In mathematics, the metric derivative is a notion of derivative appropriate to parametrized paths in metric spaces. It generalizes the notion of "speed" or "absolute velocity" to spaces which have a notion of distance (i.e. metric spaces) but not direction (such as vector spaces).
Let
(M,d)
E\subseteqR
t\inR
\gamma:E\toM
\gamma
t
|\gamma'|(t)
|\gamma'|(t):=\lims
d(\gamma(t+s),\gamma(t)) | |
|s| |
,
if this limit exists.
Recall that ACp(I; X) is the space of curves γ : I → X such that
d\left(\gamma(s),\gamma(t)\right)\leq
t | |
\int | |
s |
m(\tau)d\tauforall[s,t]\subseteqI
for some m in the Lp space Lp(I; R). For γ ∈ ACp(I; X), the metric derivative of γ exists for Lebesgue-almost all times in I, and the metric derivative is the smallest m ∈ Lp(I; R) such that the above inequality holds.
Rn
\|-\|
\gamma |
:E\toV*
|\gamma'|(t)=\|
\gamma |
(t)\|,
where
d(x,y):=\|x-y\|