Ball-Tipping Plank: Solve Problem with Answers Here

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Homework Help Overview

The discussion revolves around a physics problem involving a plank that is tipping, specifically analyzing the forces and torques at play when the plank begins to pivot. The subject area includes concepts of equilibrium, torque, and forces in mechanics.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the equilibrium conditions and attempt to set up torque equations to find the reaction forces at points A and B. Questions arise about the assumptions regarding contact forces and the implications of the plank starting to tip.

Discussion Status

Several participants have shared their attempts at solving the problem, with some providing equations and reasoning. There is ongoing exploration of the implications of the reaction forces and the conditions under which the plank tips. Guidance has been offered regarding summing forces and torques, but no consensus has been reached on the final solution.

Contextual Notes

Participants are working under the constraints of homework rules, which require them to post their attempts and relevant equations without providing complete solutions. There is also a focus on understanding the physical setup and the definitions of forces involved.

Robertd33
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Hello, I am new to the forum and am in the process of studying for a test that I have tomorrow. The attachment that I have included is a screenshot of a quiz we have taken with the answers included already, but I am not able to figure out how the problem is done.
Any help would be appreciated since I have been trying to solve it for over an hour now.
 

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What will be the reaction (normal) force at A when the plank just starts to tip? Use the equilibrium equations, please post your attempt and relevant equations for further assistance (per Forum rules), and Welcome to Physics Forums!:smile:
 
What I did was:
Torque:


Relevant equation= at equilibrium:
sum of torque= 0

Attempt:
0-Mg/3(x)+ Mg(.4)(pivotb) -Mg(.5)(center of gravity)= 0...when I solve for x I get .3, but the answer is .1
 
Robertd33 said:
What I did was:
Torque:


Relevant equation= at equilibrium:
sum of torque= 0
Don't forget sum of Fy =0
Attempt:
0-Mg/3(x)+ Mg(.4)(pivotb) -Mg(.5)(center of gravity)= 0...when I solve for x I get .3, but the answer is .1
What is the reaction force at B? It is not Mg.
 
That's what I seem to be having an issue with. Any idea? I'm assuming it's just Force * R(distance). The force in this case I assumed was Mg. What would it be?
 
Try summing forces in the vertical y direction. You know the given downward loads, and once you know what the reaction at A is, you can find the reaction at B. So, again, what must be the reaction at A when the plank is just starting to tip over and rotate about B? Hint: When it starts to tip, it loses contact with the support at A.
 
Wouldn't the reaction force just be 0 since there is no contact? How do I go about finding B?
 
After thinking about it for a while, I figured it out.

Solution question 6:

When the plank starts to pivot, it will pivot about point B. A can be neglected since it will not be in contact. Treating B as the center and the ball as the weight to the left and the center of gravity as the weight to the right, I got the following equation:

The ball will be -.4+x away from the ball and the center of gravity is at .5-
.4=.1
-Mg/3 (-.4+x) -Mg(.1)=0

Solving for x gives .1L.

Question 7:

For this part I used the original lengths given. This is the equation obtained:

-Mg/3(.1) + (x)Mg(.4) - Mg(0.5)=0

When solving for the x, 4/3 is the correct answer which corresponds to 4Mg/3.

Thank you for all of the help that lead me to the answer.
 
Last edited:
Robertd33 said:
Wouldn't the reaction force just be 0 since there is no contact? How do I go about finding B?
That's correct. So now just sum forces in the vertical y direction. You have the weight of the plank, mg, and the weight of the ball, mg/3, acting down. The reaction at A is 0, so what must be the reaction at B, acting up?? Then solve for x by summing torques = 0 about any convenient point (it is simplest to sum torques about B, now that you know that the reaction at A is 0).
 
  • #10
Robertd33 said:
After thinking about it for a while, I figured it out.

Solution question 6:

When the plank starts to pivot, it will pivot about point B. A can be neglected since it will not be in contact. Treating B as the center and the ball as the weight to the left and the center of gravity as the weight to the right, I got the following equation:

The ball will be .4-x away from the ball and the center of gravity is at .5-
.4=.1
-Mg/3 (.4-x) -Mg(.1)=0

Solving for x gives .1L.

Question 7:

For this part I used the original lengths given. This is the equation obtained:

-Mg/3(.1) + (x)Mg(.4) - Mg(0.5)=0
OK, you're ahead of me. In this equation, you are summing moments about A, in which case your equation should read

-Mg/3(.1) + (Rb)(.4) - Mg(0.5)=0, then Rb = 4mg/3
When solving for the x, 4/3 is the correct answer which corresponds to 4Mg/3.

Thank you for all of the help that lead me to the answer.
You should now check your work by looking at forces in the y direction =0. Since you have mg + mg/3 = 4mg/3 acting down. you must have Rb = 4mg/3 acting up, which agrees with your answer. Good work.
 

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