Mean Value Theorem for Fréchet Derivatives

A linear function T:R→V is totally determined with its value at 1, since T(t)=tT(1), for t∈R.

From this we get that the function ι:B(R,V)→V, with ι(T):=T(1). This is a vector isomorphism, and additionally it is an isometry since

∥T∥B(V,W)=supv∈SR∥T(v)∥V=∥T(1)∥V

Then we can identify that B(R,V) with V.

If σ:(a,b)→V is Fréchet-differentiable at the point t0∈(a,b), then we can identify the derivative σ′(t0)∈B(R,V), with its value at 1, and then for simplicity we can write σ′(t0) to refers to σ′(t0)(1). Then we see that σ′(t0)∈V, and

σ′(t0)=limt→0σ(t+t0)−σ(t0)t∈V

Which actually tells with the connection to the derivatives of functions from R to Rn, and why it behaves like that. This we can actually interpret as a velocity at t0 of σ.

Similarly we can look at the chain rule:
Let σ:(a,b)→Ω⊆V is differentiable at t0∈(a,b) and φ:Ω→W is differentiable at u0:=σ(t0), then we get

(φ∘σ)′(t0)=φ′(u0)(σ′(t0))

The thing with the with the mean value in R is that given f:[a,b]→R continuous and differentiable on (a,b), then f(a)−f(b)=(b−a)f′(c) for some c∈(a,b). The issue here is that we don't know which c, so the most important is to have a bound for |f′(c)|, so we are going to do that in general:

Mean value theorem

Let σ:[a,b]→V is a continuous function. If σ is differentiable for every t∈(a,b), and there's M>0, such that

∥σ′(t)∥≤M∀t∈(a,b)

Then

∥σ(b)−σ(a)∥≤M(b−a)

We get the corollaries:

Let Ω be an open subset of V, φ:Ω→W is of class C1 on Ω, and u0,u1∈Ω such that ut=(1−t)u0+tu1∈Ω for all t∈[0,1], meaning [u0,u1]⊆Ω, then

supt∈[0,1]∥φ′(ut)∥B(V,W)=supu∈[u0,u1]∥φ′(u)∥B(V,W)<∞

and

∥φ(u1)−φ(u0)∥W≤(supu∈[u0,u1]∥φ′(u)∥B(V,W))∥u1−u0∥

Let Ω be an open subset of V, φ:Ω→W is of class C1 on Ω, and u0,u1∈Ω such that ut=(1−t)u0+tu1∈Ω for all t∈[0,1], meaning [u0,u1]⊆Ω, for all u∈Ω, then

supt∈[0,1]∥φ′(ut)−φ′(u)∥B(V,W)<∞

and it satisfies

∥φ(u1)−φ(u0)−φ′(u)(u1−u0)∥≤(supt∈[0,1]∥φ′(ut)−φ′(u)∥)∥u1−u0∥

Let Ω be an open and connected set of a Banach space V, φ:Ω→V is differentiable on Ω, and φ′(u)=0 for all u∈Ω, the φ is constant in Ω.