Applying Newton's Laws — Question 6

Section 5-8 · Physics pages 762–763

Question 6 An elevator’s acceleration changes tensions through a hanging chain Take g = 10 m/s2. Two masses, 2 kg above and 3 kg below, hang in series from an elevator ceiling by light cords. The elevator accelerates upward at 1 m/s2; both masses stay fixed relative to it. Tu 2 kg Tl 3 kg The upper cord carries the demands of both masses; the lower cord carries only the lower one. (a) Find the lower cord tension. (b) Find the upper cord tension. (c) Find both tensions if the elevator instead descends at constant velocity.
Show solutionHide solution
Question 6 - Solution An elevator’s acceleration changes tensions through a hanging chain Tu 2 kg Tl 3 kg (a) Isolate the lower mass. Tl −3g = 3a ⇒ Tl = 3(10 + 1) = 33 N Tl −30 = 3(1) gives Tl = 33 N. (b) Support and accelerate both masses. Tu −(2 + 3)g = (2 + 3)a ⇒Tu = 5(11) = 55 N Tu −50 = 5(1) gives Tu = 55 N. Equivalently, the upper mass obeys Tu −Tl −20 = 2(1). (c) Use acceleration rather than travel direction. a = 0 : Tl = 3g = 30 N, Tu = 5g = 50 N Constant velocity means zero acceleration, so Tl = 30 N and Tu = 50 N. Downward motion alone does not reduce the load.

Question 6

An elevator’s acceleration changes tensions through a hanging chain

Take g=10g=10 m/s2^2. Two masses, 2 kg above and 3 kg below, hang in series from an elevator ceiling by light cords. The elevator accelerates upward at 1 m/s2^2; both masses stay fixed relative to it.

Diagram shown in the original SVG worksheet.

  1. Find the lower cord tension.

  2. Find the upper cord tension.

  3. Find both tensions if the elevator instead descends at constant velocity.

Question 6 - Solution

An elevator’s acceleration changes tensions through a hanging chain

Diagram shown in the original SVG worksheet.

(a) Isolate the lower mass.

Tl−3g=3a⇒Tl=3(10+1)=33NT_l-3g=3a\ \Rightarrow\ \boxed{T_l=3(10+1)=33\,\mathrm N} Tl−30=3(1)T_l-30=3(1) gives Tl=33T_l=33 N.

(b) Support and accelerate both masses.

Tu−(2+3)g=(2+3)a⇒Tu=5(11)=55NT_u-(2+3)g=(2+3)a\ \Rightarrow\ T_u=5(11)=55\,\mathrm N Tu−50=5(1)T_u-50=5(1) gives Tu=55T_u=55 N. Equivalently, the upper mass obeys Tu−Tl−20=2(1)T_u-T_l-20=2(1).

(c) Use acceleration rather than travel direction.

a=0:Tl=3g=30N,Tu=5g=50Na=0:\quad T_l=3g=30\,\mathrm N,\quad T_u=5g=50\,\mathrm N Constant velocity means zero acceleration, so Tl=30T_l=30 N and Tu=50T_u=50 N. Downward motion alone does not reduce the load.