Mechanics - moment, Euler's second law

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SUMMARY

The discussion focuses on deriving differential equations for a mechanical system involving a rolling ring and a half-circle inside it, utilizing Euler's second law. The user has successfully completed the kinematic analysis and is attempting to calculate moments using the equation M = I*α + rxma. Key challenges include determining the impact of the articulated pole on the half-circle and establishing correct moment equations for both the half-circle and the entire system. The user seeks confirmation of their moment equations to proceed with deriving the differential equations.

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  • Understanding of Euler's second law in mechanics
  • Familiarity with kinematic analysis of mechanical systems
  • Knowledge of moment of inertia calculations
  • Proficiency in MATLAB for simulating mechanical systems
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bjornebarn
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Homework Statement



Hello! :)
I got stuck on a problem I got for my physics class, where I am supposed to derive the differential equations for a mechanical system (x'' =, θ'' =, and φ'' =) , and then simulate how the system behaves in matlab.

Here is a picture: http://forumbilder.se/show.aspx?iid=c72201260720P7323

As you can see, there is a ring, which can roll on the ground. The ring has mass m1, radius R and center of mass G1.
Inside the ring is a half-circle, that can move frictionlessly inside the ring. It has a mass m2, radius R and center of mass G2.
At the center of mass G2 a pole is articulated, so it can move freely relative to the half-sphere. It has a uniform mass m3 and length l.

The hint for the problem is to be careful in selecting the moment points for Euler II, so that no unknown forces will have to be derived using Euler I (F=ma).

Homework Equations



Euler II:
M = I*α + rxma

The Attempt at a Solution



I have finished the kinematical analysis, and it should be correct.

First I try to calculate the moment for the pole, around the point G2, using Euler II:

G2: -m3 * g * l/2 * sin(φ) = I_G3 * φ'' + (-l/2 * sin(φ) x^ + l/2 * cos(φ) y^) x (-m3*g y^)
<=> φ'' = -(m3 * g * l * sin(φ)) / I_G3

Unsure from here:
The problem I have are for the systems half-circle + pipe, and for the whole system. I am also not quite sure how the pipe will affect the half-sphere, so I named the force ξ, to deal with it later. Here is my attempt though, for the half-circle + pipe:

G1: -(m2*g + ξ)*d*sin(θ) = I_G2 * θ'' + (d*sin(θ) x^ - d*cos(θ) y^) x m*(a_G2x x^ + a_G2y y^)

Here a_G2x and a_G2y are from the kinematical analysis, the acceleration for G2 in x and y respectively.

Lastly, I try the same for the whole system, around the moment point M, which I put where the ring is in contact with the ground:

M: -(m2*g + ξ)*d*sin(θ) = something + (d*sin(θ) x^ + (R-d)*cos(θ) y^) x m*(a_G2x x^ + a_G2y y^)

So, this is how far I get... I am very grateful for any help that you can give me! :=)
You don't need to give me the answer, as long as I am sure I have the correct moment equations, I should be able to derive the differential equations.

Thank you! :)
 
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