Reaction Force, find tension, a in the tangential, or alpha

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Homework Help Overview

The problem involves a long slender bar and a mass connected via a pulley system, where the objective is to determine the reaction force on the bearing A. The scenario includes a bar of mass 4.9 kg and a mass of 6.5 kg with a specified vertical velocity.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss splitting the reaction force into components and applying equations of motion and torque. There are attempts to solve simultaneous equations to find tension, tangential acceleration, and angular acceleration. Questions arise about the consistency of variables used in different equations and the direction of acceleration.

Discussion Status

There are multiple values for the reaction forces being calculated, with some participants expressing uncertainty about their results. Guidance is offered regarding the relationships between acceleration and angular acceleration, and there is an ongoing exploration of the signs associated with these variables.

Contextual Notes

Participants note potential issues with assumptions regarding the direction of forces and accelerations, as well as the need for clarity on the definitions of variables used in the equations.

Jonski
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Homework Statement


The diagram shows the instant when a long slender bar of mass 4.9 kg and length 4.9 m is horizontal. At this instant the mass m= 6.5 kg has a vertical velocity of 4.0 m/s.

If the pulley has negligible mass and all friction effects may be ignored, what is the magnitude of the reaction force on the bearing A
problem_Moodle.gif


2. The attempt at a solution
So I split the reaction force into its x and y components Rx and Ry.

For Mass m:
T - mg = ma

For the bar:
Sum of the moments from A:
let mass of bar = B
length of bar = L
B*g*L/2 - T.L = B*L^2/3*α

Sum of forces in the x direction:
Rx = B*a=B*ω^2*L/2

Sum of forces in the y direction:
Ry - Bg+T=B*(-a) = -B*α*L/2

I solved and got Rx = 8N, however not sure how to find tension, a in the tangential, or alpha. I have tried simultaneous equations to find them but keep getting them wrong. Please help
 
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Hello, Jonski.

You probably need to show your attempt at solving the simultaneous equations in order for us to find your error.

Something to think about: Is the "a"in your equation T - mg = ma the same "a" as in your Rx and Ry equations?
 
Hi TSny :smile:

I get Rx = 32 N (towards right) and Ry = 37.46 N (downwards) . The magnitude of reaction force equal to 49.27 N .

Are you getting the same result ?
 
Tanya Sharma said:
Hi TSny :smile:

I get Rx = 32 N (towards right) and Ry = 37.46 N (downwards) . The magnitude of reaction force equal to 49.27 N .

Are you getting the same result ?
Hi Tanya.
I get different values for Rx and Ry. For Rx, are you sure you're using the correct value for the speed of the center of mass of the rod?
 
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Okay .

Rx = 8N (towards right) and Ry = 17.35 N (downwards) ?
 
Tanya Sharma said:
Okay .

Rx = 8N (towards right) and Ry = 17.35 N (downwards) ?
OK for Rx. But I still get a different answer for Ry.
 
I will show you my working .
 
Denoting mass of bar as M , length as L , mass of block as m ,

For block of mass m , ##mg - T = ma ##

Writing torque equation for the rod about the bearing, ##Mg\frac{L}{2} - TL = \frac{ML^2}{3}\alpha##

##\alpha = \frac{a}{L}##

Solving this I get ##T = \frac{Mmg}{2(3m-M)}## and ##\alpha = \frac{3g}{2L} - \frac{3mg}{2L(3m-M)}## .

Now writing torque equation for the rod about the CM , ## R_y\frac{L}{2} - T\frac{L}{2} = \frac{ML^2}{12}\alpha## .

From this I get ##R_y = \frac{Mg}{4} + \frac{Mmg}{4(3m-M)}##
 
Last edited:
Tanya Sharma said:
For block of mass m , ##mg - T = ma ##
So, positive value of ##a## implies what direction of acceleration for the block?

Writing torque equation for the rod about the bearing, ##Mg\frac{L}{2} - TL = \frac{ML^2}{3}\alpha##
So, positive value for ##\alpha## implies what direction of tangential acceleration for the left end of the rod?

##\alpha = \frac{a}{L}##

Does ##\alpha = \frac{a}{L}## or does ##\alpha = -\frac{a}{L}##?
 
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  • #10
So,the only problem in post#8 is relationship between ##\alpha## and a ?

##\alpha = -\frac{a}{L}##
 
Last edited:
  • #11
Tanya Sharma said:
So,the only problem in post#8 is relationship between ##\alpha## and ##a## ?

##\alpha = -\frac{a}{L}## .
Yes, your first two equations in #8 look fine. I have not checked your algebra for solving for T, etc.
 
  • #12
TSny said:
Yes, your first two equations in #8 look fine. I have not checked your algebra for solving for T, etc.
Also, your equation for torque about CM looks good.
 
  • #13
Are you getting ##R_y = 28 N## ?

Some doubts regarding why did we write ##\alpha = -\frac{a}{L}## ?

It is because positive value of 'a' suggests block is going downwards which in turn means the rod is rotating clockwise . But since we have considered anticlockwise positive , we write ##a = -\alpha L## .

Not sure , if this is the correct reasoning . You remember I once made an entire thread on sign issues. I am still doing some really sloppy work :olduhh: .

How did you think about signs in this problem?
 
Last edited:
  • #14
I got 28 N too. Your reasoning for why ##a## and ##\alpha## have opposite signs is the same as how I thought about it.
 
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