Position and Displacement — Question 4

Section 4-1 · Physics pages 458–459

Question 4 An arc and its chord measure different lengths A marker moves counterclockwise on a circle of radius 4 m centered at O, from angle 30◦to 150◦, measured from positive x. It follows the shorter arc with no reversal. start finish The thick arc is the path; the dashed arrow is its displacement. (a) Find its initial and final Cartesian positions. (b) Find the displacement vector and length. (c) Find the traveled arc length and explain why adding another full turn changes only one of these quantities.
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Question 4 - Solution An arc and its chord measure different lengths start finish (a) Resolve the two radii.⃗ ri = 4(cos 30◦, sin 30◦) = (2 √ 3, 2) m,⃗ rf = (−2 √ 3, 2) m⃗ ri = (2 √ 3, 2) m and⃗rf = (−2 √ 3, 2) m. Equal vertical coordinates do not mean the positions are the same. (b) Join the actual endpoints. ∆⃗r =⃗rf −⃗ri = (−4 √ 3, 0) m , |∆⃗r| = 6.928 m ∆⃗r = (−4 √ 3, 0) m: due west, magnitude 4 √ 3 ≈6.928 m. The chord is horizontal even though the particle continually changes its heading along the arc. (c) Use radians for arc length. s = R∆θ = 4 (2π 3 ) = 8π 3 m, s+1 = s + 8π m The angular travel is 120◦= 2π/3 rad, so distance is R∆θ = 8π/3 ≈8.378 m. One additional full turn adds 2πR = 8π m to distance. It leaves both endpoint positions and therefore the displacement unchanged.

Question 4

An arc and its chord measure different lengths

A marker moves counterclockwise on a circle of radius 4 m centered at O, from angle 30∘30^\circ to 150∘150^\circ, measured from positive x. It follows the shorter arc with no reversal.

Diagram shown in the original SVG worksheet.

  1. Find its initial and final Cartesian positions.

  2. Find the displacement vector and length.

  3. Find the traveled arc length and explain why adding another full turn changes only one of these quantities.

Question 4 - Solution

An arc and its chord measure different lengths

Diagram shown in the original SVG worksheet.

(a) Resolve the two radii.

r→i=4(cos⁡30∘,sin⁡30∘)=(23,2)m,r→f=(−23,2)m\vec r_i=4(\cos30^\circ,\sin30^\circ)=(2\sqrt3,2)\,\mathrm m,\quad\vec r_f=(-2\sqrt3,2)\,\mathrm m r→i=(23,2)\vec r_i=(2\sqrt3,2) m and r→f=(−23,2)\vec r_f=(-2\sqrt3,2) m. Equal vertical coordinates do not mean the positions are the same.

(b) Join the actual endpoints.

Δr→=r→f−r→i=(−43,0)m,|Δr→|=6.928m\boxed{\Delta\vec r=\vec r_f-\vec r_i=(-4\sqrt3,0)\,\mathrm m},\quad|\Delta\vec r|=6.928\,\mathrm m Δr→=(−43,0)\Delta\vec r=(-4\sqrt3,0) m: due west, magnitude 43≈6.9284\sqrt3\approx6.928 m. The chord is horizontal even though the particle continually changes its heading along the arc.

(c) Use radians for arc length.

s=RΔθ=4(2π3)=8π3m,s+1=s+8πms=R\Delta\theta=4\left(\frac{2\pi}{3}\right)=\frac{8\pi}{3}\,\mathrm m,\quad s_{+1}=s+8\pi\,\mathrm m The angular travel is 120∘=2π/3120^\circ=2\pi/3 rad, so distance is RΔθ=8π/3≈8.378R\Delta\theta=8\pi/3\approx8.378 m. One additional full turn adds 2πR=8π2\pi R=8\pi m to distance. It leaves both endpoint positions and therefore the displacement unchanged.