Question: To solve this problem, let's use the condition of rotational equilibrium. The plank will be in equilibrium when the sum of the torques about any
To solve this problem, let's use the condition of rotational equilibrium. The plank will be in equilibrium when the sum of the torques about any point is zero.
Given:
Length of the plank: LmL textm
Mass of the plank: mplankkgmtextplanktextkg
Position of the left support: mtextm from the left end
Position of the right support: mtextm from the left end
Gravitational acceleration: gmsg textms
Let the mass placed at the right end of the plank be maddmtextadd
Step : Find the weight of the plank
The weight of the plank is given by:
WplankmplankgkgmsNWtextplank mtextplanktimes g textkgtimes textmstextN
Step : Calculate the torques
We'll take torques about the left support point located at xmx textm
Torque due to the plank's weight: The weight of the plank acts at its center of mass, which is at mtextmhalf the length of the plank The distance from the left support to the center of mass is mtextm
plankWplankmNmNmcounterclockwisetautextplank Wtextplanktimes textmtextNtimes textmtextNcdot textmquad textcounterclockwise
Torque due to the additional mass: The mass maddmtextadd is placed at the righthand end of the plank, which is mtextm away from the right support. The distance from the left support is mmmtextmtextmtextm
addmaddgmtautextadd mtextaddtimes g times textm
This torque will act clockwise because the mass is located to the right of the support.
Step : Set up the equilibrium condition
For the system to be in equilibrium, the sum of the torques must be zero:
sum tau plankaddtautextplanktautextaddNmmaddmsmtextNcdot textm mtextaddtimes textmstimes textm
Step : Solve for maddmtextadd
madd mtextaddtimes times maddkgmtextaddfractimes fracapprox textkg
Final Answer:
The maximum additional mass that can be placed on the righthand end of the plank is approximately kgboxedtextkg
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