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

AI Thread Summary
The discussion revolves around calculating the minimum coefficient of friction required to keep a wedge stationary while a block slides down its smooth surface. The problem involves analyzing forces acting on the wedge, including the horizontal force due to the block's motion and the normal force between the block and the wedge. Initial calculations suggested a coefficient of friction of 1/3, which was incorrect. Through further analysis and corrections, the final value for the minimum coefficient of friction was determined to be 0.75, achieved by substituting into the derived equations and maximizing the frictional force relative to the normal force. The collaborative effort highlighted the importance of accurately accounting for forces and angles in the calculations.
Satvik Pandey
Messages
591
Reaction score
12

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?
 
Physics news on Phys.org
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 ...
 
  • Like
Likes Satvik Pandey
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.
 
  • Like
Likes Satvik Pandey
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.
 
  • Like
Likes Satvik Pandey
  • #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
 
  • Like
Likes Satvik Pandey
  • #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.:)
 
Back
Top