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| author | Juan Marin Noguera <juan@mnpi.eu> | 2022-12-04 22:49:17 +0100 |
|---|---|---|
| committer | Juan Marin Noguera <juan@mnpi.eu> | 2022-12-04 22:49:17 +0100 |
| commit | c34b47089a133e58032fe4ea52f61efacaf5f548 (patch) | |
| tree | 4242772e26a9e7b6f7e02b1d1e00dfbe68981345 /fvv1/n3.lyx | |
| parent | 214b20d1614b09cd5c18e111df0f0d392af2e721 (diff) | |
Oops
Diffstat (limited to 'fvv1/n3.lyx')
| -rw-r--r-- | fvv1/n3.lyx | 18 |
1 files changed, 9 insertions, 9 deletions
diff --git a/fvv1/n3.lyx b/fvv1/n3.lyx index 91f5019..b6138cf 100644 --- a/fvv1/n3.lyx +++ b/fvv1/n3.lyx @@ -343,12 +343,12 @@ Demostración: \end_inset , y consideramos -\begin_inset Formula $\Delta_{t,s}:=f(t,s)-f(t,y_{0})-f(x_{0},s)+f(x_{0},y_{0})$ +\begin_inset Formula $\Delta_{t,s}\coloneqq f(t,s)-f(t,y_{0})-f(x_{0},s)+f(x_{0},y_{0})$ \end_inset . Si ahora llamamos -\begin_inset Formula $F_{\overline{s}}(\overline{t}):=f(\overline{t},\overline{s})-f(\overline{t},y_{0})$ +\begin_inset Formula $F_{\overline{s}}(\overline{t})\coloneqq f(\overline{t},\overline{s})-f(\overline{t},y_{0})$ \end_inset , vemos que @@ -360,12 +360,12 @@ Demostración: \end_inset y que entonces -\begin_inset Formula $\Delta_{t,s}=F_{s}(t)-F_{s}(x_{0})=F'_{\overline{s}}(\xi_{t,s})(t-x_{0})=\left(\frac{\partial f}{\partial x}(\xi_{t,s},s)-\frac{\partial f}{\partial x}(\xi_{t,s},y_{0})\right)(t-x_{0})\overset{\Phi(\overline{s}):=\frac{\partial f}{\partial x}(\xi_{t,s},\overline{s})}{=}(\Phi(s)-\Phi(y_{0}))(t-x_{0})\overset{\Phi\text{ derivable por hipótesis}}{=}\Phi'(\eta_{t,s})(s-y_{0})(t-x_{0})=\frac{\partial^{2}f}{\partial x\partial y}(\xi_{t,s},\eta_{t,s})(s-y_{0})(t-x_{0})$ +\begin_inset Formula $\Delta_{t,s}=F_{s}(t)-F_{s}(x_{0})=F'_{\overline{s}}(\xi_{t,s})(t-x_{0})=\left(\frac{\partial f}{\partial x}(\xi_{t,s},s)-\frac{\partial f}{\partial x}(\xi_{t,s},y_{0})\right)(t-x_{0})\overset{\Phi(\overline{s})\coloneqq \frac{\partial f}{\partial x}(\xi_{t,s},\overline{s})}{=}(\Phi(s)-\Phi(y_{0}))(t-x_{0})\overset{\Phi\text{ derivable por hipótesis}}{=}\Phi'(\eta_{t,s})(s-y_{0})(t-x_{0})=\frac{\partial^{2}f}{\partial x\partial y}(\xi_{t,s},\eta_{t,s})(s-y_{0})(t-x_{0})$ \end_inset . Permutando los papeles de las dos coordenadas (definiendo -\begin_inset Formula $\sigma_{\overline{t}}(\overline{s}):=f(\overline{t},\overline{s})-f(x,\overline{s})$ +\begin_inset Formula $\sigma_{\overline{t}}(\overline{s})\coloneqq f(\overline{t},\overline{s})-f(x,\overline{s})$ \end_inset ) obtenemos que @@ -448,7 +448,7 @@ teorema Demostración: \series default Sea -\begin_inset Formula $R(h):=f(a+h)-f(a)-df(a)(h)-\frac{1}{2}d^{2}f(a)(h,h)$ +\begin_inset Formula $R(h)\coloneqq f(a+h)-f(a)-df(a)(h)-\frac{1}{2}d^{2}f(a)(h,h)$ \end_inset , y hemos de ver que @@ -631,7 +631,7 @@ Si \end_inset -espacio vectorial con -\begin_inset Formula $k:=\dim_{K}(V)<+\infty$ +\begin_inset Formula $k\coloneqq \dim_{K}(V)<+\infty$ \end_inset y @@ -751,7 +751,7 @@ Podemos suponer que alcanza un máximo. \end_inset definimos -\begin_inset Formula $\varphi_{i}(t):=f(a_{1},\dots,a_{i-1},t,a_{i+1},\dots,a_{m})$ +\begin_inset Formula $\varphi_{i}(t)\coloneqq f(a_{1},\dots,a_{i-1},t,a_{i+1},\dots,a_{m})$ \end_inset , fijado @@ -848,7 +848,7 @@ suponiendo \end_inset dada por -\begin_inset Formula $\Phi(u):=d^{2}f(a)(u,u)=\sum_{i,j}\frac{\partial f}{\partial x_{i}\partial x_{j}}(a)u_{i}u_{j}$ +\begin_inset Formula $\Phi(u)\coloneqq d^{2}f(a)(u,u)=\sum_{i,j}\frac{\partial f}{\partial x_{i}\partial x_{j}}(a)u_{i}u_{j}$ \end_inset es continua, luego @@ -914,7 +914,7 @@ Como \end_inset y definimos -\begin_inset Formula $\varphi(t):=a+tu$ +\begin_inset Formula $\varphi(t)\coloneqq a+tu$ \end_inset como la función |
