Newtonian Mechanics — Question 10

Section 5-1 · Physics pages 630–631

Question 10 A constraint equation must hold throughout the motion Two points move on one line joined by an ideal rigid link of length 2 m, with B always to the right of A. A proposed history is xA = t2 m and xB = 2 + 3t m, with numerical t in seconds. A B fixed 2 m The line and ordering are fixed, so separation has one positive constant value. (a) Write the geometric constraint and its velocity consequence. (b) Test the proposed histories at 0 and 1 s. (c) Give a history for B compatible with A for all times, and find its acceleration.
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Question 10 - Solution A constraint equation must hold throughout the motion A B fixed 2 m (a) Differentiate a fixed separation. xB −xA = L ⇒vB −vA = 0 ⇒aB −aA = 0 The constraint is xB −xA = 2 m, so vB −vA = 0. Differentiating once more gives equal accelerations along this fixed line. (b) Check more than initial geometry. d(t) = 2 + 3t −t2 : d(0) = 2, d(1) = 4 m, ˙d(0) = 3 m/s The initial separation is 2 m, but at 1 s it is 5 −1 = 4 m. Even at t=0 the velocities, 3 and 0 m/s, violate the derivative constraint. The proposed pair is not a rigid-link history. (c) Enforce the boundary condition identically. xB = 2 + t2, vB = 2t, aB = 2 m/s2 xB = 2 + t2 m is compatible, giving vB = 2t m/s and aB = 2 m/s2. Geometric constraints reduce the independent variables before the dynamical equations are solved.

Question 10

A constraint equation must hold throughout the motion

Two points move on one line joined by an ideal rigid link of length 2 m, with B always to the right of A. A proposed history is xA=t2x_A=t^2 m and xB=2+3tx_B=2+3t m, with numerical t in seconds.

Diagram shown in the original SVG worksheet.

  1. Write the geometric constraint and its velocity consequence.

  2. Test the proposed histories at 0 and 1 s.

  3. Give a history for B compatible with A for all times, and find its acceleration.

Question 10 - Solution

A constraint equation must hold throughout the motion

Diagram shown in the original SVG worksheet.

(a) Differentiate a fixed separation.

xB−xA=L⇒vB−vA=0⇒aB−aA=0x_B-x_A=L\ \Rightarrow\ v_B-v_A=0\ \Rightarrow\ a_B-a_A=0 The constraint is xB−xA=2x_B-x_A=2 m, so vB−vA=0v_B-v_A=0. Differentiating once more gives equal accelerations along this fixed line.

(b) Check more than initial geometry.

d(t)=2+3t−t2:d(0)=2,d(1)=4m,ḋ(0)=3m/sd(t)=2+3t-t^2:\quad d(0)=2,\ d(1)=4\,\mathrm m,\quad\dot d(0)=3\,\mathrm{m/s} The initial separation is 2 m, but at 1 s it is 5−1=45-1=4 m. Even at t=0 the velocities, 3 and 0 m/s, violate the derivative constraint. The proposed pair is not a rigid-link history.

(c) Enforce the boundary condition identically.

xB=2+t2,vB=2t,aB=2m/s2\boxed{x_B=2+t^2,\quad v_B=2t,\quad a_B=2\,\mathrm{m/s^2}} xB=2+t2x_B=2+t^2 m is compatible, giving vB=2tv_B=2t m/s and aB=2a_B=2 m/s2^2. Geometric constraints reduce the independent variables before the dynamical equations are solved.