ScalingStacks

Proof. [03LL]

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Proof. Let u,v:ℝ2→ℝu,v:\mathbin{\mathbb{R}}^{2}\rightarrow\mathbin{\mathbb{R}} be solutions of (33), and define ff by

f⁡(x,y)=∫0xu⁡(s,0)​𝑑s+∫0yv⁡(x,t)​𝑑t.f(x,y)=\int_{0}^{x}u(s,0){\rm d}s+\int_{0}^{y}v(x,t){\rm d}t.

Then ∂f∂y​(x,y)=v​(x,y)\frac{\partial f}{\partial y}(x,y)=v(x,y) and f⁡(0,0)=0f(0,0)=0 are immediate, and

∂f∂x​(x,y)\displaystyle\frac{\partial f}{\partial x}(x,y) =u⁡(x,0)+∫0y∂v∂x​(x,t)​𝑑t\displaystyle=u(x,0)+\int_{0}^{y}\frac{\partial v}{\partial x}(x,t){\rm d}t
=u⁡(x,0)+∫0y∂u∂y​(x,t)​𝑑t\displaystyle=u(x,0)+\int_{0}^{y}\frac{\partial u}{\partial y}(x,t){\rm d}t
=u⁡(x,0)+[u⁡(x,t)]0y=u⁡(x,y),\displaystyle=u(x,0)+\bigl[u(x,t)\bigr]^{y}_{0}=u(x,y),

as ∂u∂y=∂v∂x\frac{\partial u}{\partial y}=\frac{\partial v}{\partial x}. This proves the first line of (39), and the second follows by substituting ∂f∂x=u\frac{\partial f}{\partial x}=u and ∂f∂y=v\frac{\partial f}{\partial y}=v into the first equation of (33). The converse is easy. □\square

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