Newton's Second Law — Question 10

Section 5-5 · Physics pages 710–711

Question 10 A force bound constrains a velocity change A 3 kg particle must change velocity from (4, 0) to (0, 3) m/s. Its net force can point in any direction but has magnitude at most 6 N at all times. Use ∆⃗v = R⃗a dt.⃗ vi⃗ vf ∆⃗v The diagonal in velocity space is the required vector change. (a) Find the required velocity-change magnitude and a lower time bound. (b) Exhibit a force history that attains the bound. (c) Why is using only the change of speed insufficient?
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Question 10 - Solution A force bound constrains a velocity change⃗ vi⃗ vf ∆⃗v (a) Bound the integral of acceleration. |∆⃗v| = |(−4, 3)| = 5, |∆⃗v| ≤ Z T 0 Fmax m dt = 2T ⇒ T ≥2.5 s ∆⃗v = (−4, 3) m/s has magnitude 5 m/s. Since |⃗a| ≤2 m/s2, 5 ≤2T, so T ≥2.5 s. (b) Use a constant force along the velocity change.⃗ a = (−4, 3) 2.5 = (−1.6, 1.2),⃗ F = 3⃗a = (−4.8, 3.6) N Choose⃗a = (−1.6, 1.2) m/s2 for 2.5 s, giving⃗F = (−4.8, 3.6) N with magnitude 6 N. It produces the exact final vector, so the bound is attainable. (c) Keep directional change. |⃗vf| −|⃗vi| = |3 −4| = 1 m/s < |⃗vf −⃗vi| = 5 m/s Speed changes only from 4 to 3 m/s, a magnitude difference of 1 m/s. The full vector change is 5 m/s because the direction turns. A time based on 1 m/s would not satisfy the specified endpoint velocities.

Question 10

A force bound constrains a velocity change

A 3 kg particle must change velocity from (4,0)(4,0) to (0,3)(0,3) m/s. Its net force can point in any direction but has magnitude at most 6 N at all times. Use Δv→=∫a→dt\Delta\vec v=\int\vec a\,dt.

Diagram shown in the original SVG worksheet.

  1. Find the required velocity-change magnitude and a lower time bound.

  2. Exhibit a force history that attains the bound.

  3. Why is using only the change of speed insufficient?

Question 10 - Solution

A force bound constrains a velocity change

Diagram shown in the original SVG worksheet.

(a) Bound the integral of acceleration.

|Δv→|=|(−4,3)|=5,|Δv→|≤∫0TFmaxmdt=2T⇒T≥2.5s|\Delta\vec v|=|(-4,3)|=5,\quad |\Delta\vec v|\le\int_0^T\frac{F_{\max}}m\,dt=2T\ \Rightarrow\ \boxed{T\ge2.5\,\mathrm s} Δv→=(−4,3)\Delta\vec v=(-4,3) m/s has magnitude 5 m/s. Since |a→|≤2|\vec a|\le2 m/s2^2, 5≤2T5\le2T, so T≥2.5T\ge2.5 s.

(b) Use a constant force along the velocity change.

a→=(−4,3)2.5=(−1.6,1.2),F→=3a→=(−4.8,3.6)N\vec a=\frac{(-4,3)}{2.5}=(-1.6,1.2),\quad\vec F=3\vec a=(-4.8,3.6)\,\mathrm N Choose a→=(−1.6,1.2)\vec a=(-1.6,1.2) m/s2^2 for 2.5 s, giving F→=(−4.8,3.6)\vec F=(-4.8,3.6) N with magnitude 6 N. It produces the exact final vector, so the bound is attainable.

(c) Keep directional change.

||v→f|−|v→i||=|3−4|=1m/s<|v→f−v→i|=5m/s\big||\vec v_f|-|\vec v_i|\big|=|3-4|=1\,\mathrm{m/s}<|\vec v_f-\vec v_i|=5\,\mathrm{m/s} Speed changes only from 4 to 3 m/s, a magnitude difference of 1 m/s. The full vector change is 5 m/s because the direction turns. A time based on 1 m/s would not satisfy the specified endpoint velocities.