Inertia from four masses connected by massless rigid rods

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Homework Help Overview

The discussion revolves around calculating the moment of inertia for a system of four masses connected by massless rigid rods. The original poster has computed the center of mass coordinates but is uncertain about the inertia calculation process.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of the parallel axis theorem and the summation of moments of inertia for individual masses. There are attempts to clarify the correct use of formulas and the significance of each term in the calculations.

Discussion Status

There is ongoing exploration of the inertia calculation, with some participants providing guidance on using the parallel axis theorem. Multiple interpretations of the calculations are being examined, and there is no explicit consensus on the correctness of the results presented.

Contextual Notes

Participants note the importance of considering all masses in the system and question the assumptions made regarding the calculations. There is mention of homework constraints and the need for clarity in presenting equations.

aivilo775
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Homework Statement
The four masses shown in (Figure 1) are connected by massless, rigid rods. Assume that m = 230 g. Find the moment of inertia about an axis that passes through mass A and is perpendicular to the plane of the image.
Relevant Equations
Ia = kg * m^2
Screen Shot 2022-10-26 at 7.50.57 PM.png

I found xcm = 6.2cm, ycm = 4.9cm, but am unsure of how to tackle the inertia part of the problem.
 
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Assuming your ##x_{cm}## and ##y_{cm}## are right (I haven't checked). Then you can merely apply the "parallel axis theorem" which in plain english states

"The moment of inertia about a given axis (presumably not the center of mass) is equal to the moment of inertia about the center of mass plus ##Mh^2## where ##M## is the total mass and ##h## is the distance from the center of mass to the axis of interest.

##I = I_{cm} + Mh^2##

You've already done the hard part. The answer to your second question is seconds away.

So I suggest you find the Moment of Inertia about the center of mass that you calculated and just add ##Mh^2##
 
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I'm going to do it both manually and by using the parallel axis theorem just to make sure I'm not going crazy.

You should do the same.

Remember ##I = \sum \limits_{i=1}^{n} m_i r_i^2## for each of the ##n## particles and the axis of interest.
 
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PhDeezNutz said:
Remember I=∑i=1nmiri2 for each of the n particles and the axis of interest.
So I did I = Ia +Ib+Ic+Id. Since it's rotating through mass A, I set Ia = 0. I then did I = (.5)(230/1000)(8/100)^2 + (.5)(300/1000)(sqrt[(10/100)^2 + (8/100)^2)])^2 + (.5)(230/1000)(10/100)^2

I got that I = 0.004346 kg * m^2

Does this seem right?

Or I suppose I shouldn't use the .5 so
I = (230/1000)(8/100)^2 + (300/1000)(sqrt[(10/100)^2 + (8/100)^2)])^2 + (230/1000)(10/100)^2 = 0.008692
 
aivilo775 said:
So I did I = Ia +Ib+Ic+Id. Since it's rotating through mass A, I set Ia = 0. I then did I = (.5)(230/1000)(8/100)^2 + (.5)(300/1000)(sqrt[(10/100)^2 + (8/100)^2)])^2 + (.5)(230/1000)(10/100)^2

I got that I = 0.004346 kg * m^2

Does this seem right?
It doesn't seem right. Why are you multiplying each term by 0.5? Please post your equations in symbolic form then substitute the numbers at the very end. If you don't know how to use LaTeX for posting equations, click on the link "LaTeX Guide", lower left.
 
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Still incorrect. There are three masses to consider, so there are three terms to add. I see only two. Also, only one mass is in your expression, the one in the second term.
 
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aivilo775 said:
Homework Statement:: The four masses shown in (Figure 1) are connected by massless, rigid rods. Assume that m = 230 g. Find the moment of inertia about an axis that passes through mass A and is perpendicular to the plane of the image.
Relevant Equations:: Ia = kg * m^2

I found xcm = 6.2cm, ycm = 4.9cm
It is rarely helpful to find the common mass centre of an assemblage. Moments of inertia are additive, as shown in post #3. This gives you a much easier way.
 
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