How can the window washer move at constant velocity with unbalanced forces?

In summary, when solving for a pulley problem, it is helpful to set the direction of motion as positive. In this case, there are two forces acting towards the right side and one towards the left. For the man to move at a constant velocity, the net force on him must be zero. The free body diagram for the washer and bucket has three forces: two equal upward tension forces and the weight downward. Since the acceleration is zero, the equation can be simplified to 2T=mg. The direction of the forces does not matter, as long as the net force is zero.
  • #1
ThomasMagnus
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A window washer pulls himself upward using the bucket pulley apparatus shown. How hard must he pull downward to raise himself at a constant speed? The mass of the person and the bucket is 65kg.

My attempt:

When doing pulley problems, I like to set 'moving to the right' as positive. In this case, there are two forces acting toward the right side and one to the left.

The force that the washer pulls with will be equal to the force that the rope applies on the bucket

The forces acting on the bucket: FT-mg=0 (constant acceleration therefore a=0)
Forces acting on the right side: FT=0

Add the two equation together:
2FT=mg
mg=637N
FT=319N


My question is: How can he be moving at constant velocity if there is an unbalanced force acting on the right side? Is it because there is no net force acting on him? (i.e FT-mg=0) If he is moving at constant velocity, can there be a net force on one side of the pulley, but not on another. Or if he is moving at constant velocity, does there have to be a net force of zero on the entire system?


If the sum of the forces acting on the washer and bucket is zero, then is he at rest or is he moving at constant velocity? My guess is if the forces are balance on the bucket, then he will move at constant velocity because of the force he is applying on the other side of the rope (other wise he would be at rest)


Thanks!
 
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  • #2
In order for the man to move at constant velocity the net force on him must be zero. He can't move at a constant velocity if there is an unbalanced force on the right (think about it: the right side of the rope would accelerate but the left side wouldn't? would the rope not rip in this case?). If the man doesn't apply a force to the right side would he accelerate? If so, in which direction?
 
  • #3
Hi ThomasMagnus! :smile:
ThomasMagnus said:
2FT=mg
mg=637N
FT=319N

This is correct, but I have no idea what you mean by forces acting towards the right. :confused:

The free body diagram for washer-and-bucket has only three forces, all vertical: two equal tension forces upward, and the weight downward.

Since the acceleration is zero, 2T = mg.
Or if he is moving at constant velocity, does there have to be a net force of zero on the entire system?

Yes. :smile:
If the sum of the forces acting on the washer and bucket is zero, then is he at rest or is he moving at constant velocity?

Either.
 
  • #4
Where I was getting mixed up is with the coordinate axis. Should I choose any forces that will act in the direction of the acceleration (or in this case motion) to be positive?

Thanks
 
  • #5
Hi ThomasMagnus! :wink:

(just got up :zzz: …)

You can do either … since the acceleration in this case is zero, it doesn't matter. :smile:

(Usually, it's easier to use the direction in which the acceleration is positive, so that your F = ma equation has both sides positive instead of negative! :biggrin:)
 
  • #6
ThomasMagnus said:
The forces acting on the bucket: FT-mg=0 (constant acceleration therefore a=0)
Forces acting on the right side: FT=0

Add the two equation together:
2FT=mg
mg=637N
FT=319N

You first say that FT=0 and then say FT=319N.
This does not make any sense.
Also do you mean upward direction as right?
 

Related to How can the window washer move at constant velocity with unbalanced forces?

1. What are Newton's laws of motion?

Newton's laws of motion are three laws that describe the behavior of objects in motion. The first law, also known as the law of inertia, states that an object will remain at rest or in motion with a constant velocity unless acted upon by an external force. The second law states that the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass. The third law states that for every action, there is an equal and opposite reaction.

2. How do pulleys work?

Pulleys are simple machines that consist of a wheel with a groove and a rope or cable wrapped around it. When a force is applied to one end of the rope, it causes the wheel to rotate, allowing for the lifting or moving of a heavy load. Pulleys allow for the distribution of force over a greater distance, making it easier to lift heavy objects.

3. What is the difference between a fixed and a movable pulley?

A fixed pulley is attached to a stationary object, while a movable pulley is attached to the object being lifted. In a fixed pulley system, the direction of the force applied is changed, making it easier to lift the load. In a movable pulley system, the load is distributed between the pulley and the person pulling on the rope, making it easier to lift larger loads.

4. Can pulleys violate Newton's laws of motion?

No, pulleys do not violate Newton's laws of motion. They simply make use of the laws to distribute force and make work easier. The first law still applies as the object will remain at rest or in motion unless acted upon by an external force. The second law still applies as the net force applied to the object will determine the acceleration. And the third law still applies as the force applied to the rope will result in an equal and opposite reaction from the object being lifted.

5. How are pulleys used in everyday life?

Pulleys are used in a variety of ways in everyday life. Some common examples include elevators, cranes, and exercise equipment. They are also used in simple tasks such as opening and closing blinds, raising and lowering flags, and hoisting a sail on a boat. Pulleys are also used in transportation systems, such as in cars and bicycles, to help distribute force and make movement easier.

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