On Sun, Dec 15, 2024 at 4:06 PM Jesse Mazer <[email protected]> wrote:

>
>
> On Sun, Dec 15, 2024 at 3:09 PM Alan Grayson <[email protected]>
> wrote:
>
>>
>>
>> On Sunday, December 15, 2024 at 12:54:08 PM UTC-7 Quentin Anciaux wrote:
>>
>>
>>
>> Le dim. 15 déc. 2024, 20:45, Alan Grayson <[email protected]> a écrit :
>>
>>
>>
>> On Sunday, December 15, 2024 at 11:24:36 AM UTC-7 Quentin Anciaux wrote:
>>
>> Le dim. 15 déc. 2024, 18:48, Alan Grayson <[email protected]> a écrit :
>>
>> On Sunday, December 15, 2024 at 6:45:57 AM UTC-7 Quentin Anciaux wrote:
>>
>> Le dim. 15 déc. 2024, 14:31, Alan Grayson <[email protected]> a écrit :
>>
>> On Sunday, December 15, 2024 at 6:20:47 AM UTC-7 Alan Grayson wrote:
>>
>> On Sunday, December 15, 2024 at 5:41:54 AM UTC-7 John Clark wrote:
>>
>> On Sat, Dec 14, 2024 at 11:01 PM Alan Grayson <[email protected]>
>> wrote:
>>
>> * > What bothers me is the disagreement between frames about fitness or
>> not, and why the alleged lack of simultaneity resolves the apparent
>> contradiction. AG *
>>
>>
>> *In this thought experiment I think even you would agree that no matter
>> how fast or slow the car is going there will always be times when the front
>> of the car is in the garage, and times when the back of the car is in the
>> garage; so the question of the day is " Is there any frame of reference in
>> which those two events occur SIMULTANEOUSLY?" Einstein's answer is "yes",
>> provided the car is moving fast enough. And as proof that Einstein's answer
>> was correct, in this thought experiment, above a certain speed, there is NO
>> frame of reference in which there is a car shaped hole in the back door of
>> the garage.  *
>>
>> *John K Clark    See what's on my new list at  Extropolis
>> <https://groups.google.com/g/extropolis>*
>>
>>
>> No. Above a certain speed, since the car is length contracted from the
>> pov of the garage frame, the car will fit in the garage, and waiting some
>> time, then being in a different reference frame, it could hit the back
>> door. AG
>>
>>
>> But the real question is this; if from the pov of the car frame, there is
>> a v such that the car never fits in the garage for this v and greater, why
>> is it claimed that lack of simultaneity between frames solves the problem,
>> since we're only considering simultaneity in garage frame where the car
>> fits? AG
>>
>> eua
>>
>>
>> It's crazy you're still on this... wtf is your definition of fits in
>> which doesn't involve simultaneously having rear and front of the car in
>> the garage?
>>
>> Quentin
>>
>>
>> I never denied that "fitting" requires simultaneity.
>>
>>
>>
>>  Then wtf are you trolling about ?
>>
>>
>> *Earlier you asked if I agreed that fitting requires simultaneity, and I
>> affirmed that. My problem all along, which apparently went over your head,
>> is how the two frames can give diametrically opposite results. All you were
>> capable of doing was to repeat some slogan without offering any genuine
>> explanation. *
>>
>>
>> Bullshit, everyone here explained it was about ordering of events, it's
>> nit hand waving, it's just your trollest and unwilling attitude to
>> understand, or just you as cosmin wanting to troll because you enjoy it.
>>
>>
>> *Obviously, you don't understand but indulge the illusion that you do.
>> Fact is I don't fully understand the time ordering of events, such as if
>> two events are simultaneous in one frame, and not in another, will the time
>> order necessarily be reversed in that frame and all others, and if so, why?*
>>
>
> Just to answer this question, if two events A and B have a spacelike
> separation (neither event lies in the past or future light cone of the
> other one), then there will be one frame where they are simultaneous, other
> frames where A happens before B, and other frames where A happens before B.
>

Sorry, I of course meant to write "other frames where A happens before B,
and other frames where B happens before A".


>
> It may be easier to understand why this is true intuitively if you learn
> about how to draw spacetime diagrams where you have two observers #1 and #2
> in relative motion, and you draw a diagram where the vertical axis is the T
> coordinate of observer #1 and the horizontal axis is the X coordinate of
> observer #1, and then you draw the X' and T' axes of observer #2 in that
> diagram, where both axes look like slanted lines offset from the vertical
> and horizontal, as in Fig. 5 near the top of the page at
> https://en.wikibooks.org/wiki/Special_Relativity/Simultaneity,_time_dilation_and_length_contraction
> . Since the X' axis is a set of points that all have the same T' coordinate
> for observer #2, the X' axis will show you what observer #2's surface of
> simultaneity looks like from the perspective of observer #1's frame.
> Meanwhile the T' axis would be the worldline of an object at rest in
> observer #2's frame (since it the T' axis has a constant X' coordinate)
> whose worldline passed through the origin. The X' axis will always make the
> same angle with a light ray as the T' axis (compare the x' and ct' axes
> with the yellow light ray in the diagram at
> https://commons.wikimedia.org/wiki/File:Minkowski_diagram_-_3_systems.svg
> as well as the x'' and ct'' axes for a third observer with a higher
> velocity), so if you know how to draw the worldline of an object at a given
> speed v in observer #1's frame, that's enough to give you an idea of what
> the surface of simultaneity for that object (its X' axis) would look like
> when plotted in observer #1's frame, and how it would "tilt" continuously
> as you tilt the worldline/T' axis (considering objects at higher velocity)
> relative to observer #1's frame--see the little animation of this tilting
> starting at 13:09 in the video at
> https://www.youtube.com/watch?v=5bSy18w8Dh0&t=789s
>
> Jesse
>

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