Applying Newton's Laws — Question 5

Section 5-8 · Physics pages 760–761

Question 5 Contact can transmit a push but cannot keep blocks together under a pull Blocks A and B of masses 2 and 3 kg touch on a frictionless line, A left of B. Initially at rest, A is pushed right with 10 N. In a separate trial A is pulled left with 10 N; there is no connector. A B push The side-by-side blocks have no tensile connector. (a) Find acceleration and contact force in the push trial. (b) Test a common-acceleration assumption in the pull trial. (c) Give the actual accelerations immediately after the pull begins.
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Question 5 - Solution Contact can transmit a push but cannot keep blocks together under a pull A B push (a) Use the joined motion while contact is compressive. 10 = (2 + 3)a ⇒ a = 2 m/s2, C = 3a = 6 N The common acceleration is 10/5 = 2 m/s2. The force on B is 3(2) = 6 N rightward, supplied by A’s push. (b) Check whether contact would have to pull. aassumed = −10/5 = −2, Crequired = 3(−2) = −6 N < 0 Common acceleration would be -2 m/s2, requiring -6 N on B from A. Ordinary side contact cannot pull B left, so this constraint is inadmissible. (c) Release the failed contact. C = 0 : aA = −10/2 = −5 m/s2, aB = 0 The blocks separate. A accelerates at −10/2 = −5 m/s2, B at zero, and contact force is zero. The common-acceleration model works only while a compressive contact exists.

Question 5

Contact can transmit a push but cannot keep blocks together under a pull

Blocks A and B of masses 2 and 3 kg touch on a frictionless line, A left of B. Initially at rest, A is pushed right with 10 N. In a separate trial A is pulled left with 10 N; there is no connector.

Diagram shown in the original SVG worksheet.

  1. Find acceleration and contact force in the push trial.

  2. Test a common-acceleration assumption in the pull trial.

  3. Give the actual accelerations immediately after the pull begins.

Question 5 - Solution

Contact can transmit a push but cannot keep blocks together under a pull

Diagram shown in the original SVG worksheet.

(a) Use the joined motion while contact is compressive.

10=(2+3)a⇒a=2m/s2,C=3a=6N10=(2+3)a\ \Rightarrow\ \boxed{a=2\,\mathrm{m/s^2},\quad C=3a=6\,\mathrm N} The common acceleration is 10/5=210/5=2 m/s2^2. The force on B is 3(2)=63(2)=6 N rightward, supplied by A’s push.

(b) Check whether contact would have to pull.

aassumed=−10/5=−2,Crequired=3(−2)=−6N<0a_{\mathrm{assumed}}=-10/5=-2,\quad C_{\mathrm{required}}=3(-2)=-6\,\mathrm N<0 Common acceleration would be -2 m/s2^2, requiring -6 N on B from A. Ordinary side contact cannot pull B left, so this constraint is inadmissible.

(c) Release the failed contact.

C=0:aA=−10/2=−5m/s2,aB=0C=0:\quad a_A=-10/2=-5\,\mathrm{m/s^2},\quad a_B=0 The blocks separate. A accelerates at −10/2=−5-10/2=-5 m/s2^2, B at zero, and contact force is zero. The common-acceleration model works only while a compressive contact exists.