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Chapter Summary and Problems

Summary

This chapter introduced the dynamic-system ideas needed for CCD. Physical modeling leads to differential equations, and state-space representation organizes those equations using states, inputs, outputs, and disturbances. Open-loop control relies on prediction, while closed-loop control uses feedback to respond to actual behavior. Stability describes what trajectories do near an equilibrium, and feedback changes stability and response by changing the closed-loop dynamics. Most importantly for CCD, plant design variables change the dynamic model and therefore change which controller is best.

Key terms

Dynamic system; state; control input; output; disturbance; differential equation; multidisciplinary analysis (MDA); differential-algebraic equation (DAE); index-1 DAE; algebraic constraint; state-space representation; linearization; open-loop system; closed-loop system; feedback; equilibrium; stability; asymptotic stability; eigenvalue; natural frequency; damping ratio; closed-loop poles.

Problems

  1. Nonlinear modeling and local dynamics. A torque-actuated pendulum satisfies ml2θ¨+bθ˙+mglsinθ=uml^2\ddot\theta+b\dot\theta+mgl\sin\theta=u. Derive its nonlinear state-space model and the exact linearization about the upright equilibrium, then determine the state-feedback gains that place the linearized poles at a prescribed stable conjugate pair.

  2. Plant design and controllability. A flexible two-mass system obeys M(p)q¨+Cq˙+K(p)q=b(ra)uM(p)\ddot q+C\dot q+K(p)q=b(r_a)u, where pp changes stiffness and rar_a is actuator location. Derive a modal controllability metric and use it to state a quantitative co-design criterion that prevents any retained mode from becoming weakly actuated.

  3. LQR-dependent plant selection. For x˙=[01k/mc/m]x+[01/m]u\dot x=\begin{bmatrix}0&1\\-k/m&-c/m\end{bmatrix}x+\begin{bmatrix}0\\1/m\end{bmatrix}u and J=0(xTQx+ru2)dt+γmJ=\int_0^\infty(x^TQx+ru^2)dt+\gamma m, derive the algebraic-Riccati sensitivity equations needed to compute the total derivative of the optimized closed-loop cost with respect to mm.

  4. Robust stability over a design family. The closed-loop matrix is Acl(p)=A0+pA1BKA_{cl}(p)=A_0+pA_1-BK for p[p,p+]p\in[p_-,p_+]. Formulate and justify a common quadratic Lyapunov inequality that certifies a uniform exponential decay rate over the entire interval, reducing the infinite family to finitely many matrix inequalities when the dependence is affine.

  5. Observer--plant interaction. A sensor placement variable ss changes the output matrix C(s)C(s) in x˙=A(p)x+Bu\dot x=A(p)x+Bu, y=C(s)x+vy=C(s)x+v. Derive the observability Gramian and formulate a joint placement--estimator design constraint that bounds the worst-direction state-estimation uncertainty over a finite horizon.

  6. Sampled-data feedback. For x˙=Ax+Bu\dot x=Ax+Bu with zero-order-hold control u(t)=Kx(kh)u(t)=-Kx(kh) on kht<(k+1)hkh\le t<(k+1)h, derive the exact discrete closed-loop matrix and determine the largest sampling period hh that preserves asymptotic stability for a specified numerical pair (A,B,K)(A,B,K).

  7. Disturbance attenuation. The quarter-car model is Mq¨+Cq˙+Kq=Buu+BwwM\ddot q+C\dot q+Kq=B_uu+B_ww, with performance output z=Czx+Dzuz=C_zx+D_zu. Derive the bounded-real linear matrix inequality that certifies Twz<γ\|T_{w\to z}\|_\infty<\gamma and identify which matrix terms change when suspension stiffness is a design variable.

  8. Region of attraction under actuator saturation. For x˙=Ax+Bsat(Kx,umax)\dot x=Ax+B\operatorname{sat}(-Kx,u_{\max}), derive an invariant ellipsoidal inner approximation E(P)={x:xTPx1}\mathcal E(P)=\{x:x^TPx\le1\} by combining a Lyapunov inequality with constraints ensuring the feedback remains unsaturated inside E(P)\mathcal E(P).

  9. Unmodeled flexible dynamics. A nominal rigid-body plant G0(s)=1/(Js2)G_0(s)=1/(Js^2) is augmented by a flexible mode Gf(s)=ωf2/(s2+2ζfωfs+ωf2)G_f(s)=\omega_f^2/(s^2+2\zeta_f\omega_fs+\omega_f^2). Derive a robust-stability restriction on controller bandwidth using multiplicative uncertainty and show how increasing structural stiffness can enlarge the admissible bandwidth.

  10. Dynamic feasibility of an index-one DAE. An electromechanical actuator satisfies Li˙+Ri+keω=vL\dot i+Ri+k_e\omega=v, Jω˙=ktiτLJ\dot\omega=k_ti-\tau_L, and the algebraic saturation law 0=isat(ic,imax(T))0=i-\operatorname{sat}(i_c,i_{\max}(T)). Formulate a consistent state--algebraic representation and derive the conditions under which an equilibrium and its local linearization are well defined.

References and further reading

  1. Allison, J. T., & Herber, D. R. (2014). Multidisciplinary design optimization of dynamic engineering systems. AIAA Journal, 52(4), 691–710. DOI: 10.2514/1.J052182

  2. Allison, J. T., Guo, T., & Han, Z. (2014). Co-design of an active suspension using simultaneous dynamic optimization. Journal of Mechanical Design, 136(8), Article 081003.

  3. Garcia-Sanz, M. (2019). Control co-design: An engineering game changer. Advanced Control for Applications: Engineering and Industrial Systems, 1(1), Article e18. DOI: 10.1002/adc2.18

  4. Herber, D. R., & Allison, J. T. (2019). Nested and simultaneous solution strategies for general combined plant and control design problems. Journal of Mechanical Design, 141(1), Article 011402. DOI: 10.1115/1.4040705

  5. Martins, J. R. R. A., & Ning, A. (2021). Engineering design optimization. Cambridge University Press.

  6. Franklin, G. F., Powell, J. D., & Emami-Naeini, A. (2019). Feedback control of dynamic systems (8th ed.). Pearson.

  7. Herber, D. R. (2017). Advances in Combined Architecture, Plant, and Control Design (Doctoral dissertation). University of Illinois at Urbana-Champaign.