Recent comments in /f/askscience

PapercuttingTheHell t1_j8j7mri wrote

I could answer but it's primarly borig for anyone else that electricians and electrical and electronical engineer. So just to make it clear, there's no matter involved, only electric fields, which have magnetic properties if used as so. We call it waves because as soon as we want to illustrate them ; models will turn that in something that's most understandable in the form of waves. Flies off

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bringmeadamnjuicebox t1_j8j6w9f wrote

Ventilators often run with a heated humidification system. The circuit will collect enough water that it has to be drained. Patients are coughing all sorts of gross crud into the tubing. The circuit also gets broken from time to time, as stuff gets soiled or clogged, parts need to get changed out. So there's often opportunity for bugs to get in there.

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MasterPatricko t1_j8j6gkn wrote

> according to General Relativity, a massless particle must always travel at c.

That's special relativity, not general relativity (yes, GR includes SR, but you get what I mean).

The fundamental wrong assumption people make is that a wavepacket of the EM field -- a photon -- in a vacuum is somehow "the same" as the wavepacket of the EM field in a complex background of charged particles, i.e. a real material made of atoms.

To make an analogy (of limited range, please don't abuse it :)): no-one is surprised that a classical gravity wave in water and a wave in honey behave differently. Why is it surprising for an EM wave? /u/Keudn 's description is classical and doesn't explain how to calculate the speed in a medium, but aside from that missing depth, strictly correct.

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mikerowave t1_j8j4cet wrote

One interesting example of how the very fast but finite speed of light can change what we see when we look at an object over an extended period of time is the observed light echo in V838 Monocerotis system. In the video (which is composed of individual observations over a time base of 2 or 3 years), it looks like we are watching a shell of debris expand out away from the central pair of objects, but this is actually not the case. Rather, what we are seeing is light traveling outward and illuminating successively further layers of a pre-existing but invisible shell of material

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GeriatricHydralisk t1_j8j41wp wrote

Like everything in biology, there's one, unified answer: It depends.

Specifically, how do you define "exoskeleton"?

If you define it broadly enough to simply be a hard, outer layer, then basically everything with armor fits the bill: turtles, armadillos, oysters, etc. Even a variety of protists like diatoms.

If you say it has to support body weight, it gets more tricky, but there a few examples that squeeze in here: turtles again, crocodiles have specialized muscles to "brace" against their armored hide when walking, etc.

If you specify that it has to be involved in turning muscle shortening into body motion, like in arthropods and with our endoskeleton, nematodes may fit the bill, as they have a collagenous "cuticle" which inertnal muscles attach to. But it's not truly "rigid" the way an arthropod exoskeleton is (think of it like stiff rubber).

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MasterPatricko t1_j8j3fc4 wrote

I think you're on the right track, mostly. I can try to add some detail/clarification.

> 1) you emitted a single photon, there is a high probability that photon would be detected by the detector.

Yeah, more or less -- the probability depends on the coefficient of reflection of the surface of the glass. It could be high, or low, depending on the angle and refractive index of the glass, and will match the classical calculation of the relative amplitudes of transmitted and reflected waves (Fresnel equations), because fundamentally, the photon wavefunction is obeying pretty much the same wave propagation laws. Note you only get this behaviour if the photon wavefunction spatial extent (typically many photon wavelengths) means that it has the possibility to interact with many identical atoms which are spaced in a uniform way (relative to the wavelength of the photon). This is mostly true for optical wavelengths hitting normal materials (typical atom spacing 0.1nm, optical wavelength 500nm, any random variation is too small to be "seen" by a photon) but is not necessarily true at shorter wavelengths like X-rays, or if your "glass" is only a few atoms big. Those scenarios are more complicated and you don't always end up with the "normal" ray optics rules after summing those probabilities.

The only real difference to the classical wave picture is in the moment of detection -- instead of measuring a classical wave, with some part reflected and some transmitted, we are set up for a discrete, quantum mechanical interaction in the detector. A 1 or a 0. This collapses* the wavefunction according to the probabilities mentioned before, to either interact with the detector (and so we say the photon was transmitted and then absorbed in the detector) or not (and here we can say the photon was reflected).

> 2) ... However, because they are all part of a wavefront, none of them would be emitted out the sides of the transparent material?

You can hopefully see how the previous explanation scales up to emitting many photons, the numbers of photons detected will match the probability calculations. But to address your last sentence -- in this toy example, I assumed that there was no internal absorption or scattering inside the glass. In such a case, the original+scattered wavefunctions sum up such that the only possibilities are transmission straight through or reflection right at the interface, and there is no chance for a "random" photon to emerge out of the side of the glass at some angle. This isn't to do with photons being "part of a wavefront", unless I misunderstand you. More fundamentally, photons are waves; or at least, they travel in the same ways that classical waves do, and waves moving through a uniform medium don't just randomly scatter.

Now if we make things a bit more realistic -- the glass is not going to be a perfect crystal, and the uniform background of atoms assumption is not going to be exactly true. There will now be a small possibility of the wavefunction scattering differently off some imperfection in the atomic structure. Because it's associated with an imperfection, this part of the wavefunction won't be cancelled out by all the neighbouring scattered amplitudes, and you will end up with a real (but small) probability to have a photon emerging out of the side of the glass in some random direction, in addition to the main probabilities of transmission or reflection at the surfaces.

* "The measurement problem", or what exactly wave-function collapse really means physically, is a very thorny issue to which there isn't a good answer. But we know that mathematically, it works.

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drc500free t1_j8j35ct wrote

Think of the individual photons as different locations where a single universal wave function has high density, not as distinct particles. The idea that they are distinct only holds while those locations don't interact and interfere significantly.

Once they interact, the resulting waveform will have other regions of high density. Mapping one of them back to one of the original ones and saying this new photon is the "same" as that original photon is something that might make your brain understand it better by pretending they are Newtonian objects. But it's just a model for understanding, and the further the interaction is from Newtonian collisions the more wrong it will be.

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Miss_ChanandelerBong t1_j8j1wh8 wrote

Like most things in science, the devil is in the details, and most people just don't have the expertise to parse those details out. Or, in many cases, the details aren't yet fully known. That's why it seems like there are contradictions, but, in reality, it's just different nuances.

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common_sensei t1_j8j1l8a wrote

Try it yourself!... although it probably won't work as described.

The wave would mostly regain the speed after the ping pong ball area, but it would be much reduced in height. A lot of energy would be lost to ripples going everywhere. My analogy just serves to illustrate the general concept of particles reacting to the approach and passing of the wave and generating interfering waves of their own.

However, a similar effect can be seen in wave tanks when you change the depth of the water: https://youtu.be/4_VejGC0DMM?t=261

In this case the interfering waves are bouncing from the new lower bottom of the tank, slowing down the wave.

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