When to use the material derivative?

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SUMMARY

The discussion focuses on the application of the material derivative in fluid mechanics, particularly in the context of the Navier-Stokes equations and Stokes' drag law. It clarifies that the acceleration term is represented as ##\frac{dV}{dt}## when velocity is solely dependent on time, as opposed to the more complex expression ##\frac{\partial V}{\partial t} + V \frac{dV}{dx}##, which accounts for spatial variation. The material derivative is defined as a total derivative that incorporates both time and spatial dependencies, illustrated through examples such as temperature changes in a lake and flow in a pipe.

PREREQUISITES
  • Understanding of fluid mechanics principles, specifically the Navier-Stokes equations.
  • Familiarity with Stokes' drag law and its implications for particle motion.
  • Knowledge of derivatives, including total and partial derivatives.
  • Basic concepts of flow dynamics in confined spaces, such as pipes.
NEXT STEPS
  • Study the derivation and applications of the Navier-Stokes equations in fluid dynamics.
  • Explore the implications of Stokes' drag law in various fluid flow scenarios.
  • Learn about the material derivative and its significance in both theoretical and practical fluid mechanics.
  • Investigate temperature distribution and its effects on fluid behavior in natural bodies of water.
USEFUL FOR

This discussion is beneficial for fluid mechanics students, researchers in applied physics, and engineers working on fluid dynamics problems, particularly those involving particle motion and flow analysis.

member 428835
Hi PF!
When doing a force balance in fluid mechanics, ##\sum F = D_t(mV)##. This equation typically results to the Navier-Stokes equations. I'm reading a the following problem:

For small particles at low velocities, the first (linear) term in Stokes’ drag law implies ##F = kV##, where ##k## is a constant. Suppose a particle of mass ##m## is constrained to move horizontally.

They then solve this equation for the particle's velocity by taking ##-kV = m\frac{dV}{dt}##. My question is, how do we know the acceleration term is ##\frac{dV}{dt}## instead of ##\frac{\partial V}{\partial t} + V \frac{dV}{dx}##?
 
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joshmccraney said:
Hi PF!
When doing a force balance in fluid mechanics, ##\sum F = D_t(mV)##. This equation typically results to the Navier-Stokes equations. I'm reading a the following problem:

For small particles at low velocities, the first (linear) term in Stokes’ drag law implies ##F = kV##, where ##k## is a constant. Suppose a particle of mass ##m## is constrained to move horizontally.

They then solve this equation for the particle's velocity by taking ##-kV = m\frac{dV}{dt}##. My question is, how do we know the acceleration term is ##\frac{dV}{dt}## instead of ##\frac{\partial V}{\partial t} + V \frac{dV}{dx}##?
It depends on whether your velocity depends only on time or on location as well. The material derivative is a total derivative, that depends on time and space. E.g. if you have a flow in a pipe, it only depends on time and not on the location whithin the pipe, that is ##\frac{dV}{dt}##.

Wikipedia explains by an example of a material derivation the following situation:
Given a temperature distribution on the surface of a lake which warms up, e.g. due to sunlight (time component ##\frac{\partial V}{\partial t}##) and due to warmer inflows (local component ##\frac{d V}{d x}##). The partial derivative w.r.t. time describes the change in temperature for a w.r.t. the banks standing observer in the lake, who can only observe the change in time at his fixed place. But since the water also gets warmer along certain directions, an observer in a floating boat would measure these additional changes.
 
fresh_42 said:
It depends on whether your velocity depends only on time or on location as well. The material derivative is a total derivative, that depends on time and space. E.g. if you have a flow in a pipe, it only depends on time and not on the location whithin the pipe, that is ##\frac{dV}{dt}##.
But viscous forces in a pipe slow flow down as the radial location increases, so ##\frac{dV}{dr}\neq0##.

Good analogy!
 
Had my central air system checked when it sortta wasn't working. I guess I hadn't replaced the filter. Guy suggested I might want to get a UV filter accessory. He said it would "kill bugs and particulates". I know UV can kill the former, not sure how he thinks it's gonna murder the latter. Now I'm finding out there's more than one type of UV filter: one for the air flow and one for the coil. He was suggesting we might get one for the air flow, but now we'll have to change the bulb...

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