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Why isn't scaling space and time considered the 11th dimension of the Galilean group?


Can one derive Galilean transformations from the harmonic oscillator equations of motion and the relativity principle?Relationship bewtween the principle of Galilean Relativity and absolute timeWhy does galilean invariance imply that particles that start rest stay on the same line?Noether's Theorem and scale invarianceUnderstanding the physical operations corresponding to unit conversion and scale transformation of timeDoes the Newton's law break scale invariance?The Meaning of Newton's Second Law of Motion Being Invariant Under Certain TransformationsSilly question about Galilei GroupRelationship between the Galilei Group and the Phase Space













7












$begingroup$


Galilean transformations are said to have 10 degrees of freedom. Four for translation in space and time, three for rotation, and three for direction of the uniform motion.



If I scale space axis by $alpha$ and do the same with time axis, you can see that Newton's second law remains the same.



So why don't we consider scaling (of time and space) another type of Galilean transformation?










share|cite|improve this question











$endgroup$











  • $begingroup$
    I agree that "scale" is a badly neglected degree of physical freedom.
    $endgroup$
    – Steve
    Jun 1 at 23:50










  • $begingroup$
    @Steve, it is not a degree of freedom in classical mechanics.
    $endgroup$
    – Akerai
    Jun 2 at 0:18










  • $begingroup$
    @Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
    $endgroup$
    – Steve
    Jun 2 at 0:38






  • 1




    $begingroup$
    @Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
    $endgroup$
    – Thatpotatoisaspy
    Jun 2 at 3:10











  • $begingroup$
    Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
    $endgroup$
    – AccidentalFourierTransform
    Jun 2 at 14:13















7












$begingroup$


Galilean transformations are said to have 10 degrees of freedom. Four for translation in space and time, three for rotation, and three for direction of the uniform motion.



If I scale space axis by $alpha$ and do the same with time axis, you can see that Newton's second law remains the same.



So why don't we consider scaling (of time and space) another type of Galilean transformation?










share|cite|improve this question











$endgroup$











  • $begingroup$
    I agree that "scale" is a badly neglected degree of physical freedom.
    $endgroup$
    – Steve
    Jun 1 at 23:50










  • $begingroup$
    @Steve, it is not a degree of freedom in classical mechanics.
    $endgroup$
    – Akerai
    Jun 2 at 0:18










  • $begingroup$
    @Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
    $endgroup$
    – Steve
    Jun 2 at 0:38






  • 1




    $begingroup$
    @Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
    $endgroup$
    – Thatpotatoisaspy
    Jun 2 at 3:10











  • $begingroup$
    Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
    $endgroup$
    – AccidentalFourierTransform
    Jun 2 at 14:13













7












7








7





$begingroup$


Galilean transformations are said to have 10 degrees of freedom. Four for translation in space and time, three for rotation, and three for direction of the uniform motion.



If I scale space axis by $alpha$ and do the same with time axis, you can see that Newton's second law remains the same.



So why don't we consider scaling (of time and space) another type of Galilean transformation?










share|cite|improve this question











$endgroup$




Galilean transformations are said to have 10 degrees of freedom. Four for translation in space and time, three for rotation, and three for direction of the uniform motion.



If I scale space axis by $alpha$ and do the same with time axis, you can see that Newton's second law remains the same.



So why don't we consider scaling (of time and space) another type of Galilean transformation?







galilean-relativity scale-invariance






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Jun 2 at 5:09









Qmechanic

110k122101289




110k122101289










asked Jun 1 at 23:22









Shuheng ZhengShuheng Zheng

206210




206210











  • $begingroup$
    I agree that "scale" is a badly neglected degree of physical freedom.
    $endgroup$
    – Steve
    Jun 1 at 23:50










  • $begingroup$
    @Steve, it is not a degree of freedom in classical mechanics.
    $endgroup$
    – Akerai
    Jun 2 at 0:18










  • $begingroup$
    @Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
    $endgroup$
    – Steve
    Jun 2 at 0:38






  • 1




    $begingroup$
    @Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
    $endgroup$
    – Thatpotatoisaspy
    Jun 2 at 3:10











  • $begingroup$
    Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
    $endgroup$
    – AccidentalFourierTransform
    Jun 2 at 14:13
















  • $begingroup$
    I agree that "scale" is a badly neglected degree of physical freedom.
    $endgroup$
    – Steve
    Jun 1 at 23:50










  • $begingroup$
    @Steve, it is not a degree of freedom in classical mechanics.
    $endgroup$
    – Akerai
    Jun 2 at 0:18










  • $begingroup$
    @Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
    $endgroup$
    – Steve
    Jun 2 at 0:38






  • 1




    $begingroup$
    @Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
    $endgroup$
    – Thatpotatoisaspy
    Jun 2 at 3:10











  • $begingroup$
    Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
    $endgroup$
    – AccidentalFourierTransform
    Jun 2 at 14:13















$begingroup$
I agree that "scale" is a badly neglected degree of physical freedom.
$endgroup$
– Steve
Jun 1 at 23:50




$begingroup$
I agree that "scale" is a badly neglected degree of physical freedom.
$endgroup$
– Steve
Jun 1 at 23:50












$begingroup$
@Steve, it is not a degree of freedom in classical mechanics.
$endgroup$
– Akerai
Jun 2 at 0:18




$begingroup$
@Steve, it is not a degree of freedom in classical mechanics.
$endgroup$
– Akerai
Jun 2 at 0:18












$begingroup$
@Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
$endgroup$
– Steve
Jun 2 at 0:38




$begingroup$
@Akerai, why exactly is that? Is it simply because no apparent practical means of changing the scale of physical things currently exists (and thus the theoretical possibility didn't need to be considered by the classical physicists)?
$endgroup$
– Steve
Jun 2 at 0:38




1




1




$begingroup$
@Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
$endgroup$
– Thatpotatoisaspy
Jun 2 at 3:10





$begingroup$
@Steve It’s because, as Akerai states in an answer here, the laws of classical mechanic are in fact generally not scale-invariant as OP claims.
$endgroup$
– Thatpotatoisaspy
Jun 2 at 3:10













$begingroup$
Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
$endgroup$
– AccidentalFourierTransform
Jun 2 at 14:13




$begingroup$
Interestingly enough, the Schrödinger equation is both invariant under galilean transformations and dilations, even if it has a length scale (mass). It is even conformally invariant! cf. mathoverflow.net/a/270122/106114
$endgroup$
– AccidentalFourierTransform
Jun 2 at 14:13










1 Answer
1






active

oldest

votes


















9












$begingroup$

Imagine you take the transformation you mentioned above:
$$x^i rightarrow x'^i = alpha x^i,\
t rightarrow t' = alpha t,$$

where $alpha in mathbbR$.



Then assuming the Newton's law holds in the new coordinates, it will be of the form
$$F^i = m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2 left(fracdtdt' right)^2.$$



As you can see, the derivative $dt/dt' = 1/ alpha$, and therefore the equality becomes



$$m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2frac1alpha^2 = fracmalpha fracd^2 (x^i) dt^2.$$



Therefore the Newton's law is actually not invariant under this transformation as you claimed before, the transformation actually transforms an object of mass $m/alpha$ to an object of mass $m$.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:40






  • 3




    $begingroup$
    This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:41











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1 Answer
1






active

oldest

votes








1 Answer
1






active

oldest

votes









active

oldest

votes






active

oldest

votes









9












$begingroup$

Imagine you take the transformation you mentioned above:
$$x^i rightarrow x'^i = alpha x^i,\
t rightarrow t' = alpha t,$$

where $alpha in mathbbR$.



Then assuming the Newton's law holds in the new coordinates, it will be of the form
$$F^i = m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2 left(fracdtdt' right)^2.$$



As you can see, the derivative $dt/dt' = 1/ alpha$, and therefore the equality becomes



$$m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2frac1alpha^2 = fracmalpha fracd^2 (x^i) dt^2.$$



Therefore the Newton's law is actually not invariant under this transformation as you claimed before, the transformation actually transforms an object of mass $m/alpha$ to an object of mass $m$.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:40






  • 3




    $begingroup$
    This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:41















9












$begingroup$

Imagine you take the transformation you mentioned above:
$$x^i rightarrow x'^i = alpha x^i,\
t rightarrow t' = alpha t,$$

where $alpha in mathbbR$.



Then assuming the Newton's law holds in the new coordinates, it will be of the form
$$F^i = m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2 left(fracdtdt' right)^2.$$



As you can see, the derivative $dt/dt' = 1/ alpha$, and therefore the equality becomes



$$m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2frac1alpha^2 = fracmalpha fracd^2 (x^i) dt^2.$$



Therefore the Newton's law is actually not invariant under this transformation as you claimed before, the transformation actually transforms an object of mass $m/alpha$ to an object of mass $m$.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:40






  • 3




    $begingroup$
    This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:41













9












9








9





$begingroup$

Imagine you take the transformation you mentioned above:
$$x^i rightarrow x'^i = alpha x^i,\
t rightarrow t' = alpha t,$$

where $alpha in mathbbR$.



Then assuming the Newton's law holds in the new coordinates, it will be of the form
$$F^i = m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2 left(fracdtdt' right)^2.$$



As you can see, the derivative $dt/dt' = 1/ alpha$, and therefore the equality becomes



$$m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2frac1alpha^2 = fracmalpha fracd^2 (x^i) dt^2.$$



Therefore the Newton's law is actually not invariant under this transformation as you claimed before, the transformation actually transforms an object of mass $m/alpha$ to an object of mass $m$.






share|cite|improve this answer











$endgroup$



Imagine you take the transformation you mentioned above:
$$x^i rightarrow x'^i = alpha x^i,\
t rightarrow t' = alpha t,$$

where $alpha in mathbbR$.



Then assuming the Newton's law holds in the new coordinates, it will be of the form
$$F^i = m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2 left(fracdtdt' right)^2.$$



As you can see, the derivative $dt/dt' = 1/ alpha$, and therefore the equality becomes



$$m fracd^2x'^idt' ^2 = m fracd^2 (alpha x^i) dt^2frac1alpha^2 = fracmalpha fracd^2 (x^i) dt^2.$$



Therefore the Newton's law is actually not invariant under this transformation as you claimed before, the transformation actually transforms an object of mass $m/alpha$ to an object of mass $m$.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Jun 1 at 23:48

























answered Jun 1 at 23:34









AkeraiAkerai

338110




338110











  • $begingroup$
    Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:40






  • 3




    $begingroup$
    This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:41
















  • $begingroup$
    Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:40






  • 3




    $begingroup$
    This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
    $endgroup$
    – Shuheng Zheng
    Jun 2 at 3:41















$begingroup$
Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
$endgroup$
– Shuheng Zheng
Jun 2 at 3:40




$begingroup$
Thanks, I made a mistake in my calculation. Thank you so much for clearing up.
$endgroup$
– Shuheng Zheng
Jun 2 at 3:40




3




3




$begingroup$
This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
$endgroup$
– Shuheng Zheng
Jun 2 at 3:41




$begingroup$
This make sense. If it is truly scale invariant, we probably won't need units on acceleration forces etc.
$endgroup$
– Shuheng Zheng
Jun 2 at 3:41

















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