Formula for fictitious moments

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SUMMARY

This discussion focuses on the formulation of fictitious moments experienced by solid bodies in non-inertial frames, building on established concepts of fictitious forces such as Euler, centrifugal, and Coriolis forces. The formulas for these forces are provided, including Euler force (FE = -m ⋅ dΩ/dt × OP), centrifugal force (FCe = -m ⋅ Ω × (Ω × OP)), and Coriolis force (FCo = -m ⋅ 2Ω × V). The author suggests using the action principle and Lagrangian mechanics to derive fictitious moments, particularly in the context of gyrocompasses, referencing both Wikipedia and personal lecture notes for further exploration.

PREREQUISITES
  • Understanding of fictitious forces in non-inertial frames
  • Familiarity with Lagrangian mechanics
  • Knowledge of inertia tensors and their application in solid mechanics
  • Basic concepts of rotational dynamics
NEXT STEPS
  • Study the derivation of fictitious forces in non-inertial frames
  • Explore Lagrangian mechanics with a focus on center-mass coordinates
  • Research the theoretical treatment of gyrocompasses and their applications
  • Examine inertia tensors and their role in calculating fictitious moments
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Students and professionals in physics, mechanical engineering, and applied mathematics, particularly those interested in dynamics and the effects of non-inertial reference frames on solid bodies.

taalf
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Hi All,

Everyone knows so called "fictitious" forces, also known as "inertial" forces. They are forces felt by some mass point placed in a non-inertial frame. For example: a ball in a moving car or in a carousel.

Maybe most intuitive fictitious forces are centrifugal forces, but there are also Euler forces and Coriolis forces. Formulas for such forces are well known (bold means "vector"):

Euler force: FE = -m ⋅ dΩ/dt × OP
Centrifugal force: FCe = -m ⋅ Ω × (Ω × OP)
Coriolis force: FCo = -m ⋅ 2Ω × V

with:
m the mass of the point,
Ω the rotation vector of the non inertial frame,
OP the position of the point in the non inertial frame,
V the velocity of the point in the non inertial frame.

Know, consider the object is not a mass point, but some solid with a given inertia tensor:
___|Ixx Ixy Ixz|
I = |Iyx Iyy Iyz|
___|Izx Izy Izz|

This solid, put in a non inertial frame, should not only feel fictitious forces, but also fictitious moments.

The question is: how to formulate them?
 
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That's a really interesting question. I guess it's quite complicated. That's why I right away would use the action principle and write down the Lagrangian using center-mass coordinates and Euler angles between body-fixed and space-fixed Cartesian bases but with the space-fixed frame as a non-inertial (rotating) reference frame.

A special case of this is the theoretical treatment of the gyrocompass, which you can find in the Wikipedia (although I found this more complicated than necessary):

https://en.wikipedia.org/wiki/Gyrocompass

My own attempt to explain it, you can find in my lecture notes on mechanics, which are, however, in German (p. 129ff)

https://th.physik.uni-frankfurt.de/~hees/publ/theo1-l3.pdf
 

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