Flow line in conservative vector field

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SUMMARY

The discussion focuses on the behavior of a particle moving along a flow line in a conservative vector field defined by the equation F = -grad(f), where f represents potential energy. It is established that the particle will always move towards lower potential energy, as the flow line c(t) satisfies c'(t) = F(c(t)). The limit of F(c(t)) as t approaches infinity indicates that the particle's potential energy decreases over time, confirming that the flow line leads to a stable state of minimum potential energy.

PREREQUISITES
  • Understanding of vector calculus, specifically gradient and flow lines.
  • Familiarity with conservative vector fields and potential energy concepts.
  • Knowledge of differential equations and their applications in physics.
  • Proficiency in using the chain rule for differentiation.
NEXT STEPS
  • Study the properties of conservative vector fields and their implications in physics.
  • Learn about the mathematical formulation of potential energy and its gradients.
  • Explore the concept of flow lines in more complex vector fields.
  • Investigate the stability of equilibrium points in conservative systems.
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Students of physics and mathematics, particularly those studying mechanics and vector calculus, as well as educators looking to deepen their understanding of conservative forces and potential energy dynamics.

Thomas G
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Homework Statement


Recall that a flow line, c(t), of a vector field F has c'(t)=F(c(t)) at all times t. Show all work below.
a.) Let c(t) be the flow line of a particle moving in a conservative force field F=-grad(f), where f:R^3->R, f(x,y,z) >=0 for all (x,y,z), represents the potential energy at each point in space. Prove that the particle will always move towards a point with lower potential energy. What is the limit of F(c(t)) as t goes to infinity?

Homework Equations


F=-grad(f)
c'(t)=F(c(t))

The Attempt at a Solution


We are trying to show that f(c(t)) is a decreasing function of t. So far, I have that
grad[f(c(t))]=grad(f(c(t))*c'(t) thru chain rule
grad[f(c(t))]=grad(f(c(t))*F(c(t)) because c(t) is a flow line
grad[f(c(t))]=grad(f(c(t))*-grad(f(c(t)) by the definition of F
grad[f(c(t))]=-(grad(f(c(t))^2

But I am not sure if this really helps at all. Is this the right direction to go in, or am I completely off base?
 
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Recall that vectors in a vector field are tangent to the flow lines. Since ##\vec c(t)## is a flow line, you know that ##\vec F(\vec c(t)) = \vec c'(t)##. That is, the vector field of the flow line is equal to the tangent to the flow line for all times ##t##.

You know ##\vec F## is conservative, and so ##\vec F = - \vec{\nabla f} = -(f_x \hat i + f_y \hat j + f_z \hat k)## for some potential function ##f(x, y, z) \geq 0##. The gradient of a function gives the direction of fastest increase. So minus the gradient gives the direction of fastest decrease.

Hence ##\vec F(\vec c(t)) = - \vec{\nabla f}(\vec c(t)) = \vec c'(t)##. Notice the tangent to the flow line is equal to the negative of the gradient of the potential function (which is decreasing). So it must be the case ##\vec c'(t)## is also decreasing. So as the particle moves along the flow line ##\vec c(t)##, its potential energy is decreasing.

Now what about ##\displaystyle \lim_{t \rightarrow \infty} \vec F(\vec c(t))##?
 

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