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202                                            Solutions to the Exercises

                                                                        ν
                          (i) We have seen (Exercise 1.4.6) that the sequence u   0 in W 1,2  (we have
                       shown this only up to a subsequence, but it is not difficult to see that the whole
                       sequence has this property). An elementary computation gives

                                                    ν
                                              det ∇u = −ν (1 − y) 2ν−1  .
                                            ν
                                                     1
                       Let us show that det ∇u   0 in L does not hold. Indeed, let ϕ ≡ 1 ∈ L ∞  (Ω).
                       It is not difficult to see that
                                               ZZ
                                                         ν
                                            lim    det ∇u (x, y) dxdy 6=0,
                                           ν→∞
                                                  Ω
                       and thus the result.
                                                                                         ν
                          (ii) Note first that by Rellich theorem (Theorem 1.43) we have that if u
                                                   q
                       u in W  1,p  then u ν  → u in L , ∀q ∈ [1, 2p/ (2 − p)) provided p< 2 and
                       ∀q ∈ [1, ∞) if p =2 (the case p> 2 has already been considered in Lemma
                                                              ν
                                                                                         ν
                                                                        4
                       3.23). Consequently if p> 4/3,we have u → u in L . Let therefore u =
                                            ν
                                                                                         ν
                                                                                 ν
                                                                                       ν
                                    ν
                        ν
                       u (x, y)=(ϕ (x, y) ,ψ (x, y)) and v ∈ C ∞  (Ω).Since det ∇u = ϕ ψ −
                                                                                         y
                                                                                       x
                                                              0
                               ¡
                                              ν
                                            ν
                                                                             2
                                  ν
                        ν
                       ϕ ψ ν  = ϕ ψ ν  ¢  − (ϕ ψ ) (this is allowed since u ν  ∈ C )wehave, after
                        y  x        y x       x y
                       integrating by parts,
                                  ZZ                  ZZ
                                                          ¡  ν  ν    ν  ν  ¢
                                            ν
                                      det ∇u vdxdy =      ϕ ψ v y − ϕ ψ v x dxdy .
                                                                       y
                                                              x
                                     Ω                  Ω
                                             ν
                                                                   ν
                       However we know that ψ  ψ in W   1,4/3  (since u  u in W 1,p  and p> 4/3)
                                                              ¡   ν     ν  ¢  ¡       ¢
                                                                      ν
                                                                ν
                            ν
                                      4
                       and ϕ → ϕ in L , we therefore deduce that ϕ ψ ,ϕ ψ    ϕψ ,ϕψ     in L 1
                                                                  x     y        x   y
                       (Exercise 1.3.3). Passing to the limit and integrating by parts once more we get
                       the claim, namely
                            ZZ                  ZZ                        ZZ
                                      ν
                         lim    det ∇u vdxdy =      (ϕψ v y − ϕψ v y ) dxdy =  det ∇uv dxdy .
                                                               x
                                                       x
                        ν→∞
                               Ω                  Ω                          Ω
                       Exercise 3.5.6. (i) Let x =(x 1 ,x 2 ),wethen find
                                           ⎛     2           ⎞
                                                x 2     x 1 x 2
                                                 3    −   3
                                           ⎜   |x|      |x|  ⎟        2    1
                                     ∇u =  ⎜             2   ⎟  ⇒ |∇u| =      .
                                           ⎝   x 1 x 2  x 1  ⎠            |x| 2
                                             −
                                                  3       3
                                                |x|    |x|
                       Wethereforededuce(cf. Exercise1.4.1)that u ∈ L ∞  and u ∈ W 1,p  provided
                                                              0
                       p ∈ [1, 2),but, however, u/∈ W 1,2  and u/∈ C .
                          (ii) Since
                             ZZ                       Z                   Z
                                                        1    r         2π   ν+1  s − 1
                                              q
                                  ν
                                 |u (x) − u (x)| dx =2π          q dr =  2        q  ds
                               Ω                        0  (νr +1)     ν   1     s
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