Answer to Question #132626 in Mechanics | Relativity for alfraid

Question #132626
a ball of 20 kg moves on a plank of mass 60 kg. find the distance moved by the plank when ball reaches another end of plank.
1
Expert's answer
2020-09-14T10:22:43-0400

Explanations & Calculations





  • Assume the plank is on a frictionless surface & the length of the plank is "\\small L\\,\\,(m)" .

To evaluate this question with respect to the Earth's frame of refence

  • Take the velocity of the ball relative to the plank as "\\small \\overrightarrow { V_1}"
  • Velocity of the plank relative to earth as "\\small \\overleftarrow{V}"
  • Now the velocity of the ball relative to earth is

"\\qquad\\qquad\n\\begin{aligned}\n\\small \\overrightarrow{V_{b,e}}&= \\small\\overrightarrow{ V_{b,p}} +\\overrightarrow{V_{p,e}}\\\\\n&= \\small V_1+ (-V)\\\\\n&= \\small \\overrightarrow{V_1-V}\n\\end{aligned}"

  • By conservation of linear momentum,

"\\qquad\\qquad\n\\begin{aligned}\n\\small 0 &= \\small 20\\times (V_1-V) - 60\\times V\\\\\n\\small \\frac{V_1}{V}&= \\small 4\n\\end{aligned}"

  • Now if the plank moves distance "\\small x", the ball may move "\\small L-x" then,

"\\qquad\\qquad\n\\begin{aligned}\n\\small t = \\frac{x}{V}&= \\small \\frac{L-x}{V_1-V}\\\\\n\\small \\frac{x}{L-x} &= \\small \\frac{V}{V_1-V}= \\frac{1}{3}\\\\\n\\therefore x &= \\small \\bold{\\frac{L}{4}\\,\\,(m)}\n\\end{aligned}"

To evaluate with respect to the plank's frame of reference

  • Consideration of the velocities are the same as above & that of plank's is always the same.
  • By conservation of linear momentum to the right side

"\\qquad\\qquad\n\\begin{aligned}\n\\small 0 &= \\small 20V_1-(20+60)V\\\\\n\\small \\frac{V_1}{V}&= \\small 4\\\\\n\n\\end{aligned}"

  • Now time taken for the ball to reach the other end of the plank (this is relative to the plank) is the same for plank to move a distance of "\\small x_1"
  • Then,

"\\qquad\\qquad\n\\begin{aligned}\n\\small t_1= \\frac{L}{V_1}&= \\small \\frac{x}{V}\\\\\n\\small x &= \\small L\\frac{V}{V_1}=L\\times\\frac{1}{4}\\\\\n&=\\small \\bold{\\frac{L}{4} \\,\\,(m)}\n\\end{aligned}"



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