Partial derivative of potential energy and work

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SUMMARY

The discussion focuses on the relationship between potential energy, conservative forces, and work. It establishes that for a conservative force \(\vec{F} = -\vec{\nabla} U\), the infinitesimal work \(dW\) is given by \(dW = -\vec{\nabla} U \cdot d\vec{s}\). The correct expression for the directional derivative of potential energy \(U\) is \(\vec{\nabla} U \cdot \hat{n}\), where \(\hat{n}\) is a unit vector in the direction of displacement \(d\vec{s}\). The discussion clarifies common misconceptions regarding the notation and interpretation of these mathematical expressions.

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  • Understanding of vector calculus, specifically gradients and directional derivatives.
  • Familiarity with the concepts of conservative forces and potential energy.
  • Knowledge of differential notation in physics and mathematics.
  • Basic comprehension of infinitesimal calculus and its applications in physics.
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Soren4
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For a conservative force \vec{F}=-\vec{\nabla} U \implies dW=-\vec{\nabla}U \cdot d\vec{s}

Where d\vec{s} is the infinitesimal vector displacement.

Does the following hold?

-\frac{\partial U}{\partial \vec{s}}=-\vec{\nabla} U \cdot d\vec{s}=d W, i.e. the infinitesimal work is minus the directional derivative of U in the direction of \vec{s}.
 
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No this doesn't make sense, you've written what the spatial derivative of the potential is, its ##\vec{F}## not dW.
 
Soren4 said:
For a conservative force \vec{F}=-\vec{\nabla} U \implies dW=-\vec{\nabla}U \cdot d\vec{s}

Where d\vec{s} is the infinitesimal vector displacement.

Does the following hold?

-\frac{\partial U}{\partial \vec{s}}=-\vec{\nabla} U \cdot d\vec{s}=d W, i.e. the infinitesimal work is minus the directional derivative of U in the direction of \vec{s}.
Your equation is wrong. It should read ##dU=\vec{\nabla} U \cdot \vec{ds}=-dW##
The interpretation is the infinitesimal work in the direction of ##\vec{ds}## is equal to minus the directional derivative of U in the direction of ##\vec{ds}##.
 
@jamie.j1989 Thanks for the answer, i just applied the rule that uses nabla for directional derivatives, so how to correctly write the directional derivative?@Chestermiller Thanks a lot for the reply, where is the exactly the mistake? Is it the fact of not having specified that the infinitesimal work is in the direction of ##\vec{ds}## ? Moreover how is the directional derivative of ##U## written explicitly, if ##\frac{\partial U}{\partial \vec{s}}## is wrong?
 
The directional derivative of ##U## is ##\vec{\nabla}U = \hat{i}\frac{\partial U}{\partial x}+\hat{j}\frac{\partial U}{\partial y}+\hat{k}\frac{\partial U}{\partial z}= -\left(\hat{i}F_x +\hat{j}F_y+\hat{k}F_z\right)##
 
No, ##\vec \nabla U## is the gradient of U (a vector). The directional derivative of U along a direction specified by a unit vector ##\hat n## is ##\vec \nabla U \cdot \hat n## (a scalar). If you go a distance ##ds## in the direction of ##\hat n##, then the change in U is ##dU = (\vec \nabla U \cdot \hat n) ds = \vec \nabla U \cdot (\hat n ds) = \vec \nabla U \cdot \vec{ds}##.
 
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Thanks a lot for the reply, where is the exactly the mistake? Is it the fact of not having specified that the infinitesimal work is in the direction of ##\vec{ds}## ?
No. It's that you set dU/ds equal to a differential, which, of course, it is not.

Moreover how is the directional derivative of ##U## written explicitly, if ##\frac{\partial U}{\partial \vec{s}}## is wrong?
If ##\vec{s}## is position vector from an arbitrary origin to a position in space, and ##\vec{s}+\vec{ds}## is a position vector from the origin to an adjacent position in space, then the change in potential U between ##\vec{s}## to ##\vec{s}+\vec{ds}## (in the direction of ##\vec{ds}## is given by:
$$dU=\vec{\nabla} U\cdot \vec{ds}$$The derivative of U with respect to distance in the direction of ##\vec{ds}## is obtained by dividing by the magnitude of the differential postion vector ##\vec{ds}##:
$$\frac{dU}{|\vec{ds}|}=\vec{\nabla} U\cdot \left(\frac{\vec{ds}}{|\vec{ds}|}\right)=\vec{\nabla} U\cdot \vec{n}_s$$
where ##\vec{n}_s## is a unit vector in the direction of ##\vec{ds}##.
 
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