Recent content by D.S.Beyer

  1. D.S.Beyer

    B Twin Paradox: Orbital Geodesics, Gravity, & Time Dilation

    Thanks for all the wonderful responses to this question. It sounds like, no matter if the geodesic is hyperbolic, highly elliptical, or circular, Twin A will elapse more time. One of the things that I wanted to get out of this question was if 'local acceleration' matters. Such that Twin B...
  2. D.S.Beyer

    B Twin Paradox: Orbital Geodesics, Gravity, & Time Dilation

    This is great. Thank you. How does one determine the maximal geodesic? I'm not to keen on the hard math, so if you have a geometric example, I'd love to see it.
  3. D.S.Beyer

    B Twin Paradox: Orbital Geodesics, Gravity, & Time Dilation

    I guess I was trying to get the meeting point even as far out into 'Minkowski' flat spacetime as I could, such that Twin A could basically be stationary. As PAllen says an 'asymptotically flat' spacetime. But, I guess it really doesn't change the outcome in the end.
  4. D.S.Beyer

    B Twin Paradox: Orbital Geodesics, Gravity, & Time Dilation

    ~ Shower Thoughts ~ Twin A is in a spaceship, Twin B is in a spaceship. Both in 'deep space'. B follows a highly elliptical geodesic which goes around a planet (or black hole) with strong gravity, very far away. When they meet again, who is younger and why? I genuinely don't know what this...
  5. D.S.Beyer

    I Discussing Interior Schwarzschild Proper Lengths & Gaussian Curvature

    Okay this is making more sense. I'm beginning to see some of my weird assumptions in here. I think the thing that is giving me trouble is the 're-embedment' of the lengths on the curve, back onto the ##(r,\varphi)## plane. This produces these varying ##r## values, which are not actual lengths...
  6. D.S.Beyer

    I Discussing Interior Schwarzschild Proper Lengths & Gaussian Curvature

    I'd love have a little discussion about the Interior Schwarzschild Solution. Here's a diagram I slapped together to illustrate the key points. (I assume everyone reading this familiar with embedding diagrams, and using an axis to 'project' a value, in this case the spatial z-axis is replaced by...
  7. D.S.Beyer

    B Exploring Proper Time of CMB: What Does it Mean?

    This blows my mind that this is such a difficult question, but in a good way. Why is the exchange of signals important? Can't it just be a one way thing? For example (and in wild hypothetical land), if I take a telescope in my backyard and zoom in on a clock that is strapped to the body of a...
  8. D.S.Beyer

    B Exploring Proper Time of CMB: What Does it Mean?

    Wow. I'm going to have to take a moment or two to get through this thread, but it does get to the heart of a lot of what I'm interested in.
  9. D.S.Beyer

    B Exploring Proper Time of CMB: What Does it Mean?

    Did some searches through these forums but didn't find this exact question. I'm sure it's already been asked, but I just missed it, my apologies. Please link. I’ll try and ask this question in 3 different ways, and maybe the idea behind it will become apparent. I know that semantics can really...
  10. D.S.Beyer

    B SR vs GR - Visual Difference between Length Contraction

    This is awesome! Thank you for this helpful link.
  11. D.S.Beyer

    B SR vs GR - Visual Difference between Length Contraction

    @PeterDonis "The GR phenomenon you are describing is not "length contraction"." Then, how do talk about this visual phenomena? This came up in a previous post about Christmas Lights into a black hole. From the perspective of an outside observer, the light got 'squished' together near the horizon.
  12. D.S.Beyer

    B SR vs GR - Visual Difference between Length Contraction

    The 2 Bowling Balls Ball(a) & Ball(b) (a) is in acceleration of 10m/s^2 (b) is in at fixed position in a gravitational field where g=10m/s^2 In both cases the observer is: - perpendicular to the vector of acceleration - distant enough to be in empty flat space Question : In an instantaneous...
  13. D.S.Beyer

    I Observing Christmas Lights in a Black Hole: What You See

    Awesome. I am a little shaky on the difference between length contraction in SR vs length contraction in GR. I am, most likely mistakingly, working under the assumption that the gravitational field in GR acts like the acceleration of an object in SR, to produce the length contracted effects...
  14. D.S.Beyer

    I Observing Christmas Lights in a Black Hole: What You See

    @PeterDonis thanks for bearing with me on this. I am essentially trying to setup a scenario where a visual ruler (of time ie blinking lights and space ie length) extends from a relativity low spacetime curvature (Minkowski) to a relatively high spacetime curvature (Schwarzschild black hole). I...
  15. D.S.Beyer

    I Observing Christmas Lights in a Black Hole: What You See

    I am open to suggestions. Maybe we calculate how fast Santa needs to travel to get toys to everyone?
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