Partial derivative of potential energy and work

In summary, the infinitesimal work is equal to minus the directional derivative of U in the direction of ##\vec{s}##, which is given by ##\vec{\nabla} U\cdot \vec{n}_s##.
  • #1
Soren4
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For a conservative force [itex]\vec{F}=-\vec{\nabla} U \implies dW=-\vec{\nabla}U \cdot d\vec{s}[/itex]

Where [itex]d\vec{s}[/itex] is the infinitesimal vector displacement.

Does the following hold?

[itex]-\frac{\partial U}{\partial \vec{s}}=-\vec{\nabla} U \cdot d\vec{s}=d W[/itex], i.e. the infinitesimal work is minus the directional derivative of [itex]U[/itex] in the direction of [itex]\vec{s}[/itex].
 
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  • #2
No this doesn't make sense, you've written what the spatial derivative of the potential is, its ##\vec{F}## not dW.
 
  • #3
Soren4 said:
For a conservative force [itex]\vec{F}=-\vec{\nabla} U \implies dW=-\vec{\nabla}U \cdot d\vec{s}[/itex]

Where [itex]d\vec{s}[/itex] is the infinitesimal vector displacement.

Does the following hold?

[itex]-\frac{\partial U}{\partial \vec{s}}=-\vec{\nabla} U \cdot d\vec{s}=d W[/itex], i.e. the infinitesimal work is minus the directional derivative of [itex]U[/itex] in the direction of [itex]\vec{s}[/itex].
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}##.
 
  • #4
@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?
 
  • #5
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)##
 
  • #6
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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  • #7
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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Related to Partial derivative of potential energy and work

1. What is the definition of a partial derivative of potential energy?

A partial derivative of potential energy is the rate of change of potential energy with respect to one of its independent variables, while holding all other variables constant.

2. How is the partial derivative of potential energy related to work?

The partial derivative of potential energy with respect to a specific variable is equal to the negative of the force exerted in that direction. This means that the partial derivative can be used to calculate the work done by a force in that direction.

3. Can the partial derivative of potential energy be negative?

Yes, the partial derivative of potential energy can be negative. This indicates that the force is acting in the opposite direction of the chosen variable, and therefore, the work done by the force is negative.

4. How is the partial derivative of potential energy calculated?

The partial derivative of potential energy can be calculated by taking the derivative of the potential energy function with respect to the chosen variable, while holding all other variables constant.

5. Why is it important to understand the partial derivative of potential energy and work?

Understanding the partial derivative of potential energy and work is crucial in many fields of science, such as physics and chemistry. It allows for the calculation and analysis of forces, energy, and work in complex systems, which is essential for understanding and predicting their behavior.

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