16.6. MOTION ON SPACE CURVES 345

19. Let r (t) =(

ln(t) , t2

2 ,√

2t)

for t ∈ [1,2]. Find the length of this curve.

20. Let r (t) =( 2

3 t3/2, t, t)

for t ∈ [0,1]. Find the length of this curve.

21. Let r (t) = (t,cos(3t) ,sin(3t)) for t ∈ [0,1]. Find the length of this curve.

22. Recall p′ (t) = limh→0p(t+h)−p(t)

h . Show that this is equivalent to saying either of thefollowing.

p(t +h)−p(t) = p′ (t)h+o(h)

p(t)−p(s) = p′ (s)(t − s)+o(t − s)

where limh→0o(h)

h = 0.

23. Recall that the length of a curve is approximated by the length of a polygonal curve∑

mk=1 |p(tk)−p(tk−1)| where a = t0 < · · ·< tm = b. Letting the norm of the partition

P = {t0, · · · , tm} be small enough, argue that from differentiability,

m

∑k=1

∣∣p′ (tk−1)∣∣(tk − tk−1)− ε (b−a)

m

∑k=1

|p(tk)−p(tk−1)| ≤m

∑k=1

∣∣p′ (tk−1)∣∣(tk − tk−1)+ ε (b−a)

Explain why if you let ∥Pk∥→ 0,

lim supk→∞

(∑

tk∈Pk

|p(tk)−p(tk−1)|−∫ b

a

∣∣p′ (t)∣∣dt

)

− lim infk→∞

(∑

tk∈Pk

|p(tk)−p(tk−1)|−∫ b

a

∣∣p′ (t)∣∣dt

)≤ 2ε (b−a)

Now explain why limk→∞ ∑tk∈Pk|p(tk)−p(tk−1)|=

∫ ba |p′ (t)|dt. This gives a proof

that the lengths of polygonal curves approximating the curve converge to the appro-priate integral. Thus we could have defined the length as the limit of the lengths ofthe approximating polygonal curves and replaced the definition with a theorem.

16.6 Motion on Space CurvesA fly buzzing around the room, a person riding a roller coaster, and a satellite orbiting theearth all have something in common. They are moving over some sort of curve in threedimensions.

Denote by R(t) the position vector of the point on the curve which occurs at time t.Assume that R′,R′′ exist and are continuous. Thus R′ = v, the velocity and R′′ = a isdefined as the acceleration.

16.6. MOTION ON SPACE CURVES 34519. Let r(t) = (in (t), C, v2) for t € [1,2]. Find the length of this curve.20. Let r (t) = (323/7, 1,1) for ¢ € [0,1]. Find the length of this curve.21. Let r(t) = (t,cos (3r) , sin (31)) for t € [0, 1]. Find the length of this curve.22. Recall p’ (t) =limp_40 Beth ple)following.. Show that this is equivalent to saying either of thep(tth)—p(t) = p'(t)h+o(h)p(t)—p(s) = p'(s)(t—s)+o(t—s)o(h)where lim,.9 =~ = 0.23. Recall that the length of a curve is approximated by the length of a polygonal curveve) IP (te) — p (te_1)| where a = to < --- < ty = b. Letting the norm of the partitionP = {to,-++ ,tm} be small enough, argue that from differentiability,y Ip’ (%-1)| (th —th_-1) — € (b—a)k=1¥ pte) —P (tea) < ¥. |p! (te-1)| (te —te-1) +e (b—a)k=1 k=1Explain why if you let ||P,|| > 0,blim sup ( y Pl) —Pla)I- | Hola)k—yoo thEPEb—lim inf (x P(x) —Pln)|- | 1 oa)kv \ Ph< 2e€(b-a)Now explain why lim. Yep, |P (te) — P (te-1)| = fe |p’ (t)|dt. This gives a proofthat the lengths of polygonal curves approximating the curve converge to the appro-priate integral. Thus we could have defined the length as the limit of the lengths ofthe approximating polygonal curves and replaced the definition with a theorem.16.6 Motion on Space CurvesA fly buzzing around the room, a person riding a roller coaster, and a satellite orbiting theearth all have something in common. They are moving over some sort of curve in threedimensions.Denote by R(t) the position vector of the point on the curve which occurs at time f.Assume that R’,R” exist and are continuous. Thus R’ = v, the velocity and R” = a isdefined as the acceleration.