69.1. AN UNNATURAL EXAMPLE 2357

since Lp (D) is reflexive, an application of the Hahn Banach theorem shows there existsf ∈ Lp (D) such that

⟨g∗, f ⟩(Lp(D))′,Lp(D) ̸= 0, ⟨−∆φ , f ⟩(Lp(D))′,Lp(D) = 0 (69.1.2)

for all −∆φ ∈ H. However, it was just shown H could be considered a subset of (Lp (D))′

in the manner described above. Therefore, the last equation in the above is of the form

0 = (−∆φ , f )H = ⟨ f ,φ⟩=∫

Df φdx

and since this holds for all φ ∈ H10 (D) , it follows by density of H1

0 (D) in Lp′ (D) , thatf = 0 and now this contradicts the inequality in 69.1.2.

Now ∆ is defined on H10 (D) and it delivers something in

(H1

0)′ ≡H. Of course H1

0 (D)

is dense in Lp′ (D). Can ∆ be extended to all of Lp′ (D)? The answer is yes and it is moreof the same given above. For φ ∈ H1

0 (D) ,−∆φ ∈ H ⊆ (Lp (D))′ . Then by the above, forφ ∈ H1

0 (D) and f ∈ Lp (D) ,

⟨−∆φ , f ⟩ ≡ ⟨ f ,φ⟩ ≡∫

Df φdx

|⟨−∆φ , f ⟩| ≡ |⟨ f ,φ⟩| ≡∣∣∣∣∫D

f φds∣∣∣∣≤ ||φ ||Lp′ (D)

|| f ||Lp(D)

and so −∆ is a continuous linear mapping defined on a dense subspace H10 (D) of Lp′ (D)

and so this does indeed extend to a continuous linear map defined on all of Lp′ (D) givenby the formula

⟨−∆g, f ⟩ ≡∫

Df gdx

This proves the lemma.Thus letting V ≡ Lp (D) , and H ≡

(H1

0 (D))′, it follows V ⊆H ⊆V ′ is a Gelfand triple

with the understanding of what it means for one space to be included in another describedabove. To emphasize the above, for −∆φ ∈ H, f ∈ Lp,

⟨−∆φ , f ⟩ ≡ (−∆φ , f )H ≡ ⟨ f ,φ⟩ ≡∫

Df φdx

More generally, for g ∈ Lp′ (D) ,−∆g ∈ (Lp (D))′ according to the rule

⟨−∆g, f ⟩ ≡∫

Df gdx.

With this example of a Gelfand triple, one can define a “porous medium operator”A : V →V ′. Let Ψ be a real valued function defined on R which satisfies

Ψ is continuous (69.1.3)

(t− s)(Ψ(t)−Ψ(s))≥ 0 (69.1.4)

69.1. AN UNNATURAL EXAMPLE 2357since L? (D) is reflexive, an application of the Hahn Banach theorem shows there existsf € L? (D) such that(3°. f) (L(y. L>(D) #0, (—A9, f) Loy L(D) =0 (69.1.2)for all —A@ € H. However, it was just shown H could be considered a subset of (L? (D))’in the manner described above. Therefore, the last equation in the above is of the form0=(-A9.f)y = (f.0) = | foasand since this holds for all @ € Hj (D), it follows by density of Hj (D) in L?’ (D), thatf =0 and now this contradicts the inequality in 69.1.2.Now A is defined on Hj (D) and it delivers something in (Hj )' =H. Of course H{ (D)is dense in L”’ (D). Can A be extended to all of L”’ (D)? The answer is yes and it is moreof the same given above. For @ € Hi (D),—A@ € H C (L? (D))’. Then by the above, for@ € Hj (D) and f € L? (D),(-a0.f) = (1.0) = | foaxK-48. /)1 = M/9)1 =| f £44] < lilo flloand so —A is a continuous linear mapping defined on a dense subspace Hj (D) of L’ (D)and so this does indeed extend to a continuous linear map defined on all of LP (D) givenby the formula(—Ag, f) = I fgdxThis proves the lemma. ;Thus letting V = L? (D) , and H = (Hj (D)) , it follows V C H CV’ is a Gelfand triplewith the understanding of what it means for one space to be included in another describedabove. To emphasize the above, for —A@ € H, f € L’,(-20,f)=(-80.f)y = (1.0) = | foaxMore generally, for g € L” (D),—Ag € (L? (D))' according to the rule(-as.f) = [ feds:With this example of a Gelfand triple, one can define a “porous medium operator”A:V —V’. Let ® be a real valued function defined on R which satisfiesW is continuous (69.1.3)(t—s) (W(t) —¥(s)) >0 (69.1.4)