Hey
@Demystifier . I didn't provide any update since I've been super busy with the programming job, but I also gave some thoughts on this matter and a couple of points struck me. You can answer whenever you're free - I already took so much time from you and I feel bad about this, but things I'm asking are not really explained anywhere as you explain it to me.
Point 1: In this huge thread, we have been discussing homogeneity and it turns out that ##y' = y + k## transformation and substituting ##y' - k## instead of ##y## confirms that we're using passive transformation method - i.e changing the frame while everything else stays the same - i.e object we're experimenting on only drops from single location - i.e one experiment, but just looking the same thing from different frames. I was wondering about one thing - does this method really provide a solid way of checking homogeneity - asking this because we're not really dropping the ball from multiple locations in space, but single point, so maybe we're not testing homogeneity well enough ? in the absolute sense, homogeneity should be tested as object being dropped from
different points in space. What would be your explanation why passive transformation still gives a solid way of checking homogeneity ?
Point 2: I also am trying to understand isotropy and I guess, let's also use passive transformation method here. The ball is dropped one time from some single location. first, we look at it in ##x,y## frame and then in the rotated frame(##x', y'##) frame. I understand that rotation can be described as :
##x' = xcos\theta + ysin\theta## (1)
##y' = -xsin\theta + ycos\theta## (2)
if we're in earth gravitational scenario, in ##x,y## frame, we have: ##\ddot y = -g##. In order to get e.o.m of the same ball in ##x', y'##, we first figure out what ##y## is from using (2).
##y = \frac{y' +xsin\theta}{cos\theta}##
##\frac{d^2}{dt^2}(\frac{y' +xsin\theta}{cos\theta}) = -g##
##\frac{1}{cos\theta}(\frac{d^2y'}{dt^2} + \frac{dx^2}{dt^2}sin\theta) = -g##
since ##\ddot x = 0##, we end up:
##\ddot y' = -gcos\theta##
and this is actually different(it gives us ##y'(t)## such as its behaviour is definitely not the same as of ##y(t)##).
I think I'm correct so far ? If yes, then could you quote this and say that I'm correct ?
okay, now let's do for ##V = k(x^2 + y^2)##
Using the transformation and plugging them in directly in ##V##, we see that in the rotated frame, potential ends up being the same, which confirms isotropy,
but what if we do it separately for x and y axis.
in ##x,y## frame, ##ma_x = -2kx => \ddot x = \frac{-2kx}{m}##, Now we can plug ##x'cosa - y'sina## instead of ##x## and we get: ##\ddot x'cosa - \ddot y'sina = \frac{-2k(x'cosa - y'sina)}{m}##. From this, solution ##x'(t)## doesn't seem to match with ##x(t)## from ##\ddot x = \frac{-2kx}{m}##. Any idea why ? or we should be making ##y'sina = 0##, because we're working in ##x## direction only and ##y'## or ##y## is not ##x## direction for sure, but is this a valid thing to do ? Problem that I see why I can't make ##y'sina## to be 0 is that ##y'sina## is included in the coordinate of ##x##, if I make it zero, then coordinate of ##x## is definitely wrong.