In mathematics, a weak derivative is a generalization of the concept of the derivative of a function (strong derivative) for functions not assumed differentiable, but only integrable, i.e., to lie in the Lp space L 1 ( [ a , b ] ) {\displaystyle L^{1}([a,b])} . The method of integration by parts holds that for smooth functions u {\displaystyle u} and φ {\displaystyle \varphi } we have
∫ a b u ( x ) φ ′ ( x ) d x = [ u ( x ) φ ( x ) ] a b − ∫ a b u ′ ( x ) φ ( x ) d x . {\displaystyle {\begin{aligned}\int _{a}^{b}u(x)\varphi '(x)\,dx&={\Big [}u(x)\varphi (x){\Big ]}_{a}^{b}-\int _{a}^{b}u'(x)\varphi (x)\,dx.\\[6pt]\end{aligned}}}
A function u' being the weak derivative of u is essentially defined by the requirement that this equation must hold for all smooth functions φ {\displaystyle \varphi } vanishing at the boundary points ( φ ( a ) = φ ( b ) = 0 {\displaystyle \varphi (a)=\varphi (b)=0} ).
Definition Let u {\displaystyle u} be a function in the Lebesgue space L 1 ( [ a , b ] ) {\displaystyle L^{1}([a,b])} . We say that v {\displaystyle v} in L 1 ( [ a , b ] ) {\displaystyle L^{1}([a,b])} is a weak derivative of u {\displaystyle u} if
∫ a b u ( t ) φ ′ ( t ) d t = − ∫ a b v ( t ) φ ( t ) d t {\displaystyle \int _{a}^{b}u(t)\varphi '(t)\,dt=-\int _{a}^{b}v(t)\varphi (t)\,dt}
for all infinitely differentiable functions φ {\displaystyle \varphi } with φ ( a ) = φ ( b ) = 0 {\displaystyle \varphi (a)=\varphi (b)=0} . Generalizing to n {\displaystyle n} dimensions, if u {\displaystyle u} and v {\displaystyle v} are in the space L loc 1 ( U ) {\displaystyle L_{\text{loc}}^{1}(U)} of locally integrable functions for some open set U ⊂ R n {\displaystyle U\subset \mathbb {R} ^{n}} , and if α {\displaystyle \alpha } is a multi-index, we say that v {\displaystyle v} is the α th {\displaystyle \alpha ^{\text{th}}} -weak derivative of u {\displaystyle u} if
∫ U u D α φ = ( − 1 ) | α | ∫ U v φ , {\displaystyle \int _{U}uD^{\alpha }\varphi =(-1)^{|\alpha |}\int _{U}v\varphi ,}
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