2. Suppose you analyze a 2D linear system x = Ax and find complex eigenvalues λ = λr ±iλi where X₂ = 7/2 and λ; = √√/A − (7/2)², both real. These have associated eigenvectors V+, and the the general solution is x(t) = eλrt (C+eïdi¹v+ +C_e¯ï¾‹ºv_). Use Euler's relation ei = cos 0 + i sin 0, and the fact that v₁ = V₁ ±iv, where vr and vi are both real column vectors with two entries (* shown in notes or in recitation) to write the solution in the form x(t): = : eλrt [B₁ (vr cos(λ¡t) — vį sin(\įt)) + B2 (vr sin(\¿t) + vį cos(\¿t))] How are B₁, B2 related to C+, C_? Show that even though you may find an i in one of the expressions, if the initial condition is real, then the solution will be real for all t.
2. Suppose you analyze a 2D linear system x = Ax and find complex eigenvalues λ = λr ±iλi where X₂ = 7/2 and λ; = √√/A − (7/2)², both real. These have associated eigenvectors V+, and the the general solution is x(t) = eλrt (C+eïdi¹v+ +C_e¯ï¾‹ºv_). Use Euler's relation ei = cos 0 + i sin 0, and the fact that v₁ = V₁ ±iv, where vr and vi are both real column vectors with two entries (* shown in notes or in recitation) to write the solution in the form x(t): = : eλrt [B₁ (vr cos(λ¡t) — vį sin(\įt)) + B2 (vr sin(\¿t) + vį cos(\¿t))] How are B₁, B2 related to C+, C_? Show that even though you may find an i in one of the expressions, if the initial condition is real, then the solution will be real for all t.
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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![2. Suppose you analyze a 2D linear system ẋ = Ax and find complex eigenvalues
\[
\lambda_{\pm} = \lambda_r \pm i\lambda_i
\]
where \(\lambda_r = \tau / 2\) and \(\lambda_i = \sqrt{\Delta - (\tau/2)^2}\), both real. These have associated eigenvectors \(\mathbf{v}_{\pm}\), and the general solution is
\[
\mathbf{x}(t) = e^{\lambda_r t} \left( C_+ e^{i \lambda_i t} \mathbf{v}_+ + C_- e^{-i \lambda_i t} \mathbf{v}_- \right).
\]
Use Euler’s relation \(e^{i\theta} = \cos \theta + i \sin \theta\), and the fact that \(\mathbf{v}_{\pm} = \mathbf{v}_r \pm i \mathbf{v}_i\) where \(\mathbf{v}_r\) and \(\mathbf{v}_i\) are both real column vectors with two entries (* shown in notes or in recitation) to write the solution in the form
\[
\mathbf{x}(t) = e^{\lambda_r t} \left[B_1 \left(\mathbf{v}_r \cos(\lambda_i t) - \mathbf{v}_i \sin(\lambda_i t)\right) + B_2 \left(\mathbf{v}_r \sin(\lambda_i t) + \mathbf{v}_i \cos(\lambda_i t)\right)\right]
\]
How are \(B_1, B_2\) related to \(C_+, C_-\)? Show that even though you may find an \(i\) in one of the expressions, if the initial condition is real, then the solution will be real for all \(t\).](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F97e612ef-1556-436b-b62c-352b280e9e69%2F43004ee1-95e9-4d70-82de-39f441cc18cc%2F60oeew_processed.png&w=3840&q=75)
Transcribed Image Text:2. Suppose you analyze a 2D linear system ẋ = Ax and find complex eigenvalues
\[
\lambda_{\pm} = \lambda_r \pm i\lambda_i
\]
where \(\lambda_r = \tau / 2\) and \(\lambda_i = \sqrt{\Delta - (\tau/2)^2}\), both real. These have associated eigenvectors \(\mathbf{v}_{\pm}\), and the general solution is
\[
\mathbf{x}(t) = e^{\lambda_r t} \left( C_+ e^{i \lambda_i t} \mathbf{v}_+ + C_- e^{-i \lambda_i t} \mathbf{v}_- \right).
\]
Use Euler’s relation \(e^{i\theta} = \cos \theta + i \sin \theta\), and the fact that \(\mathbf{v}_{\pm} = \mathbf{v}_r \pm i \mathbf{v}_i\) where \(\mathbf{v}_r\) and \(\mathbf{v}_i\) are both real column vectors with two entries (* shown in notes or in recitation) to write the solution in the form
\[
\mathbf{x}(t) = e^{\lambda_r t} \left[B_1 \left(\mathbf{v}_r \cos(\lambda_i t) - \mathbf{v}_i \sin(\lambda_i t)\right) + B_2 \left(\mathbf{v}_r \sin(\lambda_i t) + \mathbf{v}_i \cos(\lambda_i t)\right)\right]
\]
How are \(B_1, B_2\) related to \(C_+, C_-\)? Show that even though you may find an \(i\) in one of the expressions, if the initial condition is real, then the solution will be real for all \(t\).
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