About Compressive Forces on Control Volumes

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SUMMARY

Forces acting on control volumes in fluid dynamics are considered compressive due to the nature of pressure as an isotropic component of the stress tensor. In the context of incompressible fluids, the stress tensor is defined as σ = -pI + σ_v, where σ_v represents the viscous stress component and I is the identity tensor. The Cauchy stress relationship confirms that the pressure term contributes to a compressive traction vector on surfaces of arbitrary orientation, which is fundamental in the derivation of the Navier-Stokes equations.

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masshakar
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Why is it that forces (for changes in pressure across a fluid) on the control volume are generally considered compressive? Even in the derivation of the Navier-Stokes equation, it is assumed that forces from fluid pressure will be compressive? Why?
 
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masshakar said:
Why is it that forces (for changes in pressure across a fluid) on the control volume are generally considered compressive? Even in the derivation of the Navier-Stokes equation, it is assumed that forces from fluid pressure will be compressive? Why?
Hi Masshakar. Welcome to Physics Forums!

Pressure represents the isotropic part of the overall stress tensor. In the overall stress tensor [itex]\vec{σ}[/itex] for an incompressible fluid, the stress tensor is represented by:
[tex]\vec{σ}=-p\vec{I}+\vec{σ_v}[/tex]
where [itex]\vec{σ_v}[/itex] represents the viscous part of the stress tensor and [itex]\vec{I}[/itex] is the identity tensor. If we use the Cauchy stress relationship to determine the stress on a surface of arbitrary orientation (by dotting the stress tensor with a unit normal), the contribution of the pressure term to the overall traction vector is compressive.

Chet
 

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