• Welcome to the new Internet Infidels Discussion Board, formerly Talk Freethought.

“The Unravelling of Space-Time”

pood

Veteran Member
Joined
Oct 25, 2021
Messages
4,603
Basic Beliefs
agnostic
Looks to be a interesting series here, divided into nine parts, at Quanta, called “The Unravelling of Space-Time.” The interactive intro page to which the link takes you is inventive, especially at the end where you can manipulate an entire concluding paragraph to fall down a black hole, but still rather annoying for all that. Just because you can do something, doesn’t mean you should. Wisdom from Jurassic Park

However, the page is participatory, a nice intro the first essay.

The first essay, the only one I’ve read so far, is on John Wheeler and his participatory universe. Wheeler seemed to be taking us very close to abandoning metaphysical naturalism in favor of metaphysical idealism, and the latter has always intrigued me as a live possibility. An extract from the essay:

In 1977, Wheeler gave a talk emphasizing that “no elementary phenomenon is a phenomenon until it is an observed phenomenon.” Afterward, the physicist Paul Dirac asked, “The formation of the solar system is a phenomenon. Is it only a phenomenon when it is observed?” Wheeler responded: “Yes.”

How much this is like old Schopenhauer, who lived before relativity, quantum physics, modern science, et al, and yet was motivated to write:

The existence of this whole world remains ever dependent upon the first eye that opened, even if it were that of an insect

Toward the end, it recounts how Wheeler agonized over how it is, in a participatory universe, that there is any consensus reality at all. And I couldn’t help wonder whether he was even moving beyond potential metaphysical idealism to potential metaphysical solipsism.

But even before Wheeler, special relativity was telling us we all have our own private space-time. That there is any superficial consensus about it is because in the main we share the same reference frame.

Anyhow, even though Wheeler was a scientist I put this in the philosophy forum, which is perfectly OK because IMO science and philosophy and inextricably intertwined. I’ll read all the essays as time permits and hopefully others will, too, and offer comments. To me, this is so much more interesting than mere politics, though unfortunately politics is probably more important for everyday life, especially now.
 
Schrodinger came up with his cat problem to illustrate the ridiculous ways QM can be interpreted..

Or the old 'if a tree falls in the woods and there is no one there to heat it does it make a sound?'.

I heard that as a kid.

Experimentally in a a particle experiment the instrumentation is the observer. We interpreter the interaction of the test apparatus and the particle.

The Brookhaven site has descriptions of the RHIC collider and how particles are detected in a collision experiment.
 
Schrodinger came up with his cat problem to illustrate the ridiculous ways QM can be interpreted..

Yes, it was intended as a reductio, but did it really do what he intended?
 
Schroedinger apparently intended the cat as a reductio of Copenhagen QM, which is that quantum particles are in superposition until measured. The cat set-up scales up QM to the macro level, suggesting the cat was both alive and dead until measured. He felt that was absurd, but in 1952 he broached the idea that the cat was both alive and dead in different universes. Hugh Everett presented his worked-out thesis of this notion five years later.
 
Schrodinger came up with his cat problem to illustrate the ridiculous ways QM can be interpreted..

Or the old 'if a tree falls in the woods and there is no one there to heat it does it make a sound?'.

I heard that as a kid.

Experimentally in a a particle experiment the instrumentation is the observer. We interpreter the interaction of the test apparatus and the particle.

The Brookhaven site has descriptions of the RHIC collider and how particles are detected in a collision experiment.
Test apparatus and particles: pulling information about "a particle" inevitably requires a change in the particle to generate that information except in very rare cases such as time crystals, and that's less "not changing" and more "changing back again completely after the interaction"
 
That is the problem with QM measurements.

Put a thermometer into a glass of water. You do not resume the water you measure the temperature of thermometer, water, and glass. There are very small low mass thermal sensors to minimize the disturbance created by the sensor. Analogy to quantum measurements.

Energy from the water is lost to heat up the tmermometr.

Put a thermometer into a large lake and the mass f the thermometer is insignificant. Macro Newtonian measurements.

Whether something exists until measured or observed to me is semantics.

Flip a coin in the air in a dark room. Periodically flash a light while it is in the air and there is a probability of it being in a certain orientation.

When it settles on the floor the wave function has collapsed from a 50/50 probability of heads or tails to an actual observable heads or tails. At no time does the coin not exist in a measurable state.
 
That is the problem with QM measurements.

Put a thermometer into a glass of water. You do not resume the water you measure the temperature of thermometer, water, and glass. There are very small low mass thermal sensors to minimize the disturbance created by the sensor. Analogy to quantum measurements.

Energy from the water is lost to heat up the tmermometr.

Put a thermometer into a large lake and the mass f the thermometer is insignificant. Macro Newtonian measurements.

Whether something exists until measured or observed to me is semantics.

Flip a coin in the air in a dark room. Periodically flash a light while it is in the air and there is a probability of it being in a certain orientation.

When it settles on the floor the wave function has collapsed from a 50/50 probability of heads or tails to an actual observable heads or tails. At no time does the coin not exist in a measurable state.
The coin toss is not the same in quantum as in classical. In classical, you could predict the outcome of the toss if you had knowledge of all the variables, a practical impossibility but possible in principle. In QM this not possible even in principle.
 
.A coin toss is the same principle. A wave function can be derived to model the toss.

The way I remember it put is as you go from quantum to Newtonian scale the density of states is such that it appears continuous. Like a piece of copper. What we seen as a Newtonian scale block of metal is the superposition of all the instantaneous states of each atom in the block.

The problem with QM is the relative energies. In electronics it usually easy to s reduce the interaction of apparatus and what is being measured such that the effect is inconsequential.and quantfy the effect of a measurement apparatus.

Put6v a battery at exactly 10 volts acrostwo resistors in series each at exactly 1 ohm and the voltage across each resistor will be exact 5 volts. Put a meter across a resistor to measure the voltage an it will not read exactly 5 volts. The meter reads the voltage due to the subsystem inclusive of the circuit and measure mt apparatus. The input resistance of the meter becomes part of the circuit.

Does what we perceive as a particle in an experiment a a manifestation of the measurement or does the particle exist as we model it?
 
A semi-rebuttal to Quanta’s series on The Unraveling of Space-Time, in which the author contends that the series is
“ironic science.”
 
.A coin toss is the same principle. A wave function can be derived to model the toss.

The way I remember it put is as you go from quantum to Newtonian scale the density of states is such that it appears continuous. Like a piece of copper. What we seen as a Newtonian scale block of metal is the superposition of all the instantaneous states of each atom in the block.

The problem with QM is the relative energies. In electronics it usually easy to s reduce the interaction of apparatus and what is being measured such that the effect is inconsequential.and quantfy the effect of a measurement apparatus.

Put6v a battery at exactly 10 volts acrostwo resistors in series each at exactly 1 ohm and the voltage across each resistor will be exact 5 volts. Put a meter across a resistor to measure the voltage an it will not read exactly 5 volts. The meter reads the voltage due to the subsystem inclusive of the circuit and measure mt apparatus. The input resistance of the meter becomes part of the circuit.

Does what we perceive as a particle in an experiment a a manifestation of the measurement or does the particle exist as we model it?

Regarding the coin toss. Why not consider the entire process, including the state when the coin is in mid-air and its outcome is still undetermined, as part of a single state? Is it not possible that the coin’s undetermined state isn’t just a precursor to the determined state but is itself an essential part of determined state?

The undetermined state is not something that can be directly measured. right? That's telling. We can calculate the probabilities (e.g., 50/50 chance of heads or tails), but we can't definitively capture its exact outcome until the coin lands.

In quantum mechanics, the brainiac's seem to be dealing with probabilities until measurement "collapses" the wave function. So, my taking an uneducated guess, both the undetermined and determined states are part of a unified process, rather than separate states. The states determined/undetermined might seem separate do to some other phenomena giving us that illusion. Could it be that the act of measurement introduces a form of space/time interference, not actually changing the state from undetermined to determined, but instead giving us the illusion that these states are separate? Perhaps the distinction between undetermined and determined states is an artifact of limitations in our measurement tools, rather than a true reflection of our underlying reality?

It reminds me of those old cheap baseball cards you’d find in cereal boxes—when you slowly tilt the card, you can see the batter swing and hit the ball. The image changes as you adjust your perspective, but it’s really just one card showing different phases.

Please forgive me—but my formal education is not strong, my imagination is. :)
 
What happens in QM is you get the probabilities, but never the certainties, of outcomes by squaring the amplitude of the wave function. This is in direct conflict with determinism. But Newton, in his genius but lacking the tools at the time for figuring this out, sensed there was something wrong with determinism and with classical reality. He simply asked himself a rather obvious question that seems never to have occurred to anyone else, or, if it did, they never mentioned it. Why is a window transparent to most light, but not ALL of it? If windows were fully transparent, we could not see any reflections in them. The answer is quantum mechanics. There is a calculable chance that about five percent of photos, by random chance, will not go through the window.
 
Incidentally, Newton also had serious doubts about his theory of gravity. The description was fine (at that time) and still is mostly fine, but he fretted over what gravity IS. So already he anticipated Einstein, who showed it was not a force at all but the warping of spacetime around the masses of objects.
 
my formal education is not strong, my imagination is.
So are your baseball cards. I ain't never had nuthin like that.

My memory isn’t the best—I’m starting to think they might not have been baseball cards after all. I just looked it up, and they’re called lenticular cards. That’s what I was thinking of, though maybe they didn’t come from cereal boxes.
 
What happens in QM is you get the probabilities, but never the certainties, of outcomes by squaring the amplitude of the wave function. This is in direct conflict with determinism. But Newton, in his genius but lacking the tools at the time for figuring this out, sensed there was something wrong with determinism and with classical reality. He simply asked himself a rather obvious question that seems never to have occurred to anyone else, or, if it did, they never mentioned it. Why is a window transparent to most light, but not ALL of it? If windows were fully transparent, we could not see any reflections in them. The answer is quantum mechanics. There is a calculable chance that about five percent of photos, by random chance, will not go through the window.
I believe one can calculate the Fresnel coefficients (i.e., how much light is reflected rather than transmitted at an air-glass interface) without relying on QM and giving in to "random chance". But, I admit, it's been a while since I've seen such a derivation so I would have to go look it up. I'll admit that it may be that the coefficients rely on QM properties underneath them that were not known, but still measurable, at the time of Fresnel and others.
 
Incidentally, Newton also had serious doubts about his theory of gravity. The description was fine (at that time) and still is mostly fine, but he fretted over what gravity IS. So already he anticipated Einstein, who showed it was not a force at all but the warping of spacetime around the masses of objects.
That may not be what it IS, if there's even an answer to a question like that, but it certainly is a highly successful expansion of the Newtonian model.
 
Back
Top Bottom