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    Two-grid P02–P1 mixed finite element methods combined with Crank–Nicolson scheme for a class of nonlinear parabolic equations
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    1.1 MotivationWhy do mathematicians use Sobolev spaces instead of the simpler looking spaces of continuously differentiable functions?The most famous Sobolev space is H1(Ω), the set of all functions u which are square integrable, together with all their first derivatives, in Ω, an open subset of ℝn, the usual n-dimensional Euclidian space. The derivatives are to be understood in the sense of distributions. It is not even true that any function in H1(Ω) is continuous. For instance, the functionu(x,y)=|ln12(x2+y2)|1/3is in H1(Ω1), where Ω1 is the unit circle in the plane:Ω1={(x,y)∈ℝ2,x2+y2<1}.However, u is not continuous at (0, 0) and not even bounded. Such spaces are obviously not easy to handle.
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