I Can time be another basis vector under Galilean relativity?

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The discussion critiques a video that attempts to frame Galilean relativity in terms of spacetime as a vector space, suggesting that this approach obscures rather than clarifies the transition to special relativity (SR). It argues that in Galilean relativity, time and space are fundamentally different, with time not being a homogeneous unit that can be combined with spatial dimensions. The concept of a Galilean spacetime interval is deemed impractical and lacking in utility, as it does not solve any real problems. Additionally, the absence of an invariant speed in Galilean relativity contrasts with SR, where time and space are homogenized through the speed of light. Ultimately, the discussion emphasizes that while mathematical representations may be convenient, they do not capture the distinct nature of time in the Galilean framework.
  • #121
robphy said:
These authors appear to think such terms are also appropriate.
I don't think those authors are using the terms the way you were trying to use them.

Schutz appears to be using "spatial components" to mean the components ##U_x##, ##U_y##, ##U_z## of the 4-velocity ##U## in some particular frame. You're trying to use terms like "component" to refer to a complete 4-vector, which is what I'm objecting to.

Geroch doesn't use the word "component" or "part" or similar words, except right at the end of the quote you give (and I would object to his usage there on the grounds that it's not consistent with his usage elsewhere in that quote). He uses the word "displacement", which suggests a complete 4-vector, not a piece of one, which is of course consistent with the equation he gives, which is basically the same one we have written here, expressing the 4-velocity of particle 1 in terms of the sum of two 4-vectors: one parallel to the 4-velocity of particle 2 and one orthogonal to it.

Wald uses "components" the same way Schutz does; see above.

MTW uses "spatial part" to refer to a 3-vector, not a 4-vector.

Hartle and Rindler appear to be using "components" the same way Schutz does; see above.
 
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  • #122
robphy said:
What makes them different is that
  • the Minkowski metric defines the unit tangent vector
    so that the tips of the 4-velocities from an event lie on a hyperbola/hyperboloid.
  • the Galilean metric defines the unit tangent vector
    so that the tips of the 4-velocities from an event lie on a hyperplane.
  • just as the Euclidean metric defines the unit tangent vector
    so that the tips of the unit vector from a point lie on a circle/sphere.
One other difference is that in the Galilean case there is no spacetime metric; the "Galilean metric" you refer to is the temporal metric, and there is a separate spatial metric. So there is no well-defined concept of "orthogonality" between timelike vectors and spacelike vectors (and of course there are no null vectors).
 
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  • #123
Saw said:
is that tangent space really a "vector space"?
Yes, definitely. You can check for yourself that it satisfies all of the vector space axioms.
 
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  • #124
Saw said:
I am assuming a world with no acceleration where the tangent is always parallel to the worldline.
A tangent vector is always parallel to the worldline at the point where it is tangent.

Proper acceleration means path curvature, i.e., the tangent vector is not parallel transported along the worldline.
 
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  • #125
Saw said:
For me, at Galilean level, time is a scalar
That is true, but you have to carefully consider what that means. Time being a scalar means that there is an invariant number ##t## at every event, which doesn't change when you change inertial frames. But you can still pick out a "time axis" for each inertial frame by simply using the worldline of its spatial origin.

Saw said:
and time axis does not overlap the worldline
The "time axis" must always overlap some worldline, because some worldline will always be the time axis (the worldline of the spatial origin of whichever frame you have chosen).

If you make a Galilean boost from one inertial frame to another, the planes of simultaneity stay the same, but, heuristically, they "slide" horizontally relative to one another, so that some different worldline is now vertical and becomes the time axis of the new frame. This worldline will be the worldline of the spatial origin of the new frame.

Saw said:
I would see concepts like Galilean 4-velocity as a "place-holder"
No, they're not. They're perfectly well-defined in Galilean relativity. They don't work the same as they do in SR, but that doesn't mean they're not well-defined and valid.
 
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  • #126
Saw said:
"tangent space" where the time basis vector is the 4-velocity with first component being 1 (dimensionless) and rest of components = 0 (also dimensionless)?
(…j
is that tangent space really a "vector space"?

PeterDonis said:
Yes, definitely. You can check for yourself that it satisfies all of the vector space axioms.

Tangent spaces in general, yes. But this particular tangent space is supposed to be made of 4-velocity vectors, right? And if I look at the first axiom of a vector space and try to add one 4-velocity vector to another, I have doubts. Can you do that?
 
  • #127
PeterDonis said:
The "time axis" must always overlap some worldline, because some worldline will always be the time axis (the worldline of the spatial origin of whichever frame you have chosen).

If you make a Galilean boost from one inertial frame to another, the planes of simultaneity stay the same, but, heuristically, they "slide" horizontally relative to one another, so that some different worldline is now vertical and becomes the time axis of the new frame. This worldline will be the worldline of the spatial origin of the new frame..
If you told me that you can paint it there, overlapping the worldlines, well, the paper accepts anything. But if you affirm that this has a “heuristic“ sense, which one is it? Is it that Bob’s wristwatch is at rest with Bob, so it is always spatially located by the origin of his frame? But that is not “enabling us to learn or discover“ anything about Galilean time, which is Newton’s absolute time and is the same regardless the motion of the clock that registers it. What other heuristic sense do you have in mind?
 
  • #128
Saw said:
I would see concepts like Galilean 4-velocity as a "place-holder". i.e. something that does not really exist in Galilean relativity but is holding a place for another thing that will appear in SR, when you actually need to move forward to the latter.

PeterDonis said:
No, they're not. They're perfectly well-defined in Galilean relativity. They don't work the same as they do in SR, but that doesn't mean they're not well-defined and valid.
Well-defined? Yes, Galilean 4-velocity is 3-velocity to which one adds a coordinate time over proper time component which is 1 in all reference frames, since in this context both things coincide. What is the added value of this concept, i.e. its practical use? If it were none, it would fit in the notion of “place-holder”, i.e. an idea for which in this context there is no practical use but may have one once that you move into another territory where coordinate time and proper time do differ.
 
  • #129
Saw said:
Can you do that?
Sure, just add their components as you would with any pair of vectors.

Saw said:
this particular tangent space is supposed to be made of 4-velocity vectors, right?
Not just 4-velocity vectors, no. All vectors at a point. A vector does not have to have unit norm.
 
  • #130
Saw said:
Galilean 4-velocity is 3-velocity to which one adds a coordinate time over proper time component which is 1 in all reference frames
If you allow the 3-velocity to change if you change frames, according to the Galilean boost equations, yes, this is one way of defining Galilean 4-velocity.

Saw said:
What is the added value of this concept, i.e. its practical use?
What is the practical use of any mathematical definition? It depends on who is using it and what they are using it for.
 
  • #131
Saw said:
if you affirm that this has a “heuristic“ sense
All I meant by "heuristic" is that I was giving an ordinary language description, not the actual math. Don't read too much into it.
 
  • #132
PeterDonis said:
Sure, just add their components as you would with any pair of vectors.

I looked at Wikipedia entry for 4-velocity and it does say (at a note) that a tangent space is a vector space (like the entry about tangent space itself), but the thing is that it also says this with regard to 4-velocity: "addition of two four-velocities does not yield a four-velocity: the space of four-velocities is not itself a vector space."

How does that match with 4-velocity being the time basis vector, given that what you do with basis vectors is precisely scaling them?

PeterDonis said:
Not just 4-velocity vectors, no. All vectors at a point. A vector does not have to have unit norm.
I guess you refer to other derivatives, like 4-force or 4-acceleration... But focusing again on 4-velocity, which is our object of interest because it i said to be at least one option for the time basis vector, I would come back to the issue mentioned before: a basis vector, in a normalized basis, must be unitary but then its role is being scaled by a certain coefficient...

Furthermore, the fact that it is unitary does not mean that it is not a unit of something, i.e. a second, a meter or whatever, how is that consistent with being dimensionless?

To sum up, I have difficulties to see the role of the 4-velocity as the time basis vector. But since this concerns SR and not in particular the Galilean version of the 4-velocity, should I maybe start another thread? Before that, is there any source I should read to know more about the matter?
 
  • #133
In special relavity the four-velocity is by definition
$$u^{\mu}=\frac{\mathrm{d} x^{\mu}}{\mathrm{d} \tau},$$
which implies the constraint
$$u_{\mu} u^{\mu}=c^2,$$
i.e., the four-velocity vectors are "on shell" and as such don't form a vector space.

As I repeatedly said, I don't think that in Galilean spacetime a four-vector formalism makes too much sense, although you can of course formulate everything also in an extended Hamilton formalism with an additional arbitrary parameter and then describing the motion of a particle by ##t(\lambda)## and ##\vec{x}(\lambda)##.
 
  • #134
vanhees71 said:
In special relavity the four-velocity is by definition
$$u^{\mu}=\frac{\mathrm{d} x^{\mu}}{\mathrm{d} \tau},$$
which implies the constraint
$$u_{\mu} u^{\mu}=c^2,$$
i.e., the four-velocity vectors are "on shell" and as such don't form a vector space.

As I repeatedly said, I don't think that in Galilean spacetime a four-vector formalism makes too much sense, although you can of course formulate everything also in an extended Hamilton formalism with an additional arbitrary parameter and then describing the motion of a particle by ##t(\lambda)## and ##\vec{x}(\lambda)##.
See for this Hamilton formalism of a non-relativistic point particle e.g. chapter 3 of my thesis "Newton-Cartan gravity revisited",

https://www.google.com/url?sa=t&rct=j&q=&esrc=s&source=web&cd=&ved=2ahUKEwiO677A5YP9AhX4gP0HHQumC8kQFnoECBMQAQ&url=https://research.rug.nl/files/34926446/Complete_thesis.pdf&usg=AOvVaw3xeIMItlns2gjYN4ANv5Bd

On page 78 you find the general-covariant action of a point particle in curved (Newtonian) spacetime, eqn. 5.14. There you also see the role of the gauge field belonging to the central extension: it couples to the 4-velocity in the same way as the electromagnetic 4-potential couples to a relativistic particle. Basically this extra coupling is needed if you invoke local Galilei-boosts as a symmetry.
 
  • #135
Saw said:
the thing is that it also says this with regard to 4-velocity
That's because, as I said, the tangent space is the space of all vectors at a point, not just the space of all unit timelike vectors (which is the space of 4-velocities).

Saw said:
How does that match with 4-velocity being the time basis vector, given that what you do with basis vectors is precisely scaling them?
I have no idea what you mean here. Basis vectors do not have to be unit vectors; in fact, if you choose a null basis vector it obviously can't be a unit vector. An orthonormal basis in spacetime is a basis consisting of one timelike and three spacelike unit vectors, all mutually orthogonal, but that is not the only possible kind of basis. In any case, there is no requirement that basis vectors form a vector space all by themselves; the only requirement is that every vector in the vector space must be a linear combination of basis vectors.

Saw said:
I guess you refer to other derivatives, like 4-force or 4-acceleration
No. I'm just using the simple obvious definition of a vector space.

Take any timelike unit vector and multiply it by any real number. That gives you another timelike vector that is in the tangent space.

Take any spacelike unit vector and multiply it by any real number. That gives you another spacelike vector that is also in the tangent space.

Take any null vector. That is also a vector in the tangent space.

Take any linear combination of the above with real coefficients. That is also a vector in the tangent space.
 
  • #136
Saw said:
a basis vector, in a normalized basis, must be unitary but then its role is being scaled by a certain coefficient
Scaled how? Where? What are you talking about?

Saw said:
the fact that it is unitary does not mean that it is not a unit of something, i.e. a second, a meter or whatever, how is that consistent with being dimensionless?
A vector with dimensionless units still has a norm, which is a real number.

Saw said:
I have difficulties to see the role of the 4-velocity as the time basis vector.
So far all you have shown is that you have difficulties understanding how vector spaces work.
 
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  • #137
Saw said:
it also says this with regard to 4-velocity: "addition of two four-velocities does not yield a four-velocity: the space of four-velocities is not itself a vector space."

How does that match with 4-velocity being the time basis vector, given that what you do with basis vectors is precisely scaling them?
PeterDonis said:
I have no idea what you mean here.
There may be a misunderstanding here. The fact that the 4-velocities do not form by themselves a vector space is another issue. My "that" refers to the part in red: if you cannot add two four-velocities it means that you cannot multiply one four-velocity by the real number two, i.e. "scale" it by two.

Saw said:
How does that match with 4-velocity being the time basis vector, given that what you do with basis vectors is precisely scaling them?

(...) a basis vector, in a normalized basis, must be unitary but then its role is being scaled by a certain coefficient...
PeterDonis said:
Scaled how? Where? What are you talking about?
I don't think that my use of the verb "scale" is so abnormal or out of place here.

A basis (a set of basis vectors) serves to span a vector space. This means that you can describe any member of the vector space in terms of those basis vectors, i.e. as a linear combination of the latter. The word "linear" is there to denote that you simply scale each basis vector by a scalar, without higher powers. The "combination" part means that, once you have scaled the basis vectors, you add them up. "Scalar" is a generic term that stands for either real or complex numbers, although, as you said, here (SR) we use real numbers (after the idea of scaling time with the imaginary number i has been dropped). A synonym of scalar would be here the term that you also used, coefficients. For the avoidance of doubt, when I say that we scale the time basis vector, what I mean is that we measure with a clock when events 1 and 2 take place and the difference between the two recordings (say, 2 seconds) is what we scale the basis vector by, so as to say that the time component of the spacetime interval separating events 1 and 2 is 2 seconds (or rather c * 2 s).

For completeness, I am aware that we also talk about a scalar as the outcome of a dot product, which is invariant. But that is not really a different meaning. Actually, the dot product of the above-mentioned spacetime interval with itself gives off a scalar because what you do that way is extracting one of those coefficients or scalars accompanying the basis vectors, as it can be readily seen in the example where the two events are measured by the same clock and the outcome of the dot product is the clock's reading (the proper time).

PeterDonis said:
So far all you have shown is that you have difficulties understanding how vector spaces work.

I did not try to show anything, I only asked questions and I think that I have proved that the questions were not without a reason. There will probably be an answer that will prove my doubts groundless, but asking the questions was not unreasonable.

In the light of that, before going ahead with other issues, I would appreciate if you could withdraw that comment, which IMHO is not constructive!
 
  • #138
Saw said:
The fact that the 4-velocities do not form by themselves a vector space is another issue.
No, it's not an issue. There is no requirement that the 4-velocities all by themselves form a vector space.

Saw said:
if you cannot add two four-velocities
You can; you just don't get another 4-velocity. As above, that is not an issue; there is no requirement that adding two 4-velocities must give another 4-velocity.

Saw said:
it means that you cannot multiply one four-velocity by the real number two, i.e. "scale" it by two.
Wrong. Addition of vectors in a vector space is a different operation from scalar multiplication. There is no relationship between the two.

Again, you do not appear to understand the basics of how vector spaces work. You need that understanding for the subject under discussion.

Saw said:
I don't think that my use of the verb "scale" is so abnormal or out of place here.
It's not a question of your usage (although your usage is not standard). It's a question of you having a proper understanding of the concepts we are discussing. You do not appear to have such an understanding.

Saw said:
I did not try to show anything
I didn't say you did. Your posts show that you don't have a good understanding of vector spaces even though you weren't trying to show that at all.

Saw said:
There will probably be an answer that will prove my doubts groundless
An answer to what? So far you have not asked a cogent question. Everything you have asked is based on an incorrect understanding of the subject matter. The only answer to that is that you need to fix your understanding.

Saw said:
I would appreciate if you could withdraw that comment, which IMHO is not constructive!
Your opinion is mistaken. I am giving you the constructive feedback of telling you that you don't understand a key concept for this discussion, namely vector spaces. Even if I were to withdraw that comment, which I won't, it would not change the fact that you have an incorrect understanding and that is preventing you from even being able to frame a cogent question.
 
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  • #139
PeterDonis said:
Wrong. Addition of vectors in a vector space is a different operation from scalar multiplication. There is no relationship between the two.
This proves that you don't understand the question.

Addition of two vectors of the same magnitude but pointing in different directions is obviously not the same as scaling any of the two vectors by the real number 2.

Addition of two vectors of the same magnitude and being colinear obviously yields the same result as scaling any of them by 2.

Therefore, if you ban the possibility of addition of two vectors, you ban the possibility of adding colinear vectors and therefore you also seem to ban the possibility of scaling them. And if not, you have not mentioned any reason why not.

PeterDonis said:
there is no requirement that adding two 4-velocities must give another 4-velocity.
There seems to be this requirement if 4-velocity is to act as a time basis vector, which is what we are talking about, since what you do with basis vectors, as I explained (without being contradicted), is scaling them, in which case the result of this scaling is obviously the same entity as the non-scaled one. And if not, you have not mentioned any reason why not. If you don't have any reason, say it. If you have it, say it as well, because it is improper for you as a mentor to keep aces up in your sleeve. We are here to learn, not to play childish ego games.

The rest of your post...

PeterDonis said:
Again, you do not appear to understand the basics of how vector spaces work. You need that understanding for the subject under discussion.It's not a question of your usage (although your usage is not standard). It's a question of you having a proper understanding of the concepts we are discussing. You do not appear to have such an understanding.I didn't say you did. Your posts show that you don't have a good understanding of vector spaces even though you weren't trying to show that at all.An answer to what? So far you have not asked a cogent question. Everything you have asked is based on an incorrect understanding of the subject matter. The only answer to that is that you need to fix your understanding.Your opinion is mistaken. I am giving you the constructive feedback of telling you that you don't understand a key concept for this discussion, namely vector spaces. Even if I were to withdraw that comment, which I won't, it would not change the fact that you have an incorrect understanding and that is preventing you from even being able to frame a cogent question.

... is a surprisingly lengthy and repetitive way of reiterating the ad hominem attacks.

If you don't feel like mentoring me, please just leave the discussion, but don't prevent others from doing it by closing a new thread of mine, which is probably what you are paving the way for with your aggressive comments.

Who knows? There may be someone of a different opinion. You don't need to be always right, which seems to be your main goal and activity. For example, not so long ago, you replied to me:

Saw said:
I would see concepts like Galilean 4-velocity as a "place-holder". i.e. something that does not really exist in Galilean relativity but is holding a place for another thing that will appear in SR, when you actually need to move forward to the latter.

PeterDonis said:
No, they're not. They're perfectly well-defined in Galilean relativity. They don't work the same as they do in SR, but that doesn't mean they're not well-defined and valid.

But recently someone commented:

vanhees71 said:
As I repeatedly said, I don't think that in Galilean spacetime a four-vector formalism makes too much sense

I would kindly request you to engage in a discussion about that, if you wish, and let others help me with my own queries, if they feel like that.

Should you prefer to keep sabotaging me, then I would like to report the situation and ask for an impartial analysis as to whether my questions are "worthy of a polite answer" or not. The analysis should not be, though, whether my questions are "cogent". You know, "cogent" means "persuasive" and is an adjective that is usually applied to "arguments". But, let me insist, I am not trying to persuade anybody about anything, I am only asking questions as a student. And it would be ridiculous that PhysicsForums became known, from now on, thanks to you, as the place where you can only obtain guidance if you convince your mentor from the very beginning that you don't need any guidance, because your question is "cogent"!
 
  • #140
Saw said:
Addition of two vectors of the same magnitude but pointing in different directions is obviously not the same as scaling any of the two vectors by the real number 2.
Agreed. I have never said otherwise.

Saw said:
Addition of two vectors of the same magnitude and being colinear obviously yields the same result as scaling any of them by 2.
Agreed. I have never said otherwise.

Saw said:
Therefore, if you ban the possibility of addition of two vectors
Nobody has done any such thing. You are the one who keeps making an issue of the fact that adding two 4-velocity vectors gives a vector that is not a unit vector. By making an issue of that non-issue, you are showing that you do not understand the subject under discussion. Yes, it is a fact that adding two unit vectors gives a vector that is not a unit vector. No, that is not a problem, because unit vectors by themselves don't form a vector space. Which is also not a problem, because nobody needs them to be a vector space. You do not appear to understand this.

Saw said:
what you do with basis vectors, as I explained (without being contradicted), is scaling them, in which case the result of this scaling is obviously the same entity as the non-scaled one
I have no idea where you are getting this from. Multiplying a unit vector by the scalar ##2## gives a vector whose norm is ##2##, not a unit vector. Yes, that's correct. No, it's not a problem. See above.
 
  • #141
Saw said:
We are here to learn, not to play childish ego games.
Saw said:
a surprisingly lengthy and repetitive way of reiterating the ad hominem attacks.
Saw said:
Should you prefer to keep sabotaging me
These comments are uncalled for and further indicate that you do not understand the points I have been trying to make. They are also likely to get you a warning if you continue along these lines.

Saw said:
I would like to report the situation
You are always free to use the Report button.
 
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  • #142
Saw said:
vanhees71 said:
As I repeatedly said, I don't think that in Galilean spacetime a four-vector formalism makes too much sense

I would kindly request you to engage in a discussion about that
A discussion about that is fine if you frame a question based on it.

The subthread you are complaining about started with your incorrect assertion in post #126 that the tangent space is only composed of 4-velocity vectors (i.e., unit timelike vectors). It's not. Instead of realizing that it's not and rethinking your position in the light of that new knowledge, you have continued to make further erroneous claims, which I have been correcting (see my post #140 for my latest corrections).

Bear in mind that this thread is not just for you, even though you're the OP. People come to PF all the time to read threads, which means when incorrect statements are made in PF threads, we try to correct them.
 
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  • #143
PeterDonis said:
You are the one who keeps making an issue of the fact that adding two 4-velocity vectors gives a vector that is not a unit vector.
I don't have a problem with that. How could I? It is obvious that, if you scale a unit vector, you get that vector scaled by whatever scalar you have multiplied it by, i.e. not a unit vector anymore.

However, the statement by Wikipedia is the following: "addition of two four-velocities does not yield a four-velocity". That seems to be a problem because it implies that the addition gives off a different object (something that is not a 4-velocity vector), not the same object (a 4-velocity vector) with a coefficient other than 1.

It seems that your ace in the sleeve is that a 4-velocity's magnitude is always 1. You don't need to keep it, I am saying it right now. But if so, what is then the object that yields the addition of two colinear 4-velocities or in general the scaling thereof by some coefficient? What is its name and what kind of object is it?
 
  • #144
Saw said:
the statement by Wikipedia is the following: "addition of two four-velocities does not yield a four-velocity".
Yes, that's correct. Adding two unit vectors does not give another unit vector. That is what Wikipedia is saying, though of course it's Wikipedia and you should not expect it to say things rigorously.

Saw said:
That seems to be a problem because it implies that the addition gives off a different object
No, it doesn't. You are adding two vectors and getting another vector.

Saw said:
It seems that your ace in the sleeve is that a 4-velocity's magnitude is always 1
It's not an "ace in the sleeve", it's part of the definition of a 4-velocity. It's a unit timelike vector tangent to an object's worldline.

Saw said:
what is then the object that yields the addition of two colinear 4-velocities or in general the scaling thereof by some coefficient? What is its name and what kind of object is it?
A vector. I have already said this multiple times. As above, you are adding two vectors and getting another vector. Or you are multiplying a vector by some scalar and getting another vector. This is vector spaces 101. If you seriously don't understand how this works, please take some time to learn it from a textbook or similar source on the basics of vector spaces.

Your issue seems to be that "4-velocity" or "unit vector" is somehow some "different" type of object from other vectors. As far as vector addition and scalar multiplication is concerned, it's not. It's just a vector. The fact of having unit norm is useful for some other purposes, but it has no significance as far as the basics of vector spaces are concerned.
 
  • #145
PeterDonis said:
The subthread you are complaining about started with your incorrect assertion in post #126 that the tangent space is only composed of 4-velocity vectors (i.e., unit timelike vectors). It's not. Instead of realizing that it's not and rethinking your position in the light of that new knowledge, you have continued to make further erroneous claims, which I have been correcting (see my post #140 for my latest corrections).
False. As you can see below, I received the information that the tangent space is composed of things other than 4-velocity, I accepted it as good knowledge, and it simply happens that I returned to the question that interested me, because it is related to the object of the thread: where is the time basis vector in Galilean relativity as compared to SR, which is what we are discussing now.

Saw said:
I guess you refer to other derivatives, like 4-force or 4-acceleration... But focusing again on 4-velocity, which is our object of interest because it i said to be at least one option for the time basis vector, I would come back to the issue mentioned before...

I am just trying to understand something that looks weird to me, that the 4-velocity is the time basis vector and I do think that others may have this legitimate lack of understanding. And I do find puzzling this twisted way of mentoring where the objective seems to be, not answering things, but convincing the asker that she should not ask. And I guess there may be many askers who have suffered these methods and may be thinking the same. And this is a shame for PhysicsForums and it should be stopped because it is a most valuable place that does not deserve to gain this ugly image.
 
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  • #146
Saw said:
I am just trying to understand something that looks weird to me, that the 4-velocity is the time basis vector
The 4-velocity is not necessarily the time basis vector. A particular object's 4-velocity can be the time basis vector, if you choose to work in that object's rest frame and you want to use unit vectors as your basis vectors (which is usually a good choice but is not a requirement).

I still do not understand what the issue is. In the previous post of yours that you quoted from, you cut off your quote; here is the rest of that paragraph of your post:

Saw said:
a basis vector, in a normalized basis, must be unitary but then its role is being scaled by a certain coefficient...
I don't see what the issue is here. Yes, an arbitrary vector in a vector space can be written, given a choice of basis, as a linear combination of the basis vectors, i.e., with each basis vector multiplied by some scalar coefficient. As I said before, this is vector spaces 101. I cannot understand what the problem is.

(Btw, "unitary" does not mean the same thing as "unit vector", which is what basis vectors will be in a normalized basis. "Unitary" is a term that applies to operators and means something quite different.)

Saw said:
this twisted way of mentoring where the objective seems to be, not answering things, but convincing the asker that she should not ask
As I have already said, if people make incorrect statements here, we try to correct them. You have made a number of them in this thread, which I have corrected. All of that is a separate issue from what your actual question is (as above, I still don't understand what it is) and getting that question answered.
 
  • #147
Thread is closed temporarily for a Mentor discussion...
 

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