And now jesss, you don't understand English 🤔🙃🤣

What's the goal here ? You know, I know, everybody here knows, that will
lead nowhere, there is nothing to win here other than losing precious
seconds of your life to a stupid person.

Le mer. 29 janv. 2025, 20:54, Alan Grayson <[email protected]> a
écrit :

>
> On Wednesday, January 29, 2025 at 11:06:18 AM UTC-7 Jesse Mazer wrote:
>
> On Wed, Jan 29, 2025 at 12:37 PM Alan Grayson <[email protected]> wrote:
>
> On Wednesday, January 29, 2025 at 9:23:31 AM UTC-7 Jesse Mazer wrote:
>
> On Wed, Jan 29, 2025 at 3:30 AM Alan Grayson <[email protected]> wrote:
>
> On Wednesday, January 29, 2025 at 12:24:33 AM UTC-7 Jesse Mazer wrote:
>
> On Wed, Jan 29, 2025 at 1:24 AM Alan Grayson <[email protected]> wrote:
>
> On Tuesday, January 28, 2025 at 9:01:14 PM UTC-7 Jesse Mazer wrote:
>
> On Tue, Jan 28, 2025 at 8:54 PM Alan Grayson <[email protected]> wrote:
>
> On Tuesday, January 28, 2025 at 2:56:32 PM UTC-7 Brent Meeker wrote:
>
> On 1/28/2025 6:49 AM, Alan Grayson wrote:
>
> I figured you'd jump on my word "separation". You have no idea what I
> mean? Of course, events with different coordinates are separated in a
> physical sense. Otherwise they'd have the SAME coordinates! But separated
> wrt spacetime events means no causal connections; whereas timelike events
> DO have causal connections. Of course, you know this, so please stop
> splitting hairs to make an argument. As for relative velocity, if you don't
> know what I mean, then you don't know what the v means in the gamma
> function. Again, stop splitting hairs. Oh, about GPS, I will look up this
> issue, but I was informed of it from a Ph'D in physics from Brent's Ph'D
> alma mater, University of Texas at Austin. It's surely NOT a distraction if
> it establishes that results in SR are physically real, not just
> appearances. AG
>
>
> There's an unfortunate but common confusion.  The un-intuitive aspects of
> special relativity are physically real, but not it the sense that they happen
> to the moving object.  If SR predicts length contraction, is the object is
> really shorter?  (1) It's really shorter in the reference frame where it's
> moving.  (2) It's not shorter in it's own frame.  And (3) it's a different
> degree of shorter in other reference frames where it is moving with
> different velocities.  Just looking at (2) people assume that it means (1)
> and (3) are just appearances.  What's true is that
>
> *the contraction, relative to things in some reference frame, with respect
> to which it's moving, is real. *Brent
>
>
> *It's a baffling result. The LT doesn't tell us what will be MEASURED in a
> moving target frame being observed from a rest frame wrt length contraction
> and time dilation, so the result is just an APPEARANCE from the pov of the
> rest frame; and yet, from the pov of GPS clocks, these effects are real and
> measureable. This was the conclusion I argued, which is why I referenced
> the GPS clocks. *
>
>
> Brent's comment wasn't saying there was any disagreement between what
> coordinates the LT predicts for a given frame and what is really true (or
> really measured) in that frame, just like I wasn't saying that (see my last
> response above). You're really deluding yourself by rushing to read every
> explanation people give you as confirmation of your pre-existing fixed
> opinions.
>
> Jesse
>
>
> IMO you're deluding yourself in one important respect; your insistence
> that the results of the LT from the pov of some rest frame predicting
> length contraction in a frame moving wrt to it, can be measured in that
> moving frame;
>
>
> This statement is hard to follow because you ignore the distinction I made
> between frames and objects--
>
>
> *I can't help you if you refuse to use your imagination. A rod or any
> object moving wrt a fixed source frame using the LT, or an object in moving
> frame at rest in that frame when the LT is applied from a fixed source
> frame, will be predicted as contracted. Period. AG*
>
>
> Your idiosyncratic way of talking is very hard to follow,
>
>
> *One frame moving and another at rest is very very very hard to
> understand? AG*
>
>
> I don't really understand the phrase "an object in moving frame at rest in
> that frame when the LT is applied from a fixed source frame".
>
>
> *Again, very very very hard to understand? AG*
>
>
> Can you please just use my terminology of v_rs representing the velocity
> of the rod in the source frame's coordinates, and v_rt representing the
> velocity of the rod in the target frame's coordinates? What I'm asking
> about is a scenario where v_rs is nonzero in the source frame's
> coordinates, then we use the LT to predict the coordinates of the
> worldlines of the front and back of the rod as defined in the target frame,
> and get the result that in the target frame the rod has v_rt = 0 so it's at
> rest in the target frame (i.e. both front and back have position
> coordinates which don't change with time in the target frame). If we then
> calculate the predicted length of the rod as defined in the target frame
> (where 'length' just means subtracting the position coordinate of the back
> of the rod from the position coordinate of the front), are you saying it
> will be predicted to be CONTRACTED compared to the length as defined by the
> original coordinates of the source frame?
>
>
>
>
> if we have some object whose length we want to talk about, and we know the
> coordinates of the worldlines of the front and back of the object in the
> first (source) frame and then use the LT to predict its coordinates (giving
> us its length) in the second (target) frame, you can't make any general
> statement about whether the LT will be "predicting length contraction" of
> the object until you know the velocity of the object itself in each frame.
> If the object has a higher velocity v_rt in the target frame than its
> velocity v_rs in the source frame, the LT will predict the object will be
> contracted in the target frame; on the other hand, if the object has a
> lower velocity v_rt in the target frame (including the case I analyzed
> where v_rt = 0) than its velocity v_rs in the source frame, the LT will
> predict the object is EXPANDED in the target frame, not contracted,
> compared to its length in the source frame. In the past you disagreed with
> this, do you still disagree or have you changed your mind?
>
> Please give a clear answer on this, telling me whether you now AGREE or
> DISAGREE that when the rod has v_rt in the target frame lower than its v_rs
> in the source frame, the LT predicts the rod's length in the target frame
> is expanded, not contracted. And if you disagree, please address the
> questions I asked in my last reply to you (the one before my reply to your
> comment on Brent's post).
>
>
> *The target frame is moving wrt the source frame. Objects in the target
> frame are at rest within that frame,*
>
>
> More verbal confusion here,
>
>
> *If you claim you don't understand my statement, you're either lying or I
> can't help you to understand what I consideer to be a simpe statement. A*G
>
>
> No, in this case I didn't say I had any trouble understanding your
> statement,
>
>
> *Then re-write it consistent with your preferred "standard terminology"
> style. AG *
>
> what I was concerned with was that your terminology here might be leading
> YOU to misinterpret MY previous statement "its length in the source frame",
> since you were using "within that frame" to mean at rest in a frame but I
> was using "in" a frame just to mean "expressed using the coordinates of
> that frame" without presupposing the object is at rest in that frame. So, I
> asked you to tell me what terminology you would prefer for my own statement
> to avoid any potential for confusion between these two meanings of
> within/in.
>
> As for the other statements of yours that I did have trouble understanding
> because it was unclear whether you were using "moving" and "rest" in the
> standard way or your own non-standard way (and why you seemed to suggest
> the question of whether one frame is 'moving' would have any bearing on the
> answer to my physics question, when I had thought that even in your own
> terminology the choice to label one frame as 'at rest' and the other
> 'moving' was purely intended to be a linguistic convention with no physical
> significance), if you don't know how to translate them into statements
> about coordinate velocity/coordinate length as I asked, then that implies
> they are "not even wrong" as statements about SR, since as I said all SR
> statements about velocity/length are understood to be purely shorthand for
> such coordinate statements. (Do you disagree that this is how physicists
> understand such statements?)
>
>
> *This is getting tedious, very tedious. You don't seem to understand
> simple English. In another very recent post of mine which you ignore, I
> clearly established your error in interpreting what the LT implies when it
> is applied in fixed frame, calculating what it predicts for measuring
> lengths in a moving frame. AG*
>
>
> Jesse
>
>
>
> when I said "its length in the source frame" I just meant the coordinate
> length assigned by the source frame, whereas your last comment "Objects in
> the target frame are at rest within that frame" seems to say you are using
> "within that frame" to specifically mean a velocity of zero using the
> frame's coordinates. If you don't like my wording, just tell me what
> wording YOU would prefer for talking about the coordinates assigned to an
> arbitrary object by a given frame, regardless of whether it has a velocity
> of zero relative to that frame or not. For example if the source frame uses
> unprimed coordinates x and t, and the position as a function of time for
> the back of the rod as defined in the source frame is x = 0.8c*t while the
> position as a function of time for the front of the rod is x = 7.2 +
> 0.8c*t, then at any given value of t in the source frame the coordinate
> distance between the x-coordinate of the front and the x-coordinate of the
> back will be 7.2, so that is what I meant by "its length in the source
> frame" even though the rod is not "at rest within that frame" according to
> your terminology. (I would also say in this case the rod's velocity in the
> source frame is 0.8c) Is it OK with you if I continue to say things like
> "its length in the source frame" or "its velocity in the source frame" to
> refer to coordinate judgments like this, and if not what wording would you
> prefer?
>
>
>
> * and contracted according to relativity. One can also consider a moving
> rod as the frame AND the object under consideration.  This is how to model
> and analyze a shortened trip to Andromeda. If you have a better way to
> model it, I am all ears. AG*
>
>
> You didn't answer my straightforward question: "Please give a clear answer
> on this, telling me whether you now AGREE or DISAGREE that when the rod has
> v_rt in the target frame lower than its v_rs in the source frame, the LT
> predicts the rod's length in the target frame is expanded, not contracted".
> Keep in mind that a lower v_rt in the target frame could include the case
> we were discussing where the rod is at rest as measured in the coordinates
> of the target frame (v_rt = 0)--do you AGREE or DISAGREE that in this case
> the LT predicts the rod's length in the target frame is expanded, not
> contracted?
>
> In your followup reply you said "The source frame is always fixed if the
> LT is applied, so offhand I can't say I agree or disagree in this case. If
> the rod is moving, it is contracted from the pov of the source frame. If
> you want the source frame to be moving, then the only way to apply the LT
> is to consider relative motion, with one frame at rest. Offhand I can't say
> I agree or disagree, except to say that from the pov of whatever frame is
> fixed, to new target is contracted. AG"
>
> Here your confusing terminology, where you sometime use "moving" and "at
> rest" in a standard way (relative to a specified frame) and sometimes in a
> non-standard way (where you arbitrarily designate one frame as "at rest"
> and the other as "moving" thoughout the whole problem), again makes it hard
> for me to follow what point you are trying to make here. What does it even
> mean to say "if you want the source frame to be moving"? I thought in
> Alan-speak the designation of one frame as "moving" and the other as "at
> rest" in your terminology was supposed to be an arbitrary linguistic label,
> one which therefore should have no effect on the answer to any physical
> question like whether the rod is contracted in the coordinates of either
> frame?
>
> Again, the standard terminology is just to use explicitly relative phrases
> like "the rod is moving relative to the Earth" or "the rod is moving in the
> Earth's frame", both of which just mean that the position coordinates
> assigned to the rod by the Earth frame are different at different values of
> the time coordinate (as in the example above where the back of the rod has
> coordinates x=0.8c*t, so for example at t=10 it would have x=8, then at
> t=20 it would have x=16 etc). Likewise saying "the rod is at rest in the
> rod frame" just means the position coordinates of the front and back of the
> rod are unchanging in the rod frame, they don't change at different values
> of the time coordinate. Modern physicists don't use non-relative phrasing
> like "frame A is moving", and it's not just a terminological matter because
> in cases like the above where you talk this way I genuinely can't parse how
> your statement would translate into a statement about the coordinates
> assigned by different frames, which is all that the LT is ultimately
> dealing with. Likewise "length" in each frame is ultimately just a
> coordinate matter, defined purely in terms of the coordinate distance
> between the ends of the object at any single value of coordinate time.
>
> If you think SR involves any concept of "velocity", "rest", "length" in a
> given frame that is *not* just a shorthand for talking about coordinates
> assigned to objects by that frame (with all coordinates based on local
> measurements by a system of rulers and clocks at rest in that frame), then
> you are confused. If you agree it's all ultimately about coordinates, you
> need to find a way of talking that doesn't lead to so much confusion about
> how your statements could be translated into coordinate terms, like my
> request to speak in terms of v_rs and v_rt.
>
>
>
>
>
> So we're both correct from different points of view, but you were mistaken
> to ignore my comments about GPS. Also, to be candid, I don't appreciate
> your comment that I am rushing to accept an opinion that confirms my
> pre-existing fixed opinions. You like to focus on coordinates, but the fact
> is you were mistaken in claiming the LT makes a measurable prediction of
> what a source frame predicts. It does in the GPS case, but not in the case
> of what a target frame predicts internally. AG
>
>
> You never addressed my response to you about the GPS in my post at
> https://groups.google.com/g/everything-list/c/ykkIYDAL3mTg/m/ximYgKzKDAAJ
> <https://groups.google.com/g/everything-list/c/ykkIYDL3mTg/m/ximYgKzKDAAJ>
> -- any coordinate system covering a non-infinitesimal region of curved
> spacetime is non-inertial, and the LT isn't relevant to non-inertial
> coordinate systems.
>
>
> *An object in free fall is in inertial motion, called a geodesic in GR.
> The LT is probably applicable for infinitesmal motion notwithstanding that
> this is occurring in curved spacetime. But I'm NOT an expert on how or why
> SR is used in GPS to make clock corrections. What I do know is that it IS
> used, that consequently the LT is likely applied in some way, and I gave
> this example just to show that whereas the LT does NOT give predictions
> concerning what is predicted for objects moving wrt a fixed frame, one
> cannot categorically claim that it never does.*
>
>
> If we're talking about a scenario where a GPS type system was used in flat
> spacetime, the LT would certainly "give predictions concerning what is
> predicted for objects moving wrt a fixed frame", as I said in the last
> sentence below you'd just have to include the way the clocks are
> artificially slowed down (relative to standard clocks) in the source frame
> before doing things like calculating elapsed time on a clock for some
> interval of coordinate time in the source frame, or applying the LT to
> predict the clocks' behavior in the target frame.
>
> Jesse
>
>
>
>
>
> But looking into this a little more, it seems based on p. 2-3 of
> http://math.bme.hu/~matolcsi/gpsmegjelentejp.pdf that at some point in
> the GPS calculations they do use an approximation that treats the spacetime
> around the Earth as flat so an inertial coordinate system can be used, and
> then they add higher-order corrections to account for the fact that the
> spacetime is actually curved and this is relevant to gravitational time
> dilation.
>
> But even if there were no gravity and we were just trying to define a
> GPS-like system to adjust clocks with various states of motion so they were
> all synchronized in a single inertial frame (as in the 'Suppose for a
> moment there were no gravitational fields' comment in the second to last
> paragraph in 'the realization of coordinate time' section of the GPS paper
> at https://pmc.ncbi.nlm.nih.gov/articles/PMC5253894/#Sec4 ), say the
> frame where the center of the Earth is at rest, I still don't understand
> why you think this would indicate any conflict between what the LT predicts
> and what is measured--the whole point of a GPS system is that the ticking
> rate of the clocks is being artificially adjusted so it no longer matches
> the "proper time" of an un-adjusted clock following the same trajectory,
> but instead matches the coordinate time in some preferred coordinate system
> you've programmed the clocks to keep pace with. If you have a system of
> adjustments like this for clocks in flat spacetime where inertial frames
> can be used, then if you know the adjusted ticking rate of a clock in some
> source frame (along with the coordinates of its worldline in this frame),
> you can use the LT to correctly predict the adjusted ticking rate of that
> same clock in a different target frame.
>
> Jesse
>
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