Friction - 3 Blocks and a Pulley

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The discussion revolves around the dynamics of two blocks connected by static friction and the calculations of forces acting on them. Initially, the poster incorrectly calculated the force of static friction on Block 1 as dependent solely on the normal force from Block 2, leading to confusion about the acceleration and net forces. After clarification, it was established that the force of static friction can vary up to a maximum value, and when an external force is applied, it adjusts accordingly to prevent motion until its limit is reached. The correct application of Newton's Second Law reveals that the force of static friction on Block 1 is equal to the product of its mass and acceleration. Ultimately, the poster realized their earlier miscalculations and corrected their understanding of static friction's role in the system.
FredericChopin
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Homework Statement


http://imgur.com/C0XYEKw

Homework Equations


Fnet = m*a
FG = m*g
fstatic = μ*N

The Attempt at a Solution


If both Block 1 and Block 2 have acceleration a in the x-direction and have an acceleration of 0 in the y-direction, then the force of static friction on Block 1 due to Block 2 doesn't seem to depend at all on what Block 2 is doing. This is because the normal force on Block 1 due to Block 2 is still the same as it is at rest and the force of static friction on Block 1 due to Block 2 is the only force acting in the x-direction on Block 1.

I tried this by considering only Block 1 as a system.

In the y-direction, the forces acting on Block 1 are the normal force on Block 1 due to Block 2, N12, and the gravitational force on Block 1 due to the Earth, F1E. The acceleration, ay, is equal to 0.

Thus:

Σ Fnet,y = 0 = N12 - F1E = N12 - m1*g

Thus:

N12 = m1*g

In the x-direction, the only force acting on Block 1 is the force of static friction, which is acting in the right, positive x-direction. The acceleration, ax, is equal to a.

Thus:

Σ Fnet, x = m1*a = fstatic = μ*N12 = μ*m1*g

Thus the force and direction of the force of static friction on Block 1 due to Block 2 is:

fstatic = μ*m1*g

This, however, is the wrong answer.

I don't understand why though. Where am I going wrong?

Thank you.
 
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FredericChopin said:

Homework Statement


http://imgur.com/C0XYEKw

Homework Equations


Fnet = m*a
FG = m*g
fstatic = μ*N

The Attempt at a Solution


If both Block 1 and Block 2 have acceleration a in the x-direction and have an acceleration of 0 in the y-direction, then the force of static friction on Block 1 due to Block 2 doesn't seem to depend at all on what Block 2 is doing. This is because the normal force on Block 1 due to Block 2 is still the same as it is at rest and the force of static friction on Block 1 due to Block 2 is the only force acting in the x-direction on Block 1.

I tried this by considering only Block 1 as a system.

In the y-direction, the forces acting on Block 1 are the normal force on Block 1 due to Block 2, N12, and the gravitational force on Block 1 due to the Earth, F1E. The acceleration, ay, is equal to 0.

Thus:

Σ Fnet,y = 0 = N12 - F1E = N12 - m1*g

Thus:

N12 = m1*g

In the x-direction, the only force acting on Block 1 is the force of static friction, which is acting in the right, positive x-direction. The acceleration, ax, is equal to a.

Thus:

Σ Fnet, x = m1*a = fstatic = μ*N12 = μ*m1*g

Thus the force and direction of the force of static friction on Block 1 due to Block 2 is:

fstatic = μ*m1*g

This, however, is the wrong answer.

I don't understand why though. Where am I going wrong?

Thank you.

What is the difference between kinetic and static friction?
Imagine that you have a block in rest on a table. The mass of the block is 2 kg, the coefficient of static friction is μs=0.5.

You push the block with force F=1N force. Will the block move? What is the force of friction?
You push the block with F=9 N force. Will the block move? What is the force of friction now?
 
O.K., I realized I grossly overcomplicated things.

Since the force of static friction on Block 1 due to Block 2 is the only force in the x-direction acting on Block 1, and Block 1 has acceleration a, then Newton's Second Law states that:

∑ Fx = m1*a = fs12

Thus, the force of static friction on Block 1 due to Block 2 is:

fs12 = m1*a

EDIT: Responding to your original question, the force of static friction can take on any value up to a maximum value of μ*m1*g. So, when an applied force of 1 N is acting on Block 1, the force of static friction is 1 N in the opposite direction. As a result, the net force is 0 N and Block 1 does not move. If an applied force of 9 N is acting on Block 1, the force of static friction is at its maximum 9 N (if g = 10 m/s2) in the opposite direction. As a result, Block 1 travels at a constant velocity in the direction of applied force.
 
Last edited:
FredericChopin said:
O.K., I realized I grossly overcomplicated things.

Since the force of static friction on Block 1 due to Block 2 is the only force in the x-direction acting on Block 1, and Block 1 has acceleration a, then Newton's Second Law states that:

∑ Fx = m1*a = fs12

Thus, the force of static friction on Block 1 due to Block 2 is:

fs12 = m1*a
That is correct now.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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