Stress-energy tensor for a rotating object

In summary, stress-energy tensors have components that represent different physical quantities, including density and pressure. Angular momentum is likely included in the T0k terms, which represent energy flow in a rotating object. The quantities T21, T31, and T32 may also have a role in this. To incorporate the rotational kinetic energy of a neutron star with a frequency of 1000 Hz, one could use the equation E_k=1/2\cdot 0.4mr^2\cdot (f\pi2)^2. Additionally, the shear stress quantities T12, T13, and T23 may apply in certain situations, but further investigation is needed.
  • #1
stevebd1
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I'm currently looking at stress-energy tensors and while I understand that T00 is density and T11, T22 and T33 are pressure, where does angular momentum fit in this? I'm assuming the quantities T21, T31 and T32 might have something to do with this. For example, how would you incorporate the rotational kinetic energy of a neutron star with a frequency of 1000 Hz? [itex](E_k=1/2\cdot 0.4mr^2\cdot (f\pi2)^2)[/itex] Also, when might the shear stress quantities, T12, T13 and T23 apply? Cheers.

Steve
 

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  • #2
I think angular momentum is in the T0k terms. This represents an energy flow, which clearly exists in a rotating object.
 
  • #3
,

The stress-energy tensor for a rotating object takes into account both mass-energy and angular momentum. The quantities T21, T31, and T32 represent the components of the tensor that correspond to the angular momentum of the object. This means that they describe the flow of angular momentum in different directions.

To incorporate the rotational kinetic energy of a neutron star with a frequency of 1000 Hz, you would need to calculate the energy density at each point in the object using the formula you provided (E_k=1/2\cdot 0.4mr^2\cdot (f\pi2)^2). This energy density would then be included in the T00 component of the tensor, which represents the total energy density of the object.

The shear stress quantities, T12, T13, and T23, would apply in situations where there is a shearing force acting on the object, such as in the case of a rotating object. These components of the tensor represent the stresses that arise due to the object's rotation and its resistance to deformation.

I hope this helps clarify the role of angular momentum and shear stress in the stress-energy tensor for a rotating object. Let me know if you have any further questions. Cheers!
 

Related to Stress-energy tensor for a rotating object

What is the stress-energy tensor for a rotating object?

The stress-energy tensor for a rotating object is a mathematical representation of the distribution of energy and momentum in a rotating system. It is a 4x4 matrix that describes the flow of energy and momentum in space and time.

How is the stress-energy tensor calculated for a rotating object?

The stress-energy tensor is calculated using the equations of general relativity and the properties of the rotating object, such as its mass, angular velocity, and moment of inertia. It takes into account both the gravitational and rotational effects on the energy and momentum in the system.

What information can be obtained from the stress-energy tensor for a rotating object?

The stress-energy tensor provides information about the energy density, momentum density, and stress distribution in a rotating system. It can also be used to calculate the gravitational and inertial effects of the object on the surrounding space.

How does the stress-energy tensor for a rotating object differ from that of a stationary object?

The stress-energy tensor for a rotating object includes additional terms that account for the rotational energy and momentum of the system. These terms are not present in the stress-energy tensor for a stationary object. Additionally, the overall structure of the tensor is different due to the presence of rotational effects.

Why is the stress-energy tensor important for understanding rotating objects?

The stress-energy tensor is important because it allows for a comprehensive understanding of the energy and momentum distribution in a rotating system. It is a crucial tool in the study of general relativity and helps to explain the effects of rotation on space and time. It also has practical applications in areas such as astrophysics and engineering.

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