3.4: Sistemas de Segundo Orden
- Page ID
- 117951
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)Aquí consideramos el sistema
\ begin {ecuación}
\ label {systwo}
\ suma_ {k, l=1} ^na^ {kl} (x, u,\ nabla u) u_ {x_kx_l} +\ mbox {términos de orden inferior} =0,
\ end {ecuación}
donde\(A^{kl}\) están\((m\times m)\) las matrices y\(u=(u_1,\ldots,u_m)^T\). Asumimos\(A^{kl}=A^{lk}\), que no es restricción de generalidad siempre que se satisfagan $u\ en C^2$.
Al igual que en los apartados anteriores, la clasificación se desprende de la pregunta de si podemos o no calcular formalmente la solución a partir de las ecuaciones diferenciales, si se dan bastantes datos sobre un colector inicial. Que el colector inicial\(\mathcal{S}\) sea dado por\(\chi(x)=0\) y asuma eso\(\nabla\chi\not=0\). El mapeo\(x=x(\lambda)\), ver secciones anteriores, lleva a
$$
\ sum_ {k, l=1} ^na^ {kl}\ chi_ {x_k}\ chi_ {x_l} v_ {\ lambda_n\ lambda_n} =\ mbox {términos conocidos en}\\ mathcal {S},
$$
donde\(v(\lambda)=u(x(\lambda))\).
La ecuación característica está aquí
$$
\ det\ left (\ suma_ {k, l=1} ^Na^ {kl}\ chi_ {x_k}\ chi_ {x_l}\ right) =0.
$$
Si hay una solución\(\chi\) con\(\nabla\chi\not=0\), entonces es posible que los segundos derivados no sean continuos en un barrio de\(\mathcal{S}\).
Definición. El sistema se llama elíptico si
$$
\ det\ left (\ sum_ {k, l=1} ^na^ {kl}\ zeta_k\ zeta_l\ right)\ not=0
$$
para todos\(\zeta\in\mathbb{R}\),\(\zeta\not=0\).