The color of an apple (light absorption and emission)

In summary, the apple in the picture is illuminated by daylight, and the main part of the light it reflects is in the red area of the visible spectrum. Molecules in the skin of the apple absorb the blue and the green part of the spectrum and this causes the apple to appear black under blue light but red under white light.
  • #1
kenewbie
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Emission of light from a solid object

From my textbook (explaining why an apple is red):

We imagine that the red apple in the picture is illuminated by daylight, IE light which contains all the wavelengths of the visible spectrum. The apple is red because the main part of the light it reflects is in the red area of the visible spectrum.


This is all good, and is what I expected. My understanding of this is that the atom is exited by a photon of a certain wavelength, and then when it returns to its original energy level it emits a photon of the same wavelength again. This is why it reflects the light.

However the next sentence goes on to say:

Molecules in the skin of the apple absorbs the photons in the blue and the green part of the spectrum. If we look at it with a strictly blue light, the apple will appear black.


This threw me off. My understanding is that matter will only interact with photons of certain wavelengths, and the wavelengths an atom can absorb are the exact same which it can emit. Other wavelengths should not interact with it at all?

So if the atoms in the skin of the apple absorbs the blue light, it should also emit it once the atoms return to their original energy level?

It seems to me that the the first paragraph is enough to explain the red color of the apple, and I am at a loss of what they mean with the second one.

Is my understanding of this way off?

Any and all help appreciated.

k
 
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  • #2
As a matter of fact, an apple does not consist of isolated atoms but of molecules which are themselves interacting with each other. While an atom has in deed very sharp absorption lines, molecules absorb in broad frequency ranges (bands). Furthermore, as they have internal degrees of freedom, namely vibrations, the energy absorbed can be transformed into vibrational energy and finally into heat. Thats called internal conversion (IC). Hence molecules will re-emit (fluorescence) only a small fraction of the light they absorbed and even this usually not at the same wavelength, but at longer wavelengths.
 
  • #3
kenewbie said:
This is all good, and is what I expected. My understanding of this is that the atom is exited by a photon of a certain wavelength, and then when it returns to its original energy level it emits a photon of the same wavelength again. This is why it reflects the light.

No. That's not correct - that does not explain reflection. What you're thinking of is absorption and re-emission of light along the spectral lines of the atoms. This is not what's happening in reflection.

I have my own fuzzy theory on reflection - but maybe someone could give the standard and accepted version.
 
  • #4
DrDu said:
Furthermore, as they have internal degrees of freedom, namely vibrations, the energy absorbed can be transformed into vibrational energy and finally into heat.

Ok, that makes sense. My only question then is if absorption and conversion to heat is an emergent behavior in molecules, or if this happen at the layer of individual atoms as well?
 
  • #5
kenewbie said:
Ok, that makes sense. My only question then is if absorption and conversion to heat is an emergent behavior in molecules, or if this happen at the layer of individual atoms as well?

That is an oxymoron. Either the atoms are individual or there is a layer of them on the surface of a 'condensed object'. There is a great difference between the interaction of photons with individual atoms and with large numbers of atoms in close proximity.
When an isolated atom absorbs a photon, under normal circumstances, it will re-radiate light at the same frequency that it observed. But there is a possibility of the decay being in two or more jumps if the appropriate energy level in the atom. (Look at the operation of a Laser, for instance).
When an atom or molecule on the surface of an object (dense material) absorbs an optical photon there are many more possible energy levels involved (bands, rather than discrete levels, in fact) and the incident photon's energy can be redistributed in the material of the object in many different ways and a broad range of frequencies will be absorbed, as a consequence. (No line absorption spectrum)

So your apple will absorb all sorts of green(ish) and blue(ish) wavelength photons but not the red(ish) ones. Under white light illumination, the apple will look red. But if there is no red in the incident light, the apple will look black(ish).
 
  • #6
It is quite astonishing that already a hand full of atoms forming a molecule is sufficiently complex a system to justify a thermodynamical description. So yes, it is an emergent thermodynamical property of molecules.
Just yesterday there was a related question in the chemistry forum. Maybe you want to have a look at the classic article by Bixon and Jortner I cited there:
https://www.physicsforums.com/showthread.php?t=621627
 
  • #7
sophiecentaur said:
That is an oxymoron. Either the atoms are individual or there is a layer of them on the surface of a 'condensed object'. There is a great difference between the interaction of photons with individual atoms and with large numbers of atoms in close proximity.

Still it came as a big surprise in the 1960's that essentially irreversible behaviour was found already for rather small isolated molecules like benzene in the gas phase.
 
  • #8
DrDu said:
It is quite astonishing that already a hand full of atoms forming a molecule is sufficiently complex a system to justify a thermodynamical description. So yes, it is an emergent thermodynamical property of molecules.
Just yesterday there was a related question in the chemistry forum. Maybe you want to have a look at the classic article by Bixon and Jortner I cited there:
https://www.physicsforums.com/showthread.php?t=621627

I guess it's just a matter of nCm, which involves Factorials. It's very easy to get large numbers from a molecule with three or more atoms in it and when several of the electrons in each atom are interacting with those in the other atoms. And then there are the vibrational modes etc.

The old Hydrogen Atom stuff we start with is just not enough to deal with anything more complicated - but, deep down, we want it to.
 
  • #9
sophiecentaur said:
I guess it's just a matter of nCm, ...
That's the point. In a molecule like benzene you have already 31 vibrational modes. Given that the electronic excitation energy corresponds to an order of magnitude [itex] \sqrt{m/M}\approx 100 [/itex] (with m electron and M nuclear mass) vibrational quanta, the number of vibrational states to decay into is already astronomical.
 
  • #10


Hi kenewbie. I think your question is a very good one. Since no one else has yet replied, I will try to give some explanation as I understand it.

You are right that an atom (molecule) that jumps to an excited state by absorbing a photon of a specific frequency could "de-excite" by emitting a photon of the same frequency. But, when atoms are crowded together in a solid or liquid, an excited atom is more likely to pass the energy to its neighboring atoms in the form of motional energy of the atoms (heat) rather than re-emit the energy as a photon. So, the original photon that excited the atom has become absorbed by the material with no light being re-emitted. That's why if you shine only blue light onto an apple, the apple will appear dark.

But then why is it that when you shine red light on an apple, the apple reflects the red light? Even though red light does not have the right energy of photons to excite the atoms or molecules to higher energy states, the light nevertheless does interact with the electrons in the molecules and causes the light to be scattered. The reflection of the red light from the apple is this scattered light.

The best non-mathematical discussion on this topic that I have ever seen is the article How Light Interacts with Matter by Victor Weisskopf which was published in the book Lasers and Light, Readings From Scientific American 1968. Could be hard to find, but well worth the effort.
 
  • #11
sophiecentaur said:
That is an oxymoron. Either the atoms are individual or there is a layer of them on the surface of a 'condensed object'.

I had to re-read this a few times but I think i have found that my choice of the word "layer" was poor, as it seems to have a specific meaning. What I meant to ask was if individual atoms sometimes absorb photons without emitting photons, or if this is behavior which only happens in molecules.

And you did answer my question, so thanks :)
 
  • #12
DrDu said:
It is quite astonishing that already a hand full of atoms forming a molecule is sufficiently complex a system to justify a thermodynamical description. So yes, it is an emergent thermodynamical property of molecules.
Just yesterday there was a related question in the chemistry forum. Maybe you want to have a look at the classic article by Bixon and Jortner I cited there:
https://www.physicsforums.com/showthread.php?t=621627

Thanks, I'll read that. The question now is, of course, HOW can this behavior arise, what is happening which makes this possible. But I'll read that thread and do a little digging on my own, it is far ahead of what I am supposed to be looking at anyway.

Thanks again.
 
  • #13


I'd go along with that ... I found:
http://www.madsci.org/posts/archives/aug99/934381368.Ph.r.html
... which aught to be a nice overview but longer. It would be nice if http://www.nature.com/scientificamerican/journal/v219/n3/pdf/scientificamerican0968-60.pdf were not behind a paywall: it's very commonly cited.

BTW: the absorption description of color for opaque matter also explains the commonly observed difference between mixing light and mixing paint ... in paint, if you combine blue and yellow you get green ... but with light, blue+yellow=blue+(red+green)=white. Also how come you get brown when you mix all the colors in paint.
 
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  • #14
kenewbie said:
Thanks, I'll read that. The question now is, of course, HOW can this behavior arise, what is happening which makes this possible. But I'll read that thread and do a little digging on my own, it is far ahead of what I am supposed to be looking at anyway.

Thanks again.
It's what you get with 'large numbers'. Combinations within small numbers of items can rapidly lead to large numbers. Just take the game of Poker and see how much theory and lore is associated with picking just five cards out of 52.
 

FAQ: The color of an apple (light absorption and emission)

1. What gives an apple its color?

The color of an apple is determined by the pigments present in its skin. These pigments absorb certain wavelengths of light and reflect others, giving the apple its characteristic color.

2. How does an apple absorb light?

An apple absorbs light through the pigments in its skin. These pigments have molecules that are able to absorb specific wavelengths of light, while reflecting others. The absorbed light is then converted into energy.

3. What is the role of chlorophyll in an apple's color?

Chlorophyll is a green pigment found in the skin of an apple. It plays a vital role in the process of photosynthesis, where it absorbs light energy and converts it into chemical energy. Chlorophyll is also responsible for giving apples their green color.

4. Can the color of an apple change?

Yes, the color of an apple can change. As apples ripen, the chlorophyll in their skin breaks down, revealing other pigments such as anthocyanins, which give the apple a red or purple color. Some apples may also change color due to bruising or exposure to sunlight.

5. How does an apple emit light?

An apple does not emit light on its own. However, it may reflect light that is shone on it, and this reflected light may appear as if the apple is emitting light. This is due to the pigments in the skin that are reflecting certain wavelengths of light, giving the appearance of light emission.

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