Moment of Inertia of helicopter blades.

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SUMMARY

The discussion focuses on calculating the moment of inertia (MOI) for a model of helicopter blades, specifically using a square wooden base and four styrofoam blades. Participants suggest approximating the blades as rods and using the formula for angular inertia, I = mL²/3. They also discuss the moment of inertia for rectangular plates, given by I = 1/12 m(a² + b²), and how to incorporate additional triangular sections into the calculations. The conversation emphasizes the importance of understanding the geometry and density of the materials involved.

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eptheta
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I have built a model of rotating blades of a helicopter and want to mathematically calculate it's moment of inertia. I am unsure on how to do that.
Its a simple model:
a square wooden base with uniform thickness and 4 equally long blades made of styrofoam from the midpoints of the 4 sides of the square.
The rotational axis is through the centre of the square

Lets just say i know the density, mass and thickness of the base and the blades, how do i get moment of inertia for a specific length of blades ?

Thank you
 
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What if i have something like this:
http://img706.imageshack.us/img706/418/moin.png
I have those extra triangles at the center to deal with. can i just get the MOI of the triangles and add it to the MOI of the rectangular blades ?
yeah, i know I'm approximating a LOT, but it'll have to do.
Can anyone help ? Can anyone show me the derivation of it as well ?
 
Last edited by a moderator:
eptheta said:
I have built a model of rotating blades of a helicopter and want to mathematically calculate it's moment of inertia. I am unsure on how to do that.
Its a simple model:
a square wooden base with uniform thickness and 4 equally long blades made of styrofoam from the midpoints of the 4 sides of the square.
The rotational axis is through the centre of the square

Lets just say i know the density, mass and thickness of the base and the blades, how do i get moment of inertia for a specific length of blades ?

Thank you

The moment of inertia of a rectangular plate might get you even closer depending how you want to set it up. Its usually given in textbooks. I personally don't like to do the integration on some of these figures.

The moment of inertia of a rectangular plate is 1/12m(a^2 + b^2) where a is the width and b the length of the plate. Note that this is the moment of inertia taken from the center of mass of the plate.

I see your picture. So a and b are b and l...

So really one plate would have length 2l +b and width b... and there are two of them.
 
Last edited:
The moment of inertia of a rectangular plate might get you even closer depending how you want to set it up. Its usually given in textbooks. I personally don't like to do the integration on some of these figures.

The moment of inertia of a rectangular plate is 1/12m(a^2 + b^2) where a is the width and b the length of the plate. Note that this is the moment of inertia taken from the center of mass of the plate.

I see your picture. So a and b are b and l...

So really one plate would have length 2l +b and width b... and there are two of them.
From what you've said, if i take two rectangular plates, then after adding the two MOIs i' have an extra square in between. And i don't think i can just subtract that...

Also, do you know the derivation of 1/12 M(a2+b2) or a link to it ? I can't find it in my textbook.

I'm not sure if this is correct, but i tried my best to do the integration based on the baterials densities. I havn't added limits yet, but can you verify this for me ?:For the triangle in the middle for each blade:
{σ : density of triangle}
m=1/2 r2hσ
r2=2m/hσ
therefore I=∫2m/hσ
=m2/hσ dm=dx*b*h*rho where dx is a small distance on the wing.
{ρ: density of blade}
therefore ∫r2 dm
substituting for dm:
=∫x2*b*h*ρ dx
=1/3 b*h*ρ*x3

The dimensions are right [ML2] but I'm really not too sure...
Thanks
 
eptheta said:
From what you've said, if i take two rectangular plates, then after adding the two MOIs i' have an extra square in between. And i don't think i can just subtract that...

Also, do you know the derivation of 1/12 M(a2+b2) or a link to it ? I can't find it in my textbook.

I'm not sure if this is correct, but i tried my best to do the integration based on the baterials densities. I havn't added limits yet, but can you verify this for me ?:


For the triangle in the middle for each blade:
{σ : density of triangle}
m=1/2 r2hσ
r2=2m/hσ
therefore I=∫2m/hσ
=m2/hσ


dm=dx*b*h*rho where dx is a small distance on the wing.
{ρ: density of blade}
therefore ∫r2 dm
substituting for dm:
=∫x2*b*h*ρ dx
=1/3 b*h*ρ*x3

The dimensions are right [ML2] but I'm really not too sure...
Thanks

You don't have to worry about the middle square its taken care of if you use the sides I gave you.

And I am going to admit I don't like doing the math on these. So here is an old discussion on this board.
https://www.physicsforums.com/showthread.php?t=57119
 
Really ? So i just multiply it by 2 ? i.e I= 1/6 M(a2+b2)
 

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