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?










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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.)
    – marmot
    1 hour ago















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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?










share|cite|improve this question









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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.)
    – marmot
    1 hour ago













up vote
1
down vote

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?










share|cite|improve this question









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jboy is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
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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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edited 1 hour ago









Ben Crowell

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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.)
    – 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.)
    – 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.)
– 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.)
– marmot
1 hour ago











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.






share|cite|improve this answer




















  • 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.
    – Void
    1 hour ago

















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:



$partial_nu T^munu = 0$






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    2 Answers
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    active

    oldest

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    2 Answers
    2






    active

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    active

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    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.






    share|cite|improve this answer




















    • 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.
      – Void
      1 hour ago














    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.






    share|cite|improve this answer




















    • 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.
      – Void
      1 hour ago












    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.






    share|cite|improve this answer












    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.







    share|cite|improve this answer












    share|cite|improve this answer



    share|cite|improve this answer










    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.
      – 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.
      – 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.
    – 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.
    – Void
    1 hour ago










    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:



    $partial_nu T^munu = 0$






    share|cite








    New contributor




    Matteo Campagnoli is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.





















      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:



      $partial_nu T^munu = 0$






      share|cite








      New contributor




      Matteo Campagnoli is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
      Check out our Code of Conduct.



















        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:



        $partial_nu T^munu = 0$






        share|cite








        New contributor




        Matteo Campagnoli is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
        Check out our Code of Conduct.









        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:



        $partial_nu T^munu = 0$







        share|cite








        New contributor




        Matteo Campagnoli is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
        Check out our Code of Conduct.









        share|cite



        share|cite






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        answered 7 mins ago









        Matteo Campagnoli

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