Understanding Inertia to its Uses and Importance in Physics

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SUMMARY

The discussion centers on the concept of inertia, emphasizing its role as a property of bodies that maintain their state of motion or rest unless acted upon by external forces. Inertia is recognized as a useful tool in simplifying calculations, particularly in non-inertial reference frames. However, some participants argue against referring to inertia as a force, citing Newton's laws and the absence of a reaction force for the term "M*A." The conversation highlights the ongoing debate about the utility of fictitious forces in physics, particularly in the context of D'Alembert's principle and accelerated reference frames.

PREREQUISITES
  • Understanding of Newton's Laws of Motion
  • Familiarity with non-inertial reference frames
  • Knowledge of D'Alembert's principle
  • Basic concepts of fictitious forces in physics
NEXT STEPS
  • Research the implications of Newton's 2nd and 3rd laws on fictitious forces
  • Study the application of D'Alembert's principle in dynamics
  • Explore the role of inertia in non-inertial reference frames
  • Investigate common misconceptions about forces in physics
USEFUL FOR

Physics students, educators, and professionals interested in classical mechanics and the application of inertia in problem-solving within non-inertial frames.

bobie
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The force of inertia is the property common to all bodies that remain in their state, either at rest or in motion, unless some external cause is introduced to make them alter this state.Is the concept of inertia still used? When is it useful as a fictitious force?

Can you list a few situations in which, if we didn't use this tool we might be in difficulty?
 
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I would disagree with the previous responses and say that it is NEVER useful as a force. Consider these ideas, please:

1. Newton's 2nd law says Sum F = M * A
This means that all of the real forces appear on the left side (or in the first term if you want to set it all to zero). The M * A is not a force, and therefore should not appear in the force sum.

2. There will be some who will say, "well, it looks just like a force when we look at the 2nd law," and that is true. But the 3rd law says that for every action (force) there is an equal and opposite reaction (force) somewhere in the universe. There simply is no reaction to an "M*A" force, so it must not be a force.

Simon noted above that it is useful "anytime it simplifies the calculation." That is hard to argue with except to ask, "how does it simplify the calculation?" The usual effect to cause the user to pay less than full attention to the expression of the acceleration (usually assuming an unduly simple form), so that it leads to an error.

I strongly suggest, leave D'Alembert in his grave and stick with Newton (or Lagange).
 
Useful or not it is sometimes still used - yes, imagine my shock.
We get a lot of questions here about accelerated reference frames where the calculations are best done in those frames.
... but I prefer not to use the phrase "force of inertia" to help people with them as it's too confusing.
 
Dr.D said:
2. There will be some who will say, "well, it looks just like a force when we look at the 2nd law," and that is true. But the 3rd law says that for every action (force) there is an equal and opposite reaction (force) somewhere in the universe. There simply is no reaction to an "M*A" force, so it must not be a force.

Well, this is only because such an inertial 'force' does not act upon a body from any external body (except, perhaps a la Newton, from absolute space). I'm not sure the 3rd law is then applicable to it, although this obviously depends heavily on the particular formulation of this law. I'd prefer something like F_{AB} = - F_{BA} rather than the colloquial equal and opposite reaction...
 

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