
Originally Posted by
Woozie
Thanks for the explanations and links, Tristam and SilentRoy.
So true.
Well technically, the term still wouldn't apply. My specific interest would be particle physics if the job market wasn't a problem. The only person (to my knowledge) who's sticking to anything specifically space related is Miz.
The same guy I talked to about biology made a good point about engineers.
I don't care about applications to my research, I learn it just for fun. However, the funding I get from my research are going to be from people who do care about applications. So, technically, we rely on engineers for us to be able to continue our own research.
I still say we get rid them though.
I'm on my sleeping pills while typing this and I'm not going to proof read. So there's bound to be lots of mistakes, and some of the stuff I say may not even make sense.
I'm going to use frequency in my explanation instead of wavelengths. When it comes to color, it makes no difference since every specific wavelength corresponds to some specific frequency. So you could say color depends on wavelength, or equivalently that it depends on frequency. Since frequency is easier to work with mathematically, it's what I'm used to using. As you probably already know, lower frequency means higher wavelength and vice versa.
Our perception of color is pretty much something our brain makes up to distinguish wavelengths, kind of like how we can distinguish pitch. SciAm had an article once about how they could make people see strange or unusual color perceptions by tricking the brain to interpret signals differently somehow.
You are correct in that objects don't have color, they simply absorb and reflect different wavelengths. The reason there are differences between what's absorbed and reflected is related to the quantum nature of light.
First note that the energy of a photon is directly related to it's frequency (the constant of proportionality is planks constant). So red light, which is the lower frequency of the visible spectrum, is simply light composed of photons with lower energy. Blue is light composed of photons with higher energy. So the color we perceive is simply a matter of how energetic the photons in the light are.
For simplicity, suppose we have a hydrogen atom. The electron on the atom will have a certain amount of energy at any given point in time. Quantum theory puts a limit on how low the energy can possibly be. So in other words, you can't make the energy of the electron zero (or arbitrarily close to zero). You're eventually going to reach what's called the ground state, where the electron's energy cannot drop any further under any circumstance.
The electron can become more energetic though. But not by arbitrary amounts. The electron is going to have a "next highest" state. In other words, the electron will either have the ground state energy, or the energy of the next highest state (which we call the first excited state). The electron cannot have any energy between these two states or under the first state. It's either in the first or the second.
So what if I attempt to give the electron an energy between the two states? Suppose, for example, I bombard the atom with photons who's energy is exactly half the amount required to jump from the ground state to the first excited state. Will the electron go halfway up?
Well, as I said, quantum theory wont allow this. So these photons will simply bounce off of the atom instead of being absorbed. We call this "scattering". So whatever energy these photons are, if we divide it by planks constant, we get the frequency (the color) of that light. Since this light is being scattered, we see the object as being that color.
What would happen if we shined a light at exactly the frequency we need to jump from ground to the first excited state (or some other excited state)? The photon would be absorbed. So the object would appear black.
If instead of shining light of one energy on it, we were to shine white light on it, the color we perceive would be the combination of all of the frequencies that are scattered.
For objects other than the hydrogen atom, it works basically the same way. Certain energies are allowed, and certain energies aren't. So certain photons are scattered, and certain photons are not.
Actually, I guess my post has been somewhat misleading so far. There are a bunch of different types of scattering that occur for different reasons. I can't get into those without a bunch of math, so I wont. Just note that the color of an object depends on what frequencies are scattered more easily for any reason. Most of the scattering isn't really the process I described above.
But I did describe the process above for a good reason. Scattering only determines the color of objects that don't emit their own light. In the example above, the frequencies that the hydrogen absorbed are the "absorption spectra" (see Eli's post). When the electron gets excited, it wants to go back to it's ground state. In order to do so, it has to emit a photon. The photon energies it can emit are the same as those it can absorb.
As Eli explained, this is what gives neon its color. The neon is excited by electricity, falls back to a less excited state, and emits light of the frequencies corresponding to changes in energy level. We see the frequencies associated with these energies. In Eli's picture, we see that the emission spectra is simply a bunch of stripes. In most everyday materials, the emission spectrum will be broad bands instead of stripes, or the entire spectrum will be the emission spectrum. In other words, most objects can emit light at any wavelength. However, they do not emit all frequencies equally. Some frequencies will be emitted a lot more than others. The amount of each wavelength emitted depends on the temperature of the object.
If you were to look at a piece of metal, it doesn't appear to emit any light. It actually does, but it emits a very small amount, and at wavelengths that we can't see. The human body emits it in the infrared frequencies, which is why we can track people down with infrared vision technologies. If our eyes could naturally see infrared, everybody would look as if they were gave off their own light (because they do, but we just can't see the infrared frequencies). If we heat up a piece of metal, it eventually starts to emit much more radiation at the red frequencies, so the light appears red. This is essentially where the color of objects who give off their own light come from.
By the way, you misspelled color. For some reason you put a "u" in it, but everyone knows color has no u.