F = ma 2012 #20 (Apparent weight when dunking wood in water)

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Homework Help Overview

The problem involves a container of water on a scale and a block of wood suspended from another scale. The scenario examines the apparent weight readings on both scales when the block of wood is partially submerged in water. The subject area includes concepts of buoyancy, density, and forces acting on objects in fluids.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between buoyancy and apparent weight, questioning how forces interact when the wood is submerged. There are attempts to clarify why buoyancy should be considered in the weight readings and how different scenarios (floating vs. submerged) affect the forces involved.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of buoyancy and weight. Some guidance has been offered regarding the forces acting on the wood and the water, but no consensus has been reached on the implications of these forces for the scale readings.

Contextual Notes

Participants are considering the effects of different configurations of the wood (partially submerged, floating, and fully submerged) on the buoyancy force and the resulting scale readings. There is an emphasis on understanding the principles rather than arriving at a definitive answer.

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Homework Statement


20. A container of water is sitting on a scale. Originally, the scale reads M1 = 45 kg. A block of wood is suspended
from a second scale; originally the scale read M2 = 12 kg. The density of wood is 0.60 g/cm^3; the density of the
water is 1.00 g/cm3
. The block of wood is lowered into the water until half of the block is beneath the surface.
What is the resulting reading on the scales?
45.0 kg ? kg
? kg
12.0 kg
(A) M1 = 45 kg and M2 = 2 kg.
(B) M1 = 45 kg and M2 = 6 kg.
(C) M1 = 45 kg and M2 = 10 kg.
(D) M1 = 55 kg and M2 = 6 kg.
(E) M1 = 55 kg and M2 = 2 kg CORRECT


Homework Equations


F_apparent = F_g - F_b
F_g = mg
F_b = m_fg
F_b = ρ_fV_fg
F_b = ρVg

The Attempt at a Solution


I've heard that one easy approach is to consider that the initial net external forces is the same as the final net external forces. So the only answer that makes sense is E -- which sums to 57. Why is this approach valid?

But my approach was as follows:
Wood:
F_app = 12g - (1000 kg / m^3)(6 kg)(1 m^3 / 600 kg)g
F_app = 2 g
m_app = 2kg

Water:
In this case, the apparent weight should be:
F_app = 45g + that mess up there with the densities
F-app = 55 g
m_app = 55 kg

But why should the buoyancy force be added to the weight?
 
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But why should the buoyancy force be added to the weight?
Every action has an equal and opposite reaction.
Draw the free-body diagram.
 
Ok so we have F_b up and normal force of the scale up. So the scale will read 55kg?
 
The wood experiences the buoyancy force up and gravity down... is all the weight of the wood supported by the buoyancy force?

The water experiences the buoyancy force and gravity down, and the scales up to match.

You've actually answered these questions: I'm going for understanding.
What if the wood were floating in the water instead of being suspended in it?
What if it were pushed under the water so it was completely submerged?
 
If the wood were completely floating in the water; then F_b = 0, if a fraction, then buoyancy force is βmg, where B is the fraction under water.
If the wood were pushed under the water; Fb > Fg, and the difference is the force of the push.
 
Try again.

When an object is floating, it is being supported somehow... otherwise we say it is "sinking". An object floats when this force is equal and opposite the object's weight. It is not going to be zero.

The supporting force depends on the relative density of the object and fluid.
It may float with part sticking out of the water, or, if the relative density is 1, at any depth.

When it is floating, it displaces it's mass of the fluid.
When submerged, it displaces it's volume of fluid.
 

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