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EE611 Deterministic Systems
Solutions of Linear Dynamical Equations Kevin D. Donohue Electrical and Computer Engineering University of Kentucky
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Time-Domain Solution of LTI State Equation
Given a LTI state-space equation: Show the solution for the state can be expressed as: and output as: x π‘ =Ax π‘ +Bu π‘ y π‘ =Cx π‘ +Du π‘ x π‘ =exp Aπ‘ x π‘ exp ξA π‘βΟ ξ Bu Ο πΟ y π‘ =Cexp Aπ‘ x 0 +C 0 π‘ exp ξA π‘βΟ ξ Bu Ο πΟ+Du π‘
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Laplace-Domain Solution of LTI State Equation
Given a LTI state-space equation: Show the solution for the Laplace transform of the state can be expressed as: and output as: x π‘ =Ax π‘ +Bu π‘ y π‘ =Cx π‘ +Du π‘ x Λ ξπ ξ = ξπ IβAξ β1 x ξπξ + ξπ IβAξ β1 B u Λ π y Λ ξπ ξ =C ξπ IβAξ β1 x ξπξ + ξC ξπ IβAξ β1 B+Dξ u Λ π
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Examples Find the unit step response to the following state-space equation for t ο³ 0: Show: x = β2 3 0 β1 x π’ π‘ withx 0 = β1 1 y= x x π‘ = β 5 2 exp β2π‘ 1 forπ‘β₯0 π¦ π‘ = 1 2 ξ3β5exp β2π‘ ξ forπ‘β₯0
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Discretization Consider sampling the inputs and outputs of a state-space equation with sampling interval T = 1/fs where fs is the sampling frequency. Show that the corresponding discrete system can be represented by: where k corresponds to t=kT and: x π‘ =Ax π‘ +Bu π‘ y π‘ =Cx π‘ +Du π‘ x π+1 = A π x π + B π u π y π = C π x π + D π u π B π = ξ 0 π exp AΟ πΟξ B A π =exp Aπ C π =C D π =D
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Solution of Discrete LTI State Equation
Given a discrete-time state equation: Show that the solution can be written as: x π+1 =Ax π +Bu π y π =Cx π +Du π x π = A π x 0 + π=0 πβ1 A πβ1βπ Bu π y π =C ξ A π x 0 + π=0 πβ1 A πβ1βπ Bu π ξ +Du π
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Examples Find the solution to the following discrete-time state equation for k ο³ 0 and no input (zero input response): show: x π+1 = β x π π’ π‘ withx 0 = 0 β1 x π = β ξ ξ π sin .588π β ξ ξ π cos .588π forπβ₯0
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Equivalence Given an n by n nonsingular matrix P that represents a change of basis then the following systems are (algebraically) equivalent: where x Λ =Px x Λ π‘ = A Λ x Λ π‘ + B Λ u π‘ x π‘ =Ax π‘ +Bu π‘ y π‘ = C Λ x Λ π‘ + D Λ u π‘ y π‘ =Cx π‘ +Du π‘ A Λ =PA P β1 B Λ =PB C Λ =C P β1 D Λ =D
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Zero-State Equivalence
State equations are zero-state equivalent iff they have the same transfer matrix: It can be shown that 2 LTI state equations are zero-state equivalent iff C ξπ IβAξ β1 B+D= C Λ ξπ Iβ A Λ ξ β1 B Λ + D Λ {A,B,C,D} { A Λ , B Λ , C Λ , D Λ } D= D Λ C A π¦ B= C Λ A Λ π¦ B Λ forπ=0,1,2,...
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Modal Form Complex Eigenvalues
Consider the following Jordan form A similarity transformation can be preformed to convert it to all real values in the following modal form: Ξ» Ξ± 1 +π Ξ² Ξ± 1 βπ Ξ² Ξ± 2 +π Ξ² Ξ± 2 βπ Ξ² 2 Ξ» Ξ± 1 Ξ² β Ξ² 1 Ξ± Ξ± 2 Ξ² β Ξ² 2 Ξ± 2
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Modal Form Complex Eigenvalues
Given a matrix A with complex eigenvalues, it can be diagonalized with eigenvector Q, and then a matrix can be found to put in modal form. Example: Find similarity transformation to perform the form change: Show Q Λ PAQ= A ππ’ππ π¨π§ππ₯ P Λ A ππ’ππ π¨π§ππ₯ Q Λ = A π¦π¨πππ₯ P Λ PAQ Q Λ = A π¦π¨πππ₯ Ξ± 1 +π Ξ² Ξ± 1 βπ Ξ² 1 Ξ± 1 Ξ² 1 β Ξ² 1 Ξ± 1 P= 1 βπ 1 π Q= π βπ
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Modal Form Complex Eigenvalues
In general for any A with complex eigenvalues, can be found directly from the eigenvalues associated with where q1 and q2 are associated with a complex conjugate eigenvalues (note the eigenvector will also be complex conjugate pairs as well). Then Q Q Λ Q Q= q π , q π ,..., q n Q Q Λ = ππππ₯ q π ,ππ¦ππ q π ,..., q n
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Lecture Note Homework U5.1
Find the solution y[k] for: given the system is relaxed at k = 0 and input is the unit impulse. x π+1 = 0.5 β x π u π y π = π π x π
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