Some Particular Forces — Question 9

Section 5-6 · Physics pages 728–729

Question 9 Two inclined cords share a load through their vertical components A 6 kg lamp hangs at rest from two identical light cords, each at 30◦above horizontal and directed upward to opposite sides. Take g = 10 m/s2. T T mg Each cord contributes a vertical component; neither generally carries half the weight in tension. (a) Find the tension in each cord. (b) Find tension if each angle becomes 60◦. (c) Explain what happens to the required tension as the cords approach horizontal.
Show solutionHide solution
Question 9 - Solution Two inclined cords share a load through their vertical components T T mg (a) Cancel horizontal components and support weight. 2T sin θ −mg = 0 ⇒ T30 = 60 2 sin 30◦= 60 N 2T sin 30◦= 60 N, so each tension is 60 N. (b) Increase the vertical share. T60 = 60 2 sin 60◦= 20 √ 3 = 34.641 N T = 60/(2 sin 60◦) = 20 √ 3 ≈34.641 N. (c) Examine the small-angle limit. T = mg 2 sin θ, lim θ→0+ T = +∞ T = mg/(2 sin θ) grows without bound as θ →0+. Exactly horizontal cords supply no upward component at finite tension, so they cannot support this nonzero weight in the ideal geometry.

Question 9

Two inclined cords share a load through their vertical components

A 6 kg lamp hangs at rest from two identical light cords, each at 30∘30^\circ above horizontal and directed upward to opposite sides. Take g=10g=10 m/s2^2.

Diagram shown in the original SVG worksheet.

  1. Find the tension in each cord.

  2. Find tension if each angle becomes 60∘60^\circ.

  3. Explain what happens to the required tension as the cords approach horizontal.

Question 9 - Solution

Two inclined cords share a load through their vertical components

Diagram shown in the original SVG worksheet.

(a) Cancel horizontal components and support weight.

2Tsin⁡θ−mg=0⇒T30=602sin⁡30∘=60N2T\sin\theta-mg=0\ \Rightarrow\ \boxed{T_{30}=\frac{60}{2\sin30^\circ}=60\,\mathrm N} 2Tsin⁡30∘=602T\sin30^\circ=60 N, so each tension is 60 N.

(b) Increase the vertical share.

T60=602sin⁡60∘=203=34.641NT_{60}=\frac{60}{2\sin60^\circ}=20\sqrt3=34.641\,\mathrm N T=60/(2sin⁡60∘)=203≈34.641T=60/(2\sin60^\circ)=20\sqrt3\approx34.641 N.

(c) Examine the small-angle limit.

T=mg2sin⁡θ,limθ→0+T=+∞T=\frac{mg}{2\sin\theta},\quad\lim_{\theta\to0^+}T=+\infty T=mg/(2sin⁡θ)T=mg/(2\sin\theta) grows without bound as θ→0+\theta\to0^+. Exactly horizontal cords supply no upward component at finite tension, so they cannot support this nonzero weight in the ideal geometry.