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- {\partial \sigma _{xx}}{\partial x}}+{\frac {\partial \sigma _{xy}}{\partial y}}=0,\qquad {\frac {\partial \sigma _{yx}}{\partial x}}+{\frac {\partial \sigma…8 kB (1300 palabras) - 13:09 3 sep 2019
- ϵ 0 ∂ E ∂ t {\displaystyle {\frac {\partial B}{\partial x}}=-\mu _{0}\epsilon _{0}{\dfrac {\partial E}{\partial t}}} Serway, R. A. (2009). Cervantes…3 kB (462 palabras) - 06:41 17 nov 2020
- {\partial f}{\partial x}},{\frac {\partial }{\partial x}}f,D_{1}f,\partial _{x}f,f_{x}^{\prime }{\text{ o }}f_{x}.} Donde ∂ {\displaystyle \partial }…20 kB (3554 palabras) - 18:58 17 nov 2023
{\begin{bmatrix}{\partial f_{1} \over \partial u}&{\partial f_{1} \over \partial v}\\{\partial f_{2} \over \partial u}&{\partial f_{2} \over \partial v}\\{\partial f_{3}…22 kB (3301 palabras) - 03:26 24 may 2024
{\partial (\rho F_{\rho })}{\partial \rho }}+{\frac {1}{\rho }}{\frac {\partial F_{\varphi }}{\partial \varphi }}+{\frac {\partial F_{z}}{\partial z}}}…7 kB (1351 palabras) - 11:44 21 oct 2023
{\partial m_{x}}{\partial x}}+{\cfrac {\partial m_{xy}}{\partial y}}=v_{x}\\{\cfrac {\partial m_{xy}}{\partial x}}+{\cfrac {\partial m_{y}}{\partial…21 kB (3224 palabras) - 08:32 27 may 2024- Onda elástica (sección Ondas planas){\displaystyle {\frac {\partial \sigma _{ij}}{\partial x_{j}}}=\rho \left({\frac {\partial v_{i}}{\partial t}}+v_{j}{\frac {\partial v_{i}}{\partial x_{j}}}\right)}…10 kB (1859 palabras) - 22:28 27 ene 2024
{\displaystyle {\frac {\partial F}{\partial x}}dx=-\rho Adx{\frac {{\partial }^{2}\Psi }{{\partial t}^{2}}}\rightarrow {\frac {\partial F}{\partial x}}=-\rho A{\frac…35 kB (5027 palabras) - 10:49 25 jul 2023- r}{\partial \over \partial r}\left(r{\partial f \over \partial r}\right)+{1 \over r^{2}}{\partial ^{2}f \over \partial \theta ^{2}}={1 \over r}{\partial f…11 kB (1976 palabras) - 18:18 14 may 2024
{\partial ^{2}x^{k}}{\partial \tau ^{2}}}+m\sum _{i,j=0}^{3}\Gamma _{ij}^{k}{\frac {\partial x^{i}}{\partial \tau }}{\frac {\partial x^{j}}{\partial \tau…10 kB (1657 palabras) - 17:07 28 may 2024
{\displaystyle {\frac {\partial ^{4}w}{\partial ^{4}x}}+2{\frac {\partial ^{4}w}{\partial ^{2}x\partial ^{2}y}}+{\frac {\partial ^{4}w}{\partial ^{4}y}}={\frac…3 kB (496 palabras) - 00:51 27 sep 2022
{\partial x}{\partial X}}&{\cfrac {\partial x}{\partial Y}}&{\cfrac {\partial x}{\partial Z}}\\{\cfrac {\partial y}{\partial X}}&{\cfrac {\partial y}{\partial…29 kB (4966 palabras) - 18:18 26 may 2024- {\partial \phi }{\partial y}},\tau _{zy}=-{\frac {\partial \phi }{\partial x}},\qquad {\frac {\partial ^{2}\phi }{\partial x^{2}}}+{\frac {\partial ^{2}\phi…7 kB (1241 palabras) - 19:30 13 dic 2022
_{xx}={\frac {\partial u_{x}}{\partial x}}=-z{\frac {\partial ^{2}w}{\partial x^{2}}}\qquad \varepsilon _{yy}={\frac {\partial u_{y}}{\partial y}}=-z{\frac…17 kB (3175 palabras) - 18:54 14 nov 2023
{\displaystyle {\frac {\partial \mathbf {r} (u_{0},v_{0})}{\partial u}}\times {\frac {\partial \mathbf {r} (u_{0},v_{0})}{\partial v}}\neq \mathbf {0} }…19 kB (3760 palabras) - 16:20 13 nov 2023
\\\\{\begin{bmatrix}\partial _{x_{1}}f_{1}(\mathbf {a} )&\dots &\partial _{x_{n}}f_{1}(\mathbf {a} )\\\dots &\dots &\dots \\\partial _{x_{1}}f_{n}(\mathbf…3 kB (402 palabras) - 09:09 30 ene 2023- \partial S=\{0,2\}\,} . Si S = Z {\displaystyle S=\mathbb {Z} } , ∂ S = Z {\displaystyle \partial S=\mathbb {Z} } . ∂ Q = R {\displaystyle \partial \mathbb…4 kB (650 palabras) - 02:16 27 jul 2022
{\partial u}{\partial y}}+{\frac {\partial v}{\partial x}}={\frac {\partial (-z\theta _{x})}{\partial y}}+{\frac {\partial (-z\theta _{y})}{\partial x}}=-2z{\frac…16 kB (3012 palabras) - 20:07 11 ene 2021
(}{\frac {\partial g_{j}}{\partial x_{j}}}{\frac {\partial }{\partial x_{j}}}+g_{j}\nabla _{\frac {\partial }{\partial x_{i}}}{\frac {\partial }{\partial x_{j}}}{\bigg…14 kB (2506 palabras) - 14:16 18 abr 2024
{\begin{aligned}\rho {\frac {\partial ^{2}u_{i}}{\partial t^{2}}}&=\partial _{i}\lambda \partial _{k}u_{k}+\partial _{j}\mu \left(\partial _{i}u_{j}+\partial _{j}u_{i}\right)\\&=\lambda…8 kB (1220 palabras) - 03:55 20 abr 2021
- {\partial E_{z}}{\partial y}}-{\frac {\partial E_{y}}{\partial z}}){\hat {i}}+({\frac {\partial E_{x}}{\partial z}}-{\frac {\partial E_{z}}{\partial x}})){\hat
- {f}{2B_{eq}}}\right)}\partial f}\\&\int _{-\infty }^{\infty }{\left|H(f)\right|^{2}\partial f}=\int _{-B_{eq}}^{B_{eq}}{\left|H(f)\right|_{\max }^{2}\partial f}\\&\int
- {\tfrac {\partial p}{\partial t}}+{\tfrac {\partial \rho v_{2}}{\partial x_{1}}}+{\tfrac {\partial \rho v_{2}}{\partial x_{2}}}+{\tfrac {\partial \rho v_{3}}{\partial