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Balance Laws 1 Lecture 2 ME EN 412 Andrew Ning aning@byu.edu - PDF document

Balance Laws 1 Lecture 2 ME EN 412 Andrew Ning aning@byu.edu Outline Practice Problems Fundamental Principles Mass Balance Momentum Balance Practice Problems Prob 7.37 A sphere of diameter d falls slowly in a highly viscous fluid. What


  1. Balance Laws 1 Lecture 2 ME EN 412 Andrew Ning aning@byu.edu Outline Practice Problems Fundamental Principles Mass Balance Momentum Balance

  2. Practice Problems Prob 7.37 A sphere of diameter d falls slowly in a highly viscous fluid. What parameters might be important?

  3. Only a limited number of experiments can be performed. Can we build a predictive model for the settling velocity? From one experimental run: • V = 0 . 42 ft/s • d = 0.1 in • µ = 0 . 03 lb-s /ft 2 • ∆ γ = 10 lb/ft 3 Fundamental Principles

  4. • Mass is conserved. • F = ma (Newton’s second law) and its angular counterpart. • Energy is conserved (first law of thermodynamics). • Entropy will always increase over time (second law of thermodynamics). It can be produced but not destroyed. All of these concepts can be expressed in terms of balance laws: rate of accumulation = rate of inflow − rate of outflow + rate of production

  5. Control Volumes Mass Balance

  6. Derive mass balance. ∂ � � ρ � W · d � ρdV – + A = 0 ∂t V – S

  7. W is the relative velocity Total velocity: V = � � W + � VV – Momentum Balance

  8. rate of momentum accumulation + rate of outflow − rate of inflow = rate of production Newton’s 2nd Law F = d ( m� V ) Σ � dt

  9. ∂ � � ρ� ρ� V ( � W · d � A ) = Σ � V dV – + F ∂t V – S Any external forces can be applied, but the most common are the fluid pressure forces, fluid viscous forces, and gravitational forces. Pressure: � Σ � pd � F p = − A S Viscous shear stress: � Σ � τ · d � ↔ F v = A S

  10. ∂ � � ρ� ρ� V ( � W · d � – + A ) = V dV ∂t V – S � � � � pd � τ · d � ↔ A + A + F other − S S

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