Partial derivatives - proving force is conservative

In summary, the conversation is discussing the concept of conservatism in the context of a force F= k [x, 2y, 3z]. The speaker mentions taking the cross product of the force and the partial derivatives, and questions if everything in the derivatives is constant. They then discuss the process of working out the cross products and mention taking everything in front of the derivatives. The expert summarizer explains that the derivatives are zero because they are unrelated to the respective components, and the conversation continues to clarify and understand the concept.
  • #1
Oblio
398
0
I'm trying to show that the force F= k [x, 2y, 3z] (where k is a constant)

is conservative.

If I take the cross product of:

[tex]\nabla x F, [/tex] that equals [tex]\frac{\partial}{\partial y} F_{z} - \frac{\partial}{\partial z} F_{y}[/tex]

= [tex]\frac{\partial}{\partial y} k3z - \frac{\partial}{\partial z} k2y[/tex]


isn't everything in the derivatives constants? ... or is that the point. lol

Thanks alot
 
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  • #2
You've only worked out the x component of the cross product, what about the rest?
 
  • #3
Hootenanny said:
You've only worked out the x component of the cross product, what about the rest?

I wasn't sure if I had to, the example in my book only did F(x).

Is that much correct though?
If you bring all the constants out, can you be left with nothing in the derivative?

[tex] k3z \frac{\partial}{\partial y} - k2y \frac{\partial}{\partial z} [/tex]
 
  • #4
Oblio said:
I wasn't sure if I had to, the example in my book only did F(x).

Is that much correct though?
If you bring all the constants out, can you be left with nothing in the derivative?

[tex] k3z \frac{\partial}{\partial y} - k2y \frac{\partial}{\partial z} [/tex]
Yup, looks good to me, now all you need to do is continue on with working out the rest of the cross products, do you know how to do that?
 
  • #5
(Didn't mean to double post, sorry. I usually go in the introductory physics and I realized after I was in the advanced; incorrectly I thought)
 
  • #6
Oblio said:
(Didn't mean to double post, sorry. I usually go in the introductory physics and I realized after I was in the advanced; incorrectly I thought)
No worries, just don't do it again, we have big sticks you know...
 
  • #7
Hootenanny said:
Yup, looks good to me, now all you need to do is continue on with working out the rest of the cross products, do you know how to do that?

In the same way I guess... no?

I didn't know I could take everything of a derivative either. cool!
 
  • #8
Hootenanny said:
No worries, just don't do it again, we have big sticks you know...

Not answering my questions might be worse then a good ol' fashion beating :)
 
  • #9
Oblio said:
I wasn't sure if I had to, the example in my book only did F(x).

Is that much correct though?
If you bring all the constants out, can you be left with nothing in the derivative?

[tex] k3z \frac{\partial}{\partial y} - k2y \frac{\partial}{\partial z} [/tex]

Doesn't that leave me with not 0 ? (which I want?)

k3z-k2y ?
 
  • #10
Doesn't look good to me :smile:, you better not be left with nothing in the derivative.
But you're almost there -- I agree with all steps except the one where you take everything in front of the derivative. You can indeed take the numbers and k's out. Then you just need to think about dz/dy and dy/dz (hint: y does not depend on x and z - trivially).
 
  • #11
Okay, so for the full definition;

If we have some vector function such that

[tex]\underline{F} = F_x\hat{i} + F_y\hat{j} + F_z\hat{j}[/tex]

Then;

[tex]curl(\underline{F}) = \nabla\times\underline{F} = \left|\begin{array}
\hat{i} & \hat{j} & \hat{i} \\
\partial/\partial x & \partial/\partial y & \partial/\partial z \\
F_x & F_y & F_z \\
\end{array}\right|[/tex]
 
  • #12
Oblio said:
In the same way I guess... no?

I didn't know I could take everything of a derivative either. cool!

CompuChip said:
Doesn't look good to me :smile:, you better not be left with nothing in the derivative.
But you're almost there -- I agree with all steps except the one where you take everything in front of the derivative. You can indeed take the numbers and k's out. Then you just need to think about dz/dy and dy/dz (hint: y does not depend on x and z - trivially).

I know [tex] \frac{\partial y}{\partial z} [/tex] would be 0 since they're unrelated, but again, the example in my book does indeed take z out of a simliar situation.
 
  • #13
One can take everything in front of the derivative since they are independent of the variable we are taking the derivative wrt.
 
  • #14
That leaves me non zero though, that's not ok is it?
 
  • #15
Oblio said:
That leaves me non zero though, that's not ok is it?
You must have made an error, the curl of that vector field is definitely zero. If you show me your working, I'll point out where you've gone wrong.
 
  • #16
Hootenanny said:
You must have made an error, the curl of that vector field is definitely zero. If you show me your working, I'll point out where you've gone wrong.

Well just factoring out all those constants,

k3z-k2y [tex]\neq[/tex] 0 right?
 
  • #17
Oblio said:
Well just factoring out all those constants,

k3z-k2y [tex]\neq[/tex] 0 right?
Yes, but you don't just have k3z-k2y do you? What else do you have?
 
  • #18
Your saying the y and z components will make it cancel?

I thought this was supposed to (looking at my example again :P )
 
  • #19
Okay, let's look at this again;

[tex]\frac{\partial}{\partial y} k3z - \frac{\partial}{\partial z} k2y = 0 - 0 = 0[/tex]

Since you are taking the derivatives wrt different variables than the respective components both the derivative are equal to zero. Or we can rewrite it like this

[tex]k3z \frac{\partial}{\partial y} 1- k2y\frac{\partial}{\partial z}1 = 0 - 0 = 0[/tex]

Make sense?
 
  • #20
im getting Fy to cancel out, but Fx and Fz adding up to 2Fx and -2k3z
 
  • #21
(i posted that last one before seeing YOUR last one)
 
  • #22
Hootenanny said:
Okay, let's look at this again;

[tex]\frac{\partial}{\partial y} k3z - \frac{\partial}{\partial z} k2y = 0 - 0 = 0[/tex]

Since you are taking the derivatives wrt different variables than the respective components both the derivative are equal to zero. Or we can rewrite it like this

[tex]k3z \frac{\partial}{\partial y} 1- k2y\frac{\partial}{\partial z}1 = 0 - 0 = 0[/tex]

Make sense?

So, its zero since their derivatives are zero?
 
  • #23
Oblio said:
So, its zero since their derivatives are zero?
Yup, essentially your multiplying some constants by zero.
 
  • #24
I thought you were saying something different before, that's why i was confused over something simple:P
 
  • #25
I'm supposed to substitute to verify, using F = -[tex]\nabla U[/tex]

hows this look?

U(x) = -[tex]\int Fx dx = - \int kx = -kxt[/tex]F = -[tex]\nabla U[/tex], so...[tex] =- \frac{\partial}{\partial x} (-kxt) = kt = F (x)[/tex]

I don't know how to work limits into latex but i guess its technically xo -->x

?
 
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  • #26
I'm only not sure because Fx dx in the integral are Fx and dx prime...
 
  • #27
from what I'm reading I think I might need to add a path of the particle?

yes?
I'm confused because the answer seems like its right lol.
 
  • #28
Oblio said:
--- Post #22 ---
Don't get confused, what you had there was correct.
Now what are the equations for the y and z components of the curl?
What do you get when working them out (show the calculation)?
 

FAQ: Partial derivatives - proving force is conservative

How do you define a partial derivative?

A partial derivative is a mathematical concept that measures the rate of change of a function with respect to one of its variables, while holding all other variables constant. It is denoted by the symbol ∂ and is similar to a regular derivative, but with multiple variables involved.

What does it mean for a force to be conservative?

A force is considered conservative if the work done by the force on an object is independent of the path taken. This means that the total work done by the force to move an object from one point to another is the same, regardless of the path taken between the two points.

How can partial derivatives be used to prove that a force is conservative?

To prove that a force is conservative using partial derivatives, we can use the fundamental theorem of calculus. This theorem states that the integral of a function over an interval can be evaluated by finding the antiderivative of the function and evaluating it at the endpoints of the interval. If the partial derivatives of the force in the x and y directions are equal, then the force is conservative.

Are there any real-world applications of proving a force to be conservative?

Yes, there are many real-world applications of proving a force to be conservative. For example, in physics and engineering, it is important to know if a force is conservative in order to accurately predict the motion of objects. In thermodynamics, the concept of a conservative force is used to explain the relationship between heat and work. Additionally, in economics, conservative forces are used to analyze the flow of money in financial systems.

What are some common mistakes when proving a force to be conservative using partial derivatives?

One common mistake is assuming that if the partial derivatives of a force are equal, then the force is automatically conservative. This is not always true, as there are other conditions that need to be met. Another mistake is not considering the domain of the force, as a force may be conservative in one region but not in another. It is also important to be careful with the calculations and make sure to properly apply the fundamental theorem of calculus.

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