Block on wedge which is not fixed.Find minimum μ to keep the wedge at rest.

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Homework Help Overview

The problem involves a wedge of mass m with a quarter circular upper surface that is smooth, while the lower part is rough. A block of the same mass is placed at the top of the wedge, and the task is to find the minimum coefficient of friction required to keep the wedge stationary as the block slides down.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the angle at which the horizontal force on the wedge is maximized and explore the relationship between forces acting on the wedge and the block. There are questions about the correctness of expressions for normal forces and horizontal forces, as well as the implications of conservation of energy in this context.

Discussion Status

The discussion is ongoing, with participants questioning assumptions about the forces involved and the relationships between them. Some participants are attempting to derive expressions for the coefficient of friction in terms of the angle, while others are exploring the implications of their findings on the values of theta and friction.

Contextual Notes

There are indications of confusion regarding the definitions of forces and variables used in the equations, particularly concerning the normal force and its relationship to the wedge's motion. Participants are also considering the impact of differentiating expressions to find maximum values.

Satvik Pandey
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Homework Statement


Consider a wedge of mass m whose upper surface is a quarter circle and is smooth. The lower part is rough. A small block of same mass is kept at the topmost position and the initial position is shown in figure. The block slides down the wedge.

Find the minimum value of coefficient of friction between floor and lower surface of wedge so that the wedge remains stationery during the block's motion on it.
9f0d7815b5.4122fa5d51.Xk4w50.png


Homework Equations


The Attempt at a Solution


I tried to find the angle 'theta' at which horizontal force on the wedge is maximum.
9f0d7815b5.4122fa5d51.Xk4w50.png

By conservation of energy
##mgr=mgr(1-sin\theta )+\frac { m{ v }^{ 2 } }{ 2 } ##

So ##{ v }^{ 2 }=2grsin\theta ##

Horizontal force on the wedge(Fx) is ##\frac { m{ v }^{ 2 } }{ r } cos\theta ##So ##Fx=\frac { m }{ r } 2grsin\theta cos\theta ##

##Fx=mgsin2\theta##

For Fx to be maximum ##d(Fx)/d\theta=0##

so
##mg\frac { d }{ d\theta } sin2\theta =0##

##\theta ##=45

So ##{ v }^{ 2 }=\sqrt { 2 } \ gr ##
9f0d7815b5.4122fa5d51.Xk4w50.png


Normal force on the wedge = ##mg+mg+\frac { m{ v }^{ 2 } }{ 2 } sin\theta ##=3mg

Horizontal force on wedge= ##mgsin2\theta##=mg

As wedge should remain at rest so
## 3\mu mg=mg##
So ## \mu =1/3##

But this is not correct.Where did I go wrong?
 
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Satvik Pandey said:

Homework Statement


Consider a wedge of mass m whose upper surface is a quarter circle and is smooth. The lower part is rough. A small block of same mass is kept at the topmost position and the initial position is shown in figure. The block slides down the wedge.

Find the minimum value of coefficient of friction between floor and lower surface of wedge so that the wedge remains stationery during the block's motion on it.
9f0d7815b5.4122fa5d51.Xk4w50.png


Homework Equations


The Attempt at a Solution


I tried to find the angle 'theta' at which horizontal force on the wedge is maximum.
Are you sure? The force of friction depends on the normal force between the ground and the wedge, and it is not equal to the weight of the wedge.

Satvik Pandey said:
View attachment 73667
By conservation of energy
##mgr=mgr(1-sin\theta )+\frac { m{ v }^{ 2 } }{ 2 } ##

So ##{ v }^{ 2 }=2grsin\theta ##

Horizontal force on the wedge(Fx) is ##\frac { m{ v }^{ 2 } }{ r } cos\theta ##

The horizontal force of the wedge is the horizontal component of the normal force between the small block and the wedge. The normal force is not equal to the centripetal force. Do not forget agravity.

ehild
 
ehild said:
Are you sure? The force of friction depends on the normal force between the ground and the wedge, and it is not equal to the weight of the wedge.
The horizontal force of the wedge is the horizontal component of the normal force between the small block and the wedge. The normal force is not equal to the centripetal force. Do not forget agravity.

ehild
Untitled.png


From figure 2

##N=\frac { m{ v }^{ 2 } }{ R } +mgcos(90-\theta )##

or ##N=\frac { m{ v }^{ 2 } }{ R } +mgsin\theta ##

Horizontal force in wedge ##Fx=Ncos\theta =\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) cos\theta ##

From figure 3

##R=mg+Nsin\theta ##

##R=mg+\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) sin\theta ##

Are these equations correct?
Is my expression of v2 in #post1 correct?
 
Satvik Pandey said:
View attachment 73671

From figure 2

##N=\frac { m{ v }^{ 2 } }{ R } +mgcos(90-\theta )##

or ##N=\frac { m{ v }^{ 2 } }{ R } +mgsin\theta ##

And you got already that ##v^2=2gR\sin(\theta)##, so N= ??

Horizontal force in wedge ##Fx=Ncos\theta =\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) cos\theta ##

Satvik Pandey said:
[
##R=mg+Nsin\theta ##

##R=mg+\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) sin\theta ##

Are these equations correct?
Certainly not, R is the radius, a length, it can not be force ...
 
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ehild said:
And you got already that ##v^2=2gR\sin(\theta)##, so N= ??

Horizontal force in wedge ##Fx=Ncos\theta =\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) cos\theta ##Certainly not, R is the radius, a length, it can not be force ...

##N=\frac { m2gR\sin (\theta ) }{ R } +mgsin\theta =3 mg\sin (\theta )##

## Fx=3 mg\sin (\theta )cos\theta ##...(1)

The 'R' in the RHS is not radius.It is reactionary force on wedge.Sorry I should have choose other variable for it, let it be A.
So
##A=mg+Nsin\theta ##

##A=mg+\left( \frac { m{ v }^{ 2 } }{ R } +mgsin\theta \right) sin\theta ##
Please consider reactionary force on wedge in figure(3) in #post 3 be A.
 
On differentiating eq(1) wrt to ##\theta## and equating it to 0 I got ##\theta=45## maximum value of ##Fx=3mg/2##
 
Satvik Pandey said:
On differentiating eq(1) wrt to ##\theta## and equating it to 0 I got ##\theta=45## maximum value of ##Fx=3mg/2##

You need maximum coefficient of friction, not the maximum horizontal force. The force of friction also depends on the normal force and on theta.

And substitute for v2 also in the expression of A.
 
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ehild said:
You need maximum coefficient of friction, not the maximum horizontal force. The force of friction also depends on the normal force and on theta.

And substitute for v2 also in the expression of A.
ehild said:
You need maximum coefficient of friction, not the maximum horizontal force. The force of friction also depends on the normal force and on theta.

And substitute for v2 also in the expression of A.
##A=mg+3mg{ sin }^{ 2 }\theta ##
I thought by equating ## \mu A=Fx## I can solve for ##\mu##?
 
Satvik Pandey said:
##A=mg+3mg{ sin }^{ 2 }\theta ##
I thought by equating ## \mu A=Fx## I can solve for ##\mu##?
Solve for mu and find the smallest value.
 
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  • #10
ehild said:
Solve for mu and find the smallest value.
Should ##\theta=45##?
 
  • #11
Satvik Pandey said:
Should ##\theta=45##?
No, why? Solve for mu in terms of theta, and find the minimum value of mu.
 
  • #12
I got ##\mu=3/5##
ehild said:
No, why? Solve for mu in terms of theta, and find the minimum value of mu.
Oh! Sorry.
Putting value in ## \mu A=Fx##

I got ##μ(mg+3mg{ sin }^{ 2 }\theta )=3mgsin\theta cos\theta ##

or ##μ=\frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } ##

In order to have ##\mu## maximum

##\frac { d }{ d\theta } \left( \frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } \right) =0##

or ##\frac { d }{ d\theta } \left( \frac { sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } \right) =0##or ##\frac { (1+3{ sin }^{ 2 }\theta )\frac { d }{ d\theta } (sin\theta cos\theta )-(sin\theta cos\theta )\frac { d }{ d\theta } (1+3{ sin }^{ 2 }\theta ) }{ { (1+3{ sin }^{ 2 }\theta ) }^{ 2 } } =0##or ##(1+3{ sin }^{ 2 }\theta )\frac { d }{ d\theta } (sin\theta cos\theta )-(sin\theta cos\theta )\frac { d }{ d\theta } (1+3{ sin }^{ 2 }\theta )=0##

or ##(1+3{ sin }^{ 2 }\theta )cos2\theta -(sin\theta cos\theta )(3sin2\theta )=0##

or ##2(1+3{ sin }^{ 2 }\theta )cos2\theta =2(sin\theta cos\theta )(3sin2\theta )##

or ##2(1+3{ sin }^{ 2 }\theta )cos2\theta =3{ sin }^{ 2 }2\theta ##

or ##2(1+3{ sin }^{ 2 }\theta )(1-2{ sin }^{ 2 }\theta )=3{ sin }^{ 2 }2\theta ##

How to solve for ##\theta##?
 
  • #13
Satvik Pandey said:
I got ##\mu=3/5##

Oh! Sorry.
Putting value in ## \mu A=Fx##

I got ##μ(mg+3mg{ sin }^{ 2 }\theta )=3mgsin\theta cos\theta ##

or ##μ=\frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } ##

In order to have ##\mu## maximum

##\mu## need to be minimum.

Satvik Pandey said:
##\frac { d }{ d\theta } \left( \frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } \right) =0##
Change to double angles. You have turned ##\sin(\theta)\cos(\theta)## to ##0.5 \sin(2\theta)## already, but remember the very important formulas

##\cos^2(\theta)= \frac{1+\cos(2\theta )}{2}##

and

##\sin^2(\theta)= \frac{1-\cos(2\theta) }{2}##

Store them in your memory!

ehild
 
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  • #14
ehild said:
##\mu## need to be minimum.
That was a typo.
ehild said:
Change to double angles. You have turned ##\sin(\theta)\cos(\theta)## to ##0.5 \sin(2\theta)## already, but remember the very important formulas

##\cos^2(\theta)= \frac{1+\cos(2\theta )}{2}##

and

##\sin^2(\theta)= \frac{1-\cos(2\theta) }{2}##

Store them in your memory!

ehild

Is ##\theta ={ cos }^{ -1 }\left( \frac { 3 }{ 5 } \right) \times \frac { 1 }{ 2 } ##??
 
  • #15
Satvik Pandey said:
μ=3sinθcosθ1+3sin2θμ=\frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta }
Satvik Pandey said:
That was a typo.

Is ##\theta ={ cos }^{ -1 }\left( \frac { 3 }{ 5 } \right) \times \frac { 1 }{ 2 } ##??

So ##\theta =26.565##

As ##μ=\frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } ##

or ##μ=\frac { 3sin2\theta }{ 2(1+3{ sin }^{ 2 }\theta ) } =\frac { 3\times 0.8 }{ 3.199 } =0.75##

##\mu=0.75##
Got correct answer :D.
Thank you ehild.
 
  • #16
Satvik Pandey said:
So ##\theta =26.565##

As ##μ=\frac { 3sin\theta cos\theta }{ 1+3{ sin }^{ 2 }\theta } ##

or ##μ=\frac { 3sin2\theta }{ 2(1+3{ sin }^{ 2 }\theta ) } =\frac { 3\times 0.8 }{ 3.199 } =0.75##

##\mu=0.75##
Got correct answer :D.
Thank you ehild.

Splendid !

ehild
 
  • #17
ehild said:
Splendid !

ehild
Thank you ehild. I could't have solved it without your help.:)
 

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