Some Particular Forces — Question 6

Section 5-6 · Physics pages 722–723

Question 6 An ideal taut cord pulls along its own line A 3 kg mass hangs from a light taut cord. The mass accelerates upward at 2 m/s2. Take g = 10 m/s2. T mg Free-body diagram of the selected body; arrow lengths are schematic. (a) Find the tension. (b) Find tension for downward acceleration of 2 m/s2. (c) Can the same cord provide a downward force if the mass requires one?
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Question 6 - Solution An ideal taut cord pulls along its own line T mg (a) Balance force difference with inertia. T −mg = may ⇒ T = 3(10 + 2) = 36 N T −mg = ma gives T = 3(10 + 2) = 36 N. (b) Reverse acceleration, not the tension direction. T = 3(10 −2) = 24 N, T −mg = −6 N T = 3(10 −2) = 24 N. The tension still pulls upward even though the net force is downward. (c) Use the unilateral nature of a cord. T ≥0 ⇒ay ≥−g for this taut-cord inventory An ordinary flexible cord under tension pulls; it does not push the hanging mass downward. If the equations require negative tension, the assumed taut configuration fails and a slack-cord or additional-interaction model is needed.

Question 6

An ideal taut cord pulls along its own line

A 3 kg mass hangs from a light taut cord. The mass accelerates upward at 2 m/s2^2. Take g=10g=10 m/s2^2.

Diagram shown in the original SVG worksheet.

  1. Find the tension.

  2. Find tension for downward acceleration of 2 m/s2^2.

  3. Can the same cord provide a downward force if the mass requires one?

Question 6 - Solution

An ideal taut cord pulls along its own line

Diagram shown in the original SVG worksheet.

(a) Balance force difference with inertia.

T−mg=may⇒T=3(10+2)=36NT-mg=ma_y\ \Rightarrow\ \boxed{T=3(10+2)=36\,\mathrm N} T−mg=maT-mg=ma gives T=3(10+2)=36T=3(10+2)=36 N.

(b) Reverse acceleration, not the tension direction.

T=3(10−2)=24N,T−mg=−6NT=3(10-2)=24\,\mathrm N,\quad T-mg=-6\,\mathrm N T=3(10−2)=24T=3(10-2)=24 N. The tension still pulls upward even though the net force is downward.

(c) Use the unilateral nature of a cord.

T≥0⇒ay≥−gfor this taut-cord inventoryT\ge0\ \Rightarrow\ a_y\ge-g\quad\text{for this taut-cord inventory} An ordinary flexible cord under tension pulls; it does not push the hanging mass downward. If the equations require negative tension, the assumed taut configuration fails and a slack-cord or additional-interaction model is needed.