Flow line in conservative vector field

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In a conservative vector field defined by F=-grad(f), flow lines c(t) represent the motion of a particle influenced by potential energy f. The discussion demonstrates that as the particle moves along the flow line, its potential energy f(c(t)) decreases, confirming that the particle always moves towards regions of lower potential energy. The relationship between the flow line and the gradient indicates that the tangent to the flow line is directed opposite to the gradient, reinforcing the decrease in potential energy. The limit of F(c(t)) as t approaches infinity suggests that the particle will eventually stabilize at a point of minimum potential energy. Overall, the analysis confirms the behavior of particles in conservative fields, emphasizing the connection between flow lines and potential energy gradients.
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))##?
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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