Let $\Omega\subseteq\mathbb R^n$ be open. $u\in\mathcal L^1_\text{loc}(\Omega)$ is called weakly differentiable $:\Leftrightarrow$ $\exists v\in\mathcal L^1_\text{loc}(\Omega;\mathbb R^n)$ with $$\int_\Omega\psi v\;d\lambda^n=-\int_\Omega u\nabla\psi\;\;\;\text{for all }\psi\in C_c^1(\Omega)\;.$$ Now, let $u\in W_0^{1,2}(\Omega)=:H$. I want to show, that $u$ is weakly differentiable. By definition, $H$ is the completion of $C_c^1(\Omega)$ with respect to the norm $$\left\|\psi\right\|_H^2:=\int_\Omega|\nabla\psi|^2+\psi^2\;d\lambda^n\;\;\;\text{for }\psi\in C_c^1(\Omega)\;.$$ So, there is a sequence $\left(\psi_k\right)_{k\in\mathbb N}\subseteq C_c^1(\Omega)$ with $$\psi_k\stackrel H{\to}u\;.\tag{1}$$ Let $\psi\in C_c^1(\Omega)$. Then, $$\left\|\left(u-\psi_k\right)\frac{\partial\psi}{\partial x_i}\right\|_{L^2(\Omega)}\le\left\|u-\psi_k\right\|_{L^2(\Omega)}\left\|\frac{\partial\psi}{\partial x_i}\right\|_{L^2(\Omega)}\stackrel{k\to\infty}{\to}0\;.$$ Hence, $$-\int_\Omega u\frac{\partial\psi}{\partial x_i}\;d\lambda^n=-\lim_{k\to\infty}\int_\Omega\psi_k\frac{\partial\psi}{\partial x_i}\;d\lambda^n\;\;\;\text{in }L^2(\Omega)\;.\tag{2}$$ How do I need to proceed from here? Clearly, by $(1)$ we know that $\nabla\psi_k$ converges in $L^2(\Omega;\mathbb R^n)$ agains some $v$.
2026-03-27 20:19:44.1774642784
Prove that each $W_0^{1,2}$-function is weakly differentiable
308 Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail At
1
There are 1 best solutions below
Related Questions in ORDINARY-DIFFERENTIAL-EQUATIONS
- The Runge-Kutta method for a system of equations
- Analytical solution of a nonlinear ordinary differential equation
- Stability of system of ordinary nonlinear differential equations
- Maximal interval of existence of the IVP
- Power series solution of $y''+e^xy' - y=0$
- Change of variables in a differential equation
- Dimension of solution space of homogeneous differential equation, proof
- Solve the initial value problem $x^2y'+y(x-y)=0$
- Stability of system of parameters $\kappa, \lambda$ when there is a zero eigenvalue
- Derive an equation with Faraday's law
Related Questions in PARTIAL-DIFFERENTIAL-EQUATIONS
- PDE Separation of Variables Generality
- Partial Derivative vs Total Derivative: Function depending Implicitly and Explicitly on Variable
- Transition from theory of PDEs to applied analysis and industrial problems and models with PDEs
- Harmonic Functions are Analytic Evan’s Proof
- If $A$ generates the $C_0$-semigroup $\{T_t;t\ge0\}$, then $Au=f \Rightarrow u=-\int_0^\infty T_t f dt$?
- Regular surfaces with boundary and $C^1$ domains
- How might we express a second order PDE as a system of first order PDE's?
- Inhomogeneous biharmonic equation on $\mathbb{R}^d$
- PDE: Determine the region above the $x$-axis for which there is a classical solution.
- Division in differential equations when the dividing function is equal to $0$
Related Questions in CONVERGENCE-DIVERGENCE
- Finding radius of convergence $\sum _{n=0}^{}(2+(-1)^n)^nz^n$
- Conditions for the convergence of :$\cos\left( \sum_{n\geq0}{a_n}x^n\right)$
- Proving whether function-series $f_n(x) = \frac{(-1)^nx}n$
- Pointwise and uniform convergence of function series $f_n = x^n$
- studying the convergence of a series:
- Convergence in measure preserves measurability
- If $a_{1}>2$and $a_{n+1}=a_{n}^{2}-2$ then Find $\sum_{n=1}^{\infty}$ $\frac{1}{a_{1}a_{2}......a_{n}}$
- Convergence radius of power series can be derived from root and ratio test.
- Does this sequence converge? And if so to what?
- Seeking an example of Schwartz function $f$ such that $ \int_{\bf R}\left|\frac{f(x-y)}{y}\right|\ dy=\infty$
Related Questions in SOBOLEV-SPACES
- On sufficient condition for pre-compactness "in measure"(i.e. in Young measure space)
- $\mbox{Cap}_p$-measurability
- If $u\in W^{1,p}(\Omega )$ is s.t. $\nabla u=0$ then $u$ is constant a.e.
- Weak formulation of Robin boundary condition problem
- Variational Formulation - inhomogeneous Neumann boundary
- Why the Sobolev space $W^{1,2}(M,N)$ weak-sequencially closed in $W^{1,2}(\mathbb R^K)$?
- Sobolev space $H^s(Q)$ is Hilbert
- Duhamel's principle for heat equation.
- How to define discrete Sobolev dual norm so that it can be computed?
- Weakly sequentially continuous maps
Related Questions in WEAK-DERIVATIVES
- Existence and uniqueness of weak solutions to the homogeneous biharmonic equation.
- Is the square of an $H^1$ function also $H^1$?
- Regularity of the Divergence of Weak Solutions to Elliptic PDEs
- Recovering classical solution from weak one for the Laplace equation
- Exercise on first and second order derivative in sense of distributions.
- Radon-Nikodym derivative of discrete measure
- $\mathbb{1}_{B_1(0)}$ doesn't have a $\partial_{x_i}$weak derivative in $\mathbb{R}^n$
- Ito's formula for merely continuous functions
- Sobolev spaces on different domains
- Why the generalized derivatives defined? Why was it needed?
Trending Questions
- Induction on the number of equations
- How to convince a math teacher of this simple and obvious fact?
- Find $E[XY|Y+Z=1 ]$
- Refuting the Anti-Cantor Cranks
- What are imaginary numbers?
- Determine the adjoint of $\tilde Q(x)$ for $\tilde Q(x)u:=(Qu)(x)$ where $Q:U→L^2(Ω,ℝ^d$ is a Hilbert-Schmidt operator and $U$ is a Hilbert space
- Why does this innovative method of subtraction from a third grader always work?
- How do we know that the number $1$ is not equal to the number $-1$?
- What are the Implications of having VΩ as a model for a theory?
- Defining a Galois Field based on primitive element versus polynomial?
- Can't find the relationship between two columns of numbers. Please Help
- Is computer science a branch of mathematics?
- Is there a bijection of $\mathbb{R}^n$ with itself such that the forward map is connected but the inverse is not?
- Identification of a quadrilateral as a trapezoid, rectangle, or square
- Generator of inertia group in function field extension
Popular # Hahtags
second-order-logic
numerical-methods
puzzle
logic
probability
number-theory
winding-number
real-analysis
integration
calculus
complex-analysis
sequences-and-series
proof-writing
set-theory
functions
homotopy-theory
elementary-number-theory
ordinary-differential-equations
circles
derivatives
game-theory
definite-integrals
elementary-set-theory
limits
multivariable-calculus
geometry
algebraic-number-theory
proof-verification
partial-derivative
algebra-precalculus
Popular Questions
- What is the integral of 1/x?
- How many squares actually ARE in this picture? Is this a trick question with no right answer?
- Is a matrix multiplied with its transpose something special?
- What is the difference between independent and mutually exclusive events?
- Visually stunning math concepts which are easy to explain
- taylor series of $\ln(1+x)$?
- How to tell if a set of vectors spans a space?
- Calculus question taking derivative to find horizontal tangent line
- How to determine if a function is one-to-one?
- Determine if vectors are linearly independent
- What does it mean to have a determinant equal to zero?
- Is this Batman equation for real?
- How to find perpendicular vector to another vector?
- How to find mean and median from histogram
- How many sides does a circle have?
Please do not use the same symbol for your function and test functions. You are confusing yourself.
We assume $u\in H$ and $(u_n)\subset C_c^1$ such that $u_n\to u$ in $H$, which in particular means that $u_n\to u$ in $L^2$ and $\partial_i u_n\to v_i$ in $L^2$ for each $i=1,\ldots, N$. Then we observe that, for any $\varphi\in C_c^1$, $$ \int_\Omega u\,\partial_i \varphi\,dx=\lim_{n\to\infty}\int_\Omega u_n\,\partial_i \varphi\,dx = \lim_{n\to \infty}-\int_\Omega\partial_i u_n\,\varphi\,dx = -\int_\Omega v_i\,\varphi\,dx. $$ Both first and last equality are justified by $L^2$ convergence. Finally by definition of weak derivative, you know $v_i$ is $i$-partial weak derivative of $u$.