Could be possible to build a 4-vector in special relativity whose spatial component was the electric field E?
Hi everyone and sorry for my English.
I would like to know if I can build a legitimate 4-vector as $E^alpha=(E^0,mathbf{E})$.
I'd like you to check if my way is correct.
1- We already know that $mathbf{E}$ transforms under Lorentz boost as:
begin{equation}label{sdf}
begin{aligned}
mathbf{E}'&=gammaleft(mathbf{E}+vec{beta}timesmathbf{B} right)-dfrac{gamma^2}{gamma+1}vec{beta}left(vec{beta}cdotmathbf{E}right)\[5mm]
&text{So:}\[5mm]
E'_parallel&=E_parallel\
mathbf{E}_perp'&=gammaleft(mathbf{E}_perp+vec{beta}timesmathbf{B} right)
end{aligned}
end{equation}
2- While the spatial component of any 4-vector must obey the following rule:
begin{equation}
begin{aligned}
E_parallel'&=gamma(E_{parallel}-beta E^0)\
mathbf{E}_perp'&=mathbf{E}_perp
end{aligned}
end{equation}
So both expressions must to be equal:
begin{equation}
left{
begin{aligned}
gamma E_parallel-gammabeta E^0&=E_parallel\
gammamathbf{E}_perp+gammavec{beta}timesmathbf{B}&=mathbf{E}_perp
end{aligned}
right.
end{equation}
From the first one we can conclude that time component of 4-vector must be $E^0=dfrac{gamma-1}{gammabeta}E_parallel$ or $E^0=dfrac{gamma-1}{gammabeta^2}vec{beta}cdotmathbf{E}$
But what can we conclude for the second one? Is therefore possible to build that 4-vector $E^alpha$?
Thank you very much
special-relativity tensor-calculus classical-electrodynamics lorentz-symmetry
New contributor
add a comment |
Hi everyone and sorry for my English.
I would like to know if I can build a legitimate 4-vector as $E^alpha=(E^0,mathbf{E})$.
I'd like you to check if my way is correct.
1- We already know that $mathbf{E}$ transforms under Lorentz boost as:
begin{equation}label{sdf}
begin{aligned}
mathbf{E}'&=gammaleft(mathbf{E}+vec{beta}timesmathbf{B} right)-dfrac{gamma^2}{gamma+1}vec{beta}left(vec{beta}cdotmathbf{E}right)\[5mm]
&text{So:}\[5mm]
E'_parallel&=E_parallel\
mathbf{E}_perp'&=gammaleft(mathbf{E}_perp+vec{beta}timesmathbf{B} right)
end{aligned}
end{equation}
2- While the spatial component of any 4-vector must obey the following rule:
begin{equation}
begin{aligned}
E_parallel'&=gamma(E_{parallel}-beta E^0)\
mathbf{E}_perp'&=mathbf{E}_perp
end{aligned}
end{equation}
So both expressions must to be equal:
begin{equation}
left{
begin{aligned}
gamma E_parallel-gammabeta E^0&=E_parallel\
gammamathbf{E}_perp+gammavec{beta}timesmathbf{B}&=mathbf{E}_perp
end{aligned}
right.
end{equation}
From the first one we can conclude that time component of 4-vector must be $E^0=dfrac{gamma-1}{gammabeta}E_parallel$ or $E^0=dfrac{gamma-1}{gammabeta^2}vec{beta}cdotmathbf{E}$
But what can we conclude for the second one? Is therefore possible to build that 4-vector $E^alpha$?
Thank you very much
special-relativity tensor-calculus classical-electrodynamics lorentz-symmetry
New contributor
add a comment |
Hi everyone and sorry for my English.
I would like to know if I can build a legitimate 4-vector as $E^alpha=(E^0,mathbf{E})$.
I'd like you to check if my way is correct.
1- We already know that $mathbf{E}$ transforms under Lorentz boost as:
begin{equation}label{sdf}
begin{aligned}
mathbf{E}'&=gammaleft(mathbf{E}+vec{beta}timesmathbf{B} right)-dfrac{gamma^2}{gamma+1}vec{beta}left(vec{beta}cdotmathbf{E}right)\[5mm]
&text{So:}\[5mm]
E'_parallel&=E_parallel\
mathbf{E}_perp'&=gammaleft(mathbf{E}_perp+vec{beta}timesmathbf{B} right)
end{aligned}
end{equation}
2- While the spatial component of any 4-vector must obey the following rule:
begin{equation}
begin{aligned}
E_parallel'&=gamma(E_{parallel}-beta E^0)\
mathbf{E}_perp'&=mathbf{E}_perp
end{aligned}
end{equation}
So both expressions must to be equal:
begin{equation}
left{
begin{aligned}
gamma E_parallel-gammabeta E^0&=E_parallel\
gammamathbf{E}_perp+gammavec{beta}timesmathbf{B}&=mathbf{E}_perp
end{aligned}
right.
end{equation}
From the first one we can conclude that time component of 4-vector must be $E^0=dfrac{gamma-1}{gammabeta}E_parallel$ or $E^0=dfrac{gamma-1}{gammabeta^2}vec{beta}cdotmathbf{E}$
But what can we conclude for the second one? Is therefore possible to build that 4-vector $E^alpha$?
Thank you very much
special-relativity tensor-calculus classical-electrodynamics lorentz-symmetry
New contributor
Hi everyone and sorry for my English.
I would like to know if I can build a legitimate 4-vector as $E^alpha=(E^0,mathbf{E})$.
I'd like you to check if my way is correct.
1- We already know that $mathbf{E}$ transforms under Lorentz boost as:
begin{equation}label{sdf}
begin{aligned}
mathbf{E}'&=gammaleft(mathbf{E}+vec{beta}timesmathbf{B} right)-dfrac{gamma^2}{gamma+1}vec{beta}left(vec{beta}cdotmathbf{E}right)\[5mm]
&text{So:}\[5mm]
E'_parallel&=E_parallel\
mathbf{E}_perp'&=gammaleft(mathbf{E}_perp+vec{beta}timesmathbf{B} right)
end{aligned}
end{equation}
2- While the spatial component of any 4-vector must obey the following rule:
begin{equation}
begin{aligned}
E_parallel'&=gamma(E_{parallel}-beta E^0)\
mathbf{E}_perp'&=mathbf{E}_perp
end{aligned}
end{equation}
So both expressions must to be equal:
begin{equation}
left{
begin{aligned}
gamma E_parallel-gammabeta E^0&=E_parallel\
gammamathbf{E}_perp+gammavec{beta}timesmathbf{B}&=mathbf{E}_perp
end{aligned}
right.
end{equation}
From the first one we can conclude that time component of 4-vector must be $E^0=dfrac{gamma-1}{gammabeta}E_parallel$ or $E^0=dfrac{gamma-1}{gammabeta^2}vec{beta}cdotmathbf{E}$
But what can we conclude for the second one? Is therefore possible to build that 4-vector $E^alpha$?
Thank you very much
special-relativity tensor-calculus classical-electrodynamics lorentz-symmetry
special-relativity tensor-calculus classical-electrodynamics lorentz-symmetry
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DaniDani
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I thought G. Smith's answer was fine in terms of explaining the physics involved, but the OP says:
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction?
Your deduction is of the form X => Y, where X seems to be the proposition that one can make a four-vector of the form $(E^0,textbf{E})$. What is not totally clear to me about your X is what other data you think should be allowed to be encoded in $E^0$, but anyway I think it's possible to give a nonexistence proof without needing to clarify that point.
You've proved some equations involving $E^0$ which vanish when the electric field is zero. Therefore when the field is zero, your 4-vector vanishes. But a Lorentz transformation on a zero vector always gives a zero vector, so you've proved that if an electric field is zero in one frame of reference, it's zero in all other frames. This is false, so we have a proof by contradiction that X is false.
add a comment |
No, it is not possible to make a four-vector from the electric field. But from the electric field and the magnetic field together you can make a four-tensor, $F_{munu}$.
https://en.m.wikipedia.org/wiki/Electromagnetic_tensor
This is because electric and magnetic fields transform into each other under Lorentz transformations. The transformed electric field is a linear combination of the untransformed electric field and the untransformed magnetic field. Amd similarly for the transformed magnetic field.
The lesson is that electric and magnetic fields are just two aspects of one unified thing, the electromagnetic field.
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
add a comment |
Your formula for $E_0$ depends on $beta$. If there WERE a legal four-vector for the electric field, it's components can't depend on the Lorentz transformation you do. Your formula for $E_0$ should be independent of $beta$. But as you show with your algebra above, this is not possible.
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
add a comment |
Maybe I could say that my derivation is not possible because the time coordinate $E^0$ depends on another coordinate ($E_parallel$) and it is not allowed because coordinates in a 4-vector must be independent? Is this a factible answer that proofs what I want to?
New contributor
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
add a comment |
As observed by an inertial observer,
the Electric Field is a spatial vector,
which means that its time-component in that frame is always zero.
In addition, the Magnetic Field is also a spatial vector... and thus has zero time-component.
As @G. Smith notes, the electric and magnetic fields transform by mixing components (because the electric and magnetic fields are components of a two-index tensor).. and remain spatial,
which are not like 4-vectors (since the time-component of a 4-vector won't generally stay zero after transformation).
update:
Up to sign conventions, $$E_b=F_{ab}u^a$$
is the electric-field according to the observer with 4-velocity $u^a$.
(It is an observer-dependent four-vector.)
But since $F_{ab}=F_{[ab]}$, it follows that
$$E_bu^b=F_{ab}u^a u^b=0,$$
that is, the observer with 4-velocity $u^b$ measures the time-component of $E_b$ to be zero. Thus, $E_b$ has only spatial-components for that observer.
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
add a comment |
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5 Answers
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active
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5 Answers
5
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I thought G. Smith's answer was fine in terms of explaining the physics involved, but the OP says:
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction?
Your deduction is of the form X => Y, where X seems to be the proposition that one can make a four-vector of the form $(E^0,textbf{E})$. What is not totally clear to me about your X is what other data you think should be allowed to be encoded in $E^0$, but anyway I think it's possible to give a nonexistence proof without needing to clarify that point.
You've proved some equations involving $E^0$ which vanish when the electric field is zero. Therefore when the field is zero, your 4-vector vanishes. But a Lorentz transformation on a zero vector always gives a zero vector, so you've proved that if an electric field is zero in one frame of reference, it's zero in all other frames. This is false, so we have a proof by contradiction that X is false.
add a comment |
I thought G. Smith's answer was fine in terms of explaining the physics involved, but the OP says:
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction?
Your deduction is of the form X => Y, where X seems to be the proposition that one can make a four-vector of the form $(E^0,textbf{E})$. What is not totally clear to me about your X is what other data you think should be allowed to be encoded in $E^0$, but anyway I think it's possible to give a nonexistence proof without needing to clarify that point.
You've proved some equations involving $E^0$ which vanish when the electric field is zero. Therefore when the field is zero, your 4-vector vanishes. But a Lorentz transformation on a zero vector always gives a zero vector, so you've proved that if an electric field is zero in one frame of reference, it's zero in all other frames. This is false, so we have a proof by contradiction that X is false.
add a comment |
I thought G. Smith's answer was fine in terms of explaining the physics involved, but the OP says:
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction?
Your deduction is of the form X => Y, where X seems to be the proposition that one can make a four-vector of the form $(E^0,textbf{E})$. What is not totally clear to me about your X is what other data you think should be allowed to be encoded in $E^0$, but anyway I think it's possible to give a nonexistence proof without needing to clarify that point.
You've proved some equations involving $E^0$ which vanish when the electric field is zero. Therefore when the field is zero, your 4-vector vanishes. But a Lorentz transformation on a zero vector always gives a zero vector, so you've proved that if an electric field is zero in one frame of reference, it's zero in all other frames. This is false, so we have a proof by contradiction that X is false.
I thought G. Smith's answer was fine in terms of explaining the physics involved, but the OP says:
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction?
Your deduction is of the form X => Y, where X seems to be the proposition that one can make a four-vector of the form $(E^0,textbf{E})$. What is not totally clear to me about your X is what other data you think should be allowed to be encoded in $E^0$, but anyway I think it's possible to give a nonexistence proof without needing to clarify that point.
You've proved some equations involving $E^0$ which vanish when the electric field is zero. Therefore when the field is zero, your 4-vector vanishes. But a Lorentz transformation on a zero vector always gives a zero vector, so you've proved that if an electric field is zero in one frame of reference, it's zero in all other frames. This is false, so we have a proof by contradiction that X is false.
answered 19 hours ago
Ben CrowellBen Crowell
49.1k4153294
49.1k4153294
add a comment |
add a comment |
No, it is not possible to make a four-vector from the electric field. But from the electric field and the magnetic field together you can make a four-tensor, $F_{munu}$.
https://en.m.wikipedia.org/wiki/Electromagnetic_tensor
This is because electric and magnetic fields transform into each other under Lorentz transformations. The transformed electric field is a linear combination of the untransformed electric field and the untransformed magnetic field. Amd similarly for the transformed magnetic field.
The lesson is that electric and magnetic fields are just two aspects of one unified thing, the electromagnetic field.
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
add a comment |
No, it is not possible to make a four-vector from the electric field. But from the electric field and the magnetic field together you can make a four-tensor, $F_{munu}$.
https://en.m.wikipedia.org/wiki/Electromagnetic_tensor
This is because electric and magnetic fields transform into each other under Lorentz transformations. The transformed electric field is a linear combination of the untransformed electric field and the untransformed magnetic field. Amd similarly for the transformed magnetic field.
The lesson is that electric and magnetic fields are just two aspects of one unified thing, the electromagnetic field.
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
add a comment |
No, it is not possible to make a four-vector from the electric field. But from the electric field and the magnetic field together you can make a four-tensor, $F_{munu}$.
https://en.m.wikipedia.org/wiki/Electromagnetic_tensor
This is because electric and magnetic fields transform into each other under Lorentz transformations. The transformed electric field is a linear combination of the untransformed electric field and the untransformed magnetic field. Amd similarly for the transformed magnetic field.
The lesson is that electric and magnetic fields are just two aspects of one unified thing, the electromagnetic field.
No, it is not possible to make a four-vector from the electric field. But from the electric field and the magnetic field together you can make a four-tensor, $F_{munu}$.
https://en.m.wikipedia.org/wiki/Electromagnetic_tensor
This is because electric and magnetic fields transform into each other under Lorentz transformations. The transformed electric field is a linear combination of the untransformed electric field and the untransformed magnetic field. Amd similarly for the transformed magnetic field.
The lesson is that electric and magnetic fields are just two aspects of one unified thing, the electromagnetic field.
edited 20 hours ago
answered 20 hours ago
G. SmithG. Smith
5,3391021
5,3391021
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
add a comment |
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
1
1
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Here is a nice article about the unification of $vec{E}$ and $vec{B}$. arxiv.org/abs/1111.7126
– N. Steinle
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
Thank you G.Smith. I know about the electromagnetic tensor and its properties, but i was wondering if there is a formal proof about the imposibility of building that $E^alpha$ tensor, based on the allowed transformations, as I've tried. What's wrong with my deduction? Thanks!
– Dani
19 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You don’t have a deduction to criticize! You failed to find a four-vector that satisied the equations you wrote down. Since your second equation involves the magnetic field, how could you possibly expect to satisfy it, when your first equation requires $E^0$ to be a combination of the components of the electric field? This seems like proof to me that what you want is impossible. And, of course, if what you were trying to do were possible, it would have been done 100 years ago.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
You may “know about the electromagnetic tensor and its properties” but you didn’t grasp its relevance. If electric and magnetic fields mix together under a Lorentz transformation, then they cannot also stay unmixed under a Lorentz transformation, as in your failed attempt. Things either mix or they don’t. They can’t do both.
– G. Smith
18 hours ago
add a comment |
Your formula for $E_0$ depends on $beta$. If there WERE a legal four-vector for the electric field, it's components can't depend on the Lorentz transformation you do. Your formula for $E_0$ should be independent of $beta$. But as you show with your algebra above, this is not possible.
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
add a comment |
Your formula for $E_0$ depends on $beta$. If there WERE a legal four-vector for the electric field, it's components can't depend on the Lorentz transformation you do. Your formula for $E_0$ should be independent of $beta$. But as you show with your algebra above, this is not possible.
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
add a comment |
Your formula for $E_0$ depends on $beta$. If there WERE a legal four-vector for the electric field, it's components can't depend on the Lorentz transformation you do. Your formula for $E_0$ should be independent of $beta$. But as you show with your algebra above, this is not possible.
Your formula for $E_0$ depends on $beta$. If there WERE a legal four-vector for the electric field, it's components can't depend on the Lorentz transformation you do. Your formula for $E_0$ should be independent of $beta$. But as you show with your algebra above, this is not possible.
answered 14 hours ago
Jahan ClaesJahan Claes
5,0331032
5,0331032
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
add a comment |
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
1
1
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
(I'll add that you also can't solve your second equation at all if you allow arbitrary magnetic fields. You can easily see this by taking the derivative with respect to any components of the magnetic field on both sides of that equation. One side with have the derivative be zero, the other will not. So it simply can't be solved)
– Jahan Claes
14 hours ago
add a comment |
Maybe I could say that my derivation is not possible because the time coordinate $E^0$ depends on another coordinate ($E_parallel$) and it is not allowed because coordinates in a 4-vector must be independent? Is this a factible answer that proofs what I want to?
New contributor
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
add a comment |
Maybe I could say that my derivation is not possible because the time coordinate $E^0$ depends on another coordinate ($E_parallel$) and it is not allowed because coordinates in a 4-vector must be independent? Is this a factible answer that proofs what I want to?
New contributor
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
add a comment |
Maybe I could say that my derivation is not possible because the time coordinate $E^0$ depends on another coordinate ($E_parallel$) and it is not allowed because coordinates in a 4-vector must be independent? Is this a factible answer that proofs what I want to?
New contributor
Maybe I could say that my derivation is not possible because the time coordinate $E^0$ depends on another coordinate ($E_parallel$) and it is not allowed because coordinates in a 4-vector must be independent? Is this a factible answer that proofs what I want to?
New contributor
New contributor
answered 19 hours ago
DaniDani
161
161
New contributor
New contributor
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
add a comment |
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
The problem is your time coordinate depends on $beta$. It's perfectly fine to have it depend on spacial stuff.
– Jahan Claes
14 hours ago
add a comment |
As observed by an inertial observer,
the Electric Field is a spatial vector,
which means that its time-component in that frame is always zero.
In addition, the Magnetic Field is also a spatial vector... and thus has zero time-component.
As @G. Smith notes, the electric and magnetic fields transform by mixing components (because the electric and magnetic fields are components of a two-index tensor).. and remain spatial,
which are not like 4-vectors (since the time-component of a 4-vector won't generally stay zero after transformation).
update:
Up to sign conventions, $$E_b=F_{ab}u^a$$
is the electric-field according to the observer with 4-velocity $u^a$.
(It is an observer-dependent four-vector.)
But since $F_{ab}=F_{[ab]}$, it follows that
$$E_bu^b=F_{ab}u^a u^b=0,$$
that is, the observer with 4-velocity $u^b$ measures the time-component of $E_b$ to be zero. Thus, $E_b$ has only spatial-components for that observer.
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
add a comment |
As observed by an inertial observer,
the Electric Field is a spatial vector,
which means that its time-component in that frame is always zero.
In addition, the Magnetic Field is also a spatial vector... and thus has zero time-component.
As @G. Smith notes, the electric and magnetic fields transform by mixing components (because the electric and magnetic fields are components of a two-index tensor).. and remain spatial,
which are not like 4-vectors (since the time-component of a 4-vector won't generally stay zero after transformation).
update:
Up to sign conventions, $$E_b=F_{ab}u^a$$
is the electric-field according to the observer with 4-velocity $u^a$.
(It is an observer-dependent four-vector.)
But since $F_{ab}=F_{[ab]}$, it follows that
$$E_bu^b=F_{ab}u^a u^b=0,$$
that is, the observer with 4-velocity $u^b$ measures the time-component of $E_b$ to be zero. Thus, $E_b$ has only spatial-components for that observer.
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
add a comment |
As observed by an inertial observer,
the Electric Field is a spatial vector,
which means that its time-component in that frame is always zero.
In addition, the Magnetic Field is also a spatial vector... and thus has zero time-component.
As @G. Smith notes, the electric and magnetic fields transform by mixing components (because the electric and magnetic fields are components of a two-index tensor).. and remain spatial,
which are not like 4-vectors (since the time-component of a 4-vector won't generally stay zero after transformation).
update:
Up to sign conventions, $$E_b=F_{ab}u^a$$
is the electric-field according to the observer with 4-velocity $u^a$.
(It is an observer-dependent four-vector.)
But since $F_{ab}=F_{[ab]}$, it follows that
$$E_bu^b=F_{ab}u^a u^b=0,$$
that is, the observer with 4-velocity $u^b$ measures the time-component of $E_b$ to be zero. Thus, $E_b$ has only spatial-components for that observer.
As observed by an inertial observer,
the Electric Field is a spatial vector,
which means that its time-component in that frame is always zero.
In addition, the Magnetic Field is also a spatial vector... and thus has zero time-component.
As @G. Smith notes, the electric and magnetic fields transform by mixing components (because the electric and magnetic fields are components of a two-index tensor).. and remain spatial,
which are not like 4-vectors (since the time-component of a 4-vector won't generally stay zero after transformation).
update:
Up to sign conventions, $$E_b=F_{ab}u^a$$
is the electric-field according to the observer with 4-velocity $u^a$.
(It is an observer-dependent four-vector.)
But since $F_{ab}=F_{[ab]}$, it follows that
$$E_bu^b=F_{ab}u^a u^b=0,$$
that is, the observer with 4-velocity $u^b$ measures the time-component of $E_b$ to be zero. Thus, $E_b$ has only spatial-components for that observer.
edited 18 hours ago
answered 19 hours ago
robphyrobphy
1,872238
1,872238
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
add a comment |
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
1
1
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This reasoning seems a little circular. Of course if you assume that the putative electric field four-vector is equal to the first row of the electromagnetic field tensor, then it's trivially true that has a zero timelike component and has the wrong transformation properties.
– Ben Crowell
15 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
This formulation is based on a tensorial development of the field tensor and Maxwell Equations, as found in Misner-Thorne-Wheeler [Ch 3.1] and in Wald [Ch 4.2], which is more geometrical and elegant compared to matrix representations and clumsy 3-vector formulations. The magnetic field is defined analogously with the Hodge-dual *F. (In other words, is there a more elegant way to describe the clumsier coordinate-based calculations and transformation formulas to demonstrate Lorentz invariance? Yes, use tensors through out.)
– robphy
14 hours ago
add a comment |
Dani is a new contributor. Be nice, and check out our Code of Conduct.
Dani is a new contributor. Be nice, and check out our Code of Conduct.
Dani is a new contributor. Be nice, and check out our Code of Conduct.
Dani is a new contributor. Be nice, and check out our Code of Conduct.
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