Applying Newton's Laws — Question 2

Section 5-8 · Physics pages 754–755

Question 2 A table block and hanging mass have different force inventories Take g = 10 m/s2. A 4 kg block lies on a frictionless horizontal table. A light cord runs from it over an ideal fixed edge pulley to a hanging 1 kg mass. The cord is taut. 4 kg 1 kg The cord changes direction at the ideal edge guide; its tension magnitude is shared. (a) Find their common acceleration magnitude and the tension. (b) Find the table’s normal force on the block. (c) If both start from rest, find the time for the hanging mass to descend 0.4 m.
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Question 2 - Solution A table block and hanging mass have different force inventories 4 kg 1 kg (a) Couple the separate body equations. T = 4a, 10 −T = a ⇒ a = 2 m/s2, T = 8 N The table block obeys T = 4a. The hanging mass obeys 10 −T = a. Hence a = 2 m/s2 and T = 8 N. (b) Keep the table block’s vertical constraint. ∑ Fy = N −4g = 0 ⇒N = 40 N The cord is horizontal at the block, so N = 4g = 40 N. This normal does not enter the horizontal acceleration equation. (c) Use the available travel interval. 0.4 = 1 2at2 ⇒t = √ 2(0.4) 2 = 0.6325 s 0.4 = 1 2(2)t2, hence t = √ 0.4 ≈0.6325 s, provided neither body hits a stop before that descent.

Question 2

A table block and hanging mass have different force inventories

Take g=10g=10 m/s2^2. A 4 kg block lies on a frictionless horizontal table. A light cord runs from it over an ideal fixed edge pulley to a hanging 1 kg mass. The cord is taut.

Diagram shown in the original SVG worksheet.

  1. Find their common acceleration magnitude and the tension.

  2. Find the table’s normal force on the block.

  3. If both start from rest, find the time for the hanging mass to descend 0.4 m.

Question 2 - Solution

A table block and hanging mass have different force inventories

Diagram shown in the original SVG worksheet.

(a) Couple the separate body equations.

T=4a,10−T=a⇒a=2m/s2,T=8NT=4a,\quad10-T=a\ \Rightarrow\ \boxed{a=2\,\mathrm{m/s^2},\quad T=8\,\mathrm N} The table block obeys T=4aT=4a. The hanging mass obeys 10−T=a10-T=a. Hence a=2a=2 m/s2^2 and T=8T=8 N.

(b) Keep the table block’s vertical constraint.

∑Fy=N−4g=0⇒N=40N\sum F_y=N-4g=0\ \Rightarrow\ N=40\,\mathrm N The cord is horizontal at the block, so N=4g=40N=4g=40 N. This normal does not enter the horizontal acceleration equation.

(c) Use the available travel interval.

0.4=12at2⇒t=2(0.4)2=0.6325s0.4=\tfrac12at^2\ \Rightarrow\ t=\sqrt{\frac{2(0.4)}2}=0.6325\,\mathrm s 0.4=12(2)t20.4=\tfrac12(2)t^2, hence t=0.4≈0.6325t=\sqrt{0.4}\approx0.6325 s, provided neither body hits a stop before that descent.