non-zero divergence of stress energy tensor
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are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
if the divergence of the energy momentum tensor is non-zero, what does that tell us about the spacetime aside from the fact that energy momentum is not conserved?
general-relativity stress-energy-momentum-tensor
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are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
if the divergence of the energy momentum tensor is non-zero, what does that tell us about the spacetime aside from the fact that energy momentum is not conserved?
general-relativity stress-energy-momentum-tensor
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@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago
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favorite
up vote
1
down vote
favorite
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
if the divergence of the energy momentum tensor is non-zero, what does that tell us about the spacetime aside from the fact that energy momentum is not conserved?
general-relativity stress-energy-momentum-tensor
New contributor
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
if the divergence of the energy momentum tensor is non-zero, what does that tell us about the spacetime aside from the fact that energy momentum is not conserved?
general-relativity stress-energy-momentum-tensor
general-relativity stress-energy-momentum-tensor
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edited 1 hour ago
Ben Crowell
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asked 1 hour ago
jboy
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@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago
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@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago
@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago
@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago
add a comment |Â
2 Answers
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General relativity does not allow a stress-energy tensor with a nonvanishing divergence. The Einstein field equations set the Einstein curvature tensor proportional to the stress-energy tensor. The Einstein curvature tensor is constructed in such a way that it is automatically divergence-free.
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
No. If you write down a metric, the way you find the corresponding stress-energy tensor is to use the Einstein field equations, but the field equations will always give a divergence-free stress-energy tensor.
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
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Stress-Energy Tensor is defined, at least in QFT, as the Noehter current associated with infinitesimal space-time translations. Let me explain, consider an infinitesimal space-time translations such as
$x'^mu = x^mu-epsilon^mu$
If we require the field $phi$ to be invariant under the transformation we've just written down, we can then apply Noether's Theorem. Thus, we say there are four conserved currents, one for each space-time direction. Putting this four currents all together in a big $4times4$ matrix, we get the Stress-Energy Tensor $T^munu$
$T^munu = fracpartialmathcalLpartial(partial_mu phi)partial_nu phi-delta^munumathcalL$
It can be easly shown that, since the $T^munu$ is made up of conserved currents, it has zero divergence:
$partial_nu T^munu = 0$
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2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
5
down vote
General relativity does not allow a stress-energy tensor with a nonvanishing divergence. The Einstein field equations set the Einstein curvature tensor proportional to the stress-energy tensor. The Einstein curvature tensor is constructed in such a way that it is automatically divergence-free.
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
No. If you write down a metric, the way you find the corresponding stress-energy tensor is to use the Einstein field equations, but the field equations will always give a divergence-free stress-energy tensor.
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
add a comment |Â
up vote
5
down vote
General relativity does not allow a stress-energy tensor with a nonvanishing divergence. The Einstein field equations set the Einstein curvature tensor proportional to the stress-energy tensor. The Einstein curvature tensor is constructed in such a way that it is automatically divergence-free.
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
No. If you write down a metric, the way you find the corresponding stress-energy tensor is to use the Einstein field equations, but the field equations will always give a divergence-free stress-energy tensor.
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
add a comment |Â
up vote
5
down vote
up vote
5
down vote
General relativity does not allow a stress-energy tensor with a nonvanishing divergence. The Einstein field equations set the Einstein curvature tensor proportional to the stress-energy tensor. The Einstein curvature tensor is constructed in such a way that it is automatically divergence-free.
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
No. If you write down a metric, the way you find the corresponding stress-energy tensor is to use the Einstein field equations, but the field equations will always give a divergence-free stress-energy tensor.
General relativity does not allow a stress-energy tensor with a nonvanishing divergence. The Einstein field equations set the Einstein curvature tensor proportional to the stress-energy tensor. The Einstein curvature tensor is constructed in such a way that it is automatically divergence-free.
are there spacetime metrics where $nabla_nuT^munu ne 0$ ?
No. If you write down a metric, the way you find the corresponding stress-energy tensor is to use the Einstein field equations, but the field equations will always give a divergence-free stress-energy tensor.
answered 1 hour ago
Ben Crowell
44.5k3146271
44.5k3146271
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
add a comment |Â
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
The only comment I would add is the fact that there are space-times that "almost" have a violation of stress-energy that is created by assuming a situation that cannot be in equilibrium (such as two static black holes next to each other). These kinds of assumptions result in the various "strut" and "string" singularities in solutions to Einstein equations.
â Void
1 hour ago
add a comment |Â
up vote
1
down vote
Stress-Energy Tensor is defined, at least in QFT, as the Noehter current associated with infinitesimal space-time translations. Let me explain, consider an infinitesimal space-time translations such as
$x'^mu = x^mu-epsilon^mu$
If we require the field $phi$ to be invariant under the transformation we've just written down, we can then apply Noether's Theorem. Thus, we say there are four conserved currents, one for each space-time direction. Putting this four currents all together in a big $4times4$ matrix, we get the Stress-Energy Tensor $T^munu$
$T^munu = fracpartialmathcalLpartial(partial_mu phi)partial_nu phi-delta^munumathcalL$
It can be easly shown that, since the $T^munu$ is made up of conserved currents, it has zero divergence:
$partial_nu T^munu = 0$
New contributor
add a comment |Â
up vote
1
down vote
Stress-Energy Tensor is defined, at least in QFT, as the Noehter current associated with infinitesimal space-time translations. Let me explain, consider an infinitesimal space-time translations such as
$x'^mu = x^mu-epsilon^mu$
If we require the field $phi$ to be invariant under the transformation we've just written down, we can then apply Noether's Theorem. Thus, we say there are four conserved currents, one for each space-time direction. Putting this four currents all together in a big $4times4$ matrix, we get the Stress-Energy Tensor $T^munu$
$T^munu = fracpartialmathcalLpartial(partial_mu phi)partial_nu phi-delta^munumathcalL$
It can be easly shown that, since the $T^munu$ is made up of conserved currents, it has zero divergence:
$partial_nu T^munu = 0$
New contributor
add a comment |Â
up vote
1
down vote
up vote
1
down vote
Stress-Energy Tensor is defined, at least in QFT, as the Noehter current associated with infinitesimal space-time translations. Let me explain, consider an infinitesimal space-time translations such as
$x'^mu = x^mu-epsilon^mu$
If we require the field $phi$ to be invariant under the transformation we've just written down, we can then apply Noether's Theorem. Thus, we say there are four conserved currents, one for each space-time direction. Putting this four currents all together in a big $4times4$ matrix, we get the Stress-Energy Tensor $T^munu$
$T^munu = fracpartialmathcalLpartial(partial_mu phi)partial_nu phi-delta^munumathcalL$
It can be easly shown that, since the $T^munu$ is made up of conserved currents, it has zero divergence:
$partial_nu T^munu = 0$
New contributor
Stress-Energy Tensor is defined, at least in QFT, as the Noehter current associated with infinitesimal space-time translations. Let me explain, consider an infinitesimal space-time translations such as
$x'^mu = x^mu-epsilon^mu$
If we require the field $phi$ to be invariant under the transformation we've just written down, we can then apply Noether's Theorem. Thus, we say there are four conserved currents, one for each space-time direction. Putting this four currents all together in a big $4times4$ matrix, we get the Stress-Energy Tensor $T^munu$
$T^munu = fracpartialmathcalLpartial(partial_mu phi)partial_nu phi-delta^munumathcalL$
It can be easly shown that, since the $T^munu$ is made up of conserved currents, it has zero divergence:
$partial_nu T^munu = 0$
New contributor
New contributor
answered 7 mins ago
Matteo Campagnoli
814
814
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New contributor
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jboy is a new contributor. Be nice, and check out our Code of Conduct.
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@BenCrowell Yes. Still the fact that you have to use the field equations in your answer worries me. Maybe you should add that these are classical statements. (But you are right, I misread the question.)
â marmot
1 hour ago