What are non-inertial frames of reference?

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Discussion Overview

The discussion centers around the concept of non-inertial frames of reference, exploring definitions, examples, and implications in both classical and relativistic contexts. Participants examine the nature of acceleration in relation to reference frames and how this affects observations and measurements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants propose that a non-inertial frame of reference is one that is undergoing non-zero acceleration.
  • Others argue that a more precise definition involves the relationship between forces and motion, suggesting that a non-inertial frame is one where objects with no net force acting on them do not maintain a constant velocity.
  • Examples of non-inertial frames include a coordinate system attached to a rotating turntable or an accelerating rocket, where observers at different positions may experience time differently due to acceleration.
  • A participant emphasizes the local nature of accelerated reference frames, suggesting that their applicability diminishes beyond certain distances.
  • Concerns are raised about the clarity of definitions, particularly regarding what it means for a frame to "undergo acceleration," as frames are conventions for assigning coordinates rather than physical entities.
  • One participant attempts to define a reference frame in terms of origin and unit vectors, noting that in non-inertial frames, these vectors may depend on time.
  • Another participant references a source that frames non-inertial frames in the context of Newton's first law, suggesting that such frames violate this law by not allowing force-free objects to move in straight lines at constant speeds.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of non-inertial frames, with no clear consensus reached on a singular definition or understanding. The discussion remains unresolved regarding the most accurate characterization of non-inertial frames.

Contextual Notes

Some definitions and examples provided may depend on specific interpretations of classical mechanics versus relativistic contexts, and there are unresolved questions about the implications of acceleration on reference frames.

General Scientist
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I am reading through a textbook on AP Physics, and I came across a few references to non-inertial frames of reference. It doesn't clearly say what a non-inertial frame of reference is. Based on the examples it gives, I assume that it is a frame of reference where the observer is experiencing acceleration.

Am I right?
 
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A non-inertial frame of reference is one that is undergoing a non zero acceleration.
 
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QuantumQuest said:
A non-inertial frame of reference is one that is undergoing a non zero acceleration.
Thanks a lot!
 
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An example of a noninertial frame would be a coordinate system attached to and rotating with a spinning turntable.
 
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QuantumQuest said:
A non-inertial frame of reference is one that is undergoing a non zero acceleration.

I think one should be cautios here. As is pointed out in MTW "Gravitation" (6.3) the accelerated reference frame is a local thing - it does not cover the whole space. What does it mean? Well, according to my back-of-the-envelope calculation, if you were to stand at the front of the rocket of length ##L## which is accelerating with uniform acceleration ##a##, and your friend would stay at the very back of the same rocket, your clocks would tick differently. The relationship between your (##\tau_1##) and your friend's (##\tau_2##) proper times would be:

##\tau_2\approx(1-\frac{aL}{c^2})\tau_1## in the limit of ##a\to0##

Where ##c## is the speed of light. So as the space you include in your "accelerated reference frame" is small (##aL/c^2 \ll 1##), you can talk about a reference frame. Once you go beyond distance ##c^2/a##, the accelerated reference frame no longer makes sense.
 
vsv86 said:
I think one should be cautios here. As is pointed out in MTW "Gravitation" (6.3) the accelerated reference frame is a local thing - it does not cover the whole space. What does it mean? Well, according to my back-of-the-envelope calculation, if you were to stand at the front of the rocket of length ##L## which is accelerating with uniform acceleration ##a##, and your friend would stay at the very back of the same rocket, your clocks would tick differently. The relationship between your (##\tau_1##) and your friend's (##\tau_2##) proper times would be:

##\tau_2\approx(1-\frac{aL}{c^2})\tau_1## in the limit of ##a\to0##

Where ##c## is the speed of light. So as the space you include in your "accelerated reference frame" is small (##aL/c^2 \ll 1##), you can talk about a reference frame. Once you go beyond distance ##c^2/a##, the accelerated reference frame no longer makes sense.

What I really don't understand is why did you quote my post. The question of the OP was (quoting from post #1)

General Scientist said:
... It doesn't clearly say what a non-inertial frame of reference is. Based on the examples it gives, I assume that it is a frame of reference where the observer is experiencing acceleration.

Am I right?

Is a non-inertial frame of reference something different from what I wrote?
 
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QuantumQuest said:
Is a non-inertial frame of reference something different from what I wrote?
You wrote "A non-inertial frame of reference is one that is undergoing a non zero acceleration."

I suggest that a more generally accepted definition is something along the lines of: An inertial frame is one in which a body with no net force acting on it does not accelerate. Conversely, if an object with no net force acting on it does accelerate in a given frame, then that frame is not inertial. Examples of each are left as an exercise for the reader - and everyone is reminded that this is the classical physics forum, so gravity is a considered a real force.

The problem with your definition is that it is not at all clear what it means to speak of a "frame undergoing acceleration". Objects can have acceleration, but a frame is just a convention for assigning time and space coordinates to events, and it's not clear how to accelerate a convention. That doesn't stop people from talking about "accelerated reference frames", but that's because natural language sacrifices precision for convenience.
 
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vsv86 said:
I think one should be cautious here. As is pointed out in MTW "Gravitation" (6.3) the accelerated reference frame is a local thing - it does not cover the whole space...
This is correct, and it points out one of the pitfalls in the "accelerated frame" concept... But MTW (for the uninitiated, that's a graduate-level general relativity textbook, and one of the more demanding ones at that) would not be my go-to source for a B-level thread in the classical physics subforum.
 
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This thread is open again after removing a long digression.
 
  • #10
General Scientist said:
I am reading through a textbook on AP Physics, and I came across a few references to non-inertial frames of reference. It doesn't clearly say what a non-inertial frame of reference is. Based on the examples it gives, I assume that it is a frame of reference where the observer is experiencing acceleration.

Am I right?

How about we try to define a reference frame? I will not try to be rigrous here, but merely gather the things I think are necessary for this concept.

Nothwithstanding my previous digression (I agree it was a digression - my bad) to relativity, in Newtonian mechanics we can define a reference frame as an origin ##O## and a set of unit vectors, ##\hat{\vec{a}}, \hat{\vec{b}}, \hat{\vec{c}}##, such that any vector ##\vec{v}## in space can be written as a linear combination of this set ##\vec{v}=v_a\hat{\vec{a}}+v_b\hat{\vec{b}}+v_c\hat{\vec{c}}##.

Next we can define an "observer in the reference frame" as observer who's position is (relative to ##O##): ##\vec{u}=u_a\hat{\vec{a}}+u_b\hat{\vec{b}}+u_c\hat{\vec{c}}##, where ##u_{a,b,c}## are constant in time.

Now the difference between the intertial reference frame and a non-intertial one is simply that the basis vectors depend on time (t): ##\hat{\vec{a}}=\hat{\vec{a}}(t)## and same for others. More precisely, for a non-inertial reference frame the dependence of the basis vectors on time, should be at least quadratic (so that second derivative should not vanish).

We can now easily deduce that the observer in the non-intertial reference will be accelerating.

This all may seem quite trivial, but the TC complained about the lack of definition of the reference frame. I think my little sketch above contains sufficient flexibility to cover all exercises with non-inertial reference frames I have seen thusfar.

PS: Of course on must also allow for unit-vectors to depend on position to have the full generality of treatment.
 
  • #11
General Scientist said:
I came across a few references to non-inertial frames of reference. It doesn't clearly say what a non-inertial frame of reference is.
I would tend to take the approach outlined here:

http://farside.ph.utexas.edu/teaching/336k/Newtonhtml/node9.html

Basically, the idea is to understand Newton’s first law as a definition of an inertial frame. Then a non inertial frame is simply one that violates Newton’s first law such that force free objects do not travel in a straight line with constant speed.
 
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  • #12
I want to apologize for digressing in this thread. It was really not my intention to do so.

Nugatory said:
You wrote "A non-inertial frame of reference is one that is undergoing a non zero acceleration."

I suggest that a more generally accepted definition is something along the lines of: An inertial frame is one in which a body with no net force acting on it does not accelerate. Conversely, if an object with no net force acting on it does accelerate in a given frame, then that frame is not inertial. Examples of each are left as an exercise for the reader - and everyone is reminded that this is the classical physics forum, so gravity is a considered a real force.

The problem with your definition is that it is not at all clear what it means to speak of a "frame undergoing acceleration". Objects can have acceleration, but a frame is just a convention for assigning time and space coordinates to events, and it's not clear how to accelerate a convention. That doesn't stop people from talking about "accelerated reference frames", but that's because natural language sacrifices precision for convenience.

Yes, you're absolutely right. I thought that it was sufficient to write it like I did i.e. that it would convey the meaning I intended to, but yes, I think that I should phrase it in a better way so I apologize for this too.
 
  • #13
QuantumQuest said:
A non-inertial frame of reference is one that is undergoing a non zero acceleration.

Don't you need a second system to define the acceleration of the first, which only raises the question if the second system is inertial?

Now you could argue that there exist accelerometers. But they use Newton's laws to work, which already require an inertial frame in their assumptions. This seems like a circular argument.
 
  • #14
Possibly useful:
Frames of Reference (1960) .. go to 13m27s
 
  • #15
greypilgrim said:
Don't you need a second system to define the acceleration of the first, which only raises the question if the second system is inertial?

Now you could argue that there exist accelerometers. But they use Newton's laws to work, which already require an inertial frame in their assumptions. This seems like a circular argument.

Yes, all motion is relative but in a non-inertial frame of reference an object (having no force acting on it) does accelerate while in an inertial frame of reference it does not.
 
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  • #16
greypilgrim said:
Now you could argue that there exist accelerometers. But they use Newton's laws to work, which already require an inertial frame in their assumptions. This seems like a circular argument.
Accelerometers may use Newton’s laws to work, but that needn’t be part of their definition. They can be defined simply by instructions to build one. Similarly with clocks, rulers, and force plates. That eliminates the circularity.

However, a little bit of circularity is not in and of itself a problem, as long as everything is self consistent and subject to experimental verification and falsification.
 

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