Why does combining hydrogen atoms result in decreased energy?

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The discussion centers on the phenomenon where the combined energy of two hydrogen atoms forming H2 is lower than the energy of individual hydrogen atoms. This reduction in energy is attributed to several factors, including electron motion and the resulting changes in kinetic energy, as explained through quantum mechanical models such as the particle-in-a-box effect. The binding energy of H2 is established at 15.43 eV, significantly lower than the total energy of separated atoms, which is calculated to be 228 eV. The conversation emphasizes the importance of considering both classical electrostatic energy and quantum effects in understanding chemical bonding.

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Why is it that when two hydrogen atoms combine together, their combined energy is less than the energy of one hydrogen atom by itself? Why wouldn't the combined energy be twice as much?
 
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6021023 said:
Why is it that when two hydrogen atoms combine together, their combined energy is less than the energy of one hydrogen atom by itself? Why wouldn't the combined energy be twice as much?
To what combined energy is one referring?
 
The combined energy of the two hydrogen atoms when they come together to form H2.
 
Last edited:
I.e. the binding energy. Okay, well how detailed an answer do you want?

A simple "conceptual" hand-waving answer would be something like:
1) Because electrons are in motion, they don't fully screen the nuclear charge. So even though a hydrogen atom is neutral, the electron on the other hydrogen atom will 'see' a charge from the other nucleus. Therefore, the total electronic energy will be lower if the two nuclei are closer together, up to the point where the nuclear-nuclear repulsion becomes greater than this effect.
2) The electron-electron repulsion, on the other hand, is offset by the correlation of electron motion, in other words, the electrons 'choose' patterns of motion such that they avoid each other.

Less hand-waving justifications start with http://www.springerlink.com/content/j434g68810rj5315/?p=9bb29ff33304469ea1fd7f1b8a80e527&pi=5".

In-between you've got explanations in terms of Lewis structures (binding gives a full shell), MO theory (the two 1s orbitals combine to form a bonding \sigma orbital), Valence-Bond theory, Hartree-Fock, etc.
 
Last edited by a moderator:
6021023 said:
The combined energy of the two hydrogen atoms when they come together to form H2.
I'm guessing one means binding energy as alxm mentions.

physics.nist.gov/cgi-bin/Ionization/table.pl?ionization=H2

This might be of use - http://cnx.org/content/m14777/latest/
 
There is a change in the classical electrostatic energy associated with the rearranged charge distribution, which others have described above. But there is also a purely quantum-mechanical effect, which is basically just a particle-in-a-box effect. The electrons' wavefunctions spread out to encompass both atoms, increasing their wavelengths and reducing their kinetic energies. Roughly, you're doubling the wavelength along one axis. Suppose the original kinetic energy corresponding to the wavelength of each electron along each of the three axes is K. Then the separated atoms have total kinetic energy 6K. If you treat the atom as a particle in a box, with a length of 0.1 nm, then you get K=38 eV. When the two atoms form a molecule, the wavelengths parallel to the bond axis are both roughly doubled. This reduces two of the K terms to K/4, giving a total kinetic energy of about 4.5K. This makes the binding energy 1.5K=57 eV. The actual binding energy is 15.43 eV. So the particle-in-a-box argument is crude, but it does give a result on the right order of magnitude to be an important contribution to the total binding energy.
 
bcrowell said:
There is a change in the classical electrostatic energy associated with the rearranged charge distribution, which others have described above. But there is also a purely quantum-mechanical effect, which is basically just a particle-in-a-box effect. The electrons' wavefunctions spread out to encompass both atoms, increasing their wavelengths and reducing their kinetic energies. Roughly, you're doubling the wavelength along one axis. Suppose the original kinetic energy corresponding to the wavelength of each electron along each of the three axes is K. Then the separated atoms have total kinetic energy 6K. If you treat the atom as a particle in a box, with a length of 0.1 nm, then you get K=38 eV. When the two atoms form a molecule, the wavelengths parallel to the bond axis are both roughly doubled. This reduces two of the K terms to K/4, giving a total kinetic energy of about 4.5K. This makes the binding energy 1.5K=57 eV. The actual binding energy is 15.43 eV. So the particle-in-a-box argument is crude, but it does give a result on the right order of magnitude to be an important contribution to the total binding energy.

So if the total energy of two atoms apart is 6*38 eV=228 eV, and a particle-in-a-box says that close together, the total energy is 57 eV, but the real answer is 15.43 eV, would that mean the majority of the energy reduction is the particle-in-a-box effect? The other stuff would then only account for the remaining drop of 57 eV-15.43 eV, while the particle-in-a-box accounts for a drop of 228 eV-57 eV. In fact, the latter drop is 4 times as much as the former drop.
 
bcrowell's approach doesn't quite work as a rationale (except in showing that it's significant)
I'm not sure where that number came from, but the electronic energy of two hydrogen atoms is 1.0 Hartree = 27.2 eV. The binding energy of H2 is 4.52 eV.

The kinetic energy of the electrons is an order of magnitude greater than the binding energy and so is significant, but so is the nuclear attraction and electronic repulsion. The exchange/correlation energy is about on the same order.

So you can't really neglect anything in the electronic Hamiltonian and still get a decent picture of chemical bonding; (or quantum chemistry would be a lot easier) Or to put it another way: Chemistry is a very subtle effect.
 
alxm said:
bcrowell's approach doesn't quite work as a rationale (except in showing that it's significant)
That's all I was claiming -- that it was an argument to show it was significant.

alxm said:
I'm not sure where that number came from, but the electronic energy of two hydrogen atoms is 1.0 Hartree = 27.2 eV. The binding energy of H2 is 4.52 eV.

You have a particle in a box of length L=0.1 nm. \lambda=2L, p=h/\lambda, K=p^2/2m
 
  • #10
RedX said:
So if the total energy of two atoms apart is 6*38 eV=228 eV, and a particle-in-a-box says that close together, the total energy is 57 eV, but the real answer is 15.43 eV, would that mean the majority of the energy reduction is the particle-in-a-box effect?

No, the whole thing is just an order-of-magnitude estimate that shows that the change in kinetic energy is of the right order of magnitude to be relevant to the binding energy. The effect is also in the right direction to help explain the binding. (It makes the bound system more bound.)
 
  • #11
bcrowell said:
No, the whole thing is just an order-of-magnitude estimate that shows that the change in kinetic energy is of the right order of magnitude to be relevant to the binding energy. The effect is also in the right direction to help explain the binding. (It makes the bound system more bound.)

So it's sort of like measuring the strength of nuclear forces by knowing the size of a nucleus and modeling it as a particle-in-a-box (or just using the uncertainty principle) and ignoring all the nuclear physics that goes on? Everything is just based on size?
 
  • #12
RedX said:
So it's sort of like measuring the strength of nuclear forces by knowing the size of a nucleus and modeling it as a particle-in-a-box (or just using the uncertainty principle) and ignoring all the nuclear physics that goes on? Everything is just based on size?

Right. It's actually a better approximation in nuclear physics, because the nuclear potential has a flat bottom, not a singularity like the one an atomic potential has in the middle.
 

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