Optimizing Force for Pushing Wheel over Bump

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Homework Help Overview

The problem involves determining the minimum horizontal force required to push a wheel of mass m and radius R over a block of height h. The original poster attempts to analyze the situation by modeling the wheel as a lever and applying principles of equilibrium and moments.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of lever principles, questioning the assumptions about the lever arms of the forces involved. There is mention of using moments and the point of contact as a fulcrum. Some participants express confusion regarding the angles involved in the calculations.

Discussion Status

The discussion is ongoing, with participants providing insights and corrections regarding the setup of the problem. There is a recognition of errors in trigonometric calculations, and some guidance is offered on using the point of contact as the pivot. Multiple interpretations of the force and gravity's application are being explored.

Contextual Notes

Participants note the importance of correctly identifying the angles and lengths involved in the lever arms, as well as the implications of the force's point of application on the wheel.

PrestonBlake
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Homework Statement



You have a wheel of mass m and radius R you're trying to push it onto a block of height h that it's next to. Find the minimum force F that will let you do this. F is completely horizontal and acts upon the center of the wheel.

Homework Equations



I'm trying to solve this by pretending the wheel is a lever attached to the edge of the block. It has two forces acting on it F and gravity. To find the minimum force I assume F*sin(theta)*R=G*Sin(theta)*R

The Attempt at a Solution



I believe that the line from the part where the wheel touches the block to the center of the wheel makes a degree of arcsin(1-h/r) Then I try to calculate the degree each force makes with the perpendicular of the imaginary lever to get g*m*cos(Pi/2-arcsin(1-h/r))==F*cos(arcsin(1-h/r)). Then I solve for F and get a wrong answer.
 
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PrestonBlake said:


Homework Equations



I'm trying to solve this by pretending the wheel is a lever attached to the edge of the block. It has two forces acting on it F and gravity. To find the minimum force I assume F*sin(theta)*R=G*Sin(theta)*R


The lever arm of gravity is not the same as that of the force F.

ehild
 
Are you sure? It's a given that F is pushing on the center and I'm assuming that gravity is working on the center of mass, which should be the same as the center.
 
Use the point of contact between wheel and the block as fulcrum.
Use moments to solve the problem.
 
azizlwl said:
Use the point of contact between wheel and the block as fulcrum.

That's what I did, but apparently I messed up the trig on my way to the answer.
 
PrestonBlake said:
Are you sure? It's a given that F is pushing on the center and I'm assuming that gravity is working on the center of mass, which should be the same as the center.

Gravity is vertical, the force is horizontal. You use the touching point between ball and block as pivot point. The arms are not equal.

ehild
 
Use phytagoras theorem to find arms length.
For using trig function,
Weight, it should be mgCosθ.R
 
azizlwl said:
Use phytagoras theorem to find arms length.
For using trig function,
Weight, it should be mgCosθ.R

Thanks, it turns out I had switched the angle of gravity with the angle of the force.
 
As a second question, what would the arm length be if the force was acting at the top of the wheel instead of at the middle.
 

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