Angular momentum of a rod rotating about an axis

[zeralda21]

Homework Statement

I'll provide a picture for clearer understanding. The problem is to calculate the angular momentum of the rod rotating about the z-axis. I have serious difficulties in deriving the inertia matrix, that's all I need help with.

Progress

Since the rod is rotating about the z-axis $\Rightarrow \omega _{x}=\omega _{y}=0$ the angular momentum simplifies to

$\boldsymbol{L}_{O}=-I_{xz}\omega _{z}\hat{\mathbf{i}}-I_{yz}\omega _{z}\boldsymbol{\hat{j}}+I_{zz}\omega_{z}\boldsymbol{\hat{k}}$

Split the rod in three parts (SEE FIGURE) and calculate for each body.

I have correct terms for body A.

For B:

$I_{xz}=\overline{I}_{xz}+md_{x}d_{z} = 0 +\rho b(0)(\frac{b}{2})=0$
$I_{yz}=\overline{I}_{yz}+md_{y}d_{z} = 0 +\rho b(b)(\frac{b}{2})=\frac{1}{2}\rho b^3$
(Wrong)$I_{zz}=\overline{I}_{zz}+md^2 = 0 + (\rho b)(b^2+(\frac{b}{2})^2)=\frac{5}{4}\rho b^3$ (d is distance from midpoint of B to origin O)

For C:

$I_{xz}=\overline{I}_{xz}+md_{x}d_{z} = 0 +\rho b(\frac{b}{2})(b)=\frac{1}{2}\rho b^3$
$I_{yz}=\overline{I}_{yz}+md_{y}d_{z} = 0 +\rho b(b)(b)=\rho b^3$
(Wrong)$I_{zz}=\overline{I}_{zz}+md^2 = \frac{1}{3}(\rho b)(b^2)+(\rho b)((2b^2)^2+(\frac{b}{2})^2)=\frac{55}{12}\rho b^3$ (distance d is from midpoint of C to origin O)

 

[BiGyElLoWhAt]

Curious, why is Ibar_zz = 0? are you treating the radius to be zero? if that's the case then your md^2 term should be rho(b)(a^2) as a is the distance from the z axis. If you aren't taking the segment to have 0 radius, then Ibar_zz should be non zero, and your term for md^2 should be rho(b)(a+radius_b)^2, not (b^2 + b/2 ^2)

Follow that logic through with C. (how far is it from the z axis?)
Also I believe you want 1/12 mr^2 for that rod, maybe not, I'm not up to par on moments of inertia, but I'm pretty sure a rod pivoted about one end is 1/12 mr^2.

But using the parallel axis theorem is the right place to start.

 

[zeralda21]

I think that since it is not mentioned about any radius we can safely assume it to be zero. What distance? The perpendicular distance? Or using Phytagorean ?

I think this is slighly better but still wrong..

For B:

$I_{zz}=\overline{I}_{zz}+md^2 = \frac{1}{3}(\rho b)(b^2)+(\rho b)(b^2+(\frac{b}{2})^2)=\frac{19}{12}\rho b^3$. I am not sure whether distance d is from the midpoint of B and or just the vertical distance because it is still wrong!

For C:

Correct it should be $\frac{1}{12}(\rho b)(b^2)$ since the distance of the mass particles to the axis varies. Still wrong..

 

[BiGyElLoWhAt]

Oh wait, I didn't read the picture carefully enough. Replace all the a's with b's in the md^2 term

 

[BiGyElLoWhAt]

Ok, so for A, it's cut and dry, $\frac{1}{3} \rho b^3$because$[(mb^2)=(\rho b)b^2]$
B, you have no moment before the axis shift, which leaves $\rho b^3$ after the shift
C you have $\frac{1}{3} mb^2 + md^2 = \frac{4}{3} \rho b^3$

I don't know where you're getting this $\frac{b}{2}$ term from.

Your total I about the z axis should be $\frac{1}{3} \rho b^3 + \rho b^3 +\frac{4}{3} \rho b^3 = \frac{8}{3} \rho b^3$

The only thing that's throwing me for a loop is the C chunk, it's not rotating like a bar with one end on the axis... do you see what I'm saying? So this solution may or may not be good...

 

[BiGyElLoWhAt]

and yes it is the perpendicular distance.

https://www.efunda.com/math/areas/ParallelAxisTheorem.cfm