Where Will the Center of Gravity of the Wooden Plank Be?

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SUMMARY

The discussion focuses on determining the position of the center of gravity (C.G.) of a 1-meter wooden plank partially submerged in water. The equilibrium condition is established by equating the moments of the buoyancy force and the weight about the point of contact with the stone. The analysis reveals that if more than 50 cm of the plank is submerged, the center of gravity lies within the water; otherwise, it remains outside. Key calculations involve the mass of the plank (70 g) and the buoyancy force proportional to the submerged length (x cm).

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Homework Statement


A thin wooden plank 1m long is kept on the protruding stone with some of its part immersed in water.
Will the centre of gravity of the wooden plank be inside the water or outside?

Homework Equations


The Attempt at a Solution



For the wooden plank to be in equilibrium, moments of buoyancy force and weight about the point of contact of stone should be equal.
Buoyancy force acts at the midpoint of the immersed part.
But what will be the position of the centre of mass (gravity) of the plank?
 

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How long is the rod?
 
1 metre
 
The position of the centre of mass (gravity) of the plank is the mid point of the plank.
 
rl.bhat said:
The position of the centre of mass (gravity) of the plank is the mid point of the plank.

then does it mean the torque on both side is equal?
 
rl.bhat said:
The position of the centre of mass (gravity) of the plank is the mid point of the plank.

What I asked was whether it will should lie inside the water or outside to get balanced?
 
Assume that x-axis is oriented along the thin plank and area of cross section of the plank 1 cm^2.
Density of wood = 0.7 g/cm^3 and that of water = 1 g/cm^3
Let x cm be the portion of the plank in the water.
Length of the plank is 100 cm. So the mass of the plank = 70 g.
Mass of the displaced water = x g. Then buoyancy force is proportional to x.

If R is the reaction of the stone, R = (70 - x)
Take the moment about the end of the plank out side the water.

R*10 + x(100 - x/2) = 70*50

Solve the quadratic. If x is more than 50, C.G. is inside the water. Otherwise it is outside the water.
 
How did you get R = 70-x ?
 
I have assumed that the component of the weight of the plank perpendicular to x-axis is

L*d*g*cosθ. Length of the plank is 100 cm, density 0.7 g/cm^3

Component of the weight of the displaced liquid = x*1*g*cosθ

For equilibrium, total downward with respect x-axis must be equal to the total upward force. Weight is in the downward direction and buoyancy and the reaction are in the upward direction.
Hence R*g*cosθ = 70*g*cosθ - x*g*cosθ
 
Last edited:
  • #10
Thanks!
 

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