| | #21 (permalink) | ||||
| Creating | Re: Some subtle aspects of relativity. Quote:
And you've never given any convincing reason that reparameterizing GR in your way does anything to help with quantum mechanics! Its not even obvious to me that there is a simple way to recast Einstein's field equations because in your reparameterization the stress energy tensor isn't a tensor but transforms non-trivially observer to observer. Also, you still haven't responded to my question- if the universe were governed by scale invariant equations, then it should be scale invariant- how come none of the fundamental forces demonstrate this feature? Why isn't the CMB background truly scale invariant instead of merely approximately scale invariant? etc. Quote:
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-Will | ||||
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| | #22 (permalink) | |||
| Understanding | Re: Some subtle aspects of relativity. Quote:
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Have fun -- Dick | |||
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| | #23 (permalink) | ||
| Understanding | Re: Some subtle aspects of relativity. Sorry Anssi, I never got a notification that you had posted. But you come through as usual and I appreciate it. Quote:
Have fun -- Dick | ||
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| | #24 (permalink) | |||
| Creating | Re: Some subtle aspects of relativity. Quote:
![]() Traditionally, energy is conjugate to time and momentum to x, in your picture you rearrange both sides, but it amounts to the same identities! Further, your relationship leads to a quantum mechanical relationship of ![]() And I'm pretty sure that this doesn't yield much by way of physics, though I've only played around with it for a few minutes, it doesn't seem to yield anything useful. (mostly because mass is a central charge so doesn't traditionally have a nice operator associated with it, unlike energy which has the hamiltonian). Also, you cannot have tachyons in Einstein's picture either, without violating the rule of particles lines outside the light cone. You can't put tachyons into your picture without violating your everything moves at c rule. Also, tachyons are, in field theory, now believed to be a sign that you've done a calculation wrong (you've picked the wrong vacuum). Hence, there may be no need to fit them into either theory. Quote:
-Will | |||
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| | #25 (permalink) | |||
| Questioning | Re: Some subtle aspects of relativity. Quote:
What DD's epistemological analysis (which is the root of this relativity conundrum) tells you is rather what sorts of laws are common to all reasonable predictive models of any datastream whose meaning is fundamentally unknown. The interesting bit being, that those (entirely general) laws appear to be almost exactly what our best physical models take as the laws of the nature. Let me expand on that before I get to scale invariance. Suppose a newborn baby, or any sort of mechanical learning system, that does not have any information about what reality is like or what to expect from reality. That means, while the learning system is receiving information from its sensory system, it has absolutely no idea about how to interpret any of it in any meaningful way. Nothing can even be "perceived" without being able to interpret that data stream. I.e, it is receiving a datastream whose meaning is fundamentally unknown. Furthermore, its survival depends on it being able to predict that datastream. You could say, it needs to be able to model reality - or how it believes reality is behind that data stream - so to be able to expect dangers that lie in the future. In simple terms you could say that it tacks identity to certain patterns, and comprehends them as "objects", supposing they are governed by whatever laws explain your perception of how they move. Now, since the meaning of the datastream is fundamentally unknown, there exists many valid ways to tack identity to those patterns & making up appropriate laws that explain why such "objects" do what they do. At the end of the day, many features of such worldview will be defined through circular logic, which is completely unproblematic as far as the predictive powers go. Each worldview simply handles the same reality with different sorts of terms. (In fact this can be seen as a rather useful feature as it yields semantics, but let's not get into that now) This much was rather obvious to me before I talked to DD, but I myself had no idea how to even begin to figure out what sorts of mechanisms allow us to start building a worldview from raw data. I just knew it must be possible one way or another since I know nothing about reality for certain, but still I can interpret my sensory data in useful ways. Now, the important bit with DD's analysis is that there also exists certain features that are common to any possible "identity tacking" scheme. These are the symmetries that DD refers to, and the epistemological analysis merely investigates the logical consequences of those symmetries, with rather surprising results. At least initially surprising; it actually does make a lot of sense once you wrestle it in. One of those symmetries is scale symmetry, and don't fail to notice it does indeed refer to scale symmetry to the assignment of labels to ontological elements in the x,tau,t -space. I.e. If the raw data is mapped onto the x,tau,t -table, and then your problem is to come up with an explanation as to what that data means, then that problem is completely unchanged if you scale the mapped data one way or another. (If you are wondering, any specific mapping method is a function of your explanation and vice versa, but whatever they are, the scale symmetry exists) So the scale symmetry does NOT refer to some specific feature of some specific worldview being scale symmetric. It is instead analogous to the entire universe being scaled one way or another. And obviously that would not be observable, as you and all your measuring devices are also part of universe. Quote:
Well, hopefully that was helpful -Anssi | |||
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| | #26 (permalink) | ||
| Creating | Re: Some subtle aspects of relativity. Quote:
Further, one can check if the EXPLANATIONS we have are scale invariant (which is fairly straightforward). Despite the fact that Dick insists his master equation is the backbone of any flaw free explanation, none of the scientific theories we have are scale invariant. This leaves us with two choices: 1. Dick is right, and the other theories wrong. 2. the "standard" theories are right, and Dick has erred somewhere. To decide between 1 and 2, the simplest way should be to figure out predictions made by the two theories and where they differ, do some experiments. I contend scale invariance is one place. In regards to Einstein's spacetime, I fear you are once more missing or talking around my point. Assume the following: Something exists in need of describing Now, there are two ways we can describe this object- the first is to drop down a bunch of arbitrary labels all around it and come up with relationships between the arbitrary labels. The second is to (using the miracle of mathematics) figure out properties of your object that are INDEPENDENT of the labels. i.e. no matter how we change the labels (which are arbitrary), these properties are fixed. Which is better? Dick is doing the first, Einstein the second. I contend the second is better. -Will | ||
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| | #27 (permalink) | ||||
| Questioning | Re: Some subtle aspects of relativity. Quote:
To scale a telescope but nothing else, is just like scaling only that measurement stick but nothing else. Of course it would measure things differently, but that is only one very specific thing inside your worldview being scaled, not the "whole worldview". Quote:
It's much like having your self-coherent set of scientific theories in an algebraic equation. They have certain relationships to each others which makes it impossible to just take one term and change it willy nilly. Instead you'd need to carefully change other terms in the equation accordingly too to keep the whole thing valid. Or there can be certain operations that don't change the relationships in any way, such as multiplying each and every term by some X amount. Quote:
Hmmm, or perhaps I am. The thing is that "what constitutes an object" is part and parcel of our worldview. The latter (Einstein) view is essentially assuming that how we perceive reality, is how the ontological reality really is (which is not unproblematic since you can make multitude of assumptions regarding what happens beyond your observations). The former (DD) view is investigating properties that are found from our model of reality, but not necessarily from reality itself (since we probe reality according to an interpretation that is a function of what we believe reality is like). It could probably be deemed useless if it didn't yield any interesting results. But I do think it is rather interesting that it yields relativistic time evolution to entities, when they are just defined in specific way (which is forced upon us if we are to remain objective). That by itself is an explanation of how relativistic time evolution arises as a feature of a world model, without any knowledge about whether or not it is a feature of reality itself. Without any requirement of it being a feature of ontological reality as is. How's that for surprising? -Anssi | ||||
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| | #28 (permalink) | |
| Creating | Re: Some subtle aspects of relativity. AnssiH, to avoid talking past each other, please let me know which of the following steps you disagree with 1. The universe is scale invariant 2. This implies the universe has no scale 3. This implies that any scale in a measurement comes from the device 4. Therefore, scale dependence in a measurement should be a function of the scale of the device -Will | |
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| | #29 (permalink) | ||
| Questioning | Re: Some subtle aspects of relativity. Quote:
I mean, I could agree with #1 it if it meant "the universe - when taken as a whole - is scale invariant", i.e. when not referring to the idea that "everything in universe looks the same from all the distances", which seems to be what you are thinking of (judging from your earlier posts). I believe here's exactly where the miscommunication lies. I understand that something being scale invariant would in usual physics context mean that it would behave exactly the same way when built in different sizes (against lightspeed or whatever we'd want to use to define size). That is somewhat different issue than the x,tau,t-mapping being scale invariant. Since the x,tau,t-mapping contains your entire (modelled) universe, scaling the entire thing changes nothing in it, much like scaling an entire "spacetime block" (representing the whole universe) would change nothing in it; nothing inside that spacetime block could determine whether that spacetime was scaled or not. I.e. scaling your entire universe in its x,tau,t-mapping doesn't mean its size would go from 10 billion lightyears to 100 billion lightyears, since you'd be scaling that light as well, so to speak. -Anssi | ||
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| | #30 (permalink) | ||
| Creating | Re: Some subtle aspects of relativity. Quote:
Any statement that has real content make a prediction. So, lets try this: does the universe have an associated length scale in DD's model? -Will | ||
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