Each of these parameters is measurable from ground based tests, making it facile to predict flight system performance.
Until now, such a minuscule reduction has only been measurable from space, where the lack of atmosphere allows spacecraft to take more precise readings.
When is measurable, from (2.6), we obtain that is measurable.
Extraction for some resources has reached such proportions that evidence is measurable from space.
((H_{1})):: The mapping (F JtimesOmegatimes Yrightarrow Y) is measurable from ((Omega_{b}times Y,mathscr{P}_{b}timesmathscr{B}(Y))) into ((Y,mathscr {B}(Y))).
The mapping (F JtimesOmegatimes Yrightarrow Y) is measurable from ((Omega_{b}times Y,mathscr{P}_{b}timesmathscr{B}(Y))) into ((Y,mathscr {B}(Y))).
We say that f satisfies Carathéodory conditions if (i) for any x ∈ X, the map t → f ( t, x ) is measurable from Ω to Y; (ii) for almost all t ∈ Ω, the map x → f ( t, x ) is continuous from X to Y. . for any x ∈ X, the map t → f ( t, x ) is measurable from Ω to Y; for almost all t ∈ Ω, the map x → f ( t, x ) is continuous from X to Y. Definition 1 (Nemytskii's operator).
A function f : Ω × X → Y is said to be a Carathéodory function if (i) for any fixed x ∈ X, the function t → f ( t, x ) is measurable from Ω to Y; (ii) for almost any t ∈ Ω, the function f ( t, ⋅ ) : X → Y is continuous. . for any fixed x ∈ X, the function t → f ( t, x ) is measurable from Ω to Y; for almost any t ∈ Ω, the function f ( t, ⋅ ) : X → Y is continuous.
(S t,r omega S r,s omega)x=S t,s omega)x) for all (sleq rleq t) and (xin X), (S t,s omega)) is continuous in X for all (sleq t), for all (s< t) and (xin X), the mapping (omegamapsto S t,s omega)x) is measurable from ((Omega, mathcal{F})) to ((X,mathscr{B}(X))), for all (tinmathbb{R}, xin X), and (mathbb{P} -a.e.
