On 10/25/2024 2:44 AM, Alan Grayson wrote:


On Friday, October 25, 2024 at 2:44:06 AM UTC-6 Brent Meeker wrote:




    On 10/25/2024 1:36 AM, Alan Grayson wrote:


    On Thursday, October 24, 2024 at 11:07:18 PM UTC-6 Brent Meeker
    wrote:




        On 10/24/2024 5:46 PM, Alan Grayson wrote:


        On Thursday, October 24, 2024 at 1:30:32 PM UTC-6 Brent
        Meeker wrote:

            Here's  how a light-clock ticks in when in motion.  A
            light-clock is just two perfect mirrors a fixed distance
            apart with a photon bouncing back an forth between
            them.  It's a hypothetical ideal clock for which the
            effect of motion is easily visualized.



            These are the spacetime diagrams of three identical
            light-clocks moving at _+_c relative to the blue one.


        *Three clocks?  Black diagram? If only this was as clear as
        you claim. TY, AG*

        *You can't handle more than two?  The left clock is black
        with a red photon.  Is that hard to comprehend?  Didn't they
        teach spacetime diagrams at your kindergarten?

        Brent
        *


    *What makes you think you can teach? *
    *That I have taught and my students came back for more.*

    *I can handle dozens of clocks. I know what a spacetime diagram.
    It was taught in pre-school. Why did you introduce a red photon?
    A joke perhaps? How can a clock move at light speed? *
    *None of the clocks in the diagram are moving at light speed.  The
    black one and the red one are moving at 0.5c as the label says. 
    What is it you don't understand about this diagram?

    Brent
    *


*One thing among several that I don't understand is how the LT is applied. *
The set of points (t,x) representing a stationary light clock, two vertical lines with 45deg "photon" lines bouncing between them, is generated.  This is the blue one.  Then a Lorentz transform is applied to the that set of points.  Here's the LISP code I used:

*(defun gammma (v) (/ (sqrt (- 1.0 (* v v)))))

(defun lorentz-2d (v)
"Returns a function that takes a point (t,x) and
returns the transformed point (t',x')"
   (lambda (p)
      (let ((t0 (car p))
            (x0 (cadr p))
            (g (gammma v)))
      (list (+ (* g t0) (* g (/ x0 v))) ;this is t'
            (+ (* g x0) (* g v t0)))))) ;this is x'

(defun lorentz-trans (v points)
"Transform a set of points, e.g. a world-line"
      (translate (mapcar (lorentz-2d v) points) (car points)))*

I don't know if you read LISP but in this case it's very simple. The first line is just defining the gamma value for a given speed, in this case v=0.5.  The second function *lorentz-2d(v)* takes a speed and returns a function *lambda(p)* that takes a point and returns the point's coordinates in the frame moving at speed v.  The third function just applies that transform to every point on the given list *points*.  The *translate* function just moves the graph timewise so it lines up with a given starting point.
*For example, if we transform from one frame to another, say in E&M, IIUC we get what the fields will actually be measured by an observer in the target or primed frame. (I assume we're transferring from frame S to frame S'). But when we use it to establish time dilation say, we don't get what's actually measured in the target frame, but rather how it appears from the pov of the source or unprimed frame. *
Right.
*Presumably, that's why you say that after a LT, the internal situation in each transformed frame remains unchanged (or something to that effect). AG*
Right.  A coordinate transform shouldn't change anything local.  In this case it is just distances and times that are different than one expects from Euclidean space+time.  Everyone in their own local inertial is /ex hypothesi/ looking at an identical perfect clock.

Brent*
*
*
*

    **
    *It's a real muddle. I think you meant well, but you don't have
    the maturity to contain your temper. Nonetheless, the photon
    clock gave me a good idea, which I just wrote about. AG *

        **

            Because the speed of light is invariant the photon paths
            are at unit slope inside all three clocks, so it is
            easily seen why the relative motion makes the clock seem
            slow although each clock is ticking at the same rate in
            it's own reference frame.  The red diagram is just the
            blue diagram Lorentz transformed as it would be seen in
            a frame moving the left at 0.5c, and the black diagram
            as it would be seen from a frame moving to the right.

            Brent


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