Coefficients of kinetic and static friction in a pulley

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SUMMARY

The discussion centers on calculating the coefficients of static and kinetic friction for a block (M1 = 5.00 kg) on a 30-degree inclined plane, connected to a variable mass (M2). When M2 is 3.20 kg, M1 begins to slide up the slope with an acceleration of 0.20 m/s². The coefficient of static friction is determined to be approximately 0.162, while the coefficient of kinetic friction is calculated to be around 0.123. The calculations involve resolving forces and applying Newton's second law to both masses in the system.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Knowledge of static and kinetic friction coefficients
  • Ability to resolve forces on inclined planes
  • Familiarity with basic algebra and trigonometry
NEXT STEPS
  • Study the derivation of friction coefficients in different scenarios
  • Learn about the dynamics of pulleys and tension in connected systems
  • Explore advanced applications of Newton's laws in multi-body systems
  • Investigate the effects of varying mass on friction and motion
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Students in physics, particularly those studying mechanics, as well as educators and anyone interested in understanding the principles of friction on inclined planes and pulley systems.

marsupial
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Homework Statement


A block of mass ## M_1 ## is on an inclined plane (the plane is inclined at 30 degrees), and is attached with a light cord over a light, frictionless pulley to another mass ## M_2 ##. ## M_1 ## is fixed at 5.00kg, and ## M_2 ## can be varied.

When ## M_2 = 3.20 kg ##, ## M_1 ## just begins to slide up the slope, acclerating at ## 0.20 m/s^2 ##.

Determine the coefficients of static and kinetic friction between ## M_1 ## and the plane.

Homework Equations


## F_{fr_static} = \mu (static) F_N ##
## F_{fr_kinetic} = \mu (kinetic) F_N ##
F = ma

The Attempt at a Solution


After resolving the components of mg into x, and y: ## F_N = y = 5.00gCos30 = 42.435244 N ##
The component of mg in the x direction: mgsin30 = 24.5N

To determine the coefficient of static friction, there must be no net horizontal force. I am not sure of this, but I am wondering if I just ignore the pulley and the mass at the end to calculate the static friction coefficient? But then that assumes that it will sit on the plane without sliding down, and I am not sure if I should make that assumption.

If I did make that assumption, and ignored the pulley for the moment, then:
## F_{fr} - 5.00gsin30 = 0 --> \mu F_N = 24.5 --> \mu (static) = 24.5/42.43 = 0.577 ##

To determine the coefficient of kinetic friction:
## net F_x = 3.20 * 0.20 ##
## F_{tension} - F_{fr_kinetic} - F_{mg-xcomponent} = 3.20 * 0.2 ##
## F_{tension} = 3.20g ##
## F_{fr_kinetic} = (F_{tension} - F_{mg-xcomponent})/ (3.20 * 0.2) ##
## F_{fr_kinetic} = (3.20g - 24.5)/ (3.20 * 0.2) = 10.71875 ##
## \mu (kinetic) = F_{fr_kinetic} / F_N = 10.71875/ 42.435244 = 0.253 ##

I'm not sure in particular about the coefficient of static friction.
 
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I don't think you can assume the tension is 3.20 x g.
The tension in the rope reduces when the system accelerates.
Analyze the motion of M2 to determine the tension in the rope.
 
## mg - F_{tension} = 0.20 * 3.2 --> F_{tension} = 3.2g - 0.64 = 30.72 ##

Is this right? Also, was I right in my assumptions with the static friction coefficient?
 
marsupial said:
## mg - F_{tension} = 0.20 * 3.2 --> F_{tension} = 3.2g - 0.64 = 30.72 ## Is this right ?

Correct .

marsupial said:
Also, was I right in my assumptions with the static friction coefficient?

No . You cannot ignore the mass at the end . You also need to take tension into account .

Have you copied the question correctly ? I am finding the data inconsistent . I might be wrong but it would be nice if you could check the question .
 
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Vibhor, the question is correct
 
Ok . Let us first deal with static friction case .

What are the forces acting on M1 along the plane ? What would be the direction of static friction ? Can you resolve the forces along the inclined plane and use Newton's II Law ? Please use symbols . Do not put any numbers .
 
Regarding taking the tension into account, given the mass is variable, and that it begins to move at 3.20kg, then ## F_{tension} < 3.2g ##. That seems an imprecise way of expressing it.

Just saw your follow-up post Vibhor.

## F_{tension} + F_{fr-static} - F_{mg-x} = 0 ##
## m_2 g + \mu m_1 g cos30 - m_1 g sin 30 = 0 ##
## \mu = (m_1 g sin30 - m_2g) / m_1 g cos30 ##
## \mu = tan30 - (m_2/m_1cos30) ##

But I don't know what to do about m_2 as it is varied, and all I think we can say about the max mass before it moves is that it is less than 3.2. But how much less? 3.1, 3.1999?
 
Forget about M2 being variable . Think that when M2 = 3.2 Kg M1 just starts moving up the slope . In other words , When M2 =3.2 Kg , M1 and M2 are as good as not moving . You can treat them as in equilibrium . But once M1 and M2 start moving , things change ( we will deal with it later in kinetic friction case). They will no more be in equilibrium .

So for the case of static friction , consider M1 and M2 to be in equilibrium and apply Newton's II law .

Just write the equation in terms of symbols T , M1 , M2 , g , θ , μs .
 
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Like I did? (albeit with 30 instead of theta and m2 g instead of T)
 
  • #10
marsupial said:
Like I did? (albeit with 30 instead of theta and m2 g instead of T)

What would be the direction of friction ?
 
  • #11
I thought it would be in the same direction as ## F_T ##, given it is opposing the x component of mg
 
  • #12
marsupial said:
I thought it would be in the same direction as ## F_T ##, given it is opposing the x component of mg

Static friction acts so as to oppose the (potential) relative motion between the surfaces in contact . If there were no friction between M1 and the plane , in which direction would M1 be moving , up the slope or down the slope ?
 
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  • #13
That would depend on the mass of M2 wouldn't it? M2 at 3.2, and it moves up the slope (so in this case friction would go in the direction of mg_x). I am not sure if it would in any instance slide down the slope.
 
  • #14
marsupial said:
That would depend on the mass of M2 wouldn't it? M2 at 3.2, and it moves up the slope (so in this case friction would go in the direction of mg_x). I am not sure if it would in any instance slide down the slope.

What is mg_x ? I do not understand the notation .
 
  • #15
It is the x component of m1 * g
 
  • #16
marsupial said:
It is the x component of m1 * g

And what is the x direction :smile: ?
 
  • #17
the horizontal of the incline. The direction of the x component of mg is down the incline.
 
  • #18
Ok . So now do you see what is the error in post#7 ?
 
  • #19
Sure, it should be: ## F_T - F_{fr-static} - F_{x-mg} = 0 ##

## m_2 g - \mu m_1 g cos30 - m_1 g sin 30 = 0 ##
## \mu = (m_2 g - m_1 gsin30)/ m_1 g cos30 ##
## \mu = (m_2/m_1cos30) - tan30 ##
## \mu = 3.2/(5cos30) - tan30 = 0.162 ##

Is the rest okay?
 
  • #20
marsupial said:
Sure, it should be: ## F_T - F_{fr-static} - F_{x-mg} = 0 ##

## m_2 g - \mu m_1 g cos30 - m_1 g sin 30 = 0 ##
## \mu = (m_2 g - m_1 gsin30)/ m_1 g cos30 ##
## \mu = (m_2/m_1cos30) - tan30 ##
## \mu = 3.2/(5cos30) - tan30 = 0.162 ##

Correct .

marsupial said:
Is the rest okay?
"rest" what ?
 
  • #21
The way I worked out the kinetic coefficient above.
 
  • #22
marsupial said:
The way I worked out the kinetic coefficient above.

It is incorrect . Once the masses start moving tension is not equal to M2g .
 
  • #23
I know, I meant the process. Recalculated with the tension taking into account
## F_{tension} =3.2g−0.64 ##, ## \mu = 0.229 ##
 
  • #24
marsupial said:
I know, I meant the process. Recalculated with the tension taking into account
## F_{tension} =3.2g−0.64 ##, ## \mu = 0.229 ##

Tension is correct but I get a different value of ## \mu ## . As a sanity check , coefficient of static friction is greater than coefficient of kinetic friction i.e ##μ_s≥μ_k ##

marsupial said:
## net F_x = 3.20 * 0.20 ##
## F_{tension} - F_{fr_kinetic} - F_{mg-xcomponent} = 3.20 * 0.2 ##
## F_{tension} = 3.20g ##
## F_{fr_kinetic} = (F_{tension} - F_{mg-xcomponent})/ (3.20 * 0.2) ##
## F_{fr_kinetic} = (3.20g - 24.5)/ (3.20 * 0.2) = 10.71875 ##
## \mu (kinetic) = F_{fr_kinetic} / F_N = 10.71875/ 42.435244 = 0.253 ##

Wrong . I know you have replaced value of tension from 31.36 to 30.72 . But It is still wrong . Not only is equation wrong but you have also made algebra mistakes . How has ##(3.20 * 0.2)## slipped into the denominator :rolleyes: ?

Please use Newton's II law separately for the two masses . Work with symbols . Do not plug numbers too soon . You might not require value of tension at all in your final calculation :smile: .
 
Last edited:
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  • #25
Vibhor said:
Wrong . I know you have replaced value of tension from 31.36 to 30.72 . But It is still wrong . Not only is equation wrong but you have also made algebra mistakes . How has ##(3.20 * 0.2)## slipped into the denominator :rolleyes: ?

Just noticed that! Note to self, don't do physics when you're really tired!

## F_T - F_{fr} - F_{mg-x} = m_2 a ##
## m_2 g - F_T = m_2 a --> F_T = m_2 g - m_2 a ##
## F_{fr} = F_T - F_{mg-x} - m_2 a ##
## F_{fr} = m_2 g - 2 (m_2 a) - m_1 gsin30 ##
## \mu = F_{fr} / F_N ##
## \mu = (m_2 g - 2 (m_2 a) - m_1 gsin30 )/ m_1 gcos30 ##
## \mu = (3.2g - 2(3.2 * 0.2) - 5gsin30) / 5gcos30 = (31.36 - 1.28 - 24.5) / 42.4352 = 0.131 ##

Is that better?
 
  • #26
marsupial said:
Just noticed that! Note to self, don't do physics when you're really tired!
True
marsupial said:
## F_T - F_{fr} - F_{mg-x} = m_2 a ##

Why ##m_2## ?
 
  • #27
lol, I meant m1. Fatigue again. Nearly 1am after a long day. So, that would make it

## F_{fr} = m_2 g - m_2 a - m_1 a - m_1 gsin30 ##
...
## \mu = (3.2g - (3.2 * 0.2) - (5*0.2) - 5gsin30) / 5gcos30 = (31.36 - 0.64 - 1 - 24.5) / 42.4352 = 0.123 ##
 
  • #28
marsupial said:
lol, I meant m1. Fatigue again. Nearly 1am after a long day. So, that would make it

## F_{fr} = m_2 g - m_2 a - m_1 a - m_1 gsin30 ##
...
## \mu = (3.2g - (3.2 * 0.2) - (5*0.2) - 5gsin30) / 5gcos30 = (31.36 - 0.64 - 1 - 24.5) / 42.4352 = 0.123 ##

Good work .
 
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  • #29
Thank you so much for your help!
 

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