Difference between revisions of "CDS 140a Winter 2015 Homework 3"
(Created page with "{{CDS homework  instructor = R. Murray  course = CDS 140  semester = Winter 2015  title = Problem Set #3  issued = 19 Jan 2015  due = 28 Jan 2015 at 12:30 pm<br>In...") 

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<li>'''Perko, Section 2.7, problem 1'''  <li>'''Perko, Section 2.7, problem 1'''  
Write the system  Write the system  
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with $\lambda_1<0$, $\lambda_2>0$ and $G(y)$ is quadratic in $y_1$ and $y_2$.  with $\lambda_1<0$, $\lambda_2>0$ and $G(y)$ is quadratic in $y_1$ and $y_2$.  
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+  <! 2014 TA comments: A lot of people also were confused about solving for the unstable manifold by simply letting xdot =  f(x) on #1. >  
<li>'''Perko, Section 2.7, problem 2'''  <li>'''Perko, Section 2.7, problem 2'''  
Find the first three successive approximations $u^{(1)}(t,a)$, $u^{(2)}(t,a)$, and $u^{(3)}(t,a)$ for  Find the first three successive approximations $u^{(1)}(t,a)$, $u^{(2)}(t,a)$, and $u^{(3)}(t,a)$ for  
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+  <! TA comment: I told a couple of students that since their successive approximations converged exactly in problem 1, that they could simply state in problem 2 that their approximations to the stable and unstable manifold were just in fact exact. if you wanted them to do #2 by actually solving the system of differential equations analytically and then figuring out the stable and unstable manifolds by inspection, then maybe you could email the class and make that clear. >  
<li>'''Perko, Section 2.7, problem 3'''  <li>'''Perko, Section 2.7, problem 3'''  
Show that $S$ and $U$ for the previous problem are given by  Show that $S$ and $U$ for the previous problem are given by  
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<! Lots of people didn't see the part about using this result to compute the stable manifold for the problem above >  <! Lots of people didn't see the part about using this result to compute the stable manifold for the problem above >  
+  <! Most people didn't have any idea on how to solve for problem 3, or why finding the normal vector to the tangent of the stable manifold, or to the vector field, is important for this problem. Perhaps for future years the hint for R^2, about the normal vector being orthogonal to the vector field could be explained as meaning that anytime a trajectory starts off on the stable manifold, it stays on the stable manifold since there is no verticle component to "lift" the trajectory off of the stable manifold. >  
<li> Consider a dynamical system with $x = (u, v) \in {\Bbb R}^n$. For the case $n = 2$, prove that if  <li> Consider a dynamical system with $x = (u, v) \in {\Bbb R}^n$. For the case $n = 2$, prove that if  
<center><amsmath>  <center><amsmath>  
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<li> '''Perko, Section 2.7, Problem 6'''  <li> '''Perko, Section 2.7, Problem 6'''  
Let $E$ be an open subset of $\mathbb{R}^n$ containing the origin. Use the fact that if $F\in C^1(E)$ then for all $x, y\in N_\delta(0)\subset E$ there exists a $\xi\in N_\delta(0)$ such that  Let $E$ be an open subset of $\mathbb{R}^n$ containing the origin. Use the fact that if $F\in C^1(E)$ then for all $x, y\in N_\delta(0)\subset E$ there exists a $\xi\in N_\delta(0)$ such that  
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</amsmath></center>  </amsmath></center>  
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<li>'''Perko, Section 2.9, problem 2(a)(b)'''  <li>'''Perko, Section 2.9, problem 2(a)(b)'''  
Determine the stability of the equilibrium points of the system (1) with $f(x)$ given by  Determine the stability of the equilibrium points of the system (1) with $f(x)$ given by  
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</amsmath></center>  </amsmath></center>  
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<! New for 2014 >  <! New for 2014 >  
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<font color=blue>And any two of the following:</font>  <font color=blue>And any two of the following:</font>  
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Note that these formulae actually determine the global stable and unstable manifolds $W^s(0)$ and $W^u(0)$ respectively.  Note that these formulae actually determine the global stable and unstable manifolds $W^s(0)$ and $W^u(0)$ respectively.  
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<li>  <li> 
Revision as of 23:56, 19 January 2015
R. Murray  Issued: 19 Jan 2015 
CDS 140, Winter 2015  Due: 28 Jan 2015 at 12:30 pm In class or to box across 107 STL 
__MATHJAX__
Note: In the upper left hand corner of the second page of your homework set, please put the number of hours that you spent on this homework set (including reading).
 Perko, Section 2.7, problem 1
Write the system
<amsmath> \aligned \dot{x}_1&=x_1+6x_2+x_1x_2,\\ \dot{x}_2&=4x_1+3x_2x_1^2 \endaligned
</amsmath>in the form
<amsmath> \dot{y}=By+G(y)
</amsmath>where
<amsmath> B=\begin{bmatrix}\lambda_1&0\\0&\lambda_2\end{bmatrix}
</amsmath>with $\lambda_1<0$, $\lambda_2>0$ and $G(y)$ is quadratic in $y_1$ and $y_2$.
 Perko, Section 2.7, problem 2
Find the first three successive approximations $u^{(1)}(t,a)$, $u^{(2)}(t,a)$, and $u^{(3)}(t,a)$ for
<amsmath> \aligned \dot{x}_1&=x_1,\\ \dot{x}_2&=x_2+x_1^2 \endaligned
</amsmath>and use $u^{(3)}(t,a)$ to approximate $S$ near the origin. Also approximate the unstable manifold $U$ near the origin for this system. Note that $u^{(2)}(t,a)=u^{(3)}(t,a)$ and therefore $u^{(j+1)}(t,a)=u^{(j)}(t,a)$ for $j\geq 2$. Thus $u(t,a)=u^{(2)}(t,a)$ which gives the exact function defining $S$.
 Perko, Section 2.7, problem 3
Show that $S$ and $U$ for the previous problem are given by
<amsmath> S:\,x_2=\frac{x_1^2}{3}
</amsmath><amsmath> U:\,x_1=0
</amsmath>Sketch $S$, $U$, $E^s$ and $E^u$.
 Consider a dynamical system with $x = (u, v) \in {\Bbb R}^n$. For the case $n = 2$, prove that if
<amsmath> \aligned \dot{u}&=f(u,v),\qquad u\in\mathbb{R}^k\\ \dot{v}&=g(u,v),\qquad v\in\mathbb{R}^{nk} \endaligned
</amsmath>then the manifold $S=\{(u,v)\in\mathbb R^k\times\mathbb R^{nk}v=h(u)\}$ is an invariant manifold of the system if
<amsmath> g(u,h(u))=Dh(u)f(u,h(u))
</amsmath>Use this result to compute the stable manifold for the system of problem 1 and 2 above using the Taylor series for $h(x)$ to define $S=\{(x_1,x_2)x_2=h(x)\}$ and matching coefficients to solve for $h(x)$.
 Note: The result holds for ${\Bbb R^n}$, but you only need to consider the case $n = 2$ and $k = 1$ (although you are free to prove the more general case if you prefer).
 Hint: One way to show $S$ is an invariant manifold in $\mathbb R^2$ is to show that the normal vector (orthogonal to the tangent to $S$ at $(x,h(x))$) is orthogonal to the vector field $(f,g)$ at that point. (It is sufficient to prove the result for $\mathbb R^2$.)
 Perko, Section 2.7, Problem 6
Let $E$ be an open subset of $\mathbb{R}^n$ containing the origin. Use the fact that if $F\in C^1(E)$ then for all $x, y\in N_\delta(0)\subset E$ there exists a $\xi\in N_\delta(0)$ such that
<amsmath> F(x)F(y)\leq\DF(\xi)\\,xy
</amsmath>(cf. Theorem 4.19 and the proof of Theorem 9.19 in [R]) to prove that if $F\in C^1(E)$ and $F(0)=DF(0)=0$ then given any $\epsilon>0$ there exists a $\delta>0$ such that for all $x, y\in N_\delta(0)$ we have
<amsmath> F(x)F(y)<\epsilon xy
</amsmath>  Perko, Section 2.9, problem 2(a)(b)
Determine the stability of the equilibrium points of the system (1) with $f(x)$ given by
<amsmath> (a)\quad\begin{bmatrix}x_1^2x_2^21\\2x_2\end{bmatrix}
</amsmath><amsmath> (b)\quad\begin{bmatrix}x_2x_1^2+2\\2x_2^22x_1x_2\end{bmatrix}
</amsmath>  Perko, Section 2.6, problem 3
Show that the continuous map $H:{\Bbb R}^3 \to {\Bbb R}^3$ defined by
<amsmath> \begin{bmatrix} y_1 \\ y_2 \\ y_3 \end{bmatrix} = H(x) = \begin{bmatrix} x_1 \\ x_2 + x_1^2 \\ x_3 + x_1^2 / 3 \end{bmatrix}
</amsmath>has a continuous inverse $H^{1}:{\Bbb R}^3 \to {\Bbb R}^3$ and that the nonlinear system
<amsmath> \frac{dx}{dt} = \begin{bmatrix} x_1 \\ x_2 + x_1^2 \\ x_3 + x_1^2 \end{bmatrix}
</amsmath>is transformed into a linear system using this transformation, i.e., if $y = H(x)$, show that $\dot y = A x$ for an appropriate $A$. Use this transformation to compute and sketch the stable and unstable manifolds for the nonlinear system.
 Note: since the nonlinear system can be transformed into a linear one, it follows that $S = H^{1}(E^s)$ and $U = H^{1}(E^u)$.
And any two of the following:

Perko, Section 2.7, problem 4
Find the first four successive approximations $u^{(1)}(t,a)$, $u^{(2)}(t,a)$, $u^{(3)}(t,a)$, and $u^{(4)}(t,a)$ for the system
<amsmath> \aligned \dot{x}_1&=x_1\\ \dot{x}_2&=x_2+x_1^2\\ \dot{x}_3&=x_3+x_2^2 \endaligned
</amsmath>Show that $u^{(3)}(t,a)=u^{(4)}(t,a)=\cdots$ and hence $u(t,a)=u^{(3)}(t,a)$. Find $S$ and $U$ for this problem.
 Perko, Section 2.7, problem 5
Solve the system and show that
<amsmath> S:\,\,x_3=\frac{1}{3}x_2^2\frac{1}{6}x_1^2x_2\frac{1}{30}x_1^4
</amsmath>and
<amsmath> U:\,\,x_1=x_2=0
</amsmath>Note that these formulae actually determine the global stable and unstable manifolds $W^s(0)$ and $W^u(0)$ respectively.

Perko, Section 2.8, Problem 1
Solve the system
<amsmath> \aligned \dot{y}_1&=y_1\\ \dot{y}_2&=y_2+z^2\\ \dot{z}&=z \endaligned
</amsmath>and show that the successive approximations $\Phi^(k)\rightarrow\Phi$ and $\Psi^(k)\rightarrow\Psi$ as $k\rightarrow\infty$ for all $x=(y_1,y_2,z)\in{\mathbb R}^3$. Define $H_0=(\Phi,\Psi)^T$ and use this homeomorphism to find
<amsmath> H (x) =\int_0^1 e^{As} H_0 \bigl(\phi_s(x) \bigr) ds,
</amsmath>where $A$ is the linearization of the nonlinear dynamics at the origin and $\phi_t(x)$ is the flow of the full system. Use the homemorphism $H$ to find the stable and unstable manifolds
<amsmath> W^s(0)=H^{1}(E^s)\quad {\mathrm{and}}\quad W^u(0)=H^{1}(E^u)
</amsmath>for this system.
 Note: this problem involves some simple but somewhat tedious computations. If you know how to use Mathematica or a similar program, you may wish to carry out the computations for the successive approximations using that software. However, make sure to show the results at each step of the calculation.
 Hint: You should find
<amsmath> H(y_1,y_2,z) = \begin{bmatrix} y_1 \\ y_2z^2/3 \\ z \end{bmatrix}, \qquad \aligned W^s(0) &=\{x\in{\mathbb{R}}z=0\}, \\ W^u(0) &=\{x\in{\mathbb{R}}y_1=0,y_2=z^2/3\}. \endaligned
</amsmath>
Notes:
 The problems are transcribed above in case you don't have access to Perko. However, in the case of discrepancy, you should use Perko as the definitive source of the problem statement.