Converting differential equations to State-Space/Transfer Function representation
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I'm trying to solve some Control Systems questions, but having trouble with a few of them:

Basically, the question asks for the state-space representation of each system.
I used odeToVectorField for systems a and b:
syms y(t) u(t) t
yd = diff(y);
ydd = diff(y, 2);
yddd = diff(y, 3);
EQD = ydd + 3*yd + y == u
[SS, Sbs] = odeToVectorField(EQD)
EQD2 = yddd + 5*ydd + 8*yd + 12*y == u
[SS2, Sbs2] = odeToVectorField(EQD2)
from which I can get the state-space representation.
But when I get to the other systems (for example, system f), it gets trickier, and most of the systems can't even be solved using odeToVectorField.
syms y(t) u(t) t
yd = diff(y);
ydd = diff(y, 2);
yddd = diff(y, 3);
yi = int(y, 0, t);
ud = diff(u);
EQD = ydd + 2*yd + y + yi == ud + 5*u
[SS, Sbs] = odeToVectorField(EQD)
Is there an easier way to get the state-space representation (or transfer function) directly from the differential equations? And how can I do the same for the more complex differential equations (like f and g, for example)?
Thank you
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採用された回答
Paul
2021 年 11 月 23 日
編集済み: Paul
2021 年 11 月 23 日
There really is no need to use the symbolic stuff (though you can if you really want, at least for part of the problem). Suppose Z(s) is the Laplace transform of z(t). You just need know how to express the Laplace transform of dz(t)/dt and integral(z(t)) (using bad notation) in terms of Z(s). You will find these relationships in your class notes or text book or any number of on line sources. Once you know how to do that, you'll be able to solve each of those equations for the ratio Y(s)/U(s). At that point you can use ss() to find a (not "the") state space representation.
For example, suppose you found: Y(s)/U(s) = (2s + 1)/(s^2 + s + 2). You can find a state space model as
ss(tf([2 1],[1 1 2]))
But you'll have to find Y(s)/U(s) first.
Problem g is trickier. There you'll have to find the matrix M(s) such that [Y1(s);Y2(s)] = M(s)*[U1(s);U2(s), then express M as a tf object, and then use ss(M).
5 件のコメント
Paul
2021 年 11 月 24 日
Here you go
syms y(t) u(t) tau
eqn = diff(y(t),t,2)+2*diff(y(t),t) + y + int(y(tau),tau,0,t) == diff(u(t),t) + 5*u(t)
Leqn = laplace(eqn)
syms Dy0
Leqn = subs(Leqn,subs(diff(y(t), t), t, 0),Dy0)
Leqn = subs(Leqn,[y(0) Dy0 u(0)],[0 0 0])
syms Y U s
Leqn = subs(Leqn,[laplace(y(t),t,s) laplace(u(t),t,s)],[Y U])
Y = solve(Leqn,Y)
H(s) = Y/U
H = simplify(H)
その他の回答 (1 件)
Samim Unlusoy
2022 年 12 月 22 日
The following approach may be useful. State equations for the classical ordinary matrix differential equations
[M]{yddot} + [C]{ydot} + [K]{y} = [F]{q}
are given by:
[0] [I] [0]
{xdot} = [A]{x} + [B]{u] = {x} + {u}
-inv[M] [K] -inv[M] [C] inv[M] [C]
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