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Prove using vector tensor operations that for a Newtonian fluid the linear momentum equations: DtDv=g+[((v)+(v)T)32(v)I]PI Can be rewritten as: DtDv=g+2v+31(v)P Where I represents the identity

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Prove using vector tensor operations that for a Newtonian fluid the linear momentum equations: DtDv=g+[((v)+(v)T)32(v)I]PI Can be rewritten as: DtDv=g+2v+31(v)P Where I represents the identity matrix What assumptions do we make to translate this to our typical form of Navier-Stokes found in Appendix B.6

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