Undergrad Derivative operators in Galilean transformations

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The discussion centers on the transformation of derivatives under Galilean transformations, specifically addressing a perceived contradiction in the equations presented. The confusion arises from misinterpreting the relationship between time and space coordinates during the transformation, particularly the distinction between total and partial derivatives. It is clarified that the Galilean transformation treats time and space as independent variables, leading to specific derivative relationships that must be adhered to. The algebraic manipulation leading to incorrect conclusions stems from treating certain variables as constants when they should not be. Understanding these nuances is crucial for correctly applying the transformation equations in non-relativistic contexts.
TomServo
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I'm confused about how the derivative with respect to time transforms under a Galilean transformation.
I'm studying how derivatives and partial derivatives transform under a Galilean transformation.

On this page:

http://www.physics.princeton.edu/~mcdonald/examples/wave_velocity.pdf

Equation (16) relies on ##\frac{\partial t'}{\partial x}=0## but ##\frac{\partial x'}{\partial t}=-v##

But this seems like a contradiction to me. If you swap primed/unprimed you get ##\frac{\partial t}{\partial x'}=0## but ##\frac{\partial x}{\partial t'}=v##, in which case you have ##x=vt+x_0## and ##t=t'=\frac{x-x_0}{v}##. Thus ##\frac{dt'}{dx}=\frac{\partial t'}{\partial x}=\frac{1}{v}##, in violation of Eq. (16).

So where have I gone wrong? Thanks.
 
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##t## is not given by ##(x-x_0)/v##, that can be true only for a very particular world-line and that is not what you are considering, you are considering the transformation of coordinates. ##\partial x/\partial t’ = v## is a partial differential, not a total differential.
 
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The Galilei transformation reads
$$t'=t, \quad \vec{x}'=\vec{x}-\vec{v} t.$$
You consider ##t## and ##\vec{x}## as independent variables when it comes to (non-relativistic) field equations. Thus you have
$$\frac{\partial t'}{\partial t}=1, \quad \vec{\nabla} t'=0, \quad \partial_t \vec{x}'=-\vec{v}, \quad \vec{\nabla} \otimes \vec{x}=\hat{1}.$$
 
Orodruin said:
##t## is not given by ##(x-x_0)/v##, that can be true only for a very particular world-line and that is not what you are considering, you are considering the transformation of coordinates. ##\partial x/\partial t’ = v## is a partial differential, not a total differential.
Could you further explain what you mean here? I know what worldlines are, but it seems to me (just algebraically) that the ##t=\frac{x-x’}{v}## relation holds in general. After all, I’m just solving the transformation equation for t. I know this is wrong, but I’m trying to understand why the algebra leads me astray (or seems to).
 
And where I wrote ##x_0## originally I meant ##x’##.
 
Then you are treating x’ as a constant when differentiating with respect to x. That is incorrect. What is being kept constant when you take the partial with respect to x is t, not x’.
 
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