Newton's First Law — Question 4

Section 5-2 · Physics pages 638–639

Question 4 An instant of rest is not a first-law state A bead has x(t) = (t −2)2 m with numerical seconds near t=2 s, in an inertial frame. t −2 x The minimum of position is an instant of zero slope, not a flat time history. (a) Find velocity and acceleration at 2 s. (b) Can the bead’s net force be zero throughout a neighborhood of that instant? (c) Compare this event with a bead that remains at x=0.
Show solutionHide solution
Question 4 - Solution An instant of rest is not a first-law state t −2 x (a) Differentiate the history. v = 2(t −2), v(2) = 0, a(2) = 2 m/s2 v = 2(t −2) m/s and a = 2 m/s2. At 2 s the velocity is zero while acceleration is nonzero. (b) Use an interval, not a snapshot. Fnet,x = ma = 2m m/s2̸ = 0 It reverses direction through that instant. Constant velocity does not hold in any surrounding interval, so the history is not a zero-net-force first-law motion. (c) Distinguish lasting rest. xfixed(t) = 0 ⇒vfixed = 0, afixed = 0 A bead staying at x=0 has velocity and acceleration zero throughout the interval. A single photograph of either at x=0 could look the same; neighboring observations distinguish their dynamical states.

Question 4

An instant of rest is not a first-law state

A bead has x(t)=(t−2)2x(t)=(t-2)^2 m with numerical seconds near t=2 s, in an inertial frame.

Diagram shown in the original SVG worksheet.

  1. Find velocity and acceleration at 2 s.

  2. Can the bead’s net force be zero throughout a neighborhood of that instant?

  3. Compare this event with a bead that remains at x=0.

Question 4 - Solution

An instant of rest is not a first-law state

Diagram shown in the original SVG worksheet.

(a) Differentiate the history.

v=2(t−2),v(2)=0,a(2)=2m/s2v=2(t-2),\quad \boxed{v(2)=0,\quad a(2)=2\,\mathrm{m/s^2}} v=2(t−2)v=2(t-2) m/s and a=2a=2 m/s2^2. At 2 s the velocity is zero while acceleration is nonzero.

(b) Use an interval, not a snapshot.

Fnet,x=ma=2mm/s2≠0F_{{\mathrm{net}},x}=ma=2m\,\mathrm{m/s^2}\ne0 It reverses direction through that instant. Constant velocity does not hold in any surrounding interval, so the history is not a zero-net-force first-law motion.

(c) Distinguish lasting rest.

xfixed(t)=0⇒vfixed=0,afixed=0x_{\mathrm{fixed}}(t)=0\ \Rightarrow\ v_{\mathrm{fixed}}=0,\quad a_{\mathrm{fixed}}=0 A bead staying at x=0 has velocity and acceleration zero throughout the interval. A single photograph of either at x=0 could look the same; neighboring observations distinguish their dynamical states.