the problem continued under Torsten post. I was trying a manual implementation of the these solvers in a higher order. I will give feedback after trying the 6th order, Thanks

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