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Science Forum Index » Physics Forum » Does Newton's third law hold in Special Relativity?
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| ram.rachum@gmail.com |
Posted: Sat Apr 05, 2008 12:20 pm |
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Guest
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Hello,
Does Newton's third law, that says that every force has an equal and
opposite counter force, still applies in Special Relativity?
The reason I'm confused over this is that according to the force
equations for electro-magnetic force, it seems that this law doesn't
hold. But on the other hand, since there is still a conservation of
momentum in special relativity, and force is just the change of
momentum, it makes sense that the total force should always remain
zero, so that the momentum will not change.
So what is the right answer? Does Newton's third law hold in Special
Relativity?
Best Wishes,
Ram Rachum. |
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| Darwin123 |
Posted: Sat Apr 05, 2008 1:19 pm |
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On Apr 5, 6:20 pm, "ram.rac...@gmail.com" <ram.rac...@gmail.com>
wrote:
Quote: Hello,
Does Newton's third law, that says that every force has an equal and
opposite counter force, still applies in Special Relativity?
From Principia, by Isaac Newton (translated by Andrew Motte) page
19:
"Law III: To every action there is always opposed an equal reaction:
or the mutual actions of two bodies upon each other are always equal
and directed to contrary parts."
The "action" and "reaction" part of this law isn't very clear. It
really is just a short summary of the second half. However, look
carefully on the second half of this law.
"The mutual actions of two bodies upon each other are always equal and
directed to contrary parts."
By "actions," I take it to mean "forces" and by "bodies," I take
to mean "matter objects." And the sentence is in present tense.
Therefore, the electromagnetic field described by Maxwell doesn't
satisfy the third law. The actions have to be at the same time equal.
If there is a delay, the third law doesn't apply.
The forces between two electrically charged bodies are not always
equal and opposite according to Maxwell's equations. If two like
charges a large distance apart have been in position a long time, the
electric force between them may be equal. However, if one charge is
suddenly moved toward the other charge, it will be subject to a larger
force from the second body. However, the second body won't experience
the change in force for a long time. The electric force can't can't
propagate faster than the speed of light according to Maxwell's
equation. Furthermore, you can't count the "force" on the
electromagnetic field because the electromagnetic field isn't a
material "body." Therefore, the third law of Newton and Maxwell's
equations are technically in contradiction.
Maxwell's equations and Newton's Laws are in logical
contradiction. Newton's Laws were stated in the present tense as
though forces are instantaneous, but in actuality forces propagate at
a finite speed. I think this contradiction preceded special
relativity. I suspect that this contradiction lead to relativity.
Special relativity started as a means of modifying Newton's Laws so
that there is no logical contradiction.
H.A. Lorentz started working out the consequences of a finite
speed of propagation. A. Einstein finished H. A. Lorentz's program. |
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| Robert J. Kolker |
Posted: Sat Apr 05, 2008 6:03 pm |
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ram.rachum@gmail.com wrote:
Quote: Hello,
Does Newton's third law, that says that every force has an equal and
opposite counter force, still applies in Special Relativity?
Relativistic momentum is conserved.
Bob Kolker |
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| Robert J. Kolker |
Posted: Sun Apr 06, 2008 10:29 am |
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Guest
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Darwin123 wrote:
Newton and Maxwell's
Quote: equations are technically in contradiction.
Maxwell's equations and Newton's Laws are in logical
contradiction. Newton's Laws were stated in the present tense as
though forces are instantaneous, but in actuality forces propagate at
a finite speed. I think this contradiction preceded special
relativity. I suspect that this contradiction lead to relativity.
Special relativity started as a means of modifying Newton's Laws so
that there is no logical contradiction.
Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
Bob Kolker |
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| Androcles |
Posted: Sun Apr 06, 2008 10:40 am |
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--
This message is brought to you by Androcles
http://www.androcles01.pwp.blueyonder.co.uk/
"Robert J. Kolker" <bobkolker@comcast.net> wrote in message
news:pPqdnTx62_sicWXanZ2dnUVZ_oWdnZ2d@comcast.com...
| Darwin123 wrote:
| Newton and Maxwell's
| > equations are technically in contradiction.
| >
| > Maxwell's equations and Newton's Laws are in logical
| > contradiction. Newton's Laws were stated in the present tense as
| > though forces are instantaneous, but in actuality forces propagate at
| > a finite speed. I think this contradiction preceded special
| > relativity. I suspect that this contradiction lead to relativity.
| > Special relativity started as a means of modifying Newton's Laws so
| > that there is no logical contradiction.
|
| Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
|
Newton's Laws are not Lorentz Invariant. Therefore they are right, crank. |
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| Darwin123 |
Posted: Sun Apr 06, 2008 2:08 pm |
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On Apr 6, 11:29 am, "Robert J. Kolker" <bobkol...@comcast.net> wrote:
Quote: Darwin123 wrote:
Newton and Maxwell's
equations are technically in contradiction.
Maxwell's equations and Newton's Laws are in logical
contradiction. Newton's Laws were stated in the present tense as
though forces are instantaneous, but in actuality forces propagate at
a finite speed. I think this contradiction preceded special
relativity. I suspect that this contradiction lead to relativity.
Special relativity started as a means of modifying Newton's Laws so
that there is no logical contradiction.
Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
Bob Kolker
I was pointing out WHY Newton's Laws are not consistent with
special relativity. In particular, Newton's Laws are not Lorentz
invariant. However, I don't think this is immediately obvious even to
somebody with a mathematical background. I myself was a little
confused on this point for a while. There is no explicit constraint on
the form of the force laws in Principia. If a force law is Lorentz
invariant, can't one simply use Newtons Laws to calculate the results?
The answer is that there is no Lorentz invariant force law that is
consistent with Newton's Laws.
A nonmathematical way to show that Newton's Laws are not
consistent with special relativity is simply to look carefully at the
sentences in Principia. They are all in present tense. In other words,
only instantaneous forces are allowed in Principia. Therefore, one
can't have a "force field" with a "finite propagation velocity."
The question was at heart historical, although phrased in an
offensive way. I interpreted his question as meaning this, aside from
the jealous attacks on Einstein. The question is, "Why in the days
before Einstein didn't scientists merely modify the force laws
describing the Michaelson Morley experiment in such a way as to
explain the experimental results?"
I conjectured that the reason is that Newton's Laws and Maxwell's
equations are logically inconsistent. I pointed out where the
inconsistency is in Principia. There are several statements made both
by H. A. Lorentz and A. Einstein that pointed me to that conjecture,
but I honestly can't be 100% sure that this is relevant.
I see ad hominum statements as a cry for help. Calling Einstein
stupid is a desperate plea by a scientific illiterate clarification on
a misunderstood point that irritates his or her learning disability. I
try relieve the inner conflict by providing a historical conjecture
that will help him or her make sense of a world that is beyond their
feeble comprehension. |
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| ram.rachum@gmail.com |
Posted: Sun Apr 06, 2008 9:59 pm |
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On Apr 7, 3:08 am, Darwin123 <drosen0...@yahoo.com> wrote:
Quote: On Apr 6, 11:29 am, "Robert J. Kolker" <bobkol...@comcast.net> wrote:
Darwin123 wrote:
Newton and Maxwell's
equations are technically in contradiction.
Maxwell's equations and Newton's Laws are in logical
contradiction. Newton's Laws were stated in the present tense as
though forces are instantaneous, but in actuality forces propagate at
a finite speed. I think this contradiction preceded special
relativity. I suspect that this contradiction lead to relativity.
Special relativity started as a means of modifying Newton's Laws so
that there is no logical contradiction.
Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
Bob Kolker
I was pointing out WHY Newton's Laws are not consistent with
special relativity. In particular, Newton's Laws are not Lorentz
invariant. However, I don't think this is immediately obvious even to
somebody with a mathematical background. I myself was a little
confused on this point for a while. There is no explicit constraint on
the form of the force laws in Principia. If a force law is Lorentz
invariant, can't one simply use Newtons Laws to calculate the results?
The answer is that there is no Lorentz invariant force law that is
consistent with Newton's Laws.
A nonmathematical way to show that Newton's Laws are not
consistent with special relativity is simply to look carefully at the
sentences in Principia. They are all in present tense. In other words,
only instantaneous forces are allowed in Principia. Therefore, one
can't have a "force field" with a "finite propagation velocity."
The question was at heart historical, although phrased in an
offensive way. I interpreted his question as meaning this, aside from
the jealous attacks on Einstein. The question is, "Why in the days
before Einstein didn't scientists merely modify the force laws
describing the Michaelson Morley experiment in such a way as to
explain the experimental results?"
I conjectured that the reason is that Newton's Laws and Maxwell's
equations are logically inconsistent. I pointed out where the
inconsistency is in Principia. There are several statements made both
by H. A. Lorentz and A. Einstein that pointed me to that conjecture,
but I honestly can't be 100% sure that this is relevant.
I see ad hominum statements as a cry for help. Calling Einstein
stupid is a desperate plea by a scientific illiterate clarification on
a misunderstood point that irritates his or her learning disability. I
try relieve the inner conflict by providing a historical conjecture
that will help him or her make sense of a world that is beyond their
feeble comprehension.
Darwin123, you have not explained the most important part.
The reason I was confused over this is because of the conservation of
momentum. Assume you're right, and the third law doesn't hold. Observe
this. Momentum is conserved in Special Relativity. Momentum remains a
constant. Force is the change of momentum over time. Therefore, the
total force must always be zero. But that would mean that for every 2-
body system, Newton's third law WILL hold. So how do you explain that?
Ram. |
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| Darwin123 |
Posted: Mon Apr 07, 2008 4:51 am |
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On Apr 7, 3:59 am, "ram.rac...@gmail.com" <ram.rac...@gmail.com>
wrote:
Quote: On Apr 7, 3:08 am, Darwin123 <drosen0...@yahoo.com> wrote:
On Apr 6, 11:29 am, "Robert J. Kolker" <bobkol...@comcast.net> wrote:
Darwin123 wrote:
Newton and Maxwell's
equations are technically in contradiction.
Maxwell's equations and Newton's Laws are in logical
contradiction. Newton's Laws were stated in the present tense as
though forces are instantaneous, but in actuality forces propagate at
a finite speed. I think this contradiction preceded special
relativity. I suspect that this contradiction lead to relativity.
Special relativity started as a means of modifying Newton's Laws so
that there is no logical contradiction.
Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
Bob Kolker
I was pointing out WHY Newton's Laws are not consistent with
special relativity. In particular, Newton's Laws are not Lorentz
invariant. However, I don't think this is immediately obvious even to
somebody with a mathematical background. I myself was a little
confused on this point for a while. There is no explicit constraint on
the form of the force laws in Principia. If a force law is Lorentz
invariant, can't one simply use Newtons Laws to calculate the results?
The answer is that there is no Lorentz invariant force law that is
consistent with Newton's Laws.
A nonmathematical way to show that Newton's Laws are not
consistent with special relativity is simply to look carefully at the
sentences in Principia. They are all in present tense. In other words,
only instantaneous forces are allowed in Principia. Therefore, one
can't have a "force field" with a "finite propagation velocity."
The question was at heart historical, although phrased in an
offensive way. I interpreted his question as meaning this, aside from
the jealous attacks on Einstein. The question is, "Why in the days
before Einstein didn't scientists merely modify the force laws
describing the Michaelson Morley experiment in such a way as to
explain the experimental results?"
I conjectured that the reason is that Newton's Laws and Maxwell's
equations are logically inconsistent. I pointed out where the
inconsistency is in Principia. There are several statements made both
by H. A. Lorentz and A. Einstein that pointed me to that conjecture,
but I honestly can't be 100% sure that this is relevant.
I see ad hominum statements as a cry for help. Calling Einstein
stupid is a desperate plea by a scientific illiterate clarification on
a misunderstood point that irritates his or her learning disability. I
try relieve the inner conflict by providing a historical conjecture
that will help him or her make sense of a world that is beyond their
feeble comprehension.
Darwin123, you have not explained the most important part.
The reason I was confused over this is because of the conservation of
momentum. Assume you're right, and the third law doesn't hold. Observe
this. Momentum is conserved in Special Relativity. Momentum remains a
constant. Force is the change of momentum over time. Therefore, the
total force must always be zero. But that would mean that for every 2-
body system, Newton's third law WILL hold. So how do you explain that?
Ram.
Because in addition to bodies, as described by Newton, the
universe includes fields. Disturbances in the fields carry momentum
and energy, and in a broad way can be said to carry mass. The
electromagnetic field was "discovered" by Faraday. However, it was not
recognized as a "body" in the language of Newton. For one thing, it
can not be localized as a "particle." The bodies described by Newton,
and analyzed in his diagrams, are extremely localized.
There are other types of "fields" by the way. GR describes
everything in terms of field equations. In fact, the fanciest
modern physics describes just about everything as a disturbance in a
field. However, these fields do not have all the properties assigned
to a "body" that is described in Principia. Therefore, the description
of the universe in Principia has a flaw in it. This may have been
recognized by some scientists as soon as Faraday published his results
on fields. When Maxwells equations came out, it was certain there was
a flaw. It was definitely on the mind of H. A. Lorentz.
One way around this may be to define bodies as being any material
body or as a localized disturbance in a field. A lot of people prefer
to describe light as "photons," which do satisfy some of the
requirements of being a "body" as described in Principia.
Unfortunately, they follow the rules of quantum mechanics. So defining
photons as a "body" doesn't work completely.
I get the feeling that the problem really started with "fields."
Both SR and GR handle fields in a logically self consistent way.
I am not going to say Einstein solved the problem completely all by
himself. In fact, he was certainly working on a problem that other
people were working on. That was why his work was so interesting, and
why his ideas caught on almost immediately (relative to other
breakthroughs, of course).
Interestingly, the electromagnetic field without electric charges
is both Galilean and Lorentz invariant. If you work at it, you may
find a set of "Galilean transformations" that work for photons without
electric charges. This theory would work for light and light alone.
Adding an electron would throw off all the calculations. In other
words, a universe with photons and photons only would be both Galilean
and Lorentz invariant, because either transformation would work. It
turns out that electrically charged "bodies" are not Galilean
invariant, only Lorentz invariant. Since we are all made of
electrically charged "bodies," this theory would not be very useful.
A lot of cranks try to "prove" relativity wrong by developing a
Galilean theory that works ONLY for electromagnetic fields. I like
watching them. Its sort of like watching a fakir doing some amazing
feat of self abuse. |
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| Rock Brentwood |
Posted: Mon Apr 07, 2008 9:44 am |
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On Apr 6, 5:40 pm, "Androcles" <Headmas...@Hogwarts.physics> wrote:
Quote: --
This message is brought to you by Androcles
http://www.androcles01.pwp.blueyonder.co.uk/
"Robert J. Kolker" <bobkol...@comcast.net> wrote in messagenews:pPqdnTx62_sicWXanZ2dnUVZ_oWdnZ2d@comcast.com...| Darwin123 wrote:
| Newton and Maxwell's
| > equations are technically in contradiction.
|
| > Maxwell's equations and Newton's Laws are in logical
| > contradiction. Newton's Laws were stated in the present tense as
| > though forces are instantaneous, but in actuality forces propagate at
| > a finite speed. I think this contradiction preceded special
| > relativity. I suspect that this contradiction lead to relativity.
| > Special relativity started as a means of modifying Newton's Laws so
| > that there is no logical contradiction.
|
| Newton's Laws are not Lorentz Invariant. Therefore they are wrong.
|
Newton's Laws are not Lorentz Invariant. Therefore they are right, crank.
The Lorentz relations D = epsilon_0 E, B = mu_0 H for the
electromagnetic field in free space in vacuuo are both Lorentz
invariant and right -- and quite obviously so, since that´s, in large
measure, how where the name "Lorentz invariance" came from in the
first place! Therefore, you're wrong for saying "therefore", since
this serves as a counter-example of something that is Lorentz-
invariant and yet not wrong. |
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| Darwin123 |
Posted: Mon Apr 07, 2008 12:42 pm |
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On Apr 7, 4:41 pm, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
Quote: On Mon, 7 Apr 2008, ram.rac...@gmail.com wrote:
The reason I was confused over this is because of the conservation of
momentum. Assume you're right, and the third law doesn't hold. Observe
this. Momentum is conserved in Special Relativity. Momentum remains a
constant. Force is the change of momentum over time. Therefore, the
total force must always be zero. But that would mean that for every 2-
body system, Newton's third law WILL hold. So how do you explain that?
Newton's 3 laws of motion can be summarised as "momentum is conserved",
with a definition of force thrown in for good measure. Sounds nicely
compatible with special relativity (given some care in what the derivative
in the rate of change of momentum in the definition of force is taken
w.r.t.).
What is incompatible between Newton and SR are: (a) Newton's definition of
mass, as the quantity of matter, vs SR magnitude of the energy-momentum
4-vector, (b) Newton's definition of momentum, and (c) if you include it
as part of Newtonian dynamics, Newton's law of universal gravitation.
In SR, there are no separated 2-body systems with forces. If the 2 bodies
are separated, and there is a force acting between them, it's mediated by
a field, and this field can transport energy and momentum. For 2-body
systems where the bodies only interact when in contact, Newton's 3rd will
be fine. For separated 2-body+field systems, it'll work too, if you assume
that you can exert a force on a field, defined by Newton's 2nd.
I don't think a field, or even a little piece of a field, can be
thought of as a body in the Principia sense. Fields obey the laws of
vector addition, while bodies do not. Bodies have no equivalent to
interference and diffraction, such as waves. Waves are simply
disturbances in the field, the interference and diffraction is a
result of the vector addition of fields. Principia is a complete
description of the dynamics of bodies. However, there is nothing in
Principia that corresponds to interference between bodies.
One can not use Newtons Laws to describe the behavior of light,
as known in the nineteenth century. If you apply Newton's Third Law to
the electromagnetic field, you get a result that indeed conserves
momentum but doesn't describe diffraction. The real electromagnetic
field obeys the law of superposition. Therefore, one can't consider
the electromagnetic field a body. But more important, you can't
consider the Third Law of motion to be exactly equivalent to
conservation of momentum.
We can wrangle about whether or not the third law is the same as
momentum conservation. I just know that H. A. Lorentz was concerned
about the contradictions between mechanics and electromagnetic theory.
He said so.
Obviously, there is some type of gap between Maxwell's equations
and Principia. I am proposing that it shows itself in the language
and diagrams of Principia. Principia seems to contradict Maxwell's
equations. There is no "field" in Principia and no "body" in Maxwell's
equations. Modern physics uses hybrid concepts that were not available
to either Einstein or Lorentz. In fact, they helped develop these
hybrid concepts.
I am not sure of all this. Relativity is an advocation of mine. I
am a physicist working in an unrelated area. If you know how Principia
and Maxwell's equation are compatible, please describe Maxwell's
equations in terms of Newton's Three Laws. |
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| Timo A. Nieminen |
Posted: Mon Apr 07, 2008 3:41 pm |
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On Mon, 7 Apr 2008, ram.rachum@gmail.com wrote:
Quote: The reason I was confused over this is because of the conservation of
momentum. Assume you're right, and the third law doesn't hold. Observe
this. Momentum is conserved in Special Relativity. Momentum remains a
constant. Force is the change of momentum over time. Therefore, the
total force must always be zero. But that would mean that for every 2-
body system, Newton's third law WILL hold. So how do you explain that?
Newton's 3 laws of motion can be summarised as "momentum is conserved",
with a definition of force thrown in for good measure. Sounds nicely
compatible with special relativity (given some care in what the derivative
in the rate of change of momentum in the definition of force is taken
w.r.t.).
What is incompatible between Newton and SR are: (a) Newton's definition of
mass, as the quantity of matter, vs SR magnitude of the energy-momentum
4-vector, (b) Newton's definition of momentum, and (c) if you include it
as part of Newtonian dynamics, Newton's law of universal gravitation.
In SR, there are no separated 2-body systems with forces. If the 2 bodies
are separated, and there is a force acting between them, it's mediated by
a field, and this field can transport energy and momentum. For 2-body
systems where the bodies only interact when in contact, Newton's 3rd will
be fine. For separated 2-body+field systems, it'll work too, if you assume
that you can exert a force on a field, defined by Newton's 2nd.
--
Timo Nieminen - Home page: http://www.physics.uq.edu.au/people/nieminen/
E-prints: http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits: http://www.users.bigpond.com/timo_nieminen/spirits.html |
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| Darwin123 |
Posted: Mon Apr 07, 2008 4:26 pm |
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On Apr 7, 8:37 pm, Timo Nieminen <t...@physics.uq.edu.au> wrote:
Quote: On Mon, 7 Apr 2008, Darwin123 wrote:
On Apr 7, 4:41 pm, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, ram.rac...@gmail.com wrote:
Rather, one would use Maxwell's equations (etc) to obtain the same result
as Newton's laws (see further below), in an appropriate limit.
Key qualifier: In the appropriate limit. Maxwell's equations are
still considered more accurate than Newton's Laws. There is no way to
extract a force law consistent with both Maxwell's equations and
Newton's Laws at the same time. As a special limit, sure.
Quote:
Probably the best way to approach this would be via Lagrangian field
theory, given that we know the equivalence between the Lagrangian
formulation of classical dynamics and Newtonian mechanics.
Yes, there are relativistic Lagrangians which describe a charged
particle and an electromagnetic field. One can defined generalized
momentum which describes both the change in momentum of both charged
particle and field. However, the effects on the field will fall
outside Principia. A field can't obey Newton's three laws of motion,
in their original formulation.
Newton's three laws can be formulated into Lagrangian form.
However, not all Lagrangians are equivalent to Newton's Three Laws.
The problem with these guys using the aether is that they assume
the aether can obey Newton's Laws. It can't. Neither can derive the
force on a charged particle using the aether. Some cranks really show
themselves when I ask, straight up, to derive the Lorentz Force Law
using the concept of aether. It can't be done.
Lorentz Force Law:
F=q(E+vxB) |
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| Timo Nieminen |
Posted: Mon Apr 07, 2008 7:37 pm |
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On Mon, 7 Apr 2008, Darwin123 wrote:
Quote: On Apr 7, 4:41 pm, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, ram.rac...@gmail.com wrote:
The reason I was confused over this is because of the conservation of
momentum. Assume you're right, and the third law doesn't hold. Observe
this. Momentum is conserved in Special Relativity. Momentum remains a
constant. Force is the change of momentum over time. Therefore, the
total force must always be zero. But that would mean that for every 2-
body system, Newton's third law WILL hold. So how do you explain that?
Newton's 3 laws of motion can be summarised as "momentum is conserved",
with a definition of force thrown in for good measure. Sounds nicely
compatible with special relativity (given some care in what the derivative
in the rate of change of momentum in the definition of force is taken
w.r.t.).
What is incompatible between Newton and SR are: (a) Newton's definition of
mass, as the quantity of matter, vs SR magnitude of the energy-momentum
4-vector, (b) Newton's definition of momentum, and (c) if you include it
as part of Newtonian dynamics, Newton's law of universal gravitation.
In SR, there are no separated 2-body systems with forces. If the 2 bodies
are separated, and there is a force acting between them, it's mediated by
a field, and this field can transport energy and momentum. For 2-body
systems where the bodies only interact when in contact, Newton's 3rd will
be fine. For separated 2-body+field systems, it'll work too, if you assume
that you can exert a force on a field, defined by Newton's 2nd.
I don't think a field, or even a little piece of a field, can be
thought of as a body in the Principia sense.
Perhaps not in a strict Principia sense (given that it can have zero
[rest] mass, it isn't a material body in any Newtonian sense), but you can
sensibly deal with it in terms of Newton's laws. This requires considering
it as "body" of infinite extent
Quote: Fields obey the laws of
vector addition, while bodies do not.
[cut etc]
Vector fields obey the laws of vector addition, scalar fields scalar
addition, etc. But this is, AFAICT, not relevant to the point.
Quote: Principia is a complete
description of the dynamics of bodies.
Strictly speaking, no. Non-rotating rigid bodies, effectively point
masses, yes. Real bodies are neither rigid nor point masses - Newton's
treatment in Principia is an idealisation.
A proper treatment would be in terms of field theory - basically classical
continuum mechanics.
(a) Classical continuum mechanics is not compatible with special
relativity. This is not in the field equations, but in the constitutive
relations. Likewise, the Maxwell equations, in and of themselves, are
compatible with both Galileian and special relativity. It's the choice of
the consitutive relations that matter. For a historical perspective,
compare Maxwell's and Hertz's choices of consitutive relations (for
reference frames moving relative to their assumed-to-exist aethers) with
Lorentz's (and Minkowski's and Einstein's) choice.
(b) There isn't any fundamental incompatibility between field theory as
such and Newton. One can have a field theory that gives Newtonian
mechanics in an appropriate limit, without taking any relativistic to
non-relativistic limit (and we have at least two, namely classical
continuum mechanics and non-relativistic quantum mechanics)
Quote: One can not use Newtons Laws to describe the behavior of light,
as known in the nineteenth century. If you apply Newton's Third Law to
the electromagnetic field, you get a result that indeed conserves
momentum but doesn't describe diffraction.
Insufficient does not mean incompatible. Neither can you describe the
behaviour of light, as known in the 20th/21st century using special
relativistic mechanics. Both Newton and SR are insufficient, since neither
is a field theory.
Quote: The real electromagnetic
field obeys the law of superposition. Therefore, one can't consider
the electromagnetic field a body. But more important, you can't
consider the Third Law of motion to be exactly equivalent to
conservation of momentum.
We can wrangle about whether or not the third law is the same as
momentum conservation.
The 3d law alone is not, but one is quite justified in saying N1+N2+N3 is
a statement about the conservation of momentum.
Anyway, take a bunch of Newtonian point masses in space. Newton's laws are
insufficient to tell you what happens - you need a force law as well.
Newton's law of universal gravitation (clearly non-relativistic) is an
addition to the laws of mechanics. True, it appears in the Principia, but
note that it doesn't appear as one of the laws of motion. Now, a
relativistically-compatible electromagnetic force law is significantly
more complicated, and we face two choices: do two bodies (charged
particles, presumably, in this case) exert forces directly on each other
(in which case, due to retardation, we need to throw away conservation of
momentum in the usual sense), or do they interact with the field, exchange
momentum with the field? The latter retains the conservation of momentum,
but _requires_ the field to be treated as a body.
But this is fundamentally little different from considering two bodies in
a fluid (or elastic solid) interacting via the fluid - changes in the
influence of one body on the other will require a non-zero time to
propagate from one body to the other. But given that in this case, the
fluid can be divided up into infinitesimal mass elements that interact
with each other according to Newton's laws, I wouldn't say that this type
of interaction is incompatible with Newton's laws.
Quote: I just know that H. A. Lorentz was concerned
about the contradictions between mechanics and electromagnetic theory.
He said so.
Obviously, there is some type of gap between Maxwell's equations
and Principia. I am proposing that it shows itself in the language
and diagrams of Principia. Principia seems to contradict Maxwell's
equations. There is no "field" in Principia and no "body" in Maxwell's
equations. Modern physics uses hybrid concepts that were not available
to either Einstein or Lorentz. In fact, they helped develop these
hybrid concepts.
I am not sure of all this. Relativity is an advocation of mine. I
am a physicist working in an unrelated area. If you know how Principia
and Maxwell's equation are compatible, please describe Maxwell's
equations in terms of Newton's Three Laws.
Rather, one would use Maxwell's equations (etc) to obtain the same result
as Newton's laws (see further below), in an appropriate limit.
Probably the best way to approach this would be via Lagrangian field
theory, given that we know the equivalence between the Lagrangian
formulation of classical dynamics and Newtonian mechanics.
That said, if one starts from a relativistic field theory, you won't get
Newtonian mechanics back out. Newton's laws of motion, sure, but not
Newton's mass or momentum. From a suitable non-relativistic field
theory, you'll get the lot. Note that my original response was restricted
to Newton's _Laws_, not Newton's Principia.
--
Timo Nieminen - Home page: http://www.physics.uq.edu.au/people/nieminen/
E-prints: http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits: http://www.users.bigpond.com/timo_nieminen/spirits.html |
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| Timo Nieminen |
Posted: Mon Apr 07, 2008 9:58 pm |
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On Mon, 7 Apr 2008, Darwin123 wrote:
Quote: On Apr 7, 8:37 pm, Timo Nieminen <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, Darwin123 wrote:
On Apr 7, 4:41 pm, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, ram.rac...@gmail.com wrote:
Rather, one would use Maxwell's equations (etc) to obtain the same result
as Newton's laws (see further below), in an appropriate limit.
Key qualifier: In the appropriate limit. Maxwell's equations are
still considered more accurate than Newton's Laws. There is no way to
extract a force law consistent with both Maxwell's equations and
Newton's Laws at the same time. As a special limit, sure.
Sure there's a way. See, e.g., Jackson pp 105-108. Once you have the
canonical energy-momentum tensor, you know what the momentum and energy
density of the field is (assuming one can identify the integrands in the
relevant conservation laws with the density of the conserved quantities).
Maxwell's equations tell you how the energy and momentum moves from one
place to another in the field, the Lorentz force tells you the forces
involved in the interaction with matter, and, given that the force
exterted by the field is indeed equal to the rate of loss of momentum of
the field, how can this _not_ be consistent with Newton's laws? Of
course, not consistent with Newton's definition of momentum.
--
Timo Nieminen - Home page: http://www.physics.uq.edu.au/people/nieminen/
E-prints: http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits: http://www.users.bigpond.com/timo_nieminen/spirits.html |
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| ram.rachum@gmail.com |
Posted: Mon Apr 07, 2008 11:10 pm |
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On Apr 8, 5:58 am, Timo Nieminen <t...@physics.uq.edu.au> wrote:
Quote: On Mon, 7 Apr 2008, Darwin123 wrote:
On Apr 7, 8:37 pm, Timo Nieminen <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, Darwin123 wrote:
On Apr 7, 4:41 pm, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
On Mon, 7 Apr 2008, ram.rac...@gmail.com wrote:
Rather, one would use Maxwell's equations (etc) to obtain the same result
as Newton's laws (see further below), in an appropriate limit.
Key qualifier: In the appropriate limit. Maxwell's equations are
still considered more accurate than Newton's Laws. There is no way to
extract a force law consistent with both Maxwell's equations and
Newton's Laws at the same time. As a special limit, sure.
Sure there's a way. See, e.g., Jackson pp 105-108. Once you have the
canonical energy-momentum tensor, you know what the momentum and energy
density of the field is (assuming one can identify the integrands in the
relevant conservation laws with the density of the conserved quantities).
Maxwell's equations tell you how the energy and momentum moves from one
place to another in the field, the Lorentz force tells you the forces
involved in the interaction with matter, and, given that the force
exterted by the field is indeed equal to the rate of loss of momentum of
the field, how can this _not_ be consistent with Newton's laws? Of
course, not consistent with Newton's definition of momentum.
--
Timo Nieminen - Home page:http://www.physics.uq.edu.au/people/nieminen/
E-prints:http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits:http://www.users.bigpond.com/timo_nieminen/spirits.html
I'm pretty confused Timo. So how do I calculate the electric force on
a particle, if that force is carried by a finite-speed field?
Ram. |
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