Math in Maxwell needle method- the formula the moment of inertia

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Homework Help Overview

The discussion revolves around calculating the moment of inertia (I1) in the context of a Maxwell needle method problem. Participants are exploring the mathematical principles involved, particularly focusing on the moment of inertia formula and its application to a specific setup depicted in an attachment.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the definition of variables and the interpretation of the moment of inertia formula. There are inquiries about the parallel axis theorem and its implications for the calculation of moment of inertia. Some participants express confusion regarding specific terms and concepts, such as the meaning of certain variables in the context of the problem.

Discussion Status

The discussion is ongoing, with several participants providing insights and clarifications regarding the moment of inertia and its calculation. Some guidance has been offered about the parallel axis theorem, and there is an exploration of the relationship between the integral form of the moment of inertia and the summation form. Multiple interpretations of the problem are being considered, and participants are actively engaging with each other's questions.

Contextual Notes

There are references to attachments that contain visual representations and definitions of variables, which some participants find unclear. The original poster has indicated a lack of understanding regarding the moment of inertia and its mathematical formulation, prompting further discussion and clarification.

Outrageous
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1. Homework Statement [
How do I get I1( the moment of inertia of the picture b) ?is just a math problem but really no idea.

Homework Equations


I=mr^2


The Attempt at a Solution


maybe centre of mass .

Guide will do . please help , thank
 

Attachments

  • maxwell.PNG
    maxwell.PNG
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  • rotational mass.PNG
    rotational mass.PNG
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  • I.PNG
    I.PNG
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I cannot work out what your picture is showing, and there's no definition of the variables in the second attachment.
Edit: Just noticed there's a tiny 3rd attachment explaining the variables...
 
What part of the equation do you not understand? Is it the 3L/8?
 
yes , exactly that part.
 
It's just the parallel axis theorem. The centre of mass of the cylinder is 3L/8 from the axis of rotation.
 
Thank you. One more to ask,
I know that moment of inertia I=mr^2
For a system, I= m(r1)^2 + m(r2)^2 + m(r3)^2 +...
or we can write I=Ʃmr^2
where the m= mass of a particle , r1 and r2 are not the same value.
This is the only thing that I understand but I=∫r^2 dm=mr^2 from this link
http://easycalculation.com/theorems/parallel-axis-moment-of-inertia.php

How can I=∫r^2 dm=mr^2 ?
here mean the r is constant ? m is the total mass?

Thank you.
 
That link is saying that if the MoI about the CoM is Ic = ∫x2.dm, where x varies, and you want the MoI Ir about a an axis displaced by an amount r then Ir = ∫(x+r)2.dm = ∫(x2+2xr+r2).dm = ∫x2.dm+2∫xr.dm+∫r2.dm = Ic + 2∫xr.dm + ∫r2.dm
Since r is a constant, Ir = Ic + 2r∫x.dm + r2∫.dm
Since x is displacement from centre of mass, by definition ∫x.dm = 0, and ∫.dm is just the total mass, M:
Ir = Ic + r2M
 
haruspex said:
That link is saying that if the MoI about the CoM is Ic = ∫x2.dm, where x varies, and you want the MoI Ir about a an axis displaced by an amount r then Ir = ∫(x+r)2.dm = ∫(x2+2xr+r2).dm = ∫x2.dm+2∫xr.dm+∫r2.dm = Ic + 2∫xr.dm + ∫r2.dm
Since r is a constant, Ir = Ic + 2r∫x.dm + r2∫.dm
Since x is displacement from centre of mass, by definition ∫x.dm = 0, and ∫.dm is just the total mass, M:
Ir = Ic + r2M

Ic = ∫x2.dm is same as
For a system, I= m(r1)^2 + m(r2)^2 + m(r3)^2 +...
or we can write I=Ʃmr^2
where the m= mass of a particle ?
Why I=integral x^2 dm , x varies. Then for I =∫x dm ,it become zero.
 
Outrageous said:
Ic = ∫x2.dm is same as
For a system, I= m(r1)^2 + m(r2)^2 + m(r3)^2 +...
or we can write I=Ʃmr^2
where the m= mass of a particle ?
Yes. Strictly, I= m1(r1)^2 + m2(r2)^2 + ...
Why I=integral x^2 dm , x varies. Then for I =∫x dm ,it become zero.
In the analysis, x is defined to be the displacement (in the x coordinate) of the element dm from the centre of mass. By definition of centre of mass, ∫x dm =0.
 
  • #10
haruspex said:
By definition of centre of mass, ∫x dm =0.

Really thank you^^
 

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