Relative Motion in Two Dimensions — Question 8

Section 4-8 · Physics pages 606–607

Question 8 Translate the frame and rotate its axes consistently A particle’s ground velocity is (5, 1) m/s. Observer B moves with ground velocity (1, −2) m/s and uses axes turned 45◦counterclockwise from the ground axes. For a vector (wx, wy), the rotated components are ((wx + wy)/ √ 2, (−wx + wy)/ √ 2). x y x′ y′ The observer’s axes are rotated but have a fixed orientation in time. (a) Find particle velocity relative to B, first in ground-oriented axes. (b) Express that relative velocity in B’s rotated axes and check its magnitude. (c) Explain why rotating the particle velocity and then subtracting the unrotated pair (1, −2) is invalid. How could rotating first be done correctly?
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Question 8 - Solution Translate the frame and rotate its axes consistently x y x′ y′ (a) Subtract velocities in one common basis.⃗ vA/B = (5, 1) −(1, −2) = (4, 3) m/s⃗ vA/B = (5, 1) −(1, −2) = (4, 3) m/s in ground-oriented axes. This relative physical vector is defined before choosing how to describe its components. (b) Project the relative vector onto the rotated basis.⃗ v′ A/B = (4 + 3 √ 2 , −4 + 3 √ 2 ) = ( 7 √ 2, −1 √ 2 ) m/s, v′ = √ 49/2 + 1/2 = 5 m/s The new pair is (7/ √ 2, −1/ √ 2) m/s. Its magnitude is √ 49/2 + 1/2 = 5 m/s, matching √ 42 + 32. The negative second component reflects the new axis orientation, not a different physical relative motion. (c) Avoid mixing bases in one subtraction. Q(⃗vA −⃗vB) = Q⃗vA −Q⃗vB = (6, −4) −(−1, −3) √ 2 = (7, −1) √ 2 m/s The proposed shortcut subtracts components referenced to different directions. If rotating first, transform both input velocities: A becomes (6/ √ 2, −4/ √ 2) and B becomes (−1/ √ 2, −3/ √ 2) m/s. Their difference again gives (7/ √ 2, −1/ √ 2) m/s because rotation is linear.

Question 8

Translate the frame and rotate its axes consistently

A particle’s ground velocity is (5,1)(5,1) m/s. Observer B moves with ground velocity (1,−2)(1,-2) m/s and uses axes turned 45∘45^\circ counterclockwise from the ground axes. For a vector (wx,wy)(w_x,w_y), the rotated components are ((wx+wy)/2,(−wx+wy)/2)((w_x+w_y)/\sqrt2,(-w_x+w_y)/\sqrt2).

Diagram shown in the original SVG worksheet.

  1. Find particle velocity relative to B, first in ground-oriented axes.

  2. Express that relative velocity in B’s rotated axes and check its magnitude.

  3. Explain why rotating the particle velocity and then subtracting the unrotated pair (1,−2)(1,-2) is invalid. How could rotating first be done correctly?

Question 8 - Solution

Translate the frame and rotate its axes consistently

Diagram shown in the original SVG worksheet.

(a) Subtract velocities in one common basis.

v→A/B=(5,1)−(1,−2)=(4,3)m/s\boxed{\vec v_{A/B}=(5,1)-(1,-2)=(4,3)\,\mathrm{m/s}} v→A/B=(5,1)−(1,−2)=(4,3)\vec v_{A/B}=(5,1)-(1,-2)=(4,3) m/s in ground-oriented axes. This relative physical vector is defined before choosing how to describe its components.

(b) Project the relative vector onto the rotated basis.

v→A/B′=(4+32,−4+32)=(72,−12)m/s,v′=49/2+1/2=5m/s\vec v'_{A/B}=\left(\frac{4+3}{\sqrt2},\frac{-4+3}{\sqrt2}\right)=\left(\frac7{\sqrt2},-\frac1{\sqrt2}\right)\,\mathrm{m/s},\quad v'=\sqrt{49/2+1/2}=5\,\mathrm{m/s} The new pair is (7/2,−1/2)(7/\sqrt2,-1/\sqrt2) m/s. Its magnitude is 49/2+1/2=5\sqrt{49/2+1/2}=5 m/s, matching 42+32\sqrt{4^2+3^2}. The negative second component reflects the new axis orientation, not a different physical relative motion.

(c) Avoid mixing bases in one subtraction.

Q(v→A−v→B)=Qv→A−Qv→B=(6,−4)−(−1,−3)2=(7,−1)2m/sQ(\vec v_A-\vec v_B)=Q\vec v_A-Q\vec v_B=\frac{(6,-4)-(-1,-3)}{\sqrt2}=\frac{(7,-1)}{\sqrt2}\quad\mathrm{m/s} The proposed shortcut subtracts components referenced to different directions. If rotating first, transform both input velocities: A becomes (6/2,−4/2)(6/\sqrt2,-4/\sqrt2) and B becomes (−1/2,−3/2)(-1/\sqrt2,-3/\sqrt2) m/s. Their difference again gives (7/2,−1/2)(7/\sqrt2,-1/\sqrt2) m/s because rotation is linear.