Friction of a sliding door with one of its wheels "frozen"

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SUMMARY

The discussion focuses on calculating the force required to slide a 133-lb sliding glass door when one of its wheels becomes "frozen." The coefficient of kinetic friction between the frozen wheel and the surface is 0.30. Participants analyze the equilibrium conditions, emphasizing the importance of understanding the normal forces at the wheels and the moments about the pivot points. The consensus is that the frozen wheel acts as a pivot, affecting the normal forces and friction calculations necessary to determine the force P required to slide the door.

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  • Understanding of static and kinetic friction, specifically the coefficient of kinetic friction.
  • Familiarity with equilibrium conditions in rigid body mechanics.
  • Knowledge of moment equations and their application in two-dimensional problems.
  • Ability to analyze forces and moments acting on a system of rigid bodies.
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  • Study the principles of equilibrium in rigid body mechanics.
  • Learn about calculating normal forces in systems with multiple contact points.
  • Explore the application of moment equations in two-dimensional force analysis.
  • Research the effects of friction on the motion of sliding objects, particularly in mechanical systems.
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Mechanical engineers, physics students, and anyone involved in the design or analysis of sliding mechanisms and frictional forces in mechanical systems.

J-dizzal
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Homework Statement


The sliding glass door rolls on the two small lower wheels A and B. Under normal conditions the upper wheels do not touch their horizontal guide. (a) Compute the force P required to slide the door at a steady speed if wheel A becomes "frozen" and does not turn in its bearing. (b) Rework the problem if wheel B becomes frozen instead of wheel A. The coefficient of kinetic friction between a frozen wheel and the supporting surface is 0.30, and the center of mass of the 133-lb door is at its geometric center. Neglect the small diameter of the wheels.
20150721_164320_zpsy3oucxyp.jpg

Homework Equations


FkkFN
where FN is the normal force.

The Attempt at a Solution


20150721_191617_zpszxm89rty.jpg

I thought symmetry of the door would result in 133/2 lb at each roller.
 
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I think there is an equilibrium problem hiding in here. The door will rotate up and one of the top wheels may contact if a wheel freezes.
 
Dr. Courtney said:
I think there is an equilibrium problem hiding in here. The door will rotate up and one of the top wheels may contact if a wheel freezes.
I was wondering what all the length dimensions were for...
So then would there be a moment about the non frozen wheel? and then that would cause one of the top wheels to touch? But if a top wheel touches it should roll freely and not add any more friction force.
 
It might depend on which wheel is frozen. The frozen wheel becomes the pivot point. You need to consider the equilibrium conditions.
 
Dr. Courtney said:
It might depend on which wheel is frozen. The frozen wheel becomes the pivot point. You need to consider the equilibrium conditions.
For equilibrium conditions, would that be finding the forces at each point knowing that the sum of forces and moments is equal to zero?

edit; ΣMA= -133(14.5) - P(40). P =-48.21 lb I am confused on why this equations solves for P but its not correct.
 
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Dr. Courtney said:
It might depend on which wheel is frozen. The frozen wheel becomes the pivot point. You need to consider the equilibrium conditions.
Ok the frozen wheel becomes the pivot point, so i did sum of moments at the frozen wheel and found P=-48.21 but its the wrong answer. I did sum of forces and I am going in circles.
My original picture is updated.
 
Im getting stuck at part A. I don't think i need the moment equations because its not tipping its slipping. so then when i do a sum of forces i can only find the normal force which is half of the weight. Then using that to find the kinetic friction force is still giving me the wrong answer for P
 
Dr. Courtney said:
The door will rotate up and one of the top wheels may contact if a wheel freezes.
...
The frozen wheel becomes the pivot point.
Not necessarily. In particular, not if A freezes.
J-dizzal said:
i can only find the normal force which is half of the weight.
The normal forces will be different at A and B. Put in unknowns for those.
In general, there may also be a normal force at the upper wheel above A.
Do you see why there can never be a normal force at the other top wheel?
Can there be a normal force at the top and bottom wheels on the same side?
How many cases does that give you?
 
haruspex said:
Not necessarily. In particular, not if A freezes.

The normal forces will be different at A and B. Put in unknowns for those.
In general, there may also be a normal force at the upper wheel above A.
Do you see why there can never be a normal force at the other top wheel?
Can there be a normal force at the top and bottom wheels on the same side?
How many cases does that give you?
For the normal forces, ill have to solve those using moment equations.
there will never be a moment force at the top above B because both the wheels move up top and the moments cancel out, like two hinges.
No, i don't think there will be a moment at the top because of the moments canceling out.
im not sure on how many cases, I only see it one way, two if you include part B of the question.
 
  • #10
J-dizzal said:
For the normal forces, ill have to solve those using moment equations.
Sure, so create unknowns and post some equations. Please use only symbols for all the variables, both known and unknown, i.e. don't plug in the numerical distances and masses etc.
J-dizzal said:
there will never be a moment force at the top above B because both the wheels move up top and the moments cancel out, like two hinges.
I asked about forces, not their moments.
J-dizzal said:
im not sure on how many cases, I only see it one way, two if you include part B of the question.
I was including both parts of the question. I agree there is only one case to consider in part A (which is that case, and why is it the only one?). There may be two cases to consider for part B.
 
  • #11
haruspex said:
Sure, so create unknowns and post some equations. Please use only symbols for all the variables, both known and unknown, i.e. don't plug in the numerical distances and masses etc.

I asked about forces, not their moments.
I was including both parts of the question. I agree there is only one case to consider in part A (which is that case, and why is it the only one?). There may be two cases to consider for part B.
ΣMA=-W(14.5) - P(40)=0. this equation solves for P but its not the correct answer. This appears to be the only moment equations i can create.
There will never be a normal force at B because the moments will rotate the door clockwise.
It is the only case to consider in part A because wheel A is the only point where moments are taken.

edit. my moment equation is missing By(29), I am missed this before thinking it was zero because its on the same line of action.
 
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  • #12
At point A if i call the resultant forces in the x and y directions Ax and Ay, is this name convention redundant because the friction force would replace Ax?
 
  • #13
haruspex said:
Sure, so create unknowns and post some equations. Please use only symbols for all the variables, both known and unknown, i.e. don't plug in the numerical distances and masses etc.

Here is what i have so far,
ΣMA=-133(14.5) - P(40) + NB=0
ΣFx=P-FkA=0
ΣFy=-133+NA+NB=0
I have 4 unknowns and only 3 equations. I think there must be a way to solve the Normal forces but i just don't see it yet.
 
  • #14
J-dizzal said:
There will never be a normal force at B because the moments will rotate the door clockwise.
That is precisely why the normal force at B will be large!
J-dizzal said:
ΣMA=-W(14.5) - P(40)=0.
What part of "please don't plug in numbers" was unclear? Please read part 1. of https://www.physicsforums.com/insights/frequently-made-errors-equation-handling/
Anyway, that would give you a negative P.

In general, for equilibrium (non-acceleration) of a rigid body in a 2D problem you have three equations available. Typically one uses two linear force balances at right angles and moments about one reference point. Quite often there is a force which is both unknown and uninteresting in regards to the question, so judicious choice of axis can eliminate that and you then only need a linear equation that also does not involve that force. (I go into more detail in part 4. of https://www.physicsforums.com/insights/frequently-made-errors-mechanics-forces/)
Since part A involves friction at A, it would seem more useful to take moments about B. Which linear force balance equation does not involve the normal force at B?
 
  • #15
haruspex said:
it would seem more useful to take moments about B. Which linear force balance equation does not involve the normal force at B?

This is what i don't understand, if B is free to rotate then how can a moment equation be made? because it only resists movement in the y axis. This is what i learned form previous equilibrium materials, why does it change now?

sum of forces in the x direction, does not involve the normal force at B.
haruspex said:
please don't plug in numbers" was unclear?
I only put in the given dimensions from the problem no calculations were made.
 
  • #16
J-dizzal said:
This is what i don't understand, if B is free to rotate then how can a moment equation be made? because it only resists movement in the y axis. This is what i learned form previous equilibrium materials, why does it change now?
I don't think I am going to understand your difficulty here unless you can quote a prior example.
It might help if you would answer a question I asked in post #10:
haruspex said:
there is only one case to consider in part A (which is that case, and why is it the only one?).

J-dizzal said:
I only put in the given dimensions from the problem no calculations were made.
That still constitutes plugging in numbers. The consequence is that I have to go back to the OP and reverse engineer your equation to figure out what those numbers represent. Sometimes that's not clear because the same number might crop up in different variables.
 
  • #17
haruspex said:
which is that case, and why is it the only one?
there is only one case here, this case is when wheel A freezes and there is a moment about A. None of the top wheels would contact their frame because the door is not tipping. It is not tipping because the location of the normal force and friction force are not at the bottom right corner. Additionally, wheel B stops tipping by contributing a normal force.

ΣMB I am getting the same result at before with the sum of moments at A.
ΣMB=W(Length of half the distance from A to B)-P(Length from P to bottom right corner)=0
If I am wrong and there is a normal force because the door is tipping then add into the moment equation: (Top A)(vertical length of door)
 
  • #18
J-dizzal said:
this case is when wheel A freezes ... It is not tipping because the location of the normal force and friction force are not at the bottom right corner.
As I wrote, there is a normal force at bottom right, but yes, the reason it won't tip is that there is no friction at bottom right. If it started to tip there'd be no friction at A either, so no horizontal force to counter P.
J-dizzal said:
ΣMB=W(Length of half the distance from A to B)-P(Length from P to bottom right corner)=0
Don't assume there's no normal force at A.
What linear force equation does not involve the normal force at B?
 
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  • #19
haruspex said:
What linear force equation does not involve the normal force at B?

sum of forces in the x direction; ΣFx=P-(force of friction at A)=0.
unknowns;P,NB,NA,and friction force at A.
But only 3 equations, moment and two linear force equations.
 
  • #20
J-dizzal said:
sum of forces in the x direction; ΣFx=P-(force of friction at A)=0.
unknowns;P,NB,NA,and friction force at A.
But only 3 equations, moment and two linear force equations.
You know the relationship between the frictional force and NA.
If you take moments about B, NB does not feature.
 

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