Some Particular Forces — Question 7

Section 5-6 · Physics pages 724–725

Question 7 Equal tensions in an ideal rope rely on the connector model A straight vertical rope segment is pulled upward at its top with force Tt and downward at its bottom with force Tb. It accelerates upward at 2 m/s2. Take g = 10 m/s2. Tt Tb + mrg Free-body diagram of the selected body; arrow lengths are schematic. (a) For a massless ideal segment, relate the two tensions. (b) For a 0.5 kg segment, find Tt −Tb. (c) If Tb = 20 N in the massive case, find Tt and explain why equality fails.
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Question 7 - Solution Equal tensions in an ideal rope rely on the connector model Tt Tb + mrg (a) Apply the zero-mass idealization. Tt −Tb −mrg = mra, mr = 0 ⇒Tt = Tb Tt −Tb = 0 for the massless segment, hence equal tensions. Its modeled weight is also zero. (b) Include inertia and weight. Tt −Tb = mr(g + a) = 0.5(10 + 2) = 6 N Tt −Tb −mrg = mra gives Tt −Tb = mr(g + a) = 0.5(12) = 6 N. (c) Supply the rope’s own demand. Tt = 20 + 6 = 26 N , 6 = 5 + 1 N Tt = 26 N. The extra 6 N both supports the rope’s 5 N weight and provides its 1 N upward resultant. Equal tension is an ideal-connector result, not an unconditional rule for every rope.

Question 7

Equal tensions in an ideal rope rely on the connector model

A straight vertical rope segment is pulled upward at its top with force TtT_t and downward at its bottom with force TbT_b. It accelerates upward at 2 m/s2^2. Take g=10g=10 m/s2^2.

Diagram shown in the original SVG worksheet.

  1. For a massless ideal segment, relate the two tensions.

  2. For a 0.5 kg segment, find Tt−TbT_t-T_b.

  3. If Tb=20T_b=20 N in the massive case, find TtT_t and explain why equality fails.

Question 7 - Solution

Equal tensions in an ideal rope rely on the connector model

Diagram shown in the original SVG worksheet.

(a) Apply the zero-mass idealization.

Tt−Tb−mrg=mra,mr=0⇒Tt=TbT_t-T_b-m_rg=m_ra,\quad m_r=0\ \Rightarrow\ T_t=T_b Tt−Tb=0T_t-T_b=0 for the massless segment, hence equal tensions. Its modeled weight is also zero.

(b) Include inertia and weight.

Tt−Tb=mr(g+a)=0.5(10+2)=6NT_t-T_b=m_r(g+a)=0.5(10+2)=6\,\mathrm N Tt−Tb−mrg=mraT_t-T_b-m_rg=m_ra gives Tt−Tb=mr(g+a)=0.5(12)=6T_t-T_b=m_r(g+a)=0.5(12)=6 N.

(c) Supply the rope’s own demand.

Tt=20+6=26N,6=5+1N\boxed{T_t=20+6=26\,\mathrm N},\quad6=5+1\quad\mathrm N Tt=26T_t=26 N. The extra 6 N both supports the rope’s 5 N weight and provides its 1 N upward resultant. Equal tension is an ideal-connector result, not an unconditional rule for every rope.