Derivative of lagrangian density

Click For Summary
The discussion centers on the correct approach to finding the derivative of the Lagrangian density in the context of Klein-Gordon theory. The main point of contention is whether the derivatives \(\partial^{\mu} \phi\) and \(\partial_{\mu} \phi\) are treated as independent variables. It is clarified that while they are not independent, they are related through the metric, leading to the conclusion that the correct derivative is \(\frac{\partial L}{\partial(\partial^{\mu}\phi)} = \partial_{\mu} \phi\). The analogy of partial derivatives involving dependent variables is debated, emphasizing the importance of understanding the relationship dictated by the metric. This highlights the nuances of handling derivatives in field theory.
kawillzocken
Messages
2
Reaction score
0
i have a mathematical question which is quite similar to one asked before, still a bit different
https://www.physicsforums.com/threa...agrangian-density-for-real-k-g-theory.781472/the first term of KG-Lagrangian is: \frac{1}{2}(\partial^{\mu} \phi)(\partial_{\mu} \phi)
when i try do find \frac{\partial L}{\partial(\partial^{\mu}\phi)}, i have two different options, where of course only one can be right.

1) \partial^{\mu} \phi and \partial_{\mu} \phi are different things, so one gets: \frac{\partial L}{\partial(\partial^{\mu}\phi)} = \frac{1}{2}\partial_{\mu} \phi

2) \partial_{\mu} \phi = \eta_{\mu \nu} \partial^{\nu} \phi \rightarrow \frac{\partial L}{\partial(\partial^{\mu}\phi)} = \frac{\partial}{\partial(\partial^{\mu}\phi)}(\frac{1}{2}\eta_{\mu \nu}(\partial^{\nu} \phi)(\partial^{\mu} \phi)) = \partial_{\mu} \phi

i am confused. several sources tell me that 2) is right, but my understanding of partial derivative tells me to do 1).

as i think of it, one may not simply put equations into others when doing the partial derivative, because it then changes. like z(x, y(x)) = 2x + y(x). partial derivative with respect to x gives 2, but it changes when i put in y(x).

help please :)
thank you
 
Physics news on Phys.org
Option 2 is correct. The quantities ##\partial_\mu\phi## and ##\partial^\mu\phi## may not be equal, but they do not correspond to different degrees of freedom (they are related by a sign). Compare this to differentiating ##-x## with respect to ##x##, ##-x## is not equal to ##x##, but it is directly dependent.
 
kawillzocken said:
i have a mathematical question which is quite similar to one asked before, still a bit different
https://www.physicsforums.com/threa...agrangian-density-for-real-k-g-theory.781472/the first term of KG-Lagrangian is: \frac{1}{2}(\partial^{\mu} \phi)(\partial_{\mu} \phi)
when i try do find \frac{\partial L}{\partial(\partial^{\mu}\phi)}, i have two different options, where of course only one can be right.

1) \partial^{\mu} \phi and \partial_{\mu} \phi are different things, so one gets: \frac{\partial L}{\partial(\partial^{\mu}\phi)} = \frac{1}{2}\partial_{\mu} \phi

No, they are definitely not independent. If you write it with the metric, then this becomes more obvious:

\mathcal{L} = \frac{1}{2}g^{\mu \nu} (\partial_{\mu} \phi\ \partial_{\nu} \phi)

So \frac{\partial \mathcal{L}}{\partial (\partial^{\sigma} \phi)} = \frac{1}{2}g^{\mu \nu} (\delta^\sigma_\mu \partial_{\nu} \phi + \delta^\sigma_\nu \partial_{\mu} \phi) = \frac{1}{2} (g^{\sigma \nu} \partial_{\nu} \phi + g^{\mu \sigma} \partial_{\mu} \phi) = \frac{1}{2} (\partial^{\sigma} \phi + \partial^{\sigma} \phi) = \partial^{\sigma} \phi
 
i do not say they are independent. y(x) and x are not indepentent either, still in a partial derivative of z with respect to x, one does not consider the y(x).

so orodruin, i see that they are related by the metric. y(x) is also related to x by its defining function. so i do still not get the point, where my z-function analogy is failing.
do y and x correspond to different degrees of freedom in z?

regards, kawillzocken
 
kawillzocken said:
i do not say they are independent. y(x) and x are not indepentent either, still in a partial derivative of z with respect to x, one does not consider the y(x).

so orodruin, i see that they are related by the metric. y(x) is also related to x by its defining function. so i do still not get the point, where my z-function analogy is failing.
do y and x correspond to different degrees of freedom in z?

regards, kawillzocken

Let's make it a lot simpler, by considering only 1 space dimension and 1 time dimension. Then the lagrangian is:

\mathcal{L} = \frac{1}{2}(\frac{\partial \phi}{\partial t} \frac{\partial \phi}{\partial t} - \frac{\partial \phi}{\partial x} \frac{\partial \phi}{\partial x})

I think it's pretty obviousthat \frac{\partial \mathcal{L}}{\partial (\frac{\partial \phi}{\partial t})} = \frac{\partial \phi}{\partial t}. Right?
 
kawillzocken said:
i do not say they are independent. y(x) and x are not indepentent either, still in a partial derivative of z with respect to x, one does not consider the y(x).

so orodruin, i see that they are related by the metric. y(x) is also related to x by its defining function. so i do still not get the point, where my z-function analogy is failing.
do y and x correspond to different degrees of freedom in z?

regards, kawillzocken

In a second-order differential equation for \phi (which is what the lagrangian equations of motion produce), to know \phi everywhere, it is good enough to specify \phi, \frac{\partial \phi}{\partial x}, \frac{\partial \phi}{\partial y}, \frac{\partial \phi}{\partial z}, \frac{\partial \phi}{\partial t} at a single point (x_0, y_0, z_0, t_0). Those are 5 completely independent choices.
 
I do not have a good working knowledge of physics yet. I tried to piece this together but after researching this, I couldn’t figure out the correct laws of physics to combine to develop a formula to answer this question. Ex. 1 - A moving object impacts a static object at a constant velocity. Ex. 2 - A moving object impacts a static object at the same velocity but is accelerating at the moment of impact. Assuming the mass of the objects is the same and the velocity at the moment of impact...

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 0 ·
Replies
0
Views
1K
  • · Replies 1 ·
Replies
1
Views
542
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
Replies
7
Views
1K
  • · Replies 4 ·
Replies
4
Views
1K