69.2. STANDARD TECHNIQUES IN EVOLUTION EQUATIONS 2365

Let φ ∈C∞c (2a−b,2b−a) . Then from the integration by parts formula,∫ 2b−a

2a−bf (t)φ

′ (t)dt

=∫ b

af (t)φ

′ (t)dt +∫ 2b−a

bf (2b− t)φ

′ (t)dt +∫ a

2a−bf (2a− t)φ

′ (t)dt

=∫ b

af (t)φ

′ (t)dt +∫ b

af (u)φ

′ (2b−u)du+∫ b

af (u)φ

′ (2a−u)du

= f (b)φ (b)− f (a)φ (a)−∫ b

af ′ (t)φ (t)dt− f (b)φ (b)+ f (a)φ (2b−a)

+∫ b

af ′ (u)φ (2b−u)du− f (b)φ (2a−b)

+ f (a)φ (a)+∫ b

af ′ (u)φ (2a−u)du

= −∫ b

af ′ (t)φ (t)dt +

∫ b

af ′ (u)φ (2b−u)du+

∫ b

af ′ (u)φ (2a−u)du

= −∫ b

af ′ (t)φ (t)dt−

∫ 2b−a

b− f ′ (2b− t)φ (t)dt−

∫ a

2a−b− f ′ (2a− t)φ (t)dt

= −∫ 2b−a

2a−bf ′ (t)φ (t)dt

where f ′ (t) is given in 69.2.8.

Definition 69.2.12 Let V be a Banach space and let H be a Hilbert space. (TypicallyH = L2 (Ω)) Suppose V ⊆ H is dense in H meaning that the closure in H of V gives H.Then it is often the case that H is identified with its dual space, and then because of thedensity of V in H, it is possible to write

V ⊆ H = H ′ ⊆V ′

When this is done, H is called a pivot space. Another notation which is often used is ⟨ f ,g⟩to denote f (g) for f ∈V ′ and g ∈V. This may also be written as ⟨ f ,g⟩V ′,V . Another termis that V ⊆ H = H ′ ⊆V ′ is called a Gelfand triple.

The next theorem is an example of a trace theorem. In this theorem, f ∈ Lp (0,T ;V )while f ′ ∈ Lp (0,T ;V ′) . It makes no sense to consider the initial values of f in V becauseit is not even continuous with values in V . However, because of the derivative of f it willturn out that f is continuous with values in a larger space and so it makes sense to considerinitial values of f in this other space. This other space is called a trace space.

Theorem 69.2.13 Let V and H be a Banach space and Hilbert space as described in Def-inition 69.2.12. Suppose f ∈ Lp (0,T ;V ) and f ′ ∈ Lp′ (0,T ;V ′) . Then f is a.e. equal to acontinuous function mapping [0,T ] to H. Furthermore, there exists f (0) ∈ H such that

12| f (t)|2H −

12| f (0)|2H =

∫ t

0

⟨f ′ (s) , f (s)

⟩ds, (69.2.10)

69.2. STANDARD TECHNIQUES IN EVOLUTION EQUATIONS 2365Let @ € C2 (2a—b,2b—a). Then from the integration by parts formula,dtaLt= [re vac? “p(2b—1)6"(Nar+ [ f(2a—1)6' (tat= [re2a—bfoes to '(2b—u aus [rye '(2a—u) du= £06)9(0)- F(a) (a) — [Fo Wa —~F0)0(0) + F(a) 920-4)‘freeones6+ ff f' (uw) (2a—u)du- "fros fir )9(2-wdut [Fw 9 Qa—w)aua= -[rooma-["-reo-nowar-f" 1 ea-nowar2a—b2b-a_,= -[ Foowaa—bwhere f (t) is given in 69.2.8. WfDefinition 69.2.12 Let V be a Banach space and let H be a Hilbert space. (TypicallyH =L* (Q)) Suppose V C H is dense in H meaning that the closure in H of V gives H.Then it is often the case that H is identified with its dual space, and then because of thedensity of V in H, it is possible to writeVCH=H'cV’'When this is done, H is called a pivot space. Another notation which is often used is (f, g)to denote f(g) for f © V' and g € V. This may also be written as (f,8)y:y . Another termis thatV CH =H!’ CV’ is called a Gelfand triple.The next theorem is an example of a trace theorem. In this theorem, f € L? (0,T;V)while f’ € L? (0,T;V’). It makes no sense to consider the initial values of f in V becauseit is not even continuous with values in V. However, because of the derivative of f it willturn out that f is continuous with values in a larger space and so it makes sense to considerinitial values of f in this other space. This other space is called a trace space.Theorem 69.2.13 Let V and H be a Banach space and Hilbert space as described in Def-inition 69.2.12. Suppose f € L?(0,T;V) and f' € L? (0,T;V'). Then f is a.e. equal toacontinuous function mapping |0,T| to H. Furthermore, there exists f (0) € H such thatsla SO = [4 ).F0))as, (69.2.10)