I with understanding of Inertia of a slender rod and plate?

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This discussion focuses on understanding the moment of inertia for a slender rod and a plate in a mechanical system. The correct equations for the moment of inertia are established: for rods fixed at the ends, use I = 1/3 * m * L^2, and for rods fixed at the center, use I = 1/12 * m * L^2. The confusion regarding the plate's inertia arises from its lack of rotational motion; the appropriate formula depends on the context of the motion being analyzed. The conversation emphasizes the importance of distinguishing between translational and rotational kinetic energy in deriving equations for natural frequency.

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mm391
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Hello,

Before I get barraged with comments about this being a homework question it isn't. It is about helping me understand inertia. I am trying to understand how to chose which form of equation for the rod and which form of equation for the plate in the diagram attached.

Am i right in saying that as the rods are attached at their ends we use 1/3*m*L^2 but had they been fixed in the middle we would have to use 1/12*m*L^2.

As for the plate I am confused about which one you would choose as it has no rotational motion about the end or the center. It has purely translational motion. So how do you know whether to chose 1/12*m*L^2 or 1/12*m(a^2+b^2)

Any help in understanding would be much appreciated.

Thanks

MM
 

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hello mm391! :smile:

(try using the X2 button just above the Reply box :wink:)
mm391 said:
Am i right in saying that as the rods are attached at their ends we use 1/3*m*L2 but had they been fixed in the middle we would have to use 1/12*m*L2.

(you probably know this, so i'll put it in small type … moment of inertia only applies to rigid bodies, so you have to deal with the pair-of-rods and the plate completely separately)

not exactly

you can always use either the centre of mass or the centre of rotation

fixed as in the diagram, you can use either (try both, you'll find they give the same result in the end)

fixed at their centres, the centre of mass and the centre of rotation are the same, so there's no choice! :biggrin:
As for the plate I am confused about which one you would choose as it has no rotational motion about the end or the center. It has purely translational motion. So how do you know whether to chose 1/12*m*L^2 or 1/12*m(a^2+b^2)

not following you :confused:

ω = 0, so why would you want to use moment of inertia at all? :wink:
 
Well I am not sure how to say much more without making it into a previous homework question. We had this question about 3 months ago and needless to say I didn't do very well. I am now revising for exams. The question asks us to derive an equation for natural frequency for the system, ωn
 
show us your work, if you like :smile:
 
I=1/3*ml^2
Angular K.E = Iω^2
Linear K.E = 1/2*mv^2
Potential Energy = mgh
ƩmIrod=2(1/3*mL^2)

ƩK.E =1/2*mv^2+Iω^2

∴ ƩK.E =1/2*mv^2+1/3*ml^2ω^2

Then I get a little confused?
 
yes, the KE of the plate is 1/2 Mv2

the KE of each rod is either 1/2 Ic.o.rω2 or 1/2 mvc.o.m2 + 1/2 Ic.o.mω2 (same thing :wink:)
 
But now I am stuck. I am not sure how to finish the revision exercise. I was told that the system conservative so d/dt(E+V)=0 which I can't get my head round either.
 
you now need an equation relating v and h :wink:
 
Sorry for not understanding but I still don't see it:

I have everything down that could be related.

m*g*h + 1/2*mv^2+2(1/3*ml^2ω^2)=0

m*g*h=1/2mv^2

g*h=1/2v^2

V=√(2gh)
 
  • #10
that's physics!

i'm talking geometry! :wink:

every problem like this has geometrical constraints … these give you the extra equation(s) you need to solve the problem!

call the angle " θ ", and find h and v as a geometrical function of θ and dθ/dt :smile:

EDIT: (just noticed) i mean the h in your mgh,

not the (different) h in your diagram! :wink:
 
Last edited:
  • #11
I will have a look in the morning and then I will hopefully post the answer or anymore problems.

Thanks Tiny-Tim
 

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