What is v(dv/dx) and how does it relate to acceleration?

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SUMMARY

The discussion centers on modeling acceleration using the expression v(dv/dx), which is derived from the chain rule in calculus. This formulation allows for the analysis of motion in one dimension, where v represents velocity as dx/dt. The relationship between v(dv/dx) and acceleration (a) is established as v(dv/dx) = dv/dt = a. This approach is particularly useful in scenarios involving variable forces, such as modeling motion with air resistance, where traditional methods using dv/dt are insufficient.

PREREQUISITES
  • Understanding of calculus, specifically the chain rule.
  • Familiarity with the concepts of velocity and acceleration in physics.
  • Knowledge of differential equations and their applications.
  • Basic principles of fluid dynamics, particularly the material derivative.
NEXT STEPS
  • Study the application of the material derivative in fluid dynamics.
  • Explore the integration of differential equations involving variable forces.
  • Learn about modeling motion with air resistance using differential equations.
  • Investigate the relationship between velocity fields and acceleration in fluid mechanics.
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in advanced mechanics and fluid dynamics will benefit from this discussion, particularly those looking to deepen their understanding of acceleration modeling in variable force scenarios.

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My mechanics syllabus suggests that we can model acceleration as ##v(dv/dx)## but what exactly does this mean? Can you give me (or link me to) some explanations and/or sample problems with worked solutions? In my experience so far we should always be using ##dv/dt## for ##a##.
 
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Consider what v actually is in one dimension:
v = \dfrac{dx}{dt}.
So in using the chain rule,
v\dfrac{dv}{dx} = \dfrac{dx}{dt}\dfrac{dv}{dx} = \dfrac{dv}{dt} = a.
Of course, you could make the same argument with any spatial coordinate. This is intimately related to what is commonly called the material derivative.
 
boneh3ad said:
Consider what v actually is in one dimension:
v = \dfrac{dx}{dt}.
So in using the chain rule,
v\dfrac{dv}{dx} = \dfrac{dx}{dt}\dfrac{dv}{dx} = \dfrac{dv}{dt} = a.
Of course, you could make the same argument with any spatial coordinate. This is intimately related to what is commonly called the material derivative.

Thanks.

What would be the usefulness of something like this? Could you, for example, model motion with air resistance using it? (This is impossible with ##dv/dt## calculus since your balanced expression for acceleration would depend on -kv2, your air resistance, but then ##v## depends on acceleration, meaning the model cannot incorporate air resistance.)
 
Suppose you have a stream of some fluid and you know the velocity field. You would like to know the acceleration of (and hence the forces on) some bit of fluid as it passes by a certain point. This formulation is useful.
 
It's useful when separating differential equations like the following:

a=\frac{k}{r^2}

So you can integrate:

vdv=\frac{k}{r^2}dr

This is used, for example, with finding the time it takes for two masses to come together under gravity.
 

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