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19b. Rectilinear and Circular Motion — Practice

Drill sheet for 19. Rectilinear & Circular Motion. Book-style solved ideas as guided checks and regenerable worksheets.


1. Evaluate vv and aa at a time​

Book. s=12t3−2ts=\tfrac12 t^{3}-2t: at t=2t=2, v=4v=4, a=6a=6.

v and a at a given t

Differentiate s, then plug in
(1)For s=12t3−2ts=\tfrac12 t^{3}-2t, find vv and aa at t=2t=2.
v=32t2−2v=\tfrac32 t^{2}-2 ⇒ v(2)=4v(2)=4.
a=3ta=3t ⇒ a(2)=6a(2)=6.
v=4v=4; a=6a=6.
(2)For s=t3−1ts=t^{3}-1t, find vv and aa at t=2t=2.
v=3t2−1v=3t^{2}-1 ⇒ v(2)=12−1v(2)=12-1.
a=6ta=6t ⇒ a(2)=12a(2)=12.
v=11v=11; a=12a=12.

2. Full analysis of a cubic path​

Book. s=t3−6t2+9t+4s=t^{3}-6t^{2}+9t+4:

v=3(t−1)(t−3),a=6(t−2).v=3(t-1)(t-3),\qquad a=6(t-2).
QuestionAnswer
v=0v=0t=1t=1: s=8s=8, a=−6a=-6; t=3t=3: s=4s=4, a=6a=6
a=0a=0t=2t=2: s=6s=6, v=−3v=-3
ss increasingt<1t<1 or t>3t>3
vv increasingt>2t>2
Direction changest=1t=1 and t=3t=3

Intervals from v and a

Factor, then read sign charts
(1)For s=t3−6t2+9t+4s=t^{3}-6t^{2}+9t+4: when is ss increasing? When does direction change?
v=3(t−1)(t−3)v=3(t-1)(t-3); ss increasing for t<1t<1 and t>3t>3.
Turns at t=1t=1 and t=3t=3 (v=0v=0, a≠0a\neq 0).
Inc. on (−∞,1)∪(3,∞)(-\infty,1)\cup(3,\infty); turns at 1,31,3.
(2)For s=t3−9t2+24ts=t^{3}-9t^{2}+24t: when is ss decreasing? When is vv increasing?
v=3(t−2)(t−4)v=3(t-2)(t-4) ⇒ ss decreasing on (2,4)(2,4).
a=6(t−3)a=6(t-3) ⇒ vv increasing for t>3t>3.
Dec. on (2,4)(2,4); vv inc. for t>3t>3.

3. Total distance with turns​

Book. s=t3−9t2+24ts=t^{3}-9t^{2}+24t: turns at t=2,4t=2,4.

s(0)=0→s(2)=20→s(4)=16→s(5)=20s(0)=0\to s(2)=20\to s(4)=16\to s(5)=20: total distance 20+4+4=2820+4+4=28 ft.

Fig. 19-5 — total distance 28 ft

Total distance traveled

Sum |Δs| between consecutive critical times
(1)Particle: s(0)=3s(0)=3, moves left to s(2.5)=−27/16s(2.5)=-27/16, then to s(3)=0s(3)=0. Total distance on [0,3][0,3]?
3−(−27/16)+∣0−(−27/16)∣=3+27/16+27/16=51/83-(-27/16)+|0-(-27/16)|=3+27/16+27/16=51/8.
51/851/8.
(2)Particle: s(0)=3s(0)=3, moves left to s(2.5)=−27/16s(2.5)=-27/16, then to s(3)=0s(3)=0. Total distance on [0,3][0,3]?
3−(−27/16)+∣0−(−27/16)∣=3+27/16+27/16=51/83-(-27/16)+|0-(-27/16)|=3+27/16+27/16=51/8.
51/851/8.

4. Speed vs velocity​

Book. v=2(t−1)2(2t−5)v=2(t-1)^{2}(2t-5), a=12(t−1)(t−2)a=12(t-1)(t-2).

Speed ∣v∣|v| increases when vv and aa have the same sign; decreases when they have opposite signs. Direction changes at t=2.5t=2.5 (simple zero of vv that is an extremum of ss). Total distance on [0,3][0,3] is 51/851/8.

Fig. 19-6 — total distance 51/8

5. Projected upward​

Book. s=112t−16t2s=112t-16t^{2}: v=112−32tv=112-32t, a=−32a=-32.

  • t=3t=3: rising at 1616 ft/s; t=4t=4: falling at 1616 ft/s
  • Peak: v=0v=0 ⇒ t=3.5t=3.5, s=196s=196 ft
  • Height 9696 ft at t=1t=1 (rising) and t=6t=6 (falling)

6. Circular motion numbers​

Book. θ=t3/50−t\theta=t^{3}/50-t: at t=10t=10, θ=10\theta=10, ω=5\omega=5, α=6/5\alpha=6/5.

θ, ω, α

Differentiate the angle function
(1)If θ=2t2\theta=2t^{2}, find ω\omega and α\alpha at t=2t=2.
ω=2⋅2t=4t\omega=2\cdot2t=4t ⇒ ω(2)=8\omega(2)=8.
α=4\alpha=4 (constant).
ω=8\omega=8; α=4\alpha=4.
(2)If θ=2t2\theta=2t^{2}, find ω\omega and α\alpha at t=2t=2.
ω=2⋅2t=4t\omega=2\cdot2t=4t ⇒ ω(2)=8\omega(2)=8.
α=4\alpha=4 (constant).
ω=8\omega=8; α=4\alpha=4.

7–8. Dropped stone and rocket​

Book 7. Dropped from 10241024 ft: s=1024−16t2s=1024-16t^{2} ⇒ hit at t=8t=8 with speed 256256 ft/s =174611=174\tfrac{6}{11} mi/h via

x ft/s=1522x mi/h.(19.3)x\ \mathrm{ft/s}=\frac{15}{22}x\ \mathrm{mi/h}. \tag{19.3}

Book 8. Rocket v0=192v_0=192: peak at t=6t=6, height 576576 ft; back at t=12t=12 with speed 192192 ft/s (symmetric flight).

Free-fall applications

Peak, impact, unit conversion
(1)Dropped from 10241024 ft (v0=0v_0=0). When does it hit, and with what speed?
1024−16t2=01024-16t^{2}=0 ⇒ t=8t=8.
v=−32⋅8=−256v=-32\cdot 8=-256 ft/s; speed 256256 ft/s.
t=8t=8 s; speed 256256 ft/s.
(2)Dropped from 10241024 ft (v0=0v_0=0). When does it hit, and with what speed?
1024−16t2=01024-16t^{2}=0 ⇒ t=8t=8.
v=−32⋅8=−256v=-32\cdot 8=-256 ft/s; speed 256256 ft/s.
t=8t=8 s; speed 256256 ft/s.
(3)Rocket: v0=192v_0=192 ft/s from ground. Max height time and height? Return time?
v=192−32t=0v=192-32t=0 ⇒ t=6t=6, s=576s=576 ft.
Ground again at t=12t=12; impact speed 192192 ft/s.
66 s; 576576 ft; 1212 s.

Supplementary Problems​

9. Prove the speed criterion​

Speed S=∣v∣S=|v|. If v>0v>0 then S=vS=v and dS/dt=adS/dt=a. If v<0v<0 then S=−vS=-v and dS/dt=−adS/dt=-a. So SS increases when vv and aa have the same sign, and decreases when they have opposite signs.

10. Snapshots along s=t3−6t2+9ts=t^{3}-6t^{2}+9t​

At each tt, report ss, direction (sign of vv), and whether speed is increasing.

ttssmotionspeed
1/21/225/825/8rightdecreasing
3/23/227/827/8leftincreasing
5/25/25/85/8leftdecreasing
4444rightincreasing

Position · direction · speed trend

Problem 10 style
(1)For s=t3−6t2+9ts=t^{3}-6t^{2}+9t: at t=1/2t=1/2 and t=3/2t=3/2, give direction and whether speed is increasing.
v=3(t−1)(t−3)v=3(t-1)(t-3), a=6(t−2)a=6(t-2).
t=1/2t=1/2: v>0v>0, a<0a<0 ⇒ right, speed decreasing.
t=3/2t=3/2: v<0v<0, a<0a<0 ⇒ left, speed increasing.
Right, slowing; left, speeding up.
(2)For s=t3−6t2+9ts=t^{3}-6t^{2}+9t at t=4t=4: ss, vv, and speed trend?
s=4s=4; v=9v=9 (right); a>0a>0 ⇒ speed increasing.
s=4s=4; right at 99 ft/s; speeding up.

11–12. Reverse gear / direction changes​

Book 11. Locomotive s=3t4−44t3+144t2s=3t^{4}-44t^{3}+144t^{2} is in reverse on 3<t<83<t<8.

Book 12. Direction changes: (a) t=2,4t=2,4; (b) none; (c) t=1,3t=1,3; (d) t=1t=1.

When does direction change?

Factor v; discard double roots that do not reverse
(1)Direction changes for s=2t3−12t2+18t−5s=2t^{3}-12t^{2}+18t-5?
v=6(t−1)(t−3)v=6(t-1)(t-3); turns at 11 and 33.
t=1t=1 and t=3t=3.
(2)Direction changes for s=2t3−12t2+18t−5s=2t^{3}-12t^{2}+18t-5?
v=6(t−1)(t−3)v=6(t-1)(t-3); turns at 11 and 33.
t=1t=1 and t=3t=3.

13–14 / 16–17 / 20. More free fall​

Book 13. s=64t−16t2s=64t-16t^{2}: at 4848 ft of rise, v=v0/2v=v_0/2.

Book 14. From roof, s=96t−16t2s=96t-16t^{2}; street 112112 ft below. At t=2t=2: 240240 ft above street, 3232 ft/s up; impact v=−128v=-128 ft/s.

Book 16–17. Drop 144144 ft → 33 s; drop 100100 ft → 5461154\tfrac{6}{11} mi/h.

Book 20. Ground-to-ground in 1515 s ⇒ v0=240v_0=240 ft/s.

Free-fall supplementary

Half-velocity, roofs, wells, unit conversion
(1)Ball from roof: s=96t−16t2s=96t-16t^{2} relative to roof; street is 112112 ft below. Velocity when it hits the street?
Street: s=−112=96t−16t2s=-112=96t-16t^{2} ⇒ 16t2−96t−112=016t^{2}-96t-112=0 ⇒ t2−6t−7=0t^{2}-6t-7=0 ⇒ t=7t=7 (t≥0t\ge 0).
v=96−32tv=96-32t; v(7)=−128v(7)=-128 ft/s.
−128-128 ft/s (book uses s=96t−16t2s=96t-16t^{2} from roof).
(2)Dropped from a 1010-story building (100100 ft). Impact speed in mi/h?
100−16t2=0100-16t^{2}=0 ⇒ t=2.5t=2.5; ∣v∣=80|v|=80 ft/s.
1522⋅80=54611\tfrac{15}{22}\cdot 80=54\tfrac{6}{11} mi/h.
5461154\tfrac{6}{11} mi/h.
(3)For s=64t−16t2s=64t-16t^{2}, show velocity is halved after the first 4848 ft of rise.
v=64−32tv=64-32t; v0=64v_0=64.
48=64t−16t248=64t-16t^{2} ⇒ t2−4t+3=0t^{2}-4t+3=0 ⇒ t=1t=1 (rising).
v(1)=32=v0/2v(1)=32=v_0/2.
At s=48s=48, v=32=v0/2v=32=v_0/2.

15 / 18–19. Wheel and road distance​

Book 15. θ=128t−12t2\theta=128t-12t^{2} at t=3t=3: ω=56\omega=56, α=−24\alpha=-24.

Book 18. s=8t3−12t2+6t−1s=8t^{3}-12t^{2}+6t-1 on [0,1][0,1]: distance 22 mi (v≥0v\ge 0).

Book 19. s=5t−t2s=5t-t^{2} on [0,3][0,3]: turn at t=2.5t=2.5; distance 6.56.5 mi.

Angular rates & path length

Problems 15, 18–19
(1)Wheel θ=128t−12t2\theta=128t-12t^{2}. Find ω\omega and α\alpha at t=3t=3.
ω=128−24t\omega=128-24t ⇒ ω(3)=56\omega(3)=56.
α=−24\alpha=-24.
ω=56\omega=56 rad/s; α=−24\alpha=-24 rad/s².
(2)Car s=5t−t2s=5t-t^{2} from t=0t=0 to t=3t=3. Total distance?
v=5−2t=0v=5-2t=0 at t=2.5t=2.5; s(0)=0s(0)=0, s(2.5)=6.25s(2.5)=6.25, s(3)=6s(3)=6.
Distance 6.25+∣6−6.25∣=6.56.25+|6-6.25|=6.5 miles.
6.56.5 miles.

21–22. Calculator / exact roots​

Book 21. s=t4−3t2+2ts=t^{4}-3t^{2}+2t: turns at t=1t=1 and t=(−1±3)/2t=(-1\pm\sqrt{3})/2; left on (−∞,(−1−3)/2)(-\infty,(-1-\sqrt{3})/2) and ((−1+3)/2,1)((-1+\sqrt{3})/2,1).

Book 22. Paths s=3t−t2s=3t-t^{2} and s=t3−t2+1s=t^{3}-t^{2}+1: same position near 0.350.35 and 1.531.53; same velocity at t=±1t=\pm 1; at meetings they move opposite ways.


Mixed review​

Motion mixed set

Rectilinear · distance · free fall · circular · supplementary
(1)Dropped from 10241024 ft (v0=0v_0=0). When does it hit, and with what speed?
1024−16t2=01024-16t^{2}=0 ⇒ t=8t=8.
v=−32⋅8=−256v=-32\cdot 8=-256 ft/s; speed 256256 ft/s.
t=8t=8 s; speed 256256 ft/s.
(2)From rest: θ=t3/50−t\theta=t^{3}/50-t. Find θ,ω,α\theta,\omega,\alpha at t=10t=10.
θ=10\theta=10 rad.
ω=3t2/50−1=5\omega=3t^{2}/50-1=5 rad/s.
α=6t/50=6/5\alpha=6t/50=6/5 rad/s².
1010; 55; 6/56/5.
(3)For s=t3−6t2+9ts=t^{3}-6t^{2}+9t at t=5/2t=5/2: position, direction, speed trend?
s=5/8s=5/8; v=−9/4v=-9/4 (left); a>0a>0 with v<0v<0 ⇒ speed decreasing.
s=5/8s=5/8; left; speed decreasing.
(4)For s=t3−6t2+9ts=t^{3}-6t^{2}+9t at t=5/2t=5/2: position, direction, speed trend?
s=5/8s=5/8; v=−9/4v=-9/4 (left); a>0a>0 with v<0v<0 ⇒ speed decreasing.
s=5/8s=5/8; left; speed decreasing.
(5)For s=t3−6t2+9t+4s=t^{3}-6t^{2}+9t+4: find ss and aa when v=0v=0.
t=1t=1: s=8s=8, a=−6a=-6; t=3t=3: s=4s=4, a=6a=6.
(s,a)=(8,−6)(s,a)=(8,-6) and (4,6)(4,6).
(6)Does s=t3−3t2+3t+3s=t^{3}-3t^{2}+3t+3 ever change direction?
v=3(t−1)2≥0v=3(t-1)^{2}\ge 0; double root at t=1t=1 is not a turn.
No turns.

Self-check​

Quiz

Motion practice review

1 / 7

For s = ½t³ − 2t, a at t = 2 equals…

Pick an answer to see if you are right.

Further Reading​