Difference between revisions of "Arc length"
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The speed at {{M|t}} of {{M|\gamma}} is <math>\|\dot{\gamma}(t)\|</math> | The speed at {{M|t}} of {{M|\gamma}} is <math>\|\dot{\gamma}(t)\|</math> | ||
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+ | ==See also== | ||
+ | * [[The arc length of a regular parametrisation is smooth]] | ||
{{Definition|Differential Geometry|Geometry of Curves and Surfaces}} | {{Definition|Differential Geometry|Geometry of Curves and Surfaces}} |
Latest revision as of 20:59, 30 March 2015
Arc length of curves here is defined with respect to parametrisations - it is fundamental for defining unit speed parametrisations
Contents
[hide]Definition
TODO: Add picture
Like before we can take small steps δt apart, the length of the line joining such points is ∥γ(t+δt)−γ(t)∥ (where ∥⋅∥ denotes the Euclidean norm)
Noting that ∥γ(t+δt)−γ(t)∥≈∥˙γ(t)δt∥=∥˙γ(t)∥δt
We can now sum over intervals, taking the limit of δt→0 we see that an infinitesimal section of arc length is ∥˙γ(t)∥dt.
Choosing a starting point t0 we can define arc length, s(t) as:
s(t)=∫tt0∥˙γ(u)∥du
Rebasing arc length
Suppose we want the arc length to be measured from ~t0 then:
˜s(t)=∫t~t0∥˙γ(u)∥du =∫t0~t0∥˙γ(u)∥du+∫tt0∥˙γ(u)∥du =∫t0~t0∥˙γ(u)∥du+s(t)
Differentiating arc length
Easy:
ddt[s(t)]=ddt[∫tt0∥˙γ(u)∥du]=∥˙γ(t)∥ by the Fundamental theorem of Calculus
Speed
Speed is the rate of change of distance (velocity is the rate of change of position - which are both vector quantities) - from differentiating the arc length (above) we define speed as:
The speed at t of γ is ∥˙γ(t)∥