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

AI Thread Summary
The discussion centers on determining the position of the center of gravity of a 1-meter wooden plank partially submerged in water. For the plank to be in equilibrium, the moments of the buoyancy force and the weight must balance around the point of contact with the stone. The center of mass of the plank is at its midpoint, and the buoyancy force acts at the midpoint of the submerged portion. By analyzing the forces and moments, it is concluded that if more than 50 cm of the plank is submerged, the center of gravity will be inside the water; otherwise, it will be outside. The calculations involve the density of the wood and water, leading to a quadratic equation to find the submerged length.
zorro
Messages
1,378
Reaction score
0

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?
 

Attachments

  • rod.jpg
    rod.jpg
    3.2 KB · Views: 491
Last edited:
Physics news on Phys.org
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!
 
Back
Top