Newtonian Mechanics — Question 8

Section 5-1 · Physics pages 626–627

Question 8 Initial conditions complete a motion prediction A model stipulates constant acceleration a = 2 m/s2. Run A starts at x = 0 with v = 1 m/s. Run B starts at x = 5 m with v = −1 m/s. Use the same time origin. x (m) A: x0 = 0 B: x0 = 5 v0A = +1 m/s v0B = −1 m/s a = +2 m/s2 (both) Schematic; labels specify the data. Arrow lengths are not a common scale. (a) Write each position history. (b) Find their positions and velocities at 2 s. (c) Explain why one acceleration law does not predict a unique trajectory without initial data.
Show solutionHide solution
Question 8 - Solution Initial conditions complete a motion prediction x (m) A: x0 = 0 B: x0 = 5 v0A = +1 m/s v0B = −1 m/s a = +2 m/s2 (both) (a) Integrate with the correct constants. x = x0 + v0t + 1 2at2 : xA = t + t2, xB = 5 −t + t2 xA = t + t2 m and xB = 5 −t + t2 m for numerical seconds. Velocities are 1 + 2t and −1 + 2t m/s. (b) Evaluate the distinct states. (xA, vA)t=2 = (6, 5) , (xB, vB)t=2 = (7, 3) (SI) At 2 s, (xA, vA) = (6 m, 5 m/s) and (xB, vB) = (7 m, 3 m/s). (c) Retain integration constants. v(t) = v0 + ∫t 0 a du, x(t) = x0 + ∫t 0 v(u) du Acceleration fixes how velocity changes. Initial velocity sets the starting rate, and initial position sets the spatial offset. Both constants are needed even when the dynamical rule itself is fixed.

Question 8

Initial conditions complete a motion prediction

A model stipulates constant acceleration a=2a=2 m/s2^2. Run A starts at x=0x=0 with v=1v=1 m/s. Run B starts at x=5x=5 m with v=−1v=-1 m/s. Use the same time origin.

Diagram shown in the original SVG worksheet.

  1. Write each position history.

  2. Find their positions and velocities at 2 s.

  3. Explain why one acceleration law does not predict a unique trajectory without initial data.

Question 8 - Solution

Initial conditions complete a motion prediction

Diagram shown in the original SVG worksheet.

(a) Integrate with the correct constants.

x=x0+v0t+12at2:xA=t+t2,xB=5−t+t2x=x_0+v_0t+\tfrac12at^2:\quad x_A=t+t^2,\quad x_B=5-t+t^2 xA=t+t2x_A=t+t^2 m and xB=5−t+t2x_B=5-t+t^2 m for numerical seconds. Velocities are 1+2t1+2t and −1+2t-1+2t m/s.

(b) Evaluate the distinct states.

(xA,vA)t=2=(6,5),(xB,vB)t=2=(7,3)(SI)\boxed{(x_A,v_A)_{t=2}=(6,5)},\quad\boxed{(x_B,v_B)_{t=2}=(7,3)}\quad\text{(SI)} At 2 s, (xA,vA)=(6m,5m/s)(x_A,v_A)=(6\ \mathrm m,5\ \mathrm{m/s}) and (xB,vB)=(7m,3m/s)(x_B,v_B)=(7\ \mathrm m,3\ \mathrm{m/s}).

(c) Retain integration constants.

v(t)=v0+∫0tadu,x(t)=x0+∫0tv(u)duv(t)=v_0+\int_0^t a\,du,\qquad x(t)=x_0+\int_0^t v(u)\,du Acceleration fixes how velocity changes. Initial velocity sets the starting rate, and initial position sets the spatial offset. Both constants are needed even when the dynamical rule itself is fixed.