Newton's Second Law Integral Form

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SUMMARY

The discussion centers on the integral form of Newton's Second Law as applied to fluid dynamics, specifically the equations governing control volumes (CV) and control surfaces (CS). The first equation presented, $$\sum \vec{F} = \frac{\partial}{\partial t} \iiint_{CV} \rho \vec{u} dV +\iint_{CS} \rho \vec{u} ( \vec{u_{rel}} \cdot \hat{n}) dS$$, outlines the forces acting on a control volume. The second equation, $$m_{CV} \frac{d}{dt} \vec{u_{CV}} = \frac{\partial}{\partial t} \iiint_{CV} \rho \vec{u_{CV}} dV +\iint_{CS} \rho \vec{u_{CV}} ( \vec{u_{rel}} \cdot \hat{n}) dS$$, introduces the concept of the control volume's velocity, ##u_{CV}##, which is crucial for understanding the dynamics of fluid motion relative to the control volume. The distinction between fluid velocity and relative velocity is clarified, emphasizing the importance of ##u_{rel}## in determining flux across the control surface.

PREREQUISITES
  • Understanding of fluid dynamics principles
  • Familiarity with control volume and control surface concepts
  • Knowledge of vector calculus and partial derivatives
  • Basic grasp of Newton's laws of motion
NEXT STEPS
  • Study the derivation of the Navier-Stokes equations
  • Learn about the application of Reynolds Transport Theorem in fluid mechanics
  • Explore the concept of mass flow rate and its implications in control volumes
  • Investigate the role of boundary conditions in fluid dynamics problems
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Students and professionals in fluid mechanics, mechanical engineers, and anyone studying the application of Newton's laws in fluid dynamics will benefit from this discussion.

member 428835
Hi PF!

I was reading my book and I understand the following $$\sum \vec{F} = \frac{\partial}{\partial t} \iiint_{CV} \rho \vec{u} dV +\iint_{CS} \rho \vec{u} ( \vec{u_{rel}} \cdot \hat{n}) dS$$ ##CV## is a control volume, ##CS## is control surface, ##u## is velocity, ##u_{rel}## is velocity relative to control volume, and the rest is self-spoken for. However, then the book states the following $$m_{CV} \frac{d}{dt} \vec{u_{CV}} = \frac{\partial}{\partial t} \iiint_{CV} \rho \vec{u_{CV}} dV +\iint_{CS} \rho \vec{u_{CV}} ( \vec{u_{rel}} \cdot \hat{n}) dS$$ where ##u_{CV}## is the velocity of the control volume. Any help in understanding why this is?
 
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The first equation looks OK to me if ##u_{rel}## were replaced by just u. In the second equation, I'm not sure what ##u_{CV}## is supposed to represent.
 
##\vec{u}## is the fluid velocity relative to an inertial frame, while ##\vec{u_{rel}} = \vec{u} − \vec{u_{CV}}## is the fluid velocity relative to the control volume. Then only the fluid velocity relative to the control volume boundary will induce a flux through this boundary. Does that look correct?
 

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