Acceleration for a non-inertial reference frame

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Homework Help Overview

The discussion revolves around the acceleration in non-inertial reference frames, specifically focusing on a system involving a platform and a slider. Participants are analyzing the equations of motion and the forces acting within this context.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the equation for acceleration in non-inertial systems and question the assumptions made regarding the reference frames. There is a focus on the definitions of various terms like ##a_0## and ##v_{rel}##, and the implications of using different frames of reference.

Discussion Status

Some participants are seeking clarification on the setup and the definitions used, while others are attempting to derive expressions for the normal force ##N## in terms of the given symbols. There is an ongoing dialogue about ensuring that expressions are symbolic before substituting numerical values.

Contextual Notes

Participants note the presence of two non-inertial frames and discuss the implications of choosing one over the other. There is also mention of the need to consider the direction of angular velocity and the nature of the forces acting on the system.

Like Tony Stark
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Homework Statement
The disk with a slot rotates with ##\omega =20 \frac{rad}{s}## about a vertical axis that passes through its centre. There's a slider of mass ##0.73 kg## that oscilates because of the action of a spring (not shown in the picture) and it has a positive velocity ##90 \frac{cm}{s}## relative to the disk when it is in ##x=0##. Determine the normal force exerted by the slot on the slider when ##x=0##.
Relevant Equations
##a_I=a_o+\dot \omega \times r+\omega \times (\omega \times r)+2(\omega \times v_{rel}) +a_{rel}##.
Well, first a wrote the equation for acceleration in non inertial systems.

##a_I=a_o+\dot \omega \times r+\omega \times (\omega \times r)+2(\omega \times v_{rel}) +a_{rel}##.

Then, ##a_o=0## (because the system doesn't move), ##a_i=0## (because it is measured from the non inertial system), ##\dot \omega =0## (because the angular velocity is constant), ##r=0## (because ##x=0##)

So we get
##-2 (\omega \times v_{rel})=a_{rel}##

Then, we write Newton's equations
##x) Fe=m.a_{rel}##
##y) N-F_{Cor}=0##

Where ##Fe## is the elastic force and ##F_{Cor}=2(\vec \omega \times v_{rel})##

So I just have to replace with the numbers that I was given and get ##N##.

Are my ideas correct?
 

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There are two non-inertial frames, one fixed on the platform and one fixed on the slider. Which one are you considering? When you say that ##a_0=0## because the "system doesn't move" which system is this? What are you going to use for ##v_{rel}##? Also, don't replace any numbers before you get an expression for ##N## in terms of symbols all of which are given. That will make it easier to check your work.
 
kuruman said:
There are two non-inertial frames, one fixed on the platform and one fixed on the slider. Which one are you considering? When you say that ##a_0=0## because the "system doesn't move" which system is this? What are you going to use for ##v_{rel}##? Also, don't replace any numbers before you get an expression for ##N## in terms of symbols all of which are given. That will make it easier to check your work.
I'm considering a system fixed to the platform. I said that ##a_0=0## because the origin doesn't move. Then I said that ##a_i## is the acceleration measured from an inertial frame, but as I took the disk frame, I said that it was 0.

As for not replacing the numbers, yes, I'll take your advice, but I replaced them to check if the data that I plugged in was ok.
 
So what's your symbolic answer?
 
kuruman said:
So what's your symbolic answer?
##y)N-\Sigma F_{rely}=m.a_{rely}##
##N=\Sigma F_{rely}+m.a_{rely}##

Where ##\Sigma F_{rely}## is the sum of the pseudo-forces acting on the ##y## direction and ##a_{rely}## is the acceleration of the slider relative to the disk.
 
Like Tony Stark said:
##y)N-\Sigma F_{rely}=m.a_{rely}##
##N=\Sigma F_{rely}+m.a_{rely}##

Where ##\Sigma F_{rely}## is the sum of the pseudo-forces acting on the ##y## direction and ##a_{rely}## is the acceleration of the slider relative to the disk.
Not what I had in mind. I am asking for an expression giving ##N## in terms of symbols for which you have numbers. You don't have numbers for any of the quantities on the right hand side except for the mass ##m##.
 
kuruman said:
Not what I had in mind. I am asking for an expression giving ##N## in terms of symbols for which you have numbers. You don't have numbers for any of the quantities on the right hand side except for the mass ##m##.
##y)N=m.a_{rely} -2(\omega \times v_{rel})##

##m##, ##\omega## and ##v_{rel}## are a given values; ##a_{rely}=0## because the slider just moves in ##x##
 
Almost correct. You need to multiply the second term by the mass. Also, the problem gives only magnitude of ##\omega##, but I think it is safe to assume that it is in the ##+z## direction.
 

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