Is Gravity an Inertial Force According to the Equivalence Principle?

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Discussion Overview

The discussion revolves around the nature of gravity in relation to the equivalence principle, exploring whether gravity can be considered an inertial force similar to fictitious forces in non-inertial frames. Participants examine the distinctions between real forces and apparent forces, particularly in the context of Newtonian mechanics and General Relativity (GR).

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that gravity can be viewed as an inertial force due to the equivalence principle, likening it to Coriolis and centrifugal forces in non-inertial frames.
  • Others argue that in Newtonian mechanics, gravity is a real force, not an inertial one, and that mixing concepts from GR and Newtonian mechanics may lead to confusion.
  • A participant presents a mathematical transformation in Newtonian mechanics that suggests gravity could be treated as an inertial force under certain conditions.
  • Another participant points out that while one can set the acceleration of one object to zero, one cannot do so for both objects interacting gravitationally.
  • Some participants discuss the implications of the Riemann tensor and curvature in distinguishing real forces from fictitious ones, suggesting that gravity's nature as a geometric phenomenon complicates its classification as an inertial force.
  • There is a mention that the equivalence principle could be interpreted in various ways, with some viewing it as a fundamental aspect of GR and others as a coincidence in Newtonian mechanics.
  • A participant questions the definition of gravity, referencing Einstein's view of gravity as a geometric property of spacetime rather than a force.
  • Another participant agrees that the concept of "acceleration due to gravity" becomes problematic due to the equivalence principle.

Areas of Agreement / Disagreement

Participants express multiple competing views on whether gravity should be classified as an inertial force or a real force, and the discussion remains unresolved with no consensus reached.

Contextual Notes

The discussion involves complex interpretations of the equivalence principle, the distinction between real and fictitious forces, and the implications of mathematical transformations in different frameworks. There are unresolved assumptions regarding the definitions and implications of these concepts.

dulrich
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I've often thought that one way to restate the equivalence principle is that the force of gravity is a manifestation of using a frame that is not in free-fall. In other words, it's an inertial force akin to the Coriolis and centrifugal forces in a rotating frame of reference.

However, I just read the following quote from http://plato.stanford.edu/entries/Newton-principia/#NewLawMot
Real forces, in contrast to such apparent forces as Coriolis forces (of which Newton was entirely aware, though of course not under this name), are forces for which the third law, as well as the first two, hold, for only by means of this law can real forces and hence changes of motion be distinguished from apparent ones.

For some reason, I've never seen the third law being invoked to distinguish real and "apparent" forces.

Now, the deflection of objects in a gravitational field is due to the curvature of spacetime, so I should think of it as inertial. But spacetime wouldn't be curved except a second object were doing the curving. It truly is an interaction between the two via the intermediary of the gravitational field. Hence, it is not really inertial in the same sense as the Coriolis force.

So I guess gravity stands alone: it's the only inertial force that is also "real".

Does this make any sense?
 
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dulrich said:
For some reason, I've never seen the third law being invoked to distinguish real and "apparent" forces.
It's an excellent way to make the distinction, in Newtonian mechanics. In Newtonian mechanics, real forces are made by one object acting on another object. If a "force" isn't made by one object on another object, then you can't even define Newton's third law.

dulrich said:
So I guess gravity stands alone: it's the only inertial force that is also "real".
A general comment on your OP is that you seem to be mixing statements about GR and Newtonian mechanics, which isn't necessarily valid.

In Newtonian mechanics, gravity is not an inertial force, it's a real force.

In GR, the gravitational field is indeed treated differently from other fields (it's the only one treated geometrically), but force isn't even a really useful concept.
 
But in Newtonian mechanics I can do the coordinate transformation

[tex] x^i \rightarrow x^i + \frac{1}{2}a^i t^2[/tex]

where a is a uniform acceleration (and this transfo is ofcourse not an element of the Galilei group). My "geodesic equation" x-dubbeldot is zero becomes

[tex] \ddot{x}^i + a^i = 0[/tex]

If I now use the equivalence principe (which is perfectly allowed in classical mechanics) I rewrite for the gravitational potential phi

[tex] \ddot{x}^i + \frac{\partial\phi}{\partial x^i} = 0[/tex]

Can't I regard gravity as being an inertial force in this sense?
 
haushofer said:
Can't I regard gravity as being an inertial force in this sense?

Suppose planets A and B are interacting gravitationally. You can do a transformation like this to set one of the planets' accelerations equal to zero, but you can't make both accelerations vanish, just one of them.
 
I suppose I do not see the big dichotomy. Rewrite Newton's laws in a geometric form (Newton-Cartan) and it is "suddenly" force free?
 
bcrowell said:
Suppose planets A and B are interacting gravitationally. You can do a transformation like this to set one of the planets' accelerations equal to zero, but you can't make both accelerations vanish, just one of them.

That's true, that's something I haven't realized :)
 
The difference between a real gravitational force and a fictious inertial force is that the Riemann tensor does not vanish in a region of space-time when there is a real force, as opposite to a fictious force. The reason is that when there is curvature it is impossible to find a GCT such that the metric tensor is Minkowskian everywhere. When considering a fictious inertial force such a trafo is possible and the observer concludes the force is not a real one. So you should be careful to consider gravitation as an intertial phenomenon. Curvature is an observer independent feature of physical reality, whereas intertial forces are by definition not. (The mathematical reason being that you cannot fix the second order derivative of the metric completely by changing coordinates).
 
dulrich said:
I've often thought that one way to restate the equivalence principle is that the force of gravity is a manifestation of using a frame that is not in free-fall.
The EP could also be a weird coincidence, like in Newonian mechanics. Your statement is the core of GR, where the EP is interpreted that way.
hendriko373 said:
So you should be careful to consider gravitation as an intertial phenomenon.
Of course. Gravitational force being fictitious does not mean that there's no gravity.
 
sorry pls correct me if I am wrong.

Didn't Einstein say that Gravity is nothing but a geometry curved only? It is NOT a force and we are living in curved space.

isn't it?
Alex
 
  • #10
Yes. Due to the equivalence principle the notion of "acceleration due to gravity" is ill-defined.
 

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