TY - JOUR
T1 - A physically motivated class of scattering passive linear systems
AU - Staffans, Olof J.
AU - Weiss, George
PY - 2012
Y1 - 2012
N2 - We introduce a class of scattering passive linear systems motivated by examples from mathematical physics. The state space of the system is X = H φ E, where H and E are Hilbert spaces. We also have a Hilbert space E 0 which is dense in E, with continuous embedding, and E' 0 is the dual of E 0 with respect to the pivot space E. The input space is the same as the output space, and it is denoted by U. The semigroup generator has the structure A = [ 0L*G-1/2 -LK*K] where L ε L(E 0,H) and K ε L(E 0,U) are such that [L/K], with domain E 0, is closed as an unbounded operator from E to H φ U. The operator G ε L(E 0, E' 0) is such that Re(Gω 0,ω 0) ≤ 0 for all ω 0 ε E 0. The observation operator is C = [0 -K], the control operator is B = -C *, and the output equation is y = Cx + u = -Kw + u, where u is the input function, x = [zω] is the state trajectory, and y is the corresponding output function. We show that this system is scattering passive (hence, well-posed) and that classical solutions of the system equation x = Ax + Bu satisfy d /dt ||x(t)|| 2 = ||u(t)|| 2 - ||y(t)|| 2 + 2Re (Gω,ω). Moreover, the dual system satisfies a similar power balance equation. Hence, this system is scattering conservative if and only if Re(Gω 0, ω 0) = 0 for all ω 0 ε E 0. We give two examples involving the beam equation and one with Maxwell's equations.
AB - We introduce a class of scattering passive linear systems motivated by examples from mathematical physics. The state space of the system is X = H φ E, where H and E are Hilbert spaces. We also have a Hilbert space E 0 which is dense in E, with continuous embedding, and E' 0 is the dual of E 0 with respect to the pivot space E. The input space is the same as the output space, and it is denoted by U. The semigroup generator has the structure A = [ 0L*G-1/2 -LK*K] where L ε L(E 0,H) and K ε L(E 0,U) are such that [L/K], with domain E 0, is closed as an unbounded operator from E to H φ U. The operator G ε L(E 0, E' 0) is such that Re(Gω 0,ω 0) ≤ 0 for all ω 0 ε E 0. The observation operator is C = [0 -K], the control operator is B = -C *, and the output equation is y = Cx + u = -Kw + u, where u is the input function, x = [zω] is the state trajectory, and y is the corresponding output function. We show that this system is scattering passive (hence, well-posed) and that classical solutions of the system equation x = Ax + Bu satisfy d /dt ||x(t)|| 2 = ||u(t)|| 2 - ||y(t)|| 2 + 2Re (Gω,ω). Moreover, the dual system satisfies a similar power balance equation. Hence, this system is scattering conservative if and only if Re(Gω 0, ω 0) = 0 for all ω 0 ε E 0. We give two examples involving the beam equation and one with Maxwell's equations.
KW - Beam equation
KW - Cayley transform
KW - Maxwell's equations
KW - Scattering conservative system
KW - Scattering passive system
KW - System node
UR - http://www.scopus.com/inward/record.url?scp=84868383220&partnerID=8YFLogxK
U2 - 10.1137/110846403
DO - 10.1137/110846403
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:84868383220
SN - 0363-0129
VL - 50
SP - 3083
EP - 3112
JO - SIAM Journal on Control and Optimization
JF - SIAM Journal on Control and Optimization
IS - 5
ER -