Pulley on Incline: Finding Forces & Tension

  • Thread starter Thread starter Riman643
  • Start date Start date
  • Tags Tags
    Incline Pulley
Click For Summary
SUMMARY

The discussion focuses on calculating forces and tension in a pulley system with a block on an incline. Key calculations include the gravitational force (GA) acting on block A, which is broken down into components: GAx = 68.02 N and GAy = 63.43 N. The normal force (NA) is equal to GAy, resulting in NA = 63.43 N. Frictional forces are calculated using coefficients of static (μsA = 0.40) and kinetic friction (μkA = 0.22), yielding fsA = 25.37 N and fkA = 13.95 N. The tension force (TA) must exceed the sum of the kinetic friction and gravitational forces for block A to move up the ramp.

PREREQUISITES
  • Understanding of free body diagrams (FBDs)
  • Knowledge of gravitational force calculations
  • Familiarity with static and kinetic friction coefficients
  • Basic principles of Newton's laws of motion
NEXT STEPS
  • Study the equations for static and kinetic friction in detail
  • Learn how to construct and analyze free body diagrams for complex systems
  • Explore the relationship between tension and acceleration in pulley systems
  • Investigate the effects of different angles of incline on force calculations
USEFUL FOR

Students studying physics, particularly those focusing on mechanics, as well as educators and tutors looking to clarify concepts related to forces in pulley systems and inclined planes.

Riman643
Messages
62
Reaction score
2
Homework Statement
Body A in the figure weighs 93 N, and body B weighs 57 N. The coefficients of friction between A and the incline are μs = 0.40 and μk = 0.22. Angle θ is 47°. Let the
positive direction of an x axis be up the incline. What is the acceleration of A if A is initially (a) at rest, (b) moving up the incline, and (c) moving down the incline?
Relevant Equations
fs = Nμs
fk = Nμk
F = ma
a) I figured this part out. Because A is at rest that means the acceleration is 0

b&c) I am completely lost how to go about this. I drew a free body diagram for A and I was able to determine 4 forces acting on it.

1: The Gravitational force on A (GA). Using the angle (θ), and the incline as my x-axis I was able to determine
GAx = GAsin(θ) = 93sin(47) = 68.02 N
GAy = GAcos(θ) = 93cos(47) = 63.43 N

2: The Normal force on A (NA). This is equal to GAy.
NA = GAy = 63.43 N

3: The static and kinectic frictional forces on A (fsA, fkA). I found these using the static and kinetic friction coefficients (μsA, μkA) and the Normal force.
fsA = NAμsA = 0.40(63.43) = 25.37 N
fkA = NAμkA = 0.22(63.43) = 13.95 N

4: The Tension force on A (TA). It is very tempting to say that it is equal to weight of B, but for the forces to be at rest or for A to move up the ramp TA would have to be much greater.

I really need help in 1) Finding TA and 2) Figuring out how the two frictional forces play a role in this. Since A would already be moving in either direction I feel like I would need to use kinetic friction somehow, but then, what would the point of including static friction in the problem? Any help/tips would be greatly appreciated.
 

Attachments

  • img1352880023991_5362570821946429.gif
    img1352880023991_5362570821946429.gif
    3.8 KB · Views: 293
Physics news on Phys.org
Riman643 said:
Because A is at rest
It is initially at rest. It is not guaranteed to remain at rest.
Riman643 said:
fs = Nμs
That is not generally true. What is the correct version?
Riman643 said:
very tempting to say that it is equal to weight of B, but for the forces to be at rest or for A to move up the ramp TA would have to be much greater.
Don't confuse motion with acceleration.
 
Thanks for the reply but I am still lost. I got part “a” of this problem right. I know the acceleration is the net force of the block in one direction divided by the mass of A. What I am having trouble determining is how to calculate the net force. Going up the ramp the net force would have to be greater than the static force and gravitational force in the x direction. But if it’s moving I would also have to factor in the kinetic friction force right? I’m just confused on how to tie it all together.
 
Riman643 said:
I got part “a” of this problem right.
You got the right answer by chance; the reasoning is wrong.

First step is to decide whether static friction is enough to prevent motion. For that, you need to get your standard equation for static friction right. Can you see what is wrong with the equation you quoted? Hint: it's the bit in the middle.

For parts b and c you are given that the block is moving initially, so static friction is irrelevant.
 
  • Like
Likes   Reactions: Riman643
haruspex said:
You got the right answer by chance; the reasoning is wrong.

Could you explain how? If the object is at rest or at a constant velocity that would mean the acceleration is zero, right?

haruspex said:
First step is to decide whether static friction is enough to prevent motion. For that, you need to get your standard equation for static friction right. Can you see what is wrong with the equation you quoted?

Would it be that fsA <= NAμsA?

haruspex said:
For parts b and c you are given that the block is moving initially, so static friction is irrelevant.

Okay so that would mean if the block is moving up the ramp (along the x - axis in the free body diagram) that the net force would have to be greater than the kinetic friction and the gravitational force in the x direction.
So:
TA > fkA + GAx
 
Last edited:
Riman643 said:
If the object is at rest or at a constant velocity that would mean the acceleration is zero, right?
Yes, but you are not told it remains at rest. You are told it is initially stationary; it could immediately accelerate. A stone thrown straight up is instantaneously at rest at the top of its flight, but it accelerates down at g all the while.
Riman643 said:
Would it be that fsA <= NAμsA?
Yes.
Riman643 said:
Okay so that would mean if the block is moving up the ramp (along the x - axis in the free body diagram) that the net force would have to be greater than the kinetic friction and the gravitational force in the x direction.
No. As I posted you are confusing motion with acceleration. Consider the stone again. When you throw it up it moves up, but the acceleration is down.
 
haruspex said:
No. As I posted you are confusing motion with acceleration. Consider the stone again. When you throw it up it moves up, but the acceleration is down.

So would that mean that the acceleration when it is moving up or down the ramp would be the same? And how would I figure this out? I tried subtracting the Tension force from the sum kinetic friction force and gravitational force in the x direction and found the difference to be 2.99 N. I then divided this force by the mass to give me the acceleration but it was wrong.
 
Riman643 said:
So would that mean that the acceleration when it is moving up or down the ramp would be the same?
Only if all the forces are the same in the two cases, in magnitude and direction. Would they be?
Riman643 said:
tried subtracting the Tension force from the sum kinetic friction force and gravitational force in the x direction and found the difference to be 2.99 N
You don't know the tension yet, so you can't do that.
There are two masses, undergoing the same magnitude of acceleration and subject to opposite ends of the same tension. You need a FBD for each.
 
haruspex said:
Only if all the forces are the same in the two cases, in magnitude and direction. Would they be?

Yes? I have no idea at this point.
 
  • #10
Riman643 said:
Yes? I have no idea at this point.
Think about the kinetic friction force direction.
 
  • Like
Likes   Reactions: Riman643
  • #11
Thanks! I was able to solve it. Just had to step back and think about a little.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
886
  • · Replies 10 ·
Replies
10
Views
5K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
19
Views
4K
  • · Replies 9 ·
Replies
9
Views
3K
Replies
18
Views
2K
Replies
2
Views
2K
  • · Replies 36 ·
2
Replies
36
Views
6K
Replies
8
Views
3K