We prove that in a bounded Lipschitz domain of R3\documentclass[12pt]{minimal}
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\begin{document}$${\mathbb {R}}^3$$\end{document} the steady-state Navier–Stokes equations with boundary data in L2(∂Ω)\documentclass[12pt]{minimal}
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\begin{document}$$L^2(\partial \Omega )$$\end{document} have a very weak solution u∈L3(Ω)\documentclass[12pt]{minimal}
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\begin{document}$$\varvec{u}\in L^3(\Omega )$$\end{document}, unique for large viscosity.