Do I have to know the General Relativity theory to understand the concept of inertial frame?
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I have read answers on this site as well as the Wikipedia article, but they all add to the confusion. Some people suggest that a freely falling frame is an inertial frame. I learnt in classical mechanics that the frame attached to the surface of the earth is approximately inertial. Are there different definitions of it? The concept of inertial frames seemed easy and intuitive at first, but became complicated as I read more. So I am wondering wether you have to be well versed in general relativity to really understand this concept? If not, can anyone please explain the concept of the inertial frames, and how do we determine wether some real world frame is inertial?
newtonian-mechanics general-relativity reference-frames inertial-frames machs-principle
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add a comment |
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I have read answers on this site as well as the Wikipedia article, but they all add to the confusion. Some people suggest that a freely falling frame is an inertial frame. I learnt in classical mechanics that the frame attached to the surface of the earth is approximately inertial. Are there different definitions of it? The concept of inertial frames seemed easy and intuitive at first, but became complicated as I read more. So I am wondering wether you have to be well versed in general relativity to really understand this concept? If not, can anyone please explain the concept of the inertial frames, and how do we determine wether some real world frame is inertial?
newtonian-mechanics general-relativity reference-frames inertial-frames machs-principle
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2
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Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
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– lalala
Mar 20 at 11:41
1
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No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
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– mathreadler
Mar 20 at 18:35
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Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
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– JosephDoggie
Mar 20 at 18:44
2
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Related: physics.stackexchange.com/q/15349/520
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– dmckee♦
Mar 21 at 0:43
add a comment |
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I have read answers on this site as well as the Wikipedia article, but they all add to the confusion. Some people suggest that a freely falling frame is an inertial frame. I learnt in classical mechanics that the frame attached to the surface of the earth is approximately inertial. Are there different definitions of it? The concept of inertial frames seemed easy and intuitive at first, but became complicated as I read more. So I am wondering wether you have to be well versed in general relativity to really understand this concept? If not, can anyone please explain the concept of the inertial frames, and how do we determine wether some real world frame is inertial?
newtonian-mechanics general-relativity reference-frames inertial-frames machs-principle
$endgroup$
I have read answers on this site as well as the Wikipedia article, but they all add to the confusion. Some people suggest that a freely falling frame is an inertial frame. I learnt in classical mechanics that the frame attached to the surface of the earth is approximately inertial. Are there different definitions of it? The concept of inertial frames seemed easy and intuitive at first, but became complicated as I read more. So I am wondering wether you have to be well versed in general relativity to really understand this concept? If not, can anyone please explain the concept of the inertial frames, and how do we determine wether some real world frame is inertial?
newtonian-mechanics general-relativity reference-frames inertial-frames machs-principle
newtonian-mechanics general-relativity reference-frames inertial-frames machs-principle
edited Mar 20 at 9:45
Qmechanic♦
106k121961227
106k121961227
asked Mar 20 at 9:17
Black balloonBlack balloon
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9118
2
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Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
$endgroup$
– lalala
Mar 20 at 11:41
1
$begingroup$
No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
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– mathreadler
Mar 20 at 18:35
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Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
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– JosephDoggie
Mar 20 at 18:44
2
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Related: physics.stackexchange.com/q/15349/520
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– dmckee♦
Mar 21 at 0:43
add a comment |
2
$begingroup$
Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
$endgroup$
– lalala
Mar 20 at 11:41
1
$begingroup$
No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
$endgroup$
– mathreadler
Mar 20 at 18:35
$begingroup$
Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
$endgroup$
– JosephDoggie
Mar 20 at 18:44
2
$begingroup$
Related: physics.stackexchange.com/q/15349/520
$endgroup$
– dmckee♦
Mar 21 at 0:43
2
2
$begingroup$
Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
$endgroup$
– lalala
Mar 20 at 11:41
$begingroup$
Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
$endgroup$
– lalala
Mar 20 at 11:41
1
1
$begingroup$
No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
$endgroup$
– mathreadler
Mar 20 at 18:35
$begingroup$
No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
$endgroup$
– mathreadler
Mar 20 at 18:35
$begingroup$
Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
$endgroup$
– JosephDoggie
Mar 20 at 18:44
$begingroup$
Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
$endgroup$
– JosephDoggie
Mar 20 at 18:44
2
2
$begingroup$
Related: physics.stackexchange.com/q/15349/520
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– dmckee♦
Mar 21 at 0:43
$begingroup$
Related: physics.stackexchange.com/q/15349/520
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– dmckee♦
Mar 21 at 0:43
add a comment |
3 Answers
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The principle is surprisingly simple. Suppose you are holding an object and you let go of it. What happens to that object? If the object just floats next to you without moving then you are in an inertial frame. If the object accelerates away from you then you are in a non-inertial frame.
Where general relativity comes in is that in GR inertial frames can be surprising. For example if you are sitting in your chair typing on your computer than this seems like it should be an inertial frame. After all, you aren't going anywhere. But if you hold out your pen and let go the pen accelerates downwards away from you, and this shows you are not in an inertial frame. You are in an accelerated frame, where the acceleration is equal to the gravitational acceleration of the Earth.
Now suppose you've just jumped off a cliff and are plummeting downwards (ignore air resistance). This seems like an accelerating frame, but if you now hold out your pen and let go the pen won't move away because both you and the pen are falling with the same acceleration. So this is an inertial frame.
General relativity explains why frames can look inertial to some observers but not to others. The explanation is very simple but involves some maths that won't be familiar to most people so I won't go into it here. The bottom line is not to worry about anything outside your immediate vicinity. You can always tell whether your frame is inertial or not by observing what happens to an object you drop.
If you're interested in finding out more about this I go into more detail in my answers to Two meanings of acceleration in gravitational fields? and Can we determine an absolute frame of reference taking into account general relativity?
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2
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In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
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– 8protons
Mar 20 at 19:15
3
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@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
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– wizzwizz4
Mar 20 at 19:58
2
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But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
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– The Vee
Mar 21 at 7:29
add a comment |
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The basic definition is, that physics has to be the same in every inertial frame (Classical Mechanics). As one gets fictitious forces in accelerated frames (e.g. Centrifugal, Coriolis force), these frames are not inertial. But if the forces in phenomena you want to observe are way bigger than the fictitious forces, you may approximate your frame (on the surface of earth) as inertial. SR and GR further build on this concept but aren't necessary to understand it.
New contributor
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5
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A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
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– gandalf61
Mar 20 at 15:29
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Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
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– JosephDoggie
Mar 20 at 18:45
1
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@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
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– gandalf61
Mar 21 at 11:42
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@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
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– JosephDoggie
Mar 21 at 12:21
1
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@JosephDoggie Agreed - fictitious forces can still be really bad for you !
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– gandalf61
Mar 21 at 13:02
add a comment |
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No, you do not need to understand GR to understand inertialframes. An inertial reference frame is one in which Newton's first law holds. Newton's first law is a core concept in classical mechanics that you probably learned about in high school.
The surface of the Earth is approximately inertial, so long as you treat gravity as a force. An example of a non-rotating frame would be if you're on a merry-go-round: Newton's first law does not hold; free objects appear to move (thanks to centripetal force).
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add a comment |
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3 Answers
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active
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3 Answers
3
active
oldest
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$begingroup$
The principle is surprisingly simple. Suppose you are holding an object and you let go of it. What happens to that object? If the object just floats next to you without moving then you are in an inertial frame. If the object accelerates away from you then you are in a non-inertial frame.
Where general relativity comes in is that in GR inertial frames can be surprising. For example if you are sitting in your chair typing on your computer than this seems like it should be an inertial frame. After all, you aren't going anywhere. But if you hold out your pen and let go the pen accelerates downwards away from you, and this shows you are not in an inertial frame. You are in an accelerated frame, where the acceleration is equal to the gravitational acceleration of the Earth.
Now suppose you've just jumped off a cliff and are plummeting downwards (ignore air resistance). This seems like an accelerating frame, but if you now hold out your pen and let go the pen won't move away because both you and the pen are falling with the same acceleration. So this is an inertial frame.
General relativity explains why frames can look inertial to some observers but not to others. The explanation is very simple but involves some maths that won't be familiar to most people so I won't go into it here. The bottom line is not to worry about anything outside your immediate vicinity. You can always tell whether your frame is inertial or not by observing what happens to an object you drop.
If you're interested in finding out more about this I go into more detail in my answers to Two meanings of acceleration in gravitational fields? and Can we determine an absolute frame of reference taking into account general relativity?
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2
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In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
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– 8protons
Mar 20 at 19:15
3
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
2
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
add a comment |
$begingroup$
The principle is surprisingly simple. Suppose you are holding an object and you let go of it. What happens to that object? If the object just floats next to you without moving then you are in an inertial frame. If the object accelerates away from you then you are in a non-inertial frame.
Where general relativity comes in is that in GR inertial frames can be surprising. For example if you are sitting in your chair typing on your computer than this seems like it should be an inertial frame. After all, you aren't going anywhere. But if you hold out your pen and let go the pen accelerates downwards away from you, and this shows you are not in an inertial frame. You are in an accelerated frame, where the acceleration is equal to the gravitational acceleration of the Earth.
Now suppose you've just jumped off a cliff and are plummeting downwards (ignore air resistance). This seems like an accelerating frame, but if you now hold out your pen and let go the pen won't move away because both you and the pen are falling with the same acceleration. So this is an inertial frame.
General relativity explains why frames can look inertial to some observers but not to others. The explanation is very simple but involves some maths that won't be familiar to most people so I won't go into it here. The bottom line is not to worry about anything outside your immediate vicinity. You can always tell whether your frame is inertial or not by observing what happens to an object you drop.
If you're interested in finding out more about this I go into more detail in my answers to Two meanings of acceleration in gravitational fields? and Can we determine an absolute frame of reference taking into account general relativity?
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2
$begingroup$
In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
$endgroup$
– 8protons
Mar 20 at 19:15
3
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
2
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
add a comment |
$begingroup$
The principle is surprisingly simple. Suppose you are holding an object and you let go of it. What happens to that object? If the object just floats next to you without moving then you are in an inertial frame. If the object accelerates away from you then you are in a non-inertial frame.
Where general relativity comes in is that in GR inertial frames can be surprising. For example if you are sitting in your chair typing on your computer than this seems like it should be an inertial frame. After all, you aren't going anywhere. But if you hold out your pen and let go the pen accelerates downwards away from you, and this shows you are not in an inertial frame. You are in an accelerated frame, where the acceleration is equal to the gravitational acceleration of the Earth.
Now suppose you've just jumped off a cliff and are plummeting downwards (ignore air resistance). This seems like an accelerating frame, but if you now hold out your pen and let go the pen won't move away because both you and the pen are falling with the same acceleration. So this is an inertial frame.
General relativity explains why frames can look inertial to some observers but not to others. The explanation is very simple but involves some maths that won't be familiar to most people so I won't go into it here. The bottom line is not to worry about anything outside your immediate vicinity. You can always tell whether your frame is inertial or not by observing what happens to an object you drop.
If you're interested in finding out more about this I go into more detail in my answers to Two meanings of acceleration in gravitational fields? and Can we determine an absolute frame of reference taking into account general relativity?
$endgroup$
The principle is surprisingly simple. Suppose you are holding an object and you let go of it. What happens to that object? If the object just floats next to you without moving then you are in an inertial frame. If the object accelerates away from you then you are in a non-inertial frame.
Where general relativity comes in is that in GR inertial frames can be surprising. For example if you are sitting in your chair typing on your computer than this seems like it should be an inertial frame. After all, you aren't going anywhere. But if you hold out your pen and let go the pen accelerates downwards away from you, and this shows you are not in an inertial frame. You are in an accelerated frame, where the acceleration is equal to the gravitational acceleration of the Earth.
Now suppose you've just jumped off a cliff and are plummeting downwards (ignore air resistance). This seems like an accelerating frame, but if you now hold out your pen and let go the pen won't move away because both you and the pen are falling with the same acceleration. So this is an inertial frame.
General relativity explains why frames can look inertial to some observers but not to others. The explanation is very simple but involves some maths that won't be familiar to most people so I won't go into it here. The bottom line is not to worry about anything outside your immediate vicinity. You can always tell whether your frame is inertial or not by observing what happens to an object you drop.
If you're interested in finding out more about this I go into more detail in my answers to Two meanings of acceleration in gravitational fields? and Can we determine an absolute frame of reference taking into account general relativity?
edited Mar 20 at 10:09
answered Mar 20 at 10:03
John RennieJohn Rennie
278k44555801
278k44555801
2
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In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
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– 8protons
Mar 20 at 19:15
3
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
2
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
add a comment |
2
$begingroup$
In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
$endgroup$
– 8protons
Mar 20 at 19:15
3
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
2
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
2
2
$begingroup$
In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
$endgroup$
– 8protons
Mar 20 at 19:15
$begingroup$
In your example where you and the pen are falling together w/ same acceleration, isn't that a non-inertial frame?
$endgroup$
– 8protons
Mar 20 at 19:15
3
3
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
$begingroup$
@8protons No. Because actually, you're travelling in a straight (inertial) line through spacetime, which happens to cause you to intersect with the planet. The planet – and everything on it – is accelerating towards you, and not the other way around.
$endgroup$
– wizzwizz4
Mar 20 at 19:58
2
2
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
$begingroup$
But this does not answer why we also use the term "inertial frames" in the case of myself sitting on a chair, when speaking out of the context of GR. Indeed, why the term even existed prior to GR. I'm siding with Paul below, that the definition depends on what is a fictitious force, with gravity being one in GR but not virtually anywhere else. In Newtonian mechanics, for example, it is but an external field that penetrates the frame and affects motion in it, on top of inertia.
$endgroup$
– The Vee
Mar 21 at 7:29
add a comment |
$begingroup$
The basic definition is, that physics has to be the same in every inertial frame (Classical Mechanics). As one gets fictitious forces in accelerated frames (e.g. Centrifugal, Coriolis force), these frames are not inertial. But if the forces in phenomena you want to observe are way bigger than the fictitious forces, you may approximate your frame (on the surface of earth) as inertial. SR and GR further build on this concept but aren't necessary to understand it.
New contributor
$endgroup$
5
$begingroup$
A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
$endgroup$
– gandalf61
Mar 20 at 15:29
$begingroup$
Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
$endgroup$
– JosephDoggie
Mar 20 at 18:45
1
$begingroup$
@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
$endgroup$
– gandalf61
Mar 21 at 11:42
$begingroup$
@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
$endgroup$
– JosephDoggie
Mar 21 at 12:21
1
$begingroup$
@JosephDoggie Agreed - fictitious forces can still be really bad for you !
$endgroup$
– gandalf61
Mar 21 at 13:02
add a comment |
$begingroup$
The basic definition is, that physics has to be the same in every inertial frame (Classical Mechanics). As one gets fictitious forces in accelerated frames (e.g. Centrifugal, Coriolis force), these frames are not inertial. But if the forces in phenomena you want to observe are way bigger than the fictitious forces, you may approximate your frame (on the surface of earth) as inertial. SR and GR further build on this concept but aren't necessary to understand it.
New contributor
$endgroup$
5
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A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
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– gandalf61
Mar 20 at 15:29
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Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
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– JosephDoggie
Mar 20 at 18:45
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@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
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– gandalf61
Mar 21 at 11:42
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@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
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– JosephDoggie
Mar 21 at 12:21
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@JosephDoggie Agreed - fictitious forces can still be really bad for you !
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– gandalf61
Mar 21 at 13:02
add a comment |
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The basic definition is, that physics has to be the same in every inertial frame (Classical Mechanics). As one gets fictitious forces in accelerated frames (e.g. Centrifugal, Coriolis force), these frames are not inertial. But if the forces in phenomena you want to observe are way bigger than the fictitious forces, you may approximate your frame (on the surface of earth) as inertial. SR and GR further build on this concept but aren't necessary to understand it.
New contributor
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The basic definition is, that physics has to be the same in every inertial frame (Classical Mechanics). As one gets fictitious forces in accelerated frames (e.g. Centrifugal, Coriolis force), these frames are not inertial. But if the forces in phenomena you want to observe are way bigger than the fictitious forces, you may approximate your frame (on the surface of earth) as inertial. SR and GR further build on this concept but aren't necessary to understand it.
New contributor
edited Mar 20 at 15:50
New contributor
answered Mar 20 at 9:33
PaulPaul
1598
1598
New contributor
New contributor
5
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A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
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– gandalf61
Mar 20 at 15:29
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Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
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– JosephDoggie
Mar 20 at 18:45
1
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@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
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– gandalf61
Mar 21 at 11:42
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@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
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– JosephDoggie
Mar 21 at 12:21
1
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@JosephDoggie Agreed - fictitious forces can still be really bad for you !
$endgroup$
– gandalf61
Mar 21 at 13:02
add a comment |
5
$begingroup$
A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
$endgroup$
– gandalf61
Mar 20 at 15:29
$begingroup$
Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
$endgroup$
– JosephDoggie
Mar 20 at 18:45
1
$begingroup$
@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
$endgroup$
– gandalf61
Mar 21 at 11:42
$begingroup$
@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
$endgroup$
– JosephDoggie
Mar 21 at 12:21
1
$begingroup$
@JosephDoggie Agreed - fictitious forces can still be really bad for you !
$endgroup$
– gandalf61
Mar 21 at 13:02
5
5
$begingroup$
A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
$endgroup$
– gandalf61
Mar 20 at 15:29
$begingroup$
A great answer ! And a key difference between GR and Newtonian physics is that in GR gravity is a fictitious force like centrifugal force etc. If you need to introduce a gravitational force to account for the movement of objects close to you ("local" objects) then this is a sign that you are not working in an inertial (=free-falling) frame of reference.
$endgroup$
– gandalf61
Mar 20 at 15:29
$begingroup$
Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
$endgroup$
– JosephDoggie
Mar 20 at 18:45
$begingroup$
Long time since I took physics, but I wouldn't want to think of gravity as fictitious myself!
$endgroup$
– JosephDoggie
Mar 20 at 18:45
1
1
$begingroup$
@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
$endgroup$
– gandalf61
Mar 21 at 11:42
$begingroup$
@JosephDoggie It may seem counter-intuitive, but a key lesson of physics is that our intuition, based on a limited range of human experiences, is often false. Wikipedia's article on "Fictitious force" says "Einstein was able to formulate a theory with gravity as a fictitious force and attributing the apparent acceleration of gravity to the curvature of spacetime. This idea underlies Einstein's theory of general relativity."
$endgroup$
– gandalf61
Mar 21 at 11:42
$begingroup$
@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
$endgroup$
– JosephDoggie
Mar 21 at 12:21
$begingroup$
@gandalf61 Thanks. That's interesting. But when traveling near cliffs (etc) please stick to Newtonian physics!
$endgroup$
– JosephDoggie
Mar 21 at 12:21
1
1
$begingroup$
@JosephDoggie Agreed - fictitious forces can still be really bad for you !
$endgroup$
– gandalf61
Mar 21 at 13:02
$begingroup$
@JosephDoggie Agreed - fictitious forces can still be really bad for you !
$endgroup$
– gandalf61
Mar 21 at 13:02
add a comment |
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No, you do not need to understand GR to understand inertialframes. An inertial reference frame is one in which Newton's first law holds. Newton's first law is a core concept in classical mechanics that you probably learned about in high school.
The surface of the Earth is approximately inertial, so long as you treat gravity as a force. An example of a non-rotating frame would be if you're on a merry-go-round: Newton's first law does not hold; free objects appear to move (thanks to centripetal force).
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add a comment |
$begingroup$
No, you do not need to understand GR to understand inertialframes. An inertial reference frame is one in which Newton's first law holds. Newton's first law is a core concept in classical mechanics that you probably learned about in high school.
The surface of the Earth is approximately inertial, so long as you treat gravity as a force. An example of a non-rotating frame would be if you're on a merry-go-round: Newton's first law does not hold; free objects appear to move (thanks to centripetal force).
$endgroup$
add a comment |
$begingroup$
No, you do not need to understand GR to understand inertialframes. An inertial reference frame is one in which Newton's first law holds. Newton's first law is a core concept in classical mechanics that you probably learned about in high school.
The surface of the Earth is approximately inertial, so long as you treat gravity as a force. An example of a non-rotating frame would be if you're on a merry-go-round: Newton's first law does not hold; free objects appear to move (thanks to centripetal force).
$endgroup$
No, you do not need to understand GR to understand inertialframes. An inertial reference frame is one in which Newton's first law holds. Newton's first law is a core concept in classical mechanics that you probably learned about in high school.
The surface of the Earth is approximately inertial, so long as you treat gravity as a force. An example of a non-rotating frame would be if you're on a merry-go-round: Newton's first law does not hold; free objects appear to move (thanks to centripetal force).
answered Mar 21 at 10:38
AllureAllure
1,956722
1,956722
add a comment |
add a comment |
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Just to add one point when you try later to learn GR. GR basically talks about how much the deviation from an inertial frame when you have gravity, en.wikipedia.org/wiki/Geodesic_deviation thats basically all there is to the effect of a non vanishing Riemann tensor.
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– lalala
Mar 20 at 11:41
1
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No this should not be necessary. Already in Newtonian mechanics the concept of inertial frame exists.
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– mathreadler
Mar 20 at 18:35
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Agree with @mathreader. In fact, I would try to think about the Newtonian concept first, before moving on to General Relativity; I'd even apply this to the whole physics, not just inertial frame.
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– JosephDoggie
Mar 20 at 18:44
2
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Related: physics.stackexchange.com/q/15349/520
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– dmckee♦
Mar 21 at 0:43