7 ms·
> This is a common error. Macroscopic "everyday" objects don't have a definite position and momentum. Macroscopic objects are quantum objects. But when the mass
by Sylos 7y ago
> This is a common error. Macroscopic "everyday" objects don't have a definite position and momentum. Macroscopic objects are quantum objects. But when the mass is big enough, the position and momentum can be defined simultaneously with an error that is so small that you can just ignore the uncertainty and approximate them as classical objects.
To put this into simpler terms:
Whenever we measure something, we need to throw something at it and then have that something rebound and hit us again.
In most experiments, we throw photons and have them rebound into our eyes.
Throwing a photon against a "classical object" - a chair, a ladder, bacteria - is like throwing a tennis ball against a skyscraper. You throwing that does not have no effect at all, but it's very much negligible.
But when trying to measure quanta, you're now throwing your tennis ball at a football, or at another tennis ball. You're gonna be lucky, if it rebounds at all, instead of just pushing the object that you're trying to measure out of the way. (You also don't have any smaller balls to throw.)
That's why when you measure something in quantum physics, you only know that it has this exact value in the moment that you measure it. It's going to be pushed away because you threw something at it, so after your measurement it has a different value.
You also can't observe it over a longer period, so there's no way to know whether it was only in that moment at your measured position or a long time beforehand.
- david927 7y agoThat's a nice explanation but doesn't it give the impression that if we could find a better way to do that experiment, we could find a way around the problem, when instead it's a fundamental limit on what we can know about a quantum system?
- gus_massa 7y agoI agree with both. This explanation is easier to understand, but it makes it look like a technological problem that can be solved, instead of a fundamental property of the universe.
- atomack 7y agoI think david927's intuition is more correct here. The uncertainty in the position and momentum is intrinsic to quantum mechanics - it's built into the 'wave function'. The suggestion that if one pushes away something by throwing something else builds on a purely classical intuition and wouldn't require quantum mechanics to explain if this was all we observed. The uncertainty in quantum mechanics is fundamental (to quantum mechanics) and emerges through a different, as yet unknown, mechanism.
- bonoboTP 7y agoWhy unknown? Heisenberg's uncertainty principle can be derived mathematically, using a property of the Fourier transform. It has nothing to do with disturbing the system during measurement.
- atomack 7y agoI'd say that's more a mathematical statement than physical derivation. The effort of subjects like string theory is to lay down fundamental objects and interactions from which other theories (quantum mechanics, gravity) emerge. But I don't think there is a final word at the moment of what the fundamental theories than result in quantum mechanics should look like.
- gus_massa 7y agoIn string theory, they use quantum (super)strings, not classic strings that somehow simulate quantum particles. It's quantum all the way down.
- pdkl95 7y ago3Blue1Brown has an extremely good explanation[1] of the intrinsic uncertainty, and why it's separate from measurement uncertainty. (the previous episode[2] is a recommended prerequisite for background on how the Fourier Transform works) > emerges through a different, as yet unknown, mechanism. In 3Blue1Bron's explanation[1], he shows how the intrinsic uncertainty is an inherent trade-off of trying to measure both position and frequency. A short wave packet only a few wavelengths long correlates with a narrow (precise) range of positions, but also correlates well with a very wide range of frequencies due. A Heisenberg-like uncertainty exists any time you are working with weave packets with length near the wavelength. 3Blue1Brown gives a very good example using Doppler radar. [1] https://www.youtube.com/watch?v=MBnnXbOM5S4 https://www.youtube.com/watch?v=MBnnXbOM5S4 [2] https://www.youtube.com/watch?v=spUNpyF58BY https://www.youtube.com/watch?v=spUNpyF58BY
- wodenokoto 7y agoBut isn't the reason why it is a fundamental problem, that fundamentally there is nothing smaller to throw?
- andreareina 7y agoThe problem is that fundamentally, there is a fixed amount of information that there is, that has to be distributed over two dimensions. Particles that are constrained to a small area (e.g. photons going through a slit, electrons bound to an atom) simply do not have a well-defined momentum. In fact the effect is something that you can experience with a sharp enough camera lens: as you close the aperture (therefore forcing the light going through it to be in a specific place) you slowly lose resolving power as the light stops behaving nicely and diffracts around/through the aperture.
- jacobmoe 7y agoNo, under most interpretations of QM, things literally behave differently at that scale. Under Copenhagen, the wave literally collapses into a fixed position/momentum. The pre measurement wave isn't a statement of our ignorance of the system but rather a description of reality. The many worlds is even more serious in its quantum literalism. Far from pushing around the subject of your experiment with a too-big measuring device, you're actually branching worlds where all predictions of the wave function occur.
- exoesquitur 7y agoTo me, many worlds + time (as an inviolate observed vector) being merely a consequence of our inability to observe without moving foreward in time based on our entropic process driven cociousness, seems by far the most comprehensive explanation of observable phenomenon. That observational uncertainty increases as the probability of direct interaction decreases (distance, time) strongly supports the hypothesis that observable phenomena are dictated strongly by the presentation and characteristic relationship of the observer to the phenomenon. We know on the micro scale that all possible states exist simultaneously. It seems logical, even axiomatic then that on the macro scale the same applies, but that we can only observe the bandwidth of states in which it is possible for us to exist to make the observation. To claim that this state uncertainty is magically resolved in all cases and coherently for all possible observers into a single set of states seems an extraordinary claim requiring extraordinary evidence.
- l33tman 7y agoThis is not a correct description at all of QM complementary observables. This is a purely classical explanation (and was one of the first layman "explanations" back in 1920, but that was 100 years ago and QM is much better understood now).
- mercer 7y agoCould you elaborate on that? From my extremely limited knowledge it does seem like a just-so explanation (what you're responding to), but I'm not sure why.
- chriswarbo 7y agoThe 'measuring something disturbs it' idea described above is called the observer effect https://en.wikipedia.org/wiki/Observer_effect_(physics) https://en.wikipedia.org/wiki/Observer_effect_(physics) The observer effect is a real thing, and even has interesting effects in quantum mechanics, e.g. the quantum zeno effect https://en.wikipedia.org/wiki/Quantum_Zeno_effect https://en.wikipedia.org/wiki/Quantum_Zeno_effect Yet the observer effect is not the reason why we can't know an object's position and velocity at the same time. There are two ways we can see that this supposed explanation is a red herring: - We don't need to interact with (e.g. 'bounce a photon off') a quantum system in order to observe it ( https://en.wikipedia.org/wiki/Interaction-free_measurement https://en.wikipedia.org/wiki/Interaction-free_measurement ). I particularly like the "quantum bomb detector" ( https://en.wikipedia.org/wiki/Elitzur%E2%80%93Vaidman_bomb_tester https://en.wikipedia.org/wiki/Elitzur%E2%80%93Vaidman_bomb_t... ), which can tells us whether a photon detector connected to a bomb is working or not, without hitting it with a photon and hence triggering the bomb (50% of the time, at least). - The actual reason, the uncertainty principle ( https://en.wikipedia.org/wiki/Uncertainty_principle https://en.wikipedia.org/wiki/Uncertainty_principle ), doesn't require any notion of observation at all, let alone interaction. It's a simple property of waves (the relationship between duration and frequency). 3blue1brown did a nice video on this https://www.youtube.com/watch?v=MBnnXbOM5S4 https://www.youtube.com/watch?v=MBnnXbOM5S4
- cygx 7y agoThe observer effect and the uncertainty principle are not the same thing.
- dave_sullivan 7y agoI don’t think this analogy holds up. Consider the double slit experiment: throw a bunch of basketballs at a wall and see what pattern of hits they leave by looking at where they hit the wall. If the wall is being looked at (observed), we see one pattern. If we look away, conduct the experiment, then check it, we find another. To me that suggests the act of “observance” effects the probability distribution of likely states. If a tree falls in a forest and no one is around, then it doesn’t really fall, it just has a probability of having fallen that is not resolved until someone goes to check. How does your analogy account for those effects? For me, it looks like quantum collapse is causing the states of these objects to become “resolved” where at first they were “unresolved” and this suggests we live in a universe that knows how to save on memory and is fundamentally probabilistic.
- Abishek_Muthian 7y ago>Consider the double slit experiment: throw a bunch of basketballs at a wall and see what pattern of hits they leave by looking at where they hit the wall. If the wall is being looked at (observed), we see one pattern. If the basketball was of energy 1 quantum, if the energy used to observe is 1 quantum or more the (shining light to see the result in realtime) then the pattern is different due to interference. If we don't use any energy to see the result in realtime, then result is different due to non-interference. Did what I say hold up?
- dave_sullivan 7y agoI could be wrong, but I have a different understanding on how all of that works. You keep talking about basketballs instead of waves or probability fields and I guess this is where we diverge.
- chriswarbo 7y ago> Did what I say hold up? No ;) > If the basketball was of energy 1 quantum, if the energy used to observe is 1 quantum or more the (shining light to see the result in realtime) How would we observe the light that bounced off the basket ball? Would we need to hit it with another light in order to detect where that light is? How would we detect that second particle of light; would we hit it with a third? And so on. The answer is that we don't need to shine light to see the basketball. We can detect the basketball itself; for example, if the basketball were representing a photon of light, we could cover the wall with photomultiplier tubes ( https://en.wikipedia.org/wiki/Photomultiplier_tube https://en.wikipedia.org/wiki/Photomultiplier_tube ) As sibling comments have pointed out, the parent is wrong in saying that observing the wall will change the pattern. Rather, it's observing the slits that will change the pattern. If we don't observe the slits, but we do mark the point on the wall where the basketball hits, and we do this over and over again, then the marks on the wall will show an interference pattern. Note that we're not throwing anything at the basketball: we're just waiting for it to hit the wall on its own. Also note that the marks themselves don't change anything; we could note them down on some paper instead, or type them into a spreadsheet, or whatever. What if we do observe the slits, e.g. by putting a baseball in one and a cricket ball in the other? In this case, we'll detect the basketball hitting the wall and either a baseball or cricket ball. After many goes, the pattern on the wall made by the basketball will have two peaks (one in front of each slit), not an interference pattern. This seems analogous to your 'bounce a photon off it' explanation. However, what if we got rid of the cricket ball? Half the time we would detect the baseball hitting the wall too, the other half we wouldn't (when the basketball went through the other slit). Yet the basketball will still make the two-peak-no-interference pattern, even though we didn't interact with it half of the time! In fact, we could randomise which slit we put the baseball in, and mark only those goes that the basketball didn't hit the baseball, and we would still see two peaks without an interference pattern, even though those basketballs didn't hit anything (they always went through empty slits)! This hopefully shows that your explanation (known as the observer effect) doesn't explain the interference pattern in the double-slit experiment.