Newton's Second Law — Question 5

Section 5-5 · Physics pages 700–701

Question 5 A force can be perpendicular to velocity at an instant Use ∑⃗F = m⃗a for constant mass in an inertial frame. At one instant a 2 kg particle has velocity (3, 4) m/s and net force (8, −6) N. x y⃗ v⃗ F Schematic; labels, not drawing lengths, specify the data. (a) Find acceleration and the instantaneous rate of change of speed. (b) Is the particle unaccelerated? (c) If this force stays constant, find velocity one second later and compare speeds.
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Question 5 - Solution A force can be perpendicular to velocity at an instant x y⃗ v⃗ F (a) Project acceleration onto velocity.⃗ a = (8, −6)/2 = (4, −3), ˙v =⃗v ·⃗a |⃗v| = 12 −12 5 = 0⃗ a = (4, −3) m/s2. Since⃗v ·⃗a = 12 −12 = 0, d|⃗v|/dt = (⃗v ·⃗a)/|⃗v| = 0 at that instant. (b) Keep the perpendicular component. |⃗a| = √ 42 + (−3)2 = 5 m/s2̸ = 0 Acceleration has magnitude 5 m/s2 and changes direction of motion at that instant. Zero instantaneous speed derivative does not mean zero vector acceleration. (c) Do not extend an instantaneous orthogonality claim.⃗ v(1) = (3, 4) + (4, −3) = (7, 1), |⃗v(1)| = √ 50 = 7.071 m/s One second later⃗v = (7, 1) m/s, with speed √ 50 ≈7.071 m/s, larger than the initial 5 m/s. A fixed force does not remain perpendicular to the changing velocity.

Question 5

A force can be perpendicular to velocity at an instant

Use ∑F→=ma→\sum\vec F=m\vec a for constant mass in an inertial frame. At one instant a 2 kg particle has velocity (3,4)(3,4) m/s and net force (8,−6)(8,-6) N.

Diagram shown in the original SVG worksheet.

  1. Find acceleration and the instantaneous rate of change of speed.

  2. Is the particle unaccelerated?

  3. If this force stays constant, find velocity one second later and compare speeds.

Question 5 - Solution

A force can be perpendicular to velocity at an instant

Diagram shown in the original SVG worksheet.

(a) Project acceleration onto velocity.

a→=(8,−6)/2=(4,−3),v̇=v→⋅a→|v→|=12−125=0\vec a=(8,-6)/2=(4,-3),\quad\boxed{\dot v=\frac{\vec v\cdot\vec a}{|\vec v|}=\frac{12-12}{5}=0} a→=(4,−3)\vec a=(4,-3) m/s2^2. Since v→⋅a→=12−12=0\vec v\cdot\vec a=12-12=0, d|v→|/dt=(v→⋅a→)/|v→|=0d|\vec v|/dt=(\vec v\cdot\vec a)/|\vec v|=0 at that instant.

(b) Keep the perpendicular component.

|a→|=42+(−3)2=5m/s2≠0|\vec a|=\sqrt{4^2+(-3)^2}=5\,\mathrm{m/s^2}\ne0 Acceleration has magnitude 5 m/s2^2 and changes direction of motion at that instant. Zero instantaneous speed derivative does not mean zero vector acceleration.

(c) Do not extend an instantaneous orthogonality claim.

v→(1)=(3,4)+(4,−3)=(7,1),|v→(1)|=50=7.071m/s\vec v(1)=(3,4)+(4,-3)=(7,1),\quad|\vec v(1)|=\sqrt{50}=7.071\,\mathrm{m/s} One second later v→=(7,1)\vec v=(7,1) m/s, with speed 50≈7.071\sqrt{50}\approx7.071 m/s, larger than the initial 5 m/s. A fixed force does not remain perpendicular to the changing velocity.